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	<updated>2026-10-18T17:40:05Z</updated>
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		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=User:Admin&amp;diff=8741</id>
		<title>User:Admin</title>
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		<updated>2026-10-17T08:38:29Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* &amp;amp;ge; 2020 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[File:BvM.jpg|right|]]&lt;br /&gt;
== Personal information ==&lt;br /&gt;
__NOTOC__&lt;br /&gt;
* Boudewijn van Milligen (Admin)&lt;br /&gt;
* Researcher at: &amp;lt;br&amp;gt;[[Laboratorio Nacional de Fusión]] - [[CIEMAT]] &amp;lt;br&amp;gt;Avda. Complutense 40, Edif. 66&amp;lt;br&amp;gt;28040 Madrid, España - Spain&lt;br /&gt;
* Tel. +34 - 914 962 682&lt;br /&gt;
* Email boudewijn.vanmilligen (at) ciemat.es&lt;br /&gt;
User profiles:&lt;br /&gt;
* [https://publons.com/researcher/1248698/boudewijn-ph-van-milligen/ Publons] (ResearcherID H-5121-2015)&lt;br /&gt;
* [http://orcid.org/0000-0001-5344-6274 ORCID 0000-0001-5344-6274]&lt;br /&gt;
* [https://www.scopus.com/authid/detail.uri?authorId=35476190300 Scopus AuthorID 35476190300]&lt;br /&gt;
* [http://scholar.google.com/citations?user=7z9Cr9oAAAAJ Google Scholar]&lt;br /&gt;
* [https://www.researchgate.net/profile/Boudewijn_Van_Milligen/ ResearchGate]&lt;br /&gt;
&lt;br /&gt;
== Interests ==&lt;br /&gt;
&lt;br /&gt;
* Fusion and plasma physics&lt;br /&gt;
** [[H-mode|L-H transition]], Zonal Flows&lt;br /&gt;
** [[Magnetic island]]s, MHD activity&lt;br /&gt;
* [[Anomalous transport]]&lt;br /&gt;
** Turbulence&lt;br /&gt;
** Continuous Time Random Walks&lt;br /&gt;
* Data analysis&lt;br /&gt;
** [[Causality detection]]&lt;br /&gt;
** [[Intermittence]]&lt;br /&gt;
** [[:Wikipedia:Rescaled range|Rescaled range]] or [[:Wikipedia:Hurst exponent|Hurst]] analysis&lt;br /&gt;
** [[Bayesian data analysis]]&lt;br /&gt;
** [[Biorthogonal decomposition]]&lt;br /&gt;
** [[Bicoherence]]&lt;br /&gt;
** [[TJ-II:Tomography|Tomography]]&lt;br /&gt;
&lt;br /&gt;
== Book ==&lt;br /&gt;
&lt;br /&gt;
B.Ph. van Milligen and R. Sánchez, &#039;&#039;Analysis of Turbulence in Fusion Plasmas&#039;&#039;, [[doi:10.1088/978-0-7503-4856-0|IOP Publishing (2022)]], {{ISBN|978-0-7503-4854-6}}&lt;br /&gt;
&lt;br /&gt;
== Selected publications ==&lt;br /&gt;
&lt;br /&gt;
(inverse chronological order)&lt;br /&gt;
=== &amp;amp;ge; 2020 ===&lt;br /&gt;
* Boudewijn Ph. van Milligen, Isabel García-Cortés, Kieran J. McCarthy, et al. &#039;&#039;The pump-out effect as a trigger for the electron to ion root transition in TJ-II&#039;&#039;. [[doi:10.3390/plasma9040039|Plasma, 9(4), 39 (2026)]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. van Milligen, I. Voldiner, E. de la Cal, A. Alonso Alvarez, I. Luiz Caldas and Z. Guimarães Filho, &#039;&#039;Turbulence analysis with the spectroscopic gas puff imaging diagnostic in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/1361-6587/ae92b5|Plasma Phys. Control. Fusion &#039;&#039;&#039;68&#039;&#039;&#039; (2026) 085018]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* A. Alonso Alvarez, B. P. Van Milligen, I. Voldiner, I. L. Caldas, Z. Guimarães Filho, O. Kozachok, and A. Chmyga. &#039;&#039;Edge turbulence dynamics across electron–ion root transitions during ECRH modulation experiments in the TJ-II stellarator&#039;&#039;. [[doi:10.1088/1361-6587/ae7470|Plasma Phys. Control. Fusion, &#039;&#039;&#039;68&#039;&#039;&#039; (2026) 065019]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. van Milligen, I. García-Cortés, K.J. McCarthy, et al, &#039;&#039;The rotational transform and enhanced confinement in the TJ-II stellarator&#039;&#039;, [[doi:10.1017/S0022377825100433|Journal of Plasma Physics &#039;&#039;&#039;91&#039;&#039;&#039;, 4 (2025) E98]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* Boudewijn Philip van Milligen, Teresa Estrada, Benjamin Carreras, Luis García, and TJ-II Team. &#039;&#039;Importance of the Rotational Transform for L–H Transitions in the TJ-II Stellarator&#039;&#039; [[doi:10.3390/plasma7020024|Plasma &#039;&#039;&#039;7&#039;&#039;&#039;, no. 2 (2024) 446-464]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. van Milligen, I. Voldiner, B.A. Carreras, L. García, M.A. Ochando and The TJ-II Team, &#039;&#039;Rational surfaces, flows and radial structure in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/1741-4326/aca688|Nucl. Fusion &#039;&#039;&#039;63&#039;&#039;&#039; (2023) 016027]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. Van Milligen, B.A. Carreras, L. Garcia, G. Grenfell, I. Voldiner and C. Hidalgo, &#039;&#039;The impact of radial electric fields and plasma rotation on intermittence in TJ-II&#039;&#039;, [[doi:10.1088/1361-6587/ac54e9|Plasma Phys. Control. Fusion &#039;&#039;&#039;64&#039;&#039;&#039;, 5 (2022) 055006]] ([http://documenta.ciemat.es/handle/123456789/2290 repository])&lt;br /&gt;
* B. van Milligen, A. Melnikov, B. Carreras, L. Garcia, A. Kozachek, C. Hidalgo, J. de Pablos, Ph. Khabanov, L. Eliseev, M. Drabinskij, A. Chmyga, L. Krupnik, the HIBP Team, the TJ-II Team, &#039;&#039;Topology of 2-D turbulent structures based on intermittence in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/1741-4326/ac27c9|Nucl. Fusion &#039;&#039;&#039;61&#039;&#039;&#039;, 11 (2021) 116063]] ([http://documenta.ciemat.es/handle/123456789/2281 repository])&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras, I. Voldiner, U. Losada, C. Hidalgo, and the TJ-II Team, &#039;&#039;Causality, intermittence and crossphase evolution during confinement transitions in the TJ-II stellarator&#039;&#039;, [[doi:10.1063/5.0057791|Phys. Plasmas &#039;&#039;&#039;28&#039;&#039;&#039; (2021) 092302]] ([http://documenta.ciemat.es/handle/123456789/2289 repository])&lt;br /&gt;
* B.Ph. van Milligen, B. Carreras, L. García and C. Hidalgo, &#039;&#039;The localization of low order rational surfaces based on the intermittence parameter in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/1741-4326/ab79cc|Nucl. Fusion &#039;&#039;&#039;60&#039;&#039;&#039; (2020) 056010]] ([http://documenta.ciemat.es/handle/123456789/2291 repository])&lt;br /&gt;
&lt;br /&gt;
=== 2010-2019 ===&lt;br /&gt;
* B.Ph. van Milligen, B. Carreras, L. García and J. Nicolau, &#039;&#039;The radial propagation of heat in strongly driven non-equilibrium fusion plasmas&#039;&#039;, [[doi:10.3390/e21020148|Entropy, &#039;&#039;&#039;21&#039;&#039;&#039;, 2 (2019) 148]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. van Milligen, B. Carreras, E. de la Luna and E. Solano, &#039;&#039;Radial variation of heat transport in L-mode JET discharges&#039;&#039; [[doi:10.1088/1741-4326/ab03e1|Nucl. Fusion, &#039;&#039;&#039;59&#039;&#039;&#039; (2019) 056006]] ([http://documenta.ciemat.es/handle/123456789/2292 repository])&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras, C. Hidalgo, Á. Cappa and the TJ-II Team, &#039;&#039;A possible mechanism for confinement power degradation in the TJ-II stellarator&#039;&#039;, [[doi:10.1063/1.5029881|Phys. Plasmas &#039;&#039;&#039;25&#039;&#039;&#039; (2018) 062503]] ([http://documenta.ciemat.es/handle/123456789/2308 repository])&lt;br /&gt;
* B.Ph. van Milligen, U. Hoefel, J. Nicolau, M. Hirsch, L. García, B. Carreras, C. Hidalgo and the W7-X Team, &#039;&#039;Study of radial heat transport in W7-X using the transfer entropy&#039;&#039;, [[doi:10.1088/1741-4326/aabf5d|Nucl. Fusion &#039;&#039;&#039;58&#039;&#039;&#039; (2018) 076002]] ([http://hdl.handle.net/10016/32565 repository])&lt;br /&gt;
* B.Ph. van Milligen, J. Hernández Nicolau, B. Liu, G. Grenfell, U. Losada, B. Carreras, L. Garcia and C. Hidalgo, &#039;&#039;Filaments in the edge confinement region of TJ-II&#039;&#039;, [[doi:10.1088/1741-4326/aa9db6|Nucl. Fusion &#039;&#039;&#039;58&#039;&#039;&#039; (2018) 026030]] ([http://hdl.handle.net/10016/32563 repository])&lt;br /&gt;
* B.Ph. van Milligen, J.H. Nicolau, L. García, B.A. Carreras, C. Hidalgo and the TJ-II Team, &#039;&#039;The impact of rational surfaces on radial heat transport in TJ-II&#039;&#039;, [[doi:10.1088/1741-4326/aa611f|Nucl. Fusion &#039;&#039;&#039;57&#039;&#039;&#039;, 5 (2017) 056028]], [https://arxiv.org/abs/1701.04574 arxiv:1701.04574]&lt;br /&gt;
* B.Ph. van Milligen, T. Estrada, B.A. Carreras, E. Ascasíbar, C. Hidalgo, I. Pastor, J.M. Fontdecaba, R. Balbín and the TJ-II Team, &#039;&#039;The causal impact of magnetic fluctuations in slow and fast L–H transitions at TJ-II&#039;&#039;, [[doi:10.1063/1.4958807|Phys. Plasmas &#039;&#039;&#039;23&#039;&#039;&#039; (2016) 072305]], [https://arxiv.org/abs/1512.06525 arxiv:1512.06525]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras, L. García, A. Martín de Aguilera, C. Hidalgo, J.H. Nicolau and the TJ-II Team, &#039;&#039;The causal relation between turbulent particle flux and density gradient&#039;&#039;, [[doi:10.1063/1.4958806|Phys. Plasmas &#039;&#039;&#039;23&#039;&#039;&#039; (2016) 072307]]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras and D.E. Newman, &#039;&#039;Constructing criteria to diagnose the likelihood of extreme events in the case of the electric power grid&#039;&#039;, [[doi:10.1063/1.4943569|Chaos &#039;&#039;&#039;26&#039;&#039;&#039; (2016) 033109]]&lt;br /&gt;
* B.Ph. van Milligen, T. Estrada, L. García, D. López-Bruna, B. Carreras, Y. Xu, M. Ochando, C. Hidalgo, J. Reynolds-Barredo and A. López-Fraguas, &#039;&#039;The role of magnetic islands in modifying long range temporal correlations of density fluctuations and local heat transport&#039;&#039;, [[doi:10.1088/0029-5515/56/1/016013|Nucl. Fusion, &#039;&#039;&#039;56&#039;&#039;&#039;, 1 (2016) 016013]], [https://arxiv.org/abs/1506.06890 arxiv:1506.06890]&lt;br /&gt;
* B.Ph. van Milligen, E. Sánchez, A. Alonso, M.A. Pedrosa, C. Hidalgo, A. Martín de Aguilera, A. López Fraguas, &#039;&#039;The use of the Biorthogonal Decomposition for the identification of zonal flows at TJ-II&#039;&#039;, [[doi:10.1088/0741-3335/57/2/025005|Plasma Phys. Control. Fusion &#039;&#039;&#039;57&#039;&#039;&#039;, 2 (2015) 025005]], [https://arxiv.org/abs/1408.1845 arxiv:1408.1845]&lt;br /&gt;
* B.Ph. van Milligen, P.D. Bons, &#039;&#039;Simplified numerical model for clarifying scaling behavior in the intermediate dispersion regime in homogeneous porous media&#039;&#039;, [[doi:10.1016/j.cpc.2014.09.006|Comput. Phys. Commun. &#039;&#039;&#039;185&#039;&#039;&#039; (2014) 3291]], [https://arxiv.org/abs/1409.2724 arxiv:1409.2724]&lt;br /&gt;
* B.Ph. van Milligen, G. Birkenmeier, M. Ramisch, T. Estrada, C. Hidalgo and A. Alonso, &#039;&#039;Causality detection and turbulence in fusion plasmas&#039;&#039;, [[doi:10.1088/0029-5515/54/2/023011|Nucl. Fusion &#039;&#039;&#039;54&#039;&#039;&#039; (2014), 023011]], [https://arxiv.org/abs/1309.7769 arxiv:1309.7769]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Parallel and perpendicular turbulence correlation length in the TJ-II Stellarator&#039;&#039;, [[doi:10.1088/0029-5515/53/9/093025|Nucl. Fusion &#039;&#039;&#039;53&#039;&#039;&#039; (2013) 093025]], [https://arxiv.org/abs/1306.1395 arxiv:1306.1395]&lt;br /&gt;
* P.D. Bons, B.Ph. van Milligen, P. Blum, &#039;&#039;A general unified expression for solute and heat dispersion in homogeneous porous media&#039;&#039;, [[doi:10.1002/wrcr.20488|Water Resour. Res. &#039;&#039;&#039;49&#039;&#039;&#039; (2013) 1]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Spatiotemporal and wavenumber resolved bicoherence at the low to high confinement transition in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/53/11/113034|Nucl. Fusion &#039;&#039;&#039;53&#039;&#039;&#039; (2013) 113034]], [https://arxiv.org/abs/1211.0420 arxiv:1211.0420]&lt;br /&gt;
* B. Ph. van Milligen, R. Sánchez and C. Hidalgo, &#039;&#039;Relevance of Uncorrelated Lorentzian Pulses for the Interpretation of Turbulence in the Edge of Magnetically Confined Toroidal Plasmas&#039;&#039;, [[doi:10.1103/PhysRevLett.109.105001|Phys. Rev. Lett. &#039;&#039;&#039;109&#039;&#039;&#039; (2012) 105001]], [https://arxiv.org/abs/1204.6185 arxiv:1204.6185]&lt;br /&gt;
* B.Ph. van Milligen, P.D. Bons, &#039;&#039;Analytical model for tracer dispersion in porous media&#039;&#039;, [[doi:10.1103/PhysRevE.85.011306|Phys. Rev. E 85 (2012) 011306]], [https://arxiv.org/abs/1111.6512 arxiv:1111.6512]&lt;br /&gt;
* B.Ph. van Milligen, L. García, B.A. Carreras, M.A. Pedrosa, C. Hidalgo, J.A. Alonso, T. Estrada and E. Ascasíbar, &#039;&#039;MHD mode activity and the velocity shear layer at TJ-II&#039;&#039;, [[doi:10.1088/0029-5515/52/1/013006|Nucl. Fusion &#039;&#039;&#039;52&#039;&#039;&#039; (2012) 013006]]&lt;br /&gt;
* B.Ph. van Milligen, T. Estrada, E. Ascasíbar, et al, &#039;&#039;Integrated data analysis at TJ-II: the density profile&#039;&#039;, [[doi:10.1063/1.3608551|Rev. Sci. Instrum. &#039;&#039;&#039;82&#039;&#039;&#039; (2011) 073503]]&lt;br /&gt;
* B.A. Carreras et al., &#039;&#039;Reconstruction of intermittent waveforms associated with the zonal flow at the transition leading to the edge shear flow layer&#039;&#039;, [[doi:10.1088/0029-5515/51/5/053022|Nucl. Fusion &#039;&#039;&#039;51&#039;&#039;&#039; (2011) 053022]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;A global resonance phenomenon at the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/51/1/013005|Nucl. Fusion &#039;&#039;&#039;51&#039;&#039;&#039; (2011) 013005]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;The dynamics of the formation of the edge particle transport barrier at TJ-II&#039;&#039;, [[doi:10.1088/0029-5515/51/11/113002|Nucl. Fusion &#039;&#039;&#039;51&#039;&#039;&#039; (2011) 113002]]&lt;br /&gt;
&lt;br /&gt;
=== 2000-2009 ===&lt;br /&gt;
* B.Ph. van Milligen, I. Calvo and R. Sánchez, &#039;&#039;Continuous time random walks in finite domains and general boundary conditions: some formal considerations&#039;&#039;, [[doi:10.1088/1751-8113/41/21/215004|J. Phys. A: Math. Theor. &#039;&#039;&#039;41&#039;&#039;&#039; (2008) 215004]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Quantifying profile stiffness&#039;&#039;, [http://www.jspf.or.jp/PFR/PFR_articles/pfr2008S1/pfr2008_03-S1070.html Plasma and Fusion Research, &#039;&#039;&#039;3&#039;&#039;&#039; (2008) S1070]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Bicoherence during confinement transitions in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/48/11/115003|Nucl. Fusion &#039;&#039;&#039;48&#039;&#039;&#039; (2008) 115003]]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras, V.E. Lynch and R. Sánchez, &#039;&#039;Pulse propagation in a simple probabilistic transport model&#039;&#039;, [[doi:10.1088/0029-5515/47/3/004|Nucl. Fusion &#039;&#039;&#039;47&#039;&#039;&#039; (2007) 189]]&lt;br /&gt;
* B.Ph. van Milligen, P.D. Bons, B.A. Carreras and R. Sánchez, &#039;&#039;On the applicability of Fick&#039;s Law to diffusion in inhomogeneous systems&#039;&#039;, [[doi:10.1088/0143-0807/26/5/023|Eur. J. Phys. &#039;&#039;&#039;26&#039;&#039;&#039; (2005) 913]]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras and R. Sánchez, &#039;&#039;The foundations of diffusion revisited&#039;&#039;, [[doi:10.1088/0741-3335/47/12B/S56|Plasma Phys. Control. Fusion &#039;&#039;&#039;47&#039;&#039;&#039; (2005) B743]]&lt;br /&gt;
* B.Ph. Van Milligen et al, &#039;&#039;Additional evidence for the universality of turbulent fluctuations and fluxes in the scrape-off layer region of fusion plasmas&#039;&#039;, [[doi:10.1063/1.1884615|Phys. Plasmas &#039;&#039;&#039;12&#039;&#039;&#039; (2005) 052507]]&lt;br /&gt;
* B.Ph. van Milligen, R. Sánchez and B.A. Carreras, &#039;&#039;Probabilistic finite-size transport models for fusion: anomalous transport and scaling laws&#039;&#039;, [[doi:10.1063/1.1701893|Phys. Plasmas &#039;&#039;&#039;11&#039;&#039;&#039;, 5 (2004) 2272]]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras and R. Sánchez, &#039;&#039;Uphill transport and the probabilistic transport model&#039;&#039;, [[doi:10.1063/1.1763915|Phys. Plasmas &#039;&#039;&#039;11&#039;&#039;&#039;, 3787 (2004)]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Revision of TV Thomson scattering data analysis and detection of profile structure&#039;&#039;, [[doi:10.1063/1.1597951|Rev. Sci. Instrum. &#039;&#039;&#039;74&#039;&#039;&#039; (2003) 3998]]&lt;br /&gt;
* B.Ph. van Milligen, E. de la Luna, F.L. Tabarés, et al., &#039;&#039;Ballistic transport phenomena in TJ-II&#039;&#039;, [[doi:10.1088/0029-5515/42/7/301|Nucl. Fusion &#039;&#039;&#039;42&#039;&#039;&#039; (2002) 787]]&lt;br /&gt;
=== 1990 - 1999 ===&lt;br /&gt;
* B.A. Carreras, B.Ph. van Milligen, et al, &#039;&#039;Experimental evidence of long-range correlation and self-similarity in plasma fluctuations&#039;&#039;, [[doi:10.1063/1.873490|Phys. Plasmas &#039;&#039;&#039;6&#039;&#039;&#039;, 5 (1999) 1885]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Statistically robust linear and non-linear wavelet analysis applied to plasma edge turbulence&#039;&#039;, [[doi:10.1063/1.1147727|Rev. Sci. Instrum. &#039;&#039;&#039;68&#039;&#039;&#039; (1997) 967]]&lt;br /&gt;
* B.Ph. van Milligen, V. Tribaldos, J.A. Jiménez, &#039;&#039;A neural network differential equation and plasma equilibrium solver&#039;&#039;, [[doi:10.1103/PhysRevLett.75.3594|Phys. Rev. Lett. &#039;&#039;&#039;75&#039;&#039;&#039; (1995) 3594]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Nonlinear phenomena and intermittency in plasma turbulence&#039;&#039;, [[doi:10.1103/PhysRevLett.74.395|Phys. Rev. Lett. &#039;&#039;&#039;74&#039;&#039;&#039;, 3 (1995) 395]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Wavelet bicoherence: a new turbulence analysis tool&#039;&#039;, [[doi:10.1063/1.871199|Phys. Plasmas &#039;&#039;&#039;2&#039;&#039;&#039;, 8 (1995) 3017]]&lt;br /&gt;
* B.Ph. van Milligen and A. Lopez Fraguas, &#039;&#039;Expansion of vacuum magnetic fields in toroidal harmonics&#039;&#039;, [[doi:10.1016/0010-4655(94)90112-0|Comput. Phys. Commun. &#039;&#039;&#039;81&#039;&#039;&#039;, Issues 1-2 (1994) 74-90]]&lt;br /&gt;
* B.Ph. van Milligen, A.C.A.P. van Lammeren, N.J. Lopes Cardozo, F.C. Schüller and M. Verreck, &#039;&#039;Gradients of electron temperature and density across m=2 islands in RTP&#039;&#039;, [[doi:10.1088/0029-5515/33/8/I03|Nucl. Fusion &#039;&#039;&#039;33&#039;&#039;&#039; (1993) 1119]]&lt;br /&gt;
* B.Ph. van Milligen, N.J. Lopes Cardozo, &#039;&#039;Function Parametrization: a fast inverse mapping method&#039;&#039;, [[doi:10.1016/0010-4655(91)90073-T|Comput. Phys. Commun. &#039;&#039;&#039;66&#039;&#039;&#039; (1991) 243]]&lt;br /&gt;
* B.Ph. van Milligen et al., &#039;&#039;Application of Function Parametrization to the analysis of polarimetry and interferometry data in TEXTOR&#039;&#039;, [[doi:10.1088/0029-5515/31/2/007|Nucl. Fusion &#039;&#039;&#039;31&#039;&#039;&#039; (1991) 309]]&lt;br /&gt;
* B.Ph. van Milligen, &#039;&#039;Exact relations between multipole moments of the flux and moments of the toroidal current density in tokamaks&#039;&#039;, [[doi:10.1088/0029-5515/30/1/012|Nucl. Fusion &#039;&#039;&#039;30&#039;&#039;&#039; (1990) 157]]&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8740</id>
		<title>TJ-II:Magnetic configuration</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8740"/>
		<updated>2026-10-13T12:48:20Z</updated>

		<summary type="html">&lt;p&gt;Admin: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The magnetic configuration of [[TJ-II]] in vacuum is completely determined by the currents flowing through the [[TJ-II:Coil system|external coils]].&lt;br /&gt;
Magnetic configurations are labelled as &#039;xxx_yy_zz&#039;, where&lt;br /&gt;
* &#039;xxx&#039;: 10 times the current (in kA) in the circular coil&lt;br /&gt;
* &#039;yy&#039;: 10 times the current (in kA) in the helical coil&lt;br /&gt;
* &#039;zz&#039;: 10 times the current (in kA) in the vertical field coils&lt;br /&gt;
The current in the toroidal field coils is not specified, as its value is adjusted to guarantee central absorption of the [[TJ-II:Electron Cyclotron Resonant Heating|Electron Cyclotron Resonant Heating]] source (requiring a specific &#039;resonant&#039; value of the magnetic field at the magnetic axis, &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
Configuration list:&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable sortable&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Configuration &lt;br /&gt;
! &amp;lt;math&amp;gt;r_{av}&amp;lt;/math&amp;gt; (cm) &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(0)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(a)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{m,av}&amp;lt;/math&amp;gt;(T) &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt; (T) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(0^\circ)&amp;lt;/math&amp;gt; (m) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(45^\circ)&amp;lt;/math&amp;gt; (m) &lt;br /&gt;
! Shear (%) &lt;br /&gt;
! Well (%)&lt;br /&gt;
|-&lt;br /&gt;
|0_20_13    ||1.139      || 1.185      || 1.194     ||  1.033     || 0.9504     ||  1.644      || 1.374     || 0.7793      ||5.7521E-02&lt;br /&gt;
|-&lt;br /&gt;
|0_30_15    ||4.228      || 1.518      || 1.698     ||  1.019     || 0.9500     ||  1.658      || 1.360     ||  11.85      || 1.050&lt;br /&gt;
|-&lt;br /&gt;
|0_40_18    ||5.903      || 1.756      || 2.003     ||  1.008     || 0.9505     ||  1.671      || 1.347     ||  14.09      || 1.217&lt;br /&gt;
|-&lt;br /&gt;
|0_50_22    ||6.480      || 1.936      || 2.230     || 0.9973     || 0.9502     ||  1.682      || 1.336     ||  15.17      || 2.481&lt;br /&gt;
|-&lt;br /&gt;
|0_60_26    ||8.500      || 2.073      || 2.399     || 0.9885     || 0.9502     ||  1.692      || 1.326     ||  15.70      || 3.218&lt;br /&gt;
|-&lt;br /&gt;
|0_70_29    ||7.147      || 2.187      || 2.434     || 0.9805     || 0.9503     ||  1.701      || 1.317     ||  11.30      || 2.985&lt;br /&gt;
|-&lt;br /&gt;
|0_80_34    ||6.902      || 2.284      || 2.469     || 0.9736     || 0.9506     ||  1.710      || 1.308     ||  8.084      || 2.735&lt;br /&gt;
|-&lt;br /&gt;
|0_90_38    ||6.738      || 2.366      || 2.514     || 0.9663     || 0.9503     ||  1.719      || 1.299     ||  6.269      || 2.534&lt;br /&gt;
|-&lt;br /&gt;
|0_100_42   ||12.59      || 2.436      || 2.667     || 0.9601     || 0.9505     ||  1.727      || 1.291     ||  9.493      || 4.643&lt;br /&gt;
|-&lt;br /&gt;
|0_110_46   ||10.67      || 2.493      || 2.667     || 0.9539     || 0.9503     ||  1.734      || 1.284     ||  6.980      || 4.554&lt;br /&gt;
|-&lt;br /&gt;
|0_120_50   ||12.71      || 2.548      || 2.667     || 0.9482     || 0.9504     ||  1.742      || 1.276     ||  4.683      || 4.272&lt;br /&gt;
|-&lt;br /&gt;
|10_20_18   || 2.557     ||  1.148     ||  1.184    ||   1.024    ||  0.9514    ||   1.652     ||  1.366    ||   3.183     || 0.2469&lt;br /&gt;
|-&lt;br /&gt;
|10_30_20   || 6.083     ||  1.438     ||  1.602    ||   1.010    ||  0.9501    ||   1.666     ||  1.352    ||   11.35     ||  1.398&lt;br /&gt;
|-&lt;br /&gt;
|10_40_24   || 6.921     ||  1.659     ||  1.880    ||   1.000    ||  0.9504    ||   1.678     ||  1.340    ||   13.34     ||  2.751&lt;br /&gt;
|-&lt;br /&gt;
|10_50_27   || 8.140     ||  1.826     ||  1.997    ||  0.9909    ||  0.9504    ||   1.688     ||  1.329    ||   9.321     ||  3.241&lt;br /&gt;
|-&lt;br /&gt;
|10_60_31   || 9.350     ||  1.965     ||  2.183    ||  0.9826    ||  0.9505    ||   1.698     ||  1.319    ||   11.11     ||  3.084&lt;br /&gt;
|-&lt;br /&gt;
|10_70_35   || 10.10     ||  2.077     ||  2.288    ||  0.9750    ||  0.9505    ||   1.707     ||  1.310    ||   10.16     ||  3.597&lt;br /&gt;
|-&lt;br /&gt;
|10_80_38   || 9.810     ||  2.174     ||  2.371    ||  0.9674    ||  0.9502    ||   1.716     ||  1.302    ||   9.037     ||  3.908&lt;br /&gt;
|-&lt;br /&gt;
|10_90_42   || 10.54     ||  2.257     ||  2.434    ||  0.9610    ||  0.9503    ||   1.724     ||  1.294    ||   7.851     ||  4.281&lt;br /&gt;
|-&lt;br /&gt;
|10_100_47  || 10.21     ||  2.327     ||  2.482    ||  0.9546    ||  0.9502    ||   1.732     ||  1.286    ||   6.647     ||  4.236&lt;br /&gt;
|-&lt;br /&gt;
|10_110_51  || 11.11     ||  2.395     ||  2.547    ||  0.9488    ||  0.9501    ||   1.740     ||  1.278    ||   6.331     ||  5.121&lt;br /&gt;
|-&lt;br /&gt;
|10_120_55  || 10.04     ||  2.451     ||  2.565    ||  0.9432    ||  0.9502    ||   1.747     ||  1.271    ||   4.674     ||  4.426&lt;br /&gt;
|-&lt;br /&gt;
|20_10_21   || 1.213     || 0.7902     || 0.7956    ||   1.028    ||  0.9503    ||   1.645     ||  1.373    ||  0.6830     || 3.7624E-02&lt;br /&gt;
|-&lt;br /&gt;
|20_20_22   || 3.952     ||  1.136     ||  1.185    ||   1.014    ||  0.9500    ||   1.661     ||  1.357    ||   4.350     || 0.4717&lt;br /&gt;
|-&lt;br /&gt;
|20_30_25   || 6.779     ||  1.395     ||  1.521    ||   1.003    ||  0.9502    ||   1.673     ||  1.344    ||   9.049     ||  1.550&lt;br /&gt;
|-&lt;br /&gt;
|20_40_28   || 8.475     ||  1.592     ||  1.771    ||  0.9922    ||  0.9498    ||   1.685     ||  1.333    ||   11.25     ||  2.879&lt;br /&gt;
|-&lt;br /&gt;
|20_50_32   || 8.039     ||  1.756     ||  1.906    ||  0.9842    ||  0.9505    ||   1.695     ||  1.323    ||   8.571     ||  3.131&lt;br /&gt;
|-&lt;br /&gt;
|20_60_35   || 11.21     ||  1.884     ||  1.997    ||  0.9755    ||  0.9498    ||   1.705     ||  1.313    ||   5.968     ||  1.980&lt;br /&gt;
|-&lt;br /&gt;
|20_70_39   || 11.08     ||  1.994     ||  2.154    ||  0.9689    ||  0.9504    ||   1.714     ||  1.304    ||   7.982     ||  3.385&lt;br /&gt;
|-&lt;br /&gt;
|20_80_43   || 12.14     ||  2.092     ||  2.255    ||  0.9614    ||  0.9497    ||   1.722     ||  1.296    ||   7.811     ||  4.133&lt;br /&gt;
|-&lt;br /&gt;
|20_90_47   || 12.83     ||  2.174     ||  2.324    ||  0.9558    ||  0.9503    ||   1.730     ||  1.288    ||   6.862     ||  4.713&lt;br /&gt;
|-&lt;br /&gt;
|20_100_51  || 12.68     ||  2.246     ||  2.379    ||  0.9498    ||  0.9503    ||   1.738     ||  1.280    ||   5.945     ||  4.930&lt;br /&gt;
|-&lt;br /&gt;
|20_110_55  || 13.79     ||  2.313     ||  2.434    ||  0.9443    ||  0.9505    ||   1.745     ||  1.273    ||   5.248     ||  5.117&lt;br /&gt;
|-&lt;br /&gt;
|20_120_59  || 13.91     ||  2.368     ||  2.483    ||  0.9386    ||  0.9502    ||   1.752     ||  1.265    ||   4.822     ||  5.418&lt;br /&gt;
|-&lt;br /&gt;
|30_10_25   || 2.709     || 0.8385     || 0.8507    ||   1.018    ||  0.9501    ||   1.654     ||  1.363    ||   1.452     || 0.1431&lt;br /&gt;
|-&lt;br /&gt;
|30_20_27   || 5.443     ||  1.134     ||  1.189    ||   1.007    ||  0.9514    ||   1.669     ||  1.349    ||   4.847     || 0.7001&lt;br /&gt;
|-&lt;br /&gt;
|30_30_30   || 8.180     ||  1.368     ||  1.481    ||  0.9956    ||  0.9506    ||   1.681     ||  1.337    ||   8.332     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|30_40_33   || 9.756     ||  1.550     ||  1.687    ||  0.9860    ||  0.9503    ||   1.692     ||  1.326    ||   8.877     ||  2.798&lt;br /&gt;
|-&lt;br /&gt;
|30_50_37   || 11.16     ||  1.702     ||  1.878    ||  0.9779    ||  0.9503    ||   1.702     ||  1.316    ||   10.37     ||  4.941&lt;br /&gt;
|-&lt;br /&gt;
|30_60_40   || 9.262     ||  1.827     ||  1.936    ||  0.9706    ||  0.9505    ||   1.711     ||  1.307    ||   5.952     ||  3.624&lt;br /&gt;
|-&lt;br /&gt;
|30_70_44   || 12.28     ||  1.937     ||  2.007    ||  0.9631    ||  0.9502    ||   1.720     ||  1.298    ||   3.593     ||  4.431&lt;br /&gt;
|-&lt;br /&gt;
|30_80_48   || 13.28     ||  2.033     ||  2.149    ||  0.9567    ||  0.9502    ||   1.728     ||  1.290    ||   5.702     ||  3.674&lt;br /&gt;
|-&lt;br /&gt;
|30_90_52   || 14.16     ||  2.115     ||  2.231    ||  0.9504    ||  0.9501    ||   1.736     ||  1.282    ||   5.476     ||  4.227&lt;br /&gt;
|-&lt;br /&gt;
|30_100_56  || 14.97     ||  2.187     ||  2.295    ||  0.9448    ||  0.9502    ||   1.743     ||  1.275    ||   4.949     ||  4.755&lt;br /&gt;
|-&lt;br /&gt;
|30_110_59  || 15.76     ||  2.246     ||  2.356    ||  0.9391    ||  0.9500    ||   1.751     ||  1.267    ||   4.920     ||  5.215&lt;br /&gt;
|-&lt;br /&gt;
|30_120_63  || 14.48     ||  2.306     ||  2.389    ||  0.9343    ||  0.9504    ||   1.758     ||  1.260    ||   3.573     ||  5.025&lt;br /&gt;
|-&lt;br /&gt;
|40_00_27   || 1.350     || 0.5464     || 0.5471    ||   1.024    ||  0.9504    ||   1.647     ||  1.371    ||  0.1331     || 2.4768E-02&lt;br /&gt;
|-&lt;br /&gt;
|40_10_29   || 4.111     || 0.8821     || 0.9010    ||   1.010    ||  0.9510    ||   1.663     ||  1.355    ||   2.152     || 0.2456&lt;br /&gt;
|-&lt;br /&gt;
|40_20_31   || 6.646     ||  1.146     ||  1.202    ||  0.9975    ||  0.9501    ||   1.677     ||  1.341    ||   4.928     || 0.8185&lt;br /&gt;
|-&lt;br /&gt;
|40_30_34   || 9.328     ||  1.354     ||  1.452    ||  0.9884    ||  0.9506    ||   1.688     ||  1.330    ||   7.247     ||  1.826&lt;br /&gt;
|-&lt;br /&gt;
|40_40_37   || 11.15     ||  1.523     ||  1.646    ||  0.9788    ||  0.9498    ||   1.699     ||  1.319    ||   8.061     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|40_50_41   || 12.66     ||  1.666     ||  1.797    ||  0.9719    ||  0.9506    ||   1.708     ||  1.310    ||   7.872     ||  4.310&lt;br /&gt;
|-&lt;br /&gt;
|40_60_44   || 12.34     ||  1.786     ||  1.927    ||  0.9637    ||  0.9497    ||   1.717     ||  1.301    ||   7.879     ||  5.834&lt;br /&gt;
|-&lt;br /&gt;
|40_70_48   || 9.734     ||  1.894     ||  1.963    ||  0.9579    ||  0.9504    ||   1.726     ||  1.292    ||   3.625     ||  3.668&lt;br /&gt;
|-&lt;br /&gt;
|40_80_52   || 13.96     ||  1.986     ||  2.067    ||  0.9515    ||  0.9503    ||   1.734     ||  1.284    ||   4.054     ||  3.028&lt;br /&gt;
|-&lt;br /&gt;
|40_90_56   || 15.39     ||  2.062     ||  2.156    ||  0.9457    ||  0.9504    ||   1.741     ||  1.277    ||   4.529     ||  3.841&lt;br /&gt;
|-&lt;br /&gt;
|40_100_60  || 16.40     ||  2.132     ||  2.232    ||  0.9400    ||  0.9502    ||   1.749     ||  1.269    ||   4.683     ||  4.355&lt;br /&gt;
|-&lt;br /&gt;
|40_110_64  || 18.12     ||  2.199     ||  2.288    ||  0.9348    ||  0.9503    ||   1.756     ||  1.262    ||   4.049     ||  4.651&lt;br /&gt;
|-&lt;br /&gt;
|40_120_68  || 16.81     ||  2.256     ||  2.327    ||  0.9295    ||  0.9501    ||   1.763     ||  1.255    ||   3.158     ||  4.904&lt;br /&gt;
|-&lt;br /&gt;
|50_00_31   || 2.818     || 0.6329     || 0.6375    ||   1.013    ||  0.9498    ||   1.657     ||  1.361    ||  0.7286     || 6.1871E-02&lt;br /&gt;
|-&lt;br /&gt;
|50_10_33   || 5.588     || 0.9254     || 0.9532    ||   1.001    ||  0.9506    ||   1.672     ||  1.346    ||   3.003     || 0.3605&lt;br /&gt;
|-&lt;br /&gt;
|50_20_36   || 8.222     ||  1.160     ||  1.216    ||  0.9902    ||  0.9502    ||   1.684     ||  1.334    ||   4.838     ||  1.060&lt;br /&gt;
|-&lt;br /&gt;
|50_30_39   || 10.67     ||  1.352     ||  1.435    ||  0.9815    ||  0.9505    ||   1.695     ||  1.323    ||   6.163     ||  2.008&lt;br /&gt;
|-&lt;br /&gt;
|50_40_42   || 12.44     ||  1.508     ||  1.609    ||  0.9733    ||  0.9504    ||   1.705     ||  1.313    ||   6.719     ||  2.910&lt;br /&gt;
|-&lt;br /&gt;
|50_50_46   || 13.94     ||  1.644     ||  1.758    ||  0.9661    ||  0.9505    ||   1.714     ||  1.303    ||   6.944     ||  4.001&lt;br /&gt;
|-&lt;br /&gt;
|50_60_49   || 15.09     ||  1.757     ||  1.887    ||  0.9587    ||  0.9502    ||   1.723     ||  1.295    ||   7.390     ||  6.217&lt;br /&gt;
|-&lt;br /&gt;
|50_70_53   || 13.03     ||  1.855     ||  1.955    ||  0.9524    ||  0.9502    ||   1.731     ||  1.287    ||   5.353     ||  5.830&lt;br /&gt;
|-&lt;br /&gt;
|50_80_56   || 16.73     ||  1.949     ||  2.004    ||  0.9463    ||  0.9501    ||   1.739     ||  1.279    ||   2.807     ||  4.003&lt;br /&gt;
|-&lt;br /&gt;
|50_90_60   || 16.70     ||  2.011     ||  2.101    ||  0.9407    ||  0.9502    ||   1.747     ||  1.271    ||   4.501     ||  3.444&lt;br /&gt;
|-&lt;br /&gt;
|50_100_64  || 18.15     ||  2.090     ||  2.183    ||  0.9351    ||  0.9500    ||   1.754     ||  1.264    ||   4.434     ||  3.907&lt;br /&gt;
|-&lt;br /&gt;
|50_110_68  || 17.53     ||  2.154     ||  2.223    ||  0.9297    ||  0.9498    ||   1.762     ||  1.256    ||   3.205     ||  4.270&lt;br /&gt;
|-&lt;br /&gt;
|50_120_72  || 19.13     ||  2.213     ||  2.288    ||  0.9250    ||  0.9501    ||   1.768     ||  1.250    ||   3.417     ||  4.378&lt;br /&gt;
|-&lt;br /&gt;
|60_00_35   || 4.247     || 0.7126     || 0.7205    ||   1.003    ||  0.9498    ||   1.667     ||  1.352    ||   1.108     || 0.1270&lt;br /&gt;
|-&lt;br /&gt;
|60_10_37   || 6.862     || 0.9679     ||  1.002    ||  0.9934    ||  0.9509    ||   1.680     ||  1.338    ||   3.520     || 0.4827&lt;br /&gt;
|-&lt;br /&gt;
|60_20_40   || 9.669     ||  1.179     ||  1.240    ||  0.9831    ||  0.9503    ||   1.692     ||  1.326    ||   5.202     ||  1.236&lt;br /&gt;
|-&lt;br /&gt;
|60_30_43   || 12.01     ||  1.354     ||  1.435    ||  0.9747    ||  0.9502    ||   1.702     ||  1.316    ||   5.973     ||  2.132&lt;br /&gt;
|-&lt;br /&gt;
|60_40_46   || 13.48     ||  1.500     ||  1.593    ||  0.9672    ||  0.9503    ||   1.712     ||  1.306    ||   6.170     ||  2.806&lt;br /&gt;
|-&lt;br /&gt;
|60_50_50   || 15.36     ||  1.627     ||  1.732    ||  0.9601    ||  0.9504    ||   1.721     ||  1.297    ||   6.467     ||  3.895&lt;br /&gt;
|-&lt;br /&gt;
|60_60_53   || 16.79     ||  1.734     ||  1.851    ||  0.9528    ||  0.9499    ||   1.729     ||  1.289    ||   6.731     ||  5.666&lt;br /&gt;
|-&lt;br /&gt;
|60_70_57   || 15.88     ||  1.829     ||  1.934    ||  0.9473    ||  0.9502    ||   1.737     ||  1.281    ||   5.736     ||  6.958&lt;br /&gt;
|-&lt;br /&gt;
|60_80_61   || 13.66     ||  1.918     ||  1.968    ||  0.9428    ||  0.9514    ||   1.745     ||  1.273    ||   2.622     ||  4.555&lt;br /&gt;
|-&lt;br /&gt;
|60_90_64   || 17.29     ||  2.009     ||  2.063    ||  0.9359    ||  0.9501    ||   1.753     ||  1.265    ||   2.640     ||  1.637&lt;br /&gt;
|-&lt;br /&gt;
|60_100_68  || 17.62     ||  2.049     ||  2.122    ||  0.9304    ||  0.9497    ||   1.760     ||  1.258    ||   3.560     ||  3.718&lt;br /&gt;
|-&lt;br /&gt;
|60_110_72  || 17.50     ||  2.118     ||  2.177    ||  0.9257    ||  0.9501    ||   1.767     ||  1.251    ||   2.811     ||  4.023&lt;br /&gt;
|-&lt;br /&gt;
|60_120_76  || 17.78     ||  2.174     ||  2.222    ||  0.9217    ||  0.9510    ||   1.774     ||  1.244    ||   2.209     ||  4.211&lt;br /&gt;
|-&lt;br /&gt;
|70_00_39   || 5.731     || 0.7825     || 0.7975    ||  0.9949    ||  0.9497    ||   1.675     ||  1.343    ||   1.908     || 0.2335&lt;br /&gt;
|-&lt;br /&gt;
|70_10_41   || 8.418     ||  1.009     ||  1.048    ||  0.9860    ||  0.9509    ||   1.688     ||  1.330    ||   3.845     || 0.6755&lt;br /&gt;
|-&lt;br /&gt;
|70_20_44   || 11.09     ||  1.201     ||  1.265    ||  0.9767    ||  0.9504    ||   1.699     ||  1.319    ||   5.345     ||  1.317&lt;br /&gt;
|-&lt;br /&gt;
|70_30_47   || 13.41     ||  1.361     ||  1.441    ||  0.9688    ||  0.9504    ||   1.709     ||  1.309    ||   5.859     ||  2.187&lt;br /&gt;
|-&lt;br /&gt;
|70_40_51   || 14.99     ||  1.496     ||  1.591    ||  0.9615    ||  0.9503    ||   1.718     ||  1.300    ||   6.348     ||  2.859&lt;br /&gt;
|-&lt;br /&gt;
|70_50_54   || 16.87     ||  1.617     ||  1.712    ||  0.9543    ||  0.9501    ||   1.727     ||  1.291    ||   5.843     ||  3.756&lt;br /&gt;
|-&lt;br /&gt;
|70_60_57   || 17.89     ||  1.718     ||  1.823    ||  0.9479    ||  0.9500    ||   1.735     ||  1.283    ||   6.140     ||  4.746&lt;br /&gt;
|-&lt;br /&gt;
|70_70_61   || 18.26     ||  1.812     ||  1.928    ||  0.9423    ||  0.9503    ||   1.743     ||  1.275    ||   6.353     ||  6.812&lt;br /&gt;
|-&lt;br /&gt;
|70_80_65   || 16.37     ||  1.896     ||  1.962    ||  0.9363    ||  0.9499    ||   1.751     ||  1.267    ||   3.469     ||  5.948&lt;br /&gt;
|-&lt;br /&gt;
|70_90_68   || 9.135     ||  1.980     ||  1.988    ||  0.9317    ||  0.9506    ||   1.758     ||  1.260    ||  0.3692     || 0.1186&lt;br /&gt;
|-&lt;br /&gt;
|70_100_72  || 18.64     ||  2.007     ||  2.094    ||  0.9267    ||  0.9506    ||   1.765     ||  1.253    ||   4.327     ||  3.356&lt;br /&gt;
|-&lt;br /&gt;
|70_110_76  || 18.23     ||  2.088     ||  2.147    ||  0.9219    ||  0.9507    ||   1.772     ||  1.246    ||   2.792     ||  3.707&lt;br /&gt;
|-&lt;br /&gt;
|70_120_80  || 17.89     ||  2.145     ||  2.184    ||  0.9171    ||  0.9506    ||   1.779     ||  1.239    ||   1.846     ||  4.043&lt;br /&gt;
|-&lt;br /&gt;
|80_00_42   ||7.247      ||0.8436      ||0.8697     || 0.9869     || 0.9497     ||  1.684      || 1.335     ||  3.094      ||0.2402&lt;br /&gt;
|-&lt;br /&gt;
|80_10_45   ||9.865      || 1.049      || 1.095     || 0.9794     || 0.9513     ||  1.695      || 1.323     ||  4.371      ||0.7359&lt;br /&gt;
|-&lt;br /&gt;
|80_20_48   ||12.28      || 1.226      || 1.290     || 0.9697     || 0.9500     ||  1.706      || 1.312     ||  5.206      || 1.327&lt;br /&gt;
|-&lt;br /&gt;
|80_30_51   ||14.38      || 1.370      || 1.454     || 0.9626     || 0.9503     ||  1.715      || 1.303     ||  6.088      || 2.102&lt;br /&gt;
|-&lt;br /&gt;
|80_40_54   ||16.47      || 1.500      || 1.594     || 0.9549     || 0.9497     ||  1.724      || 1.294     ||  6.263      || 2.799&lt;br /&gt;
|-&lt;br /&gt;
|80_50_58   ||17.63      || 1.612      || 1.706     || 0.9492     || 0.9503     ||  1.733      || 1.285     ||  5.842      || 3.329&lt;br /&gt;
|-&lt;br /&gt;
|80_60_61   ||18.84      || 1.712      || 1.814     || 0.9436     || 0.9507     ||  1.741      || 1.277     ||  5.984      || 3.990&lt;br /&gt;
|-&lt;br /&gt;
|80_70_65   ||19.27      || 1.799      || 1.898     || 0.9372     || 0.9501     ||  1.749      || 1.269     ||  5.555      || 4.728&lt;br /&gt;
|-&lt;br /&gt;
|80_80_69   ||17.96      || 1.880      || 1.935     || 0.9321     || 0.9503     ||  1.756      || 1.262     ||  2.921      || 3.774&lt;br /&gt;
|-&lt;br /&gt;
|80_90_73   ||13.42      || 1.957      || 1.982     || 0.9266     || 0.9500     ||  1.764      || 1.254     ||  1.312      ||0.6938&lt;br /&gt;
|-&lt;br /&gt;
|80_100_76  || 18.53     ||  2.008     ||  2.065    ||  0.9220    ||  0.9504    ||   1.770     ||  1.247    ||   2.839     ||  1.773&lt;br /&gt;
|-&lt;br /&gt;
|80_110_80  || 18.41     ||  2.059     ||  2.117    ||  0.9176    ||  0.9507    ||   1.777     ||  1.241    ||   2.847     ||  3.632&lt;br /&gt;
|-&lt;br /&gt;
|80_120_84  || 18.26     ||  2.117     ||  2.157    ||  0.9122    ||  0.9496    ||   1.784     ||  1.234    ||   1.872     ||  3.986&lt;br /&gt;
|-&lt;br /&gt;
|90_00_46   || 8.679     || 0.9022     || 0.9354    ||  0.9802    ||  0.9501    ||   1.691     ||  1.327    ||   3.678     || 0.3981&lt;br /&gt;
|-&lt;br /&gt;
|90_10_49   || 11.45     ||  1.090     ||  1.146    ||  0.9717    ||  0.9502    ||   1.702     ||  1.315    ||   5.148     || 0.8099&lt;br /&gt;
|-&lt;br /&gt;
|90_20_52   || 12.44     ||  1.247     ||  1.323    ||  0.9640    ||  0.9503    ||   1.712     ||  1.305    ||   6.100     ||  1.079&lt;br /&gt;
|-&lt;br /&gt;
|90_30_55   || 16.14     ||  1.383     ||  1.475    ||  0.9571    ||  0.9504    ||   1.722     ||  1.296    ||   6.607     ||  2.158&lt;br /&gt;
|-&lt;br /&gt;
|90_40_58   || 17.45     ||  1.506     ||  1.597    ||  0.9499    ||  0.9501    ||   1.731     ||  1.287    ||   6.012     ||  2.629&lt;br /&gt;
|-&lt;br /&gt;
|90_50_62   || 18.70     ||  1.609     ||  1.706    ||  0.9438    ||  0.9501    ||   1.739     ||  1.279    ||   6.003     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|90_60_65   || 18.77     ||  1.703     ||  1.789    ||  0.9381    ||  0.9502    ||   1.747     ||  1.271    ||   5.045     ||  3.047&lt;br /&gt;
|-&lt;br /&gt;
|90_70_69   || 18.43     ||  1.787     ||  1.852    ||  0.9324    ||  0.9500    ||   1.754     ||  1.263    ||   3.623     ||  3.117&lt;br /&gt;
|-&lt;br /&gt;
|90_80_73   || 17.72     ||  1.868     ||  1.909    ||  0.9269    ||  0.9497    ||   1.762     ||  1.256    ||   2.217     ||  2.354&lt;br /&gt;
|-&lt;br /&gt;
|90_90_76   || 14.40     ||  1.940     ||  1.956    ||  0.9221    ||  0.9499    ||   1.769     ||  1.249    ||  0.8079     || 0.8326&lt;br /&gt;
|-&lt;br /&gt;
|90_100_80  || 18.53     ||  2.009     ||  2.038    ||  0.9176    ||  0.9503    ||   1.776     ||  1.242    ||   1.484     ||  1.095&lt;br /&gt;
|-&lt;br /&gt;
|90_110_84  || 18.97     ||  2.021     ||  2.094    ||  0.9129    ||  0.9502    ||   1.783     ||  1.235    ||   3.625     ||  3.669&lt;br /&gt;
|-&lt;br /&gt;
|90_120_88  || 17.79     ||  2.090     ||  2.129    ||  0.9077    ||  0.9494    ||   1.789     ||  1.229    ||   1.827     ||  3.862&lt;br /&gt;
|-&lt;br /&gt;
|100_00_50  || 10.07     || 0.9544     || 0.9970    ||  0.9732    ||  0.9499    ||   1.699     ||  1.319    ||   4.471     || 0.4341&lt;br /&gt;
|-&lt;br /&gt;
|100_10_53  || 12.78     ||  1.127     ||  1.186    ||  0.9649    ||  0.9499    ||   1.710     ||  1.308    ||   5.262     || 0.9629&lt;br /&gt;
|-&lt;br /&gt;
|100_16_55  || 13.69     ||  1.215     ||  1.287    ||  0.9610    ||  0.9501    ||   1.715     ||  1.302    ||   5.901     ||  1.023&lt;br /&gt;
|-&lt;br /&gt;
|100_20_56  || 10.86     ||  1.271     ||  1.324    ||  0.9583    ||  0.9502    ||   1.719     ||  1.299    ||   4.120     || 0.8295&lt;br /&gt;
|-&lt;br /&gt;
|100_22_56  || 15.40     ||  1.309     ||  1.381    ||  0.9412    ||  0.9362    ||   1.722     ||  1.296    ||   5.552     ||  1.648&lt;br /&gt;
|-&lt;br /&gt;
|100_24_58  || 15.90     ||  1.326     ||  1.406    ||  0.9552    ||  0.9499    ||   1.722     ||  1.295    ||   6.105     ||  1.792&lt;br /&gt;
|-&lt;br /&gt;
|100_26_58  || 16.42     ||  1.352     ||  1.435    ||  0.9538    ||  0.9499    ||   1.724     ||  1.293    ||   6.137     ||  1.888&lt;br /&gt;
|-&lt;br /&gt;
|100_28_59  || 17.07     ||  1.375     ||  1.464    ||  0.9527    ||  0.9501    ||   1.726     ||  1.291    ||   6.475     ||  1.983&lt;br /&gt;
|-&lt;br /&gt;
|100_30_59  || 17.29     ||  1.398     ||  1.490    ||  0.9511    ||  0.9500    ||   1.728     ||  1.289    ||   6.561     ||  2.075&lt;br /&gt;
|-&lt;br /&gt;
|100_32_60  || 17.74     ||  1.423     ||  1.517    ||  0.9499    ||  0.9499    ||   1.730     ||  1.288    ||   6.596     ||  2.165&lt;br /&gt;
|-&lt;br /&gt;
|100_36_61  || 18.37     ||  1.467     ||  1.567    ||  0.9475    ||  0.9501    ||   1.733     ||  1.284    ||   6.819     ||  2.183&lt;br /&gt;
|-&lt;br /&gt;
|100_40_63  || 18.77     ||  1.509     ||  1.608    ||  0.9450    ||  0.9500    ||   1.736     ||  1.281    ||   6.553     ||  2.304&lt;br /&gt;
|-&lt;br /&gt;
|100_44_64  || 19.25     ||  1.551     ||  1.653    ||  0.9426    ||  0.9500    ||   1.740     ||  1.278    ||   6.569     ||  2.360&lt;br /&gt;
|-&lt;br /&gt;
|100_48_65  || 19.16     ||  1.591     ||  1.684    ||  0.9400    ||  0.9500    ||   1.743     ||  1.275    ||   5.807     ||  2.555&lt;br /&gt;
|-&lt;br /&gt;
|100_50_65  || 19.11     ||  1.613     ||  1.704    ||  0.9381    ||  0.9501    ||   1.745     ||  1.274    ||   5.628     ||  2.649&lt;br /&gt;
|-&lt;br /&gt;
|100_55_67  || 19.04     ||  1.659     ||  1.739    ||  0.9352    ||  0.9500    ||   1.749     ||  1.270    ||   4.839     ||  2.808&lt;br /&gt;
|-&lt;br /&gt;
|100_56_67  || 18.93     ||  1.667     ||  1.742    ||  0.9347    ||  0.9501    ||   1.750     ||  1.269    ||   4.522     ||  2.692&lt;br /&gt;
|-&lt;br /&gt;
|100_60_68  || 19.04     ||  1.702     ||  1.775    ||  0.9325    ||  0.9500    ||   1.753     ||  1.266    ||   4.326     ||  2.720&lt;br /&gt;
|-&lt;br /&gt;
|100_64_70  || 18.76     ||  1.733     ||  1.799    ||  0.9303    ||  0.9500    ||   1.756     ||  1.263    ||   3.774     ||  2.676&lt;br /&gt;
|-&lt;br /&gt;
|100_68_72  || 18.46     ||  1.771     ||  1.825    ||  0.9279    ||  0.9494    ||   1.759     ||  1.259    ||   3.080     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_70_73  || 18.23     ||  1.784     ||  1.841    ||  0.9277    ||  0.9500    ||   1.760     ||  1.258    ||   3.166     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_80_77  || 16.73     ||  1.855     ||  1.885    ||  0.9261    ||  0.9532    ||   1.767     ||  1.251    ||   1.617     ||  1.818&lt;br /&gt;
|-&lt;br /&gt;
|100_90_80  || 13.86     ||  1.931     ||  1.936    ||  0.9172    ||  0.9494    ||   1.774     ||  1.244    ||  0.2833     || 0.7382&lt;br /&gt;
|-&lt;br /&gt;
|100_95_82  || 11.27     ||  1.967     ||  1.964    ||  0.9243    ||  0.9582    ||   1.777     ||  1.241    || -0.1435     || 6.8954E-02&lt;br /&gt;
|-&lt;br /&gt;
|100_105_86 || 16.96     ||  2.019     ||  2.045    ||  0.9233    ||  0.9617    ||   1.783     ||  1.235    ||   1.268     ||  1.425&lt;br /&gt;
|-&lt;br /&gt;
|100_110_88 || 18.88     ||  2.020     ||  2.073    ||  0.9229    ||  0.9634    ||   1.786     ||  1.232    ||   2.618     ||  2.366&lt;br /&gt;
|-&lt;br /&gt;
|100_120_92 || 17.63     ||  2.064     ||  2.113    ||  0.9044    ||  0.9501    ||   1.794     ||  1.224    ||   2.379     ||  3.790&lt;br /&gt;
|-&lt;br /&gt;
|110_00_54  || 11.70     ||  1.006     ||  1.060    ||  0.9663    ||  0.9498    ||   1.706     ||  1.312    ||   5.370     || 0.4642&lt;br /&gt;
|-&lt;br /&gt;
|110_10_57  || 13.97     ||  1.160     ||  1.232    ||  0.9593    ||  0.9502    ||   1.716     ||  1.301    ||   6.136     || 0.8247&lt;br /&gt;
|-&lt;br /&gt;
|110_20_60  || 15.75     ||  1.298     ||  1.372    ||  0.9526    ||  0.9504    ||   1.726     ||  1.292    ||   5.739     ||  1.330&lt;br /&gt;
|-&lt;br /&gt;
|110_30_63  || 18.56     ||  1.415     ||  1.516    ||  0.9455    ||  0.9500    ||   1.734     ||  1.284    ||   7.122     ||  1.849&lt;br /&gt;
|-&lt;br /&gt;
|110_40_66  || 19.50     ||  1.521     ||  1.622    ||  0.9398    ||  0.9503    ||   1.743     ||  1.275    ||   6.602     ||  1.921&lt;br /&gt;
|-&lt;br /&gt;
|110_50_70  || 19.07     ||  1.618     ||  1.696    ||  0.9336    ||  0.9498    ||   1.751     ||  1.267    ||   4.873     ||  2.085&lt;br /&gt;
|-&lt;br /&gt;
|110_60_73  || 18.32     ||  1.702     ||  1.761    ||  0.9291    ||  0.9507    ||   1.758     ||  1.260    ||   3.471     ||  2.033&lt;br /&gt;
|-&lt;br /&gt;
|110_70_77  || 17.13     ||  1.782     ||  1.816    ||  0.9237    ||  0.9504    ||   1.766     ||  1.252    ||   1.948     ||  1.838&lt;br /&gt;
|-&lt;br /&gt;
|110_80_81  || 15.56     ||  1.853     ||  1.871    ||  0.9192    ||  0.9508    ||   1.773     ||  1.245    ||  0.9878     ||  1.332&lt;br /&gt;
|-&lt;br /&gt;
|110_90_84  || 13.12     ||  1.923     ||  1.926    ||  0.9142    ||  0.9506    ||   1.780     ||  1.238    ||  0.1639     || 0.5301&lt;br /&gt;
|-&lt;br /&gt;
|110_95_86  || 10.73     ||  1.963     ||  1.955    ||  0.9095    ||  0.9486    ||   1.783     ||  1.235    || -0.3746     || 8.1449E-04&lt;br /&gt;
|-&lt;br /&gt;
|110_110_92 || 17.29     ||  2.020     ||  2.055    ||  0.9056    ||  0.9509    ||   1.793     ||  1.225    ||   1.768     ||  2.045&lt;br /&gt;
|-&lt;br /&gt;
|110_120_95 || 17.55     ||  2.048     ||  2.095    ||  0.9014    ||  0.9510    ||   1.799     ||  1.219    ||   2.314     ||  3.774&lt;br /&gt;
|-&lt;br /&gt;
|120_00_57  || 13.14     ||  1.050     ||  1.117    ||  0.9599    ||  0.9497    ||   1.714     ||  1.305    ||   6.304     || 0.4861&lt;br /&gt;
|-&lt;br /&gt;
|120_10_60  || 14.81     ||  1.196     ||  1.268    ||  0.9534    ||  0.9501    ||   1.723     ||  1.295    ||   6.054     || 0.8382&lt;br /&gt;
|-&lt;br /&gt;
|120_20_63  || 17.57     ||  1.323     ||  1.409    ||  0.9458    ||  0.9494    ||   1.732     ||  1.286    ||   6.504     ||  1.409&lt;br /&gt;
|-&lt;br /&gt;
|120_30_67  || 19.50     ||  1.435     ||  1.539    ||  0.9407    ||  0.9503    ||   1.741     ||  1.277    ||   7.263     ||  1.529&lt;br /&gt;
|-&lt;br /&gt;
|120_40_70  || 19.38     ||  1.534     ||  1.621    ||  0.9335    ||  0.9492    ||   1.749     ||  1.269    ||   5.695     ||  1.632&lt;br /&gt;
|-&lt;br /&gt;
|120_50_74  || 18.34     ||  1.621     ||  1.684    ||  0.9294    ||  0.9503    ||   1.756     ||  1.262    ||   3.910     ||  1.864&lt;br /&gt;
|-&lt;br /&gt;
|120_60_77  || 17.24     ||  1.703     ||  1.743    ||  0.9246    ||  0.9507    ||   1.764     ||  1.254    ||   2.381     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|120_70_81  || 16.02     ||  1.780     ||  1.803    ||  0.9197    ||  0.9509    ||   1.771     ||  1.247    ||   1.312     ||  1.511&lt;br /&gt;
|-&lt;br /&gt;
|120_80_84  || 14.49     ||  1.850     ||  1.860    ||  0.9150    ||  0.9509    ||   1.778     ||  1.240    ||  0.5347     ||  1.076&lt;br /&gt;
|-&lt;br /&gt;
|120_90_88  || 12.18     ||  1.918     ||  1.918    ||  0.9096    ||  0.9501    ||   1.785     ||  1.233    || -4.1127E-02 || 0.3613&lt;br /&gt;
|-&lt;br /&gt;
|120_95_90  || 10.06     ||  1.957     ||  1.950    ||  0.9071    ||  0.9499    ||   1.788     ||  1.230    || -0.3241     ||  0.000&lt;br /&gt;
|-&lt;br /&gt;
|120_115_97 || 16.46     ||  2.020     ||  2.066    ||  0.8983    ||  0.9497    ||   1.801     ||  1.216    ||   2.258     ||  2.404&lt;br /&gt;
|-&lt;br /&gt;
|120_120_99 || 17.58     ||  2.008     ||  2.092    ||  0.8967    ||  0.9501    ||   1.804     ||  1.213    ||   4.186     ||  3.647&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Flexibility ==&lt;br /&gt;
&lt;br /&gt;
[[File:Flexibility TJ-II.png|300px|thumb|right|Flexibility diagram of TJ-II magnetic configurations. Several lines of constant rotational transform are highlighted and labelled with the corresponding edge &amp;lt;math&amp;gt;\iota/2\pi&amp;lt;/math&amp;gt;-value.]]&lt;br /&gt;
TJ-II has considerable configurational flexibility, as observed in the &#039;flexibility diagram&#039;&amp;lt;ref&amp;gt;E. Ascasíbar, T. Estrada, F. Castejón, A. López-Fraguas, I. Pastor, J. Sánchez, U. Stroth, J. Qin and TJ-II Team, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/45/4/009|Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276–284]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
The sum &amp;lt;math&amp;gt;I_{CC}+I_{HX}&amp;lt;/math&amp;gt; is an important factor determining the size of the plasma, and should not be too small. Thus, reasonably-sized plasmas are limited to the upper right triangle of this diagram.&lt;br /&gt;
Some of this flexibility space has been explored, as in the &#039;magnetic well scan&#039; experiments&amp;lt;ref&amp;gt;A. de Aguilera, F. Castejón, E. Ascasíbar, et al. &#039;&#039;Magnetic well scan and confinement in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/55/11/113014|Nucl. Fusion, 55(11):113014, 2015]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
More recently, the [[rotational transform]] in the plasma edge region was found to be of importance for [[H-mode|L-H]] confinement transitions&amp;lt;ref&amp;gt;B. P. van Milligen, T. Estrada, B. Carreras, L. García, and TJ-II Team. &#039;&#039;Importance of the rotational transform for L–H transitions in the TJ-II stellarator&#039;&#039;, [[doi:10.3390/plasma7020024|Plasma, 7(2):446–464, 2024]].&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8735</id>
		<title>TJ-II:Magnetic configuration</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8735"/>
		<updated>2026-10-13T09:52:53Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* Flexibility */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The magnetic configuration of [[TJ-II]] in vacuum is completely determined by the currents flowing through the [[TJ-II:Coil system|external coils]].&lt;br /&gt;
Magnetic configurations are labelled as &#039;xxx_yy_zz&#039;, where&lt;br /&gt;
* &#039;xxx&#039;: 10 times the current (in kA) in the circular coil&lt;br /&gt;
* &#039;yy&#039;: 10 times the current (in kA) in the helical coil&lt;br /&gt;
* &#039;zz&#039;: 10 times the current (in kA) in the vertical field coils&lt;br /&gt;
The current in the toroidal field coils is not specified, as its value is adjusted to guarantee central absorption of the [[TJ-II:Electron Cyclotron Resonant Heating|Electron Cyclotron Resonant Heating]] source (requiring a specific &#039;resonant&#039; value of the magnetic field at the magnetic axis, &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
Configuration list:&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;width: 100%&amp;quot; border=&amp;quot;1&amp;quot;||&lt;br /&gt;
|-&lt;br /&gt;
! Configuration &lt;br /&gt;
! &amp;lt;math&amp;gt;r_{av}&amp;lt;/math&amp;gt; (cm) &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(0)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(a)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{m,av}&amp;lt;/math&amp;gt;(T) &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt; (T) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(0^\circ)&amp;lt;/math&amp;gt; (m) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(45^\circ)&amp;lt;/math&amp;gt; (m) &lt;br /&gt;
! Shear (%) &lt;br /&gt;
! Well (%)&lt;br /&gt;
|-&lt;br /&gt;
|0_20_13    ||1.139      || 1.185      || 1.194     ||  1.033     || 0.9504     ||  1.644      || 1.374     || 0.7793      ||5.7521E-02&lt;br /&gt;
|-&lt;br /&gt;
|0_30_15    ||4.228      || 1.518      || 1.698     ||  1.019     || 0.9500     ||  1.658      || 1.360     ||  11.85      || 1.050&lt;br /&gt;
|-&lt;br /&gt;
|0_40_18    ||5.903      || 1.756      || 2.003     ||  1.008     || 0.9505     ||  1.671      || 1.347     ||  14.09      || 1.217&lt;br /&gt;
|-&lt;br /&gt;
|0_50_22    ||6.480      || 1.936      || 2.230     || 0.9973     || 0.9502     ||  1.682      || 1.336     ||  15.17      || 2.481&lt;br /&gt;
|-&lt;br /&gt;
|0_60_26    ||8.500      || 2.073      || 2.399     || 0.9885     || 0.9502     ||  1.692      || 1.326     ||  15.70      || 3.218&lt;br /&gt;
|-&lt;br /&gt;
|0_70_29    ||7.147      || 2.187      || 2.434     || 0.9805     || 0.9503     ||  1.701      || 1.317     ||  11.30      || 2.985&lt;br /&gt;
|-&lt;br /&gt;
|0_80_34    ||6.902      || 2.284      || 2.469     || 0.9736     || 0.9506     ||  1.710      || 1.308     ||  8.084      || 2.735&lt;br /&gt;
|-&lt;br /&gt;
|0_90_38    ||6.738      || 2.366      || 2.514     || 0.9663     || 0.9503     ||  1.719      || 1.299     ||  6.269      || 2.534&lt;br /&gt;
|-&lt;br /&gt;
|0_100_42   ||12.59      || 2.436      || 2.667     || 0.9601     || 0.9505     ||  1.727      || 1.291     ||  9.493      || 4.643&lt;br /&gt;
|-&lt;br /&gt;
|0_110_46   ||10.67      || 2.493      || 2.667     || 0.9539     || 0.9503     ||  1.734      || 1.284     ||  6.980      || 4.554&lt;br /&gt;
|-&lt;br /&gt;
|0_120_50   ||12.71      || 2.548      || 2.667     || 0.9482     || 0.9504     ||  1.742      || 1.276     ||  4.683      || 4.272&lt;br /&gt;
|-&lt;br /&gt;
|10_20_18   || 2.557     ||  1.148     ||  1.184    ||   1.024    ||  0.9514    ||   1.652     ||  1.366    ||   3.183     || 0.2469&lt;br /&gt;
|-&lt;br /&gt;
|10_30_20   || 6.083     ||  1.438     ||  1.602    ||   1.010    ||  0.9501    ||   1.666     ||  1.352    ||   11.35     ||  1.398&lt;br /&gt;
|-&lt;br /&gt;
|10_40_24   || 6.921     ||  1.659     ||  1.880    ||   1.000    ||  0.9504    ||   1.678     ||  1.340    ||   13.34     ||  2.751&lt;br /&gt;
|-&lt;br /&gt;
|10_50_27   || 8.140     ||  1.826     ||  1.997    ||  0.9909    ||  0.9504    ||   1.688     ||  1.329    ||   9.321     ||  3.241&lt;br /&gt;
|-&lt;br /&gt;
|10_60_31   || 9.350     ||  1.965     ||  2.183    ||  0.9826    ||  0.9505    ||   1.698     ||  1.319    ||   11.11     ||  3.084&lt;br /&gt;
|-&lt;br /&gt;
|10_70_35   || 10.10     ||  2.077     ||  2.288    ||  0.9750    ||  0.9505    ||   1.707     ||  1.310    ||   10.16     ||  3.597&lt;br /&gt;
|-&lt;br /&gt;
|10_80_38   || 9.810     ||  2.174     ||  2.371    ||  0.9674    ||  0.9502    ||   1.716     ||  1.302    ||   9.037     ||  3.908&lt;br /&gt;
|-&lt;br /&gt;
|10_90_42   || 10.54     ||  2.257     ||  2.434    ||  0.9610    ||  0.9503    ||   1.724     ||  1.294    ||   7.851     ||  4.281&lt;br /&gt;
|-&lt;br /&gt;
|10_100_47  || 10.21     ||  2.327     ||  2.482    ||  0.9546    ||  0.9502    ||   1.732     ||  1.286    ||   6.647     ||  4.236&lt;br /&gt;
|-&lt;br /&gt;
|10_110_51  || 11.11     ||  2.395     ||  2.547    ||  0.9488    ||  0.9501    ||   1.740     ||  1.278    ||   6.331     ||  5.121&lt;br /&gt;
|-&lt;br /&gt;
|10_120_55  || 10.04     ||  2.451     ||  2.565    ||  0.9432    ||  0.9502    ||   1.747     ||  1.271    ||   4.674     ||  4.426&lt;br /&gt;
|-&lt;br /&gt;
|20_10_21   || 1.213     || 0.7902     || 0.7956    ||   1.028    ||  0.9503    ||   1.645     ||  1.373    ||  0.6830     || 3.7624E-02&lt;br /&gt;
|-&lt;br /&gt;
|20_20_22   || 3.952     ||  1.136     ||  1.185    ||   1.014    ||  0.9500    ||   1.661     ||  1.357    ||   4.350     || 0.4717&lt;br /&gt;
|-&lt;br /&gt;
|20_30_25   || 6.779     ||  1.395     ||  1.521    ||   1.003    ||  0.9502    ||   1.673     ||  1.344    ||   9.049     ||  1.550&lt;br /&gt;
|-&lt;br /&gt;
|20_40_28   || 8.475     ||  1.592     ||  1.771    ||  0.9922    ||  0.9498    ||   1.685     ||  1.333    ||   11.25     ||  2.879&lt;br /&gt;
|-&lt;br /&gt;
|20_50_32   || 8.039     ||  1.756     ||  1.906    ||  0.9842    ||  0.9505    ||   1.695     ||  1.323    ||   8.571     ||  3.131&lt;br /&gt;
|-&lt;br /&gt;
|20_60_35   || 11.21     ||  1.884     ||  1.997    ||  0.9755    ||  0.9498    ||   1.705     ||  1.313    ||   5.968     ||  1.980&lt;br /&gt;
|-&lt;br /&gt;
|20_70_39   || 11.08     ||  1.994     ||  2.154    ||  0.9689    ||  0.9504    ||   1.714     ||  1.304    ||   7.982     ||  3.385&lt;br /&gt;
|-&lt;br /&gt;
|20_80_43   || 12.14     ||  2.092     ||  2.255    ||  0.9614    ||  0.9497    ||   1.722     ||  1.296    ||   7.811     ||  4.133&lt;br /&gt;
|-&lt;br /&gt;
|20_90_47   || 12.83     ||  2.174     ||  2.324    ||  0.9558    ||  0.9503    ||   1.730     ||  1.288    ||   6.862     ||  4.713&lt;br /&gt;
|-&lt;br /&gt;
|20_100_51  || 12.68     ||  2.246     ||  2.379    ||  0.9498    ||  0.9503    ||   1.738     ||  1.280    ||   5.945     ||  4.930&lt;br /&gt;
|-&lt;br /&gt;
|20_110_55  || 13.79     ||  2.313     ||  2.434    ||  0.9443    ||  0.9505    ||   1.745     ||  1.273    ||   5.248     ||  5.117&lt;br /&gt;
|-&lt;br /&gt;
|20_120_59  || 13.91     ||  2.368     ||  2.483    ||  0.9386    ||  0.9502    ||   1.752     ||  1.265    ||   4.822     ||  5.418&lt;br /&gt;
|-&lt;br /&gt;
|30_10_25   || 2.709     || 0.8385     || 0.8507    ||   1.018    ||  0.9501    ||   1.654     ||  1.363    ||   1.452     || 0.1431&lt;br /&gt;
|-&lt;br /&gt;
|30_20_27   || 5.443     ||  1.134     ||  1.189    ||   1.007    ||  0.9514    ||   1.669     ||  1.349    ||   4.847     || 0.7001&lt;br /&gt;
|-&lt;br /&gt;
|30_30_30   || 8.180     ||  1.368     ||  1.481    ||  0.9956    ||  0.9506    ||   1.681     ||  1.337    ||   8.332     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|30_40_33   || 9.756     ||  1.550     ||  1.687    ||  0.9860    ||  0.9503    ||   1.692     ||  1.326    ||   8.877     ||  2.798&lt;br /&gt;
|-&lt;br /&gt;
|30_50_37   || 11.16     ||  1.702     ||  1.878    ||  0.9779    ||  0.9503    ||   1.702     ||  1.316    ||   10.37     ||  4.941&lt;br /&gt;
|-&lt;br /&gt;
|30_60_40   || 9.262     ||  1.827     ||  1.936    ||  0.9706    ||  0.9505    ||   1.711     ||  1.307    ||   5.952     ||  3.624&lt;br /&gt;
|-&lt;br /&gt;
|30_70_44   || 12.28     ||  1.937     ||  2.007    ||  0.9631    ||  0.9502    ||   1.720     ||  1.298    ||   3.593     ||  4.431&lt;br /&gt;
|-&lt;br /&gt;
|30_80_48   || 13.28     ||  2.033     ||  2.149    ||  0.9567    ||  0.9502    ||   1.728     ||  1.290    ||   5.702     ||  3.674&lt;br /&gt;
|-&lt;br /&gt;
|30_90_52   || 14.16     ||  2.115     ||  2.231    ||  0.9504    ||  0.9501    ||   1.736     ||  1.282    ||   5.476     ||  4.227&lt;br /&gt;
|-&lt;br /&gt;
|30_100_56  || 14.97     ||  2.187     ||  2.295    ||  0.9448    ||  0.9502    ||   1.743     ||  1.275    ||   4.949     ||  4.755&lt;br /&gt;
|-&lt;br /&gt;
|30_110_59  || 15.76     ||  2.246     ||  2.356    ||  0.9391    ||  0.9500    ||   1.751     ||  1.267    ||   4.920     ||  5.215&lt;br /&gt;
|-&lt;br /&gt;
|30_120_63  || 14.48     ||  2.306     ||  2.389    ||  0.9343    ||  0.9504    ||   1.758     ||  1.260    ||   3.573     ||  5.025&lt;br /&gt;
|-&lt;br /&gt;
|40_00_27   || 1.350     || 0.5464     || 0.5471    ||   1.024    ||  0.9504    ||   1.647     ||  1.371    ||  0.1331     || 2.4768E-02&lt;br /&gt;
|-&lt;br /&gt;
|40_10_29   || 4.111     || 0.8821     || 0.9010    ||   1.010    ||  0.9510    ||   1.663     ||  1.355    ||   2.152     || 0.2456&lt;br /&gt;
|-&lt;br /&gt;
|40_20_31   || 6.646     ||  1.146     ||  1.202    ||  0.9975    ||  0.9501    ||   1.677     ||  1.341    ||   4.928     || 0.8185&lt;br /&gt;
|-&lt;br /&gt;
|40_30_34   || 9.328     ||  1.354     ||  1.452    ||  0.9884    ||  0.9506    ||   1.688     ||  1.330    ||   7.247     ||  1.826&lt;br /&gt;
|-&lt;br /&gt;
|40_40_37   || 11.15     ||  1.523     ||  1.646    ||  0.9788    ||  0.9498    ||   1.699     ||  1.319    ||   8.061     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|40_50_41   || 12.66     ||  1.666     ||  1.797    ||  0.9719    ||  0.9506    ||   1.708     ||  1.310    ||   7.872     ||  4.310&lt;br /&gt;
|-&lt;br /&gt;
|40_60_44   || 12.34     ||  1.786     ||  1.927    ||  0.9637    ||  0.9497    ||   1.717     ||  1.301    ||   7.879     ||  5.834&lt;br /&gt;
|-&lt;br /&gt;
|40_70_48   || 9.734     ||  1.894     ||  1.963    ||  0.9579    ||  0.9504    ||   1.726     ||  1.292    ||   3.625     ||  3.668&lt;br /&gt;
|-&lt;br /&gt;
|40_80_52   || 13.96     ||  1.986     ||  2.067    ||  0.9515    ||  0.9503    ||   1.734     ||  1.284    ||   4.054     ||  3.028&lt;br /&gt;
|-&lt;br /&gt;
|40_90_56   || 15.39     ||  2.062     ||  2.156    ||  0.9457    ||  0.9504    ||   1.741     ||  1.277    ||   4.529     ||  3.841&lt;br /&gt;
|-&lt;br /&gt;
|40_100_60  || 16.40     ||  2.132     ||  2.232    ||  0.9400    ||  0.9502    ||   1.749     ||  1.269    ||   4.683     ||  4.355&lt;br /&gt;
|-&lt;br /&gt;
|40_110_64  || 18.12     ||  2.199     ||  2.288    ||  0.9348    ||  0.9503    ||   1.756     ||  1.262    ||   4.049     ||  4.651&lt;br /&gt;
|-&lt;br /&gt;
|40_120_68  || 16.81     ||  2.256     ||  2.327    ||  0.9295    ||  0.9501    ||   1.763     ||  1.255    ||   3.158     ||  4.904&lt;br /&gt;
|-&lt;br /&gt;
|50_00_31   || 2.818     || 0.6329     || 0.6375    ||   1.013    ||  0.9498    ||   1.657     ||  1.361    ||  0.7286     || 6.1871E-02&lt;br /&gt;
|-&lt;br /&gt;
|50_10_33   || 5.588     || 0.9254     || 0.9532    ||   1.001    ||  0.9506    ||   1.672     ||  1.346    ||   3.003     || 0.3605&lt;br /&gt;
|-&lt;br /&gt;
|50_20_36   || 8.222     ||  1.160     ||  1.216    ||  0.9902    ||  0.9502    ||   1.684     ||  1.334    ||   4.838     ||  1.060&lt;br /&gt;
|-&lt;br /&gt;
|50_30_39   || 10.67     ||  1.352     ||  1.435    ||  0.9815    ||  0.9505    ||   1.695     ||  1.323    ||   6.163     ||  2.008&lt;br /&gt;
|-&lt;br /&gt;
|50_40_42   || 12.44     ||  1.508     ||  1.609    ||  0.9733    ||  0.9504    ||   1.705     ||  1.313    ||   6.719     ||  2.910&lt;br /&gt;
|-&lt;br /&gt;
|50_50_46   || 13.94     ||  1.644     ||  1.758    ||  0.9661    ||  0.9505    ||   1.714     ||  1.303    ||   6.944     ||  4.001&lt;br /&gt;
|-&lt;br /&gt;
|50_60_49   || 15.09     ||  1.757     ||  1.887    ||  0.9587    ||  0.9502    ||   1.723     ||  1.295    ||   7.390     ||  6.217&lt;br /&gt;
|-&lt;br /&gt;
|50_70_53   || 13.03     ||  1.855     ||  1.955    ||  0.9524    ||  0.9502    ||   1.731     ||  1.287    ||   5.353     ||  5.830&lt;br /&gt;
|-&lt;br /&gt;
|50_80_56   || 16.73     ||  1.949     ||  2.004    ||  0.9463    ||  0.9501    ||   1.739     ||  1.279    ||   2.807     ||  4.003&lt;br /&gt;
|-&lt;br /&gt;
|50_90_60   || 16.70     ||  2.011     ||  2.101    ||  0.9407    ||  0.9502    ||   1.747     ||  1.271    ||   4.501     ||  3.444&lt;br /&gt;
|-&lt;br /&gt;
|50_100_64  || 18.15     ||  2.090     ||  2.183    ||  0.9351    ||  0.9500    ||   1.754     ||  1.264    ||   4.434     ||  3.907&lt;br /&gt;
|-&lt;br /&gt;
|50_110_68  || 17.53     ||  2.154     ||  2.223    ||  0.9297    ||  0.9498    ||   1.762     ||  1.256    ||   3.205     ||  4.270&lt;br /&gt;
|-&lt;br /&gt;
|50_120_72  || 19.13     ||  2.213     ||  2.288    ||  0.9250    ||  0.9501    ||   1.768     ||  1.250    ||   3.417     ||  4.378&lt;br /&gt;
|-&lt;br /&gt;
|60_00_35   || 4.247     || 0.7126     || 0.7205    ||   1.003    ||  0.9498    ||   1.667     ||  1.352    ||   1.108     || 0.1270&lt;br /&gt;
|-&lt;br /&gt;
|60_10_37   || 6.862     || 0.9679     ||  1.002    ||  0.9934    ||  0.9509    ||   1.680     ||  1.338    ||   3.520     || 0.4827&lt;br /&gt;
|-&lt;br /&gt;
|60_20_40   || 9.669     ||  1.179     ||  1.240    ||  0.9831    ||  0.9503    ||   1.692     ||  1.326    ||   5.202     ||  1.236&lt;br /&gt;
|-&lt;br /&gt;
|60_30_43   || 12.01     ||  1.354     ||  1.435    ||  0.9747    ||  0.9502    ||   1.702     ||  1.316    ||   5.973     ||  2.132&lt;br /&gt;
|-&lt;br /&gt;
|60_40_46   || 13.48     ||  1.500     ||  1.593    ||  0.9672    ||  0.9503    ||   1.712     ||  1.306    ||   6.170     ||  2.806&lt;br /&gt;
|-&lt;br /&gt;
|60_50_50   || 15.36     ||  1.627     ||  1.732    ||  0.9601    ||  0.9504    ||   1.721     ||  1.297    ||   6.467     ||  3.895&lt;br /&gt;
|-&lt;br /&gt;
|60_60_53   || 16.79     ||  1.734     ||  1.851    ||  0.9528    ||  0.9499    ||   1.729     ||  1.289    ||   6.731     ||  5.666&lt;br /&gt;
|-&lt;br /&gt;
|60_70_57   || 15.88     ||  1.829     ||  1.934    ||  0.9473    ||  0.9502    ||   1.737     ||  1.281    ||   5.736     ||  6.958&lt;br /&gt;
|-&lt;br /&gt;
|60_80_61   || 13.66     ||  1.918     ||  1.968    ||  0.9428    ||  0.9514    ||   1.745     ||  1.273    ||   2.622     ||  4.555&lt;br /&gt;
|-&lt;br /&gt;
|60_90_64   || 17.29     ||  2.009     ||  2.063    ||  0.9359    ||  0.9501    ||   1.753     ||  1.265    ||   2.640     ||  1.637&lt;br /&gt;
|-&lt;br /&gt;
|60_100_68  || 17.62     ||  2.049     ||  2.122    ||  0.9304    ||  0.9497    ||   1.760     ||  1.258    ||   3.560     ||  3.718&lt;br /&gt;
|-&lt;br /&gt;
|60_110_72  || 17.50     ||  2.118     ||  2.177    ||  0.9257    ||  0.9501    ||   1.767     ||  1.251    ||   2.811     ||  4.023&lt;br /&gt;
|-&lt;br /&gt;
|60_120_76  || 17.78     ||  2.174     ||  2.222    ||  0.9217    ||  0.9510    ||   1.774     ||  1.244    ||   2.209     ||  4.211&lt;br /&gt;
|-&lt;br /&gt;
|70_00_39   || 5.731     || 0.7825     || 0.7975    ||  0.9949    ||  0.9497    ||   1.675     ||  1.343    ||   1.908     || 0.2335&lt;br /&gt;
|-&lt;br /&gt;
|70_10_41   || 8.418     ||  1.009     ||  1.048    ||  0.9860    ||  0.9509    ||   1.688     ||  1.330    ||   3.845     || 0.6755&lt;br /&gt;
|-&lt;br /&gt;
|70_20_44   || 11.09     ||  1.201     ||  1.265    ||  0.9767    ||  0.9504    ||   1.699     ||  1.319    ||   5.345     ||  1.317&lt;br /&gt;
|-&lt;br /&gt;
|70_30_47   || 13.41     ||  1.361     ||  1.441    ||  0.9688    ||  0.9504    ||   1.709     ||  1.309    ||   5.859     ||  2.187&lt;br /&gt;
|-&lt;br /&gt;
|70_40_51   || 14.99     ||  1.496     ||  1.591    ||  0.9615    ||  0.9503    ||   1.718     ||  1.300    ||   6.348     ||  2.859&lt;br /&gt;
|-&lt;br /&gt;
|70_50_54   || 16.87     ||  1.617     ||  1.712    ||  0.9543    ||  0.9501    ||   1.727     ||  1.291    ||   5.843     ||  3.756&lt;br /&gt;
|-&lt;br /&gt;
|70_60_57   || 17.89     ||  1.718     ||  1.823    ||  0.9479    ||  0.9500    ||   1.735     ||  1.283    ||   6.140     ||  4.746&lt;br /&gt;
|-&lt;br /&gt;
|70_70_61   || 18.26     ||  1.812     ||  1.928    ||  0.9423    ||  0.9503    ||   1.743     ||  1.275    ||   6.353     ||  6.812&lt;br /&gt;
|-&lt;br /&gt;
|70_80_65   || 16.37     ||  1.896     ||  1.962    ||  0.9363    ||  0.9499    ||   1.751     ||  1.267    ||   3.469     ||  5.948&lt;br /&gt;
|-&lt;br /&gt;
|70_90_68   || 9.135     ||  1.980     ||  1.988    ||  0.9317    ||  0.9506    ||   1.758     ||  1.260    ||  0.3692     || 0.1186&lt;br /&gt;
|-&lt;br /&gt;
|70_100_72  || 18.64     ||  2.007     ||  2.094    ||  0.9267    ||  0.9506    ||   1.765     ||  1.253    ||   4.327     ||  3.356&lt;br /&gt;
|-&lt;br /&gt;
|70_110_76  || 18.23     ||  2.088     ||  2.147    ||  0.9219    ||  0.9507    ||   1.772     ||  1.246    ||   2.792     ||  3.707&lt;br /&gt;
|-&lt;br /&gt;
|70_120_80  || 17.89     ||  2.145     ||  2.184    ||  0.9171    ||  0.9506    ||   1.779     ||  1.239    ||   1.846     ||  4.043&lt;br /&gt;
|-&lt;br /&gt;
|80_00_42   ||7.247      ||0.8436      ||0.8697     || 0.9869     || 0.9497     ||  1.684      || 1.335     ||  3.094      ||0.2402&lt;br /&gt;
|-&lt;br /&gt;
|80_10_45   ||9.865      || 1.049      || 1.095     || 0.9794     || 0.9513     ||  1.695      || 1.323     ||  4.371      ||0.7359&lt;br /&gt;
|-&lt;br /&gt;
|80_20_48   ||12.28      || 1.226      || 1.290     || 0.9697     || 0.9500     ||  1.706      || 1.312     ||  5.206      || 1.327&lt;br /&gt;
|-&lt;br /&gt;
|80_30_51   ||14.38      || 1.370      || 1.454     || 0.9626     || 0.9503     ||  1.715      || 1.303     ||  6.088      || 2.102&lt;br /&gt;
|-&lt;br /&gt;
|80_40_54   ||16.47      || 1.500      || 1.594     || 0.9549     || 0.9497     ||  1.724      || 1.294     ||  6.263      || 2.799&lt;br /&gt;
|-&lt;br /&gt;
|80_50_58   ||17.63      || 1.612      || 1.706     || 0.9492     || 0.9503     ||  1.733      || 1.285     ||  5.842      || 3.329&lt;br /&gt;
|-&lt;br /&gt;
|80_60_61   ||18.84      || 1.712      || 1.814     || 0.9436     || 0.9507     ||  1.741      || 1.277     ||  5.984      || 3.990&lt;br /&gt;
|-&lt;br /&gt;
|80_70_65   ||19.27      || 1.799      || 1.898     || 0.9372     || 0.9501     ||  1.749      || 1.269     ||  5.555      || 4.728&lt;br /&gt;
|-&lt;br /&gt;
|80_80_69   ||17.96      || 1.880      || 1.935     || 0.9321     || 0.9503     ||  1.756      || 1.262     ||  2.921      || 3.774&lt;br /&gt;
|-&lt;br /&gt;
|80_90_73   ||13.42      || 1.957      || 1.982     || 0.9266     || 0.9500     ||  1.764      || 1.254     ||  1.312      ||0.6938&lt;br /&gt;
|-&lt;br /&gt;
|80_100_76  || 18.53     ||  2.008     ||  2.065    ||  0.9220    ||  0.9504    ||   1.770     ||  1.247    ||   2.839     ||  1.773&lt;br /&gt;
|-&lt;br /&gt;
|80_110_80  || 18.41     ||  2.059     ||  2.117    ||  0.9176    ||  0.9507    ||   1.777     ||  1.241    ||   2.847     ||  3.632&lt;br /&gt;
|-&lt;br /&gt;
|80_120_84  || 18.26     ||  2.117     ||  2.157    ||  0.9122    ||  0.9496    ||   1.784     ||  1.234    ||   1.872     ||  3.986&lt;br /&gt;
|-&lt;br /&gt;
|90_00_46   || 8.679     || 0.9022     || 0.9354    ||  0.9802    ||  0.9501    ||   1.691     ||  1.327    ||   3.678     || 0.3981&lt;br /&gt;
|-&lt;br /&gt;
|90_10_49   || 11.45     ||  1.090     ||  1.146    ||  0.9717    ||  0.9502    ||   1.702     ||  1.315    ||   5.148     || 0.8099&lt;br /&gt;
|-&lt;br /&gt;
|90_20_52   || 12.44     ||  1.247     ||  1.323    ||  0.9640    ||  0.9503    ||   1.712     ||  1.305    ||   6.100     ||  1.079&lt;br /&gt;
|-&lt;br /&gt;
|90_30_55   || 16.14     ||  1.383     ||  1.475    ||  0.9571    ||  0.9504    ||   1.722     ||  1.296    ||   6.607     ||  2.158&lt;br /&gt;
|-&lt;br /&gt;
|90_40_58   || 17.45     ||  1.506     ||  1.597    ||  0.9499    ||  0.9501    ||   1.731     ||  1.287    ||   6.012     ||  2.629&lt;br /&gt;
|-&lt;br /&gt;
|90_50_62   || 18.70     ||  1.609     ||  1.706    ||  0.9438    ||  0.9501    ||   1.739     ||  1.279    ||   6.003     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|90_60_65   || 18.77     ||  1.703     ||  1.789    ||  0.9381    ||  0.9502    ||   1.747     ||  1.271    ||   5.045     ||  3.047&lt;br /&gt;
|-&lt;br /&gt;
|90_70_69   || 18.43     ||  1.787     ||  1.852    ||  0.9324    ||  0.9500    ||   1.754     ||  1.263    ||   3.623     ||  3.117&lt;br /&gt;
|-&lt;br /&gt;
|90_80_73   || 17.72     ||  1.868     ||  1.909    ||  0.9269    ||  0.9497    ||   1.762     ||  1.256    ||   2.217     ||  2.354&lt;br /&gt;
|-&lt;br /&gt;
|90_90_76   || 14.40     ||  1.940     ||  1.956    ||  0.9221    ||  0.9499    ||   1.769     ||  1.249    ||  0.8079     || 0.8326&lt;br /&gt;
|-&lt;br /&gt;
|90_100_80  || 18.53     ||  2.009     ||  2.038    ||  0.9176    ||  0.9503    ||   1.776     ||  1.242    ||   1.484     ||  1.095&lt;br /&gt;
|-&lt;br /&gt;
|90_110_84  || 18.97     ||  2.021     ||  2.094    ||  0.9129    ||  0.9502    ||   1.783     ||  1.235    ||   3.625     ||  3.669&lt;br /&gt;
|-&lt;br /&gt;
|90_120_88  || 17.79     ||  2.090     ||  2.129    ||  0.9077    ||  0.9494    ||   1.789     ||  1.229    ||   1.827     ||  3.862&lt;br /&gt;
|-&lt;br /&gt;
|100_00_50  || 10.07     || 0.9544     || 0.9970    ||  0.9732    ||  0.9499    ||   1.699     ||  1.319    ||   4.471     || 0.4341&lt;br /&gt;
|-&lt;br /&gt;
|100_10_53  || 12.78     ||  1.127     ||  1.186    ||  0.9649    ||  0.9499    ||   1.710     ||  1.308    ||   5.262     || 0.9629&lt;br /&gt;
|-&lt;br /&gt;
|100_16_55  || 13.69     ||  1.215     ||  1.287    ||  0.9610    ||  0.9501    ||   1.715     ||  1.302    ||   5.901     ||  1.023&lt;br /&gt;
|-&lt;br /&gt;
|100_20_56  || 10.86     ||  1.271     ||  1.324    ||  0.9583    ||  0.9502    ||   1.719     ||  1.299    ||   4.120     || 0.8295&lt;br /&gt;
|-&lt;br /&gt;
|100_22_56  || 15.40     ||  1.309     ||  1.381    ||  0.9412    ||  0.9362    ||   1.722     ||  1.296    ||   5.552     ||  1.648&lt;br /&gt;
|-&lt;br /&gt;
|100_24_58  || 15.90     ||  1.326     ||  1.406    ||  0.9552    ||  0.9499    ||   1.722     ||  1.295    ||   6.105     ||  1.792&lt;br /&gt;
|-&lt;br /&gt;
|100_26_58  || 16.42     ||  1.352     ||  1.435    ||  0.9538    ||  0.9499    ||   1.724     ||  1.293    ||   6.137     ||  1.888&lt;br /&gt;
|-&lt;br /&gt;
|100_28_59  || 17.07     ||  1.375     ||  1.464    ||  0.9527    ||  0.9501    ||   1.726     ||  1.291    ||   6.475     ||  1.983&lt;br /&gt;
|-&lt;br /&gt;
|100_30_59  || 17.29     ||  1.398     ||  1.490    ||  0.9511    ||  0.9500    ||   1.728     ||  1.289    ||   6.561     ||  2.075&lt;br /&gt;
|-&lt;br /&gt;
|100_32_60  || 17.74     ||  1.423     ||  1.517    ||  0.9499    ||  0.9499    ||   1.730     ||  1.288    ||   6.596     ||  2.165&lt;br /&gt;
|-&lt;br /&gt;
|100_36_61  || 18.37     ||  1.467     ||  1.567    ||  0.9475    ||  0.9501    ||   1.733     ||  1.284    ||   6.819     ||  2.183&lt;br /&gt;
|-&lt;br /&gt;
|100_40_63  || 18.77     ||  1.509     ||  1.608    ||  0.9450    ||  0.9500    ||   1.736     ||  1.281    ||   6.553     ||  2.304&lt;br /&gt;
|-&lt;br /&gt;
|100_44_64  || 19.25     ||  1.551     ||  1.653    ||  0.9426    ||  0.9500    ||   1.740     ||  1.278    ||   6.569     ||  2.360&lt;br /&gt;
|-&lt;br /&gt;
|100_48_65  || 19.16     ||  1.591     ||  1.684    ||  0.9400    ||  0.9500    ||   1.743     ||  1.275    ||   5.807     ||  2.555&lt;br /&gt;
|-&lt;br /&gt;
|100_50_65  || 19.11     ||  1.613     ||  1.704    ||  0.9381    ||  0.9501    ||   1.745     ||  1.274    ||   5.628     ||  2.649&lt;br /&gt;
|-&lt;br /&gt;
|100_55_67  || 19.04     ||  1.659     ||  1.739    ||  0.9352    ||  0.9500    ||   1.749     ||  1.270    ||   4.839     ||  2.808&lt;br /&gt;
|-&lt;br /&gt;
|100_56_67  || 18.93     ||  1.667     ||  1.742    ||  0.9347    ||  0.9501    ||   1.750     ||  1.269    ||   4.522     ||  2.692&lt;br /&gt;
|-&lt;br /&gt;
|100_60_68  || 19.04     ||  1.702     ||  1.775    ||  0.9325    ||  0.9500    ||   1.753     ||  1.266    ||   4.326     ||  2.720&lt;br /&gt;
|-&lt;br /&gt;
|100_64_70  || 18.76     ||  1.733     ||  1.799    ||  0.9303    ||  0.9500    ||   1.756     ||  1.263    ||   3.774     ||  2.676&lt;br /&gt;
|-&lt;br /&gt;
|100_68_72  || 18.46     ||  1.771     ||  1.825    ||  0.9279    ||  0.9494    ||   1.759     ||  1.259    ||   3.080     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_70_73  || 18.23     ||  1.784     ||  1.841    ||  0.9277    ||  0.9500    ||   1.760     ||  1.258    ||   3.166     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_80_77  || 16.73     ||  1.855     ||  1.885    ||  0.9261    ||  0.9532    ||   1.767     ||  1.251    ||   1.617     ||  1.818&lt;br /&gt;
|-&lt;br /&gt;
|100_90_80  || 13.86     ||  1.931     ||  1.936    ||  0.9172    ||  0.9494    ||   1.774     ||  1.244    ||  0.2833     || 0.7382&lt;br /&gt;
|-&lt;br /&gt;
|100_95_82  || 11.27     ||  1.967     ||  1.964    ||  0.9243    ||  0.9582    ||   1.777     ||  1.241    || -0.1435     || 6.8954E-02&lt;br /&gt;
|-&lt;br /&gt;
|100_105_86 || 16.96     ||  2.019     ||  2.045    ||  0.9233    ||  0.9617    ||   1.783     ||  1.235    ||   1.268     ||  1.425&lt;br /&gt;
|-&lt;br /&gt;
|100_110_88 || 18.88     ||  2.020     ||  2.073    ||  0.9229    ||  0.9634    ||   1.786     ||  1.232    ||   2.618     ||  2.366&lt;br /&gt;
|-&lt;br /&gt;
|100_120_92 || 17.63     ||  2.064     ||  2.113    ||  0.9044    ||  0.9501    ||   1.794     ||  1.224    ||   2.379     ||  3.790&lt;br /&gt;
|-&lt;br /&gt;
|110_00_54  || 11.70     ||  1.006     ||  1.060    ||  0.9663    ||  0.9498    ||   1.706     ||  1.312    ||   5.370     || 0.4642&lt;br /&gt;
|-&lt;br /&gt;
|110_10_57  || 13.97     ||  1.160     ||  1.232    ||  0.9593    ||  0.9502    ||   1.716     ||  1.301    ||   6.136     || 0.8247&lt;br /&gt;
|-&lt;br /&gt;
|110_20_60  || 15.75     ||  1.298     ||  1.372    ||  0.9526    ||  0.9504    ||   1.726     ||  1.292    ||   5.739     ||  1.330&lt;br /&gt;
|-&lt;br /&gt;
|110_30_63  || 18.56     ||  1.415     ||  1.516    ||  0.9455    ||  0.9500    ||   1.734     ||  1.284    ||   7.122     ||  1.849&lt;br /&gt;
|-&lt;br /&gt;
|110_40_66  || 19.50     ||  1.521     ||  1.622    ||  0.9398    ||  0.9503    ||   1.743     ||  1.275    ||   6.602     ||  1.921&lt;br /&gt;
|-&lt;br /&gt;
|110_50_70  || 19.07     ||  1.618     ||  1.696    ||  0.9336    ||  0.9498    ||   1.751     ||  1.267    ||   4.873     ||  2.085&lt;br /&gt;
|-&lt;br /&gt;
|110_60_73  || 18.32     ||  1.702     ||  1.761    ||  0.9291    ||  0.9507    ||   1.758     ||  1.260    ||   3.471     ||  2.033&lt;br /&gt;
|-&lt;br /&gt;
|110_70_77  || 17.13     ||  1.782     ||  1.816    ||  0.9237    ||  0.9504    ||   1.766     ||  1.252    ||   1.948     ||  1.838&lt;br /&gt;
|-&lt;br /&gt;
|110_80_81  || 15.56     ||  1.853     ||  1.871    ||  0.9192    ||  0.9508    ||   1.773     ||  1.245    ||  0.9878     ||  1.332&lt;br /&gt;
|-&lt;br /&gt;
|110_90_84  || 13.12     ||  1.923     ||  1.926    ||  0.9142    ||  0.9506    ||   1.780     ||  1.238    ||  0.1639     || 0.5301&lt;br /&gt;
|-&lt;br /&gt;
|110_95_86  || 10.73     ||  1.963     ||  1.955    ||  0.9095    ||  0.9486    ||   1.783     ||  1.235    || -0.3746     || 8.1449E-04&lt;br /&gt;
|-&lt;br /&gt;
|110_110_92 || 17.29     ||  2.020     ||  2.055    ||  0.9056    ||  0.9509    ||   1.793     ||  1.225    ||   1.768     ||  2.045&lt;br /&gt;
|-&lt;br /&gt;
|110_120_95 || 17.55     ||  2.048     ||  2.095    ||  0.9014    ||  0.9510    ||   1.799     ||  1.219    ||   2.314     ||  3.774&lt;br /&gt;
|-&lt;br /&gt;
|120_00_57  || 13.14     ||  1.050     ||  1.117    ||  0.9599    ||  0.9497    ||   1.714     ||  1.305    ||   6.304     || 0.4861&lt;br /&gt;
|-&lt;br /&gt;
|120_10_60  || 14.81     ||  1.196     ||  1.268    ||  0.9534    ||  0.9501    ||   1.723     ||  1.295    ||   6.054     || 0.8382&lt;br /&gt;
|-&lt;br /&gt;
|120_20_63  || 17.57     ||  1.323     ||  1.409    ||  0.9458    ||  0.9494    ||   1.732     ||  1.286    ||   6.504     ||  1.409&lt;br /&gt;
|-&lt;br /&gt;
|120_30_67  || 19.50     ||  1.435     ||  1.539    ||  0.9407    ||  0.9503    ||   1.741     ||  1.277    ||   7.263     ||  1.529&lt;br /&gt;
|-&lt;br /&gt;
|120_40_70  || 19.38     ||  1.534     ||  1.621    ||  0.9335    ||  0.9492    ||   1.749     ||  1.269    ||   5.695     ||  1.632&lt;br /&gt;
|-&lt;br /&gt;
|120_50_74  || 18.34     ||  1.621     ||  1.684    ||  0.9294    ||  0.9503    ||   1.756     ||  1.262    ||   3.910     ||  1.864&lt;br /&gt;
|-&lt;br /&gt;
|120_60_77  || 17.24     ||  1.703     ||  1.743    ||  0.9246    ||  0.9507    ||   1.764     ||  1.254    ||   2.381     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|120_70_81  || 16.02     ||  1.780     ||  1.803    ||  0.9197    ||  0.9509    ||   1.771     ||  1.247    ||   1.312     ||  1.511&lt;br /&gt;
|-&lt;br /&gt;
|120_80_84  || 14.49     ||  1.850     ||  1.860    ||  0.9150    ||  0.9509    ||   1.778     ||  1.240    ||  0.5347     ||  1.076&lt;br /&gt;
|-&lt;br /&gt;
|120_90_88  || 12.18     ||  1.918     ||  1.918    ||  0.9096    ||  0.9501    ||   1.785     ||  1.233    || -4.1127E-02 || 0.3613&lt;br /&gt;
|-&lt;br /&gt;
|120_95_90  || 10.06     ||  1.957     ||  1.950    ||  0.9071    ||  0.9499    ||   1.788     ||  1.230    || -0.3241     ||  0.000&lt;br /&gt;
|-&lt;br /&gt;
|120_115_97 || 16.46     ||  2.020     ||  2.066    ||  0.8983    ||  0.9497    ||   1.801     ||  1.216    ||   2.258     ||  2.404&lt;br /&gt;
|-&lt;br /&gt;
|120_120_99 || 17.58     ||  2.008     ||  2.092    ||  0.8967    ||  0.9501    ||   1.804     ||  1.213    ||   4.186     ||  3.647&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Flexibility ==&lt;br /&gt;
&lt;br /&gt;
[[File:Flexibility TJ-II.png|300px|thumb|right|Flexibility diagram of TJ-II magnetic configurations. Several lines of constant rotational transform are highlighted and labelled with the corresponding edge &amp;lt;math&amp;gt;\iota/2\pi&amp;lt;/math&amp;gt;-value.]]&lt;br /&gt;
TJ-II has considerable configurational flexibility, as observed in the &#039;flexibility diagram&#039;&amp;lt;ref&amp;gt;E. Ascasíbar, T. Estrada, F. Castejón, A. López-Fraguas, I. Pastor, J. Sánchez, U. Stroth, J. Qin and TJ-II Team, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/45/4/009|Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276–284]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
The sum &amp;lt;math&amp;gt;I_{CC}+I_{HX}&amp;lt;/math&amp;gt; is an important factor determining the size of the plasma, and should not be too small. Thus, reasonably-sized plasmas are limited to the upper right triangle of this diagram.&lt;br /&gt;
Some of this flexibility space has been explored, as in the &#039;magnetic well scan&#039; experiments&amp;lt;ref&amp;gt;A. de Aguilera, F. Castejón, E. Ascasíbar, et al. &#039;&#039;Magnetic well scan and confinement in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/55/11/113014|Nucl. Fusion, 55(11):113014, 2015]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
More recently, the [[rotational transform]] in the plasma edge region was found to be of importance for [[H-mode|L-H]] confinement transitions&amp;lt;ref&amp;gt;B. P. van Milligen, T. Estrada, B. Carreras, L. García, and TJ-II Team. &#039;&#039;Importance of the rotational transform for L–H transitions in the TJ-II stellarator&#039;&#039;, [[doi:10.3390/plasma7020024|Plasma, 7(2):446–464, 2024]].&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=LNF:(2022-2026)_Estudio_de_transporte_y_turbulencia_en_plasmas_con_m%C3%A9todos_de_gran_resoluci%C3%B3n_espacial&amp;diff=8734</id>
		<title>LNF:(2022-2026) Estudio de transporte y turbulencia en plasmas con métodos de gran resolución espacial</title>
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		<updated>2026-10-13T08:34:01Z</updated>

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&lt;div&gt;== LNF - Nationally funded project ==&lt;br /&gt;
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&#039;&#039;&#039;Title&#039;&#039;&#039;: &#039;&#039;&#039;Estudio de transporte y turbulencia en plasmas con métodos de gran resolución espacial&#039;&#039;&#039;&lt;br /&gt;
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&#039;&#039;&#039;Reference&#039;&#039;&#039;: PID2021-124883NB-I00&lt;br /&gt;
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&#039;&#039;&#039;Programme and date&#039;&#039;&#039;: Proyectos de investigación no orientada (2021)&lt;br /&gt;
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&#039;&#039;&#039;Programme type (Modalidad de proyecto)&#039;&#039;&#039;: Proyectos de Generación de Conocimiento&lt;br /&gt;
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&#039;&#039;&#039;Area/subarea (Área temática / subárea)&#039;&#039;&#039;: Energía y transporte / Energía&lt;br /&gt;
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&#039;&#039;&#039;Principal Investigator(s)&#039;&#039;&#039;: [https://orcid.org/0000-0002-3850-0196 José Luis de Pablos Hernández] y [https://orcid.org/0000-0001-5344-6274 Boudewijn van Milligen]&lt;br /&gt;
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&#039;&#039;&#039;Project type&#039;&#039;&#039;: Proyecto individual&lt;br /&gt;
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&#039;&#039;&#039;Start-end dates&#039;&#039;&#039;: 01/09/2022 - 31/08/2026&lt;br /&gt;
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&#039;&#039;&#039;Financing granted (direct costs)&#039;&#039;&#039;: 150.000 €&lt;br /&gt;
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&#039;&#039;&#039;Acknowledgement&#039;&#039;&#039;: Grant PID2021-124883NB-I00 funded by MICIU/AEI/10.13039/501100011033 and by “ERDF/EU”. &lt;br /&gt;
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[[File:LogoOficial_PlanNacional_2021.png|500px]] &lt;br /&gt;
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== Description of the project ==&lt;br /&gt;
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The general goal of the present proposal is to investigate the interaction of turbulence, plasmas flows and the magnetic topology and determine the impact of the resulting complex interactions on plasma transport. This topic could be important for ITER and DEMO.&lt;br /&gt;
To reach this goal, we need to reach the following objectives:&lt;br /&gt;
# Development of novel low noise electronics in vacuum and test it to obtain a better SNR than the actual one with the help of Ciemat electronics team. This upgrade is essential to be able to measure phase relations between fluctuating fields and understand their mutual interaction.&lt;br /&gt;
# Study the impact of the magnetic configuration on turbulent properties. We expect to find that the location of major rational surfaces plays a significant role in radial transport.&lt;br /&gt;
# Study the impact of confinement transitions on turbulence, and flows on plasma turbulence. &lt;br /&gt;
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&amp;lt;!-- If applicable: references --&amp;gt;&lt;br /&gt;
&amp;lt;!-- == Project documentation ==&lt;br /&gt;
(Optional) Add the project proposal and the final report at the end of the project, and any other information related with the project --&amp;gt;&lt;br /&gt;
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== Main results ==&lt;br /&gt;
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El proyecto ha permitido avanzar significativamente en la comprensión de los mecanismos que regulan la turbulencia y la transición al régimen de alto confinamiento (L-H) en el stellarator TJ-II, un aspecto clave para el desarrollo de la energía de fusión. Aprovechando la flexibilidad del dispositivo para modificar con precisión la configuración magnética, se han realizado experimentos pioneros que han puesto de manifiesto la influencia de las superficies racionales y de la corriente neta del plasma sobre las propiedades turbulentas y el confinamiento.&lt;br /&gt;
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Entre los principales resultados destaca la identificación de la intermitencia como un nuevo parámetro para caracterizar la turbulencia, demostrando su sensibilidad tanto a la configuración magnética como a los flujos de plasma. Asimismo, mediante experimentos con variaciones dinámicas de la configuración magnética se ha establecido una relación directa entre la evolución temporal de la turbulencia y la presencia de superficies racionales de bajo orden.&lt;br /&gt;
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El proyecto también ha demostrado que la transición L-H y la mejora del confinamiento dependen de forma sistemática de la corriente neta del plasma y, por tanto, de la configuración magnética. El análisis combinado de experimentos y simulaciones de turbulencia MHD resistiva ha permitido proponer mecanismos físicos que explican esta dependencia, relacionados con la distribución de superficies racionales y la generación de flujos zonales capaces de suprimir la turbulencia.&lt;br /&gt;
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Estos resultados contribuyen a mejorar la comprensión de los procesos fundamentales que determinan el confinamiento del plasma y proporcionan nuevos criterios para optimizar el funcionamiento de futuros dispositivos de fusión, reforzando el liderazgo científico en el ámbito del confinamiento magnético.&lt;br /&gt;
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== Dissemination of project results (peer-reviewed publications and conference presentations) ==&lt;br /&gt;
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# C. Hidalgo, E. Ascasíbar, D. Alegre, A. Alonso, J. Alonso, R. Antón, A. Baciero, J. Baldzuhn, J. Barcala, L. Barrera, E. Blanco, J. Botija, L. Bueno, S. Cabrera, A. de Castro, E. de la Cal, I. Calvo, A. Cappa, D. Carralero, R. Carrasco, B. Carreras, R. Castro, A. de Castro, L. Cebrián, A. Chmyga, M. Chamorro, P. Colino, F. de Aragón, M. Drabinskiy, J. Duque, L. Eliseev, F. Escoto, T. Estrada, M. Ezzat, F. Fraguas, D. Fernández-Ruiz, J. Fontdecaba, A. Gabriel, D. Gadariya, L. García, I. García-Cortés, R. García- Gómez, J. García-Regaña, A. González-Jerez, G. Grenfell, J. Guasp, V. Guisse, J. Hernández-Sánchez, J. Hernanz, A. Jiménez-Denche, P. Khabanov, N. Kharchev, R. Kleiber, F. Koechl, T. Kobayashi, G. Kocsis, M. Koepke, A. Kozachek, L. Krupnik, F. Lapayese, M. Liniers, B. Liu, D. López-Bruna, B. López- Miranda, U. Losada, E. de la Luna, S. Lysenko, F. Martín-Díaz, G. Martín-Gómez, E. Maragkoudakis, J. Martínez-Fernández, K. McCarthy, F. Medina, M. Medrano, A. Melnikov, P. Méndez, F. Miguel, B. van Milligen, A. Molinero, G. Motojima, S. Mulas, Y. Narushima, M. Navarro, I. Nedzelskiy, R. Nuñez, M. Ochando, S. Ohshima, E. Oyarzábal, J. de Pablos, F. Palomares, N. Panadero, F. Papousek, F. Parra, C. Pastor, I. Pastor, A. de la Peña, R. Peralta, A. Pereira, P. Pons-Villalonga, H. Polaino, A. Portas, E. Poveda, F. Ramos, G. Rattá, M. Redondo, C. Reynoso, E. Rincón, C. Rodríguez-Fernández, L. Rodríguez-Rodrigo, A. Ros, E. Sánchez, J. Sánchez, E. Sánchez-Sarabia, S. Satake, J. Sebastián, R. Sharma, N. Smith, C. Silva, E. Solano, A. Soleto, M. Spolaore, T. Szepesi, F. Tabarés, D. Tafalla, H. Takahashi, N. Tamura, H. Thienpondt, A. Tolkachev, R. Unamuno, J. Varela, J. Vega, J. Velasco, I. Voldiner, S. Yamamoto, and the TJ-II Team. Overview of the TJ-II stellarator research programme towards model validation in fusion plasmas. [[doi:10.1088/1741-4326/ac2ca1|Nuclear Fusion, 62(4):042025, 2022]].	&lt;br /&gt;
# B. P. van Milligen, B. A. Carreras, L. García, G. Grenfell, I. Voldiner, and C. Hidalgo. The impact of radial electric fields and plasma rotation on intermittence in TJ-II. [[doi:10.1088/1361-6587/ac54e9|Plasma Phys. Control. Fusion, 64(5):055006, 2022]].	&lt;br /&gt;
# Melnikov, V, A., Eliseev, L. G., Barcala, J. M., Cappa, A., Chmyga, A. A., Drabinskiy, M. A., Hidalgo, C., Khabanov, P. O., Kharchev, N. K., Kozachek, A. S., Liniers, M., Lopez-Bruna, D., Losada, U., Lysenko, S. E., Medina, F., Molinero, A., Ochando, M., De Pablos, J. L., Pastor, I and TJ-II Team, 2D distributions of potential and density mean-values and oscillations in the ECRH and NBI plasmas at the TJ-II stellarator, [[doi:10.1088/1361-6587/ac5b4c|Plasma Phys. Control. Fusion 64:054009, 2022]].	&lt;br /&gt;
# B. van Milligen, I. Voldiner, B. Carreras, L. García, M. Ochando, and the TJ-II Team. Rational surfaces, flows and radial structure in the TJ-II stellarator. [[doi:10.1088/1741-4326/aca688|Nucl. Fusion, 63:016027, 2023]].		&lt;br /&gt;
# I. García-Cortés, K. J. McCarthy, T. Estrada, V. Tribaldos, D. Medina-Roque, B. van Milligen, E. Ascasíbar, R. Carrasco, A. A. Chmyga, R. García, J. Hernández-Sánchez, C. Hidalgo, A. S. Kozachek, F. Medina, M. A. Ochando, J. L. de Pablos, N. Panadero, and I. Pastor. Enhanced confinement induced by pellet injection in the stellarator TJ-II. [[doi:10.1063/5.0151395|Phys. Plasmas, 30(7):072506, 2023]].	&lt;br /&gt;
# L. García, I. García-Cortés, B. Carreras, K. McCarthy, and B. van Milligen. The effect of pellet injection on turbulent transport in TJ-II. [[doi:10.1063/5.0163832|Phys. Plasmas, 30:092303, 2023]].	&lt;br /&gt;
# Krupnik, L. I. and Barcala, J. M. and Cappa, A. and Chmyga, O. O. and Dreval, M. B. and Hidalgo, C. and Khrebtov, S. M. and Komarov, O. D. and Kozachok, O. S. and Martinez, J. and Molinero, A. and de Pablos, J. L. and TJ-II Team, Plasma profiles, self -organization and Alfven eigenmodes studies using the HIBP diagnostic in the TJ-II stellarator, [[doi:10.46813/2023-143-122|Problems of atomic science and technology, 1:122-125, 2023]].	&lt;br /&gt;
# K.J. McCarthy, I. García-Cortés, J.A. Alonso, A. Arias-Camisón, E. Ascasíbar, A. Baciero, A. Cappa, R. Carrasco, O.O. Chmyga, T. Estrada, R. García, J. Hernández-Sánchez, F.J. Hernanz, O.S. Kozachok, B. López Miranda, F. Medina, D. Medina-Roque, B. van Milligen, M. Navarro, M.A. Ochando, J.L. de Pablos, N. Panadero, I. Pastor, J. de la Riva, M. C. Rodríguez, D. Tafalla, V. Tribaldos, and TJ-II Team. [[doi:10.1088/1741-4326/ad4047 |Multi-pellet injection into the NBI-heated phase of TJ-II plasmas. Nuclear Fusion, 64(6):066019, 2024]].	&lt;br /&gt;
# B.Ph. van Milligen, T. Estrada, B.A. Carreras, L. García, and the TJ-II Team. Importance of the rotational transform for L–H transitions in the TJ-II stellarator. [[doi:10.3390/plasma7020024|Plasma, 7(2):446–464, 2024]].	&lt;br /&gt;
# J.A. Alonso, D. Alegre, J. Alonso, R. Antón, A. Arias-Camisón, E. Ascasíbar, A. Baciero, J.M. Barcala, M. Barnes, E. Blanco, L. Bueno, A. Bustos, S. Cabrera, E. de la Cal, I. Calvo, A. Cappa, D. Carralero, R. Carrasco, B. Carreras, R. Castro, A. de Castro, L. Cebrián, M. Chamorro, A.A. Chmyga, P. Colino, J. Duque, F.J. Escoto, T. Estrada, A. Fernández, J. Fraguas, J.M. Fontdecaba, A. Gabriel, L. García, I. García-Cortés, R. García-Gómez, J.M. García-Regaña, G. Godino-Sedano, J. Gómez-Manchón, A. González, A. González-Jerez, V. Guisse, J. Hernández-Sánchez, J. Hernanz, C. Hidalgo, P. Ivanova, A. Jiménez-Denche, D. Jiménez-Rey, G. Kocsis, M. Koepke, A.S. Kozachek, F. Lapayese, M. Liniers, D. López, D. López-Bruna, B. López-Miranda, E. de la Luna, E. Maragkoudakis, F. Martín-Díaz, G. Martín-Gómez, J. Martínez-Fernández, K.J. McCarthy, F. Medina, D. Medina-Roque, M. Medrano, P. Méndez, F.J. Miguel, B. van Milligen, A. Molinero, G. Motojima, S. Mulas, M. Navarro, I. Nedzelskiy, R. Nuñez, M. Ochando, E. Oyarzábal, J.L. de Pablos, F. Palomares, N. Panadero, F.I. Parra, C. Pastor, I. Pastor, A. de la Peña, R. Peralta, A. Pereira, P. Pons-Villalonga, A.B. Portas, E. Poveda, F.J. Ramos, G.A. Rattá, M. Redondo, C. Reynoso, E. Rincón, J. de la Riva, C. Rodríguez-Fernández, A. Ros, E. Sánchez, J. Sánchez, E. Sánchez-Sarabia, J.A. Sebastián, E.R. Solano, A. Soleto, T. Szepesi, F.L. Tabarés, D. Tafalla, H. Takahashi, N. Tamura, H. Thienpondt, A. Tolkachev, V. Tribaldos, R. Unamuno, J. Varela, J. Vega, J.L. Velasco, and I. Voldiner. Density profiles in stellarators: an overview of particle transport, fuelling and profile shaping studies at TJ-II. [[doi:10.1088/1741-4326/ad67ef|Nuclear Fusion, 64(11):112018, 2024]].&lt;br /&gt;
# H. Bsharat, Igor Voldiner, B. Ph. van Milligen, and C. Xiao. Conditional cross-correlation analysis of floating potential fluctuations in the TJ-II stellarator. [[doi:10.1080/10420150.2024.2434503|Radiation Effects and Defects in Solids, 179(11-12):1527, 2024]].	&lt;br /&gt;
#  B.Ph. van Milligen, I. García-Cortés, K.J. McCarthy, B.A. Carreras, L. García, A. Cappa, P. Pons-Villalonga, T. Estrada, D. Medina-Roque, J. Hernández Sánchez, R. García, O.S. Kozachok, O.O. Chmyga, J.L. de Pablos, J.M. Barcala, A. Molinero, I. Pastor, D. Tafalla, A. de la Peña, F. Lapayese, and the TJ-II Team. The rotational transform and enhanced confinement in the TJ-II stellarator. [[doi:10.1017/S0022377825100433|J. Plasma Phys., 91(4):E98, 2025]].	&lt;br /&gt;
# G. Grenfell, M. Griener, M. Bernert, J. Adamek, D. Brida, M. Faitsch, P. Manz, B.Ph. van Milligen, U. Stroth, the ASDEX Upgrade Team, and the EUROfusion Tokamak Exploitation Team. On the evolution of profiles and fluctuations towards the L-mode density limit in ASDEX Upgrade. [[doi:10.1088/1741-4326/adeda1|Nuclear Fusion, 65(8):086023, 2025]].	&lt;br /&gt;
# J. Ortiz, J. Varela, L. Herrera Quesada, P. Pons-Villalonga, A. Cappa, U. Losada, F. Papousek, B. Ph. van Milligen, L. Garcia, D. A. Spong, Y. Ghai, M. A. Ochando, and C. Hidalgo. Analysis of the HAE activity in the TJ-II stellarator using a Landau closure model. [[doi:10.1063/5.0263300|Phys. Plasmas, 32:072506, 2025]].	&lt;br /&gt;
# Paulo Aguayo, Gonzalo Farias, Alejandro González-Ganzábal, Ernesto Fabregas, Teresa Estrada, Boudewijn van Milligen, Alfonso Baciero, Belén López-Miranda, Francisco Medina, and Giuseppe A. Rattá Gutiérrez. A data-driven approach to estimate plasma density in TJ-II stellarator. [[doi:10.1016/j.fusengdes.2025.115596|Fusion Engineering and Design, 224:115596, 2026]].	&lt;br /&gt;
# A. González Ganzábal, G.A. Rattá, T. Estrada, J. Martínez-Fernández, N. Panadero, A. Cappa,B. López-Miranda, A. Baciero, F. Martín, D. Tafalla, B.P. Van Milligen, F. Medina, A. de la Peña, and S. Dormido-Canto. A comprehensive database of TJ-II signals and diagnostics for statistically based models. [[doi:10.1016/j.fusengdes.2025.115613|Fusion Engineering and Design, 224:115613, 2026]].	&lt;br /&gt;
# I Voldiner, E de la Cal, B van Milligen, and TJ-II Team. Spectroscopic gas puff imaging diagnostic for the measurement of two-dimensional electron density and temperature distributions. [[doi:10.1088/1361-6587/ae5686|Plasma Physics and Controlled Fusion, 68(4):045017, 2026]].	&lt;br /&gt;
# Arnold Alonso Alvarez, Boudewijn Ph Van Milligen, Igor Voldiner, Ibere Luiz Caldas, Zwinglio Guimarães Filho, Oleksandr Kozachok, and Alexander Chmyga. Edge turbulence dynamics across electron–ion root transitions during ECRH modulation experiments in the TJ-II stellarator. [[doi:10.1088/1361-6587/ae7470|Plasma Physics and Controlled Fusion, 68(6):065019, 2026]].	&lt;br /&gt;
# Andres Cureño-Ramirez, Luis Gerardo de la Fraga, Giuseppe A. Rattá, Alejandro González-Ganzábal, Alfonso Baciero, Belén López-Miranda, Boudewijn van Milligen, Alfonso Pardo, and Jesús Calle-Cancho. Data-driven estimation of experimental signals in TJ-II: A proof of principle. [[doi:10.1016/j.fusengdes.2026.115847|Fusion Engineering and Design, 230:115847, 2026]].	&lt;br /&gt;
# B.Ph. van Milligen, I. Voldiner, E. de la Cal, A. Alonso Alvarez, I. Luiz Caldas and Z. Guimarães Filho, Turbulence analysis with the spectroscopic gas puff imaging diagnostic in the TJ-II stellarator, [[doi:10.1088/1361-6587/ae92b5|Plasma Phys. Control. Fusion (2026)]] &lt;br /&gt;
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=== Conferences ===&lt;br /&gt;
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# Oral: K. J. McCarthy, I. García-Cortés, V. Tribaldos, D. Medina-Roque, N. Panadero, E. Ascasíbar, A. A. Chmyga, T. Estrada, J. Hernández-Sánchez, A. S. Kozachek, M. Liniers, P. Medina, M. A. Ochando, J. L. de Pablos, I. Pastor, C. Toledo, B. van Milligen, and TJ-II Team. Enhanced confinement after multi-pellet injection into neutral beam injection heated plasmas in the stellarator TJ-II. In Proc. 48th EPS Conference on Plasma Physics, volume 46A of ECA, page O2.103. European Physical Society, 2022.&lt;br /&gt;
# Poster: I. Voldiner, E. de la Cal, B. van Milligen, C. Hidalgo, and TJ-II Team. Novel high speed spectrally resolved imaging system for simultaneous 2-D Te and ne edge plasma measurements with temporal resolution up to 100 kHz. In Proc. 48th EPS Conference on Plasma Physics, volume 46A of ECA, page P2b.106. European Physical Society, 2022.&lt;br /&gt;
# Poster: D. Medina-Roque, I. García-Cortés, K. J. McCarthy, N. Tamura, N. Panadero, E.Ascasíbar, T. Estrada, J. Hernández-Sánchez, A. S. Kozachek, M. Liniers, P. Medina, M. Ochando, J. L. de Pablos, I. Pastor, C. Toledo, B. van Milligen, and TJ-II Team. New insights into cryogenic and TESPEL pellet physics in TJ-II. In Proc. 48th EPS Conference on Plasma Physics, volume 46A of ECA, page P2b.113. European Physical Society, 2022.&lt;br /&gt;
# Oral:  I. Voldiner, E. de la Cal, B. van Milligen and TJ-II Team, Two-dimensional ne and Te measurements of the edge plasma turbulence in TJ-II. In Proc. 49th EPS Conference on Plasma Physics, European Physical Society, In Proc. 49th EPS Conference on Plasma Physics, volume 47A of ECA, page O2.102, 2023.&lt;br /&gt;
# Poster:  I. García-Cortés, K. J. McCarthy, V. Tribaldos, D. Medina-Roque, N. Panadero, E. Ascasíbar, T.Estrada, J. Hernández-Sánchez, A. S. Kozachek, R. Carrasco, B. López-Miranda, P. Medina, M.A. Ochando, J. L. de Pablos, I. Pastor, B. van Milligen &amp;amp; TJ-II team.  Enhanced confinement induced by multi-pellet injection into neutral beam injection heated plasmas in the stellarator TJ-II.  In Proc. 49th EPS Conference on Plasma Physics, European Physical Society,  In Proc. 49th EPS Conference on Plasma Physics, volume 47A of ECA, page P4.008, 2023&lt;br /&gt;
# Poster: L. García, I. García-Cortés, B. Carreras, K. McCarthy, and B. van Milligen. Consequences of pellet injection on the turbulent transport in TJ-II. In Proc. 49th EPS Conference on Plasma Physics, volume 47A of ECA, page P4.079. European Physical Society, 2023.&lt;br /&gt;
# Oral: J. A. Alonso and D. Alegre and J. Alonso and R. Antón and A. Arias-Camisón and E. Ascasíbar and A. Baciero and J.M. Barcala and M. Barnes and E. Blanco and L. Bueno and A. Bustos and S. Cabrera and A. de Castro and E. de la Cal and I. Calvo and A. Cappa and D. Carralero and R. Carrasco and B. Carreras and R. Castro and A. de Castro and L. Cebrián and A.A. Chmyga and M. Chamorro and P. Colino and J. Duque and F.J. Escoto and T. Estrada and A. Fernández and J. Fraguas and J.M. Fontdecaba and A. Gabriel and L. García and I. García-Cortés and R. García-Gómez and J.M. García-Regaña and G. Godino-Sedano and J. Gómez-Manchón and A. González-Jerez and V. Guisse and J. Hernández-Sánchez and J. Hernanz and C. Hidalgo and P. Ivanova and A. Jiménez-Denche and D. Jiménez-Rey and G. Kocsis and M. Koepke and A.S. Kozachek and F. Lapayese and M. Liniers and D. López and D. López-Bruna and B. López-Miranda and E. de la Luna and E. Maragkoudakis and F. Martín-Díaz and G. Martín-Gómez and J. Martínez-Fernández and K.J. McCarthy and F. Medina and D. Medina-Roque and M. Medrano and P. Méndez and F.J. Miguel and B. van Milligen and A. Molinero and G. Motojima and S. Mulas and M. Navarro and I. Nedzelskiy and R. Nuñez and M. Ochando and E. Oyarzábal and J.L. de Pablos and F. Palomares and N. Panadero and F.I. Parra and C. Pastor and I. Pastor and A. de la Peña and R. Peralta and A. Pereira and P. Pons-Villalonga and A.B. Portas and E. Poveda and F.J. Ramos and G.A. Rattá and M. Redondo and C. Reynoso and E. Rincón and J. de la Riva and C. Rodríguez-Fernández and A. Ros and E. Sánchez and J. Sánchez and E. Sánchez-Sarabia and J.A. Sebastián and E.R. Solano and A. Soleto and T. Szepesi and F.L. Tabarés and D. Tafalla and H. Takahashi and N. Tamura and H. Thienpondt and A. Tolkachev and V. Tribaldos and R. Unamuno and J. Varela and J. Vega and J.L. Velasco and I. Voldiner. Density profiles in stellarators: an overview of particle transport, fueling and profile shaping studies at TJ-II. 29th IAEA Fusion Energy Conference, IAEA-CN-316/2223, 2023&lt;br /&gt;
# Poster: K. J. McCarthy, I. García-Cortés, T. Estrada, D. Medina-Roque, B. Van Milligen, N. Pandero, E. Ascasíbar, R. Carrasco, R. García, J. Hernández-Sánchez, B. López Miranda, TJ-II Team, V. Tribaldos, A. A. Chmyga, S. Kozachek. Enhanced plasma performance after pellet injection in the stellarator TJ-II. 29th IAEA Fusion Energy Conference, IAEA-CN-316/1875, 2023&lt;br /&gt;
# Poster: J.L de Pablos, B. van Milligen, J.M. Barcala, A. Molinero, I. García-Cortés, O. Chmyga, O.S. Kozachok, G. Martín, R. García, R. Sánchez, J.M. Reynolds-Barredo, C. Hidalgo, and the TJ-II Team. Turbulence control through feedback of zonal flows. In 50th EPS Conference on Plasma Physics, volume 48A of ECA, page P2.070. EPS, European Physical Society, 2024.&lt;br /&gt;
# Poster: L. García, B.A. Carreras, B.Ph. van Milligen, I. García-Cortés, K.J. McCarthy, and the TJ-II Team. Impact of low order rationals in the enhanced confinement by pellet injection in TJ-II. In 50th EPS Conference on Plasma Physics, volume 48A of ECA, page P4.074. EPS, European Physical Society, 2024.&lt;br /&gt;
# Poster: I. García-Cortés, K.J. McCarthy, B. van Milligen, T. Estrada, D. Medina-Roque, A. Baciero, B.A. Carreras, A. Cappa, A.A. Chmyga, F. Medina, L. Garcia, R. García, J. Hernández-Sánchez, F.J. Hernanz, A.S. Kozachek, F. Lapayese, B. Lopez-Miranda, D. Lopez-Bruna, J.L. De Pablos, N. Panadero, I. Pastor, A. de la Peña, P. Pons-Villalonga, M.C. Rodriguez, D. Tafalla, V. Tribaldos, and TJ-II Team. Exploring enhanced plasma performance after pellet injections via rotational transform modulation in the TJ-II stellarator. In Proc. 29th IAEA Fusion Energy Conference, volume IAEA-CN-316/2795, pages P1–2803. IAEA, 2025.&lt;br /&gt;
# Poster: K. J. McCarthy, I. García-Cortés, B. van Milligen, A. Baciero, R. Carrasco, T. Estrada, R. García, J. Hernández Sánchez, B. López Miranda, F. Medina, D. Medina-Roque, M. Navarro, N. Panadero, I. Pastor, M. C. Rodríguez, and TJ-II Team. Interpreting structures observed in pellet ablation profiles in the stellarator TJ-II. In Proc. 29th IAEA Fusion Energy Conference, pages IAEA–CN–316/2795. IAEA, 2025.&lt;br /&gt;
# Poster: V. Tribaldos, I. García-Cortés, K.J. Mccarthy, J.M. Reynolds-Barredo, D. Medina-Roque, A. Baciero, O.O. Chmyga, T. Estrada, O.S. Kozachok, D. López-Bruna, F. Medina, B. van Milligen, J.L. de Pablos, N. Panadero, I. Pastor, J. de la Riva, and TJ-II Team. Confinement modelling of enhanced plasma performance after multiple pellet injections in the TJ-II stellarator. In Proc. 29th IAEA Fusion Energy Conference, pages IAEA–CN–316–2804. IAEA, 2025.&lt;br /&gt;
# Poster: A. González Ganzábal, G.A. Rattá, T. Estrada, J. Martínez-Fernández, N. Panadero, A. Cappa, B. López-Miranda, A. Baciero, F. Martín, D. Tafalla, B.P. Van Milligen, F. Medina, A. de la Peña, S. Dormido-Canto, and the TJ-II team. Development of a standardised TJ-II database for machine learning models and applications. In International Stellarator and Heliotron Workshop, 2026.&lt;br /&gt;
# Poster: B.Ph. van Milligen, I. García-Cortés, K.J. McCarthy, B.A. Carreras, L. García, O.S. Kozachok, O.O. Chmyga, J.L. de Pablos, and the TJ-II Team. Impact of the rotational transform and pellets on enhanced confinement and turbulence in the TJ-II stellarator. In 52nd EPS Conference on Plasma Physics, ECA, P2.1095. EPS, European Physical Society, 2026.&lt;br /&gt;
# Poster: B.Ph. van Milligen, I. Voldiner, E. de la Cal, Arnold A. Alvarez, I.L. Caldas, Z.O. Guimarães-Filho, and the TJ-II Team. Turbulence analysis with the spectral gas puff imaging diagnostic in the TJ-II stellarator. In 52nd EPS Conference on Plasma Physics, ECA, P2.1117. EPS, European Physical Society, 2026.&lt;br /&gt;
# Poster: Arnold A. Alvarez, Boudewijn Ph. van Milligen, Igor Voldiner, Iberê L. Caldas, Zwinglio O. Guimarães-Filho, O.S. Kozachok, O.O. Chmyga, and the TJ-II Team. Turbulence and transport across electron-ion root transitions during ECRH modulation in the TJ-II stellarator. In 52nd EPS Conference on Plasma Physics, ECA, P2.1001. EPS, European Physical Society, 2026. &lt;br /&gt;
# Poster: V. Tribaldos, I. García-Cortés, K.J. Mc-Carthy, J.M. Reynolds-Barredo, B. Van Milligen, A. Baciero, J. De La Riva, J.L. De Pablos, O.S. Kozachek, I. Pastor, and the TJ-II Team. Validation of neoclassical Er predictions in multi-pellet induced enhanced confinement regimes in TJ-II. In 52nd EPS Conference on Plasma Physics, ECA, P3.1167. EPS, European Physical Society, 2026.&lt;br /&gt;
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		<title>LNF:(2022-2026) Estudio de transporte y turbulencia en plasmas con métodos de gran resolución espacial</title>
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		<updated>2026-10-13T08:32:30Z</updated>

		<summary type="html">&lt;p&gt;Admin: &lt;/p&gt;
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&lt;div&gt;== LNF - Nationally funded project ==&lt;br /&gt;
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&#039;&#039;&#039;Title&#039;&#039;&#039;: &#039;&#039;&#039;Estudio de transporte y turbulencia en plasmas con métodos de gran resolución espacial&#039;&#039;&#039;&lt;br /&gt;
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&#039;&#039;&#039;Reference&#039;&#039;&#039;: PID2021-124883NB-I00&lt;br /&gt;
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&#039;&#039;&#039;Programme and date&#039;&#039;&#039;: Proyectos de investigación no orientada (2021)&lt;br /&gt;
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&#039;&#039;&#039;Programme type (Modalidad de proyecto)&#039;&#039;&#039;: Proyectos de Generación de Conocimiento&lt;br /&gt;
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&#039;&#039;&#039;Area/subarea (Área temática / subárea)&#039;&#039;&#039;: Energía y transporte / Energía&lt;br /&gt;
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&#039;&#039;&#039;Principal Investigator(s)&#039;&#039;&#039;: [https://orcid.org/0000-0002-3850-0196 José Luis de Pablos Hernández] y [https://orcid.org/0000-0001-5344-6274 Boudewijn van Milligen]&lt;br /&gt;
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&#039;&#039;&#039;Project type&#039;&#039;&#039;: Proyecto individual&lt;br /&gt;
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&#039;&#039;&#039;Start-end dates&#039;&#039;&#039;: 01/09/2022 - 31/08/2026&lt;br /&gt;
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&#039;&#039;&#039;Financing granted (direct costs)&#039;&#039;&#039;: 150.000 €&lt;br /&gt;
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&#039;&#039;&#039;Acknowledgement&#039;&#039;&#039;: Grant PID2021-124883NB-I00 funded by MICIU/AEI/10.13039/501100011033 and by “ERDF/EU”. &lt;br /&gt;
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[[File:LogoOficial_PlanNacional_2021.png|500px]] &lt;br /&gt;
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== Description of the project ==&lt;br /&gt;
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The general goal of the present proposal is to investigate the interaction of turbulence, plasmas flows and the magnetic topology and determine the impact of the resulting complex interactions on plasma transport. This topic could be important for ITER and DEMO.&lt;br /&gt;
To reach this goal, we need to reach the following objectives:&lt;br /&gt;
# Development of novel low noise electronics in vacuum and test it to obtain a better SNR than the actual one with the help of Ciemat electronics team. This upgrade is essential to be able to measure phase relations between fluctuating fields and understand their mutual interaction.&lt;br /&gt;
# Study the impact of the magnetic configuration on turbulent properties. We expect to find that the location of major rational surfaces plays a significant role in radial transport.&lt;br /&gt;
# Study the impact of confinement transitions on turbulence, and flows on plasma turbulence. &lt;br /&gt;
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&amp;lt;!-- == Project documentation ==&lt;br /&gt;
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== Main results ==&lt;br /&gt;
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El proyecto ha permitido avanzar significativamente en la comprensión de los mecanismos que regulan la turbulencia y la transición al régimen de alto confinamiento (L-H) en el stellarator TJ-II, un aspecto clave para el desarrollo de la energía de fusión. Aprovechando la flexibilidad del dispositivo para modificar con precisión la configuración magnética, se han realizado experimentos pioneros que han puesto de manifiesto la influencia de las superficies racionales y de la corriente neta del plasma sobre las propiedades turbulentas y el confinamiento.&lt;br /&gt;
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Entre los principales resultados destaca la identificación de la intermitencia como un nuevo parámetro para caracterizar la turbulencia, demostrando su sensibilidad tanto a la configuración magnética como a los flujos de plasma. Asimismo, mediante experimentos con variaciones dinámicas de la configuración magnética se ha establecido una relación directa entre la evolución temporal de la turbulencia y la presencia de superficies racionales de bajo orden.&lt;br /&gt;
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El proyecto también ha demostrado que la transición L-H y la mejora del confinamiento dependen de forma sistemática de la corriente neta del plasma y, por tanto, de la configuración magnética. El análisis combinado de experimentos y simulaciones de turbulencia MHD resistiva ha permitido proponer mecanismos físicos que explican esta dependencia, relacionados con la distribución de superficies racionales y la generación de flujos zonales capaces de suprimir la turbulencia.&lt;br /&gt;
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Estos resultados contribuyen a mejorar la comprensión de los procesos fundamentales que determinan el confinamiento del plasma y proporcionan nuevos criterios para optimizar el funcionamiento de futuros dispositivos de fusión, reforzando el liderazgo científico en el ámbito del confinamiento magnético.&lt;br /&gt;
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== Dissemination of project results (peer-reviewed publications and conference presentations) ==&lt;br /&gt;
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# C. Hidalgo, E. Ascasíbar, D. Alegre, A. Alonso, J. Alonso, R. Antón, A. Baciero, J. Baldzuhn, J. Barcala, L. Barrera, E. Blanco, J. Botija, L. Bueno, S. Cabrera, A. de Castro, E. de la Cal, I. Calvo, A. Cappa, D. Carralero, R. Carrasco, B. Carreras, R. Castro, A. de Castro, L. Cebrián, A. Chmyga, M. Chamorro, P. Colino, F. de Aragón, M. Drabinskiy, J. Duque, L. Eliseev, F. Escoto, T. Estrada, M. Ezzat, F. Fraguas, D. Fernández-Ruiz, J. Fontdecaba, A. Gabriel, D. Gadariya, L. García, I. García-Cortés, R. García- Gómez, J. García-Regaña, A. González-Jerez, G. Grenfell, J. Guasp, V. Guisse, J. Hernández-Sánchez, J. Hernanz, A. Jiménez-Denche, P. Khabanov, N. Kharchev, R. Kleiber, F. Koechl, T. Kobayashi, G. Kocsis, M. Koepke, A. Kozachek, L. Krupnik, F. Lapayese, M. Liniers, B. Liu, D. López-Bruna, B. López- Miranda, U. Losada, E. de la Luna, S. Lysenko, F. Martín-Díaz, G. Martín-Gómez, E. Maragkoudakis, J. Martínez-Fernández, K. McCarthy, F. Medina, M. Medrano, A. Melnikov, P. Méndez, F. Miguel, B. van Milligen, A. Molinero, G. Motojima, S. Mulas, Y. Narushima, M. Navarro, I. Nedzelskiy, R. Nuñez, M. Ochando, S. Ohshima, E. Oyarzábal, J. de Pablos, F. Palomares, N. Panadero, F. Papousek, F. Parra, C. Pastor, I. Pastor, A. de la Peña, R. Peralta, A. Pereira, P. Pons-Villalonga, H. Polaino, A. Portas, E. Poveda, F. Ramos, G. Rattá, M. Redondo, C. Reynoso, E. Rincón, C. Rodríguez-Fernández, L. Rodríguez-Rodrigo, A. Ros, E. Sánchez, J. Sánchez, E. Sánchez-Sarabia, S. Satake, J. Sebastián, R. Sharma, N. Smith, C. Silva, E. Solano, A. Soleto, M. Spolaore, T. Szepesi, F. Tabarés, D. Tafalla, H. Takahashi, N. Tamura, H. Thienpondt, A. Tolkachev, R. Unamuno, J. Varela, J. Vega, J. Velasco, I. Voldiner, S. Yamamoto, and the TJ-II Team. Overview of the TJ-II stellarator research programme towards model validation in fusion plasmas. [[doi:10.1088/1741-4326/ac2ca1|Nuclear Fusion, 62(4):042025, 2022]].	&lt;br /&gt;
# B. P. van Milligen, B. A. Carreras, L. García, G. Grenfell, I. Voldiner, and C. Hidalgo. The impact of radial electric fields and plasma rotation on intermittence in TJ-II. [[doi:10.1088/1361-6587/ac54e9|Plasma Phys. Control. Fusion, 64(5):055006, 2022]].	&lt;br /&gt;
# Melnikov, V, A., Eliseev, L. G., Barcala, J. M., Cappa, A., Chmyga, A. A., Drabinskiy, M. A., Hidalgo, C., Khabanov, P. O., Kharchev, N. K., Kozachek, A. S., Liniers, M., Lopez-Bruna, D., Losada, U., Lysenko, S. E., Medina, F., Molinero, A., Ochando, M., De Pablos, J. L., Pastor, I and TJ-II Team, 2D distributions of potential and density mean-values and oscillations in the ECRH and NBI plasmas at the TJ-II stellarator, [[doi:10.1088/1361-6587/ac5b4c|Plasma Phys. Control. Fusion 64:054009, 2022]].	&lt;br /&gt;
# B. van Milligen, I. Voldiner, B. Carreras, L. García, M. Ochando, and the TJ-II Team. Rational surfaces, flows and radial structure in the TJ-II stellarator. [[doi:10.1088/1741-4326/aca688|Nucl. Fusion, 63:016027, 2023]].		&lt;br /&gt;
# I. García-Cortés, K. J. McCarthy, T. Estrada, V. Tribaldos, D. Medina-Roque, B. van Milligen, E. Ascasíbar, R. Carrasco, A. A. Chmyga, R. García, J. Hernández-Sánchez, C. Hidalgo, A. S. Kozachek, F. Medina, M. A. Ochando, J. L. de Pablos, N. Panadero, and I. Pastor. Enhanced confinement induced by pellet injection in the stellarator TJ-II. [[doi:10.1063/5.0151395|Phys. Plasmas, 30(7):072506, 2023]].	&lt;br /&gt;
# L. García, I. García-Cortés, B. Carreras, K. McCarthy, and B. van Milligen. The effect of pellet injection on turbulent transport in TJ-II. [[doi:10.1063/5.0163832|Phys. Plasmas, 30:092303, 2023]].	&lt;br /&gt;
# Krupnik, L. I. and Barcala, J. M. and Cappa, A. and Chmyga, O. O. and Dreval, M. B. and Hidalgo, C. and Khrebtov, S. M. and Komarov, O. D. and Kozachok, O. S. and Martinez, J. and Molinero, A. and de Pablos, J. L. and TJ-II Team, Plasma profiles, self -organization and Alfven eigenmodes studies using the HIBP diagnostic in the TJ-II stellarator, [[doi:10.46813/2023-143-122|Problems of atomic science and technology, 1:122-125, 2023]].	&lt;br /&gt;
# K.J. McCarthy, I. García-Cortés, J.A. Alonso, A. Arias-Camisón, E. Ascasíbar, A. Baciero, A. Cappa, R. Carrasco, O.O. Chmyga, T. Estrada, R. García, J. Hernández-Sánchez, F.J. Hernanz, O.S. Kozachok, B. López Miranda, F. Medina, D. Medina-Roque, B. van Milligen, M. Navarro, M.A. Ochando, J.L. de Pablos, N. Panadero, I. Pastor, J. de la Riva, M. C. Rodríguez, D. Tafalla, V. Tribaldos, and TJ-II Team. [[doi:10.1088/1741-4326/ad4047 |Multi-pellet injection into the NBI-heated phase of TJ-II plasmas. Nuclear Fusion, 64(6):066019, 2024]].	&lt;br /&gt;
# B.Ph. van Milligen, T. Estrada, B.A. Carreras, L. García, and the TJ-II Team. Importance of the rotational transform for L–H transitions in the TJ-II stellarator. [[doi:10.3390/plasma7020024|Plasma, 7(2):446–464, 2024]].	&lt;br /&gt;
# J.A. Alonso, D. Alegre, J. Alonso, R. Antón, A. Arias-Camisón, E. Ascasíbar, A. Baciero, J.M. Barcala, M. Barnes, E. Blanco, L. Bueno, A. Bustos, S. Cabrera, E. de la Cal, I. Calvo, A. Cappa, D. Carralero, R. Carrasco, B. Carreras, R. Castro, A. de Castro, L. Cebrián, M. Chamorro, A.A. Chmyga, P. Colino, J. Duque, F.J. Escoto, T. Estrada, A. Fernández, J. Fraguas, J.M. Fontdecaba, A. Gabriel, L. García, I. García-Cortés, R. García-Gómez, J.M. García-Regaña, G. Godino-Sedano, J. Gómez-Manchón, A. González, A. González-Jerez, V. Guisse, J. Hernández-Sánchez, J. Hernanz, C. Hidalgo, P. Ivanova, A. Jiménez-Denche, D. Jiménez-Rey, G. Kocsis, M. Koepke, A.S. Kozachek, F. Lapayese, M. Liniers, D. López, D. López-Bruna, B. López-Miranda, E. de la Luna, E. Maragkoudakis, F. Martín-Díaz, G. Martín-Gómez, J. Martínez-Fernández, K.J. McCarthy, F. Medina, D. Medina-Roque, M. Medrano, P. Méndez, F.J. Miguel, B. van Milligen, A. Molinero, G. Motojima, S. Mulas, M. Navarro, I. Nedzelskiy, R. Nuñez, M. Ochando, E. Oyarzábal, J.L. de Pablos, F. Palomares, N. Panadero, F.I. Parra, C. Pastor, I. Pastor, A. de la Peña, R. Peralta, A. Pereira, P. Pons-Villalonga, A.B. Portas, E. Poveda, F.J. Ramos, G.A. Rattá, M. Redondo, C. Reynoso, E. Rincón, J. de la Riva, C. Rodríguez-Fernández, A. Ros, E. Sánchez, J. Sánchez, E. Sánchez-Sarabia, J.A. Sebastián, E.R. Solano, A. Soleto, T. Szepesi, F.L. Tabarés, D. Tafalla, H. Takahashi, N. Tamura, H. Thienpondt, A. Tolkachev, V. Tribaldos, R. Unamuno, J. Varela, J. Vega, J.L. Velasco, and I. Voldiner. Density profiles in stellarators: an overview of particle transport, fuelling and profile shaping studies at TJ-II. [[doi:10.1088/1741-4326/ad67ef|Nuclear Fusion, 64(11):112018, 2024]].&lt;br /&gt;
# H. Bsharat, Igor Voldiner, B. Ph. van Milligen, and C. Xiao. Conditional cross-correlation analysis of floating potential fluctuations in the TJ-II stellarator. [[doi:10.1080/10420150.2024.2434503|Radiation Effects and Defects in Solids, 179(11-12):1527, 2024]].	&lt;br /&gt;
#  B.Ph. van Milligen, I. García-Cortés, K.J. McCarthy, B.A. Carreras, L. García, A. Cappa, P. Pons-Villalonga, T. Estrada, D. Medina-Roque, J. Hernández Sánchez, R. García, O.S. Kozachok, O.O. Chmyga, J.L. de Pablos, J.M. Barcala, A. Molinero, I. Pastor, D. Tafalla, A. de la Peña, F. Lapayese, and the TJ-II Team. The rotational transform and enhanced confinement in the TJ-II stellarator. [[doi:10.1017/S0022377825100433|J. Plasma Phys., 91(4):E98, 2025]].	&lt;br /&gt;
# G. Grenfell, M. Griener, M. Bernert, J. Adamek, D. Brida, M. Faitsch, P. Manz, B.Ph. van Milligen, U. Stroth, the ASDEX Upgrade Team, and the EUROfusion Tokamak Exploitation Team. On the evolution of profiles and fluctuations towards the L-mode density limit in ASDEX Upgrade. [[doi:10.1088/1741-4326/adeda1|Nuclear Fusion, 65(8):086023, 2025]].	&lt;br /&gt;
# J. Ortiz, J. Varela, L. Herrera Quesada, P. Pons-Villalonga, A. Cappa, U. Losada, F. Papousek, B. Ph. van Milligen, L. Garcia, D. A. Spong, Y. Ghai, M. A. Ochando, and C. Hidalgo. Analysis of the HAE activity in the TJ-II stellarator using a Landau closure model. [[doi:10.1063/5.0263300|Phys. Plasmas, 32:072506, 2025]].	&lt;br /&gt;
# Paulo Aguayo, Gonzalo Farias, Alejandro González-Ganzábal, Ernesto Fabregas, Teresa Estrada, Boudewijn van Milligen, Alfonso Baciero, Belén López-Miranda, Francisco Medina, and Giuseppe A. Rattá Gutiérrez. A data-driven approach to estimate plasma density in TJ-II stellarator. [[doi:10.1016/j.fusengdes.2025.115596|Fusion Engineering and Design, 224:115596, 2026]].	&lt;br /&gt;
# A. González Ganzábal, G.A. Rattá, T. Estrada, J. Martínez-Fernández, N. Panadero, A. Cappa,B. López-Miranda, A. Baciero, F. Martín, D. Tafalla, B.P. Van Milligen, F. Medina, A. de la Peña, and S. Dormido-Canto. A comprehensive database of TJ-II signals and diagnostics for statistically based models. [[doi:10.1016/j.fusengdes.2025.115613|Fusion Engineering and Design, 224:115613, 2026]].	&lt;br /&gt;
# I Voldiner, E de la Cal, B van Milligen, and TJ-II Team. Spectroscopic gas puff imaging diagnostic for the measurement of two-dimensional electron density and temperature distributions. [[doi:10.1088/1361-6587/ae5686|Plasma Physics and Controlled Fusion, 68(4):045017, 2026]].	&lt;br /&gt;
# Arnold Alonso Alvarez, Boudewijn Ph Van Milligen, Igor Voldiner, Ibere Luiz Caldas, Zwinglio Guimarães Filho, Oleksandr Kozachok, and Alexander Chmyga. Edge turbulence dynamics across electron–ion root transitions during ECRH modulation experiments in the TJ-II stellarator. [[doi:10.1088/1361-6587/ae7470|Plasma Physics and Controlled Fusion, 68(6):065019, 2026]].	&lt;br /&gt;
# Andres Cureño-Ramirez, Luis Gerardo de la Fraga, Giuseppe A. Rattá, Alejandro González-Ganzábal, Alfonso Baciero, Belén López-Miranda, Boudewijn van Milligen, Alfonso Pardo, and Jesús Calle-Cancho. Data-driven estimation of experimental signals in TJ-II: A proof of principle. [[doi:10.1016/j.fusengdes.2026.115847|Fusion Engineering and Design, 230:115847, 2026]].	&lt;br /&gt;
# B.Ph. van Milligen, I. Voldiner, E. de la Cal, A. Alonso Alvarez, I. Luiz Caldas and Z. Guimarães Filho, Turbulence analysis with the spectroscopic gas puff imaging diagnostic in the TJ-II stellarator, [[doi:10.1088/1361-6587/ae92b5|Plasma Phys. Control. Fusion (2026)]] &lt;br /&gt;
&lt;br /&gt;
=== Conferences ===&lt;br /&gt;
&lt;br /&gt;
# Oral: K. J. McCarthy, I. García-Cortés, V. Tribaldos, D. Medina-Roque, N. Panadero, E. Ascasíbar, A. A. Chmyga, T. Estrada, J. Hernández-Sánchez, A. S. Kozachek, M. Liniers, P. Medina, M. A. Ochando, J. L. de Pablos, I. Pastor, C. Toledo, B. van Milligen, and TJ-II Team. Enhanced confinement after multi-pellet injection into neutral beam injection heated plasmas in the stellarator TJ-II. In Proc. 48th EPS Conference on Plasma Physics, volume 46A of ECA, page O2.103. European Physical Society, 2022.&lt;br /&gt;
# Poster: I. Voldiner, E. de la Cal, B. van Milligen, C. Hidalgo, and TJ-II Team. Novel high speed spectrally resolved imaging system for simultaneous 2-D Te and ne edge plasma measurements with temporal resolution up to 100 kHz. In Proc. 48th EPS Conference on Plasma Physics, volume 46A of ECA, page P2b.106. European Physical Society, 2022.&lt;br /&gt;
# Poster: D. Medina-Roque, I. García-Cortés, K. J. McCarthy, N. Tamura, N. Panadero, E.Ascasíbar, T. Estrada, J. Hernández-Sánchez, A. S. Kozachek, M. Liniers, P. Medina, M. Ochando, J. L. de Pablos, I. Pastor, C. Toledo, B. van Milligen, and TJ-II Team. New insights into cryogenic and TESPEL pellet physics in TJ-II. In Proc. 48th EPS Conference on Plasma Physics, volume 46A of ECA, page P2b.113. European Physical Society, 2022.&lt;br /&gt;
# Oral:  I. Voldiner, E. de la Cal, B. van Milligen and TJ-II Team, Two-dimensional ne and Te measurements of the edge plasma turbulence in TJ-II. In Proc. 49th EPS Conference on Plasma Physics, European Physical Society, In Proc. 49th EPS Conference on Plasma Physics, volume 47A of ECA, page O2.102, 2023.&lt;br /&gt;
# Poster:  I. García-Cortés, K. J. McCarthy, V. Tribaldos, D. Medina-Roque, N. Panadero, E. Ascasíbar, T.Estrada, J. Hernández-Sánchez, A. S. Kozachek, R. Carrasco, B. López-Miranda, P. Medina, M.A. Ochando, J. L. de Pablos, I. Pastor, B. van Milligen &amp;amp; TJ-II team.  Enhanced confinement induced by multi-pellet injection into neutral beam injection heated plasmas in the stellarator TJ-II.  In Proc. 49th EPS Conference on Plasma Physics, European Physical Society,  In Proc. 49th EPS Conference on Plasma Physics, volume 47A of ECA, page P4.008, 2023&lt;br /&gt;
# Poster: L. García, I. García-Cortés, B. Carreras, K. McCarthy, and B. van Milligen. Consequences of pellet injection on the turbulent transport in TJ-II. In Proc. 49th EPS Conference on Plasma Physics, volume 47A of ECA, page P4.079. European Physical Society, 2023.&lt;br /&gt;
# Oral: J. A. Alonso and D. Alegre and J. Alonso and R. Antón and A. Arias-Camisón and E. Ascasíbar and A. Baciero and J.M. Barcala and M. Barnes and E. Blanco and L. Bueno and A. Bustos and S. Cabrera and A. de Castro and E. de la Cal and I. Calvo and A. Cappa and D. Carralero and R. Carrasco and B. Carreras and R. Castro and A. de Castro and L. Cebrián and A.A. Chmyga and M. Chamorro and P. Colino and J. Duque and F.J. Escoto and T. Estrada and A. Fernández and J. Fraguas and J.M. Fontdecaba and A. Gabriel and L. García and I. García-Cortés and R. García-Gómez and J.M. García-Regaña and G. Godino-Sedano and J. Gómez-Manchón and A. González-Jerez and V. Guisse and J. Hernández-Sánchez and J. Hernanz and C. Hidalgo and P. Ivanova and A. Jiménez-Denche and D. Jiménez-Rey and G. Kocsis and M. Koepke and A.S. Kozachek and F. Lapayese and M. Liniers and D. López and D. López-Bruna and B. López-Miranda and E. de la Luna and E. Maragkoudakis and F. Martín-Díaz and G. Martín-Gómez and J. Martínez-Fernández and K.J. McCarthy and F. Medina and D. Medina-Roque and M. Medrano and P. Méndez and F.J. Miguel and B. van Milligen and A. Molinero and G. Motojima and S. Mulas and M. Navarro and I. Nedzelskiy and R. Nuñez and M. Ochando and E. Oyarzábal and J.L. de Pablos and F. Palomares and N. Panadero and F.I. Parra and C. Pastor and I. Pastor and A. de la Peña and R. Peralta and A. Pereira and P. Pons-Villalonga and A.B. Portas and E. Poveda and F.J. Ramos and G.A. Rattá and M. Redondo and C. Reynoso and E. Rincón and J. de la Riva and C. Rodríguez-Fernández and A. Ros and E. Sánchez and J. Sánchez and E. Sánchez-Sarabia and J.A. Sebastián and E.R. Solano and A. Soleto and T. Szepesi and F.L. Tabarés and D. Tafalla and H. Takahashi and N. Tamura and H. Thienpondt and A. Tolkachev and V. Tribaldos and R. Unamuno and J. Varela and J. Vega and J.L. Velasco and I. Voldiner. Density profiles in stellarators: an overview of particle transport, fueling and profile shaping studies at TJ-II. 29th IAEA Fusion Energy Conference, IAEA-CN-316/2223, 2023&lt;br /&gt;
# Poster: K. J. McCarthy, I. García-Cortés, T. Estrada, D. Medina-Roque, B. Van Milligen, N. Pandero, E. Ascasíbar, R. Carrasco, R. García, J. Hernández-Sánchez, B. López Miranda, TJ-II Team, V. Tribaldos, A. A. Chmyga, S. Kozachek. Enhanced plasma performance after pellet injection in the stellarator TJ-II. 29th IAEA Fusion Energy Conference, IAEA-CN-316/1875, 2023&lt;br /&gt;
# Poster: J.L de Pablos, B. van Milligen, J.M. Barcala, A. Molinero, I. García-Cortés, O. Chmyga, O.S. Kozachok, G. Martín, R. García, R. Sánchez, J.M. Reynolds-Barredo, C. Hidalgo, and the TJ-II Team. Turbulence control through feedback of zonal flows. In 50th EPS Conference on Plasma Physics, volume 48A of ECA, page P2.070. EPS, European Physical Society, 2024.&lt;br /&gt;
# Poster: L. García, B.A. Carreras, B.Ph. van Milligen, I. García-Cortés, K.J. McCarthy, and the TJ-II Team. Impact of low order rationals in the enhanced confinement by pellet injection in TJ-II. In 50th EPS Conference on Plasma Physics, volume 48A of ECA, page P4.074. EPS, European Physical Society, 2024.&lt;br /&gt;
# Poster: I. García-Cortés, K.J. McCarthy, B. van Milligen, T. Estrada, D. Medina-Roque, A. Baciero, B.A. Carreras, A. Cappa, A.A. Chmyga, F. Medina, L. Garcia, R. García, J. Hernández-Sánchez, F.J. Hernanz, A.S. Kozachek, F. Lapayese, B. Lopez-Miranda, D. Lopez-Bruna, J.L. De Pablos, N. Panadero, I. Pastor, A. de la Peña, P. Pons-Villalonga, M.C. Rodriguez, D. Tafalla, V. Tribaldos, and TJ-II Team. Exploring enhanced plasma performance after pellet injections via rotational transform modulation in the TJ-II stellarator. In Proc. 29th IAEA Fusion Energy Conference, volume IAEA-CN-316/2795, pages P1–2803. IAEA, 2025.&lt;br /&gt;
# Poster: K. J. McCarthy, I. García-Cortés, B. van Milligen, A. Baciero, R. Carrasco, T. Estrada, R. García, J. Hernández Sánchez, B. López Miranda, F. Medina, D. Medina-Roque, M. Navarro, N. Panadero, I. Pastor, M. C. Rodríguez, and TJ-II Team. Interpreting structures observed in pellet ablation profiles in the stellarator TJ-II. In Proc. 29th IAEA Fusion Energy Conference, pages IAEA–CN–316/2795. IAEA, 2025.&lt;br /&gt;
# Poster: V. Tribaldos, I. García-Cortés, K.J. Mccarthy, J.M. Reynolds-Barredo, D. Medina-Roque, A. Baciero, O.O. Chmyga, T. Estrada, O.S. Kozachok, D. López-Bruna, F. Medina, B. van Milligen, J.L. de Pablos, N. Panadero, I. Pastor, J. de la Riva, and TJ-II Team. Confinement modelling of enhanced plasma performance after multiple pellet injections in the TJ-II stellarator. In Proc. 29th IAEA Fusion Energy Conference, pages IAEA–CN–316–2804. IAEA, 2025.&lt;br /&gt;
# Poster: A. González Ganzábal, G.A. Rattá, T. Estrada, J. Martínez-Fernández, N. Panadero, A. Cappa, B. López-Miranda, A. Baciero, F. Martín, D. Tafalla, B.P. Van Milligen, F. Medina, A. de la Peña, S. Dormido-Canto, and the TJ-II team. Development of a standardised TJ-II database for machine learning models and applications. In International Stellarator and Heliotron Workshop, 2026.&lt;br /&gt;
# Poster: B.Ph. van Milligen, I. García-Cortés, K.J. McCarthy, B.A. Carreras, L. García, O.S. Kozachok, O.O. Chmyga, J.L. de Pablos, and the TJ-II Team. Impact of the rotational transform and pellets on enhanced confinement and turbulence in the TJ-II stellarator. In 52nd EPS Conference on Plasma Physics, ECA, P2.1095. EPS, European Physical Society, 2026.&lt;br /&gt;
# Poster: B.Ph. van Milligen, I. Voldiner, E. de la Cal, Arnold A. Alvarez, I.L. Caldas, Z.O. Guimarães-Filho, and the TJ-II Team. Turbulence analysis with the spectral gas puff imaging diagnostic in the TJ-II stellarator. In 52nd EPS Conference on Plasma Physics, ECA, P2.1117. EPS, European Physical Society, 2026.&lt;br /&gt;
# Poster: Arnold A. Alvarez, Boudewijn Ph. van Milligen, Igor Voldiner, Iberê L. Caldas, Zwinglio O. Guimarães-Filho, O.S. Kozachok, O.O. Chmyga, and the TJ-II Team. Turbulence and transport across electron-ion root transitions during ECRH modulation in the TJ-II stellarator. In 52nd EPS Conference on Plasma Physics, ECA, P2.1001. EPS, European Physical Society, 2026. &lt;br /&gt;
# Poster: V. Tribaldos, I. García-Cortés, K.J. Mc-Carthy, J.M. Reynolds-Barredo, B. Van Milligen, A. Baciero, J. De La Riva, J.L. De Pablos, O.S. Kozachek, I. Pastor, and the TJ-II Team. Validation of neoclassical Er predictions in multi-pellet induced enhanced confinement regimes in TJ-II. In 52nd EPS Conference on Plasma Physics, ECA, P3.1167. EPS, European Physical Society, 2026.&lt;br /&gt;
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&amp;lt;!-- Change category to [[Category:LNF Nationally Funded Projects - finished]] once the project is finished --&amp;gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=LNF:(2022-2026)_Estudio_de_transporte_y_turbulencia_en_plasmas_con_m%C3%A9todos_de_gran_resoluci%C3%B3n_espacial&amp;diff=8732</id>
		<title>LNF:(2022-2026) Estudio de transporte y turbulencia en plasmas con métodos de gran resolución espacial</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=LNF:(2022-2026)_Estudio_de_transporte_y_turbulencia_en_plasmas_con_m%C3%A9todos_de_gran_resoluci%C3%B3n_espacial&amp;diff=8732"/>
		<updated>2026-10-13T08:19:23Z</updated>

		<summary type="html">&lt;p&gt;Admin: Created page with &amp;quot;== LNF - Nationally funded project ==  &amp;#039;&amp;#039;&amp;#039;Title&amp;#039;&amp;#039;&amp;#039;: &amp;#039;&amp;#039;&amp;#039;Estudio de transporte y turbulencia en plasmas con métodos de gran resolución espacial&amp;#039;&amp;#039;&amp;#039;  &amp;#039;&amp;#039;&amp;#039;Reference&amp;#039;&amp;#039;&amp;#039;: PID2021-124883NB-I00  &amp;#039;&amp;#039;&amp;#039;Programme and date&amp;#039;&amp;#039;&amp;#039;: Proyectos de investigación no orientada (2021)  &amp;#039;&amp;#039;&amp;#039;Programme type (Modalidad de proyecto)&amp;#039;&amp;#039;&amp;#039;: Proyectos de Generación de Conocimiento  &amp;#039;&amp;#039;&amp;#039;Area/subarea (Área temática / subárea)&amp;#039;&amp;#039;&amp;#039;: Energía y transporte / Energía  &amp;#039;&amp;#039;&amp;#039;Principal Investigator(s)&amp;#039;&amp;#039;&amp;#039;: [https://...&amp;quot;&lt;/p&gt;
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&lt;div&gt;== LNF - Nationally funded project ==&lt;br /&gt;
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&#039;&#039;&#039;Title&#039;&#039;&#039;: &#039;&#039;&#039;Estudio de transporte y turbulencia en plasmas con métodos de gran resolución espacial&#039;&#039;&#039;&lt;br /&gt;
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&#039;&#039;&#039;Reference&#039;&#039;&#039;: PID2021-124883NB-I00&lt;br /&gt;
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&#039;&#039;&#039;Programme and date&#039;&#039;&#039;: Proyectos de investigación no orientada (2021)&lt;br /&gt;
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&#039;&#039;&#039;Programme type (Modalidad de proyecto)&#039;&#039;&#039;: Proyectos de Generación de Conocimiento&lt;br /&gt;
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&#039;&#039;&#039;Area/subarea (Área temática / subárea)&#039;&#039;&#039;: Energía y transporte / Energía&lt;br /&gt;
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&#039;&#039;&#039;Principal Investigator(s)&#039;&#039;&#039;: [https://orcid.org/0000-0002-3850-0196 José Luis de Pablos Hernández] y [https://orcid.org/0000-0001-5344-6274 Boudewijn van Milligen]&lt;br /&gt;
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&#039;&#039;&#039;Project type&#039;&#039;&#039;: Proyecto individual&lt;br /&gt;
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&#039;&#039;&#039;Start-end dates&#039;&#039;&#039;: 01/09/2022 - 31/08/2026&lt;br /&gt;
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&#039;&#039;&#039;Financing granted (direct costs)&#039;&#039;&#039;: 150.000 €&lt;br /&gt;
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&#039;&#039;&#039;Acknowledgement&#039;&#039;&#039;: Grant PID2021-124883NB-I00 funded by MICIU/AEI/10.13039/501100011033 and by “ERDF/EU”. &lt;br /&gt;
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[[File:LogoOficial_PlanNacional_2021.png|500px]] &lt;br /&gt;
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== Description of the project ==&lt;br /&gt;
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The general goal of the present proposal is to investigate the interaction of turbulence, plasmas flows and the magnetic topology and determine the impact of the resulting complex interactions on plasma transport. This topic could be important for ITER and DEMO.&lt;br /&gt;
To reach this goal, we need to reach the following objectives:&lt;br /&gt;
# Development of novel low noise electronics in vacuum and test it to obtain a better SNR than the actual one with the help of Ciemat electronics team. This upgrade is essential to be able to measure phase relations between fluctuating fields and understand their mutual interaction.&lt;br /&gt;
# Study the impact of the magnetic configuration on turbulent properties. We expect to find that the location of major rational surfaces plays a significant role in radial transport.&lt;br /&gt;
# Study the impact of confinement transitions on turbulence, and flows on plasma turbulence. &lt;br /&gt;
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== Main results ==&lt;br /&gt;
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El proyecto ha permitido avanzar significativamente en la comprensión de los mecanismos que regulan la turbulencia y la transición al régimen de alto confinamiento (L-H) en el stellarator TJ-II, un aspecto clave para el desarrollo de la energía de fusión. Aprovechando la flexibilidad del dispositivo para modificar con precisión la configuración magnética, se han realizado experimentos pioneros que han puesto de manifiesto la influencia de las superficies racionales y de la corriente neta del plasma sobre las propiedades turbulentas y el confinamiento.&lt;br /&gt;
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Entre los principales resultados destaca la identificación de la intermitencia como un nuevo parámetro para caracterizar la turbulencia, demostrando su sensibilidad tanto a la configuración magnética como a los flujos de plasma. Asimismo, mediante experimentos con variaciones dinámicas de la configuración magnética se ha establecido una relación directa entre la evolución temporal de la turbulencia y la presencia de superficies racionales de bajo orden.&lt;br /&gt;
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El proyecto también ha demostrado que la transición L-H y la mejora del confinamiento dependen de forma sistemática de la corriente neta del plasma y, por tanto, de la configuración magnética. El análisis combinado de experimentos y simulaciones de turbulencia MHD resistiva ha permitido proponer mecanismos físicos que explican esta dependencia, relacionados con la distribución de superficies racionales y la generación de flujos zonales capaces de suprimir la turbulencia.&lt;br /&gt;
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Estos resultados contribuyen a mejorar la comprensión de los procesos fundamentales que determinan el confinamiento del plasma y proporcionan nuevos criterios para optimizar el funcionamiento de futuros dispositivos de fusión, reforzando el liderazgo científico en el ámbito del confinamiento magnético.&lt;br /&gt;
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== Dissemination of project results (peer-reviewed publications and conference presentations) ==&lt;br /&gt;
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	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8731</id>
		<title>TJ-II:Magnetic configuration</title>
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		<updated>2026-10-10T18:56:04Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* Flexibility */&lt;/p&gt;
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&lt;div&gt;The magnetic configuration of [[TJ-II]] in vacuum is completely determined by the currents flowing through the [[TJ-II:Coil system|external coils]].&lt;br /&gt;
Magnetic configurations are labelled as &#039;xxx_yy_zz&#039;, where&lt;br /&gt;
* &#039;xxx&#039;: 10 times the current (in kA) in the circular coil&lt;br /&gt;
* &#039;yy&#039;: 10 times the current (in kA) in the helical coil&lt;br /&gt;
* &#039;zz&#039;: 10 times the current (in kA) in the vertical field coils&lt;br /&gt;
The current in the toroidal field coils is not specified, as its value is adjusted to guarantee central absorption of the [[TJ-II:Electron Cyclotron Resonant Heating|Electron Cyclotron Resonant Heating]] source (requiring a specific &#039;resonant&#039; value of the magnetic field at the magnetic axis, &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
Configuration list:&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;width: 100%&amp;quot; border=&amp;quot;1&amp;quot;||&lt;br /&gt;
|-&lt;br /&gt;
! Configuration &lt;br /&gt;
! &amp;lt;math&amp;gt;r_{av}&amp;lt;/math&amp;gt; (cm) &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(0)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(a)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{m,av}&amp;lt;/math&amp;gt;(T) &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt; (T) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(0^\circ)&amp;lt;/math&amp;gt; (m) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(45^\circ)&amp;lt;/math&amp;gt; (m) &lt;br /&gt;
! Shear (%) &lt;br /&gt;
! Well (%)&lt;br /&gt;
|-&lt;br /&gt;
|0_20_13    ||1.139      || 1.185      || 1.194     ||  1.033     || 0.9504     ||  1.644      || 1.374     || 0.7793      ||5.7521E-02&lt;br /&gt;
|-&lt;br /&gt;
|0_30_15    ||4.228      || 1.518      || 1.698     ||  1.019     || 0.9500     ||  1.658      || 1.360     ||  11.85      || 1.050&lt;br /&gt;
|-&lt;br /&gt;
|0_40_18    ||5.903      || 1.756      || 2.003     ||  1.008     || 0.9505     ||  1.671      || 1.347     ||  14.09      || 1.217&lt;br /&gt;
|-&lt;br /&gt;
|0_50_22    ||6.480      || 1.936      || 2.230     || 0.9973     || 0.9502     ||  1.682      || 1.336     ||  15.17      || 2.481&lt;br /&gt;
|-&lt;br /&gt;
|0_60_26    ||8.500      || 2.073      || 2.399     || 0.9885     || 0.9502     ||  1.692      || 1.326     ||  15.70      || 3.218&lt;br /&gt;
|-&lt;br /&gt;
|0_70_29    ||7.147      || 2.187      || 2.434     || 0.9805     || 0.9503     ||  1.701      || 1.317     ||  11.30      || 2.985&lt;br /&gt;
|-&lt;br /&gt;
|0_80_34    ||6.902      || 2.284      || 2.469     || 0.9736     || 0.9506     ||  1.710      || 1.308     ||  8.084      || 2.735&lt;br /&gt;
|-&lt;br /&gt;
|0_90_38    ||6.738      || 2.366      || 2.514     || 0.9663     || 0.9503     ||  1.719      || 1.299     ||  6.269      || 2.534&lt;br /&gt;
|-&lt;br /&gt;
|0_100_42   ||12.59      || 2.436      || 2.667     || 0.9601     || 0.9505     ||  1.727      || 1.291     ||  9.493      || 4.643&lt;br /&gt;
|-&lt;br /&gt;
|0_110_46   ||10.67      || 2.493      || 2.667     || 0.9539     || 0.9503     ||  1.734      || 1.284     ||  6.980      || 4.554&lt;br /&gt;
|-&lt;br /&gt;
|0_120_50   ||12.71      || 2.548      || 2.667     || 0.9482     || 0.9504     ||  1.742      || 1.276     ||  4.683      || 4.272&lt;br /&gt;
|-&lt;br /&gt;
|10_20_18   || 2.557     ||  1.148     ||  1.184    ||   1.024    ||  0.9514    ||   1.652     ||  1.366    ||   3.183     || 0.2469&lt;br /&gt;
|-&lt;br /&gt;
|10_30_20   || 6.083     ||  1.438     ||  1.602    ||   1.010    ||  0.9501    ||   1.666     ||  1.352    ||   11.35     ||  1.398&lt;br /&gt;
|-&lt;br /&gt;
|10_40_24   || 6.921     ||  1.659     ||  1.880    ||   1.000    ||  0.9504    ||   1.678     ||  1.340    ||   13.34     ||  2.751&lt;br /&gt;
|-&lt;br /&gt;
|10_50_27   || 8.140     ||  1.826     ||  1.997    ||  0.9909    ||  0.9504    ||   1.688     ||  1.329    ||   9.321     ||  3.241&lt;br /&gt;
|-&lt;br /&gt;
|10_60_31   || 9.350     ||  1.965     ||  2.183    ||  0.9826    ||  0.9505    ||   1.698     ||  1.319    ||   11.11     ||  3.084&lt;br /&gt;
|-&lt;br /&gt;
|10_70_35   || 10.10     ||  2.077     ||  2.288    ||  0.9750    ||  0.9505    ||   1.707     ||  1.310    ||   10.16     ||  3.597&lt;br /&gt;
|-&lt;br /&gt;
|10_80_38   || 9.810     ||  2.174     ||  2.371    ||  0.9674    ||  0.9502    ||   1.716     ||  1.302    ||   9.037     ||  3.908&lt;br /&gt;
|-&lt;br /&gt;
|10_90_42   || 10.54     ||  2.257     ||  2.434    ||  0.9610    ||  0.9503    ||   1.724     ||  1.294    ||   7.851     ||  4.281&lt;br /&gt;
|-&lt;br /&gt;
|10_100_47  || 10.21     ||  2.327     ||  2.482    ||  0.9546    ||  0.9502    ||   1.732     ||  1.286    ||   6.647     ||  4.236&lt;br /&gt;
|-&lt;br /&gt;
|10_110_51  || 11.11     ||  2.395     ||  2.547    ||  0.9488    ||  0.9501    ||   1.740     ||  1.278    ||   6.331     ||  5.121&lt;br /&gt;
|-&lt;br /&gt;
|10_120_55  || 10.04     ||  2.451     ||  2.565    ||  0.9432    ||  0.9502    ||   1.747     ||  1.271    ||   4.674     ||  4.426&lt;br /&gt;
|-&lt;br /&gt;
|20_10_21   || 1.213     || 0.7902     || 0.7956    ||   1.028    ||  0.9503    ||   1.645     ||  1.373    ||  0.6830     || 3.7624E-02&lt;br /&gt;
|-&lt;br /&gt;
|20_20_22   || 3.952     ||  1.136     ||  1.185    ||   1.014    ||  0.9500    ||   1.661     ||  1.357    ||   4.350     || 0.4717&lt;br /&gt;
|-&lt;br /&gt;
|20_30_25   || 6.779     ||  1.395     ||  1.521    ||   1.003    ||  0.9502    ||   1.673     ||  1.344    ||   9.049     ||  1.550&lt;br /&gt;
|-&lt;br /&gt;
|20_40_28   || 8.475     ||  1.592     ||  1.771    ||  0.9922    ||  0.9498    ||   1.685     ||  1.333    ||   11.25     ||  2.879&lt;br /&gt;
|-&lt;br /&gt;
|20_50_32   || 8.039     ||  1.756     ||  1.906    ||  0.9842    ||  0.9505    ||   1.695     ||  1.323    ||   8.571     ||  3.131&lt;br /&gt;
|-&lt;br /&gt;
|20_60_35   || 11.21     ||  1.884     ||  1.997    ||  0.9755    ||  0.9498    ||   1.705     ||  1.313    ||   5.968     ||  1.980&lt;br /&gt;
|-&lt;br /&gt;
|20_70_39   || 11.08     ||  1.994     ||  2.154    ||  0.9689    ||  0.9504    ||   1.714     ||  1.304    ||   7.982     ||  3.385&lt;br /&gt;
|-&lt;br /&gt;
|20_80_43   || 12.14     ||  2.092     ||  2.255    ||  0.9614    ||  0.9497    ||   1.722     ||  1.296    ||   7.811     ||  4.133&lt;br /&gt;
|-&lt;br /&gt;
|20_90_47   || 12.83     ||  2.174     ||  2.324    ||  0.9558    ||  0.9503    ||   1.730     ||  1.288    ||   6.862     ||  4.713&lt;br /&gt;
|-&lt;br /&gt;
|20_100_51  || 12.68     ||  2.246     ||  2.379    ||  0.9498    ||  0.9503    ||   1.738     ||  1.280    ||   5.945     ||  4.930&lt;br /&gt;
|-&lt;br /&gt;
|20_110_55  || 13.79     ||  2.313     ||  2.434    ||  0.9443    ||  0.9505    ||   1.745     ||  1.273    ||   5.248     ||  5.117&lt;br /&gt;
|-&lt;br /&gt;
|20_120_59  || 13.91     ||  2.368     ||  2.483    ||  0.9386    ||  0.9502    ||   1.752     ||  1.265    ||   4.822     ||  5.418&lt;br /&gt;
|-&lt;br /&gt;
|30_10_25   || 2.709     || 0.8385     || 0.8507    ||   1.018    ||  0.9501    ||   1.654     ||  1.363    ||   1.452     || 0.1431&lt;br /&gt;
|-&lt;br /&gt;
|30_20_27   || 5.443     ||  1.134     ||  1.189    ||   1.007    ||  0.9514    ||   1.669     ||  1.349    ||   4.847     || 0.7001&lt;br /&gt;
|-&lt;br /&gt;
|30_30_30   || 8.180     ||  1.368     ||  1.481    ||  0.9956    ||  0.9506    ||   1.681     ||  1.337    ||   8.332     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|30_40_33   || 9.756     ||  1.550     ||  1.687    ||  0.9860    ||  0.9503    ||   1.692     ||  1.326    ||   8.877     ||  2.798&lt;br /&gt;
|-&lt;br /&gt;
|30_50_37   || 11.16     ||  1.702     ||  1.878    ||  0.9779    ||  0.9503    ||   1.702     ||  1.316    ||   10.37     ||  4.941&lt;br /&gt;
|-&lt;br /&gt;
|30_60_40   || 9.262     ||  1.827     ||  1.936    ||  0.9706    ||  0.9505    ||   1.711     ||  1.307    ||   5.952     ||  3.624&lt;br /&gt;
|-&lt;br /&gt;
|30_70_44   || 12.28     ||  1.937     ||  2.007    ||  0.9631    ||  0.9502    ||   1.720     ||  1.298    ||   3.593     ||  4.431&lt;br /&gt;
|-&lt;br /&gt;
|30_80_48   || 13.28     ||  2.033     ||  2.149    ||  0.9567    ||  0.9502    ||   1.728     ||  1.290    ||   5.702     ||  3.674&lt;br /&gt;
|-&lt;br /&gt;
|30_90_52   || 14.16     ||  2.115     ||  2.231    ||  0.9504    ||  0.9501    ||   1.736     ||  1.282    ||   5.476     ||  4.227&lt;br /&gt;
|-&lt;br /&gt;
|30_100_56  || 14.97     ||  2.187     ||  2.295    ||  0.9448    ||  0.9502    ||   1.743     ||  1.275    ||   4.949     ||  4.755&lt;br /&gt;
|-&lt;br /&gt;
|30_110_59  || 15.76     ||  2.246     ||  2.356    ||  0.9391    ||  0.9500    ||   1.751     ||  1.267    ||   4.920     ||  5.215&lt;br /&gt;
|-&lt;br /&gt;
|30_120_63  || 14.48     ||  2.306     ||  2.389    ||  0.9343    ||  0.9504    ||   1.758     ||  1.260    ||   3.573     ||  5.025&lt;br /&gt;
|-&lt;br /&gt;
|40_00_27   || 1.350     || 0.5464     || 0.5471    ||   1.024    ||  0.9504    ||   1.647     ||  1.371    ||  0.1331     || 2.4768E-02&lt;br /&gt;
|-&lt;br /&gt;
|40_10_29   || 4.111     || 0.8821     || 0.9010    ||   1.010    ||  0.9510    ||   1.663     ||  1.355    ||   2.152     || 0.2456&lt;br /&gt;
|-&lt;br /&gt;
|40_20_31   || 6.646     ||  1.146     ||  1.202    ||  0.9975    ||  0.9501    ||   1.677     ||  1.341    ||   4.928     || 0.8185&lt;br /&gt;
|-&lt;br /&gt;
|40_30_34   || 9.328     ||  1.354     ||  1.452    ||  0.9884    ||  0.9506    ||   1.688     ||  1.330    ||   7.247     ||  1.826&lt;br /&gt;
|-&lt;br /&gt;
|40_40_37   || 11.15     ||  1.523     ||  1.646    ||  0.9788    ||  0.9498    ||   1.699     ||  1.319    ||   8.061     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|40_50_41   || 12.66     ||  1.666     ||  1.797    ||  0.9719    ||  0.9506    ||   1.708     ||  1.310    ||   7.872     ||  4.310&lt;br /&gt;
|-&lt;br /&gt;
|40_60_44   || 12.34     ||  1.786     ||  1.927    ||  0.9637    ||  0.9497    ||   1.717     ||  1.301    ||   7.879     ||  5.834&lt;br /&gt;
|-&lt;br /&gt;
|40_70_48   || 9.734     ||  1.894     ||  1.963    ||  0.9579    ||  0.9504    ||   1.726     ||  1.292    ||   3.625     ||  3.668&lt;br /&gt;
|-&lt;br /&gt;
|40_80_52   || 13.96     ||  1.986     ||  2.067    ||  0.9515    ||  0.9503    ||   1.734     ||  1.284    ||   4.054     ||  3.028&lt;br /&gt;
|-&lt;br /&gt;
|40_90_56   || 15.39     ||  2.062     ||  2.156    ||  0.9457    ||  0.9504    ||   1.741     ||  1.277    ||   4.529     ||  3.841&lt;br /&gt;
|-&lt;br /&gt;
|40_100_60  || 16.40     ||  2.132     ||  2.232    ||  0.9400    ||  0.9502    ||   1.749     ||  1.269    ||   4.683     ||  4.355&lt;br /&gt;
|-&lt;br /&gt;
|40_110_64  || 18.12     ||  2.199     ||  2.288    ||  0.9348    ||  0.9503    ||   1.756     ||  1.262    ||   4.049     ||  4.651&lt;br /&gt;
|-&lt;br /&gt;
|40_120_68  || 16.81     ||  2.256     ||  2.327    ||  0.9295    ||  0.9501    ||   1.763     ||  1.255    ||   3.158     ||  4.904&lt;br /&gt;
|-&lt;br /&gt;
|50_00_31   || 2.818     || 0.6329     || 0.6375    ||   1.013    ||  0.9498    ||   1.657     ||  1.361    ||  0.7286     || 6.1871E-02&lt;br /&gt;
|-&lt;br /&gt;
|50_10_33   || 5.588     || 0.9254     || 0.9532    ||   1.001    ||  0.9506    ||   1.672     ||  1.346    ||   3.003     || 0.3605&lt;br /&gt;
|-&lt;br /&gt;
|50_20_36   || 8.222     ||  1.160     ||  1.216    ||  0.9902    ||  0.9502    ||   1.684     ||  1.334    ||   4.838     ||  1.060&lt;br /&gt;
|-&lt;br /&gt;
|50_30_39   || 10.67     ||  1.352     ||  1.435    ||  0.9815    ||  0.9505    ||   1.695     ||  1.323    ||   6.163     ||  2.008&lt;br /&gt;
|-&lt;br /&gt;
|50_40_42   || 12.44     ||  1.508     ||  1.609    ||  0.9733    ||  0.9504    ||   1.705     ||  1.313    ||   6.719     ||  2.910&lt;br /&gt;
|-&lt;br /&gt;
|50_50_46   || 13.94     ||  1.644     ||  1.758    ||  0.9661    ||  0.9505    ||   1.714     ||  1.303    ||   6.944     ||  4.001&lt;br /&gt;
|-&lt;br /&gt;
|50_60_49   || 15.09     ||  1.757     ||  1.887    ||  0.9587    ||  0.9502    ||   1.723     ||  1.295    ||   7.390     ||  6.217&lt;br /&gt;
|-&lt;br /&gt;
|50_70_53   || 13.03     ||  1.855     ||  1.955    ||  0.9524    ||  0.9502    ||   1.731     ||  1.287    ||   5.353     ||  5.830&lt;br /&gt;
|-&lt;br /&gt;
|50_80_56   || 16.73     ||  1.949     ||  2.004    ||  0.9463    ||  0.9501    ||   1.739     ||  1.279    ||   2.807     ||  4.003&lt;br /&gt;
|-&lt;br /&gt;
|50_90_60   || 16.70     ||  2.011     ||  2.101    ||  0.9407    ||  0.9502    ||   1.747     ||  1.271    ||   4.501     ||  3.444&lt;br /&gt;
|-&lt;br /&gt;
|50_100_64  || 18.15     ||  2.090     ||  2.183    ||  0.9351    ||  0.9500    ||   1.754     ||  1.264    ||   4.434     ||  3.907&lt;br /&gt;
|-&lt;br /&gt;
|50_110_68  || 17.53     ||  2.154     ||  2.223    ||  0.9297    ||  0.9498    ||   1.762     ||  1.256    ||   3.205     ||  4.270&lt;br /&gt;
|-&lt;br /&gt;
|50_120_72  || 19.13     ||  2.213     ||  2.288    ||  0.9250    ||  0.9501    ||   1.768     ||  1.250    ||   3.417     ||  4.378&lt;br /&gt;
|-&lt;br /&gt;
|60_00_35   || 4.247     || 0.7126     || 0.7205    ||   1.003    ||  0.9498    ||   1.667     ||  1.352    ||   1.108     || 0.1270&lt;br /&gt;
|-&lt;br /&gt;
|60_10_37   || 6.862     || 0.9679     ||  1.002    ||  0.9934    ||  0.9509    ||   1.680     ||  1.338    ||   3.520     || 0.4827&lt;br /&gt;
|-&lt;br /&gt;
|60_20_40   || 9.669     ||  1.179     ||  1.240    ||  0.9831    ||  0.9503    ||   1.692     ||  1.326    ||   5.202     ||  1.236&lt;br /&gt;
|-&lt;br /&gt;
|60_30_43   || 12.01     ||  1.354     ||  1.435    ||  0.9747    ||  0.9502    ||   1.702     ||  1.316    ||   5.973     ||  2.132&lt;br /&gt;
|-&lt;br /&gt;
|60_40_46   || 13.48     ||  1.500     ||  1.593    ||  0.9672    ||  0.9503    ||   1.712     ||  1.306    ||   6.170     ||  2.806&lt;br /&gt;
|-&lt;br /&gt;
|60_50_50   || 15.36     ||  1.627     ||  1.732    ||  0.9601    ||  0.9504    ||   1.721     ||  1.297    ||   6.467     ||  3.895&lt;br /&gt;
|-&lt;br /&gt;
|60_60_53   || 16.79     ||  1.734     ||  1.851    ||  0.9528    ||  0.9499    ||   1.729     ||  1.289    ||   6.731     ||  5.666&lt;br /&gt;
|-&lt;br /&gt;
|60_70_57   || 15.88     ||  1.829     ||  1.934    ||  0.9473    ||  0.9502    ||   1.737     ||  1.281    ||   5.736     ||  6.958&lt;br /&gt;
|-&lt;br /&gt;
|60_80_61   || 13.66     ||  1.918     ||  1.968    ||  0.9428    ||  0.9514    ||   1.745     ||  1.273    ||   2.622     ||  4.555&lt;br /&gt;
|-&lt;br /&gt;
|60_90_64   || 17.29     ||  2.009     ||  2.063    ||  0.9359    ||  0.9501    ||   1.753     ||  1.265    ||   2.640     ||  1.637&lt;br /&gt;
|-&lt;br /&gt;
|60_100_68  || 17.62     ||  2.049     ||  2.122    ||  0.9304    ||  0.9497    ||   1.760     ||  1.258    ||   3.560     ||  3.718&lt;br /&gt;
|-&lt;br /&gt;
|60_110_72  || 17.50     ||  2.118     ||  2.177    ||  0.9257    ||  0.9501    ||   1.767     ||  1.251    ||   2.811     ||  4.023&lt;br /&gt;
|-&lt;br /&gt;
|60_120_76  || 17.78     ||  2.174     ||  2.222    ||  0.9217    ||  0.9510    ||   1.774     ||  1.244    ||   2.209     ||  4.211&lt;br /&gt;
|-&lt;br /&gt;
|70_00_39   || 5.731     || 0.7825     || 0.7975    ||  0.9949    ||  0.9497    ||   1.675     ||  1.343    ||   1.908     || 0.2335&lt;br /&gt;
|-&lt;br /&gt;
|70_10_41   || 8.418     ||  1.009     ||  1.048    ||  0.9860    ||  0.9509    ||   1.688     ||  1.330    ||   3.845     || 0.6755&lt;br /&gt;
|-&lt;br /&gt;
|70_20_44   || 11.09     ||  1.201     ||  1.265    ||  0.9767    ||  0.9504    ||   1.699     ||  1.319    ||   5.345     ||  1.317&lt;br /&gt;
|-&lt;br /&gt;
|70_30_47   || 13.41     ||  1.361     ||  1.441    ||  0.9688    ||  0.9504    ||   1.709     ||  1.309    ||   5.859     ||  2.187&lt;br /&gt;
|-&lt;br /&gt;
|70_40_51   || 14.99     ||  1.496     ||  1.591    ||  0.9615    ||  0.9503    ||   1.718     ||  1.300    ||   6.348     ||  2.859&lt;br /&gt;
|-&lt;br /&gt;
|70_50_54   || 16.87     ||  1.617     ||  1.712    ||  0.9543    ||  0.9501    ||   1.727     ||  1.291    ||   5.843     ||  3.756&lt;br /&gt;
|-&lt;br /&gt;
|70_60_57   || 17.89     ||  1.718     ||  1.823    ||  0.9479    ||  0.9500    ||   1.735     ||  1.283    ||   6.140     ||  4.746&lt;br /&gt;
|-&lt;br /&gt;
|70_70_61   || 18.26     ||  1.812     ||  1.928    ||  0.9423    ||  0.9503    ||   1.743     ||  1.275    ||   6.353     ||  6.812&lt;br /&gt;
|-&lt;br /&gt;
|70_80_65   || 16.37     ||  1.896     ||  1.962    ||  0.9363    ||  0.9499    ||   1.751     ||  1.267    ||   3.469     ||  5.948&lt;br /&gt;
|-&lt;br /&gt;
|70_90_68   || 9.135     ||  1.980     ||  1.988    ||  0.9317    ||  0.9506    ||   1.758     ||  1.260    ||  0.3692     || 0.1186&lt;br /&gt;
|-&lt;br /&gt;
|70_100_72  || 18.64     ||  2.007     ||  2.094    ||  0.9267    ||  0.9506    ||   1.765     ||  1.253    ||   4.327     ||  3.356&lt;br /&gt;
|-&lt;br /&gt;
|70_110_76  || 18.23     ||  2.088     ||  2.147    ||  0.9219    ||  0.9507    ||   1.772     ||  1.246    ||   2.792     ||  3.707&lt;br /&gt;
|-&lt;br /&gt;
|70_120_80  || 17.89     ||  2.145     ||  2.184    ||  0.9171    ||  0.9506    ||   1.779     ||  1.239    ||   1.846     ||  4.043&lt;br /&gt;
|-&lt;br /&gt;
|80_00_42   ||7.247      ||0.8436      ||0.8697     || 0.9869     || 0.9497     ||  1.684      || 1.335     ||  3.094      ||0.2402&lt;br /&gt;
|-&lt;br /&gt;
|80_10_45   ||9.865      || 1.049      || 1.095     || 0.9794     || 0.9513     ||  1.695      || 1.323     ||  4.371      ||0.7359&lt;br /&gt;
|-&lt;br /&gt;
|80_20_48   ||12.28      || 1.226      || 1.290     || 0.9697     || 0.9500     ||  1.706      || 1.312     ||  5.206      || 1.327&lt;br /&gt;
|-&lt;br /&gt;
|80_30_51   ||14.38      || 1.370      || 1.454     || 0.9626     || 0.9503     ||  1.715      || 1.303     ||  6.088      || 2.102&lt;br /&gt;
|-&lt;br /&gt;
|80_40_54   ||16.47      || 1.500      || 1.594     || 0.9549     || 0.9497     ||  1.724      || 1.294     ||  6.263      || 2.799&lt;br /&gt;
|-&lt;br /&gt;
|80_50_58   ||17.63      || 1.612      || 1.706     || 0.9492     || 0.9503     ||  1.733      || 1.285     ||  5.842      || 3.329&lt;br /&gt;
|-&lt;br /&gt;
|80_60_61   ||18.84      || 1.712      || 1.814     || 0.9436     || 0.9507     ||  1.741      || 1.277     ||  5.984      || 3.990&lt;br /&gt;
|-&lt;br /&gt;
|80_70_65   ||19.27      || 1.799      || 1.898     || 0.9372     || 0.9501     ||  1.749      || 1.269     ||  5.555      || 4.728&lt;br /&gt;
|-&lt;br /&gt;
|80_80_69   ||17.96      || 1.880      || 1.935     || 0.9321     || 0.9503     ||  1.756      || 1.262     ||  2.921      || 3.774&lt;br /&gt;
|-&lt;br /&gt;
|80_90_73   ||13.42      || 1.957      || 1.982     || 0.9266     || 0.9500     ||  1.764      || 1.254     ||  1.312      ||0.6938&lt;br /&gt;
|-&lt;br /&gt;
|80_100_76  || 18.53     ||  2.008     ||  2.065    ||  0.9220    ||  0.9504    ||   1.770     ||  1.247    ||   2.839     ||  1.773&lt;br /&gt;
|-&lt;br /&gt;
|80_110_80  || 18.41     ||  2.059     ||  2.117    ||  0.9176    ||  0.9507    ||   1.777     ||  1.241    ||   2.847     ||  3.632&lt;br /&gt;
|-&lt;br /&gt;
|80_120_84  || 18.26     ||  2.117     ||  2.157    ||  0.9122    ||  0.9496    ||   1.784     ||  1.234    ||   1.872     ||  3.986&lt;br /&gt;
|-&lt;br /&gt;
|90_00_46   || 8.679     || 0.9022     || 0.9354    ||  0.9802    ||  0.9501    ||   1.691     ||  1.327    ||   3.678     || 0.3981&lt;br /&gt;
|-&lt;br /&gt;
|90_10_49   || 11.45     ||  1.090     ||  1.146    ||  0.9717    ||  0.9502    ||   1.702     ||  1.315    ||   5.148     || 0.8099&lt;br /&gt;
|-&lt;br /&gt;
|90_20_52   || 12.44     ||  1.247     ||  1.323    ||  0.9640    ||  0.9503    ||   1.712     ||  1.305    ||   6.100     ||  1.079&lt;br /&gt;
|-&lt;br /&gt;
|90_30_55   || 16.14     ||  1.383     ||  1.475    ||  0.9571    ||  0.9504    ||   1.722     ||  1.296    ||   6.607     ||  2.158&lt;br /&gt;
|-&lt;br /&gt;
|90_40_58   || 17.45     ||  1.506     ||  1.597    ||  0.9499    ||  0.9501    ||   1.731     ||  1.287    ||   6.012     ||  2.629&lt;br /&gt;
|-&lt;br /&gt;
|90_50_62   || 18.70     ||  1.609     ||  1.706    ||  0.9438    ||  0.9501    ||   1.739     ||  1.279    ||   6.003     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|90_60_65   || 18.77     ||  1.703     ||  1.789    ||  0.9381    ||  0.9502    ||   1.747     ||  1.271    ||   5.045     ||  3.047&lt;br /&gt;
|-&lt;br /&gt;
|90_70_69   || 18.43     ||  1.787     ||  1.852    ||  0.9324    ||  0.9500    ||   1.754     ||  1.263    ||   3.623     ||  3.117&lt;br /&gt;
|-&lt;br /&gt;
|90_80_73   || 17.72     ||  1.868     ||  1.909    ||  0.9269    ||  0.9497    ||   1.762     ||  1.256    ||   2.217     ||  2.354&lt;br /&gt;
|-&lt;br /&gt;
|90_90_76   || 14.40     ||  1.940     ||  1.956    ||  0.9221    ||  0.9499    ||   1.769     ||  1.249    ||  0.8079     || 0.8326&lt;br /&gt;
|-&lt;br /&gt;
|90_100_80  || 18.53     ||  2.009     ||  2.038    ||  0.9176    ||  0.9503    ||   1.776     ||  1.242    ||   1.484     ||  1.095&lt;br /&gt;
|-&lt;br /&gt;
|90_110_84  || 18.97     ||  2.021     ||  2.094    ||  0.9129    ||  0.9502    ||   1.783     ||  1.235    ||   3.625     ||  3.669&lt;br /&gt;
|-&lt;br /&gt;
|90_120_88  || 17.79     ||  2.090     ||  2.129    ||  0.9077    ||  0.9494    ||   1.789     ||  1.229    ||   1.827     ||  3.862&lt;br /&gt;
|-&lt;br /&gt;
|100_00_50  || 10.07     || 0.9544     || 0.9970    ||  0.9732    ||  0.9499    ||   1.699     ||  1.319    ||   4.471     || 0.4341&lt;br /&gt;
|-&lt;br /&gt;
|100_10_53  || 12.78     ||  1.127     ||  1.186    ||  0.9649    ||  0.9499    ||   1.710     ||  1.308    ||   5.262     || 0.9629&lt;br /&gt;
|-&lt;br /&gt;
|100_16_55  || 13.69     ||  1.215     ||  1.287    ||  0.9610    ||  0.9501    ||   1.715     ||  1.302    ||   5.901     ||  1.023&lt;br /&gt;
|-&lt;br /&gt;
|100_20_56  || 10.86     ||  1.271     ||  1.324    ||  0.9583    ||  0.9502    ||   1.719     ||  1.299    ||   4.120     || 0.8295&lt;br /&gt;
|-&lt;br /&gt;
|100_22_56  || 15.40     ||  1.309     ||  1.381    ||  0.9412    ||  0.9362    ||   1.722     ||  1.296    ||   5.552     ||  1.648&lt;br /&gt;
|-&lt;br /&gt;
|100_24_58  || 15.90     ||  1.326     ||  1.406    ||  0.9552    ||  0.9499    ||   1.722     ||  1.295    ||   6.105     ||  1.792&lt;br /&gt;
|-&lt;br /&gt;
|100_26_58  || 16.42     ||  1.352     ||  1.435    ||  0.9538    ||  0.9499    ||   1.724     ||  1.293    ||   6.137     ||  1.888&lt;br /&gt;
|-&lt;br /&gt;
|100_28_59  || 17.07     ||  1.375     ||  1.464    ||  0.9527    ||  0.9501    ||   1.726     ||  1.291    ||   6.475     ||  1.983&lt;br /&gt;
|-&lt;br /&gt;
|100_30_59  || 17.29     ||  1.398     ||  1.490    ||  0.9511    ||  0.9500    ||   1.728     ||  1.289    ||   6.561     ||  2.075&lt;br /&gt;
|-&lt;br /&gt;
|100_32_60  || 17.74     ||  1.423     ||  1.517    ||  0.9499    ||  0.9499    ||   1.730     ||  1.288    ||   6.596     ||  2.165&lt;br /&gt;
|-&lt;br /&gt;
|100_36_61  || 18.37     ||  1.467     ||  1.567    ||  0.9475    ||  0.9501    ||   1.733     ||  1.284    ||   6.819     ||  2.183&lt;br /&gt;
|-&lt;br /&gt;
|100_40_63  || 18.77     ||  1.509     ||  1.608    ||  0.9450    ||  0.9500    ||   1.736     ||  1.281    ||   6.553     ||  2.304&lt;br /&gt;
|-&lt;br /&gt;
|100_44_64  || 19.25     ||  1.551     ||  1.653    ||  0.9426    ||  0.9500    ||   1.740     ||  1.278    ||   6.569     ||  2.360&lt;br /&gt;
|-&lt;br /&gt;
|100_48_65  || 19.16     ||  1.591     ||  1.684    ||  0.9400    ||  0.9500    ||   1.743     ||  1.275    ||   5.807     ||  2.555&lt;br /&gt;
|-&lt;br /&gt;
|100_50_65  || 19.11     ||  1.613     ||  1.704    ||  0.9381    ||  0.9501    ||   1.745     ||  1.274    ||   5.628     ||  2.649&lt;br /&gt;
|-&lt;br /&gt;
|100_55_67  || 19.04     ||  1.659     ||  1.739    ||  0.9352    ||  0.9500    ||   1.749     ||  1.270    ||   4.839     ||  2.808&lt;br /&gt;
|-&lt;br /&gt;
|100_56_67  || 18.93     ||  1.667     ||  1.742    ||  0.9347    ||  0.9501    ||   1.750     ||  1.269    ||   4.522     ||  2.692&lt;br /&gt;
|-&lt;br /&gt;
|100_60_68  || 19.04     ||  1.702     ||  1.775    ||  0.9325    ||  0.9500    ||   1.753     ||  1.266    ||   4.326     ||  2.720&lt;br /&gt;
|-&lt;br /&gt;
|100_64_70  || 18.76     ||  1.733     ||  1.799    ||  0.9303    ||  0.9500    ||   1.756     ||  1.263    ||   3.774     ||  2.676&lt;br /&gt;
|-&lt;br /&gt;
|100_68_72  || 18.46     ||  1.771     ||  1.825    ||  0.9279    ||  0.9494    ||   1.759     ||  1.259    ||   3.080     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_70_73  || 18.23     ||  1.784     ||  1.841    ||  0.9277    ||  0.9500    ||   1.760     ||  1.258    ||   3.166     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_80_77  || 16.73     ||  1.855     ||  1.885    ||  0.9261    ||  0.9532    ||   1.767     ||  1.251    ||   1.617     ||  1.818&lt;br /&gt;
|-&lt;br /&gt;
|100_90_80  || 13.86     ||  1.931     ||  1.936    ||  0.9172    ||  0.9494    ||   1.774     ||  1.244    ||  0.2833     || 0.7382&lt;br /&gt;
|-&lt;br /&gt;
|100_95_82  || 11.27     ||  1.967     ||  1.964    ||  0.9243    ||  0.9582    ||   1.777     ||  1.241    || -0.1435     || 6.8954E-02&lt;br /&gt;
|-&lt;br /&gt;
|100_105_86 || 16.96     ||  2.019     ||  2.045    ||  0.9233    ||  0.9617    ||   1.783     ||  1.235    ||   1.268     ||  1.425&lt;br /&gt;
|-&lt;br /&gt;
|100_110_88 || 18.88     ||  2.020     ||  2.073    ||  0.9229    ||  0.9634    ||   1.786     ||  1.232    ||   2.618     ||  2.366&lt;br /&gt;
|-&lt;br /&gt;
|100_120_92 || 17.63     ||  2.064     ||  2.113    ||  0.9044    ||  0.9501    ||   1.794     ||  1.224    ||   2.379     ||  3.790&lt;br /&gt;
|-&lt;br /&gt;
|110_00_54  || 11.70     ||  1.006     ||  1.060    ||  0.9663    ||  0.9498    ||   1.706     ||  1.312    ||   5.370     || 0.4642&lt;br /&gt;
|-&lt;br /&gt;
|110_10_57  || 13.97     ||  1.160     ||  1.232    ||  0.9593    ||  0.9502    ||   1.716     ||  1.301    ||   6.136     || 0.8247&lt;br /&gt;
|-&lt;br /&gt;
|110_20_60  || 15.75     ||  1.298     ||  1.372    ||  0.9526    ||  0.9504    ||   1.726     ||  1.292    ||   5.739     ||  1.330&lt;br /&gt;
|-&lt;br /&gt;
|110_30_63  || 18.56     ||  1.415     ||  1.516    ||  0.9455    ||  0.9500    ||   1.734     ||  1.284    ||   7.122     ||  1.849&lt;br /&gt;
|-&lt;br /&gt;
|110_40_66  || 19.50     ||  1.521     ||  1.622    ||  0.9398    ||  0.9503    ||   1.743     ||  1.275    ||   6.602     ||  1.921&lt;br /&gt;
|-&lt;br /&gt;
|110_50_70  || 19.07     ||  1.618     ||  1.696    ||  0.9336    ||  0.9498    ||   1.751     ||  1.267    ||   4.873     ||  2.085&lt;br /&gt;
|-&lt;br /&gt;
|110_60_73  || 18.32     ||  1.702     ||  1.761    ||  0.9291    ||  0.9507    ||   1.758     ||  1.260    ||   3.471     ||  2.033&lt;br /&gt;
|-&lt;br /&gt;
|110_70_77  || 17.13     ||  1.782     ||  1.816    ||  0.9237    ||  0.9504    ||   1.766     ||  1.252    ||   1.948     ||  1.838&lt;br /&gt;
|-&lt;br /&gt;
|110_80_81  || 15.56     ||  1.853     ||  1.871    ||  0.9192    ||  0.9508    ||   1.773     ||  1.245    ||  0.9878     ||  1.332&lt;br /&gt;
|-&lt;br /&gt;
|110_90_84  || 13.12     ||  1.923     ||  1.926    ||  0.9142    ||  0.9506    ||   1.780     ||  1.238    ||  0.1639     || 0.5301&lt;br /&gt;
|-&lt;br /&gt;
|110_95_86  || 10.73     ||  1.963     ||  1.955    ||  0.9095    ||  0.9486    ||   1.783     ||  1.235    || -0.3746     || 8.1449E-04&lt;br /&gt;
|-&lt;br /&gt;
|110_110_92 || 17.29     ||  2.020     ||  2.055    ||  0.9056    ||  0.9509    ||   1.793     ||  1.225    ||   1.768     ||  2.045&lt;br /&gt;
|-&lt;br /&gt;
|110_120_95 || 17.55     ||  2.048     ||  2.095    ||  0.9014    ||  0.9510    ||   1.799     ||  1.219    ||   2.314     ||  3.774&lt;br /&gt;
|-&lt;br /&gt;
|120_00_57  || 13.14     ||  1.050     ||  1.117    ||  0.9599    ||  0.9497    ||   1.714     ||  1.305    ||   6.304     || 0.4861&lt;br /&gt;
|-&lt;br /&gt;
|120_10_60  || 14.81     ||  1.196     ||  1.268    ||  0.9534    ||  0.9501    ||   1.723     ||  1.295    ||   6.054     || 0.8382&lt;br /&gt;
|-&lt;br /&gt;
|120_20_63  || 17.57     ||  1.323     ||  1.409    ||  0.9458    ||  0.9494    ||   1.732     ||  1.286    ||   6.504     ||  1.409&lt;br /&gt;
|-&lt;br /&gt;
|120_30_67  || 19.50     ||  1.435     ||  1.539    ||  0.9407    ||  0.9503    ||   1.741     ||  1.277    ||   7.263     ||  1.529&lt;br /&gt;
|-&lt;br /&gt;
|120_40_70  || 19.38     ||  1.534     ||  1.621    ||  0.9335    ||  0.9492    ||   1.749     ||  1.269    ||   5.695     ||  1.632&lt;br /&gt;
|-&lt;br /&gt;
|120_50_74  || 18.34     ||  1.621     ||  1.684    ||  0.9294    ||  0.9503    ||   1.756     ||  1.262    ||   3.910     ||  1.864&lt;br /&gt;
|-&lt;br /&gt;
|120_60_77  || 17.24     ||  1.703     ||  1.743    ||  0.9246    ||  0.9507    ||   1.764     ||  1.254    ||   2.381     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|120_70_81  || 16.02     ||  1.780     ||  1.803    ||  0.9197    ||  0.9509    ||   1.771     ||  1.247    ||   1.312     ||  1.511&lt;br /&gt;
|-&lt;br /&gt;
|120_80_84  || 14.49     ||  1.850     ||  1.860    ||  0.9150    ||  0.9509    ||   1.778     ||  1.240    ||  0.5347     ||  1.076&lt;br /&gt;
|-&lt;br /&gt;
|120_90_88  || 12.18     ||  1.918     ||  1.918    ||  0.9096    ||  0.9501    ||   1.785     ||  1.233    || -4.1127E-02 || 0.3613&lt;br /&gt;
|-&lt;br /&gt;
|120_95_90  || 10.06     ||  1.957     ||  1.950    ||  0.9071    ||  0.9499    ||   1.788     ||  1.230    || -0.3241     ||  0.000&lt;br /&gt;
|-&lt;br /&gt;
|120_115_97 || 16.46     ||  2.020     ||  2.066    ||  0.8983    ||  0.9497    ||   1.801     ||  1.216    ||   2.258     ||  2.404&lt;br /&gt;
|-&lt;br /&gt;
|120_120_99 || 17.58     ||  2.008     ||  2.092    ||  0.8967    ||  0.9501    ||   1.804     ||  1.213    ||   4.186     ||  3.647&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Flexibility ==&lt;br /&gt;
&lt;br /&gt;
[[File:Flexibility TJ-II.png|300px|thumb|right|Flexibility diagram of TJ-II magnetic configurations. Several lines of constant rotational transform are highlighted and labelled with the corresponding edge &amp;lt;math&amp;gt;\iota/2\pi&amp;lt;/math&amp;gt;-value.]]&lt;br /&gt;
TJ-II has considerable configurational flexibility, as observed in the &#039;flexibility diagram&#039;&amp;lt;ref&amp;gt;E. Ascasíbar, T. Estrada, F. Castejón, A. López-Fraguas, I. Pastor, J. Sánchez, U. Stroth, J. Qin and TJ-II Team, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/45/4/009|Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276–284]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
Some of this flexibility space has been explored, as in the &#039;magnetic well scan&#039; experiments&amp;lt;ref&amp;gt;A. de Aguilera, F. Castejón, E. Ascasíbar, et al. &#039;&#039;Magnetic well scan and confinement in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/55/11/113014|Nucl. Fusion, 55(11):113014, 2015]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
More recently, the [[rotational transform]] in the plasma edge region was found to be of importance for [[H-mode|L-H]] confinement transitions&amp;lt;ref&amp;gt;B. P. van Milligen, T. Estrada, B. Carreras, L. García, and TJ-II Team. &#039;&#039;Importance of the rotational transform for L–H transitions in the TJ-II stellarator&#039;&#039;, [[doi:10.3390/plasma7020024|Plasma, 7(2):446–464, 2024]].&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8730</id>
		<title>TJ-II:Magnetic configuration</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8730"/>
		<updated>2026-10-08T09:12:12Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* Flexibility */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The magnetic configuration of [[TJ-II]] in vacuum is completely determined by the currents flowing through the [[TJ-II:Coil system|external coils]].&lt;br /&gt;
Magnetic configurations are labelled as &#039;xxx_yy_zz&#039;, where&lt;br /&gt;
* &#039;xxx&#039;: 10 times the current (in kA) in the circular coil&lt;br /&gt;
* &#039;yy&#039;: 10 times the current (in kA) in the helical coil&lt;br /&gt;
* &#039;zz&#039;: 10 times the current (in kA) in the vertical field coils&lt;br /&gt;
The current in the toroidal field coils is not specified, as its value is adjusted to guarantee central absorption of the [[TJ-II:Electron Cyclotron Resonant Heating|Electron Cyclotron Resonant Heating]] source (requiring a specific &#039;resonant&#039; value of the magnetic field at the magnetic axis, &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
Configuration list:&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;width: 100%&amp;quot; border=&amp;quot;1&amp;quot;||&lt;br /&gt;
|-&lt;br /&gt;
! Configuration &lt;br /&gt;
! &amp;lt;math&amp;gt;r_{av}&amp;lt;/math&amp;gt; (cm) &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(0)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(a)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{m,av}&amp;lt;/math&amp;gt;(T) &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt; (T) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(0^\circ)&amp;lt;/math&amp;gt; (m) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(45^\circ)&amp;lt;/math&amp;gt; (m) &lt;br /&gt;
! Shear (%) &lt;br /&gt;
! Well (%)&lt;br /&gt;
|-&lt;br /&gt;
|0_20_13    ||1.139      || 1.185      || 1.194     ||  1.033     || 0.9504     ||  1.644      || 1.374     || 0.7793      ||5.7521E-02&lt;br /&gt;
|-&lt;br /&gt;
|0_30_15    ||4.228      || 1.518      || 1.698     ||  1.019     || 0.9500     ||  1.658      || 1.360     ||  11.85      || 1.050&lt;br /&gt;
|-&lt;br /&gt;
|0_40_18    ||5.903      || 1.756      || 2.003     ||  1.008     || 0.9505     ||  1.671      || 1.347     ||  14.09      || 1.217&lt;br /&gt;
|-&lt;br /&gt;
|0_50_22    ||6.480      || 1.936      || 2.230     || 0.9973     || 0.9502     ||  1.682      || 1.336     ||  15.17      || 2.481&lt;br /&gt;
|-&lt;br /&gt;
|0_60_26    ||8.500      || 2.073      || 2.399     || 0.9885     || 0.9502     ||  1.692      || 1.326     ||  15.70      || 3.218&lt;br /&gt;
|-&lt;br /&gt;
|0_70_29    ||7.147      || 2.187      || 2.434     || 0.9805     || 0.9503     ||  1.701      || 1.317     ||  11.30      || 2.985&lt;br /&gt;
|-&lt;br /&gt;
|0_80_34    ||6.902      || 2.284      || 2.469     || 0.9736     || 0.9506     ||  1.710      || 1.308     ||  8.084      || 2.735&lt;br /&gt;
|-&lt;br /&gt;
|0_90_38    ||6.738      || 2.366      || 2.514     || 0.9663     || 0.9503     ||  1.719      || 1.299     ||  6.269      || 2.534&lt;br /&gt;
|-&lt;br /&gt;
|0_100_42   ||12.59      || 2.436      || 2.667     || 0.9601     || 0.9505     ||  1.727      || 1.291     ||  9.493      || 4.643&lt;br /&gt;
|-&lt;br /&gt;
|0_110_46   ||10.67      || 2.493      || 2.667     || 0.9539     || 0.9503     ||  1.734      || 1.284     ||  6.980      || 4.554&lt;br /&gt;
|-&lt;br /&gt;
|0_120_50   ||12.71      || 2.548      || 2.667     || 0.9482     || 0.9504     ||  1.742      || 1.276     ||  4.683      || 4.272&lt;br /&gt;
|-&lt;br /&gt;
|10_20_18   || 2.557     ||  1.148     ||  1.184    ||   1.024    ||  0.9514    ||   1.652     ||  1.366    ||   3.183     || 0.2469&lt;br /&gt;
|-&lt;br /&gt;
|10_30_20   || 6.083     ||  1.438     ||  1.602    ||   1.010    ||  0.9501    ||   1.666     ||  1.352    ||   11.35     ||  1.398&lt;br /&gt;
|-&lt;br /&gt;
|10_40_24   || 6.921     ||  1.659     ||  1.880    ||   1.000    ||  0.9504    ||   1.678     ||  1.340    ||   13.34     ||  2.751&lt;br /&gt;
|-&lt;br /&gt;
|10_50_27   || 8.140     ||  1.826     ||  1.997    ||  0.9909    ||  0.9504    ||   1.688     ||  1.329    ||   9.321     ||  3.241&lt;br /&gt;
|-&lt;br /&gt;
|10_60_31   || 9.350     ||  1.965     ||  2.183    ||  0.9826    ||  0.9505    ||   1.698     ||  1.319    ||   11.11     ||  3.084&lt;br /&gt;
|-&lt;br /&gt;
|10_70_35   || 10.10     ||  2.077     ||  2.288    ||  0.9750    ||  0.9505    ||   1.707     ||  1.310    ||   10.16     ||  3.597&lt;br /&gt;
|-&lt;br /&gt;
|10_80_38   || 9.810     ||  2.174     ||  2.371    ||  0.9674    ||  0.9502    ||   1.716     ||  1.302    ||   9.037     ||  3.908&lt;br /&gt;
|-&lt;br /&gt;
|10_90_42   || 10.54     ||  2.257     ||  2.434    ||  0.9610    ||  0.9503    ||   1.724     ||  1.294    ||   7.851     ||  4.281&lt;br /&gt;
|-&lt;br /&gt;
|10_100_47  || 10.21     ||  2.327     ||  2.482    ||  0.9546    ||  0.9502    ||   1.732     ||  1.286    ||   6.647     ||  4.236&lt;br /&gt;
|-&lt;br /&gt;
|10_110_51  || 11.11     ||  2.395     ||  2.547    ||  0.9488    ||  0.9501    ||   1.740     ||  1.278    ||   6.331     ||  5.121&lt;br /&gt;
|-&lt;br /&gt;
|10_120_55  || 10.04     ||  2.451     ||  2.565    ||  0.9432    ||  0.9502    ||   1.747     ||  1.271    ||   4.674     ||  4.426&lt;br /&gt;
|-&lt;br /&gt;
|20_10_21   || 1.213     || 0.7902     || 0.7956    ||   1.028    ||  0.9503    ||   1.645     ||  1.373    ||  0.6830     || 3.7624E-02&lt;br /&gt;
|-&lt;br /&gt;
|20_20_22   || 3.952     ||  1.136     ||  1.185    ||   1.014    ||  0.9500    ||   1.661     ||  1.357    ||   4.350     || 0.4717&lt;br /&gt;
|-&lt;br /&gt;
|20_30_25   || 6.779     ||  1.395     ||  1.521    ||   1.003    ||  0.9502    ||   1.673     ||  1.344    ||   9.049     ||  1.550&lt;br /&gt;
|-&lt;br /&gt;
|20_40_28   || 8.475     ||  1.592     ||  1.771    ||  0.9922    ||  0.9498    ||   1.685     ||  1.333    ||   11.25     ||  2.879&lt;br /&gt;
|-&lt;br /&gt;
|20_50_32   || 8.039     ||  1.756     ||  1.906    ||  0.9842    ||  0.9505    ||   1.695     ||  1.323    ||   8.571     ||  3.131&lt;br /&gt;
|-&lt;br /&gt;
|20_60_35   || 11.21     ||  1.884     ||  1.997    ||  0.9755    ||  0.9498    ||   1.705     ||  1.313    ||   5.968     ||  1.980&lt;br /&gt;
|-&lt;br /&gt;
|20_70_39   || 11.08     ||  1.994     ||  2.154    ||  0.9689    ||  0.9504    ||   1.714     ||  1.304    ||   7.982     ||  3.385&lt;br /&gt;
|-&lt;br /&gt;
|20_80_43   || 12.14     ||  2.092     ||  2.255    ||  0.9614    ||  0.9497    ||   1.722     ||  1.296    ||   7.811     ||  4.133&lt;br /&gt;
|-&lt;br /&gt;
|20_90_47   || 12.83     ||  2.174     ||  2.324    ||  0.9558    ||  0.9503    ||   1.730     ||  1.288    ||   6.862     ||  4.713&lt;br /&gt;
|-&lt;br /&gt;
|20_100_51  || 12.68     ||  2.246     ||  2.379    ||  0.9498    ||  0.9503    ||   1.738     ||  1.280    ||   5.945     ||  4.930&lt;br /&gt;
|-&lt;br /&gt;
|20_110_55  || 13.79     ||  2.313     ||  2.434    ||  0.9443    ||  0.9505    ||   1.745     ||  1.273    ||   5.248     ||  5.117&lt;br /&gt;
|-&lt;br /&gt;
|20_120_59  || 13.91     ||  2.368     ||  2.483    ||  0.9386    ||  0.9502    ||   1.752     ||  1.265    ||   4.822     ||  5.418&lt;br /&gt;
|-&lt;br /&gt;
|30_10_25   || 2.709     || 0.8385     || 0.8507    ||   1.018    ||  0.9501    ||   1.654     ||  1.363    ||   1.452     || 0.1431&lt;br /&gt;
|-&lt;br /&gt;
|30_20_27   || 5.443     ||  1.134     ||  1.189    ||   1.007    ||  0.9514    ||   1.669     ||  1.349    ||   4.847     || 0.7001&lt;br /&gt;
|-&lt;br /&gt;
|30_30_30   || 8.180     ||  1.368     ||  1.481    ||  0.9956    ||  0.9506    ||   1.681     ||  1.337    ||   8.332     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|30_40_33   || 9.756     ||  1.550     ||  1.687    ||  0.9860    ||  0.9503    ||   1.692     ||  1.326    ||   8.877     ||  2.798&lt;br /&gt;
|-&lt;br /&gt;
|30_50_37   || 11.16     ||  1.702     ||  1.878    ||  0.9779    ||  0.9503    ||   1.702     ||  1.316    ||   10.37     ||  4.941&lt;br /&gt;
|-&lt;br /&gt;
|30_60_40   || 9.262     ||  1.827     ||  1.936    ||  0.9706    ||  0.9505    ||   1.711     ||  1.307    ||   5.952     ||  3.624&lt;br /&gt;
|-&lt;br /&gt;
|30_70_44   || 12.28     ||  1.937     ||  2.007    ||  0.9631    ||  0.9502    ||   1.720     ||  1.298    ||   3.593     ||  4.431&lt;br /&gt;
|-&lt;br /&gt;
|30_80_48   || 13.28     ||  2.033     ||  2.149    ||  0.9567    ||  0.9502    ||   1.728     ||  1.290    ||   5.702     ||  3.674&lt;br /&gt;
|-&lt;br /&gt;
|30_90_52   || 14.16     ||  2.115     ||  2.231    ||  0.9504    ||  0.9501    ||   1.736     ||  1.282    ||   5.476     ||  4.227&lt;br /&gt;
|-&lt;br /&gt;
|30_100_56  || 14.97     ||  2.187     ||  2.295    ||  0.9448    ||  0.9502    ||   1.743     ||  1.275    ||   4.949     ||  4.755&lt;br /&gt;
|-&lt;br /&gt;
|30_110_59  || 15.76     ||  2.246     ||  2.356    ||  0.9391    ||  0.9500    ||   1.751     ||  1.267    ||   4.920     ||  5.215&lt;br /&gt;
|-&lt;br /&gt;
|30_120_63  || 14.48     ||  2.306     ||  2.389    ||  0.9343    ||  0.9504    ||   1.758     ||  1.260    ||   3.573     ||  5.025&lt;br /&gt;
|-&lt;br /&gt;
|40_00_27   || 1.350     || 0.5464     || 0.5471    ||   1.024    ||  0.9504    ||   1.647     ||  1.371    ||  0.1331     || 2.4768E-02&lt;br /&gt;
|-&lt;br /&gt;
|40_10_29   || 4.111     || 0.8821     || 0.9010    ||   1.010    ||  0.9510    ||   1.663     ||  1.355    ||   2.152     || 0.2456&lt;br /&gt;
|-&lt;br /&gt;
|40_20_31   || 6.646     ||  1.146     ||  1.202    ||  0.9975    ||  0.9501    ||   1.677     ||  1.341    ||   4.928     || 0.8185&lt;br /&gt;
|-&lt;br /&gt;
|40_30_34   || 9.328     ||  1.354     ||  1.452    ||  0.9884    ||  0.9506    ||   1.688     ||  1.330    ||   7.247     ||  1.826&lt;br /&gt;
|-&lt;br /&gt;
|40_40_37   || 11.15     ||  1.523     ||  1.646    ||  0.9788    ||  0.9498    ||   1.699     ||  1.319    ||   8.061     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|40_50_41   || 12.66     ||  1.666     ||  1.797    ||  0.9719    ||  0.9506    ||   1.708     ||  1.310    ||   7.872     ||  4.310&lt;br /&gt;
|-&lt;br /&gt;
|40_60_44   || 12.34     ||  1.786     ||  1.927    ||  0.9637    ||  0.9497    ||   1.717     ||  1.301    ||   7.879     ||  5.834&lt;br /&gt;
|-&lt;br /&gt;
|40_70_48   || 9.734     ||  1.894     ||  1.963    ||  0.9579    ||  0.9504    ||   1.726     ||  1.292    ||   3.625     ||  3.668&lt;br /&gt;
|-&lt;br /&gt;
|40_80_52   || 13.96     ||  1.986     ||  2.067    ||  0.9515    ||  0.9503    ||   1.734     ||  1.284    ||   4.054     ||  3.028&lt;br /&gt;
|-&lt;br /&gt;
|40_90_56   || 15.39     ||  2.062     ||  2.156    ||  0.9457    ||  0.9504    ||   1.741     ||  1.277    ||   4.529     ||  3.841&lt;br /&gt;
|-&lt;br /&gt;
|40_100_60  || 16.40     ||  2.132     ||  2.232    ||  0.9400    ||  0.9502    ||   1.749     ||  1.269    ||   4.683     ||  4.355&lt;br /&gt;
|-&lt;br /&gt;
|40_110_64  || 18.12     ||  2.199     ||  2.288    ||  0.9348    ||  0.9503    ||   1.756     ||  1.262    ||   4.049     ||  4.651&lt;br /&gt;
|-&lt;br /&gt;
|40_120_68  || 16.81     ||  2.256     ||  2.327    ||  0.9295    ||  0.9501    ||   1.763     ||  1.255    ||   3.158     ||  4.904&lt;br /&gt;
|-&lt;br /&gt;
|50_00_31   || 2.818     || 0.6329     || 0.6375    ||   1.013    ||  0.9498    ||   1.657     ||  1.361    ||  0.7286     || 6.1871E-02&lt;br /&gt;
|-&lt;br /&gt;
|50_10_33   || 5.588     || 0.9254     || 0.9532    ||   1.001    ||  0.9506    ||   1.672     ||  1.346    ||   3.003     || 0.3605&lt;br /&gt;
|-&lt;br /&gt;
|50_20_36   || 8.222     ||  1.160     ||  1.216    ||  0.9902    ||  0.9502    ||   1.684     ||  1.334    ||   4.838     ||  1.060&lt;br /&gt;
|-&lt;br /&gt;
|50_30_39   || 10.67     ||  1.352     ||  1.435    ||  0.9815    ||  0.9505    ||   1.695     ||  1.323    ||   6.163     ||  2.008&lt;br /&gt;
|-&lt;br /&gt;
|50_40_42   || 12.44     ||  1.508     ||  1.609    ||  0.9733    ||  0.9504    ||   1.705     ||  1.313    ||   6.719     ||  2.910&lt;br /&gt;
|-&lt;br /&gt;
|50_50_46   || 13.94     ||  1.644     ||  1.758    ||  0.9661    ||  0.9505    ||   1.714     ||  1.303    ||   6.944     ||  4.001&lt;br /&gt;
|-&lt;br /&gt;
|50_60_49   || 15.09     ||  1.757     ||  1.887    ||  0.9587    ||  0.9502    ||   1.723     ||  1.295    ||   7.390     ||  6.217&lt;br /&gt;
|-&lt;br /&gt;
|50_70_53   || 13.03     ||  1.855     ||  1.955    ||  0.9524    ||  0.9502    ||   1.731     ||  1.287    ||   5.353     ||  5.830&lt;br /&gt;
|-&lt;br /&gt;
|50_80_56   || 16.73     ||  1.949     ||  2.004    ||  0.9463    ||  0.9501    ||   1.739     ||  1.279    ||   2.807     ||  4.003&lt;br /&gt;
|-&lt;br /&gt;
|50_90_60   || 16.70     ||  2.011     ||  2.101    ||  0.9407    ||  0.9502    ||   1.747     ||  1.271    ||   4.501     ||  3.444&lt;br /&gt;
|-&lt;br /&gt;
|50_100_64  || 18.15     ||  2.090     ||  2.183    ||  0.9351    ||  0.9500    ||   1.754     ||  1.264    ||   4.434     ||  3.907&lt;br /&gt;
|-&lt;br /&gt;
|50_110_68  || 17.53     ||  2.154     ||  2.223    ||  0.9297    ||  0.9498    ||   1.762     ||  1.256    ||   3.205     ||  4.270&lt;br /&gt;
|-&lt;br /&gt;
|50_120_72  || 19.13     ||  2.213     ||  2.288    ||  0.9250    ||  0.9501    ||   1.768     ||  1.250    ||   3.417     ||  4.378&lt;br /&gt;
|-&lt;br /&gt;
|60_00_35   || 4.247     || 0.7126     || 0.7205    ||   1.003    ||  0.9498    ||   1.667     ||  1.352    ||   1.108     || 0.1270&lt;br /&gt;
|-&lt;br /&gt;
|60_10_37   || 6.862     || 0.9679     ||  1.002    ||  0.9934    ||  0.9509    ||   1.680     ||  1.338    ||   3.520     || 0.4827&lt;br /&gt;
|-&lt;br /&gt;
|60_20_40   || 9.669     ||  1.179     ||  1.240    ||  0.9831    ||  0.9503    ||   1.692     ||  1.326    ||   5.202     ||  1.236&lt;br /&gt;
|-&lt;br /&gt;
|60_30_43   || 12.01     ||  1.354     ||  1.435    ||  0.9747    ||  0.9502    ||   1.702     ||  1.316    ||   5.973     ||  2.132&lt;br /&gt;
|-&lt;br /&gt;
|60_40_46   || 13.48     ||  1.500     ||  1.593    ||  0.9672    ||  0.9503    ||   1.712     ||  1.306    ||   6.170     ||  2.806&lt;br /&gt;
|-&lt;br /&gt;
|60_50_50   || 15.36     ||  1.627     ||  1.732    ||  0.9601    ||  0.9504    ||   1.721     ||  1.297    ||   6.467     ||  3.895&lt;br /&gt;
|-&lt;br /&gt;
|60_60_53   || 16.79     ||  1.734     ||  1.851    ||  0.9528    ||  0.9499    ||   1.729     ||  1.289    ||   6.731     ||  5.666&lt;br /&gt;
|-&lt;br /&gt;
|60_70_57   || 15.88     ||  1.829     ||  1.934    ||  0.9473    ||  0.9502    ||   1.737     ||  1.281    ||   5.736     ||  6.958&lt;br /&gt;
|-&lt;br /&gt;
|60_80_61   || 13.66     ||  1.918     ||  1.968    ||  0.9428    ||  0.9514    ||   1.745     ||  1.273    ||   2.622     ||  4.555&lt;br /&gt;
|-&lt;br /&gt;
|60_90_64   || 17.29     ||  2.009     ||  2.063    ||  0.9359    ||  0.9501    ||   1.753     ||  1.265    ||   2.640     ||  1.637&lt;br /&gt;
|-&lt;br /&gt;
|60_100_68  || 17.62     ||  2.049     ||  2.122    ||  0.9304    ||  0.9497    ||   1.760     ||  1.258    ||   3.560     ||  3.718&lt;br /&gt;
|-&lt;br /&gt;
|60_110_72  || 17.50     ||  2.118     ||  2.177    ||  0.9257    ||  0.9501    ||   1.767     ||  1.251    ||   2.811     ||  4.023&lt;br /&gt;
|-&lt;br /&gt;
|60_120_76  || 17.78     ||  2.174     ||  2.222    ||  0.9217    ||  0.9510    ||   1.774     ||  1.244    ||   2.209     ||  4.211&lt;br /&gt;
|-&lt;br /&gt;
|70_00_39   || 5.731     || 0.7825     || 0.7975    ||  0.9949    ||  0.9497    ||   1.675     ||  1.343    ||   1.908     || 0.2335&lt;br /&gt;
|-&lt;br /&gt;
|70_10_41   || 8.418     ||  1.009     ||  1.048    ||  0.9860    ||  0.9509    ||   1.688     ||  1.330    ||   3.845     || 0.6755&lt;br /&gt;
|-&lt;br /&gt;
|70_20_44   || 11.09     ||  1.201     ||  1.265    ||  0.9767    ||  0.9504    ||   1.699     ||  1.319    ||   5.345     ||  1.317&lt;br /&gt;
|-&lt;br /&gt;
|70_30_47   || 13.41     ||  1.361     ||  1.441    ||  0.9688    ||  0.9504    ||   1.709     ||  1.309    ||   5.859     ||  2.187&lt;br /&gt;
|-&lt;br /&gt;
|70_40_51   || 14.99     ||  1.496     ||  1.591    ||  0.9615    ||  0.9503    ||   1.718     ||  1.300    ||   6.348     ||  2.859&lt;br /&gt;
|-&lt;br /&gt;
|70_50_54   || 16.87     ||  1.617     ||  1.712    ||  0.9543    ||  0.9501    ||   1.727     ||  1.291    ||   5.843     ||  3.756&lt;br /&gt;
|-&lt;br /&gt;
|70_60_57   || 17.89     ||  1.718     ||  1.823    ||  0.9479    ||  0.9500    ||   1.735     ||  1.283    ||   6.140     ||  4.746&lt;br /&gt;
|-&lt;br /&gt;
|70_70_61   || 18.26     ||  1.812     ||  1.928    ||  0.9423    ||  0.9503    ||   1.743     ||  1.275    ||   6.353     ||  6.812&lt;br /&gt;
|-&lt;br /&gt;
|70_80_65   || 16.37     ||  1.896     ||  1.962    ||  0.9363    ||  0.9499    ||   1.751     ||  1.267    ||   3.469     ||  5.948&lt;br /&gt;
|-&lt;br /&gt;
|70_90_68   || 9.135     ||  1.980     ||  1.988    ||  0.9317    ||  0.9506    ||   1.758     ||  1.260    ||  0.3692     || 0.1186&lt;br /&gt;
|-&lt;br /&gt;
|70_100_72  || 18.64     ||  2.007     ||  2.094    ||  0.9267    ||  0.9506    ||   1.765     ||  1.253    ||   4.327     ||  3.356&lt;br /&gt;
|-&lt;br /&gt;
|70_110_76  || 18.23     ||  2.088     ||  2.147    ||  0.9219    ||  0.9507    ||   1.772     ||  1.246    ||   2.792     ||  3.707&lt;br /&gt;
|-&lt;br /&gt;
|70_120_80  || 17.89     ||  2.145     ||  2.184    ||  0.9171    ||  0.9506    ||   1.779     ||  1.239    ||   1.846     ||  4.043&lt;br /&gt;
|-&lt;br /&gt;
|80_00_42   ||7.247      ||0.8436      ||0.8697     || 0.9869     || 0.9497     ||  1.684      || 1.335     ||  3.094      ||0.2402&lt;br /&gt;
|-&lt;br /&gt;
|80_10_45   ||9.865      || 1.049      || 1.095     || 0.9794     || 0.9513     ||  1.695      || 1.323     ||  4.371      ||0.7359&lt;br /&gt;
|-&lt;br /&gt;
|80_20_48   ||12.28      || 1.226      || 1.290     || 0.9697     || 0.9500     ||  1.706      || 1.312     ||  5.206      || 1.327&lt;br /&gt;
|-&lt;br /&gt;
|80_30_51   ||14.38      || 1.370      || 1.454     || 0.9626     || 0.9503     ||  1.715      || 1.303     ||  6.088      || 2.102&lt;br /&gt;
|-&lt;br /&gt;
|80_40_54   ||16.47      || 1.500      || 1.594     || 0.9549     || 0.9497     ||  1.724      || 1.294     ||  6.263      || 2.799&lt;br /&gt;
|-&lt;br /&gt;
|80_50_58   ||17.63      || 1.612      || 1.706     || 0.9492     || 0.9503     ||  1.733      || 1.285     ||  5.842      || 3.329&lt;br /&gt;
|-&lt;br /&gt;
|80_60_61   ||18.84      || 1.712      || 1.814     || 0.9436     || 0.9507     ||  1.741      || 1.277     ||  5.984      || 3.990&lt;br /&gt;
|-&lt;br /&gt;
|80_70_65   ||19.27      || 1.799      || 1.898     || 0.9372     || 0.9501     ||  1.749      || 1.269     ||  5.555      || 4.728&lt;br /&gt;
|-&lt;br /&gt;
|80_80_69   ||17.96      || 1.880      || 1.935     || 0.9321     || 0.9503     ||  1.756      || 1.262     ||  2.921      || 3.774&lt;br /&gt;
|-&lt;br /&gt;
|80_90_73   ||13.42      || 1.957      || 1.982     || 0.9266     || 0.9500     ||  1.764      || 1.254     ||  1.312      ||0.6938&lt;br /&gt;
|-&lt;br /&gt;
|80_100_76  || 18.53     ||  2.008     ||  2.065    ||  0.9220    ||  0.9504    ||   1.770     ||  1.247    ||   2.839     ||  1.773&lt;br /&gt;
|-&lt;br /&gt;
|80_110_80  || 18.41     ||  2.059     ||  2.117    ||  0.9176    ||  0.9507    ||   1.777     ||  1.241    ||   2.847     ||  3.632&lt;br /&gt;
|-&lt;br /&gt;
|80_120_84  || 18.26     ||  2.117     ||  2.157    ||  0.9122    ||  0.9496    ||   1.784     ||  1.234    ||   1.872     ||  3.986&lt;br /&gt;
|-&lt;br /&gt;
|90_00_46   || 8.679     || 0.9022     || 0.9354    ||  0.9802    ||  0.9501    ||   1.691     ||  1.327    ||   3.678     || 0.3981&lt;br /&gt;
|-&lt;br /&gt;
|90_10_49   || 11.45     ||  1.090     ||  1.146    ||  0.9717    ||  0.9502    ||   1.702     ||  1.315    ||   5.148     || 0.8099&lt;br /&gt;
|-&lt;br /&gt;
|90_20_52   || 12.44     ||  1.247     ||  1.323    ||  0.9640    ||  0.9503    ||   1.712     ||  1.305    ||   6.100     ||  1.079&lt;br /&gt;
|-&lt;br /&gt;
|90_30_55   || 16.14     ||  1.383     ||  1.475    ||  0.9571    ||  0.9504    ||   1.722     ||  1.296    ||   6.607     ||  2.158&lt;br /&gt;
|-&lt;br /&gt;
|90_40_58   || 17.45     ||  1.506     ||  1.597    ||  0.9499    ||  0.9501    ||   1.731     ||  1.287    ||   6.012     ||  2.629&lt;br /&gt;
|-&lt;br /&gt;
|90_50_62   || 18.70     ||  1.609     ||  1.706    ||  0.9438    ||  0.9501    ||   1.739     ||  1.279    ||   6.003     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|90_60_65   || 18.77     ||  1.703     ||  1.789    ||  0.9381    ||  0.9502    ||   1.747     ||  1.271    ||   5.045     ||  3.047&lt;br /&gt;
|-&lt;br /&gt;
|90_70_69   || 18.43     ||  1.787     ||  1.852    ||  0.9324    ||  0.9500    ||   1.754     ||  1.263    ||   3.623     ||  3.117&lt;br /&gt;
|-&lt;br /&gt;
|90_80_73   || 17.72     ||  1.868     ||  1.909    ||  0.9269    ||  0.9497    ||   1.762     ||  1.256    ||   2.217     ||  2.354&lt;br /&gt;
|-&lt;br /&gt;
|90_90_76   || 14.40     ||  1.940     ||  1.956    ||  0.9221    ||  0.9499    ||   1.769     ||  1.249    ||  0.8079     || 0.8326&lt;br /&gt;
|-&lt;br /&gt;
|90_100_80  || 18.53     ||  2.009     ||  2.038    ||  0.9176    ||  0.9503    ||   1.776     ||  1.242    ||   1.484     ||  1.095&lt;br /&gt;
|-&lt;br /&gt;
|90_110_84  || 18.97     ||  2.021     ||  2.094    ||  0.9129    ||  0.9502    ||   1.783     ||  1.235    ||   3.625     ||  3.669&lt;br /&gt;
|-&lt;br /&gt;
|90_120_88  || 17.79     ||  2.090     ||  2.129    ||  0.9077    ||  0.9494    ||   1.789     ||  1.229    ||   1.827     ||  3.862&lt;br /&gt;
|-&lt;br /&gt;
|100_00_50  || 10.07     || 0.9544     || 0.9970    ||  0.9732    ||  0.9499    ||   1.699     ||  1.319    ||   4.471     || 0.4341&lt;br /&gt;
|-&lt;br /&gt;
|100_10_53  || 12.78     ||  1.127     ||  1.186    ||  0.9649    ||  0.9499    ||   1.710     ||  1.308    ||   5.262     || 0.9629&lt;br /&gt;
|-&lt;br /&gt;
|100_16_55  || 13.69     ||  1.215     ||  1.287    ||  0.9610    ||  0.9501    ||   1.715     ||  1.302    ||   5.901     ||  1.023&lt;br /&gt;
|-&lt;br /&gt;
|100_20_56  || 10.86     ||  1.271     ||  1.324    ||  0.9583    ||  0.9502    ||   1.719     ||  1.299    ||   4.120     || 0.8295&lt;br /&gt;
|-&lt;br /&gt;
|100_22_56  || 15.40     ||  1.309     ||  1.381    ||  0.9412    ||  0.9362    ||   1.722     ||  1.296    ||   5.552     ||  1.648&lt;br /&gt;
|-&lt;br /&gt;
|100_24_58  || 15.90     ||  1.326     ||  1.406    ||  0.9552    ||  0.9499    ||   1.722     ||  1.295    ||   6.105     ||  1.792&lt;br /&gt;
|-&lt;br /&gt;
|100_26_58  || 16.42     ||  1.352     ||  1.435    ||  0.9538    ||  0.9499    ||   1.724     ||  1.293    ||   6.137     ||  1.888&lt;br /&gt;
|-&lt;br /&gt;
|100_28_59  || 17.07     ||  1.375     ||  1.464    ||  0.9527    ||  0.9501    ||   1.726     ||  1.291    ||   6.475     ||  1.983&lt;br /&gt;
|-&lt;br /&gt;
|100_30_59  || 17.29     ||  1.398     ||  1.490    ||  0.9511    ||  0.9500    ||   1.728     ||  1.289    ||   6.561     ||  2.075&lt;br /&gt;
|-&lt;br /&gt;
|100_32_60  || 17.74     ||  1.423     ||  1.517    ||  0.9499    ||  0.9499    ||   1.730     ||  1.288    ||   6.596     ||  2.165&lt;br /&gt;
|-&lt;br /&gt;
|100_36_61  || 18.37     ||  1.467     ||  1.567    ||  0.9475    ||  0.9501    ||   1.733     ||  1.284    ||   6.819     ||  2.183&lt;br /&gt;
|-&lt;br /&gt;
|100_40_63  || 18.77     ||  1.509     ||  1.608    ||  0.9450    ||  0.9500    ||   1.736     ||  1.281    ||   6.553     ||  2.304&lt;br /&gt;
|-&lt;br /&gt;
|100_44_64  || 19.25     ||  1.551     ||  1.653    ||  0.9426    ||  0.9500    ||   1.740     ||  1.278    ||   6.569     ||  2.360&lt;br /&gt;
|-&lt;br /&gt;
|100_48_65  || 19.16     ||  1.591     ||  1.684    ||  0.9400    ||  0.9500    ||   1.743     ||  1.275    ||   5.807     ||  2.555&lt;br /&gt;
|-&lt;br /&gt;
|100_50_65  || 19.11     ||  1.613     ||  1.704    ||  0.9381    ||  0.9501    ||   1.745     ||  1.274    ||   5.628     ||  2.649&lt;br /&gt;
|-&lt;br /&gt;
|100_55_67  || 19.04     ||  1.659     ||  1.739    ||  0.9352    ||  0.9500    ||   1.749     ||  1.270    ||   4.839     ||  2.808&lt;br /&gt;
|-&lt;br /&gt;
|100_56_67  || 18.93     ||  1.667     ||  1.742    ||  0.9347    ||  0.9501    ||   1.750     ||  1.269    ||   4.522     ||  2.692&lt;br /&gt;
|-&lt;br /&gt;
|100_60_68  || 19.04     ||  1.702     ||  1.775    ||  0.9325    ||  0.9500    ||   1.753     ||  1.266    ||   4.326     ||  2.720&lt;br /&gt;
|-&lt;br /&gt;
|100_64_70  || 18.76     ||  1.733     ||  1.799    ||  0.9303    ||  0.9500    ||   1.756     ||  1.263    ||   3.774     ||  2.676&lt;br /&gt;
|-&lt;br /&gt;
|100_68_72  || 18.46     ||  1.771     ||  1.825    ||  0.9279    ||  0.9494    ||   1.759     ||  1.259    ||   3.080     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_70_73  || 18.23     ||  1.784     ||  1.841    ||  0.9277    ||  0.9500    ||   1.760     ||  1.258    ||   3.166     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_80_77  || 16.73     ||  1.855     ||  1.885    ||  0.9261    ||  0.9532    ||   1.767     ||  1.251    ||   1.617     ||  1.818&lt;br /&gt;
|-&lt;br /&gt;
|100_90_80  || 13.86     ||  1.931     ||  1.936    ||  0.9172    ||  0.9494    ||   1.774     ||  1.244    ||  0.2833     || 0.7382&lt;br /&gt;
|-&lt;br /&gt;
|100_95_82  || 11.27     ||  1.967     ||  1.964    ||  0.9243    ||  0.9582    ||   1.777     ||  1.241    || -0.1435     || 6.8954E-02&lt;br /&gt;
|-&lt;br /&gt;
|100_105_86 || 16.96     ||  2.019     ||  2.045    ||  0.9233    ||  0.9617    ||   1.783     ||  1.235    ||   1.268     ||  1.425&lt;br /&gt;
|-&lt;br /&gt;
|100_110_88 || 18.88     ||  2.020     ||  2.073    ||  0.9229    ||  0.9634    ||   1.786     ||  1.232    ||   2.618     ||  2.366&lt;br /&gt;
|-&lt;br /&gt;
|100_120_92 || 17.63     ||  2.064     ||  2.113    ||  0.9044    ||  0.9501    ||   1.794     ||  1.224    ||   2.379     ||  3.790&lt;br /&gt;
|-&lt;br /&gt;
|110_00_54  || 11.70     ||  1.006     ||  1.060    ||  0.9663    ||  0.9498    ||   1.706     ||  1.312    ||   5.370     || 0.4642&lt;br /&gt;
|-&lt;br /&gt;
|110_10_57  || 13.97     ||  1.160     ||  1.232    ||  0.9593    ||  0.9502    ||   1.716     ||  1.301    ||   6.136     || 0.8247&lt;br /&gt;
|-&lt;br /&gt;
|110_20_60  || 15.75     ||  1.298     ||  1.372    ||  0.9526    ||  0.9504    ||   1.726     ||  1.292    ||   5.739     ||  1.330&lt;br /&gt;
|-&lt;br /&gt;
|110_30_63  || 18.56     ||  1.415     ||  1.516    ||  0.9455    ||  0.9500    ||   1.734     ||  1.284    ||   7.122     ||  1.849&lt;br /&gt;
|-&lt;br /&gt;
|110_40_66  || 19.50     ||  1.521     ||  1.622    ||  0.9398    ||  0.9503    ||   1.743     ||  1.275    ||   6.602     ||  1.921&lt;br /&gt;
|-&lt;br /&gt;
|110_50_70  || 19.07     ||  1.618     ||  1.696    ||  0.9336    ||  0.9498    ||   1.751     ||  1.267    ||   4.873     ||  2.085&lt;br /&gt;
|-&lt;br /&gt;
|110_60_73  || 18.32     ||  1.702     ||  1.761    ||  0.9291    ||  0.9507    ||   1.758     ||  1.260    ||   3.471     ||  2.033&lt;br /&gt;
|-&lt;br /&gt;
|110_70_77  || 17.13     ||  1.782     ||  1.816    ||  0.9237    ||  0.9504    ||   1.766     ||  1.252    ||   1.948     ||  1.838&lt;br /&gt;
|-&lt;br /&gt;
|110_80_81  || 15.56     ||  1.853     ||  1.871    ||  0.9192    ||  0.9508    ||   1.773     ||  1.245    ||  0.9878     ||  1.332&lt;br /&gt;
|-&lt;br /&gt;
|110_90_84  || 13.12     ||  1.923     ||  1.926    ||  0.9142    ||  0.9506    ||   1.780     ||  1.238    ||  0.1639     || 0.5301&lt;br /&gt;
|-&lt;br /&gt;
|110_95_86  || 10.73     ||  1.963     ||  1.955    ||  0.9095    ||  0.9486    ||   1.783     ||  1.235    || -0.3746     || 8.1449E-04&lt;br /&gt;
|-&lt;br /&gt;
|110_110_92 || 17.29     ||  2.020     ||  2.055    ||  0.9056    ||  0.9509    ||   1.793     ||  1.225    ||   1.768     ||  2.045&lt;br /&gt;
|-&lt;br /&gt;
|110_120_95 || 17.55     ||  2.048     ||  2.095    ||  0.9014    ||  0.9510    ||   1.799     ||  1.219    ||   2.314     ||  3.774&lt;br /&gt;
|-&lt;br /&gt;
|120_00_57  || 13.14     ||  1.050     ||  1.117    ||  0.9599    ||  0.9497    ||   1.714     ||  1.305    ||   6.304     || 0.4861&lt;br /&gt;
|-&lt;br /&gt;
|120_10_60  || 14.81     ||  1.196     ||  1.268    ||  0.9534    ||  0.9501    ||   1.723     ||  1.295    ||   6.054     || 0.8382&lt;br /&gt;
|-&lt;br /&gt;
|120_20_63  || 17.57     ||  1.323     ||  1.409    ||  0.9458    ||  0.9494    ||   1.732     ||  1.286    ||   6.504     ||  1.409&lt;br /&gt;
|-&lt;br /&gt;
|120_30_67  || 19.50     ||  1.435     ||  1.539    ||  0.9407    ||  0.9503    ||   1.741     ||  1.277    ||   7.263     ||  1.529&lt;br /&gt;
|-&lt;br /&gt;
|120_40_70  || 19.38     ||  1.534     ||  1.621    ||  0.9335    ||  0.9492    ||   1.749     ||  1.269    ||   5.695     ||  1.632&lt;br /&gt;
|-&lt;br /&gt;
|120_50_74  || 18.34     ||  1.621     ||  1.684    ||  0.9294    ||  0.9503    ||   1.756     ||  1.262    ||   3.910     ||  1.864&lt;br /&gt;
|-&lt;br /&gt;
|120_60_77  || 17.24     ||  1.703     ||  1.743    ||  0.9246    ||  0.9507    ||   1.764     ||  1.254    ||   2.381     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|120_70_81  || 16.02     ||  1.780     ||  1.803    ||  0.9197    ||  0.9509    ||   1.771     ||  1.247    ||   1.312     ||  1.511&lt;br /&gt;
|-&lt;br /&gt;
|120_80_84  || 14.49     ||  1.850     ||  1.860    ||  0.9150    ||  0.9509    ||   1.778     ||  1.240    ||  0.5347     ||  1.076&lt;br /&gt;
|-&lt;br /&gt;
|120_90_88  || 12.18     ||  1.918     ||  1.918    ||  0.9096    ||  0.9501    ||   1.785     ||  1.233    || -4.1127E-02 || 0.3613&lt;br /&gt;
|-&lt;br /&gt;
|120_95_90  || 10.06     ||  1.957     ||  1.950    ||  0.9071    ||  0.9499    ||   1.788     ||  1.230    || -0.3241     ||  0.000&lt;br /&gt;
|-&lt;br /&gt;
|120_115_97 || 16.46     ||  2.020     ||  2.066    ||  0.8983    ||  0.9497    ||   1.801     ||  1.216    ||   2.258     ||  2.404&lt;br /&gt;
|-&lt;br /&gt;
|120_120_99 || 17.58     ||  2.008     ||  2.092    ||  0.8967    ||  0.9501    ||   1.804     ||  1.213    ||   4.186     ||  3.647&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Flexibility ==&lt;br /&gt;
&lt;br /&gt;
[[File:Flexibility TJ-II.png|300px|thumb|right|Flexibility diagram of TJ-II magnetic configurations. Several lines of constant rotational transform are highlighted and labelled with the corresponding edge &amp;lt;math&amp;gt;\iota/2\pi&amp;lt;/math&amp;gt;-value.]]&lt;br /&gt;
TJ-II has considerable configurational flexibility, as observed in the &#039;flexibility diagram&#039;&amp;lt;ref&amp;gt;E. Ascasíbar, T. Estrada, F. Castejón, A. López-Fraguas, I. Pastor, J. Sánchez, U. Stroth, J. Qin and TJ-II Team, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/45/4/009|Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276–284]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
Some of this flexibility space has been explored, as in the &#039;magnetic well scan&#039; experiments&amp;lt;ref&amp;gt;A. de Aguilera, F. Castejón, E. Ascasíbar, et al. &#039;&#039;Magnetic well scan and confinement in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/55/11/113014|Nucl. Fusion, 55(11):113014, 2015]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
More recently, the rotational transform in the plasma edge region was found to be of importance for L-H confinement transitions&amp;lt;ref&amp;gt;B. P. van Milligen, T. Estrada, B. Carreras, L. García, and TJ-II Team. &#039;&#039;Importance of the rotational transform for L–H transitions in the TJ-II stellarator&#039;&#039;, [[doi:10.3390/plasma7020024|Plasma, 7(2):446–464, 2024]].&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=File:Flexibility_TJ-II.png&amp;diff=8729</id>
		<title>File:Flexibility TJ-II.png</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=File:Flexibility_TJ-II.png&amp;diff=8729"/>
		<updated>2026-10-08T09:11:34Z</updated>

		<summary type="html">&lt;p&gt;Admin: Admin uploaded a new version of File:Flexibility TJ-II.png&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8728</id>
		<title>TJ-II:Magnetic configuration</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8728"/>
		<updated>2026-10-07T16:29:20Z</updated>

		<summary type="html">&lt;p&gt;Admin: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The magnetic configuration of [[TJ-II]] in vacuum is completely determined by the currents flowing through the [[TJ-II:Coil system|external coils]].&lt;br /&gt;
Magnetic configurations are labelled as &#039;xxx_yy_zz&#039;, where&lt;br /&gt;
* &#039;xxx&#039;: 10 times the current (in kA) in the circular coil&lt;br /&gt;
* &#039;yy&#039;: 10 times the current (in kA) in the helical coil&lt;br /&gt;
* &#039;zz&#039;: 10 times the current (in kA) in the vertical field coils&lt;br /&gt;
The current in the toroidal field coils is not specified, as its value is adjusted to guarantee central absorption of the [[TJ-II:Electron Cyclotron Resonant Heating|Electron Cyclotron Resonant Heating]] source (requiring a specific &#039;resonant&#039; value of the magnetic field at the magnetic axis, &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
Configuration list:&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;width: 100%&amp;quot; border=&amp;quot;1&amp;quot;||&lt;br /&gt;
|-&lt;br /&gt;
! Configuration &lt;br /&gt;
! &amp;lt;math&amp;gt;r_{av}&amp;lt;/math&amp;gt; (cm) &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(0)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(a)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{m,av}&amp;lt;/math&amp;gt;(T) &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt; (T) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(0^\circ)&amp;lt;/math&amp;gt; (m) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(45^\circ)&amp;lt;/math&amp;gt; (m) &lt;br /&gt;
! Shear (%) &lt;br /&gt;
! Well (%)&lt;br /&gt;
|-&lt;br /&gt;
|0_20_13    ||1.139      || 1.185      || 1.194     ||  1.033     || 0.9504     ||  1.644      || 1.374     || 0.7793      ||5.7521E-02&lt;br /&gt;
|-&lt;br /&gt;
|0_30_15    ||4.228      || 1.518      || 1.698     ||  1.019     || 0.9500     ||  1.658      || 1.360     ||  11.85      || 1.050&lt;br /&gt;
|-&lt;br /&gt;
|0_40_18    ||5.903      || 1.756      || 2.003     ||  1.008     || 0.9505     ||  1.671      || 1.347     ||  14.09      || 1.217&lt;br /&gt;
|-&lt;br /&gt;
|0_50_22    ||6.480      || 1.936      || 2.230     || 0.9973     || 0.9502     ||  1.682      || 1.336     ||  15.17      || 2.481&lt;br /&gt;
|-&lt;br /&gt;
|0_60_26    ||8.500      || 2.073      || 2.399     || 0.9885     || 0.9502     ||  1.692      || 1.326     ||  15.70      || 3.218&lt;br /&gt;
|-&lt;br /&gt;
|0_70_29    ||7.147      || 2.187      || 2.434     || 0.9805     || 0.9503     ||  1.701      || 1.317     ||  11.30      || 2.985&lt;br /&gt;
|-&lt;br /&gt;
|0_80_34    ||6.902      || 2.284      || 2.469     || 0.9736     || 0.9506     ||  1.710      || 1.308     ||  8.084      || 2.735&lt;br /&gt;
|-&lt;br /&gt;
|0_90_38    ||6.738      || 2.366      || 2.514     || 0.9663     || 0.9503     ||  1.719      || 1.299     ||  6.269      || 2.534&lt;br /&gt;
|-&lt;br /&gt;
|0_100_42   ||12.59      || 2.436      || 2.667     || 0.9601     || 0.9505     ||  1.727      || 1.291     ||  9.493      || 4.643&lt;br /&gt;
|-&lt;br /&gt;
|0_110_46   ||10.67      || 2.493      || 2.667     || 0.9539     || 0.9503     ||  1.734      || 1.284     ||  6.980      || 4.554&lt;br /&gt;
|-&lt;br /&gt;
|0_120_50   ||12.71      || 2.548      || 2.667     || 0.9482     || 0.9504     ||  1.742      || 1.276     ||  4.683      || 4.272&lt;br /&gt;
|-&lt;br /&gt;
|10_20_18   || 2.557     ||  1.148     ||  1.184    ||   1.024    ||  0.9514    ||   1.652     ||  1.366    ||   3.183     || 0.2469&lt;br /&gt;
|-&lt;br /&gt;
|10_30_20   || 6.083     ||  1.438     ||  1.602    ||   1.010    ||  0.9501    ||   1.666     ||  1.352    ||   11.35     ||  1.398&lt;br /&gt;
|-&lt;br /&gt;
|10_40_24   || 6.921     ||  1.659     ||  1.880    ||   1.000    ||  0.9504    ||   1.678     ||  1.340    ||   13.34     ||  2.751&lt;br /&gt;
|-&lt;br /&gt;
|10_50_27   || 8.140     ||  1.826     ||  1.997    ||  0.9909    ||  0.9504    ||   1.688     ||  1.329    ||   9.321     ||  3.241&lt;br /&gt;
|-&lt;br /&gt;
|10_60_31   || 9.350     ||  1.965     ||  2.183    ||  0.9826    ||  0.9505    ||   1.698     ||  1.319    ||   11.11     ||  3.084&lt;br /&gt;
|-&lt;br /&gt;
|10_70_35   || 10.10     ||  2.077     ||  2.288    ||  0.9750    ||  0.9505    ||   1.707     ||  1.310    ||   10.16     ||  3.597&lt;br /&gt;
|-&lt;br /&gt;
|10_80_38   || 9.810     ||  2.174     ||  2.371    ||  0.9674    ||  0.9502    ||   1.716     ||  1.302    ||   9.037     ||  3.908&lt;br /&gt;
|-&lt;br /&gt;
|10_90_42   || 10.54     ||  2.257     ||  2.434    ||  0.9610    ||  0.9503    ||   1.724     ||  1.294    ||   7.851     ||  4.281&lt;br /&gt;
|-&lt;br /&gt;
|10_100_47  || 10.21     ||  2.327     ||  2.482    ||  0.9546    ||  0.9502    ||   1.732     ||  1.286    ||   6.647     ||  4.236&lt;br /&gt;
|-&lt;br /&gt;
|10_110_51  || 11.11     ||  2.395     ||  2.547    ||  0.9488    ||  0.9501    ||   1.740     ||  1.278    ||   6.331     ||  5.121&lt;br /&gt;
|-&lt;br /&gt;
|10_120_55  || 10.04     ||  2.451     ||  2.565    ||  0.9432    ||  0.9502    ||   1.747     ||  1.271    ||   4.674     ||  4.426&lt;br /&gt;
|-&lt;br /&gt;
|20_10_21   || 1.213     || 0.7902     || 0.7956    ||   1.028    ||  0.9503    ||   1.645     ||  1.373    ||  0.6830     || 3.7624E-02&lt;br /&gt;
|-&lt;br /&gt;
|20_20_22   || 3.952     ||  1.136     ||  1.185    ||   1.014    ||  0.9500    ||   1.661     ||  1.357    ||   4.350     || 0.4717&lt;br /&gt;
|-&lt;br /&gt;
|20_30_25   || 6.779     ||  1.395     ||  1.521    ||   1.003    ||  0.9502    ||   1.673     ||  1.344    ||   9.049     ||  1.550&lt;br /&gt;
|-&lt;br /&gt;
|20_40_28   || 8.475     ||  1.592     ||  1.771    ||  0.9922    ||  0.9498    ||   1.685     ||  1.333    ||   11.25     ||  2.879&lt;br /&gt;
|-&lt;br /&gt;
|20_50_32   || 8.039     ||  1.756     ||  1.906    ||  0.9842    ||  0.9505    ||   1.695     ||  1.323    ||   8.571     ||  3.131&lt;br /&gt;
|-&lt;br /&gt;
|20_60_35   || 11.21     ||  1.884     ||  1.997    ||  0.9755    ||  0.9498    ||   1.705     ||  1.313    ||   5.968     ||  1.980&lt;br /&gt;
|-&lt;br /&gt;
|20_70_39   || 11.08     ||  1.994     ||  2.154    ||  0.9689    ||  0.9504    ||   1.714     ||  1.304    ||   7.982     ||  3.385&lt;br /&gt;
|-&lt;br /&gt;
|20_80_43   || 12.14     ||  2.092     ||  2.255    ||  0.9614    ||  0.9497    ||   1.722     ||  1.296    ||   7.811     ||  4.133&lt;br /&gt;
|-&lt;br /&gt;
|20_90_47   || 12.83     ||  2.174     ||  2.324    ||  0.9558    ||  0.9503    ||   1.730     ||  1.288    ||   6.862     ||  4.713&lt;br /&gt;
|-&lt;br /&gt;
|20_100_51  || 12.68     ||  2.246     ||  2.379    ||  0.9498    ||  0.9503    ||   1.738     ||  1.280    ||   5.945     ||  4.930&lt;br /&gt;
|-&lt;br /&gt;
|20_110_55  || 13.79     ||  2.313     ||  2.434    ||  0.9443    ||  0.9505    ||   1.745     ||  1.273    ||   5.248     ||  5.117&lt;br /&gt;
|-&lt;br /&gt;
|20_120_59  || 13.91     ||  2.368     ||  2.483    ||  0.9386    ||  0.9502    ||   1.752     ||  1.265    ||   4.822     ||  5.418&lt;br /&gt;
|-&lt;br /&gt;
|30_10_25   || 2.709     || 0.8385     || 0.8507    ||   1.018    ||  0.9501    ||   1.654     ||  1.363    ||   1.452     || 0.1431&lt;br /&gt;
|-&lt;br /&gt;
|30_20_27   || 5.443     ||  1.134     ||  1.189    ||   1.007    ||  0.9514    ||   1.669     ||  1.349    ||   4.847     || 0.7001&lt;br /&gt;
|-&lt;br /&gt;
|30_30_30   || 8.180     ||  1.368     ||  1.481    ||  0.9956    ||  0.9506    ||   1.681     ||  1.337    ||   8.332     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|30_40_33   || 9.756     ||  1.550     ||  1.687    ||  0.9860    ||  0.9503    ||   1.692     ||  1.326    ||   8.877     ||  2.798&lt;br /&gt;
|-&lt;br /&gt;
|30_50_37   || 11.16     ||  1.702     ||  1.878    ||  0.9779    ||  0.9503    ||   1.702     ||  1.316    ||   10.37     ||  4.941&lt;br /&gt;
|-&lt;br /&gt;
|30_60_40   || 9.262     ||  1.827     ||  1.936    ||  0.9706    ||  0.9505    ||   1.711     ||  1.307    ||   5.952     ||  3.624&lt;br /&gt;
|-&lt;br /&gt;
|30_70_44   || 12.28     ||  1.937     ||  2.007    ||  0.9631    ||  0.9502    ||   1.720     ||  1.298    ||   3.593     ||  4.431&lt;br /&gt;
|-&lt;br /&gt;
|30_80_48   || 13.28     ||  2.033     ||  2.149    ||  0.9567    ||  0.9502    ||   1.728     ||  1.290    ||   5.702     ||  3.674&lt;br /&gt;
|-&lt;br /&gt;
|30_90_52   || 14.16     ||  2.115     ||  2.231    ||  0.9504    ||  0.9501    ||   1.736     ||  1.282    ||   5.476     ||  4.227&lt;br /&gt;
|-&lt;br /&gt;
|30_100_56  || 14.97     ||  2.187     ||  2.295    ||  0.9448    ||  0.9502    ||   1.743     ||  1.275    ||   4.949     ||  4.755&lt;br /&gt;
|-&lt;br /&gt;
|30_110_59  || 15.76     ||  2.246     ||  2.356    ||  0.9391    ||  0.9500    ||   1.751     ||  1.267    ||   4.920     ||  5.215&lt;br /&gt;
|-&lt;br /&gt;
|30_120_63  || 14.48     ||  2.306     ||  2.389    ||  0.9343    ||  0.9504    ||   1.758     ||  1.260    ||   3.573     ||  5.025&lt;br /&gt;
|-&lt;br /&gt;
|40_00_27   || 1.350     || 0.5464     || 0.5471    ||   1.024    ||  0.9504    ||   1.647     ||  1.371    ||  0.1331     || 2.4768E-02&lt;br /&gt;
|-&lt;br /&gt;
|40_10_29   || 4.111     || 0.8821     || 0.9010    ||   1.010    ||  0.9510    ||   1.663     ||  1.355    ||   2.152     || 0.2456&lt;br /&gt;
|-&lt;br /&gt;
|40_20_31   || 6.646     ||  1.146     ||  1.202    ||  0.9975    ||  0.9501    ||   1.677     ||  1.341    ||   4.928     || 0.8185&lt;br /&gt;
|-&lt;br /&gt;
|40_30_34   || 9.328     ||  1.354     ||  1.452    ||  0.9884    ||  0.9506    ||   1.688     ||  1.330    ||   7.247     ||  1.826&lt;br /&gt;
|-&lt;br /&gt;
|40_40_37   || 11.15     ||  1.523     ||  1.646    ||  0.9788    ||  0.9498    ||   1.699     ||  1.319    ||   8.061     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|40_50_41   || 12.66     ||  1.666     ||  1.797    ||  0.9719    ||  0.9506    ||   1.708     ||  1.310    ||   7.872     ||  4.310&lt;br /&gt;
|-&lt;br /&gt;
|40_60_44   || 12.34     ||  1.786     ||  1.927    ||  0.9637    ||  0.9497    ||   1.717     ||  1.301    ||   7.879     ||  5.834&lt;br /&gt;
|-&lt;br /&gt;
|40_70_48   || 9.734     ||  1.894     ||  1.963    ||  0.9579    ||  0.9504    ||   1.726     ||  1.292    ||   3.625     ||  3.668&lt;br /&gt;
|-&lt;br /&gt;
|40_80_52   || 13.96     ||  1.986     ||  2.067    ||  0.9515    ||  0.9503    ||   1.734     ||  1.284    ||   4.054     ||  3.028&lt;br /&gt;
|-&lt;br /&gt;
|40_90_56   || 15.39     ||  2.062     ||  2.156    ||  0.9457    ||  0.9504    ||   1.741     ||  1.277    ||   4.529     ||  3.841&lt;br /&gt;
|-&lt;br /&gt;
|40_100_60  || 16.40     ||  2.132     ||  2.232    ||  0.9400    ||  0.9502    ||   1.749     ||  1.269    ||   4.683     ||  4.355&lt;br /&gt;
|-&lt;br /&gt;
|40_110_64  || 18.12     ||  2.199     ||  2.288    ||  0.9348    ||  0.9503    ||   1.756     ||  1.262    ||   4.049     ||  4.651&lt;br /&gt;
|-&lt;br /&gt;
|40_120_68  || 16.81     ||  2.256     ||  2.327    ||  0.9295    ||  0.9501    ||   1.763     ||  1.255    ||   3.158     ||  4.904&lt;br /&gt;
|-&lt;br /&gt;
|50_00_31   || 2.818     || 0.6329     || 0.6375    ||   1.013    ||  0.9498    ||   1.657     ||  1.361    ||  0.7286     || 6.1871E-02&lt;br /&gt;
|-&lt;br /&gt;
|50_10_33   || 5.588     || 0.9254     || 0.9532    ||   1.001    ||  0.9506    ||   1.672     ||  1.346    ||   3.003     || 0.3605&lt;br /&gt;
|-&lt;br /&gt;
|50_20_36   || 8.222     ||  1.160     ||  1.216    ||  0.9902    ||  0.9502    ||   1.684     ||  1.334    ||   4.838     ||  1.060&lt;br /&gt;
|-&lt;br /&gt;
|50_30_39   || 10.67     ||  1.352     ||  1.435    ||  0.9815    ||  0.9505    ||   1.695     ||  1.323    ||   6.163     ||  2.008&lt;br /&gt;
|-&lt;br /&gt;
|50_40_42   || 12.44     ||  1.508     ||  1.609    ||  0.9733    ||  0.9504    ||   1.705     ||  1.313    ||   6.719     ||  2.910&lt;br /&gt;
|-&lt;br /&gt;
|50_50_46   || 13.94     ||  1.644     ||  1.758    ||  0.9661    ||  0.9505    ||   1.714     ||  1.303    ||   6.944     ||  4.001&lt;br /&gt;
|-&lt;br /&gt;
|50_60_49   || 15.09     ||  1.757     ||  1.887    ||  0.9587    ||  0.9502    ||   1.723     ||  1.295    ||   7.390     ||  6.217&lt;br /&gt;
|-&lt;br /&gt;
|50_70_53   || 13.03     ||  1.855     ||  1.955    ||  0.9524    ||  0.9502    ||   1.731     ||  1.287    ||   5.353     ||  5.830&lt;br /&gt;
|-&lt;br /&gt;
|50_80_56   || 16.73     ||  1.949     ||  2.004    ||  0.9463    ||  0.9501    ||   1.739     ||  1.279    ||   2.807     ||  4.003&lt;br /&gt;
|-&lt;br /&gt;
|50_90_60   || 16.70     ||  2.011     ||  2.101    ||  0.9407    ||  0.9502    ||   1.747     ||  1.271    ||   4.501     ||  3.444&lt;br /&gt;
|-&lt;br /&gt;
|50_100_64  || 18.15     ||  2.090     ||  2.183    ||  0.9351    ||  0.9500    ||   1.754     ||  1.264    ||   4.434     ||  3.907&lt;br /&gt;
|-&lt;br /&gt;
|50_110_68  || 17.53     ||  2.154     ||  2.223    ||  0.9297    ||  0.9498    ||   1.762     ||  1.256    ||   3.205     ||  4.270&lt;br /&gt;
|-&lt;br /&gt;
|50_120_72  || 19.13     ||  2.213     ||  2.288    ||  0.9250    ||  0.9501    ||   1.768     ||  1.250    ||   3.417     ||  4.378&lt;br /&gt;
|-&lt;br /&gt;
|60_00_35   || 4.247     || 0.7126     || 0.7205    ||   1.003    ||  0.9498    ||   1.667     ||  1.352    ||   1.108     || 0.1270&lt;br /&gt;
|-&lt;br /&gt;
|60_10_37   || 6.862     || 0.9679     ||  1.002    ||  0.9934    ||  0.9509    ||   1.680     ||  1.338    ||   3.520     || 0.4827&lt;br /&gt;
|-&lt;br /&gt;
|60_20_40   || 9.669     ||  1.179     ||  1.240    ||  0.9831    ||  0.9503    ||   1.692     ||  1.326    ||   5.202     ||  1.236&lt;br /&gt;
|-&lt;br /&gt;
|60_30_43   || 12.01     ||  1.354     ||  1.435    ||  0.9747    ||  0.9502    ||   1.702     ||  1.316    ||   5.973     ||  2.132&lt;br /&gt;
|-&lt;br /&gt;
|60_40_46   || 13.48     ||  1.500     ||  1.593    ||  0.9672    ||  0.9503    ||   1.712     ||  1.306    ||   6.170     ||  2.806&lt;br /&gt;
|-&lt;br /&gt;
|60_50_50   || 15.36     ||  1.627     ||  1.732    ||  0.9601    ||  0.9504    ||   1.721     ||  1.297    ||   6.467     ||  3.895&lt;br /&gt;
|-&lt;br /&gt;
|60_60_53   || 16.79     ||  1.734     ||  1.851    ||  0.9528    ||  0.9499    ||   1.729     ||  1.289    ||   6.731     ||  5.666&lt;br /&gt;
|-&lt;br /&gt;
|60_70_57   || 15.88     ||  1.829     ||  1.934    ||  0.9473    ||  0.9502    ||   1.737     ||  1.281    ||   5.736     ||  6.958&lt;br /&gt;
|-&lt;br /&gt;
|60_80_61   || 13.66     ||  1.918     ||  1.968    ||  0.9428    ||  0.9514    ||   1.745     ||  1.273    ||   2.622     ||  4.555&lt;br /&gt;
|-&lt;br /&gt;
|60_90_64   || 17.29     ||  2.009     ||  2.063    ||  0.9359    ||  0.9501    ||   1.753     ||  1.265    ||   2.640     ||  1.637&lt;br /&gt;
|-&lt;br /&gt;
|60_100_68  || 17.62     ||  2.049     ||  2.122    ||  0.9304    ||  0.9497    ||   1.760     ||  1.258    ||   3.560     ||  3.718&lt;br /&gt;
|-&lt;br /&gt;
|60_110_72  || 17.50     ||  2.118     ||  2.177    ||  0.9257    ||  0.9501    ||   1.767     ||  1.251    ||   2.811     ||  4.023&lt;br /&gt;
|-&lt;br /&gt;
|60_120_76  || 17.78     ||  2.174     ||  2.222    ||  0.9217    ||  0.9510    ||   1.774     ||  1.244    ||   2.209     ||  4.211&lt;br /&gt;
|-&lt;br /&gt;
|70_00_39   || 5.731     || 0.7825     || 0.7975    ||  0.9949    ||  0.9497    ||   1.675     ||  1.343    ||   1.908     || 0.2335&lt;br /&gt;
|-&lt;br /&gt;
|70_10_41   || 8.418     ||  1.009     ||  1.048    ||  0.9860    ||  0.9509    ||   1.688     ||  1.330    ||   3.845     || 0.6755&lt;br /&gt;
|-&lt;br /&gt;
|70_20_44   || 11.09     ||  1.201     ||  1.265    ||  0.9767    ||  0.9504    ||   1.699     ||  1.319    ||   5.345     ||  1.317&lt;br /&gt;
|-&lt;br /&gt;
|70_30_47   || 13.41     ||  1.361     ||  1.441    ||  0.9688    ||  0.9504    ||   1.709     ||  1.309    ||   5.859     ||  2.187&lt;br /&gt;
|-&lt;br /&gt;
|70_40_51   || 14.99     ||  1.496     ||  1.591    ||  0.9615    ||  0.9503    ||   1.718     ||  1.300    ||   6.348     ||  2.859&lt;br /&gt;
|-&lt;br /&gt;
|70_50_54   || 16.87     ||  1.617     ||  1.712    ||  0.9543    ||  0.9501    ||   1.727     ||  1.291    ||   5.843     ||  3.756&lt;br /&gt;
|-&lt;br /&gt;
|70_60_57   || 17.89     ||  1.718     ||  1.823    ||  0.9479    ||  0.9500    ||   1.735     ||  1.283    ||   6.140     ||  4.746&lt;br /&gt;
|-&lt;br /&gt;
|70_70_61   || 18.26     ||  1.812     ||  1.928    ||  0.9423    ||  0.9503    ||   1.743     ||  1.275    ||   6.353     ||  6.812&lt;br /&gt;
|-&lt;br /&gt;
|70_80_65   || 16.37     ||  1.896     ||  1.962    ||  0.9363    ||  0.9499    ||   1.751     ||  1.267    ||   3.469     ||  5.948&lt;br /&gt;
|-&lt;br /&gt;
|70_90_68   || 9.135     ||  1.980     ||  1.988    ||  0.9317    ||  0.9506    ||   1.758     ||  1.260    ||  0.3692     || 0.1186&lt;br /&gt;
|-&lt;br /&gt;
|70_100_72  || 18.64     ||  2.007     ||  2.094    ||  0.9267    ||  0.9506    ||   1.765     ||  1.253    ||   4.327     ||  3.356&lt;br /&gt;
|-&lt;br /&gt;
|70_110_76  || 18.23     ||  2.088     ||  2.147    ||  0.9219    ||  0.9507    ||   1.772     ||  1.246    ||   2.792     ||  3.707&lt;br /&gt;
|-&lt;br /&gt;
|70_120_80  || 17.89     ||  2.145     ||  2.184    ||  0.9171    ||  0.9506    ||   1.779     ||  1.239    ||   1.846     ||  4.043&lt;br /&gt;
|-&lt;br /&gt;
|80_00_42   ||7.247      ||0.8436      ||0.8697     || 0.9869     || 0.9497     ||  1.684      || 1.335     ||  3.094      ||0.2402&lt;br /&gt;
|-&lt;br /&gt;
|80_10_45   ||9.865      || 1.049      || 1.095     || 0.9794     || 0.9513     ||  1.695      || 1.323     ||  4.371      ||0.7359&lt;br /&gt;
|-&lt;br /&gt;
|80_20_48   ||12.28      || 1.226      || 1.290     || 0.9697     || 0.9500     ||  1.706      || 1.312     ||  5.206      || 1.327&lt;br /&gt;
|-&lt;br /&gt;
|80_30_51   ||14.38      || 1.370      || 1.454     || 0.9626     || 0.9503     ||  1.715      || 1.303     ||  6.088      || 2.102&lt;br /&gt;
|-&lt;br /&gt;
|80_40_54   ||16.47      || 1.500      || 1.594     || 0.9549     || 0.9497     ||  1.724      || 1.294     ||  6.263      || 2.799&lt;br /&gt;
|-&lt;br /&gt;
|80_50_58   ||17.63      || 1.612      || 1.706     || 0.9492     || 0.9503     ||  1.733      || 1.285     ||  5.842      || 3.329&lt;br /&gt;
|-&lt;br /&gt;
|80_60_61   ||18.84      || 1.712      || 1.814     || 0.9436     || 0.9507     ||  1.741      || 1.277     ||  5.984      || 3.990&lt;br /&gt;
|-&lt;br /&gt;
|80_70_65   ||19.27      || 1.799      || 1.898     || 0.9372     || 0.9501     ||  1.749      || 1.269     ||  5.555      || 4.728&lt;br /&gt;
|-&lt;br /&gt;
|80_80_69   ||17.96      || 1.880      || 1.935     || 0.9321     || 0.9503     ||  1.756      || 1.262     ||  2.921      || 3.774&lt;br /&gt;
|-&lt;br /&gt;
|80_90_73   ||13.42      || 1.957      || 1.982     || 0.9266     || 0.9500     ||  1.764      || 1.254     ||  1.312      ||0.6938&lt;br /&gt;
|-&lt;br /&gt;
|80_100_76  || 18.53     ||  2.008     ||  2.065    ||  0.9220    ||  0.9504    ||   1.770     ||  1.247    ||   2.839     ||  1.773&lt;br /&gt;
|-&lt;br /&gt;
|80_110_80  || 18.41     ||  2.059     ||  2.117    ||  0.9176    ||  0.9507    ||   1.777     ||  1.241    ||   2.847     ||  3.632&lt;br /&gt;
|-&lt;br /&gt;
|80_120_84  || 18.26     ||  2.117     ||  2.157    ||  0.9122    ||  0.9496    ||   1.784     ||  1.234    ||   1.872     ||  3.986&lt;br /&gt;
|-&lt;br /&gt;
|90_00_46   || 8.679     || 0.9022     || 0.9354    ||  0.9802    ||  0.9501    ||   1.691     ||  1.327    ||   3.678     || 0.3981&lt;br /&gt;
|-&lt;br /&gt;
|90_10_49   || 11.45     ||  1.090     ||  1.146    ||  0.9717    ||  0.9502    ||   1.702     ||  1.315    ||   5.148     || 0.8099&lt;br /&gt;
|-&lt;br /&gt;
|90_20_52   || 12.44     ||  1.247     ||  1.323    ||  0.9640    ||  0.9503    ||   1.712     ||  1.305    ||   6.100     ||  1.079&lt;br /&gt;
|-&lt;br /&gt;
|90_30_55   || 16.14     ||  1.383     ||  1.475    ||  0.9571    ||  0.9504    ||   1.722     ||  1.296    ||   6.607     ||  2.158&lt;br /&gt;
|-&lt;br /&gt;
|90_40_58   || 17.45     ||  1.506     ||  1.597    ||  0.9499    ||  0.9501    ||   1.731     ||  1.287    ||   6.012     ||  2.629&lt;br /&gt;
|-&lt;br /&gt;
|90_50_62   || 18.70     ||  1.609     ||  1.706    ||  0.9438    ||  0.9501    ||   1.739     ||  1.279    ||   6.003     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|90_60_65   || 18.77     ||  1.703     ||  1.789    ||  0.9381    ||  0.9502    ||   1.747     ||  1.271    ||   5.045     ||  3.047&lt;br /&gt;
|-&lt;br /&gt;
|90_70_69   || 18.43     ||  1.787     ||  1.852    ||  0.9324    ||  0.9500    ||   1.754     ||  1.263    ||   3.623     ||  3.117&lt;br /&gt;
|-&lt;br /&gt;
|90_80_73   || 17.72     ||  1.868     ||  1.909    ||  0.9269    ||  0.9497    ||   1.762     ||  1.256    ||   2.217     ||  2.354&lt;br /&gt;
|-&lt;br /&gt;
|90_90_76   || 14.40     ||  1.940     ||  1.956    ||  0.9221    ||  0.9499    ||   1.769     ||  1.249    ||  0.8079     || 0.8326&lt;br /&gt;
|-&lt;br /&gt;
|90_100_80  || 18.53     ||  2.009     ||  2.038    ||  0.9176    ||  0.9503    ||   1.776     ||  1.242    ||   1.484     ||  1.095&lt;br /&gt;
|-&lt;br /&gt;
|90_110_84  || 18.97     ||  2.021     ||  2.094    ||  0.9129    ||  0.9502    ||   1.783     ||  1.235    ||   3.625     ||  3.669&lt;br /&gt;
|-&lt;br /&gt;
|90_120_88  || 17.79     ||  2.090     ||  2.129    ||  0.9077    ||  0.9494    ||   1.789     ||  1.229    ||   1.827     ||  3.862&lt;br /&gt;
|-&lt;br /&gt;
|100_00_50  || 10.07     || 0.9544     || 0.9970    ||  0.9732    ||  0.9499    ||   1.699     ||  1.319    ||   4.471     || 0.4341&lt;br /&gt;
|-&lt;br /&gt;
|100_10_53  || 12.78     ||  1.127     ||  1.186    ||  0.9649    ||  0.9499    ||   1.710     ||  1.308    ||   5.262     || 0.9629&lt;br /&gt;
|-&lt;br /&gt;
|100_16_55  || 13.69     ||  1.215     ||  1.287    ||  0.9610    ||  0.9501    ||   1.715     ||  1.302    ||   5.901     ||  1.023&lt;br /&gt;
|-&lt;br /&gt;
|100_20_56  || 10.86     ||  1.271     ||  1.324    ||  0.9583    ||  0.9502    ||   1.719     ||  1.299    ||   4.120     || 0.8295&lt;br /&gt;
|-&lt;br /&gt;
|100_22_56  || 15.40     ||  1.309     ||  1.381    ||  0.9412    ||  0.9362    ||   1.722     ||  1.296    ||   5.552     ||  1.648&lt;br /&gt;
|-&lt;br /&gt;
|100_24_58  || 15.90     ||  1.326     ||  1.406    ||  0.9552    ||  0.9499    ||   1.722     ||  1.295    ||   6.105     ||  1.792&lt;br /&gt;
|-&lt;br /&gt;
|100_26_58  || 16.42     ||  1.352     ||  1.435    ||  0.9538    ||  0.9499    ||   1.724     ||  1.293    ||   6.137     ||  1.888&lt;br /&gt;
|-&lt;br /&gt;
|100_28_59  || 17.07     ||  1.375     ||  1.464    ||  0.9527    ||  0.9501    ||   1.726     ||  1.291    ||   6.475     ||  1.983&lt;br /&gt;
|-&lt;br /&gt;
|100_30_59  || 17.29     ||  1.398     ||  1.490    ||  0.9511    ||  0.9500    ||   1.728     ||  1.289    ||   6.561     ||  2.075&lt;br /&gt;
|-&lt;br /&gt;
|100_32_60  || 17.74     ||  1.423     ||  1.517    ||  0.9499    ||  0.9499    ||   1.730     ||  1.288    ||   6.596     ||  2.165&lt;br /&gt;
|-&lt;br /&gt;
|100_36_61  || 18.37     ||  1.467     ||  1.567    ||  0.9475    ||  0.9501    ||   1.733     ||  1.284    ||   6.819     ||  2.183&lt;br /&gt;
|-&lt;br /&gt;
|100_40_63  || 18.77     ||  1.509     ||  1.608    ||  0.9450    ||  0.9500    ||   1.736     ||  1.281    ||   6.553     ||  2.304&lt;br /&gt;
|-&lt;br /&gt;
|100_44_64  || 19.25     ||  1.551     ||  1.653    ||  0.9426    ||  0.9500    ||   1.740     ||  1.278    ||   6.569     ||  2.360&lt;br /&gt;
|-&lt;br /&gt;
|100_48_65  || 19.16     ||  1.591     ||  1.684    ||  0.9400    ||  0.9500    ||   1.743     ||  1.275    ||   5.807     ||  2.555&lt;br /&gt;
|-&lt;br /&gt;
|100_50_65  || 19.11     ||  1.613     ||  1.704    ||  0.9381    ||  0.9501    ||   1.745     ||  1.274    ||   5.628     ||  2.649&lt;br /&gt;
|-&lt;br /&gt;
|100_55_67  || 19.04     ||  1.659     ||  1.739    ||  0.9352    ||  0.9500    ||   1.749     ||  1.270    ||   4.839     ||  2.808&lt;br /&gt;
|-&lt;br /&gt;
|100_56_67  || 18.93     ||  1.667     ||  1.742    ||  0.9347    ||  0.9501    ||   1.750     ||  1.269    ||   4.522     ||  2.692&lt;br /&gt;
|-&lt;br /&gt;
|100_60_68  || 19.04     ||  1.702     ||  1.775    ||  0.9325    ||  0.9500    ||   1.753     ||  1.266    ||   4.326     ||  2.720&lt;br /&gt;
|-&lt;br /&gt;
|100_64_70  || 18.76     ||  1.733     ||  1.799    ||  0.9303    ||  0.9500    ||   1.756     ||  1.263    ||   3.774     ||  2.676&lt;br /&gt;
|-&lt;br /&gt;
|100_68_72  || 18.46     ||  1.771     ||  1.825    ||  0.9279    ||  0.9494    ||   1.759     ||  1.259    ||   3.080     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_70_73  || 18.23     ||  1.784     ||  1.841    ||  0.9277    ||  0.9500    ||   1.760     ||  1.258    ||   3.166     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_80_77  || 16.73     ||  1.855     ||  1.885    ||  0.9261    ||  0.9532    ||   1.767     ||  1.251    ||   1.617     ||  1.818&lt;br /&gt;
|-&lt;br /&gt;
|100_90_80  || 13.86     ||  1.931     ||  1.936    ||  0.9172    ||  0.9494    ||   1.774     ||  1.244    ||  0.2833     || 0.7382&lt;br /&gt;
|-&lt;br /&gt;
|100_95_82  || 11.27     ||  1.967     ||  1.964    ||  0.9243    ||  0.9582    ||   1.777     ||  1.241    || -0.1435     || 6.8954E-02&lt;br /&gt;
|-&lt;br /&gt;
|100_105_86 || 16.96     ||  2.019     ||  2.045    ||  0.9233    ||  0.9617    ||   1.783     ||  1.235    ||   1.268     ||  1.425&lt;br /&gt;
|-&lt;br /&gt;
|100_110_88 || 18.88     ||  2.020     ||  2.073    ||  0.9229    ||  0.9634    ||   1.786     ||  1.232    ||   2.618     ||  2.366&lt;br /&gt;
|-&lt;br /&gt;
|100_120_92 || 17.63     ||  2.064     ||  2.113    ||  0.9044    ||  0.9501    ||   1.794     ||  1.224    ||   2.379     ||  3.790&lt;br /&gt;
|-&lt;br /&gt;
|110_00_54  || 11.70     ||  1.006     ||  1.060    ||  0.9663    ||  0.9498    ||   1.706     ||  1.312    ||   5.370     || 0.4642&lt;br /&gt;
|-&lt;br /&gt;
|110_10_57  || 13.97     ||  1.160     ||  1.232    ||  0.9593    ||  0.9502    ||   1.716     ||  1.301    ||   6.136     || 0.8247&lt;br /&gt;
|-&lt;br /&gt;
|110_20_60  || 15.75     ||  1.298     ||  1.372    ||  0.9526    ||  0.9504    ||   1.726     ||  1.292    ||   5.739     ||  1.330&lt;br /&gt;
|-&lt;br /&gt;
|110_30_63  || 18.56     ||  1.415     ||  1.516    ||  0.9455    ||  0.9500    ||   1.734     ||  1.284    ||   7.122     ||  1.849&lt;br /&gt;
|-&lt;br /&gt;
|110_40_66  || 19.50     ||  1.521     ||  1.622    ||  0.9398    ||  0.9503    ||   1.743     ||  1.275    ||   6.602     ||  1.921&lt;br /&gt;
|-&lt;br /&gt;
|110_50_70  || 19.07     ||  1.618     ||  1.696    ||  0.9336    ||  0.9498    ||   1.751     ||  1.267    ||   4.873     ||  2.085&lt;br /&gt;
|-&lt;br /&gt;
|110_60_73  || 18.32     ||  1.702     ||  1.761    ||  0.9291    ||  0.9507    ||   1.758     ||  1.260    ||   3.471     ||  2.033&lt;br /&gt;
|-&lt;br /&gt;
|110_70_77  || 17.13     ||  1.782     ||  1.816    ||  0.9237    ||  0.9504    ||   1.766     ||  1.252    ||   1.948     ||  1.838&lt;br /&gt;
|-&lt;br /&gt;
|110_80_81  || 15.56     ||  1.853     ||  1.871    ||  0.9192    ||  0.9508    ||   1.773     ||  1.245    ||  0.9878     ||  1.332&lt;br /&gt;
|-&lt;br /&gt;
|110_90_84  || 13.12     ||  1.923     ||  1.926    ||  0.9142    ||  0.9506    ||   1.780     ||  1.238    ||  0.1639     || 0.5301&lt;br /&gt;
|-&lt;br /&gt;
|110_95_86  || 10.73     ||  1.963     ||  1.955    ||  0.9095    ||  0.9486    ||   1.783     ||  1.235    || -0.3746     || 8.1449E-04&lt;br /&gt;
|-&lt;br /&gt;
|110_110_92 || 17.29     ||  2.020     ||  2.055    ||  0.9056    ||  0.9509    ||   1.793     ||  1.225    ||   1.768     ||  2.045&lt;br /&gt;
|-&lt;br /&gt;
|110_120_95 || 17.55     ||  2.048     ||  2.095    ||  0.9014    ||  0.9510    ||   1.799     ||  1.219    ||   2.314     ||  3.774&lt;br /&gt;
|-&lt;br /&gt;
|120_00_57  || 13.14     ||  1.050     ||  1.117    ||  0.9599    ||  0.9497    ||   1.714     ||  1.305    ||   6.304     || 0.4861&lt;br /&gt;
|-&lt;br /&gt;
|120_10_60  || 14.81     ||  1.196     ||  1.268    ||  0.9534    ||  0.9501    ||   1.723     ||  1.295    ||   6.054     || 0.8382&lt;br /&gt;
|-&lt;br /&gt;
|120_20_63  || 17.57     ||  1.323     ||  1.409    ||  0.9458    ||  0.9494    ||   1.732     ||  1.286    ||   6.504     ||  1.409&lt;br /&gt;
|-&lt;br /&gt;
|120_30_67  || 19.50     ||  1.435     ||  1.539    ||  0.9407    ||  0.9503    ||   1.741     ||  1.277    ||   7.263     ||  1.529&lt;br /&gt;
|-&lt;br /&gt;
|120_40_70  || 19.38     ||  1.534     ||  1.621    ||  0.9335    ||  0.9492    ||   1.749     ||  1.269    ||   5.695     ||  1.632&lt;br /&gt;
|-&lt;br /&gt;
|120_50_74  || 18.34     ||  1.621     ||  1.684    ||  0.9294    ||  0.9503    ||   1.756     ||  1.262    ||   3.910     ||  1.864&lt;br /&gt;
|-&lt;br /&gt;
|120_60_77  || 17.24     ||  1.703     ||  1.743    ||  0.9246    ||  0.9507    ||   1.764     ||  1.254    ||   2.381     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|120_70_81  || 16.02     ||  1.780     ||  1.803    ||  0.9197    ||  0.9509    ||   1.771     ||  1.247    ||   1.312     ||  1.511&lt;br /&gt;
|-&lt;br /&gt;
|120_80_84  || 14.49     ||  1.850     ||  1.860    ||  0.9150    ||  0.9509    ||   1.778     ||  1.240    ||  0.5347     ||  1.076&lt;br /&gt;
|-&lt;br /&gt;
|120_90_88  || 12.18     ||  1.918     ||  1.918    ||  0.9096    ||  0.9501    ||   1.785     ||  1.233    || -4.1127E-02 || 0.3613&lt;br /&gt;
|-&lt;br /&gt;
|120_95_90  || 10.06     ||  1.957     ||  1.950    ||  0.9071    ||  0.9499    ||   1.788     ||  1.230    || -0.3241     ||  0.000&lt;br /&gt;
|-&lt;br /&gt;
|120_115_97 || 16.46     ||  2.020     ||  2.066    ||  0.8983    ||  0.9497    ||   1.801     ||  1.216    ||   2.258     ||  2.404&lt;br /&gt;
|-&lt;br /&gt;
|120_120_99 || 17.58     ||  2.008     ||  2.092    ||  0.8967    ||  0.9501    ||   1.804     ||  1.213    ||   4.186     ||  3.647&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Flexibility ==&lt;br /&gt;
&lt;br /&gt;
[[File:Flexibility TJ-II.png|300px|thumb|right|Flexibility diagram of TJ-II magnetic configurations. Several lines of constant rotational transform are highlighted and labelled with the corresponding central &amp;lt;math&amp;gt;\iota/2\pi&amp;lt;/math&amp;gt;-value.]]&lt;br /&gt;
TJ-II has considerable configurational flexibility, as observed in the &#039;flexibility diagram&#039;&amp;lt;ref&amp;gt;E. Ascasíbar, T. Estrada, F. Castejón, A. López-Fraguas, I. Pastor, J. Sánchez, U. Stroth, J. Qin and TJ-II Team, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/45/4/009|Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276–284]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
Some of this flexibility space has been explored, as in the &#039;magnetic well scan&#039; experiments&amp;lt;ref&amp;gt;A. de Aguilera, F. Castejón, E. Ascasíbar, et al. &#039;&#039;Magnetic well scan and confinement in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/55/11/113014|Nucl. Fusion, 55(11):113014, 2015]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
More recently, the rotational transform in the plasma edge region was found to be of importance for L-H confinement transitions&amp;lt;ref&amp;gt;B. P. van Milligen, T. Estrada, B. Carreras, L. García, and TJ-II Team. &#039;&#039;Importance of the rotational transform for L–H transitions in the TJ-II stellarator&#039;&#039;, [[doi:10.3390/plasma7020024|Plasma, 7(2):446–464, 2024]].&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8727</id>
		<title>TJ-II:Magnetic configuration</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8727"/>
		<updated>2026-10-07T16:26:24Z</updated>

		<summary type="html">&lt;p&gt;Admin: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The magnetic configuration of [[TJ-II]] in vacuum is completely determined by the currents flowing through the [[TJ-II:Coil system|external coils]].&lt;br /&gt;
Magnetic configurations are labelled as &#039;xxx_yy_zz&#039;, where&lt;br /&gt;
* &#039;xxx&#039;: 10 times the current (in kA) in the circular coil&lt;br /&gt;
* &#039;yy&#039;: 10 times the current (in kA) in the helical coil&lt;br /&gt;
* &#039;zz&#039;: 10 times the current (in kA) in the vertical field coils&lt;br /&gt;
The current in the toroidal field coils is not specified, as its value is adjusted to guarantee central absorption of the [[TJ-II:Electron Cyclotron Resonant Heating|Electron Cyclotron Resonant Heating]] source (requiring a specific &#039;resonant&#039; value of the magnetic field on the magnetic axis, &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
Configuration list:&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;width: 100%&amp;quot; border=&amp;quot;1&amp;quot;||&lt;br /&gt;
|-&lt;br /&gt;
! Configuration &lt;br /&gt;
! &amp;lt;math&amp;gt;r_{av}&amp;lt;/math&amp;gt; (cm) &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(0)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(a)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{m,av}&amp;lt;/math&amp;gt;(T) &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt; (T) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(0^\circ)&amp;lt;/math&amp;gt; (m) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(45^\circ)&amp;lt;/math&amp;gt; (m) &lt;br /&gt;
! Shear (%) &lt;br /&gt;
! Well (%)&lt;br /&gt;
|-&lt;br /&gt;
|0_20_13    ||1.139      || 1.185      || 1.194     ||  1.033     || 0.9504     ||  1.644      || 1.374     || 0.7793      ||5.7521E-02&lt;br /&gt;
|-&lt;br /&gt;
|0_30_15    ||4.228      || 1.518      || 1.698     ||  1.019     || 0.9500     ||  1.658      || 1.360     ||  11.85      || 1.050&lt;br /&gt;
|-&lt;br /&gt;
|0_40_18    ||5.903      || 1.756      || 2.003     ||  1.008     || 0.9505     ||  1.671      || 1.347     ||  14.09      || 1.217&lt;br /&gt;
|-&lt;br /&gt;
|0_50_22    ||6.480      || 1.936      || 2.230     || 0.9973     || 0.9502     ||  1.682      || 1.336     ||  15.17      || 2.481&lt;br /&gt;
|-&lt;br /&gt;
|0_60_26    ||8.500      || 2.073      || 2.399     || 0.9885     || 0.9502     ||  1.692      || 1.326     ||  15.70      || 3.218&lt;br /&gt;
|-&lt;br /&gt;
|0_70_29    ||7.147      || 2.187      || 2.434     || 0.9805     || 0.9503     ||  1.701      || 1.317     ||  11.30      || 2.985&lt;br /&gt;
|-&lt;br /&gt;
|0_80_34    ||6.902      || 2.284      || 2.469     || 0.9736     || 0.9506     ||  1.710      || 1.308     ||  8.084      || 2.735&lt;br /&gt;
|-&lt;br /&gt;
|0_90_38    ||6.738      || 2.366      || 2.514     || 0.9663     || 0.9503     ||  1.719      || 1.299     ||  6.269      || 2.534&lt;br /&gt;
|-&lt;br /&gt;
|0_100_42   ||12.59      || 2.436      || 2.667     || 0.9601     || 0.9505     ||  1.727      || 1.291     ||  9.493      || 4.643&lt;br /&gt;
|-&lt;br /&gt;
|0_110_46   ||10.67      || 2.493      || 2.667     || 0.9539     || 0.9503     ||  1.734      || 1.284     ||  6.980      || 4.554&lt;br /&gt;
|-&lt;br /&gt;
|0_120_50   ||12.71      || 2.548      || 2.667     || 0.9482     || 0.9504     ||  1.742      || 1.276     ||  4.683      || 4.272&lt;br /&gt;
|-&lt;br /&gt;
|10_20_18   || 2.557     ||  1.148     ||  1.184    ||   1.024    ||  0.9514    ||   1.652     ||  1.366    ||   3.183     || 0.2469&lt;br /&gt;
|-&lt;br /&gt;
|10_30_20   || 6.083     ||  1.438     ||  1.602    ||   1.010    ||  0.9501    ||   1.666     ||  1.352    ||   11.35     ||  1.398&lt;br /&gt;
|-&lt;br /&gt;
|10_40_24   || 6.921     ||  1.659     ||  1.880    ||   1.000    ||  0.9504    ||   1.678     ||  1.340    ||   13.34     ||  2.751&lt;br /&gt;
|-&lt;br /&gt;
|10_50_27   || 8.140     ||  1.826     ||  1.997    ||  0.9909    ||  0.9504    ||   1.688     ||  1.329    ||   9.321     ||  3.241&lt;br /&gt;
|-&lt;br /&gt;
|10_60_31   || 9.350     ||  1.965     ||  2.183    ||  0.9826    ||  0.9505    ||   1.698     ||  1.319    ||   11.11     ||  3.084&lt;br /&gt;
|-&lt;br /&gt;
|10_70_35   || 10.10     ||  2.077     ||  2.288    ||  0.9750    ||  0.9505    ||   1.707     ||  1.310    ||   10.16     ||  3.597&lt;br /&gt;
|-&lt;br /&gt;
|10_80_38   || 9.810     ||  2.174     ||  2.371    ||  0.9674    ||  0.9502    ||   1.716     ||  1.302    ||   9.037     ||  3.908&lt;br /&gt;
|-&lt;br /&gt;
|10_90_42   || 10.54     ||  2.257     ||  2.434    ||  0.9610    ||  0.9503    ||   1.724     ||  1.294    ||   7.851     ||  4.281&lt;br /&gt;
|-&lt;br /&gt;
|10_100_47  || 10.21     ||  2.327     ||  2.482    ||  0.9546    ||  0.9502    ||   1.732     ||  1.286    ||   6.647     ||  4.236&lt;br /&gt;
|-&lt;br /&gt;
|10_110_51  || 11.11     ||  2.395     ||  2.547    ||  0.9488    ||  0.9501    ||   1.740     ||  1.278    ||   6.331     ||  5.121&lt;br /&gt;
|-&lt;br /&gt;
|10_120_55  || 10.04     ||  2.451     ||  2.565    ||  0.9432    ||  0.9502    ||   1.747     ||  1.271    ||   4.674     ||  4.426&lt;br /&gt;
|-&lt;br /&gt;
|20_10_21   || 1.213     || 0.7902     || 0.7956    ||   1.028    ||  0.9503    ||   1.645     ||  1.373    ||  0.6830     || 3.7624E-02&lt;br /&gt;
|-&lt;br /&gt;
|20_20_22   || 3.952     ||  1.136     ||  1.185    ||   1.014    ||  0.9500    ||   1.661     ||  1.357    ||   4.350     || 0.4717&lt;br /&gt;
|-&lt;br /&gt;
|20_30_25   || 6.779     ||  1.395     ||  1.521    ||   1.003    ||  0.9502    ||   1.673     ||  1.344    ||   9.049     ||  1.550&lt;br /&gt;
|-&lt;br /&gt;
|20_40_28   || 8.475     ||  1.592     ||  1.771    ||  0.9922    ||  0.9498    ||   1.685     ||  1.333    ||   11.25     ||  2.879&lt;br /&gt;
|-&lt;br /&gt;
|20_50_32   || 8.039     ||  1.756     ||  1.906    ||  0.9842    ||  0.9505    ||   1.695     ||  1.323    ||   8.571     ||  3.131&lt;br /&gt;
|-&lt;br /&gt;
|20_60_35   || 11.21     ||  1.884     ||  1.997    ||  0.9755    ||  0.9498    ||   1.705     ||  1.313    ||   5.968     ||  1.980&lt;br /&gt;
|-&lt;br /&gt;
|20_70_39   || 11.08     ||  1.994     ||  2.154    ||  0.9689    ||  0.9504    ||   1.714     ||  1.304    ||   7.982     ||  3.385&lt;br /&gt;
|-&lt;br /&gt;
|20_80_43   || 12.14     ||  2.092     ||  2.255    ||  0.9614    ||  0.9497    ||   1.722     ||  1.296    ||   7.811     ||  4.133&lt;br /&gt;
|-&lt;br /&gt;
|20_90_47   || 12.83     ||  2.174     ||  2.324    ||  0.9558    ||  0.9503    ||   1.730     ||  1.288    ||   6.862     ||  4.713&lt;br /&gt;
|-&lt;br /&gt;
|20_100_51  || 12.68     ||  2.246     ||  2.379    ||  0.9498    ||  0.9503    ||   1.738     ||  1.280    ||   5.945     ||  4.930&lt;br /&gt;
|-&lt;br /&gt;
|20_110_55  || 13.79     ||  2.313     ||  2.434    ||  0.9443    ||  0.9505    ||   1.745     ||  1.273    ||   5.248     ||  5.117&lt;br /&gt;
|-&lt;br /&gt;
|20_120_59  || 13.91     ||  2.368     ||  2.483    ||  0.9386    ||  0.9502    ||   1.752     ||  1.265    ||   4.822     ||  5.418&lt;br /&gt;
|-&lt;br /&gt;
|30_10_25   || 2.709     || 0.8385     || 0.8507    ||   1.018    ||  0.9501    ||   1.654     ||  1.363    ||   1.452     || 0.1431&lt;br /&gt;
|-&lt;br /&gt;
|30_20_27   || 5.443     ||  1.134     ||  1.189    ||   1.007    ||  0.9514    ||   1.669     ||  1.349    ||   4.847     || 0.7001&lt;br /&gt;
|-&lt;br /&gt;
|30_30_30   || 8.180     ||  1.368     ||  1.481    ||  0.9956    ||  0.9506    ||   1.681     ||  1.337    ||   8.332     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|30_40_33   || 9.756     ||  1.550     ||  1.687    ||  0.9860    ||  0.9503    ||   1.692     ||  1.326    ||   8.877     ||  2.798&lt;br /&gt;
|-&lt;br /&gt;
|30_50_37   || 11.16     ||  1.702     ||  1.878    ||  0.9779    ||  0.9503    ||   1.702     ||  1.316    ||   10.37     ||  4.941&lt;br /&gt;
|-&lt;br /&gt;
|30_60_40   || 9.262     ||  1.827     ||  1.936    ||  0.9706    ||  0.9505    ||   1.711     ||  1.307    ||   5.952     ||  3.624&lt;br /&gt;
|-&lt;br /&gt;
|30_70_44   || 12.28     ||  1.937     ||  2.007    ||  0.9631    ||  0.9502    ||   1.720     ||  1.298    ||   3.593     ||  4.431&lt;br /&gt;
|-&lt;br /&gt;
|30_80_48   || 13.28     ||  2.033     ||  2.149    ||  0.9567    ||  0.9502    ||   1.728     ||  1.290    ||   5.702     ||  3.674&lt;br /&gt;
|-&lt;br /&gt;
|30_90_52   || 14.16     ||  2.115     ||  2.231    ||  0.9504    ||  0.9501    ||   1.736     ||  1.282    ||   5.476     ||  4.227&lt;br /&gt;
|-&lt;br /&gt;
|30_100_56  || 14.97     ||  2.187     ||  2.295    ||  0.9448    ||  0.9502    ||   1.743     ||  1.275    ||   4.949     ||  4.755&lt;br /&gt;
|-&lt;br /&gt;
|30_110_59  || 15.76     ||  2.246     ||  2.356    ||  0.9391    ||  0.9500    ||   1.751     ||  1.267    ||   4.920     ||  5.215&lt;br /&gt;
|-&lt;br /&gt;
|30_120_63  || 14.48     ||  2.306     ||  2.389    ||  0.9343    ||  0.9504    ||   1.758     ||  1.260    ||   3.573     ||  5.025&lt;br /&gt;
|-&lt;br /&gt;
|40_00_27   || 1.350     || 0.5464     || 0.5471    ||   1.024    ||  0.9504    ||   1.647     ||  1.371    ||  0.1331     || 2.4768E-02&lt;br /&gt;
|-&lt;br /&gt;
|40_10_29   || 4.111     || 0.8821     || 0.9010    ||   1.010    ||  0.9510    ||   1.663     ||  1.355    ||   2.152     || 0.2456&lt;br /&gt;
|-&lt;br /&gt;
|40_20_31   || 6.646     ||  1.146     ||  1.202    ||  0.9975    ||  0.9501    ||   1.677     ||  1.341    ||   4.928     || 0.8185&lt;br /&gt;
|-&lt;br /&gt;
|40_30_34   || 9.328     ||  1.354     ||  1.452    ||  0.9884    ||  0.9506    ||   1.688     ||  1.330    ||   7.247     ||  1.826&lt;br /&gt;
|-&lt;br /&gt;
|40_40_37   || 11.15     ||  1.523     ||  1.646    ||  0.9788    ||  0.9498    ||   1.699     ||  1.319    ||   8.061     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|40_50_41   || 12.66     ||  1.666     ||  1.797    ||  0.9719    ||  0.9506    ||   1.708     ||  1.310    ||   7.872     ||  4.310&lt;br /&gt;
|-&lt;br /&gt;
|40_60_44   || 12.34     ||  1.786     ||  1.927    ||  0.9637    ||  0.9497    ||   1.717     ||  1.301    ||   7.879     ||  5.834&lt;br /&gt;
|-&lt;br /&gt;
|40_70_48   || 9.734     ||  1.894     ||  1.963    ||  0.9579    ||  0.9504    ||   1.726     ||  1.292    ||   3.625     ||  3.668&lt;br /&gt;
|-&lt;br /&gt;
|40_80_52   || 13.96     ||  1.986     ||  2.067    ||  0.9515    ||  0.9503    ||   1.734     ||  1.284    ||   4.054     ||  3.028&lt;br /&gt;
|-&lt;br /&gt;
|40_90_56   || 15.39     ||  2.062     ||  2.156    ||  0.9457    ||  0.9504    ||   1.741     ||  1.277    ||   4.529     ||  3.841&lt;br /&gt;
|-&lt;br /&gt;
|40_100_60  || 16.40     ||  2.132     ||  2.232    ||  0.9400    ||  0.9502    ||   1.749     ||  1.269    ||   4.683     ||  4.355&lt;br /&gt;
|-&lt;br /&gt;
|40_110_64  || 18.12     ||  2.199     ||  2.288    ||  0.9348    ||  0.9503    ||   1.756     ||  1.262    ||   4.049     ||  4.651&lt;br /&gt;
|-&lt;br /&gt;
|40_120_68  || 16.81     ||  2.256     ||  2.327    ||  0.9295    ||  0.9501    ||   1.763     ||  1.255    ||   3.158     ||  4.904&lt;br /&gt;
|-&lt;br /&gt;
|50_00_31   || 2.818     || 0.6329     || 0.6375    ||   1.013    ||  0.9498    ||   1.657     ||  1.361    ||  0.7286     || 6.1871E-02&lt;br /&gt;
|-&lt;br /&gt;
|50_10_33   || 5.588     || 0.9254     || 0.9532    ||   1.001    ||  0.9506    ||   1.672     ||  1.346    ||   3.003     || 0.3605&lt;br /&gt;
|-&lt;br /&gt;
|50_20_36   || 8.222     ||  1.160     ||  1.216    ||  0.9902    ||  0.9502    ||   1.684     ||  1.334    ||   4.838     ||  1.060&lt;br /&gt;
|-&lt;br /&gt;
|50_30_39   || 10.67     ||  1.352     ||  1.435    ||  0.9815    ||  0.9505    ||   1.695     ||  1.323    ||   6.163     ||  2.008&lt;br /&gt;
|-&lt;br /&gt;
|50_40_42   || 12.44     ||  1.508     ||  1.609    ||  0.9733    ||  0.9504    ||   1.705     ||  1.313    ||   6.719     ||  2.910&lt;br /&gt;
|-&lt;br /&gt;
|50_50_46   || 13.94     ||  1.644     ||  1.758    ||  0.9661    ||  0.9505    ||   1.714     ||  1.303    ||   6.944     ||  4.001&lt;br /&gt;
|-&lt;br /&gt;
|50_60_49   || 15.09     ||  1.757     ||  1.887    ||  0.9587    ||  0.9502    ||   1.723     ||  1.295    ||   7.390     ||  6.217&lt;br /&gt;
|-&lt;br /&gt;
|50_70_53   || 13.03     ||  1.855     ||  1.955    ||  0.9524    ||  0.9502    ||   1.731     ||  1.287    ||   5.353     ||  5.830&lt;br /&gt;
|-&lt;br /&gt;
|50_80_56   || 16.73     ||  1.949     ||  2.004    ||  0.9463    ||  0.9501    ||   1.739     ||  1.279    ||   2.807     ||  4.003&lt;br /&gt;
|-&lt;br /&gt;
|50_90_60   || 16.70     ||  2.011     ||  2.101    ||  0.9407    ||  0.9502    ||   1.747     ||  1.271    ||   4.501     ||  3.444&lt;br /&gt;
|-&lt;br /&gt;
|50_100_64  || 18.15     ||  2.090     ||  2.183    ||  0.9351    ||  0.9500    ||   1.754     ||  1.264    ||   4.434     ||  3.907&lt;br /&gt;
|-&lt;br /&gt;
|50_110_68  || 17.53     ||  2.154     ||  2.223    ||  0.9297    ||  0.9498    ||   1.762     ||  1.256    ||   3.205     ||  4.270&lt;br /&gt;
|-&lt;br /&gt;
|50_120_72  || 19.13     ||  2.213     ||  2.288    ||  0.9250    ||  0.9501    ||   1.768     ||  1.250    ||   3.417     ||  4.378&lt;br /&gt;
|-&lt;br /&gt;
|60_00_35   || 4.247     || 0.7126     || 0.7205    ||   1.003    ||  0.9498    ||   1.667     ||  1.352    ||   1.108     || 0.1270&lt;br /&gt;
|-&lt;br /&gt;
|60_10_37   || 6.862     || 0.9679     ||  1.002    ||  0.9934    ||  0.9509    ||   1.680     ||  1.338    ||   3.520     || 0.4827&lt;br /&gt;
|-&lt;br /&gt;
|60_20_40   || 9.669     ||  1.179     ||  1.240    ||  0.9831    ||  0.9503    ||   1.692     ||  1.326    ||   5.202     ||  1.236&lt;br /&gt;
|-&lt;br /&gt;
|60_30_43   || 12.01     ||  1.354     ||  1.435    ||  0.9747    ||  0.9502    ||   1.702     ||  1.316    ||   5.973     ||  2.132&lt;br /&gt;
|-&lt;br /&gt;
|60_40_46   || 13.48     ||  1.500     ||  1.593    ||  0.9672    ||  0.9503    ||   1.712     ||  1.306    ||   6.170     ||  2.806&lt;br /&gt;
|-&lt;br /&gt;
|60_50_50   || 15.36     ||  1.627     ||  1.732    ||  0.9601    ||  0.9504    ||   1.721     ||  1.297    ||   6.467     ||  3.895&lt;br /&gt;
|-&lt;br /&gt;
|60_60_53   || 16.79     ||  1.734     ||  1.851    ||  0.9528    ||  0.9499    ||   1.729     ||  1.289    ||   6.731     ||  5.666&lt;br /&gt;
|-&lt;br /&gt;
|60_70_57   || 15.88     ||  1.829     ||  1.934    ||  0.9473    ||  0.9502    ||   1.737     ||  1.281    ||   5.736     ||  6.958&lt;br /&gt;
|-&lt;br /&gt;
|60_80_61   || 13.66     ||  1.918     ||  1.968    ||  0.9428    ||  0.9514    ||   1.745     ||  1.273    ||   2.622     ||  4.555&lt;br /&gt;
|-&lt;br /&gt;
|60_90_64   || 17.29     ||  2.009     ||  2.063    ||  0.9359    ||  0.9501    ||   1.753     ||  1.265    ||   2.640     ||  1.637&lt;br /&gt;
|-&lt;br /&gt;
|60_100_68  || 17.62     ||  2.049     ||  2.122    ||  0.9304    ||  0.9497    ||   1.760     ||  1.258    ||   3.560     ||  3.718&lt;br /&gt;
|-&lt;br /&gt;
|60_110_72  || 17.50     ||  2.118     ||  2.177    ||  0.9257    ||  0.9501    ||   1.767     ||  1.251    ||   2.811     ||  4.023&lt;br /&gt;
|-&lt;br /&gt;
|60_120_76  || 17.78     ||  2.174     ||  2.222    ||  0.9217    ||  0.9510    ||   1.774     ||  1.244    ||   2.209     ||  4.211&lt;br /&gt;
|-&lt;br /&gt;
|70_00_39   || 5.731     || 0.7825     || 0.7975    ||  0.9949    ||  0.9497    ||   1.675     ||  1.343    ||   1.908     || 0.2335&lt;br /&gt;
|-&lt;br /&gt;
|70_10_41   || 8.418     ||  1.009     ||  1.048    ||  0.9860    ||  0.9509    ||   1.688     ||  1.330    ||   3.845     || 0.6755&lt;br /&gt;
|-&lt;br /&gt;
|70_20_44   || 11.09     ||  1.201     ||  1.265    ||  0.9767    ||  0.9504    ||   1.699     ||  1.319    ||   5.345     ||  1.317&lt;br /&gt;
|-&lt;br /&gt;
|70_30_47   || 13.41     ||  1.361     ||  1.441    ||  0.9688    ||  0.9504    ||   1.709     ||  1.309    ||   5.859     ||  2.187&lt;br /&gt;
|-&lt;br /&gt;
|70_40_51   || 14.99     ||  1.496     ||  1.591    ||  0.9615    ||  0.9503    ||   1.718     ||  1.300    ||   6.348     ||  2.859&lt;br /&gt;
|-&lt;br /&gt;
|70_50_54   || 16.87     ||  1.617     ||  1.712    ||  0.9543    ||  0.9501    ||   1.727     ||  1.291    ||   5.843     ||  3.756&lt;br /&gt;
|-&lt;br /&gt;
|70_60_57   || 17.89     ||  1.718     ||  1.823    ||  0.9479    ||  0.9500    ||   1.735     ||  1.283    ||   6.140     ||  4.746&lt;br /&gt;
|-&lt;br /&gt;
|70_70_61   || 18.26     ||  1.812     ||  1.928    ||  0.9423    ||  0.9503    ||   1.743     ||  1.275    ||   6.353     ||  6.812&lt;br /&gt;
|-&lt;br /&gt;
|70_80_65   || 16.37     ||  1.896     ||  1.962    ||  0.9363    ||  0.9499    ||   1.751     ||  1.267    ||   3.469     ||  5.948&lt;br /&gt;
|-&lt;br /&gt;
|70_90_68   || 9.135     ||  1.980     ||  1.988    ||  0.9317    ||  0.9506    ||   1.758     ||  1.260    ||  0.3692     || 0.1186&lt;br /&gt;
|-&lt;br /&gt;
|70_100_72  || 18.64     ||  2.007     ||  2.094    ||  0.9267    ||  0.9506    ||   1.765     ||  1.253    ||   4.327     ||  3.356&lt;br /&gt;
|-&lt;br /&gt;
|70_110_76  || 18.23     ||  2.088     ||  2.147    ||  0.9219    ||  0.9507    ||   1.772     ||  1.246    ||   2.792     ||  3.707&lt;br /&gt;
|-&lt;br /&gt;
|70_120_80  || 17.89     ||  2.145     ||  2.184    ||  0.9171    ||  0.9506    ||   1.779     ||  1.239    ||   1.846     ||  4.043&lt;br /&gt;
|-&lt;br /&gt;
|80_00_42   ||7.247      ||0.8436      ||0.8697     || 0.9869     || 0.9497     ||  1.684      || 1.335     ||  3.094      ||0.2402&lt;br /&gt;
|-&lt;br /&gt;
|80_10_45   ||9.865      || 1.049      || 1.095     || 0.9794     || 0.9513     ||  1.695      || 1.323     ||  4.371      ||0.7359&lt;br /&gt;
|-&lt;br /&gt;
|80_20_48   ||12.28      || 1.226      || 1.290     || 0.9697     || 0.9500     ||  1.706      || 1.312     ||  5.206      || 1.327&lt;br /&gt;
|-&lt;br /&gt;
|80_30_51   ||14.38      || 1.370      || 1.454     || 0.9626     || 0.9503     ||  1.715      || 1.303     ||  6.088      || 2.102&lt;br /&gt;
|-&lt;br /&gt;
|80_40_54   ||16.47      || 1.500      || 1.594     || 0.9549     || 0.9497     ||  1.724      || 1.294     ||  6.263      || 2.799&lt;br /&gt;
|-&lt;br /&gt;
|80_50_58   ||17.63      || 1.612      || 1.706     || 0.9492     || 0.9503     ||  1.733      || 1.285     ||  5.842      || 3.329&lt;br /&gt;
|-&lt;br /&gt;
|80_60_61   ||18.84      || 1.712      || 1.814     || 0.9436     || 0.9507     ||  1.741      || 1.277     ||  5.984      || 3.990&lt;br /&gt;
|-&lt;br /&gt;
|80_70_65   ||19.27      || 1.799      || 1.898     || 0.9372     || 0.9501     ||  1.749      || 1.269     ||  5.555      || 4.728&lt;br /&gt;
|-&lt;br /&gt;
|80_80_69   ||17.96      || 1.880      || 1.935     || 0.9321     || 0.9503     ||  1.756      || 1.262     ||  2.921      || 3.774&lt;br /&gt;
|-&lt;br /&gt;
|80_90_73   ||13.42      || 1.957      || 1.982     || 0.9266     || 0.9500     ||  1.764      || 1.254     ||  1.312      ||0.6938&lt;br /&gt;
|-&lt;br /&gt;
|80_100_76  || 18.53     ||  2.008     ||  2.065    ||  0.9220    ||  0.9504    ||   1.770     ||  1.247    ||   2.839     ||  1.773&lt;br /&gt;
|-&lt;br /&gt;
|80_110_80  || 18.41     ||  2.059     ||  2.117    ||  0.9176    ||  0.9507    ||   1.777     ||  1.241    ||   2.847     ||  3.632&lt;br /&gt;
|-&lt;br /&gt;
|80_120_84  || 18.26     ||  2.117     ||  2.157    ||  0.9122    ||  0.9496    ||   1.784     ||  1.234    ||   1.872     ||  3.986&lt;br /&gt;
|-&lt;br /&gt;
|90_00_46   || 8.679     || 0.9022     || 0.9354    ||  0.9802    ||  0.9501    ||   1.691     ||  1.327    ||   3.678     || 0.3981&lt;br /&gt;
|-&lt;br /&gt;
|90_10_49   || 11.45     ||  1.090     ||  1.146    ||  0.9717    ||  0.9502    ||   1.702     ||  1.315    ||   5.148     || 0.8099&lt;br /&gt;
|-&lt;br /&gt;
|90_20_52   || 12.44     ||  1.247     ||  1.323    ||  0.9640    ||  0.9503    ||   1.712     ||  1.305    ||   6.100     ||  1.079&lt;br /&gt;
|-&lt;br /&gt;
|90_30_55   || 16.14     ||  1.383     ||  1.475    ||  0.9571    ||  0.9504    ||   1.722     ||  1.296    ||   6.607     ||  2.158&lt;br /&gt;
|-&lt;br /&gt;
|90_40_58   || 17.45     ||  1.506     ||  1.597    ||  0.9499    ||  0.9501    ||   1.731     ||  1.287    ||   6.012     ||  2.629&lt;br /&gt;
|-&lt;br /&gt;
|90_50_62   || 18.70     ||  1.609     ||  1.706    ||  0.9438    ||  0.9501    ||   1.739     ||  1.279    ||   6.003     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|90_60_65   || 18.77     ||  1.703     ||  1.789    ||  0.9381    ||  0.9502    ||   1.747     ||  1.271    ||   5.045     ||  3.047&lt;br /&gt;
|-&lt;br /&gt;
|90_70_69   || 18.43     ||  1.787     ||  1.852    ||  0.9324    ||  0.9500    ||   1.754     ||  1.263    ||   3.623     ||  3.117&lt;br /&gt;
|-&lt;br /&gt;
|90_80_73   || 17.72     ||  1.868     ||  1.909    ||  0.9269    ||  0.9497    ||   1.762     ||  1.256    ||   2.217     ||  2.354&lt;br /&gt;
|-&lt;br /&gt;
|90_90_76   || 14.40     ||  1.940     ||  1.956    ||  0.9221    ||  0.9499    ||   1.769     ||  1.249    ||  0.8079     || 0.8326&lt;br /&gt;
|-&lt;br /&gt;
|90_100_80  || 18.53     ||  2.009     ||  2.038    ||  0.9176    ||  0.9503    ||   1.776     ||  1.242    ||   1.484     ||  1.095&lt;br /&gt;
|-&lt;br /&gt;
|90_110_84  || 18.97     ||  2.021     ||  2.094    ||  0.9129    ||  0.9502    ||   1.783     ||  1.235    ||   3.625     ||  3.669&lt;br /&gt;
|-&lt;br /&gt;
|90_120_88  || 17.79     ||  2.090     ||  2.129    ||  0.9077    ||  0.9494    ||   1.789     ||  1.229    ||   1.827     ||  3.862&lt;br /&gt;
|-&lt;br /&gt;
|100_00_50  || 10.07     || 0.9544     || 0.9970    ||  0.9732    ||  0.9499    ||   1.699     ||  1.319    ||   4.471     || 0.4341&lt;br /&gt;
|-&lt;br /&gt;
|100_10_53  || 12.78     ||  1.127     ||  1.186    ||  0.9649    ||  0.9499    ||   1.710     ||  1.308    ||   5.262     || 0.9629&lt;br /&gt;
|-&lt;br /&gt;
|100_16_55  || 13.69     ||  1.215     ||  1.287    ||  0.9610    ||  0.9501    ||   1.715     ||  1.302    ||   5.901     ||  1.023&lt;br /&gt;
|-&lt;br /&gt;
|100_20_56  || 10.86     ||  1.271     ||  1.324    ||  0.9583    ||  0.9502    ||   1.719     ||  1.299    ||   4.120     || 0.8295&lt;br /&gt;
|-&lt;br /&gt;
|100_22_56  || 15.40     ||  1.309     ||  1.381    ||  0.9412    ||  0.9362    ||   1.722     ||  1.296    ||   5.552     ||  1.648&lt;br /&gt;
|-&lt;br /&gt;
|100_24_58  || 15.90     ||  1.326     ||  1.406    ||  0.9552    ||  0.9499    ||   1.722     ||  1.295    ||   6.105     ||  1.792&lt;br /&gt;
|-&lt;br /&gt;
|100_26_58  || 16.42     ||  1.352     ||  1.435    ||  0.9538    ||  0.9499    ||   1.724     ||  1.293    ||   6.137     ||  1.888&lt;br /&gt;
|-&lt;br /&gt;
|100_28_59  || 17.07     ||  1.375     ||  1.464    ||  0.9527    ||  0.9501    ||   1.726     ||  1.291    ||   6.475     ||  1.983&lt;br /&gt;
|-&lt;br /&gt;
|100_30_59  || 17.29     ||  1.398     ||  1.490    ||  0.9511    ||  0.9500    ||   1.728     ||  1.289    ||   6.561     ||  2.075&lt;br /&gt;
|-&lt;br /&gt;
|100_32_60  || 17.74     ||  1.423     ||  1.517    ||  0.9499    ||  0.9499    ||   1.730     ||  1.288    ||   6.596     ||  2.165&lt;br /&gt;
|-&lt;br /&gt;
|100_36_61  || 18.37     ||  1.467     ||  1.567    ||  0.9475    ||  0.9501    ||   1.733     ||  1.284    ||   6.819     ||  2.183&lt;br /&gt;
|-&lt;br /&gt;
|100_40_63  || 18.77     ||  1.509     ||  1.608    ||  0.9450    ||  0.9500    ||   1.736     ||  1.281    ||   6.553     ||  2.304&lt;br /&gt;
|-&lt;br /&gt;
|100_44_64  || 19.25     ||  1.551     ||  1.653    ||  0.9426    ||  0.9500    ||   1.740     ||  1.278    ||   6.569     ||  2.360&lt;br /&gt;
|-&lt;br /&gt;
|100_48_65  || 19.16     ||  1.591     ||  1.684    ||  0.9400    ||  0.9500    ||   1.743     ||  1.275    ||   5.807     ||  2.555&lt;br /&gt;
|-&lt;br /&gt;
|100_50_65  || 19.11     ||  1.613     ||  1.704    ||  0.9381    ||  0.9501    ||   1.745     ||  1.274    ||   5.628     ||  2.649&lt;br /&gt;
|-&lt;br /&gt;
|100_55_67  || 19.04     ||  1.659     ||  1.739    ||  0.9352    ||  0.9500    ||   1.749     ||  1.270    ||   4.839     ||  2.808&lt;br /&gt;
|-&lt;br /&gt;
|100_56_67  || 18.93     ||  1.667     ||  1.742    ||  0.9347    ||  0.9501    ||   1.750     ||  1.269    ||   4.522     ||  2.692&lt;br /&gt;
|-&lt;br /&gt;
|100_60_68  || 19.04     ||  1.702     ||  1.775    ||  0.9325    ||  0.9500    ||   1.753     ||  1.266    ||   4.326     ||  2.720&lt;br /&gt;
|-&lt;br /&gt;
|100_64_70  || 18.76     ||  1.733     ||  1.799    ||  0.9303    ||  0.9500    ||   1.756     ||  1.263    ||   3.774     ||  2.676&lt;br /&gt;
|-&lt;br /&gt;
|100_68_72  || 18.46     ||  1.771     ||  1.825    ||  0.9279    ||  0.9494    ||   1.759     ||  1.259    ||   3.080     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_70_73  || 18.23     ||  1.784     ||  1.841    ||  0.9277    ||  0.9500    ||   1.760     ||  1.258    ||   3.166     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_80_77  || 16.73     ||  1.855     ||  1.885    ||  0.9261    ||  0.9532    ||   1.767     ||  1.251    ||   1.617     ||  1.818&lt;br /&gt;
|-&lt;br /&gt;
|100_90_80  || 13.86     ||  1.931     ||  1.936    ||  0.9172    ||  0.9494    ||   1.774     ||  1.244    ||  0.2833     || 0.7382&lt;br /&gt;
|-&lt;br /&gt;
|100_95_82  || 11.27     ||  1.967     ||  1.964    ||  0.9243    ||  0.9582    ||   1.777     ||  1.241    || -0.1435     || 6.8954E-02&lt;br /&gt;
|-&lt;br /&gt;
|100_105_86 || 16.96     ||  2.019     ||  2.045    ||  0.9233    ||  0.9617    ||   1.783     ||  1.235    ||   1.268     ||  1.425&lt;br /&gt;
|-&lt;br /&gt;
|100_110_88 || 18.88     ||  2.020     ||  2.073    ||  0.9229    ||  0.9634    ||   1.786     ||  1.232    ||   2.618     ||  2.366&lt;br /&gt;
|-&lt;br /&gt;
|100_120_92 || 17.63     ||  2.064     ||  2.113    ||  0.9044    ||  0.9501    ||   1.794     ||  1.224    ||   2.379     ||  3.790&lt;br /&gt;
|-&lt;br /&gt;
|110_00_54  || 11.70     ||  1.006     ||  1.060    ||  0.9663    ||  0.9498    ||   1.706     ||  1.312    ||   5.370     || 0.4642&lt;br /&gt;
|-&lt;br /&gt;
|110_10_57  || 13.97     ||  1.160     ||  1.232    ||  0.9593    ||  0.9502    ||   1.716     ||  1.301    ||   6.136     || 0.8247&lt;br /&gt;
|-&lt;br /&gt;
|110_20_60  || 15.75     ||  1.298     ||  1.372    ||  0.9526    ||  0.9504    ||   1.726     ||  1.292    ||   5.739     ||  1.330&lt;br /&gt;
|-&lt;br /&gt;
|110_30_63  || 18.56     ||  1.415     ||  1.516    ||  0.9455    ||  0.9500    ||   1.734     ||  1.284    ||   7.122     ||  1.849&lt;br /&gt;
|-&lt;br /&gt;
|110_40_66  || 19.50     ||  1.521     ||  1.622    ||  0.9398    ||  0.9503    ||   1.743     ||  1.275    ||   6.602     ||  1.921&lt;br /&gt;
|-&lt;br /&gt;
|110_50_70  || 19.07     ||  1.618     ||  1.696    ||  0.9336    ||  0.9498    ||   1.751     ||  1.267    ||   4.873     ||  2.085&lt;br /&gt;
|-&lt;br /&gt;
|110_60_73  || 18.32     ||  1.702     ||  1.761    ||  0.9291    ||  0.9507    ||   1.758     ||  1.260    ||   3.471     ||  2.033&lt;br /&gt;
|-&lt;br /&gt;
|110_70_77  || 17.13     ||  1.782     ||  1.816    ||  0.9237    ||  0.9504    ||   1.766     ||  1.252    ||   1.948     ||  1.838&lt;br /&gt;
|-&lt;br /&gt;
|110_80_81  || 15.56     ||  1.853     ||  1.871    ||  0.9192    ||  0.9508    ||   1.773     ||  1.245    ||  0.9878     ||  1.332&lt;br /&gt;
|-&lt;br /&gt;
|110_90_84  || 13.12     ||  1.923     ||  1.926    ||  0.9142    ||  0.9506    ||   1.780     ||  1.238    ||  0.1639     || 0.5301&lt;br /&gt;
|-&lt;br /&gt;
|110_95_86  || 10.73     ||  1.963     ||  1.955    ||  0.9095    ||  0.9486    ||   1.783     ||  1.235    || -0.3746     || 8.1449E-04&lt;br /&gt;
|-&lt;br /&gt;
|110_110_92 || 17.29     ||  2.020     ||  2.055    ||  0.9056    ||  0.9509    ||   1.793     ||  1.225    ||   1.768     ||  2.045&lt;br /&gt;
|-&lt;br /&gt;
|110_120_95 || 17.55     ||  2.048     ||  2.095    ||  0.9014    ||  0.9510    ||   1.799     ||  1.219    ||   2.314     ||  3.774&lt;br /&gt;
|-&lt;br /&gt;
|120_00_57  || 13.14     ||  1.050     ||  1.117    ||  0.9599    ||  0.9497    ||   1.714     ||  1.305    ||   6.304     || 0.4861&lt;br /&gt;
|-&lt;br /&gt;
|120_10_60  || 14.81     ||  1.196     ||  1.268    ||  0.9534    ||  0.9501    ||   1.723     ||  1.295    ||   6.054     || 0.8382&lt;br /&gt;
|-&lt;br /&gt;
|120_20_63  || 17.57     ||  1.323     ||  1.409    ||  0.9458    ||  0.9494    ||   1.732     ||  1.286    ||   6.504     ||  1.409&lt;br /&gt;
|-&lt;br /&gt;
|120_30_67  || 19.50     ||  1.435     ||  1.539    ||  0.9407    ||  0.9503    ||   1.741     ||  1.277    ||   7.263     ||  1.529&lt;br /&gt;
|-&lt;br /&gt;
|120_40_70  || 19.38     ||  1.534     ||  1.621    ||  0.9335    ||  0.9492    ||   1.749     ||  1.269    ||   5.695     ||  1.632&lt;br /&gt;
|-&lt;br /&gt;
|120_50_74  || 18.34     ||  1.621     ||  1.684    ||  0.9294    ||  0.9503    ||   1.756     ||  1.262    ||   3.910     ||  1.864&lt;br /&gt;
|-&lt;br /&gt;
|120_60_77  || 17.24     ||  1.703     ||  1.743    ||  0.9246    ||  0.9507    ||   1.764     ||  1.254    ||   2.381     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|120_70_81  || 16.02     ||  1.780     ||  1.803    ||  0.9197    ||  0.9509    ||   1.771     ||  1.247    ||   1.312     ||  1.511&lt;br /&gt;
|-&lt;br /&gt;
|120_80_84  || 14.49     ||  1.850     ||  1.860    ||  0.9150    ||  0.9509    ||   1.778     ||  1.240    ||  0.5347     ||  1.076&lt;br /&gt;
|-&lt;br /&gt;
|120_90_88  || 12.18     ||  1.918     ||  1.918    ||  0.9096    ||  0.9501    ||   1.785     ||  1.233    || -4.1127E-02 || 0.3613&lt;br /&gt;
|-&lt;br /&gt;
|120_95_90  || 10.06     ||  1.957     ||  1.950    ||  0.9071    ||  0.9499    ||   1.788     ||  1.230    || -0.3241     ||  0.000&lt;br /&gt;
|-&lt;br /&gt;
|120_115_97 || 16.46     ||  2.020     ||  2.066    ||  0.8983    ||  0.9497    ||   1.801     ||  1.216    ||   2.258     ||  2.404&lt;br /&gt;
|-&lt;br /&gt;
|120_120_99 || 17.58     ||  2.008     ||  2.092    ||  0.8967    ||  0.9501    ||   1.804     ||  1.213    ||   4.186     ||  3.647&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Flexibility ==&lt;br /&gt;
&lt;br /&gt;
[[File:Flexibility TJ-II.png|300px|thumb|right|Flexibility diagram of TJ-II magnetic configurations. Several lines of constant rotational transform are highlighted and labelled with the corresponding central &amp;lt;math&amp;gt;\iota/2\pi&amp;lt;/math&amp;gt;-value.]]&lt;br /&gt;
TJ-II has considerable configurational flexibility, as observed in the &#039;flexibility diagram&#039;&amp;lt;ref&amp;gt;E. Ascasíbar, T. Estrada, F. Castejón, A. López-Fraguas, I. Pastor, J. Sánchez, U. Stroth, J. Qin and TJ-II Team, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/45/4/009|Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276–284]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
Some of this flexibility space has been explored, as in the &#039;magnetic well scan&#039; experiments&amp;lt;ref&amp;gt;A. de Aguilera, F. Castejón, E. Ascasíbar, et al. &#039;&#039;Magnetic well scan and confinement in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/55/11/113014|Nucl. Fusion, 55(11):113014, 2015]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
More recently, the rotational transform in the plasma edge region was found to be of importance for L-H confinement transitions&amp;lt;ref&amp;gt;B. P. van Milligen, T. Estrada, B. Carreras, L. García, and TJ-II Team. &#039;&#039;Importance of the rotational transform for L–H transitions in the TJ-II stellarator&#039;&#039;, [[doi:10.3390/plasma7020024|Plasma, 7(2):446–464, 2024]].&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8726</id>
		<title>TJ-II:Magnetic configuration</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8726"/>
		<updated>2026-10-07T16:25:16Z</updated>

		<summary type="html">&lt;p&gt;Admin: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The magnetic configuration of [[TJ-II]] in vacuum is completely determined by the currents flowing through the [[TJ-II:Coil system|external coils]].&lt;br /&gt;
Magnetic configurations are labelled as &#039;xxx_yy_zz&#039;, where&lt;br /&gt;
* &#039;xxx&#039;: 10 times the current (in kA) in the circular coil&lt;br /&gt;
* &#039;yy&#039;: 10 times the current (in kA) in the helical coil&lt;br /&gt;
* &#039;zz&#039;: 10 times the current (in kA) in the vertical field coils&lt;br /&gt;
The current in the toroidal field coils is not specified, as its value is adjusted to guarantee central absorption of the [[TJ-II:Electron Cyclotron Resonant Heating|Electron Cyclotron Resonant Heating]] source (requiring a specific &#039;resonant&#039; value of the magnetic field on the magnetic axis, &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
Configuration list:&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;width: 100%&amp;quot; border=&amp;quot;1&amp;quot;||&lt;br /&gt;
|-&lt;br /&gt;
! Configuration &lt;br /&gt;
! &amp;lt;math&amp;gt;r_{av}&amp;lt;/math&amp;gt; (cm) &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(0)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(a)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{m,av}&amp;lt;/math&amp;gt;(T) &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt; (T) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(0)&amp;lt;/math&amp;gt; (m) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(45)&amp;lt;/math&amp;gt; (m) &lt;br /&gt;
! Shear (%) &lt;br /&gt;
! Well (%)&lt;br /&gt;
|-&lt;br /&gt;
|0_20_13    ||1.139      || 1.185      || 1.194     ||  1.033     || 0.9504     ||  1.644      || 1.374     || 0.7793      ||5.7521E-02&lt;br /&gt;
|-&lt;br /&gt;
|0_30_15    ||4.228      || 1.518      || 1.698     ||  1.019     || 0.9500     ||  1.658      || 1.360     ||  11.85      || 1.050&lt;br /&gt;
|-&lt;br /&gt;
|0_40_18    ||5.903      || 1.756      || 2.003     ||  1.008     || 0.9505     ||  1.671      || 1.347     ||  14.09      || 1.217&lt;br /&gt;
|-&lt;br /&gt;
|0_50_22    ||6.480      || 1.936      || 2.230     || 0.9973     || 0.9502     ||  1.682      || 1.336     ||  15.17      || 2.481&lt;br /&gt;
|-&lt;br /&gt;
|0_60_26    ||8.500      || 2.073      || 2.399     || 0.9885     || 0.9502     ||  1.692      || 1.326     ||  15.70      || 3.218&lt;br /&gt;
|-&lt;br /&gt;
|0_70_29    ||7.147      || 2.187      || 2.434     || 0.9805     || 0.9503     ||  1.701      || 1.317     ||  11.30      || 2.985&lt;br /&gt;
|-&lt;br /&gt;
|0_80_34    ||6.902      || 2.284      || 2.469     || 0.9736     || 0.9506     ||  1.710      || 1.308     ||  8.084      || 2.735&lt;br /&gt;
|-&lt;br /&gt;
|0_90_38    ||6.738      || 2.366      || 2.514     || 0.9663     || 0.9503     ||  1.719      || 1.299     ||  6.269      || 2.534&lt;br /&gt;
|-&lt;br /&gt;
|0_100_42   ||12.59      || 2.436      || 2.667     || 0.9601     || 0.9505     ||  1.727      || 1.291     ||  9.493      || 4.643&lt;br /&gt;
|-&lt;br /&gt;
|0_110_46   ||10.67      || 2.493      || 2.667     || 0.9539     || 0.9503     ||  1.734      || 1.284     ||  6.980      || 4.554&lt;br /&gt;
|-&lt;br /&gt;
|0_120_50   ||12.71      || 2.548      || 2.667     || 0.9482     || 0.9504     ||  1.742      || 1.276     ||  4.683      || 4.272&lt;br /&gt;
|-&lt;br /&gt;
|10_20_18   || 2.557     ||  1.148     ||  1.184    ||   1.024    ||  0.9514    ||   1.652     ||  1.366    ||   3.183     || 0.2469&lt;br /&gt;
|-&lt;br /&gt;
|10_30_20   || 6.083     ||  1.438     ||  1.602    ||   1.010    ||  0.9501    ||   1.666     ||  1.352    ||   11.35     ||  1.398&lt;br /&gt;
|-&lt;br /&gt;
|10_40_24   || 6.921     ||  1.659     ||  1.880    ||   1.000    ||  0.9504    ||   1.678     ||  1.340    ||   13.34     ||  2.751&lt;br /&gt;
|-&lt;br /&gt;
|10_50_27   || 8.140     ||  1.826     ||  1.997    ||  0.9909    ||  0.9504    ||   1.688     ||  1.329    ||   9.321     ||  3.241&lt;br /&gt;
|-&lt;br /&gt;
|10_60_31   || 9.350     ||  1.965     ||  2.183    ||  0.9826    ||  0.9505    ||   1.698     ||  1.319    ||   11.11     ||  3.084&lt;br /&gt;
|-&lt;br /&gt;
|10_70_35   || 10.10     ||  2.077     ||  2.288    ||  0.9750    ||  0.9505    ||   1.707     ||  1.310    ||   10.16     ||  3.597&lt;br /&gt;
|-&lt;br /&gt;
|10_80_38   || 9.810     ||  2.174     ||  2.371    ||  0.9674    ||  0.9502    ||   1.716     ||  1.302    ||   9.037     ||  3.908&lt;br /&gt;
|-&lt;br /&gt;
|10_90_42   || 10.54     ||  2.257     ||  2.434    ||  0.9610    ||  0.9503    ||   1.724     ||  1.294    ||   7.851     ||  4.281&lt;br /&gt;
|-&lt;br /&gt;
|10_100_47  || 10.21     ||  2.327     ||  2.482    ||  0.9546    ||  0.9502    ||   1.732     ||  1.286    ||   6.647     ||  4.236&lt;br /&gt;
|-&lt;br /&gt;
|10_110_51  || 11.11     ||  2.395     ||  2.547    ||  0.9488    ||  0.9501    ||   1.740     ||  1.278    ||   6.331     ||  5.121&lt;br /&gt;
|-&lt;br /&gt;
|10_120_55  || 10.04     ||  2.451     ||  2.565    ||  0.9432    ||  0.9502    ||   1.747     ||  1.271    ||   4.674     ||  4.426&lt;br /&gt;
|-&lt;br /&gt;
|20_10_21   || 1.213     || 0.7902     || 0.7956    ||   1.028    ||  0.9503    ||   1.645     ||  1.373    ||  0.6830     || 3.7624E-02&lt;br /&gt;
|-&lt;br /&gt;
|20_20_22   || 3.952     ||  1.136     ||  1.185    ||   1.014    ||  0.9500    ||   1.661     ||  1.357    ||   4.350     || 0.4717&lt;br /&gt;
|-&lt;br /&gt;
|20_30_25   || 6.779     ||  1.395     ||  1.521    ||   1.003    ||  0.9502    ||   1.673     ||  1.344    ||   9.049     ||  1.550&lt;br /&gt;
|-&lt;br /&gt;
|20_40_28   || 8.475     ||  1.592     ||  1.771    ||  0.9922    ||  0.9498    ||   1.685     ||  1.333    ||   11.25     ||  2.879&lt;br /&gt;
|-&lt;br /&gt;
|20_50_32   || 8.039     ||  1.756     ||  1.906    ||  0.9842    ||  0.9505    ||   1.695     ||  1.323    ||   8.571     ||  3.131&lt;br /&gt;
|-&lt;br /&gt;
|20_60_35   || 11.21     ||  1.884     ||  1.997    ||  0.9755    ||  0.9498    ||   1.705     ||  1.313    ||   5.968     ||  1.980&lt;br /&gt;
|-&lt;br /&gt;
|20_70_39   || 11.08     ||  1.994     ||  2.154    ||  0.9689    ||  0.9504    ||   1.714     ||  1.304    ||   7.982     ||  3.385&lt;br /&gt;
|-&lt;br /&gt;
|20_80_43   || 12.14     ||  2.092     ||  2.255    ||  0.9614    ||  0.9497    ||   1.722     ||  1.296    ||   7.811     ||  4.133&lt;br /&gt;
|-&lt;br /&gt;
|20_90_47   || 12.83     ||  2.174     ||  2.324    ||  0.9558    ||  0.9503    ||   1.730     ||  1.288    ||   6.862     ||  4.713&lt;br /&gt;
|-&lt;br /&gt;
|20_100_51  || 12.68     ||  2.246     ||  2.379    ||  0.9498    ||  0.9503    ||   1.738     ||  1.280    ||   5.945     ||  4.930&lt;br /&gt;
|-&lt;br /&gt;
|20_110_55  || 13.79     ||  2.313     ||  2.434    ||  0.9443    ||  0.9505    ||   1.745     ||  1.273    ||   5.248     ||  5.117&lt;br /&gt;
|-&lt;br /&gt;
|20_120_59  || 13.91     ||  2.368     ||  2.483    ||  0.9386    ||  0.9502    ||   1.752     ||  1.265    ||   4.822     ||  5.418&lt;br /&gt;
|-&lt;br /&gt;
|30_10_25   || 2.709     || 0.8385     || 0.8507    ||   1.018    ||  0.9501    ||   1.654     ||  1.363    ||   1.452     || 0.1431&lt;br /&gt;
|-&lt;br /&gt;
|30_20_27   || 5.443     ||  1.134     ||  1.189    ||   1.007    ||  0.9514    ||   1.669     ||  1.349    ||   4.847     || 0.7001&lt;br /&gt;
|-&lt;br /&gt;
|30_30_30   || 8.180     ||  1.368     ||  1.481    ||  0.9956    ||  0.9506    ||   1.681     ||  1.337    ||   8.332     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|30_40_33   || 9.756     ||  1.550     ||  1.687    ||  0.9860    ||  0.9503    ||   1.692     ||  1.326    ||   8.877     ||  2.798&lt;br /&gt;
|-&lt;br /&gt;
|30_50_37   || 11.16     ||  1.702     ||  1.878    ||  0.9779    ||  0.9503    ||   1.702     ||  1.316    ||   10.37     ||  4.941&lt;br /&gt;
|-&lt;br /&gt;
|30_60_40   || 9.262     ||  1.827     ||  1.936    ||  0.9706    ||  0.9505    ||   1.711     ||  1.307    ||   5.952     ||  3.624&lt;br /&gt;
|-&lt;br /&gt;
|30_70_44   || 12.28     ||  1.937     ||  2.007    ||  0.9631    ||  0.9502    ||   1.720     ||  1.298    ||   3.593     ||  4.431&lt;br /&gt;
|-&lt;br /&gt;
|30_80_48   || 13.28     ||  2.033     ||  2.149    ||  0.9567    ||  0.9502    ||   1.728     ||  1.290    ||   5.702     ||  3.674&lt;br /&gt;
|-&lt;br /&gt;
|30_90_52   || 14.16     ||  2.115     ||  2.231    ||  0.9504    ||  0.9501    ||   1.736     ||  1.282    ||   5.476     ||  4.227&lt;br /&gt;
|-&lt;br /&gt;
|30_100_56  || 14.97     ||  2.187     ||  2.295    ||  0.9448    ||  0.9502    ||   1.743     ||  1.275    ||   4.949     ||  4.755&lt;br /&gt;
|-&lt;br /&gt;
|30_110_59  || 15.76     ||  2.246     ||  2.356    ||  0.9391    ||  0.9500    ||   1.751     ||  1.267    ||   4.920     ||  5.215&lt;br /&gt;
|-&lt;br /&gt;
|30_120_63  || 14.48     ||  2.306     ||  2.389    ||  0.9343    ||  0.9504    ||   1.758     ||  1.260    ||   3.573     ||  5.025&lt;br /&gt;
|-&lt;br /&gt;
|40_00_27   || 1.350     || 0.5464     || 0.5471    ||   1.024    ||  0.9504    ||   1.647     ||  1.371    ||  0.1331     || 2.4768E-02&lt;br /&gt;
|-&lt;br /&gt;
|40_10_29   || 4.111     || 0.8821     || 0.9010    ||   1.010    ||  0.9510    ||   1.663     ||  1.355    ||   2.152     || 0.2456&lt;br /&gt;
|-&lt;br /&gt;
|40_20_31   || 6.646     ||  1.146     ||  1.202    ||  0.9975    ||  0.9501    ||   1.677     ||  1.341    ||   4.928     || 0.8185&lt;br /&gt;
|-&lt;br /&gt;
|40_30_34   || 9.328     ||  1.354     ||  1.452    ||  0.9884    ||  0.9506    ||   1.688     ||  1.330    ||   7.247     ||  1.826&lt;br /&gt;
|-&lt;br /&gt;
|40_40_37   || 11.15     ||  1.523     ||  1.646    ||  0.9788    ||  0.9498    ||   1.699     ||  1.319    ||   8.061     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|40_50_41   || 12.66     ||  1.666     ||  1.797    ||  0.9719    ||  0.9506    ||   1.708     ||  1.310    ||   7.872     ||  4.310&lt;br /&gt;
|-&lt;br /&gt;
|40_60_44   || 12.34     ||  1.786     ||  1.927    ||  0.9637    ||  0.9497    ||   1.717     ||  1.301    ||   7.879     ||  5.834&lt;br /&gt;
|-&lt;br /&gt;
|40_70_48   || 9.734     ||  1.894     ||  1.963    ||  0.9579    ||  0.9504    ||   1.726     ||  1.292    ||   3.625     ||  3.668&lt;br /&gt;
|-&lt;br /&gt;
|40_80_52   || 13.96     ||  1.986     ||  2.067    ||  0.9515    ||  0.9503    ||   1.734     ||  1.284    ||   4.054     ||  3.028&lt;br /&gt;
|-&lt;br /&gt;
|40_90_56   || 15.39     ||  2.062     ||  2.156    ||  0.9457    ||  0.9504    ||   1.741     ||  1.277    ||   4.529     ||  3.841&lt;br /&gt;
|-&lt;br /&gt;
|40_100_60  || 16.40     ||  2.132     ||  2.232    ||  0.9400    ||  0.9502    ||   1.749     ||  1.269    ||   4.683     ||  4.355&lt;br /&gt;
|-&lt;br /&gt;
|40_110_64  || 18.12     ||  2.199     ||  2.288    ||  0.9348    ||  0.9503    ||   1.756     ||  1.262    ||   4.049     ||  4.651&lt;br /&gt;
|-&lt;br /&gt;
|40_120_68  || 16.81     ||  2.256     ||  2.327    ||  0.9295    ||  0.9501    ||   1.763     ||  1.255    ||   3.158     ||  4.904&lt;br /&gt;
|-&lt;br /&gt;
|50_00_31   || 2.818     || 0.6329     || 0.6375    ||   1.013    ||  0.9498    ||   1.657     ||  1.361    ||  0.7286     || 6.1871E-02&lt;br /&gt;
|-&lt;br /&gt;
|50_10_33   || 5.588     || 0.9254     || 0.9532    ||   1.001    ||  0.9506    ||   1.672     ||  1.346    ||   3.003     || 0.3605&lt;br /&gt;
|-&lt;br /&gt;
|50_20_36   || 8.222     ||  1.160     ||  1.216    ||  0.9902    ||  0.9502    ||   1.684     ||  1.334    ||   4.838     ||  1.060&lt;br /&gt;
|-&lt;br /&gt;
|50_30_39   || 10.67     ||  1.352     ||  1.435    ||  0.9815    ||  0.9505    ||   1.695     ||  1.323    ||   6.163     ||  2.008&lt;br /&gt;
|-&lt;br /&gt;
|50_40_42   || 12.44     ||  1.508     ||  1.609    ||  0.9733    ||  0.9504    ||   1.705     ||  1.313    ||   6.719     ||  2.910&lt;br /&gt;
|-&lt;br /&gt;
|50_50_46   || 13.94     ||  1.644     ||  1.758    ||  0.9661    ||  0.9505    ||   1.714     ||  1.303    ||   6.944     ||  4.001&lt;br /&gt;
|-&lt;br /&gt;
|50_60_49   || 15.09     ||  1.757     ||  1.887    ||  0.9587    ||  0.9502    ||   1.723     ||  1.295    ||   7.390     ||  6.217&lt;br /&gt;
|-&lt;br /&gt;
|50_70_53   || 13.03     ||  1.855     ||  1.955    ||  0.9524    ||  0.9502    ||   1.731     ||  1.287    ||   5.353     ||  5.830&lt;br /&gt;
|-&lt;br /&gt;
|50_80_56   || 16.73     ||  1.949     ||  2.004    ||  0.9463    ||  0.9501    ||   1.739     ||  1.279    ||   2.807     ||  4.003&lt;br /&gt;
|-&lt;br /&gt;
|50_90_60   || 16.70     ||  2.011     ||  2.101    ||  0.9407    ||  0.9502    ||   1.747     ||  1.271    ||   4.501     ||  3.444&lt;br /&gt;
|-&lt;br /&gt;
|50_100_64  || 18.15     ||  2.090     ||  2.183    ||  0.9351    ||  0.9500    ||   1.754     ||  1.264    ||   4.434     ||  3.907&lt;br /&gt;
|-&lt;br /&gt;
|50_110_68  || 17.53     ||  2.154     ||  2.223    ||  0.9297    ||  0.9498    ||   1.762     ||  1.256    ||   3.205     ||  4.270&lt;br /&gt;
|-&lt;br /&gt;
|50_120_72  || 19.13     ||  2.213     ||  2.288    ||  0.9250    ||  0.9501    ||   1.768     ||  1.250    ||   3.417     ||  4.378&lt;br /&gt;
|-&lt;br /&gt;
|60_00_35   || 4.247     || 0.7126     || 0.7205    ||   1.003    ||  0.9498    ||   1.667     ||  1.352    ||   1.108     || 0.1270&lt;br /&gt;
|-&lt;br /&gt;
|60_10_37   || 6.862     || 0.9679     ||  1.002    ||  0.9934    ||  0.9509    ||   1.680     ||  1.338    ||   3.520     || 0.4827&lt;br /&gt;
|-&lt;br /&gt;
|60_20_40   || 9.669     ||  1.179     ||  1.240    ||  0.9831    ||  0.9503    ||   1.692     ||  1.326    ||   5.202     ||  1.236&lt;br /&gt;
|-&lt;br /&gt;
|60_30_43   || 12.01     ||  1.354     ||  1.435    ||  0.9747    ||  0.9502    ||   1.702     ||  1.316    ||   5.973     ||  2.132&lt;br /&gt;
|-&lt;br /&gt;
|60_40_46   || 13.48     ||  1.500     ||  1.593    ||  0.9672    ||  0.9503    ||   1.712     ||  1.306    ||   6.170     ||  2.806&lt;br /&gt;
|-&lt;br /&gt;
|60_50_50   || 15.36     ||  1.627     ||  1.732    ||  0.9601    ||  0.9504    ||   1.721     ||  1.297    ||   6.467     ||  3.895&lt;br /&gt;
|-&lt;br /&gt;
|60_60_53   || 16.79     ||  1.734     ||  1.851    ||  0.9528    ||  0.9499    ||   1.729     ||  1.289    ||   6.731     ||  5.666&lt;br /&gt;
|-&lt;br /&gt;
|60_70_57   || 15.88     ||  1.829     ||  1.934    ||  0.9473    ||  0.9502    ||   1.737     ||  1.281    ||   5.736     ||  6.958&lt;br /&gt;
|-&lt;br /&gt;
|60_80_61   || 13.66     ||  1.918     ||  1.968    ||  0.9428    ||  0.9514    ||   1.745     ||  1.273    ||   2.622     ||  4.555&lt;br /&gt;
|-&lt;br /&gt;
|60_90_64   || 17.29     ||  2.009     ||  2.063    ||  0.9359    ||  0.9501    ||   1.753     ||  1.265    ||   2.640     ||  1.637&lt;br /&gt;
|-&lt;br /&gt;
|60_100_68  || 17.62     ||  2.049     ||  2.122    ||  0.9304    ||  0.9497    ||   1.760     ||  1.258    ||   3.560     ||  3.718&lt;br /&gt;
|-&lt;br /&gt;
|60_110_72  || 17.50     ||  2.118     ||  2.177    ||  0.9257    ||  0.9501    ||   1.767     ||  1.251    ||   2.811     ||  4.023&lt;br /&gt;
|-&lt;br /&gt;
|60_120_76  || 17.78     ||  2.174     ||  2.222    ||  0.9217    ||  0.9510    ||   1.774     ||  1.244    ||   2.209     ||  4.211&lt;br /&gt;
|-&lt;br /&gt;
|70_00_39   || 5.731     || 0.7825     || 0.7975    ||  0.9949    ||  0.9497    ||   1.675     ||  1.343    ||   1.908     || 0.2335&lt;br /&gt;
|-&lt;br /&gt;
|70_10_41   || 8.418     ||  1.009     ||  1.048    ||  0.9860    ||  0.9509    ||   1.688     ||  1.330    ||   3.845     || 0.6755&lt;br /&gt;
|-&lt;br /&gt;
|70_20_44   || 11.09     ||  1.201     ||  1.265    ||  0.9767    ||  0.9504    ||   1.699     ||  1.319    ||   5.345     ||  1.317&lt;br /&gt;
|-&lt;br /&gt;
|70_30_47   || 13.41     ||  1.361     ||  1.441    ||  0.9688    ||  0.9504    ||   1.709     ||  1.309    ||   5.859     ||  2.187&lt;br /&gt;
|-&lt;br /&gt;
|70_40_51   || 14.99     ||  1.496     ||  1.591    ||  0.9615    ||  0.9503    ||   1.718     ||  1.300    ||   6.348     ||  2.859&lt;br /&gt;
|-&lt;br /&gt;
|70_50_54   || 16.87     ||  1.617     ||  1.712    ||  0.9543    ||  0.9501    ||   1.727     ||  1.291    ||   5.843     ||  3.756&lt;br /&gt;
|-&lt;br /&gt;
|70_60_57   || 17.89     ||  1.718     ||  1.823    ||  0.9479    ||  0.9500    ||   1.735     ||  1.283    ||   6.140     ||  4.746&lt;br /&gt;
|-&lt;br /&gt;
|70_70_61   || 18.26     ||  1.812     ||  1.928    ||  0.9423    ||  0.9503    ||   1.743     ||  1.275    ||   6.353     ||  6.812&lt;br /&gt;
|-&lt;br /&gt;
|70_80_65   || 16.37     ||  1.896     ||  1.962    ||  0.9363    ||  0.9499    ||   1.751     ||  1.267    ||   3.469     ||  5.948&lt;br /&gt;
|-&lt;br /&gt;
|70_90_68   || 9.135     ||  1.980     ||  1.988    ||  0.9317    ||  0.9506    ||   1.758     ||  1.260    ||  0.3692     || 0.1186&lt;br /&gt;
|-&lt;br /&gt;
|70_100_72  || 18.64     ||  2.007     ||  2.094    ||  0.9267    ||  0.9506    ||   1.765     ||  1.253    ||   4.327     ||  3.356&lt;br /&gt;
|-&lt;br /&gt;
|70_110_76  || 18.23     ||  2.088     ||  2.147    ||  0.9219    ||  0.9507    ||   1.772     ||  1.246    ||   2.792     ||  3.707&lt;br /&gt;
|-&lt;br /&gt;
|70_120_80  || 17.89     ||  2.145     ||  2.184    ||  0.9171    ||  0.9506    ||   1.779     ||  1.239    ||   1.846     ||  4.043&lt;br /&gt;
|-&lt;br /&gt;
|80_00_42   ||7.247      ||0.8436      ||0.8697     || 0.9869     || 0.9497     ||  1.684      || 1.335     ||  3.094      ||0.2402&lt;br /&gt;
|-&lt;br /&gt;
|80_10_45   ||9.865      || 1.049      || 1.095     || 0.9794     || 0.9513     ||  1.695      || 1.323     ||  4.371      ||0.7359&lt;br /&gt;
|-&lt;br /&gt;
|80_20_48   ||12.28      || 1.226      || 1.290     || 0.9697     || 0.9500     ||  1.706      || 1.312     ||  5.206      || 1.327&lt;br /&gt;
|-&lt;br /&gt;
|80_30_51   ||14.38      || 1.370      || 1.454     || 0.9626     || 0.9503     ||  1.715      || 1.303     ||  6.088      || 2.102&lt;br /&gt;
|-&lt;br /&gt;
|80_40_54   ||16.47      || 1.500      || 1.594     || 0.9549     || 0.9497     ||  1.724      || 1.294     ||  6.263      || 2.799&lt;br /&gt;
|-&lt;br /&gt;
|80_50_58   ||17.63      || 1.612      || 1.706     || 0.9492     || 0.9503     ||  1.733      || 1.285     ||  5.842      || 3.329&lt;br /&gt;
|-&lt;br /&gt;
|80_60_61   ||18.84      || 1.712      || 1.814     || 0.9436     || 0.9507     ||  1.741      || 1.277     ||  5.984      || 3.990&lt;br /&gt;
|-&lt;br /&gt;
|80_70_65   ||19.27      || 1.799      || 1.898     || 0.9372     || 0.9501     ||  1.749      || 1.269     ||  5.555      || 4.728&lt;br /&gt;
|-&lt;br /&gt;
|80_80_69   ||17.96      || 1.880      || 1.935     || 0.9321     || 0.9503     ||  1.756      || 1.262     ||  2.921      || 3.774&lt;br /&gt;
|-&lt;br /&gt;
|80_90_73   ||13.42      || 1.957      || 1.982     || 0.9266     || 0.9500     ||  1.764      || 1.254     ||  1.312      ||0.6938&lt;br /&gt;
|-&lt;br /&gt;
|80_100_76  || 18.53     ||  2.008     ||  2.065    ||  0.9220    ||  0.9504    ||   1.770     ||  1.247    ||   2.839     ||  1.773&lt;br /&gt;
|-&lt;br /&gt;
|80_110_80  || 18.41     ||  2.059     ||  2.117    ||  0.9176    ||  0.9507    ||   1.777     ||  1.241    ||   2.847     ||  3.632&lt;br /&gt;
|-&lt;br /&gt;
|80_120_84  || 18.26     ||  2.117     ||  2.157    ||  0.9122    ||  0.9496    ||   1.784     ||  1.234    ||   1.872     ||  3.986&lt;br /&gt;
|-&lt;br /&gt;
|90_00_46   || 8.679     || 0.9022     || 0.9354    ||  0.9802    ||  0.9501    ||   1.691     ||  1.327    ||   3.678     || 0.3981&lt;br /&gt;
|-&lt;br /&gt;
|90_10_49   || 11.45     ||  1.090     ||  1.146    ||  0.9717    ||  0.9502    ||   1.702     ||  1.315    ||   5.148     || 0.8099&lt;br /&gt;
|-&lt;br /&gt;
|90_20_52   || 12.44     ||  1.247     ||  1.323    ||  0.9640    ||  0.9503    ||   1.712     ||  1.305    ||   6.100     ||  1.079&lt;br /&gt;
|-&lt;br /&gt;
|90_30_55   || 16.14     ||  1.383     ||  1.475    ||  0.9571    ||  0.9504    ||   1.722     ||  1.296    ||   6.607     ||  2.158&lt;br /&gt;
|-&lt;br /&gt;
|90_40_58   || 17.45     ||  1.506     ||  1.597    ||  0.9499    ||  0.9501    ||   1.731     ||  1.287    ||   6.012     ||  2.629&lt;br /&gt;
|-&lt;br /&gt;
|90_50_62   || 18.70     ||  1.609     ||  1.706    ||  0.9438    ||  0.9501    ||   1.739     ||  1.279    ||   6.003     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|90_60_65   || 18.77     ||  1.703     ||  1.789    ||  0.9381    ||  0.9502    ||   1.747     ||  1.271    ||   5.045     ||  3.047&lt;br /&gt;
|-&lt;br /&gt;
|90_70_69   || 18.43     ||  1.787     ||  1.852    ||  0.9324    ||  0.9500    ||   1.754     ||  1.263    ||   3.623     ||  3.117&lt;br /&gt;
|-&lt;br /&gt;
|90_80_73   || 17.72     ||  1.868     ||  1.909    ||  0.9269    ||  0.9497    ||   1.762     ||  1.256    ||   2.217     ||  2.354&lt;br /&gt;
|-&lt;br /&gt;
|90_90_76   || 14.40     ||  1.940     ||  1.956    ||  0.9221    ||  0.9499    ||   1.769     ||  1.249    ||  0.8079     || 0.8326&lt;br /&gt;
|-&lt;br /&gt;
|90_100_80  || 18.53     ||  2.009     ||  2.038    ||  0.9176    ||  0.9503    ||   1.776     ||  1.242    ||   1.484     ||  1.095&lt;br /&gt;
|-&lt;br /&gt;
|90_110_84  || 18.97     ||  2.021     ||  2.094    ||  0.9129    ||  0.9502    ||   1.783     ||  1.235    ||   3.625     ||  3.669&lt;br /&gt;
|-&lt;br /&gt;
|90_120_88  || 17.79     ||  2.090     ||  2.129    ||  0.9077    ||  0.9494    ||   1.789     ||  1.229    ||   1.827     ||  3.862&lt;br /&gt;
|-&lt;br /&gt;
|100_00_50  || 10.07     || 0.9544     || 0.9970    ||  0.9732    ||  0.9499    ||   1.699     ||  1.319    ||   4.471     || 0.4341&lt;br /&gt;
|-&lt;br /&gt;
|100_10_53  || 12.78     ||  1.127     ||  1.186    ||  0.9649    ||  0.9499    ||   1.710     ||  1.308    ||   5.262     || 0.9629&lt;br /&gt;
|-&lt;br /&gt;
|100_16_55  || 13.69     ||  1.215     ||  1.287    ||  0.9610    ||  0.9501    ||   1.715     ||  1.302    ||   5.901     ||  1.023&lt;br /&gt;
|-&lt;br /&gt;
|100_20_56  || 10.86     ||  1.271     ||  1.324    ||  0.9583    ||  0.9502    ||   1.719     ||  1.299    ||   4.120     || 0.8295&lt;br /&gt;
|-&lt;br /&gt;
|100_22_56  || 15.40     ||  1.309     ||  1.381    ||  0.9412    ||  0.9362    ||   1.722     ||  1.296    ||   5.552     ||  1.648&lt;br /&gt;
|-&lt;br /&gt;
|100_24_58  || 15.90     ||  1.326     ||  1.406    ||  0.9552    ||  0.9499    ||   1.722     ||  1.295    ||   6.105     ||  1.792&lt;br /&gt;
|-&lt;br /&gt;
|100_26_58  || 16.42     ||  1.352     ||  1.435    ||  0.9538    ||  0.9499    ||   1.724     ||  1.293    ||   6.137     ||  1.888&lt;br /&gt;
|-&lt;br /&gt;
|100_28_59  || 17.07     ||  1.375     ||  1.464    ||  0.9527    ||  0.9501    ||   1.726     ||  1.291    ||   6.475     ||  1.983&lt;br /&gt;
|-&lt;br /&gt;
|100_30_59  || 17.29     ||  1.398     ||  1.490    ||  0.9511    ||  0.9500    ||   1.728     ||  1.289    ||   6.561     ||  2.075&lt;br /&gt;
|-&lt;br /&gt;
|100_32_60  || 17.74     ||  1.423     ||  1.517    ||  0.9499    ||  0.9499    ||   1.730     ||  1.288    ||   6.596     ||  2.165&lt;br /&gt;
|-&lt;br /&gt;
|100_36_61  || 18.37     ||  1.467     ||  1.567    ||  0.9475    ||  0.9501    ||   1.733     ||  1.284    ||   6.819     ||  2.183&lt;br /&gt;
|-&lt;br /&gt;
|100_40_63  || 18.77     ||  1.509     ||  1.608    ||  0.9450    ||  0.9500    ||   1.736     ||  1.281    ||   6.553     ||  2.304&lt;br /&gt;
|-&lt;br /&gt;
|100_44_64  || 19.25     ||  1.551     ||  1.653    ||  0.9426    ||  0.9500    ||   1.740     ||  1.278    ||   6.569     ||  2.360&lt;br /&gt;
|-&lt;br /&gt;
|100_48_65  || 19.16     ||  1.591     ||  1.684    ||  0.9400    ||  0.9500    ||   1.743     ||  1.275    ||   5.807     ||  2.555&lt;br /&gt;
|-&lt;br /&gt;
|100_50_65  || 19.11     ||  1.613     ||  1.704    ||  0.9381    ||  0.9501    ||   1.745     ||  1.274    ||   5.628     ||  2.649&lt;br /&gt;
|-&lt;br /&gt;
|100_55_67  || 19.04     ||  1.659     ||  1.739    ||  0.9352    ||  0.9500    ||   1.749     ||  1.270    ||   4.839     ||  2.808&lt;br /&gt;
|-&lt;br /&gt;
|100_56_67  || 18.93     ||  1.667     ||  1.742    ||  0.9347    ||  0.9501    ||   1.750     ||  1.269    ||   4.522     ||  2.692&lt;br /&gt;
|-&lt;br /&gt;
|100_60_68  || 19.04     ||  1.702     ||  1.775    ||  0.9325    ||  0.9500    ||   1.753     ||  1.266    ||   4.326     ||  2.720&lt;br /&gt;
|-&lt;br /&gt;
|100_64_70  || 18.76     ||  1.733     ||  1.799    ||  0.9303    ||  0.9500    ||   1.756     ||  1.263    ||   3.774     ||  2.676&lt;br /&gt;
|-&lt;br /&gt;
|100_68_72  || 18.46     ||  1.771     ||  1.825    ||  0.9279    ||  0.9494    ||   1.759     ||  1.259    ||   3.080     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_70_73  || 18.23     ||  1.784     ||  1.841    ||  0.9277    ||  0.9500    ||   1.760     ||  1.258    ||   3.166     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_80_77  || 16.73     ||  1.855     ||  1.885    ||  0.9261    ||  0.9532    ||   1.767     ||  1.251    ||   1.617     ||  1.818&lt;br /&gt;
|-&lt;br /&gt;
|100_90_80  || 13.86     ||  1.931     ||  1.936    ||  0.9172    ||  0.9494    ||   1.774     ||  1.244    ||  0.2833     || 0.7382&lt;br /&gt;
|-&lt;br /&gt;
|100_95_82  || 11.27     ||  1.967     ||  1.964    ||  0.9243    ||  0.9582    ||   1.777     ||  1.241    || -0.1435     || 6.8954E-02&lt;br /&gt;
|-&lt;br /&gt;
|100_105_86 || 16.96     ||  2.019     ||  2.045    ||  0.9233    ||  0.9617    ||   1.783     ||  1.235    ||   1.268     ||  1.425&lt;br /&gt;
|-&lt;br /&gt;
|100_110_88 || 18.88     ||  2.020     ||  2.073    ||  0.9229    ||  0.9634    ||   1.786     ||  1.232    ||   2.618     ||  2.366&lt;br /&gt;
|-&lt;br /&gt;
|100_120_92 || 17.63     ||  2.064     ||  2.113    ||  0.9044    ||  0.9501    ||   1.794     ||  1.224    ||   2.379     ||  3.790&lt;br /&gt;
|-&lt;br /&gt;
|110_00_54  || 11.70     ||  1.006     ||  1.060    ||  0.9663    ||  0.9498    ||   1.706     ||  1.312    ||   5.370     || 0.4642&lt;br /&gt;
|-&lt;br /&gt;
|110_10_57  || 13.97     ||  1.160     ||  1.232    ||  0.9593    ||  0.9502    ||   1.716     ||  1.301    ||   6.136     || 0.8247&lt;br /&gt;
|-&lt;br /&gt;
|110_20_60  || 15.75     ||  1.298     ||  1.372    ||  0.9526    ||  0.9504    ||   1.726     ||  1.292    ||   5.739     ||  1.330&lt;br /&gt;
|-&lt;br /&gt;
|110_30_63  || 18.56     ||  1.415     ||  1.516    ||  0.9455    ||  0.9500    ||   1.734     ||  1.284    ||   7.122     ||  1.849&lt;br /&gt;
|-&lt;br /&gt;
|110_40_66  || 19.50     ||  1.521     ||  1.622    ||  0.9398    ||  0.9503    ||   1.743     ||  1.275    ||   6.602     ||  1.921&lt;br /&gt;
|-&lt;br /&gt;
|110_50_70  || 19.07     ||  1.618     ||  1.696    ||  0.9336    ||  0.9498    ||   1.751     ||  1.267    ||   4.873     ||  2.085&lt;br /&gt;
|-&lt;br /&gt;
|110_60_73  || 18.32     ||  1.702     ||  1.761    ||  0.9291    ||  0.9507    ||   1.758     ||  1.260    ||   3.471     ||  2.033&lt;br /&gt;
|-&lt;br /&gt;
|110_70_77  || 17.13     ||  1.782     ||  1.816    ||  0.9237    ||  0.9504    ||   1.766     ||  1.252    ||   1.948     ||  1.838&lt;br /&gt;
|-&lt;br /&gt;
|110_80_81  || 15.56     ||  1.853     ||  1.871    ||  0.9192    ||  0.9508    ||   1.773     ||  1.245    ||  0.9878     ||  1.332&lt;br /&gt;
|-&lt;br /&gt;
|110_90_84  || 13.12     ||  1.923     ||  1.926    ||  0.9142    ||  0.9506    ||   1.780     ||  1.238    ||  0.1639     || 0.5301&lt;br /&gt;
|-&lt;br /&gt;
|110_95_86  || 10.73     ||  1.963     ||  1.955    ||  0.9095    ||  0.9486    ||   1.783     ||  1.235    || -0.3746     || 8.1449E-04&lt;br /&gt;
|-&lt;br /&gt;
|110_110_92 || 17.29     ||  2.020     ||  2.055    ||  0.9056    ||  0.9509    ||   1.793     ||  1.225    ||   1.768     ||  2.045&lt;br /&gt;
|-&lt;br /&gt;
|110_120_95 || 17.55     ||  2.048     ||  2.095    ||  0.9014    ||  0.9510    ||   1.799     ||  1.219    ||   2.314     ||  3.774&lt;br /&gt;
|-&lt;br /&gt;
|120_00_57  || 13.14     ||  1.050     ||  1.117    ||  0.9599    ||  0.9497    ||   1.714     ||  1.305    ||   6.304     || 0.4861&lt;br /&gt;
|-&lt;br /&gt;
|120_10_60  || 14.81     ||  1.196     ||  1.268    ||  0.9534    ||  0.9501    ||   1.723     ||  1.295    ||   6.054     || 0.8382&lt;br /&gt;
|-&lt;br /&gt;
|120_20_63  || 17.57     ||  1.323     ||  1.409    ||  0.9458    ||  0.9494    ||   1.732     ||  1.286    ||   6.504     ||  1.409&lt;br /&gt;
|-&lt;br /&gt;
|120_30_67  || 19.50     ||  1.435     ||  1.539    ||  0.9407    ||  0.9503    ||   1.741     ||  1.277    ||   7.263     ||  1.529&lt;br /&gt;
|-&lt;br /&gt;
|120_40_70  || 19.38     ||  1.534     ||  1.621    ||  0.9335    ||  0.9492    ||   1.749     ||  1.269    ||   5.695     ||  1.632&lt;br /&gt;
|-&lt;br /&gt;
|120_50_74  || 18.34     ||  1.621     ||  1.684    ||  0.9294    ||  0.9503    ||   1.756     ||  1.262    ||   3.910     ||  1.864&lt;br /&gt;
|-&lt;br /&gt;
|120_60_77  || 17.24     ||  1.703     ||  1.743    ||  0.9246    ||  0.9507    ||   1.764     ||  1.254    ||   2.381     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|120_70_81  || 16.02     ||  1.780     ||  1.803    ||  0.9197    ||  0.9509    ||   1.771     ||  1.247    ||   1.312     ||  1.511&lt;br /&gt;
|-&lt;br /&gt;
|120_80_84  || 14.49     ||  1.850     ||  1.860    ||  0.9150    ||  0.9509    ||   1.778     ||  1.240    ||  0.5347     ||  1.076&lt;br /&gt;
|-&lt;br /&gt;
|120_90_88  || 12.18     ||  1.918     ||  1.918    ||  0.9096    ||  0.9501    ||   1.785     ||  1.233    || -4.1127E-02 || 0.3613&lt;br /&gt;
|-&lt;br /&gt;
|120_95_90  || 10.06     ||  1.957     ||  1.950    ||  0.9071    ||  0.9499    ||   1.788     ||  1.230    || -0.3241     ||  0.000&lt;br /&gt;
|-&lt;br /&gt;
|120_115_97 || 16.46     ||  2.020     ||  2.066    ||  0.8983    ||  0.9497    ||   1.801     ||  1.216    ||   2.258     ||  2.404&lt;br /&gt;
|-&lt;br /&gt;
|120_120_99 || 17.58     ||  2.008     ||  2.092    ||  0.8967    ||  0.9501    ||   1.804     ||  1.213    ||   4.186     ||  3.647&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Flexibility ==&lt;br /&gt;
&lt;br /&gt;
[[File:Flexibility TJ-II.png|300px|thumb|right|Flexibility diagram of TJ-II magnetic configurations. Several lines of constant rotational transform are highlighted and labelled with the corresponding central &amp;lt;math&amp;gt;\iota/2\pi&amp;lt;/math&amp;gt;-value.]]&lt;br /&gt;
TJ-II has considerable configurational flexibility, as observed in the &#039;flexibility diagram&#039;&amp;lt;ref&amp;gt;E. Ascasíbar, T. Estrada, F. Castejón, A. López-Fraguas, I. Pastor, J. Sánchez, U. Stroth, J. Qin and TJ-II Team, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/45/4/009|Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276–284]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
Some of this flexibility space has been explored, as in the &#039;magnetic well scan&#039; experiments&amp;lt;ref&amp;gt;A. de Aguilera, F. Castejón, E. Ascasíbar, et al. &#039;&#039;Magnetic well scan and confinement in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/55/11/113014|Nucl. Fusion, 55(11):113014, 2015]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
More recently, the rotational transform in the plasma edge region was found to be of importance for L-H confinement transitions&amp;lt;ref&amp;gt;B. P. van Milligen, T. Estrada, B. Carreras, L. García, and TJ-II Team. &#039;&#039;Importance of the rotational transform for L–H transitions in the TJ-II stellarator&#039;&#039;, [[doi:10.3390/plasma7020024|Plasma, 7(2):446–464, 2024]].&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8725</id>
		<title>TJ-II:Magnetic configuration</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8725"/>
		<updated>2026-10-07T14:30:02Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* Flexibility */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The magnetic configuration of [[TJ-II]] in vacuum is completely determined by the currents flowing through the [[TJ-II:Coil system|external coils]].&lt;br /&gt;
Magnetic configurations are labelled as &#039;xxx_yy_zz&#039;, where&lt;br /&gt;
* &#039;xxx&#039;: 10 times the current (in kA) in the circular coil&lt;br /&gt;
* &#039;yy&#039;: 10 times the current (in kA) in the helical coil&lt;br /&gt;
* &#039;zz&#039;: 10 times the current (in kA) in the vertical field coils&lt;br /&gt;
The current in the toroidal field coils is not specified, as its value is adjusted to guarantee central absorption of the [[TJ-II:Electron Cyclotron Resonant Heating|Electron Cyclotron Resonant Heating]] source (requiring a specific &#039;resonant&#039; value of the magnetic field on the magnetic axis, &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
Configuration list:&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;width: 100%&amp;quot; border=&amp;quot;1&amp;quot;||&lt;br /&gt;
|-&lt;br /&gt;
! Configuration &lt;br /&gt;
! &amp;lt;math&amp;gt;r_{av}&amp;lt;/math&amp;gt; (cm) &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(0)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(a)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{m,av}&amp;lt;/math&amp;gt;(T) &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt; (T) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(0)&amp;lt;/math&amp;gt; (m) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(45)&amp;lt;/math&amp;gt;(m) &lt;br /&gt;
! Shear (%) &lt;br /&gt;
! Well (%)&lt;br /&gt;
|-&lt;br /&gt;
|0_20_13    ||1.139      || 1.185      || 1.194     ||  1.033     || 0.9504     ||  1.644      || 1.374     || 0.7793      ||5.7521E-02&lt;br /&gt;
|-&lt;br /&gt;
|0_30_15    ||4.228      || 1.518      || 1.698     ||  1.019     || 0.9500     ||  1.658      || 1.360     ||  11.85      || 1.050&lt;br /&gt;
|-&lt;br /&gt;
|0_40_18    ||5.903      || 1.756      || 2.003     ||  1.008     || 0.9505     ||  1.671      || 1.347     ||  14.09      || 1.217&lt;br /&gt;
|-&lt;br /&gt;
|0_50_22    ||6.480      || 1.936      || 2.230     || 0.9973     || 0.9502     ||  1.682      || 1.336     ||  15.17      || 2.481&lt;br /&gt;
|-&lt;br /&gt;
|0_60_26    ||8.500      || 2.073      || 2.399     || 0.9885     || 0.9502     ||  1.692      || 1.326     ||  15.70      || 3.218&lt;br /&gt;
|-&lt;br /&gt;
|0_70_29    ||7.147      || 2.187      || 2.434     || 0.9805     || 0.9503     ||  1.701      || 1.317     ||  11.30      || 2.985&lt;br /&gt;
|-&lt;br /&gt;
|0_80_34    ||6.902      || 2.284      || 2.469     || 0.9736     || 0.9506     ||  1.710      || 1.308     ||  8.084      || 2.735&lt;br /&gt;
|-&lt;br /&gt;
|0_90_38    ||6.738      || 2.366      || 2.514     || 0.9663     || 0.9503     ||  1.719      || 1.299     ||  6.269      || 2.534&lt;br /&gt;
|-&lt;br /&gt;
|0_100_42   ||12.59      || 2.436      || 2.667     || 0.9601     || 0.9505     ||  1.727      || 1.291     ||  9.493      || 4.643&lt;br /&gt;
|-&lt;br /&gt;
|0_110_46   ||10.67      || 2.493      || 2.667     || 0.9539     || 0.9503     ||  1.734      || 1.284     ||  6.980      || 4.554&lt;br /&gt;
|-&lt;br /&gt;
|0_120_50   ||12.71      || 2.548      || 2.667     || 0.9482     || 0.9504     ||  1.742      || 1.276     ||  4.683      || 4.272&lt;br /&gt;
|-&lt;br /&gt;
|10_20_18   || 2.557     ||  1.148     ||  1.184    ||   1.024    ||  0.9514    ||   1.652     ||  1.366    ||   3.183     || 0.2469&lt;br /&gt;
|-&lt;br /&gt;
|10_30_20   || 6.083     ||  1.438     ||  1.602    ||   1.010    ||  0.9501    ||   1.666     ||  1.352    ||   11.35     ||  1.398&lt;br /&gt;
|-&lt;br /&gt;
|10_40_24   || 6.921     ||  1.659     ||  1.880    ||   1.000    ||  0.9504    ||   1.678     ||  1.340    ||   13.34     ||  2.751&lt;br /&gt;
|-&lt;br /&gt;
|10_50_27   || 8.140     ||  1.826     ||  1.997    ||  0.9909    ||  0.9504    ||   1.688     ||  1.329    ||   9.321     ||  3.241&lt;br /&gt;
|-&lt;br /&gt;
|10_60_31   || 9.350     ||  1.965     ||  2.183    ||  0.9826    ||  0.9505    ||   1.698     ||  1.319    ||   11.11     ||  3.084&lt;br /&gt;
|-&lt;br /&gt;
|10_70_35   || 10.10     ||  2.077     ||  2.288    ||  0.9750    ||  0.9505    ||   1.707     ||  1.310    ||   10.16     ||  3.597&lt;br /&gt;
|-&lt;br /&gt;
|10_80_38   || 9.810     ||  2.174     ||  2.371    ||  0.9674    ||  0.9502    ||   1.716     ||  1.302    ||   9.037     ||  3.908&lt;br /&gt;
|-&lt;br /&gt;
|10_90_42   || 10.54     ||  2.257     ||  2.434    ||  0.9610    ||  0.9503    ||   1.724     ||  1.294    ||   7.851     ||  4.281&lt;br /&gt;
|-&lt;br /&gt;
|10_100_47  || 10.21     ||  2.327     ||  2.482    ||  0.9546    ||  0.9502    ||   1.732     ||  1.286    ||   6.647     ||  4.236&lt;br /&gt;
|-&lt;br /&gt;
|10_110_51  || 11.11     ||  2.395     ||  2.547    ||  0.9488    ||  0.9501    ||   1.740     ||  1.278    ||   6.331     ||  5.121&lt;br /&gt;
|-&lt;br /&gt;
|10_120_55  || 10.04     ||  2.451     ||  2.565    ||  0.9432    ||  0.9502    ||   1.747     ||  1.271    ||   4.674     ||  4.426&lt;br /&gt;
|-&lt;br /&gt;
|20_10_21   || 1.213     || 0.7902     || 0.7956    ||   1.028    ||  0.9503    ||   1.645     ||  1.373    ||  0.6830     || 3.7624E-02&lt;br /&gt;
|-&lt;br /&gt;
|20_20_22   || 3.952     ||  1.136     ||  1.185    ||   1.014    ||  0.9500    ||   1.661     ||  1.357    ||   4.350     || 0.4717&lt;br /&gt;
|-&lt;br /&gt;
|20_30_25   || 6.779     ||  1.395     ||  1.521    ||   1.003    ||  0.9502    ||   1.673     ||  1.344    ||   9.049     ||  1.550&lt;br /&gt;
|-&lt;br /&gt;
|20_40_28   || 8.475     ||  1.592     ||  1.771    ||  0.9922    ||  0.9498    ||   1.685     ||  1.333    ||   11.25     ||  2.879&lt;br /&gt;
|-&lt;br /&gt;
|20_50_32   || 8.039     ||  1.756     ||  1.906    ||  0.9842    ||  0.9505    ||   1.695     ||  1.323    ||   8.571     ||  3.131&lt;br /&gt;
|-&lt;br /&gt;
|20_60_35   || 11.21     ||  1.884     ||  1.997    ||  0.9755    ||  0.9498    ||   1.705     ||  1.313    ||   5.968     ||  1.980&lt;br /&gt;
|-&lt;br /&gt;
|20_70_39   || 11.08     ||  1.994     ||  2.154    ||  0.9689    ||  0.9504    ||   1.714     ||  1.304    ||   7.982     ||  3.385&lt;br /&gt;
|-&lt;br /&gt;
|20_80_43   || 12.14     ||  2.092     ||  2.255    ||  0.9614    ||  0.9497    ||   1.722     ||  1.296    ||   7.811     ||  4.133&lt;br /&gt;
|-&lt;br /&gt;
|20_90_47   || 12.83     ||  2.174     ||  2.324    ||  0.9558    ||  0.9503    ||   1.730     ||  1.288    ||   6.862     ||  4.713&lt;br /&gt;
|-&lt;br /&gt;
|20_100_51  || 12.68     ||  2.246     ||  2.379    ||  0.9498    ||  0.9503    ||   1.738     ||  1.280    ||   5.945     ||  4.930&lt;br /&gt;
|-&lt;br /&gt;
|20_110_55  || 13.79     ||  2.313     ||  2.434    ||  0.9443    ||  0.9505    ||   1.745     ||  1.273    ||   5.248     ||  5.117&lt;br /&gt;
|-&lt;br /&gt;
|20_120_59  || 13.91     ||  2.368     ||  2.483    ||  0.9386    ||  0.9502    ||   1.752     ||  1.265    ||   4.822     ||  5.418&lt;br /&gt;
|-&lt;br /&gt;
|30_10_25   || 2.709     || 0.8385     || 0.8507    ||   1.018    ||  0.9501    ||   1.654     ||  1.363    ||   1.452     || 0.1431&lt;br /&gt;
|-&lt;br /&gt;
|30_20_27   || 5.443     ||  1.134     ||  1.189    ||   1.007    ||  0.9514    ||   1.669     ||  1.349    ||   4.847     || 0.7001&lt;br /&gt;
|-&lt;br /&gt;
|30_30_30   || 8.180     ||  1.368     ||  1.481    ||  0.9956    ||  0.9506    ||   1.681     ||  1.337    ||   8.332     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|30_40_33   || 9.756     ||  1.550     ||  1.687    ||  0.9860    ||  0.9503    ||   1.692     ||  1.326    ||   8.877     ||  2.798&lt;br /&gt;
|-&lt;br /&gt;
|30_50_37   || 11.16     ||  1.702     ||  1.878    ||  0.9779    ||  0.9503    ||   1.702     ||  1.316    ||   10.37     ||  4.941&lt;br /&gt;
|-&lt;br /&gt;
|30_60_40   || 9.262     ||  1.827     ||  1.936    ||  0.9706    ||  0.9505    ||   1.711     ||  1.307    ||   5.952     ||  3.624&lt;br /&gt;
|-&lt;br /&gt;
|30_70_44   || 12.28     ||  1.937     ||  2.007    ||  0.9631    ||  0.9502    ||   1.720     ||  1.298    ||   3.593     ||  4.431&lt;br /&gt;
|-&lt;br /&gt;
|30_80_48   || 13.28     ||  2.033     ||  2.149    ||  0.9567    ||  0.9502    ||   1.728     ||  1.290    ||   5.702     ||  3.674&lt;br /&gt;
|-&lt;br /&gt;
|30_90_52   || 14.16     ||  2.115     ||  2.231    ||  0.9504    ||  0.9501    ||   1.736     ||  1.282    ||   5.476     ||  4.227&lt;br /&gt;
|-&lt;br /&gt;
|30_100_56  || 14.97     ||  2.187     ||  2.295    ||  0.9448    ||  0.9502    ||   1.743     ||  1.275    ||   4.949     ||  4.755&lt;br /&gt;
|-&lt;br /&gt;
|30_110_59  || 15.76     ||  2.246     ||  2.356    ||  0.9391    ||  0.9500    ||   1.751     ||  1.267    ||   4.920     ||  5.215&lt;br /&gt;
|-&lt;br /&gt;
|30_120_63  || 14.48     ||  2.306     ||  2.389    ||  0.9343    ||  0.9504    ||   1.758     ||  1.260    ||   3.573     ||  5.025&lt;br /&gt;
|-&lt;br /&gt;
|40_00_27   || 1.350     || 0.5464     || 0.5471    ||   1.024    ||  0.9504    ||   1.647     ||  1.371    ||  0.1331     || 2.4768E-02&lt;br /&gt;
|-&lt;br /&gt;
|40_10_29   || 4.111     || 0.8821     || 0.9010    ||   1.010    ||  0.9510    ||   1.663     ||  1.355    ||   2.152     || 0.2456&lt;br /&gt;
|-&lt;br /&gt;
|40_20_31   || 6.646     ||  1.146     ||  1.202    ||  0.9975    ||  0.9501    ||   1.677     ||  1.341    ||   4.928     || 0.8185&lt;br /&gt;
|-&lt;br /&gt;
|40_30_34   || 9.328     ||  1.354     ||  1.452    ||  0.9884    ||  0.9506    ||   1.688     ||  1.330    ||   7.247     ||  1.826&lt;br /&gt;
|-&lt;br /&gt;
|40_40_37   || 11.15     ||  1.523     ||  1.646    ||  0.9788    ||  0.9498    ||   1.699     ||  1.319    ||   8.061     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|40_50_41   || 12.66     ||  1.666     ||  1.797    ||  0.9719    ||  0.9506    ||   1.708     ||  1.310    ||   7.872     ||  4.310&lt;br /&gt;
|-&lt;br /&gt;
|40_60_44   || 12.34     ||  1.786     ||  1.927    ||  0.9637    ||  0.9497    ||   1.717     ||  1.301    ||   7.879     ||  5.834&lt;br /&gt;
|-&lt;br /&gt;
|40_70_48   || 9.734     ||  1.894     ||  1.963    ||  0.9579    ||  0.9504    ||   1.726     ||  1.292    ||   3.625     ||  3.668&lt;br /&gt;
|-&lt;br /&gt;
|40_80_52   || 13.96     ||  1.986     ||  2.067    ||  0.9515    ||  0.9503    ||   1.734     ||  1.284    ||   4.054     ||  3.028&lt;br /&gt;
|-&lt;br /&gt;
|40_90_56   || 15.39     ||  2.062     ||  2.156    ||  0.9457    ||  0.9504    ||   1.741     ||  1.277    ||   4.529     ||  3.841&lt;br /&gt;
|-&lt;br /&gt;
|40_100_60  || 16.40     ||  2.132     ||  2.232    ||  0.9400    ||  0.9502    ||   1.749     ||  1.269    ||   4.683     ||  4.355&lt;br /&gt;
|-&lt;br /&gt;
|40_110_64  || 18.12     ||  2.199     ||  2.288    ||  0.9348    ||  0.9503    ||   1.756     ||  1.262    ||   4.049     ||  4.651&lt;br /&gt;
|-&lt;br /&gt;
|40_120_68  || 16.81     ||  2.256     ||  2.327    ||  0.9295    ||  0.9501    ||   1.763     ||  1.255    ||   3.158     ||  4.904&lt;br /&gt;
|-&lt;br /&gt;
|50_00_31   || 2.818     || 0.6329     || 0.6375    ||   1.013    ||  0.9498    ||   1.657     ||  1.361    ||  0.7286     || 6.1871E-02&lt;br /&gt;
|-&lt;br /&gt;
|50_10_33   || 5.588     || 0.9254     || 0.9532    ||   1.001    ||  0.9506    ||   1.672     ||  1.346    ||   3.003     || 0.3605&lt;br /&gt;
|-&lt;br /&gt;
|50_20_36   || 8.222     ||  1.160     ||  1.216    ||  0.9902    ||  0.9502    ||   1.684     ||  1.334    ||   4.838     ||  1.060&lt;br /&gt;
|-&lt;br /&gt;
|50_30_39   || 10.67     ||  1.352     ||  1.435    ||  0.9815    ||  0.9505    ||   1.695     ||  1.323    ||   6.163     ||  2.008&lt;br /&gt;
|-&lt;br /&gt;
|50_40_42   || 12.44     ||  1.508     ||  1.609    ||  0.9733    ||  0.9504    ||   1.705     ||  1.313    ||   6.719     ||  2.910&lt;br /&gt;
|-&lt;br /&gt;
|50_50_46   || 13.94     ||  1.644     ||  1.758    ||  0.9661    ||  0.9505    ||   1.714     ||  1.303    ||   6.944     ||  4.001&lt;br /&gt;
|-&lt;br /&gt;
|50_60_49   || 15.09     ||  1.757     ||  1.887    ||  0.9587    ||  0.9502    ||   1.723     ||  1.295    ||   7.390     ||  6.217&lt;br /&gt;
|-&lt;br /&gt;
|50_70_53   || 13.03     ||  1.855     ||  1.955    ||  0.9524    ||  0.9502    ||   1.731     ||  1.287    ||   5.353     ||  5.830&lt;br /&gt;
|-&lt;br /&gt;
|50_80_56   || 16.73     ||  1.949     ||  2.004    ||  0.9463    ||  0.9501    ||   1.739     ||  1.279    ||   2.807     ||  4.003&lt;br /&gt;
|-&lt;br /&gt;
|50_90_60   || 16.70     ||  2.011     ||  2.101    ||  0.9407    ||  0.9502    ||   1.747     ||  1.271    ||   4.501     ||  3.444&lt;br /&gt;
|-&lt;br /&gt;
|50_100_64  || 18.15     ||  2.090     ||  2.183    ||  0.9351    ||  0.9500    ||   1.754     ||  1.264    ||   4.434     ||  3.907&lt;br /&gt;
|-&lt;br /&gt;
|50_110_68  || 17.53     ||  2.154     ||  2.223    ||  0.9297    ||  0.9498    ||   1.762     ||  1.256    ||   3.205     ||  4.270&lt;br /&gt;
|-&lt;br /&gt;
|50_120_72  || 19.13     ||  2.213     ||  2.288    ||  0.9250    ||  0.9501    ||   1.768     ||  1.250    ||   3.417     ||  4.378&lt;br /&gt;
|-&lt;br /&gt;
|60_00_35   || 4.247     || 0.7126     || 0.7205    ||   1.003    ||  0.9498    ||   1.667     ||  1.352    ||   1.108     || 0.1270&lt;br /&gt;
|-&lt;br /&gt;
|60_10_37   || 6.862     || 0.9679     ||  1.002    ||  0.9934    ||  0.9509    ||   1.680     ||  1.338    ||   3.520     || 0.4827&lt;br /&gt;
|-&lt;br /&gt;
|60_20_40   || 9.669     ||  1.179     ||  1.240    ||  0.9831    ||  0.9503    ||   1.692     ||  1.326    ||   5.202     ||  1.236&lt;br /&gt;
|-&lt;br /&gt;
|60_30_43   || 12.01     ||  1.354     ||  1.435    ||  0.9747    ||  0.9502    ||   1.702     ||  1.316    ||   5.973     ||  2.132&lt;br /&gt;
|-&lt;br /&gt;
|60_40_46   || 13.48     ||  1.500     ||  1.593    ||  0.9672    ||  0.9503    ||   1.712     ||  1.306    ||   6.170     ||  2.806&lt;br /&gt;
|-&lt;br /&gt;
|60_50_50   || 15.36     ||  1.627     ||  1.732    ||  0.9601    ||  0.9504    ||   1.721     ||  1.297    ||   6.467     ||  3.895&lt;br /&gt;
|-&lt;br /&gt;
|60_60_53   || 16.79     ||  1.734     ||  1.851    ||  0.9528    ||  0.9499    ||   1.729     ||  1.289    ||   6.731     ||  5.666&lt;br /&gt;
|-&lt;br /&gt;
|60_70_57   || 15.88     ||  1.829     ||  1.934    ||  0.9473    ||  0.9502    ||   1.737     ||  1.281    ||   5.736     ||  6.958&lt;br /&gt;
|-&lt;br /&gt;
|60_80_61   || 13.66     ||  1.918     ||  1.968    ||  0.9428    ||  0.9514    ||   1.745     ||  1.273    ||   2.622     ||  4.555&lt;br /&gt;
|-&lt;br /&gt;
|60_90_64   || 17.29     ||  2.009     ||  2.063    ||  0.9359    ||  0.9501    ||   1.753     ||  1.265    ||   2.640     ||  1.637&lt;br /&gt;
|-&lt;br /&gt;
|60_100_68  || 17.62     ||  2.049     ||  2.122    ||  0.9304    ||  0.9497    ||   1.760     ||  1.258    ||   3.560     ||  3.718&lt;br /&gt;
|-&lt;br /&gt;
|60_110_72  || 17.50     ||  2.118     ||  2.177    ||  0.9257    ||  0.9501    ||   1.767     ||  1.251    ||   2.811     ||  4.023&lt;br /&gt;
|-&lt;br /&gt;
|60_120_76  || 17.78     ||  2.174     ||  2.222    ||  0.9217    ||  0.9510    ||   1.774     ||  1.244    ||   2.209     ||  4.211&lt;br /&gt;
|-&lt;br /&gt;
|70_00_39   || 5.731     || 0.7825     || 0.7975    ||  0.9949    ||  0.9497    ||   1.675     ||  1.343    ||   1.908     || 0.2335&lt;br /&gt;
|-&lt;br /&gt;
|70_10_41   || 8.418     ||  1.009     ||  1.048    ||  0.9860    ||  0.9509    ||   1.688     ||  1.330    ||   3.845     || 0.6755&lt;br /&gt;
|-&lt;br /&gt;
|70_20_44   || 11.09     ||  1.201     ||  1.265    ||  0.9767    ||  0.9504    ||   1.699     ||  1.319    ||   5.345     ||  1.317&lt;br /&gt;
|-&lt;br /&gt;
|70_30_47   || 13.41     ||  1.361     ||  1.441    ||  0.9688    ||  0.9504    ||   1.709     ||  1.309    ||   5.859     ||  2.187&lt;br /&gt;
|-&lt;br /&gt;
|70_40_51   || 14.99     ||  1.496     ||  1.591    ||  0.9615    ||  0.9503    ||   1.718     ||  1.300    ||   6.348     ||  2.859&lt;br /&gt;
|-&lt;br /&gt;
|70_50_54   || 16.87     ||  1.617     ||  1.712    ||  0.9543    ||  0.9501    ||   1.727     ||  1.291    ||   5.843     ||  3.756&lt;br /&gt;
|-&lt;br /&gt;
|70_60_57   || 17.89     ||  1.718     ||  1.823    ||  0.9479    ||  0.9500    ||   1.735     ||  1.283    ||   6.140     ||  4.746&lt;br /&gt;
|-&lt;br /&gt;
|70_70_61   || 18.26     ||  1.812     ||  1.928    ||  0.9423    ||  0.9503    ||   1.743     ||  1.275    ||   6.353     ||  6.812&lt;br /&gt;
|-&lt;br /&gt;
|70_80_65   || 16.37     ||  1.896     ||  1.962    ||  0.9363    ||  0.9499    ||   1.751     ||  1.267    ||   3.469     ||  5.948&lt;br /&gt;
|-&lt;br /&gt;
|70_90_68   || 9.135     ||  1.980     ||  1.988    ||  0.9317    ||  0.9506    ||   1.758     ||  1.260    ||  0.3692     || 0.1186&lt;br /&gt;
|-&lt;br /&gt;
|70_100_72  || 18.64     ||  2.007     ||  2.094    ||  0.9267    ||  0.9506    ||   1.765     ||  1.253    ||   4.327     ||  3.356&lt;br /&gt;
|-&lt;br /&gt;
|70_110_76  || 18.23     ||  2.088     ||  2.147    ||  0.9219    ||  0.9507    ||   1.772     ||  1.246    ||   2.792     ||  3.707&lt;br /&gt;
|-&lt;br /&gt;
|70_120_80  || 17.89     ||  2.145     ||  2.184    ||  0.9171    ||  0.9506    ||   1.779     ||  1.239    ||   1.846     ||  4.043&lt;br /&gt;
|-&lt;br /&gt;
|80_00_42   ||7.247      ||0.8436      ||0.8697     || 0.9869     || 0.9497     ||  1.684      || 1.335     ||  3.094      ||0.2402&lt;br /&gt;
|-&lt;br /&gt;
|80_10_45   ||9.865      || 1.049      || 1.095     || 0.9794     || 0.9513     ||  1.695      || 1.323     ||  4.371      ||0.7359&lt;br /&gt;
|-&lt;br /&gt;
|80_20_48   ||12.28      || 1.226      || 1.290     || 0.9697     || 0.9500     ||  1.706      || 1.312     ||  5.206      || 1.327&lt;br /&gt;
|-&lt;br /&gt;
|80_30_51   ||14.38      || 1.370      || 1.454     || 0.9626     || 0.9503     ||  1.715      || 1.303     ||  6.088      || 2.102&lt;br /&gt;
|-&lt;br /&gt;
|80_40_54   ||16.47      || 1.500      || 1.594     || 0.9549     || 0.9497     ||  1.724      || 1.294     ||  6.263      || 2.799&lt;br /&gt;
|-&lt;br /&gt;
|80_50_58   ||17.63      || 1.612      || 1.706     || 0.9492     || 0.9503     ||  1.733      || 1.285     ||  5.842      || 3.329&lt;br /&gt;
|-&lt;br /&gt;
|80_60_61   ||18.84      || 1.712      || 1.814     || 0.9436     || 0.9507     ||  1.741      || 1.277     ||  5.984      || 3.990&lt;br /&gt;
|-&lt;br /&gt;
|80_70_65   ||19.27      || 1.799      || 1.898     || 0.9372     || 0.9501     ||  1.749      || 1.269     ||  5.555      || 4.728&lt;br /&gt;
|-&lt;br /&gt;
|80_80_69   ||17.96      || 1.880      || 1.935     || 0.9321     || 0.9503     ||  1.756      || 1.262     ||  2.921      || 3.774&lt;br /&gt;
|-&lt;br /&gt;
|80_90_73   ||13.42      || 1.957      || 1.982     || 0.9266     || 0.9500     ||  1.764      || 1.254     ||  1.312      ||0.6938&lt;br /&gt;
|-&lt;br /&gt;
|80_100_76  || 18.53     ||  2.008     ||  2.065    ||  0.9220    ||  0.9504    ||   1.770     ||  1.247    ||   2.839     ||  1.773&lt;br /&gt;
|-&lt;br /&gt;
|80_110_80  || 18.41     ||  2.059     ||  2.117    ||  0.9176    ||  0.9507    ||   1.777     ||  1.241    ||   2.847     ||  3.632&lt;br /&gt;
|-&lt;br /&gt;
|80_120_84  || 18.26     ||  2.117     ||  2.157    ||  0.9122    ||  0.9496    ||   1.784     ||  1.234    ||   1.872     ||  3.986&lt;br /&gt;
|-&lt;br /&gt;
|90_00_46   || 8.679     || 0.9022     || 0.9354    ||  0.9802    ||  0.9501    ||   1.691     ||  1.327    ||   3.678     || 0.3981&lt;br /&gt;
|-&lt;br /&gt;
|90_10_49   || 11.45     ||  1.090     ||  1.146    ||  0.9717    ||  0.9502    ||   1.702     ||  1.315    ||   5.148     || 0.8099&lt;br /&gt;
|-&lt;br /&gt;
|90_20_52   || 12.44     ||  1.247     ||  1.323    ||  0.9640    ||  0.9503    ||   1.712     ||  1.305    ||   6.100     ||  1.079&lt;br /&gt;
|-&lt;br /&gt;
|90_30_55   || 16.14     ||  1.383     ||  1.475    ||  0.9571    ||  0.9504    ||   1.722     ||  1.296    ||   6.607     ||  2.158&lt;br /&gt;
|-&lt;br /&gt;
|90_40_58   || 17.45     ||  1.506     ||  1.597    ||  0.9499    ||  0.9501    ||   1.731     ||  1.287    ||   6.012     ||  2.629&lt;br /&gt;
|-&lt;br /&gt;
|90_50_62   || 18.70     ||  1.609     ||  1.706    ||  0.9438    ||  0.9501    ||   1.739     ||  1.279    ||   6.003     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|90_60_65   || 18.77     ||  1.703     ||  1.789    ||  0.9381    ||  0.9502    ||   1.747     ||  1.271    ||   5.045     ||  3.047&lt;br /&gt;
|-&lt;br /&gt;
|90_70_69   || 18.43     ||  1.787     ||  1.852    ||  0.9324    ||  0.9500    ||   1.754     ||  1.263    ||   3.623     ||  3.117&lt;br /&gt;
|-&lt;br /&gt;
|90_80_73   || 17.72     ||  1.868     ||  1.909    ||  0.9269    ||  0.9497    ||   1.762     ||  1.256    ||   2.217     ||  2.354&lt;br /&gt;
|-&lt;br /&gt;
|90_90_76   || 14.40     ||  1.940     ||  1.956    ||  0.9221    ||  0.9499    ||   1.769     ||  1.249    ||  0.8079     || 0.8326&lt;br /&gt;
|-&lt;br /&gt;
|90_100_80  || 18.53     ||  2.009     ||  2.038    ||  0.9176    ||  0.9503    ||   1.776     ||  1.242    ||   1.484     ||  1.095&lt;br /&gt;
|-&lt;br /&gt;
|90_110_84  || 18.97     ||  2.021     ||  2.094    ||  0.9129    ||  0.9502    ||   1.783     ||  1.235    ||   3.625     ||  3.669&lt;br /&gt;
|-&lt;br /&gt;
|90_120_88  || 17.79     ||  2.090     ||  2.129    ||  0.9077    ||  0.9494    ||   1.789     ||  1.229    ||   1.827     ||  3.862&lt;br /&gt;
|-&lt;br /&gt;
|100_00_50  || 10.07     || 0.9544     || 0.9970    ||  0.9732    ||  0.9499    ||   1.699     ||  1.319    ||   4.471     || 0.4341&lt;br /&gt;
|-&lt;br /&gt;
|100_10_53  || 12.78     ||  1.127     ||  1.186    ||  0.9649    ||  0.9499    ||   1.710     ||  1.308    ||   5.262     || 0.9629&lt;br /&gt;
|-&lt;br /&gt;
|100_16_55  || 13.69     ||  1.215     ||  1.287    ||  0.9610    ||  0.9501    ||   1.715     ||  1.302    ||   5.901     ||  1.023&lt;br /&gt;
|-&lt;br /&gt;
|100_20_56  || 10.86     ||  1.271     ||  1.324    ||  0.9583    ||  0.9502    ||   1.719     ||  1.299    ||   4.120     || 0.8295&lt;br /&gt;
|-&lt;br /&gt;
|100_22_56  || 15.40     ||  1.309     ||  1.381    ||  0.9412    ||  0.9362    ||   1.722     ||  1.296    ||   5.552     ||  1.648&lt;br /&gt;
|-&lt;br /&gt;
|100_24_58  || 15.90     ||  1.326     ||  1.406    ||  0.9552    ||  0.9499    ||   1.722     ||  1.295    ||   6.105     ||  1.792&lt;br /&gt;
|-&lt;br /&gt;
|100_26_58  || 16.42     ||  1.352     ||  1.435    ||  0.9538    ||  0.9499    ||   1.724     ||  1.293    ||   6.137     ||  1.888&lt;br /&gt;
|-&lt;br /&gt;
|100_28_59  || 17.07     ||  1.375     ||  1.464    ||  0.9527    ||  0.9501    ||   1.726     ||  1.291    ||   6.475     ||  1.983&lt;br /&gt;
|-&lt;br /&gt;
|100_30_59  || 17.29     ||  1.398     ||  1.490    ||  0.9511    ||  0.9500    ||   1.728     ||  1.289    ||   6.561     ||  2.075&lt;br /&gt;
|-&lt;br /&gt;
|100_32_60  || 17.74     ||  1.423     ||  1.517    ||  0.9499    ||  0.9499    ||   1.730     ||  1.288    ||   6.596     ||  2.165&lt;br /&gt;
|-&lt;br /&gt;
|100_36_61  || 18.37     ||  1.467     ||  1.567    ||  0.9475    ||  0.9501    ||   1.733     ||  1.284    ||   6.819     ||  2.183&lt;br /&gt;
|-&lt;br /&gt;
|100_40_63  || 18.77     ||  1.509     ||  1.608    ||  0.9450    ||  0.9500    ||   1.736     ||  1.281    ||   6.553     ||  2.304&lt;br /&gt;
|-&lt;br /&gt;
|100_44_64  || 19.25     ||  1.551     ||  1.653    ||  0.9426    ||  0.9500    ||   1.740     ||  1.278    ||   6.569     ||  2.360&lt;br /&gt;
|-&lt;br /&gt;
|100_48_65  || 19.16     ||  1.591     ||  1.684    ||  0.9400    ||  0.9500    ||   1.743     ||  1.275    ||   5.807     ||  2.555&lt;br /&gt;
|-&lt;br /&gt;
|100_50_65  || 19.11     ||  1.613     ||  1.704    ||  0.9381    ||  0.9501    ||   1.745     ||  1.274    ||   5.628     ||  2.649&lt;br /&gt;
|-&lt;br /&gt;
|100_55_67  || 19.04     ||  1.659     ||  1.739    ||  0.9352    ||  0.9500    ||   1.749     ||  1.270    ||   4.839     ||  2.808&lt;br /&gt;
|-&lt;br /&gt;
|100_56_67  || 18.93     ||  1.667     ||  1.742    ||  0.9347    ||  0.9501    ||   1.750     ||  1.269    ||   4.522     ||  2.692&lt;br /&gt;
|-&lt;br /&gt;
|100_60_68  || 19.04     ||  1.702     ||  1.775    ||  0.9325    ||  0.9500    ||   1.753     ||  1.266    ||   4.326     ||  2.720&lt;br /&gt;
|-&lt;br /&gt;
|100_64_70  || 18.76     ||  1.733     ||  1.799    ||  0.9303    ||  0.9500    ||   1.756     ||  1.263    ||   3.774     ||  2.676&lt;br /&gt;
|-&lt;br /&gt;
|100_68_72  || 18.46     ||  1.771     ||  1.825    ||  0.9279    ||  0.9494    ||   1.759     ||  1.259    ||   3.080     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_70_73  || 18.23     ||  1.784     ||  1.841    ||  0.9277    ||  0.9500    ||   1.760     ||  1.258    ||   3.166     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_80_77  || 16.73     ||  1.855     ||  1.885    ||  0.9261    ||  0.9532    ||   1.767     ||  1.251    ||   1.617     ||  1.818&lt;br /&gt;
|-&lt;br /&gt;
|100_90_80  || 13.86     ||  1.931     ||  1.936    ||  0.9172    ||  0.9494    ||   1.774     ||  1.244    ||  0.2833     || 0.7382&lt;br /&gt;
|-&lt;br /&gt;
|100_95_82  || 11.27     ||  1.967     ||  1.964    ||  0.9243    ||  0.9582    ||   1.777     ||  1.241    || -0.1435     || 6.8954E-02&lt;br /&gt;
|-&lt;br /&gt;
|100_105_86 || 16.96     ||  2.019     ||  2.045    ||  0.9233    ||  0.9617    ||   1.783     ||  1.235    ||   1.268     ||  1.425&lt;br /&gt;
|-&lt;br /&gt;
|100_110_88 || 18.88     ||  2.020     ||  2.073    ||  0.9229    ||  0.9634    ||   1.786     ||  1.232    ||   2.618     ||  2.366&lt;br /&gt;
|-&lt;br /&gt;
|100_120_92 || 17.63     ||  2.064     ||  2.113    ||  0.9044    ||  0.9501    ||   1.794     ||  1.224    ||   2.379     ||  3.790&lt;br /&gt;
|-&lt;br /&gt;
|110_00_54  || 11.70     ||  1.006     ||  1.060    ||  0.9663    ||  0.9498    ||   1.706     ||  1.312    ||   5.370     || 0.4642&lt;br /&gt;
|-&lt;br /&gt;
|110_10_57  || 13.97     ||  1.160     ||  1.232    ||  0.9593    ||  0.9502    ||   1.716     ||  1.301    ||   6.136     || 0.8247&lt;br /&gt;
|-&lt;br /&gt;
|110_20_60  || 15.75     ||  1.298     ||  1.372    ||  0.9526    ||  0.9504    ||   1.726     ||  1.292    ||   5.739     ||  1.330&lt;br /&gt;
|-&lt;br /&gt;
|110_30_63  || 18.56     ||  1.415     ||  1.516    ||  0.9455    ||  0.9500    ||   1.734     ||  1.284    ||   7.122     ||  1.849&lt;br /&gt;
|-&lt;br /&gt;
|110_40_66  || 19.50     ||  1.521     ||  1.622    ||  0.9398    ||  0.9503    ||   1.743     ||  1.275    ||   6.602     ||  1.921&lt;br /&gt;
|-&lt;br /&gt;
|110_50_70  || 19.07     ||  1.618     ||  1.696    ||  0.9336    ||  0.9498    ||   1.751     ||  1.267    ||   4.873     ||  2.085&lt;br /&gt;
|-&lt;br /&gt;
|110_60_73  || 18.32     ||  1.702     ||  1.761    ||  0.9291    ||  0.9507    ||   1.758     ||  1.260    ||   3.471     ||  2.033&lt;br /&gt;
|-&lt;br /&gt;
|110_70_77  || 17.13     ||  1.782     ||  1.816    ||  0.9237    ||  0.9504    ||   1.766     ||  1.252    ||   1.948     ||  1.838&lt;br /&gt;
|-&lt;br /&gt;
|110_80_81  || 15.56     ||  1.853     ||  1.871    ||  0.9192    ||  0.9508    ||   1.773     ||  1.245    ||  0.9878     ||  1.332&lt;br /&gt;
|-&lt;br /&gt;
|110_90_84  || 13.12     ||  1.923     ||  1.926    ||  0.9142    ||  0.9506    ||   1.780     ||  1.238    ||  0.1639     || 0.5301&lt;br /&gt;
|-&lt;br /&gt;
|110_95_86  || 10.73     ||  1.963     ||  1.955    ||  0.9095    ||  0.9486    ||   1.783     ||  1.235    || -0.3746     || 8.1449E-04&lt;br /&gt;
|-&lt;br /&gt;
|110_110_92 || 17.29     ||  2.020     ||  2.055    ||  0.9056    ||  0.9509    ||   1.793     ||  1.225    ||   1.768     ||  2.045&lt;br /&gt;
|-&lt;br /&gt;
|110_120_95 || 17.55     ||  2.048     ||  2.095    ||  0.9014    ||  0.9510    ||   1.799     ||  1.219    ||   2.314     ||  3.774&lt;br /&gt;
|-&lt;br /&gt;
|120_00_57  || 13.14     ||  1.050     ||  1.117    ||  0.9599    ||  0.9497    ||   1.714     ||  1.305    ||   6.304     || 0.4861&lt;br /&gt;
|-&lt;br /&gt;
|120_10_60  || 14.81     ||  1.196     ||  1.268    ||  0.9534    ||  0.9501    ||   1.723     ||  1.295    ||   6.054     || 0.8382&lt;br /&gt;
|-&lt;br /&gt;
|120_20_63  || 17.57     ||  1.323     ||  1.409    ||  0.9458    ||  0.9494    ||   1.732     ||  1.286    ||   6.504     ||  1.409&lt;br /&gt;
|-&lt;br /&gt;
|120_30_67  || 19.50     ||  1.435     ||  1.539    ||  0.9407    ||  0.9503    ||   1.741     ||  1.277    ||   7.263     ||  1.529&lt;br /&gt;
|-&lt;br /&gt;
|120_40_70  || 19.38     ||  1.534     ||  1.621    ||  0.9335    ||  0.9492    ||   1.749     ||  1.269    ||   5.695     ||  1.632&lt;br /&gt;
|-&lt;br /&gt;
|120_50_74  || 18.34     ||  1.621     ||  1.684    ||  0.9294    ||  0.9503    ||   1.756     ||  1.262    ||   3.910     ||  1.864&lt;br /&gt;
|-&lt;br /&gt;
|120_60_77  || 17.24     ||  1.703     ||  1.743    ||  0.9246    ||  0.9507    ||   1.764     ||  1.254    ||   2.381     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|120_70_81  || 16.02     ||  1.780     ||  1.803    ||  0.9197    ||  0.9509    ||   1.771     ||  1.247    ||   1.312     ||  1.511&lt;br /&gt;
|-&lt;br /&gt;
|120_80_84  || 14.49     ||  1.850     ||  1.860    ||  0.9150    ||  0.9509    ||   1.778     ||  1.240    ||  0.5347     ||  1.076&lt;br /&gt;
|-&lt;br /&gt;
|120_90_88  || 12.18     ||  1.918     ||  1.918    ||  0.9096    ||  0.9501    ||   1.785     ||  1.233    || -4.1127E-02 || 0.3613&lt;br /&gt;
|-&lt;br /&gt;
|120_95_90  || 10.06     ||  1.957     ||  1.950    ||  0.9071    ||  0.9499    ||   1.788     ||  1.230    || -0.3241     ||  0.000&lt;br /&gt;
|-&lt;br /&gt;
|120_115_97 || 16.46     ||  2.020     ||  2.066    ||  0.8983    ||  0.9497    ||   1.801     ||  1.216    ||   2.258     ||  2.404&lt;br /&gt;
|-&lt;br /&gt;
|120_120_99 || 17.58     ||  2.008     ||  2.092    ||  0.8967    ||  0.9501    ||   1.804     ||  1.213    ||   4.186     ||  3.647&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Flexibility ==&lt;br /&gt;
&lt;br /&gt;
[[File:Flexibility TJ-II.png|300px|thumb|right|Flexibility diagram of TJ-II magnetic configurations. Several lines of constant rotational transform are highlighted and labelled with the corresponding central &amp;lt;math&amp;gt;\iota/2\pi&amp;lt;/math&amp;gt;-value.]]&lt;br /&gt;
TJ-II has considerable configurational flexibility, as observed in the &#039;flexibility diagram&#039;&amp;lt;ref&amp;gt;E. Ascasíbar, T. Estrada, F. Castejón, A. López-Fraguas, I. Pastor, J. Sánchez, U. Stroth, J. Qin and TJ-II Team, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/45/4/009|Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276–284]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
Some of this flexibility space has been explored, as in the &#039;magnetic well scan&#039; experiments&amp;lt;ref&amp;gt;A. de Aguilera, F. Castejón, E. Ascasíbar, et al. &#039;&#039;Magnetic well scan and confinement in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/55/11/113014|Nucl. Fusion, 55(11):113014, 2015]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
More recently, the rotational transform was found to be of importance for L-H confinement transitions&amp;lt;ref&amp;gt;B. P. van Milligen, T. Estrada, B. Carreras, L. García, and TJ-II Team. &#039;&#039;Importance of the rotational transform for L–H transitions in the TJ-II stellarator&#039;&#039;, [[doi:10.3390/plasma7020024|Plasma, 7(2):446–464, 2024]].&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8724</id>
		<title>TJ-II:Magnetic configuration</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8724"/>
		<updated>2026-10-07T14:27:31Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* Flexibility */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The magnetic configuration of [[TJ-II]] in vacuum is completely determined by the currents flowing through the [[TJ-II:Coil system|external coils]].&lt;br /&gt;
Magnetic configurations are labelled as &#039;xxx_yy_zz&#039;, where&lt;br /&gt;
* &#039;xxx&#039;: 10 times the current (in kA) in the circular coil&lt;br /&gt;
* &#039;yy&#039;: 10 times the current (in kA) in the helical coil&lt;br /&gt;
* &#039;zz&#039;: 10 times the current (in kA) in the vertical field coils&lt;br /&gt;
The current in the toroidal field coils is not specified, as its value is adjusted to guarantee central absorption of the [[TJ-II:Electron Cyclotron Resonant Heating|Electron Cyclotron Resonant Heating]] source (requiring a specific &#039;resonant&#039; value of the magnetic field on the magnetic axis, &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
Configuration list:&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;width: 100%&amp;quot; border=&amp;quot;1&amp;quot;||&lt;br /&gt;
|-&lt;br /&gt;
! Configuration &lt;br /&gt;
! &amp;lt;math&amp;gt;r_{av}&amp;lt;/math&amp;gt; (cm) &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(0)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(a)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{m,av}&amp;lt;/math&amp;gt;(T) &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt; (T) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(0)&amp;lt;/math&amp;gt; (m) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(45)&amp;lt;/math&amp;gt;(m) &lt;br /&gt;
! Shear (%) &lt;br /&gt;
! Well (%)&lt;br /&gt;
|-&lt;br /&gt;
|0_20_13    ||1.139      || 1.185      || 1.194     ||  1.033     || 0.9504     ||  1.644      || 1.374     || 0.7793      ||5.7521E-02&lt;br /&gt;
|-&lt;br /&gt;
|0_30_15    ||4.228      || 1.518      || 1.698     ||  1.019     || 0.9500     ||  1.658      || 1.360     ||  11.85      || 1.050&lt;br /&gt;
|-&lt;br /&gt;
|0_40_18    ||5.903      || 1.756      || 2.003     ||  1.008     || 0.9505     ||  1.671      || 1.347     ||  14.09      || 1.217&lt;br /&gt;
|-&lt;br /&gt;
|0_50_22    ||6.480      || 1.936      || 2.230     || 0.9973     || 0.9502     ||  1.682      || 1.336     ||  15.17      || 2.481&lt;br /&gt;
|-&lt;br /&gt;
|0_60_26    ||8.500      || 2.073      || 2.399     || 0.9885     || 0.9502     ||  1.692      || 1.326     ||  15.70      || 3.218&lt;br /&gt;
|-&lt;br /&gt;
|0_70_29    ||7.147      || 2.187      || 2.434     || 0.9805     || 0.9503     ||  1.701      || 1.317     ||  11.30      || 2.985&lt;br /&gt;
|-&lt;br /&gt;
|0_80_34    ||6.902      || 2.284      || 2.469     || 0.9736     || 0.9506     ||  1.710      || 1.308     ||  8.084      || 2.735&lt;br /&gt;
|-&lt;br /&gt;
|0_90_38    ||6.738      || 2.366      || 2.514     || 0.9663     || 0.9503     ||  1.719      || 1.299     ||  6.269      || 2.534&lt;br /&gt;
|-&lt;br /&gt;
|0_100_42   ||12.59      || 2.436      || 2.667     || 0.9601     || 0.9505     ||  1.727      || 1.291     ||  9.493      || 4.643&lt;br /&gt;
|-&lt;br /&gt;
|0_110_46   ||10.67      || 2.493      || 2.667     || 0.9539     || 0.9503     ||  1.734      || 1.284     ||  6.980      || 4.554&lt;br /&gt;
|-&lt;br /&gt;
|0_120_50   ||12.71      || 2.548      || 2.667     || 0.9482     || 0.9504     ||  1.742      || 1.276     ||  4.683      || 4.272&lt;br /&gt;
|-&lt;br /&gt;
|10_20_18   || 2.557     ||  1.148     ||  1.184    ||   1.024    ||  0.9514    ||   1.652     ||  1.366    ||   3.183     || 0.2469&lt;br /&gt;
|-&lt;br /&gt;
|10_30_20   || 6.083     ||  1.438     ||  1.602    ||   1.010    ||  0.9501    ||   1.666     ||  1.352    ||   11.35     ||  1.398&lt;br /&gt;
|-&lt;br /&gt;
|10_40_24   || 6.921     ||  1.659     ||  1.880    ||   1.000    ||  0.9504    ||   1.678     ||  1.340    ||   13.34     ||  2.751&lt;br /&gt;
|-&lt;br /&gt;
|10_50_27   || 8.140     ||  1.826     ||  1.997    ||  0.9909    ||  0.9504    ||   1.688     ||  1.329    ||   9.321     ||  3.241&lt;br /&gt;
|-&lt;br /&gt;
|10_60_31   || 9.350     ||  1.965     ||  2.183    ||  0.9826    ||  0.9505    ||   1.698     ||  1.319    ||   11.11     ||  3.084&lt;br /&gt;
|-&lt;br /&gt;
|10_70_35   || 10.10     ||  2.077     ||  2.288    ||  0.9750    ||  0.9505    ||   1.707     ||  1.310    ||   10.16     ||  3.597&lt;br /&gt;
|-&lt;br /&gt;
|10_80_38   || 9.810     ||  2.174     ||  2.371    ||  0.9674    ||  0.9502    ||   1.716     ||  1.302    ||   9.037     ||  3.908&lt;br /&gt;
|-&lt;br /&gt;
|10_90_42   || 10.54     ||  2.257     ||  2.434    ||  0.9610    ||  0.9503    ||   1.724     ||  1.294    ||   7.851     ||  4.281&lt;br /&gt;
|-&lt;br /&gt;
|10_100_47  || 10.21     ||  2.327     ||  2.482    ||  0.9546    ||  0.9502    ||   1.732     ||  1.286    ||   6.647     ||  4.236&lt;br /&gt;
|-&lt;br /&gt;
|10_110_51  || 11.11     ||  2.395     ||  2.547    ||  0.9488    ||  0.9501    ||   1.740     ||  1.278    ||   6.331     ||  5.121&lt;br /&gt;
|-&lt;br /&gt;
|10_120_55  || 10.04     ||  2.451     ||  2.565    ||  0.9432    ||  0.9502    ||   1.747     ||  1.271    ||   4.674     ||  4.426&lt;br /&gt;
|-&lt;br /&gt;
|20_10_21   || 1.213     || 0.7902     || 0.7956    ||   1.028    ||  0.9503    ||   1.645     ||  1.373    ||  0.6830     || 3.7624E-02&lt;br /&gt;
|-&lt;br /&gt;
|20_20_22   || 3.952     ||  1.136     ||  1.185    ||   1.014    ||  0.9500    ||   1.661     ||  1.357    ||   4.350     || 0.4717&lt;br /&gt;
|-&lt;br /&gt;
|20_30_25   || 6.779     ||  1.395     ||  1.521    ||   1.003    ||  0.9502    ||   1.673     ||  1.344    ||   9.049     ||  1.550&lt;br /&gt;
|-&lt;br /&gt;
|20_40_28   || 8.475     ||  1.592     ||  1.771    ||  0.9922    ||  0.9498    ||   1.685     ||  1.333    ||   11.25     ||  2.879&lt;br /&gt;
|-&lt;br /&gt;
|20_50_32   || 8.039     ||  1.756     ||  1.906    ||  0.9842    ||  0.9505    ||   1.695     ||  1.323    ||   8.571     ||  3.131&lt;br /&gt;
|-&lt;br /&gt;
|20_60_35   || 11.21     ||  1.884     ||  1.997    ||  0.9755    ||  0.9498    ||   1.705     ||  1.313    ||   5.968     ||  1.980&lt;br /&gt;
|-&lt;br /&gt;
|20_70_39   || 11.08     ||  1.994     ||  2.154    ||  0.9689    ||  0.9504    ||   1.714     ||  1.304    ||   7.982     ||  3.385&lt;br /&gt;
|-&lt;br /&gt;
|20_80_43   || 12.14     ||  2.092     ||  2.255    ||  0.9614    ||  0.9497    ||   1.722     ||  1.296    ||   7.811     ||  4.133&lt;br /&gt;
|-&lt;br /&gt;
|20_90_47   || 12.83     ||  2.174     ||  2.324    ||  0.9558    ||  0.9503    ||   1.730     ||  1.288    ||   6.862     ||  4.713&lt;br /&gt;
|-&lt;br /&gt;
|20_100_51  || 12.68     ||  2.246     ||  2.379    ||  0.9498    ||  0.9503    ||   1.738     ||  1.280    ||   5.945     ||  4.930&lt;br /&gt;
|-&lt;br /&gt;
|20_110_55  || 13.79     ||  2.313     ||  2.434    ||  0.9443    ||  0.9505    ||   1.745     ||  1.273    ||   5.248     ||  5.117&lt;br /&gt;
|-&lt;br /&gt;
|20_120_59  || 13.91     ||  2.368     ||  2.483    ||  0.9386    ||  0.9502    ||   1.752     ||  1.265    ||   4.822     ||  5.418&lt;br /&gt;
|-&lt;br /&gt;
|30_10_25   || 2.709     || 0.8385     || 0.8507    ||   1.018    ||  0.9501    ||   1.654     ||  1.363    ||   1.452     || 0.1431&lt;br /&gt;
|-&lt;br /&gt;
|30_20_27   || 5.443     ||  1.134     ||  1.189    ||   1.007    ||  0.9514    ||   1.669     ||  1.349    ||   4.847     || 0.7001&lt;br /&gt;
|-&lt;br /&gt;
|30_30_30   || 8.180     ||  1.368     ||  1.481    ||  0.9956    ||  0.9506    ||   1.681     ||  1.337    ||   8.332     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|30_40_33   || 9.756     ||  1.550     ||  1.687    ||  0.9860    ||  0.9503    ||   1.692     ||  1.326    ||   8.877     ||  2.798&lt;br /&gt;
|-&lt;br /&gt;
|30_50_37   || 11.16     ||  1.702     ||  1.878    ||  0.9779    ||  0.9503    ||   1.702     ||  1.316    ||   10.37     ||  4.941&lt;br /&gt;
|-&lt;br /&gt;
|30_60_40   || 9.262     ||  1.827     ||  1.936    ||  0.9706    ||  0.9505    ||   1.711     ||  1.307    ||   5.952     ||  3.624&lt;br /&gt;
|-&lt;br /&gt;
|30_70_44   || 12.28     ||  1.937     ||  2.007    ||  0.9631    ||  0.9502    ||   1.720     ||  1.298    ||   3.593     ||  4.431&lt;br /&gt;
|-&lt;br /&gt;
|30_80_48   || 13.28     ||  2.033     ||  2.149    ||  0.9567    ||  0.9502    ||   1.728     ||  1.290    ||   5.702     ||  3.674&lt;br /&gt;
|-&lt;br /&gt;
|30_90_52   || 14.16     ||  2.115     ||  2.231    ||  0.9504    ||  0.9501    ||   1.736     ||  1.282    ||   5.476     ||  4.227&lt;br /&gt;
|-&lt;br /&gt;
|30_100_56  || 14.97     ||  2.187     ||  2.295    ||  0.9448    ||  0.9502    ||   1.743     ||  1.275    ||   4.949     ||  4.755&lt;br /&gt;
|-&lt;br /&gt;
|30_110_59  || 15.76     ||  2.246     ||  2.356    ||  0.9391    ||  0.9500    ||   1.751     ||  1.267    ||   4.920     ||  5.215&lt;br /&gt;
|-&lt;br /&gt;
|30_120_63  || 14.48     ||  2.306     ||  2.389    ||  0.9343    ||  0.9504    ||   1.758     ||  1.260    ||   3.573     ||  5.025&lt;br /&gt;
|-&lt;br /&gt;
|40_00_27   || 1.350     || 0.5464     || 0.5471    ||   1.024    ||  0.9504    ||   1.647     ||  1.371    ||  0.1331     || 2.4768E-02&lt;br /&gt;
|-&lt;br /&gt;
|40_10_29   || 4.111     || 0.8821     || 0.9010    ||   1.010    ||  0.9510    ||   1.663     ||  1.355    ||   2.152     || 0.2456&lt;br /&gt;
|-&lt;br /&gt;
|40_20_31   || 6.646     ||  1.146     ||  1.202    ||  0.9975    ||  0.9501    ||   1.677     ||  1.341    ||   4.928     || 0.8185&lt;br /&gt;
|-&lt;br /&gt;
|40_30_34   || 9.328     ||  1.354     ||  1.452    ||  0.9884    ||  0.9506    ||   1.688     ||  1.330    ||   7.247     ||  1.826&lt;br /&gt;
|-&lt;br /&gt;
|40_40_37   || 11.15     ||  1.523     ||  1.646    ||  0.9788    ||  0.9498    ||   1.699     ||  1.319    ||   8.061     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|40_50_41   || 12.66     ||  1.666     ||  1.797    ||  0.9719    ||  0.9506    ||   1.708     ||  1.310    ||   7.872     ||  4.310&lt;br /&gt;
|-&lt;br /&gt;
|40_60_44   || 12.34     ||  1.786     ||  1.927    ||  0.9637    ||  0.9497    ||   1.717     ||  1.301    ||   7.879     ||  5.834&lt;br /&gt;
|-&lt;br /&gt;
|40_70_48   || 9.734     ||  1.894     ||  1.963    ||  0.9579    ||  0.9504    ||   1.726     ||  1.292    ||   3.625     ||  3.668&lt;br /&gt;
|-&lt;br /&gt;
|40_80_52   || 13.96     ||  1.986     ||  2.067    ||  0.9515    ||  0.9503    ||   1.734     ||  1.284    ||   4.054     ||  3.028&lt;br /&gt;
|-&lt;br /&gt;
|40_90_56   || 15.39     ||  2.062     ||  2.156    ||  0.9457    ||  0.9504    ||   1.741     ||  1.277    ||   4.529     ||  3.841&lt;br /&gt;
|-&lt;br /&gt;
|40_100_60  || 16.40     ||  2.132     ||  2.232    ||  0.9400    ||  0.9502    ||   1.749     ||  1.269    ||   4.683     ||  4.355&lt;br /&gt;
|-&lt;br /&gt;
|40_110_64  || 18.12     ||  2.199     ||  2.288    ||  0.9348    ||  0.9503    ||   1.756     ||  1.262    ||   4.049     ||  4.651&lt;br /&gt;
|-&lt;br /&gt;
|40_120_68  || 16.81     ||  2.256     ||  2.327    ||  0.9295    ||  0.9501    ||   1.763     ||  1.255    ||   3.158     ||  4.904&lt;br /&gt;
|-&lt;br /&gt;
|50_00_31   || 2.818     || 0.6329     || 0.6375    ||   1.013    ||  0.9498    ||   1.657     ||  1.361    ||  0.7286     || 6.1871E-02&lt;br /&gt;
|-&lt;br /&gt;
|50_10_33   || 5.588     || 0.9254     || 0.9532    ||   1.001    ||  0.9506    ||   1.672     ||  1.346    ||   3.003     || 0.3605&lt;br /&gt;
|-&lt;br /&gt;
|50_20_36   || 8.222     ||  1.160     ||  1.216    ||  0.9902    ||  0.9502    ||   1.684     ||  1.334    ||   4.838     ||  1.060&lt;br /&gt;
|-&lt;br /&gt;
|50_30_39   || 10.67     ||  1.352     ||  1.435    ||  0.9815    ||  0.9505    ||   1.695     ||  1.323    ||   6.163     ||  2.008&lt;br /&gt;
|-&lt;br /&gt;
|50_40_42   || 12.44     ||  1.508     ||  1.609    ||  0.9733    ||  0.9504    ||   1.705     ||  1.313    ||   6.719     ||  2.910&lt;br /&gt;
|-&lt;br /&gt;
|50_50_46   || 13.94     ||  1.644     ||  1.758    ||  0.9661    ||  0.9505    ||   1.714     ||  1.303    ||   6.944     ||  4.001&lt;br /&gt;
|-&lt;br /&gt;
|50_60_49   || 15.09     ||  1.757     ||  1.887    ||  0.9587    ||  0.9502    ||   1.723     ||  1.295    ||   7.390     ||  6.217&lt;br /&gt;
|-&lt;br /&gt;
|50_70_53   || 13.03     ||  1.855     ||  1.955    ||  0.9524    ||  0.9502    ||   1.731     ||  1.287    ||   5.353     ||  5.830&lt;br /&gt;
|-&lt;br /&gt;
|50_80_56   || 16.73     ||  1.949     ||  2.004    ||  0.9463    ||  0.9501    ||   1.739     ||  1.279    ||   2.807     ||  4.003&lt;br /&gt;
|-&lt;br /&gt;
|50_90_60   || 16.70     ||  2.011     ||  2.101    ||  0.9407    ||  0.9502    ||   1.747     ||  1.271    ||   4.501     ||  3.444&lt;br /&gt;
|-&lt;br /&gt;
|50_100_64  || 18.15     ||  2.090     ||  2.183    ||  0.9351    ||  0.9500    ||   1.754     ||  1.264    ||   4.434     ||  3.907&lt;br /&gt;
|-&lt;br /&gt;
|50_110_68  || 17.53     ||  2.154     ||  2.223    ||  0.9297    ||  0.9498    ||   1.762     ||  1.256    ||   3.205     ||  4.270&lt;br /&gt;
|-&lt;br /&gt;
|50_120_72  || 19.13     ||  2.213     ||  2.288    ||  0.9250    ||  0.9501    ||   1.768     ||  1.250    ||   3.417     ||  4.378&lt;br /&gt;
|-&lt;br /&gt;
|60_00_35   || 4.247     || 0.7126     || 0.7205    ||   1.003    ||  0.9498    ||   1.667     ||  1.352    ||   1.108     || 0.1270&lt;br /&gt;
|-&lt;br /&gt;
|60_10_37   || 6.862     || 0.9679     ||  1.002    ||  0.9934    ||  0.9509    ||   1.680     ||  1.338    ||   3.520     || 0.4827&lt;br /&gt;
|-&lt;br /&gt;
|60_20_40   || 9.669     ||  1.179     ||  1.240    ||  0.9831    ||  0.9503    ||   1.692     ||  1.326    ||   5.202     ||  1.236&lt;br /&gt;
|-&lt;br /&gt;
|60_30_43   || 12.01     ||  1.354     ||  1.435    ||  0.9747    ||  0.9502    ||   1.702     ||  1.316    ||   5.973     ||  2.132&lt;br /&gt;
|-&lt;br /&gt;
|60_40_46   || 13.48     ||  1.500     ||  1.593    ||  0.9672    ||  0.9503    ||   1.712     ||  1.306    ||   6.170     ||  2.806&lt;br /&gt;
|-&lt;br /&gt;
|60_50_50   || 15.36     ||  1.627     ||  1.732    ||  0.9601    ||  0.9504    ||   1.721     ||  1.297    ||   6.467     ||  3.895&lt;br /&gt;
|-&lt;br /&gt;
|60_60_53   || 16.79     ||  1.734     ||  1.851    ||  0.9528    ||  0.9499    ||   1.729     ||  1.289    ||   6.731     ||  5.666&lt;br /&gt;
|-&lt;br /&gt;
|60_70_57   || 15.88     ||  1.829     ||  1.934    ||  0.9473    ||  0.9502    ||   1.737     ||  1.281    ||   5.736     ||  6.958&lt;br /&gt;
|-&lt;br /&gt;
|60_80_61   || 13.66     ||  1.918     ||  1.968    ||  0.9428    ||  0.9514    ||   1.745     ||  1.273    ||   2.622     ||  4.555&lt;br /&gt;
|-&lt;br /&gt;
|60_90_64   || 17.29     ||  2.009     ||  2.063    ||  0.9359    ||  0.9501    ||   1.753     ||  1.265    ||   2.640     ||  1.637&lt;br /&gt;
|-&lt;br /&gt;
|60_100_68  || 17.62     ||  2.049     ||  2.122    ||  0.9304    ||  0.9497    ||   1.760     ||  1.258    ||   3.560     ||  3.718&lt;br /&gt;
|-&lt;br /&gt;
|60_110_72  || 17.50     ||  2.118     ||  2.177    ||  0.9257    ||  0.9501    ||   1.767     ||  1.251    ||   2.811     ||  4.023&lt;br /&gt;
|-&lt;br /&gt;
|60_120_76  || 17.78     ||  2.174     ||  2.222    ||  0.9217    ||  0.9510    ||   1.774     ||  1.244    ||   2.209     ||  4.211&lt;br /&gt;
|-&lt;br /&gt;
|70_00_39   || 5.731     || 0.7825     || 0.7975    ||  0.9949    ||  0.9497    ||   1.675     ||  1.343    ||   1.908     || 0.2335&lt;br /&gt;
|-&lt;br /&gt;
|70_10_41   || 8.418     ||  1.009     ||  1.048    ||  0.9860    ||  0.9509    ||   1.688     ||  1.330    ||   3.845     || 0.6755&lt;br /&gt;
|-&lt;br /&gt;
|70_20_44   || 11.09     ||  1.201     ||  1.265    ||  0.9767    ||  0.9504    ||   1.699     ||  1.319    ||   5.345     ||  1.317&lt;br /&gt;
|-&lt;br /&gt;
|70_30_47   || 13.41     ||  1.361     ||  1.441    ||  0.9688    ||  0.9504    ||   1.709     ||  1.309    ||   5.859     ||  2.187&lt;br /&gt;
|-&lt;br /&gt;
|70_40_51   || 14.99     ||  1.496     ||  1.591    ||  0.9615    ||  0.9503    ||   1.718     ||  1.300    ||   6.348     ||  2.859&lt;br /&gt;
|-&lt;br /&gt;
|70_50_54   || 16.87     ||  1.617     ||  1.712    ||  0.9543    ||  0.9501    ||   1.727     ||  1.291    ||   5.843     ||  3.756&lt;br /&gt;
|-&lt;br /&gt;
|70_60_57   || 17.89     ||  1.718     ||  1.823    ||  0.9479    ||  0.9500    ||   1.735     ||  1.283    ||   6.140     ||  4.746&lt;br /&gt;
|-&lt;br /&gt;
|70_70_61   || 18.26     ||  1.812     ||  1.928    ||  0.9423    ||  0.9503    ||   1.743     ||  1.275    ||   6.353     ||  6.812&lt;br /&gt;
|-&lt;br /&gt;
|70_80_65   || 16.37     ||  1.896     ||  1.962    ||  0.9363    ||  0.9499    ||   1.751     ||  1.267    ||   3.469     ||  5.948&lt;br /&gt;
|-&lt;br /&gt;
|70_90_68   || 9.135     ||  1.980     ||  1.988    ||  0.9317    ||  0.9506    ||   1.758     ||  1.260    ||  0.3692     || 0.1186&lt;br /&gt;
|-&lt;br /&gt;
|70_100_72  || 18.64     ||  2.007     ||  2.094    ||  0.9267    ||  0.9506    ||   1.765     ||  1.253    ||   4.327     ||  3.356&lt;br /&gt;
|-&lt;br /&gt;
|70_110_76  || 18.23     ||  2.088     ||  2.147    ||  0.9219    ||  0.9507    ||   1.772     ||  1.246    ||   2.792     ||  3.707&lt;br /&gt;
|-&lt;br /&gt;
|70_120_80  || 17.89     ||  2.145     ||  2.184    ||  0.9171    ||  0.9506    ||   1.779     ||  1.239    ||   1.846     ||  4.043&lt;br /&gt;
|-&lt;br /&gt;
|80_00_42   ||7.247      ||0.8436      ||0.8697     || 0.9869     || 0.9497     ||  1.684      || 1.335     ||  3.094      ||0.2402&lt;br /&gt;
|-&lt;br /&gt;
|80_10_45   ||9.865      || 1.049      || 1.095     || 0.9794     || 0.9513     ||  1.695      || 1.323     ||  4.371      ||0.7359&lt;br /&gt;
|-&lt;br /&gt;
|80_20_48   ||12.28      || 1.226      || 1.290     || 0.9697     || 0.9500     ||  1.706      || 1.312     ||  5.206      || 1.327&lt;br /&gt;
|-&lt;br /&gt;
|80_30_51   ||14.38      || 1.370      || 1.454     || 0.9626     || 0.9503     ||  1.715      || 1.303     ||  6.088      || 2.102&lt;br /&gt;
|-&lt;br /&gt;
|80_40_54   ||16.47      || 1.500      || 1.594     || 0.9549     || 0.9497     ||  1.724      || 1.294     ||  6.263      || 2.799&lt;br /&gt;
|-&lt;br /&gt;
|80_50_58   ||17.63      || 1.612      || 1.706     || 0.9492     || 0.9503     ||  1.733      || 1.285     ||  5.842      || 3.329&lt;br /&gt;
|-&lt;br /&gt;
|80_60_61   ||18.84      || 1.712      || 1.814     || 0.9436     || 0.9507     ||  1.741      || 1.277     ||  5.984      || 3.990&lt;br /&gt;
|-&lt;br /&gt;
|80_70_65   ||19.27      || 1.799      || 1.898     || 0.9372     || 0.9501     ||  1.749      || 1.269     ||  5.555      || 4.728&lt;br /&gt;
|-&lt;br /&gt;
|80_80_69   ||17.96      || 1.880      || 1.935     || 0.9321     || 0.9503     ||  1.756      || 1.262     ||  2.921      || 3.774&lt;br /&gt;
|-&lt;br /&gt;
|80_90_73   ||13.42      || 1.957      || 1.982     || 0.9266     || 0.9500     ||  1.764      || 1.254     ||  1.312      ||0.6938&lt;br /&gt;
|-&lt;br /&gt;
|80_100_76  || 18.53     ||  2.008     ||  2.065    ||  0.9220    ||  0.9504    ||   1.770     ||  1.247    ||   2.839     ||  1.773&lt;br /&gt;
|-&lt;br /&gt;
|80_110_80  || 18.41     ||  2.059     ||  2.117    ||  0.9176    ||  0.9507    ||   1.777     ||  1.241    ||   2.847     ||  3.632&lt;br /&gt;
|-&lt;br /&gt;
|80_120_84  || 18.26     ||  2.117     ||  2.157    ||  0.9122    ||  0.9496    ||   1.784     ||  1.234    ||   1.872     ||  3.986&lt;br /&gt;
|-&lt;br /&gt;
|90_00_46   || 8.679     || 0.9022     || 0.9354    ||  0.9802    ||  0.9501    ||   1.691     ||  1.327    ||   3.678     || 0.3981&lt;br /&gt;
|-&lt;br /&gt;
|90_10_49   || 11.45     ||  1.090     ||  1.146    ||  0.9717    ||  0.9502    ||   1.702     ||  1.315    ||   5.148     || 0.8099&lt;br /&gt;
|-&lt;br /&gt;
|90_20_52   || 12.44     ||  1.247     ||  1.323    ||  0.9640    ||  0.9503    ||   1.712     ||  1.305    ||   6.100     ||  1.079&lt;br /&gt;
|-&lt;br /&gt;
|90_30_55   || 16.14     ||  1.383     ||  1.475    ||  0.9571    ||  0.9504    ||   1.722     ||  1.296    ||   6.607     ||  2.158&lt;br /&gt;
|-&lt;br /&gt;
|90_40_58   || 17.45     ||  1.506     ||  1.597    ||  0.9499    ||  0.9501    ||   1.731     ||  1.287    ||   6.012     ||  2.629&lt;br /&gt;
|-&lt;br /&gt;
|90_50_62   || 18.70     ||  1.609     ||  1.706    ||  0.9438    ||  0.9501    ||   1.739     ||  1.279    ||   6.003     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|90_60_65   || 18.77     ||  1.703     ||  1.789    ||  0.9381    ||  0.9502    ||   1.747     ||  1.271    ||   5.045     ||  3.047&lt;br /&gt;
|-&lt;br /&gt;
|90_70_69   || 18.43     ||  1.787     ||  1.852    ||  0.9324    ||  0.9500    ||   1.754     ||  1.263    ||   3.623     ||  3.117&lt;br /&gt;
|-&lt;br /&gt;
|90_80_73   || 17.72     ||  1.868     ||  1.909    ||  0.9269    ||  0.9497    ||   1.762     ||  1.256    ||   2.217     ||  2.354&lt;br /&gt;
|-&lt;br /&gt;
|90_90_76   || 14.40     ||  1.940     ||  1.956    ||  0.9221    ||  0.9499    ||   1.769     ||  1.249    ||  0.8079     || 0.8326&lt;br /&gt;
|-&lt;br /&gt;
|90_100_80  || 18.53     ||  2.009     ||  2.038    ||  0.9176    ||  0.9503    ||   1.776     ||  1.242    ||   1.484     ||  1.095&lt;br /&gt;
|-&lt;br /&gt;
|90_110_84  || 18.97     ||  2.021     ||  2.094    ||  0.9129    ||  0.9502    ||   1.783     ||  1.235    ||   3.625     ||  3.669&lt;br /&gt;
|-&lt;br /&gt;
|90_120_88  || 17.79     ||  2.090     ||  2.129    ||  0.9077    ||  0.9494    ||   1.789     ||  1.229    ||   1.827     ||  3.862&lt;br /&gt;
|-&lt;br /&gt;
|100_00_50  || 10.07     || 0.9544     || 0.9970    ||  0.9732    ||  0.9499    ||   1.699     ||  1.319    ||   4.471     || 0.4341&lt;br /&gt;
|-&lt;br /&gt;
|100_10_53  || 12.78     ||  1.127     ||  1.186    ||  0.9649    ||  0.9499    ||   1.710     ||  1.308    ||   5.262     || 0.9629&lt;br /&gt;
|-&lt;br /&gt;
|100_16_55  || 13.69     ||  1.215     ||  1.287    ||  0.9610    ||  0.9501    ||   1.715     ||  1.302    ||   5.901     ||  1.023&lt;br /&gt;
|-&lt;br /&gt;
|100_20_56  || 10.86     ||  1.271     ||  1.324    ||  0.9583    ||  0.9502    ||   1.719     ||  1.299    ||   4.120     || 0.8295&lt;br /&gt;
|-&lt;br /&gt;
|100_22_56  || 15.40     ||  1.309     ||  1.381    ||  0.9412    ||  0.9362    ||   1.722     ||  1.296    ||   5.552     ||  1.648&lt;br /&gt;
|-&lt;br /&gt;
|100_24_58  || 15.90     ||  1.326     ||  1.406    ||  0.9552    ||  0.9499    ||   1.722     ||  1.295    ||   6.105     ||  1.792&lt;br /&gt;
|-&lt;br /&gt;
|100_26_58  || 16.42     ||  1.352     ||  1.435    ||  0.9538    ||  0.9499    ||   1.724     ||  1.293    ||   6.137     ||  1.888&lt;br /&gt;
|-&lt;br /&gt;
|100_28_59  || 17.07     ||  1.375     ||  1.464    ||  0.9527    ||  0.9501    ||   1.726     ||  1.291    ||   6.475     ||  1.983&lt;br /&gt;
|-&lt;br /&gt;
|100_30_59  || 17.29     ||  1.398     ||  1.490    ||  0.9511    ||  0.9500    ||   1.728     ||  1.289    ||   6.561     ||  2.075&lt;br /&gt;
|-&lt;br /&gt;
|100_32_60  || 17.74     ||  1.423     ||  1.517    ||  0.9499    ||  0.9499    ||   1.730     ||  1.288    ||   6.596     ||  2.165&lt;br /&gt;
|-&lt;br /&gt;
|100_36_61  || 18.37     ||  1.467     ||  1.567    ||  0.9475    ||  0.9501    ||   1.733     ||  1.284    ||   6.819     ||  2.183&lt;br /&gt;
|-&lt;br /&gt;
|100_40_63  || 18.77     ||  1.509     ||  1.608    ||  0.9450    ||  0.9500    ||   1.736     ||  1.281    ||   6.553     ||  2.304&lt;br /&gt;
|-&lt;br /&gt;
|100_44_64  || 19.25     ||  1.551     ||  1.653    ||  0.9426    ||  0.9500    ||   1.740     ||  1.278    ||   6.569     ||  2.360&lt;br /&gt;
|-&lt;br /&gt;
|100_48_65  || 19.16     ||  1.591     ||  1.684    ||  0.9400    ||  0.9500    ||   1.743     ||  1.275    ||   5.807     ||  2.555&lt;br /&gt;
|-&lt;br /&gt;
|100_50_65  || 19.11     ||  1.613     ||  1.704    ||  0.9381    ||  0.9501    ||   1.745     ||  1.274    ||   5.628     ||  2.649&lt;br /&gt;
|-&lt;br /&gt;
|100_55_67  || 19.04     ||  1.659     ||  1.739    ||  0.9352    ||  0.9500    ||   1.749     ||  1.270    ||   4.839     ||  2.808&lt;br /&gt;
|-&lt;br /&gt;
|100_56_67  || 18.93     ||  1.667     ||  1.742    ||  0.9347    ||  0.9501    ||   1.750     ||  1.269    ||   4.522     ||  2.692&lt;br /&gt;
|-&lt;br /&gt;
|100_60_68  || 19.04     ||  1.702     ||  1.775    ||  0.9325    ||  0.9500    ||   1.753     ||  1.266    ||   4.326     ||  2.720&lt;br /&gt;
|-&lt;br /&gt;
|100_64_70  || 18.76     ||  1.733     ||  1.799    ||  0.9303    ||  0.9500    ||   1.756     ||  1.263    ||   3.774     ||  2.676&lt;br /&gt;
|-&lt;br /&gt;
|100_68_72  || 18.46     ||  1.771     ||  1.825    ||  0.9279    ||  0.9494    ||   1.759     ||  1.259    ||   3.080     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_70_73  || 18.23     ||  1.784     ||  1.841    ||  0.9277    ||  0.9500    ||   1.760     ||  1.258    ||   3.166     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_80_77  || 16.73     ||  1.855     ||  1.885    ||  0.9261    ||  0.9532    ||   1.767     ||  1.251    ||   1.617     ||  1.818&lt;br /&gt;
|-&lt;br /&gt;
|100_90_80  || 13.86     ||  1.931     ||  1.936    ||  0.9172    ||  0.9494    ||   1.774     ||  1.244    ||  0.2833     || 0.7382&lt;br /&gt;
|-&lt;br /&gt;
|100_95_82  || 11.27     ||  1.967     ||  1.964    ||  0.9243    ||  0.9582    ||   1.777     ||  1.241    || -0.1435     || 6.8954E-02&lt;br /&gt;
|-&lt;br /&gt;
|100_105_86 || 16.96     ||  2.019     ||  2.045    ||  0.9233    ||  0.9617    ||   1.783     ||  1.235    ||   1.268     ||  1.425&lt;br /&gt;
|-&lt;br /&gt;
|100_110_88 || 18.88     ||  2.020     ||  2.073    ||  0.9229    ||  0.9634    ||   1.786     ||  1.232    ||   2.618     ||  2.366&lt;br /&gt;
|-&lt;br /&gt;
|100_120_92 || 17.63     ||  2.064     ||  2.113    ||  0.9044    ||  0.9501    ||   1.794     ||  1.224    ||   2.379     ||  3.790&lt;br /&gt;
|-&lt;br /&gt;
|110_00_54  || 11.70     ||  1.006     ||  1.060    ||  0.9663    ||  0.9498    ||   1.706     ||  1.312    ||   5.370     || 0.4642&lt;br /&gt;
|-&lt;br /&gt;
|110_10_57  || 13.97     ||  1.160     ||  1.232    ||  0.9593    ||  0.9502    ||   1.716     ||  1.301    ||   6.136     || 0.8247&lt;br /&gt;
|-&lt;br /&gt;
|110_20_60  || 15.75     ||  1.298     ||  1.372    ||  0.9526    ||  0.9504    ||   1.726     ||  1.292    ||   5.739     ||  1.330&lt;br /&gt;
|-&lt;br /&gt;
|110_30_63  || 18.56     ||  1.415     ||  1.516    ||  0.9455    ||  0.9500    ||   1.734     ||  1.284    ||   7.122     ||  1.849&lt;br /&gt;
|-&lt;br /&gt;
|110_40_66  || 19.50     ||  1.521     ||  1.622    ||  0.9398    ||  0.9503    ||   1.743     ||  1.275    ||   6.602     ||  1.921&lt;br /&gt;
|-&lt;br /&gt;
|110_50_70  || 19.07     ||  1.618     ||  1.696    ||  0.9336    ||  0.9498    ||   1.751     ||  1.267    ||   4.873     ||  2.085&lt;br /&gt;
|-&lt;br /&gt;
|110_60_73  || 18.32     ||  1.702     ||  1.761    ||  0.9291    ||  0.9507    ||   1.758     ||  1.260    ||   3.471     ||  2.033&lt;br /&gt;
|-&lt;br /&gt;
|110_70_77  || 17.13     ||  1.782     ||  1.816    ||  0.9237    ||  0.9504    ||   1.766     ||  1.252    ||   1.948     ||  1.838&lt;br /&gt;
|-&lt;br /&gt;
|110_80_81  || 15.56     ||  1.853     ||  1.871    ||  0.9192    ||  0.9508    ||   1.773     ||  1.245    ||  0.9878     ||  1.332&lt;br /&gt;
|-&lt;br /&gt;
|110_90_84  || 13.12     ||  1.923     ||  1.926    ||  0.9142    ||  0.9506    ||   1.780     ||  1.238    ||  0.1639     || 0.5301&lt;br /&gt;
|-&lt;br /&gt;
|110_95_86  || 10.73     ||  1.963     ||  1.955    ||  0.9095    ||  0.9486    ||   1.783     ||  1.235    || -0.3746     || 8.1449E-04&lt;br /&gt;
|-&lt;br /&gt;
|110_110_92 || 17.29     ||  2.020     ||  2.055    ||  0.9056    ||  0.9509    ||   1.793     ||  1.225    ||   1.768     ||  2.045&lt;br /&gt;
|-&lt;br /&gt;
|110_120_95 || 17.55     ||  2.048     ||  2.095    ||  0.9014    ||  0.9510    ||   1.799     ||  1.219    ||   2.314     ||  3.774&lt;br /&gt;
|-&lt;br /&gt;
|120_00_57  || 13.14     ||  1.050     ||  1.117    ||  0.9599    ||  0.9497    ||   1.714     ||  1.305    ||   6.304     || 0.4861&lt;br /&gt;
|-&lt;br /&gt;
|120_10_60  || 14.81     ||  1.196     ||  1.268    ||  0.9534    ||  0.9501    ||   1.723     ||  1.295    ||   6.054     || 0.8382&lt;br /&gt;
|-&lt;br /&gt;
|120_20_63  || 17.57     ||  1.323     ||  1.409    ||  0.9458    ||  0.9494    ||   1.732     ||  1.286    ||   6.504     ||  1.409&lt;br /&gt;
|-&lt;br /&gt;
|120_30_67  || 19.50     ||  1.435     ||  1.539    ||  0.9407    ||  0.9503    ||   1.741     ||  1.277    ||   7.263     ||  1.529&lt;br /&gt;
|-&lt;br /&gt;
|120_40_70  || 19.38     ||  1.534     ||  1.621    ||  0.9335    ||  0.9492    ||   1.749     ||  1.269    ||   5.695     ||  1.632&lt;br /&gt;
|-&lt;br /&gt;
|120_50_74  || 18.34     ||  1.621     ||  1.684    ||  0.9294    ||  0.9503    ||   1.756     ||  1.262    ||   3.910     ||  1.864&lt;br /&gt;
|-&lt;br /&gt;
|120_60_77  || 17.24     ||  1.703     ||  1.743    ||  0.9246    ||  0.9507    ||   1.764     ||  1.254    ||   2.381     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|120_70_81  || 16.02     ||  1.780     ||  1.803    ||  0.9197    ||  0.9509    ||   1.771     ||  1.247    ||   1.312     ||  1.511&lt;br /&gt;
|-&lt;br /&gt;
|120_80_84  || 14.49     ||  1.850     ||  1.860    ||  0.9150    ||  0.9509    ||   1.778     ||  1.240    ||  0.5347     ||  1.076&lt;br /&gt;
|-&lt;br /&gt;
|120_90_88  || 12.18     ||  1.918     ||  1.918    ||  0.9096    ||  0.9501    ||   1.785     ||  1.233    || -4.1127E-02 || 0.3613&lt;br /&gt;
|-&lt;br /&gt;
|120_95_90  || 10.06     ||  1.957     ||  1.950    ||  0.9071    ||  0.9499    ||   1.788     ||  1.230    || -0.3241     ||  0.000&lt;br /&gt;
|-&lt;br /&gt;
|120_115_97 || 16.46     ||  2.020     ||  2.066    ||  0.8983    ||  0.9497    ||   1.801     ||  1.216    ||   2.258     ||  2.404&lt;br /&gt;
|-&lt;br /&gt;
|120_120_99 || 17.58     ||  2.008     ||  2.092    ||  0.8967    ||  0.9501    ||   1.804     ||  1.213    ||   4.186     ||  3.647&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Flexibility ==&lt;br /&gt;
&lt;br /&gt;
[[File:Flexibility TJ-II.png|300px|thumb|right|Flexibility diagram of TJ-II magnetic configurations. Several lines of constant rotational transform are highlighted and labelled with the corresponding central &amp;lt;math&amp;gt;\iota/2\pi&amp;lt;/math&amp;gt;-value.]]&lt;br /&gt;
TJ-II has considerable configurational flexibility, as observed in the &#039;flexibility diagram&#039;&amp;lt;ref&amp;gt;E. Ascasíbar, T. Estrada, F. Castejón, A. López-Fraguas, I. Pastor, J. Sánchez, U. Stroth, J. Qin and TJ-II Team, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/45/4/009|Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276–284]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
Some of this flexibility space has been explored, as in the &#039;magnetic well scan&#039; experiments&amp;lt;ref&amp;gt;A. de Aguilera, F. Castejón, E. Ascasíbar, et al. &#039;&#039;Magnetic well scan and confinement in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/55/11/113014|Nucl. Fusion, 55(11):113014, 2015]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8723</id>
		<title>TJ-II:Magnetic configuration</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8723"/>
		<updated>2026-10-07T14:06:17Z</updated>

		<summary type="html">&lt;p&gt;Admin: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The magnetic configuration of [[TJ-II]] in vacuum is completely determined by the currents flowing through the [[TJ-II:Coil system|external coils]].&lt;br /&gt;
Magnetic configurations are labelled as &#039;xxx_yy_zz&#039;, where&lt;br /&gt;
* &#039;xxx&#039;: 10 times the current (in kA) in the circular coil&lt;br /&gt;
* &#039;yy&#039;: 10 times the current (in kA) in the helical coil&lt;br /&gt;
* &#039;zz&#039;: 10 times the current (in kA) in the vertical field coils&lt;br /&gt;
The current in the toroidal field coils is not specified, as its value is adjusted to guarantee central absorption of the [[TJ-II:Electron Cyclotron Resonant Heating|Electron Cyclotron Resonant Heating]] source (requiring a specific &#039;resonant&#039; value of the magnetic field on the magnetic axis, &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
Configuration list:&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;width: 100%&amp;quot; border=&amp;quot;1&amp;quot;||&lt;br /&gt;
|-&lt;br /&gt;
! Configuration &lt;br /&gt;
! &amp;lt;math&amp;gt;r_{av}&amp;lt;/math&amp;gt; (cm) &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(0)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(a)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{m,av}&amp;lt;/math&amp;gt;(T) &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt; (T) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(0)&amp;lt;/math&amp;gt; (m) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(45)&amp;lt;/math&amp;gt;(m) &lt;br /&gt;
! Shear (%) &lt;br /&gt;
! Well (%)&lt;br /&gt;
|-&lt;br /&gt;
|0_20_13    ||1.139      || 1.185      || 1.194     ||  1.033     || 0.9504     ||  1.644      || 1.374     || 0.7793      ||5.7521E-02&lt;br /&gt;
|-&lt;br /&gt;
|0_30_15    ||4.228      || 1.518      || 1.698     ||  1.019     || 0.9500     ||  1.658      || 1.360     ||  11.85      || 1.050&lt;br /&gt;
|-&lt;br /&gt;
|0_40_18    ||5.903      || 1.756      || 2.003     ||  1.008     || 0.9505     ||  1.671      || 1.347     ||  14.09      || 1.217&lt;br /&gt;
|-&lt;br /&gt;
|0_50_22    ||6.480      || 1.936      || 2.230     || 0.9973     || 0.9502     ||  1.682      || 1.336     ||  15.17      || 2.481&lt;br /&gt;
|-&lt;br /&gt;
|0_60_26    ||8.500      || 2.073      || 2.399     || 0.9885     || 0.9502     ||  1.692      || 1.326     ||  15.70      || 3.218&lt;br /&gt;
|-&lt;br /&gt;
|0_70_29    ||7.147      || 2.187      || 2.434     || 0.9805     || 0.9503     ||  1.701      || 1.317     ||  11.30      || 2.985&lt;br /&gt;
|-&lt;br /&gt;
|0_80_34    ||6.902      || 2.284      || 2.469     || 0.9736     || 0.9506     ||  1.710      || 1.308     ||  8.084      || 2.735&lt;br /&gt;
|-&lt;br /&gt;
|0_90_38    ||6.738      || 2.366      || 2.514     || 0.9663     || 0.9503     ||  1.719      || 1.299     ||  6.269      || 2.534&lt;br /&gt;
|-&lt;br /&gt;
|0_100_42   ||12.59      || 2.436      || 2.667     || 0.9601     || 0.9505     ||  1.727      || 1.291     ||  9.493      || 4.643&lt;br /&gt;
|-&lt;br /&gt;
|0_110_46   ||10.67      || 2.493      || 2.667     || 0.9539     || 0.9503     ||  1.734      || 1.284     ||  6.980      || 4.554&lt;br /&gt;
|-&lt;br /&gt;
|0_120_50   ||12.71      || 2.548      || 2.667     || 0.9482     || 0.9504     ||  1.742      || 1.276     ||  4.683      || 4.272&lt;br /&gt;
|-&lt;br /&gt;
|10_20_18   || 2.557     ||  1.148     ||  1.184    ||   1.024    ||  0.9514    ||   1.652     ||  1.366    ||   3.183     || 0.2469&lt;br /&gt;
|-&lt;br /&gt;
|10_30_20   || 6.083     ||  1.438     ||  1.602    ||   1.010    ||  0.9501    ||   1.666     ||  1.352    ||   11.35     ||  1.398&lt;br /&gt;
|-&lt;br /&gt;
|10_40_24   || 6.921     ||  1.659     ||  1.880    ||   1.000    ||  0.9504    ||   1.678     ||  1.340    ||   13.34     ||  2.751&lt;br /&gt;
|-&lt;br /&gt;
|10_50_27   || 8.140     ||  1.826     ||  1.997    ||  0.9909    ||  0.9504    ||   1.688     ||  1.329    ||   9.321     ||  3.241&lt;br /&gt;
|-&lt;br /&gt;
|10_60_31   || 9.350     ||  1.965     ||  2.183    ||  0.9826    ||  0.9505    ||   1.698     ||  1.319    ||   11.11     ||  3.084&lt;br /&gt;
|-&lt;br /&gt;
|10_70_35   || 10.10     ||  2.077     ||  2.288    ||  0.9750    ||  0.9505    ||   1.707     ||  1.310    ||   10.16     ||  3.597&lt;br /&gt;
|-&lt;br /&gt;
|10_80_38   || 9.810     ||  2.174     ||  2.371    ||  0.9674    ||  0.9502    ||   1.716     ||  1.302    ||   9.037     ||  3.908&lt;br /&gt;
|-&lt;br /&gt;
|10_90_42   || 10.54     ||  2.257     ||  2.434    ||  0.9610    ||  0.9503    ||   1.724     ||  1.294    ||   7.851     ||  4.281&lt;br /&gt;
|-&lt;br /&gt;
|10_100_47  || 10.21     ||  2.327     ||  2.482    ||  0.9546    ||  0.9502    ||   1.732     ||  1.286    ||   6.647     ||  4.236&lt;br /&gt;
|-&lt;br /&gt;
|10_110_51  || 11.11     ||  2.395     ||  2.547    ||  0.9488    ||  0.9501    ||   1.740     ||  1.278    ||   6.331     ||  5.121&lt;br /&gt;
|-&lt;br /&gt;
|10_120_55  || 10.04     ||  2.451     ||  2.565    ||  0.9432    ||  0.9502    ||   1.747     ||  1.271    ||   4.674     ||  4.426&lt;br /&gt;
|-&lt;br /&gt;
|20_10_21   || 1.213     || 0.7902     || 0.7956    ||   1.028    ||  0.9503    ||   1.645     ||  1.373    ||  0.6830     || 3.7624E-02&lt;br /&gt;
|-&lt;br /&gt;
|20_20_22   || 3.952     ||  1.136     ||  1.185    ||   1.014    ||  0.9500    ||   1.661     ||  1.357    ||   4.350     || 0.4717&lt;br /&gt;
|-&lt;br /&gt;
|20_30_25   || 6.779     ||  1.395     ||  1.521    ||   1.003    ||  0.9502    ||   1.673     ||  1.344    ||   9.049     ||  1.550&lt;br /&gt;
|-&lt;br /&gt;
|20_40_28   || 8.475     ||  1.592     ||  1.771    ||  0.9922    ||  0.9498    ||   1.685     ||  1.333    ||   11.25     ||  2.879&lt;br /&gt;
|-&lt;br /&gt;
|20_50_32   || 8.039     ||  1.756     ||  1.906    ||  0.9842    ||  0.9505    ||   1.695     ||  1.323    ||   8.571     ||  3.131&lt;br /&gt;
|-&lt;br /&gt;
|20_60_35   || 11.21     ||  1.884     ||  1.997    ||  0.9755    ||  0.9498    ||   1.705     ||  1.313    ||   5.968     ||  1.980&lt;br /&gt;
|-&lt;br /&gt;
|20_70_39   || 11.08     ||  1.994     ||  2.154    ||  0.9689    ||  0.9504    ||   1.714     ||  1.304    ||   7.982     ||  3.385&lt;br /&gt;
|-&lt;br /&gt;
|20_80_43   || 12.14     ||  2.092     ||  2.255    ||  0.9614    ||  0.9497    ||   1.722     ||  1.296    ||   7.811     ||  4.133&lt;br /&gt;
|-&lt;br /&gt;
|20_90_47   || 12.83     ||  2.174     ||  2.324    ||  0.9558    ||  0.9503    ||   1.730     ||  1.288    ||   6.862     ||  4.713&lt;br /&gt;
|-&lt;br /&gt;
|20_100_51  || 12.68     ||  2.246     ||  2.379    ||  0.9498    ||  0.9503    ||   1.738     ||  1.280    ||   5.945     ||  4.930&lt;br /&gt;
|-&lt;br /&gt;
|20_110_55  || 13.79     ||  2.313     ||  2.434    ||  0.9443    ||  0.9505    ||   1.745     ||  1.273    ||   5.248     ||  5.117&lt;br /&gt;
|-&lt;br /&gt;
|20_120_59  || 13.91     ||  2.368     ||  2.483    ||  0.9386    ||  0.9502    ||   1.752     ||  1.265    ||   4.822     ||  5.418&lt;br /&gt;
|-&lt;br /&gt;
|30_10_25   || 2.709     || 0.8385     || 0.8507    ||   1.018    ||  0.9501    ||   1.654     ||  1.363    ||   1.452     || 0.1431&lt;br /&gt;
|-&lt;br /&gt;
|30_20_27   || 5.443     ||  1.134     ||  1.189    ||   1.007    ||  0.9514    ||   1.669     ||  1.349    ||   4.847     || 0.7001&lt;br /&gt;
|-&lt;br /&gt;
|30_30_30   || 8.180     ||  1.368     ||  1.481    ||  0.9956    ||  0.9506    ||   1.681     ||  1.337    ||   8.332     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|30_40_33   || 9.756     ||  1.550     ||  1.687    ||  0.9860    ||  0.9503    ||   1.692     ||  1.326    ||   8.877     ||  2.798&lt;br /&gt;
|-&lt;br /&gt;
|30_50_37   || 11.16     ||  1.702     ||  1.878    ||  0.9779    ||  0.9503    ||   1.702     ||  1.316    ||   10.37     ||  4.941&lt;br /&gt;
|-&lt;br /&gt;
|30_60_40   || 9.262     ||  1.827     ||  1.936    ||  0.9706    ||  0.9505    ||   1.711     ||  1.307    ||   5.952     ||  3.624&lt;br /&gt;
|-&lt;br /&gt;
|30_70_44   || 12.28     ||  1.937     ||  2.007    ||  0.9631    ||  0.9502    ||   1.720     ||  1.298    ||   3.593     ||  4.431&lt;br /&gt;
|-&lt;br /&gt;
|30_80_48   || 13.28     ||  2.033     ||  2.149    ||  0.9567    ||  0.9502    ||   1.728     ||  1.290    ||   5.702     ||  3.674&lt;br /&gt;
|-&lt;br /&gt;
|30_90_52   || 14.16     ||  2.115     ||  2.231    ||  0.9504    ||  0.9501    ||   1.736     ||  1.282    ||   5.476     ||  4.227&lt;br /&gt;
|-&lt;br /&gt;
|30_100_56  || 14.97     ||  2.187     ||  2.295    ||  0.9448    ||  0.9502    ||   1.743     ||  1.275    ||   4.949     ||  4.755&lt;br /&gt;
|-&lt;br /&gt;
|30_110_59  || 15.76     ||  2.246     ||  2.356    ||  0.9391    ||  0.9500    ||   1.751     ||  1.267    ||   4.920     ||  5.215&lt;br /&gt;
|-&lt;br /&gt;
|30_120_63  || 14.48     ||  2.306     ||  2.389    ||  0.9343    ||  0.9504    ||   1.758     ||  1.260    ||   3.573     ||  5.025&lt;br /&gt;
|-&lt;br /&gt;
|40_00_27   || 1.350     || 0.5464     || 0.5471    ||   1.024    ||  0.9504    ||   1.647     ||  1.371    ||  0.1331     || 2.4768E-02&lt;br /&gt;
|-&lt;br /&gt;
|40_10_29   || 4.111     || 0.8821     || 0.9010    ||   1.010    ||  0.9510    ||   1.663     ||  1.355    ||   2.152     || 0.2456&lt;br /&gt;
|-&lt;br /&gt;
|40_20_31   || 6.646     ||  1.146     ||  1.202    ||  0.9975    ||  0.9501    ||   1.677     ||  1.341    ||   4.928     || 0.8185&lt;br /&gt;
|-&lt;br /&gt;
|40_30_34   || 9.328     ||  1.354     ||  1.452    ||  0.9884    ||  0.9506    ||   1.688     ||  1.330    ||   7.247     ||  1.826&lt;br /&gt;
|-&lt;br /&gt;
|40_40_37   || 11.15     ||  1.523     ||  1.646    ||  0.9788    ||  0.9498    ||   1.699     ||  1.319    ||   8.061     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|40_50_41   || 12.66     ||  1.666     ||  1.797    ||  0.9719    ||  0.9506    ||   1.708     ||  1.310    ||   7.872     ||  4.310&lt;br /&gt;
|-&lt;br /&gt;
|40_60_44   || 12.34     ||  1.786     ||  1.927    ||  0.9637    ||  0.9497    ||   1.717     ||  1.301    ||   7.879     ||  5.834&lt;br /&gt;
|-&lt;br /&gt;
|40_70_48   || 9.734     ||  1.894     ||  1.963    ||  0.9579    ||  0.9504    ||   1.726     ||  1.292    ||   3.625     ||  3.668&lt;br /&gt;
|-&lt;br /&gt;
|40_80_52   || 13.96     ||  1.986     ||  2.067    ||  0.9515    ||  0.9503    ||   1.734     ||  1.284    ||   4.054     ||  3.028&lt;br /&gt;
|-&lt;br /&gt;
|40_90_56   || 15.39     ||  2.062     ||  2.156    ||  0.9457    ||  0.9504    ||   1.741     ||  1.277    ||   4.529     ||  3.841&lt;br /&gt;
|-&lt;br /&gt;
|40_100_60  || 16.40     ||  2.132     ||  2.232    ||  0.9400    ||  0.9502    ||   1.749     ||  1.269    ||   4.683     ||  4.355&lt;br /&gt;
|-&lt;br /&gt;
|40_110_64  || 18.12     ||  2.199     ||  2.288    ||  0.9348    ||  0.9503    ||   1.756     ||  1.262    ||   4.049     ||  4.651&lt;br /&gt;
|-&lt;br /&gt;
|40_120_68  || 16.81     ||  2.256     ||  2.327    ||  0.9295    ||  0.9501    ||   1.763     ||  1.255    ||   3.158     ||  4.904&lt;br /&gt;
|-&lt;br /&gt;
|50_00_31   || 2.818     || 0.6329     || 0.6375    ||   1.013    ||  0.9498    ||   1.657     ||  1.361    ||  0.7286     || 6.1871E-02&lt;br /&gt;
|-&lt;br /&gt;
|50_10_33   || 5.588     || 0.9254     || 0.9532    ||   1.001    ||  0.9506    ||   1.672     ||  1.346    ||   3.003     || 0.3605&lt;br /&gt;
|-&lt;br /&gt;
|50_20_36   || 8.222     ||  1.160     ||  1.216    ||  0.9902    ||  0.9502    ||   1.684     ||  1.334    ||   4.838     ||  1.060&lt;br /&gt;
|-&lt;br /&gt;
|50_30_39   || 10.67     ||  1.352     ||  1.435    ||  0.9815    ||  0.9505    ||   1.695     ||  1.323    ||   6.163     ||  2.008&lt;br /&gt;
|-&lt;br /&gt;
|50_40_42   || 12.44     ||  1.508     ||  1.609    ||  0.9733    ||  0.9504    ||   1.705     ||  1.313    ||   6.719     ||  2.910&lt;br /&gt;
|-&lt;br /&gt;
|50_50_46   || 13.94     ||  1.644     ||  1.758    ||  0.9661    ||  0.9505    ||   1.714     ||  1.303    ||   6.944     ||  4.001&lt;br /&gt;
|-&lt;br /&gt;
|50_60_49   || 15.09     ||  1.757     ||  1.887    ||  0.9587    ||  0.9502    ||   1.723     ||  1.295    ||   7.390     ||  6.217&lt;br /&gt;
|-&lt;br /&gt;
|50_70_53   || 13.03     ||  1.855     ||  1.955    ||  0.9524    ||  0.9502    ||   1.731     ||  1.287    ||   5.353     ||  5.830&lt;br /&gt;
|-&lt;br /&gt;
|50_80_56   || 16.73     ||  1.949     ||  2.004    ||  0.9463    ||  0.9501    ||   1.739     ||  1.279    ||   2.807     ||  4.003&lt;br /&gt;
|-&lt;br /&gt;
|50_90_60   || 16.70     ||  2.011     ||  2.101    ||  0.9407    ||  0.9502    ||   1.747     ||  1.271    ||   4.501     ||  3.444&lt;br /&gt;
|-&lt;br /&gt;
|50_100_64  || 18.15     ||  2.090     ||  2.183    ||  0.9351    ||  0.9500    ||   1.754     ||  1.264    ||   4.434     ||  3.907&lt;br /&gt;
|-&lt;br /&gt;
|50_110_68  || 17.53     ||  2.154     ||  2.223    ||  0.9297    ||  0.9498    ||   1.762     ||  1.256    ||   3.205     ||  4.270&lt;br /&gt;
|-&lt;br /&gt;
|50_120_72  || 19.13     ||  2.213     ||  2.288    ||  0.9250    ||  0.9501    ||   1.768     ||  1.250    ||   3.417     ||  4.378&lt;br /&gt;
|-&lt;br /&gt;
|60_00_35   || 4.247     || 0.7126     || 0.7205    ||   1.003    ||  0.9498    ||   1.667     ||  1.352    ||   1.108     || 0.1270&lt;br /&gt;
|-&lt;br /&gt;
|60_10_37   || 6.862     || 0.9679     ||  1.002    ||  0.9934    ||  0.9509    ||   1.680     ||  1.338    ||   3.520     || 0.4827&lt;br /&gt;
|-&lt;br /&gt;
|60_20_40   || 9.669     ||  1.179     ||  1.240    ||  0.9831    ||  0.9503    ||   1.692     ||  1.326    ||   5.202     ||  1.236&lt;br /&gt;
|-&lt;br /&gt;
|60_30_43   || 12.01     ||  1.354     ||  1.435    ||  0.9747    ||  0.9502    ||   1.702     ||  1.316    ||   5.973     ||  2.132&lt;br /&gt;
|-&lt;br /&gt;
|60_40_46   || 13.48     ||  1.500     ||  1.593    ||  0.9672    ||  0.9503    ||   1.712     ||  1.306    ||   6.170     ||  2.806&lt;br /&gt;
|-&lt;br /&gt;
|60_50_50   || 15.36     ||  1.627     ||  1.732    ||  0.9601    ||  0.9504    ||   1.721     ||  1.297    ||   6.467     ||  3.895&lt;br /&gt;
|-&lt;br /&gt;
|60_60_53   || 16.79     ||  1.734     ||  1.851    ||  0.9528    ||  0.9499    ||   1.729     ||  1.289    ||   6.731     ||  5.666&lt;br /&gt;
|-&lt;br /&gt;
|60_70_57   || 15.88     ||  1.829     ||  1.934    ||  0.9473    ||  0.9502    ||   1.737     ||  1.281    ||   5.736     ||  6.958&lt;br /&gt;
|-&lt;br /&gt;
|60_80_61   || 13.66     ||  1.918     ||  1.968    ||  0.9428    ||  0.9514    ||   1.745     ||  1.273    ||   2.622     ||  4.555&lt;br /&gt;
|-&lt;br /&gt;
|60_90_64   || 17.29     ||  2.009     ||  2.063    ||  0.9359    ||  0.9501    ||   1.753     ||  1.265    ||   2.640     ||  1.637&lt;br /&gt;
|-&lt;br /&gt;
|60_100_68  || 17.62     ||  2.049     ||  2.122    ||  0.9304    ||  0.9497    ||   1.760     ||  1.258    ||   3.560     ||  3.718&lt;br /&gt;
|-&lt;br /&gt;
|60_110_72  || 17.50     ||  2.118     ||  2.177    ||  0.9257    ||  0.9501    ||   1.767     ||  1.251    ||   2.811     ||  4.023&lt;br /&gt;
|-&lt;br /&gt;
|60_120_76  || 17.78     ||  2.174     ||  2.222    ||  0.9217    ||  0.9510    ||   1.774     ||  1.244    ||   2.209     ||  4.211&lt;br /&gt;
|-&lt;br /&gt;
|70_00_39   || 5.731     || 0.7825     || 0.7975    ||  0.9949    ||  0.9497    ||   1.675     ||  1.343    ||   1.908     || 0.2335&lt;br /&gt;
|-&lt;br /&gt;
|70_10_41   || 8.418     ||  1.009     ||  1.048    ||  0.9860    ||  0.9509    ||   1.688     ||  1.330    ||   3.845     || 0.6755&lt;br /&gt;
|-&lt;br /&gt;
|70_20_44   || 11.09     ||  1.201     ||  1.265    ||  0.9767    ||  0.9504    ||   1.699     ||  1.319    ||   5.345     ||  1.317&lt;br /&gt;
|-&lt;br /&gt;
|70_30_47   || 13.41     ||  1.361     ||  1.441    ||  0.9688    ||  0.9504    ||   1.709     ||  1.309    ||   5.859     ||  2.187&lt;br /&gt;
|-&lt;br /&gt;
|70_40_51   || 14.99     ||  1.496     ||  1.591    ||  0.9615    ||  0.9503    ||   1.718     ||  1.300    ||   6.348     ||  2.859&lt;br /&gt;
|-&lt;br /&gt;
|70_50_54   || 16.87     ||  1.617     ||  1.712    ||  0.9543    ||  0.9501    ||   1.727     ||  1.291    ||   5.843     ||  3.756&lt;br /&gt;
|-&lt;br /&gt;
|70_60_57   || 17.89     ||  1.718     ||  1.823    ||  0.9479    ||  0.9500    ||   1.735     ||  1.283    ||   6.140     ||  4.746&lt;br /&gt;
|-&lt;br /&gt;
|70_70_61   || 18.26     ||  1.812     ||  1.928    ||  0.9423    ||  0.9503    ||   1.743     ||  1.275    ||   6.353     ||  6.812&lt;br /&gt;
|-&lt;br /&gt;
|70_80_65   || 16.37     ||  1.896     ||  1.962    ||  0.9363    ||  0.9499    ||   1.751     ||  1.267    ||   3.469     ||  5.948&lt;br /&gt;
|-&lt;br /&gt;
|70_90_68   || 9.135     ||  1.980     ||  1.988    ||  0.9317    ||  0.9506    ||   1.758     ||  1.260    ||  0.3692     || 0.1186&lt;br /&gt;
|-&lt;br /&gt;
|70_100_72  || 18.64     ||  2.007     ||  2.094    ||  0.9267    ||  0.9506    ||   1.765     ||  1.253    ||   4.327     ||  3.356&lt;br /&gt;
|-&lt;br /&gt;
|70_110_76  || 18.23     ||  2.088     ||  2.147    ||  0.9219    ||  0.9507    ||   1.772     ||  1.246    ||   2.792     ||  3.707&lt;br /&gt;
|-&lt;br /&gt;
|70_120_80  || 17.89     ||  2.145     ||  2.184    ||  0.9171    ||  0.9506    ||   1.779     ||  1.239    ||   1.846     ||  4.043&lt;br /&gt;
|-&lt;br /&gt;
|80_00_42   ||7.247      ||0.8436      ||0.8697     || 0.9869     || 0.9497     ||  1.684      || 1.335     ||  3.094      ||0.2402&lt;br /&gt;
|-&lt;br /&gt;
|80_10_45   ||9.865      || 1.049      || 1.095     || 0.9794     || 0.9513     ||  1.695      || 1.323     ||  4.371      ||0.7359&lt;br /&gt;
|-&lt;br /&gt;
|80_20_48   ||12.28      || 1.226      || 1.290     || 0.9697     || 0.9500     ||  1.706      || 1.312     ||  5.206      || 1.327&lt;br /&gt;
|-&lt;br /&gt;
|80_30_51   ||14.38      || 1.370      || 1.454     || 0.9626     || 0.9503     ||  1.715      || 1.303     ||  6.088      || 2.102&lt;br /&gt;
|-&lt;br /&gt;
|80_40_54   ||16.47      || 1.500      || 1.594     || 0.9549     || 0.9497     ||  1.724      || 1.294     ||  6.263      || 2.799&lt;br /&gt;
|-&lt;br /&gt;
|80_50_58   ||17.63      || 1.612      || 1.706     || 0.9492     || 0.9503     ||  1.733      || 1.285     ||  5.842      || 3.329&lt;br /&gt;
|-&lt;br /&gt;
|80_60_61   ||18.84      || 1.712      || 1.814     || 0.9436     || 0.9507     ||  1.741      || 1.277     ||  5.984      || 3.990&lt;br /&gt;
|-&lt;br /&gt;
|80_70_65   ||19.27      || 1.799      || 1.898     || 0.9372     || 0.9501     ||  1.749      || 1.269     ||  5.555      || 4.728&lt;br /&gt;
|-&lt;br /&gt;
|80_80_69   ||17.96      || 1.880      || 1.935     || 0.9321     || 0.9503     ||  1.756      || 1.262     ||  2.921      || 3.774&lt;br /&gt;
|-&lt;br /&gt;
|80_90_73   ||13.42      || 1.957      || 1.982     || 0.9266     || 0.9500     ||  1.764      || 1.254     ||  1.312      ||0.6938&lt;br /&gt;
|-&lt;br /&gt;
|80_100_76  || 18.53     ||  2.008     ||  2.065    ||  0.9220    ||  0.9504    ||   1.770     ||  1.247    ||   2.839     ||  1.773&lt;br /&gt;
|-&lt;br /&gt;
|80_110_80  || 18.41     ||  2.059     ||  2.117    ||  0.9176    ||  0.9507    ||   1.777     ||  1.241    ||   2.847     ||  3.632&lt;br /&gt;
|-&lt;br /&gt;
|80_120_84  || 18.26     ||  2.117     ||  2.157    ||  0.9122    ||  0.9496    ||   1.784     ||  1.234    ||   1.872     ||  3.986&lt;br /&gt;
|-&lt;br /&gt;
|90_00_46   || 8.679     || 0.9022     || 0.9354    ||  0.9802    ||  0.9501    ||   1.691     ||  1.327    ||   3.678     || 0.3981&lt;br /&gt;
|-&lt;br /&gt;
|90_10_49   || 11.45     ||  1.090     ||  1.146    ||  0.9717    ||  0.9502    ||   1.702     ||  1.315    ||   5.148     || 0.8099&lt;br /&gt;
|-&lt;br /&gt;
|90_20_52   || 12.44     ||  1.247     ||  1.323    ||  0.9640    ||  0.9503    ||   1.712     ||  1.305    ||   6.100     ||  1.079&lt;br /&gt;
|-&lt;br /&gt;
|90_30_55   || 16.14     ||  1.383     ||  1.475    ||  0.9571    ||  0.9504    ||   1.722     ||  1.296    ||   6.607     ||  2.158&lt;br /&gt;
|-&lt;br /&gt;
|90_40_58   || 17.45     ||  1.506     ||  1.597    ||  0.9499    ||  0.9501    ||   1.731     ||  1.287    ||   6.012     ||  2.629&lt;br /&gt;
|-&lt;br /&gt;
|90_50_62   || 18.70     ||  1.609     ||  1.706    ||  0.9438    ||  0.9501    ||   1.739     ||  1.279    ||   6.003     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|90_60_65   || 18.77     ||  1.703     ||  1.789    ||  0.9381    ||  0.9502    ||   1.747     ||  1.271    ||   5.045     ||  3.047&lt;br /&gt;
|-&lt;br /&gt;
|90_70_69   || 18.43     ||  1.787     ||  1.852    ||  0.9324    ||  0.9500    ||   1.754     ||  1.263    ||   3.623     ||  3.117&lt;br /&gt;
|-&lt;br /&gt;
|90_80_73   || 17.72     ||  1.868     ||  1.909    ||  0.9269    ||  0.9497    ||   1.762     ||  1.256    ||   2.217     ||  2.354&lt;br /&gt;
|-&lt;br /&gt;
|90_90_76   || 14.40     ||  1.940     ||  1.956    ||  0.9221    ||  0.9499    ||   1.769     ||  1.249    ||  0.8079     || 0.8326&lt;br /&gt;
|-&lt;br /&gt;
|90_100_80  || 18.53     ||  2.009     ||  2.038    ||  0.9176    ||  0.9503    ||   1.776     ||  1.242    ||   1.484     ||  1.095&lt;br /&gt;
|-&lt;br /&gt;
|90_110_84  || 18.97     ||  2.021     ||  2.094    ||  0.9129    ||  0.9502    ||   1.783     ||  1.235    ||   3.625     ||  3.669&lt;br /&gt;
|-&lt;br /&gt;
|90_120_88  || 17.79     ||  2.090     ||  2.129    ||  0.9077    ||  0.9494    ||   1.789     ||  1.229    ||   1.827     ||  3.862&lt;br /&gt;
|-&lt;br /&gt;
|100_00_50  || 10.07     || 0.9544     || 0.9970    ||  0.9732    ||  0.9499    ||   1.699     ||  1.319    ||   4.471     || 0.4341&lt;br /&gt;
|-&lt;br /&gt;
|100_10_53  || 12.78     ||  1.127     ||  1.186    ||  0.9649    ||  0.9499    ||   1.710     ||  1.308    ||   5.262     || 0.9629&lt;br /&gt;
|-&lt;br /&gt;
|100_16_55  || 13.69     ||  1.215     ||  1.287    ||  0.9610    ||  0.9501    ||   1.715     ||  1.302    ||   5.901     ||  1.023&lt;br /&gt;
|-&lt;br /&gt;
|100_20_56  || 10.86     ||  1.271     ||  1.324    ||  0.9583    ||  0.9502    ||   1.719     ||  1.299    ||   4.120     || 0.8295&lt;br /&gt;
|-&lt;br /&gt;
|100_22_56  || 15.40     ||  1.309     ||  1.381    ||  0.9412    ||  0.9362    ||   1.722     ||  1.296    ||   5.552     ||  1.648&lt;br /&gt;
|-&lt;br /&gt;
|100_24_58  || 15.90     ||  1.326     ||  1.406    ||  0.9552    ||  0.9499    ||   1.722     ||  1.295    ||   6.105     ||  1.792&lt;br /&gt;
|-&lt;br /&gt;
|100_26_58  || 16.42     ||  1.352     ||  1.435    ||  0.9538    ||  0.9499    ||   1.724     ||  1.293    ||   6.137     ||  1.888&lt;br /&gt;
|-&lt;br /&gt;
|100_28_59  || 17.07     ||  1.375     ||  1.464    ||  0.9527    ||  0.9501    ||   1.726     ||  1.291    ||   6.475     ||  1.983&lt;br /&gt;
|-&lt;br /&gt;
|100_30_59  || 17.29     ||  1.398     ||  1.490    ||  0.9511    ||  0.9500    ||   1.728     ||  1.289    ||   6.561     ||  2.075&lt;br /&gt;
|-&lt;br /&gt;
|100_32_60  || 17.74     ||  1.423     ||  1.517    ||  0.9499    ||  0.9499    ||   1.730     ||  1.288    ||   6.596     ||  2.165&lt;br /&gt;
|-&lt;br /&gt;
|100_36_61  || 18.37     ||  1.467     ||  1.567    ||  0.9475    ||  0.9501    ||   1.733     ||  1.284    ||   6.819     ||  2.183&lt;br /&gt;
|-&lt;br /&gt;
|100_40_63  || 18.77     ||  1.509     ||  1.608    ||  0.9450    ||  0.9500    ||   1.736     ||  1.281    ||   6.553     ||  2.304&lt;br /&gt;
|-&lt;br /&gt;
|100_44_64  || 19.25     ||  1.551     ||  1.653    ||  0.9426    ||  0.9500    ||   1.740     ||  1.278    ||   6.569     ||  2.360&lt;br /&gt;
|-&lt;br /&gt;
|100_48_65  || 19.16     ||  1.591     ||  1.684    ||  0.9400    ||  0.9500    ||   1.743     ||  1.275    ||   5.807     ||  2.555&lt;br /&gt;
|-&lt;br /&gt;
|100_50_65  || 19.11     ||  1.613     ||  1.704    ||  0.9381    ||  0.9501    ||   1.745     ||  1.274    ||   5.628     ||  2.649&lt;br /&gt;
|-&lt;br /&gt;
|100_55_67  || 19.04     ||  1.659     ||  1.739    ||  0.9352    ||  0.9500    ||   1.749     ||  1.270    ||   4.839     ||  2.808&lt;br /&gt;
|-&lt;br /&gt;
|100_56_67  || 18.93     ||  1.667     ||  1.742    ||  0.9347    ||  0.9501    ||   1.750     ||  1.269    ||   4.522     ||  2.692&lt;br /&gt;
|-&lt;br /&gt;
|100_60_68  || 19.04     ||  1.702     ||  1.775    ||  0.9325    ||  0.9500    ||   1.753     ||  1.266    ||   4.326     ||  2.720&lt;br /&gt;
|-&lt;br /&gt;
|100_64_70  || 18.76     ||  1.733     ||  1.799    ||  0.9303    ||  0.9500    ||   1.756     ||  1.263    ||   3.774     ||  2.676&lt;br /&gt;
|-&lt;br /&gt;
|100_68_72  || 18.46     ||  1.771     ||  1.825    ||  0.9279    ||  0.9494    ||   1.759     ||  1.259    ||   3.080     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_70_73  || 18.23     ||  1.784     ||  1.841    ||  0.9277    ||  0.9500    ||   1.760     ||  1.258    ||   3.166     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_80_77  || 16.73     ||  1.855     ||  1.885    ||  0.9261    ||  0.9532    ||   1.767     ||  1.251    ||   1.617     ||  1.818&lt;br /&gt;
|-&lt;br /&gt;
|100_90_80  || 13.86     ||  1.931     ||  1.936    ||  0.9172    ||  0.9494    ||   1.774     ||  1.244    ||  0.2833     || 0.7382&lt;br /&gt;
|-&lt;br /&gt;
|100_95_82  || 11.27     ||  1.967     ||  1.964    ||  0.9243    ||  0.9582    ||   1.777     ||  1.241    || -0.1435     || 6.8954E-02&lt;br /&gt;
|-&lt;br /&gt;
|100_105_86 || 16.96     ||  2.019     ||  2.045    ||  0.9233    ||  0.9617    ||   1.783     ||  1.235    ||   1.268     ||  1.425&lt;br /&gt;
|-&lt;br /&gt;
|100_110_88 || 18.88     ||  2.020     ||  2.073    ||  0.9229    ||  0.9634    ||   1.786     ||  1.232    ||   2.618     ||  2.366&lt;br /&gt;
|-&lt;br /&gt;
|100_120_92 || 17.63     ||  2.064     ||  2.113    ||  0.9044    ||  0.9501    ||   1.794     ||  1.224    ||   2.379     ||  3.790&lt;br /&gt;
|-&lt;br /&gt;
|110_00_54  || 11.70     ||  1.006     ||  1.060    ||  0.9663    ||  0.9498    ||   1.706     ||  1.312    ||   5.370     || 0.4642&lt;br /&gt;
|-&lt;br /&gt;
|110_10_57  || 13.97     ||  1.160     ||  1.232    ||  0.9593    ||  0.9502    ||   1.716     ||  1.301    ||   6.136     || 0.8247&lt;br /&gt;
|-&lt;br /&gt;
|110_20_60  || 15.75     ||  1.298     ||  1.372    ||  0.9526    ||  0.9504    ||   1.726     ||  1.292    ||   5.739     ||  1.330&lt;br /&gt;
|-&lt;br /&gt;
|110_30_63  || 18.56     ||  1.415     ||  1.516    ||  0.9455    ||  0.9500    ||   1.734     ||  1.284    ||   7.122     ||  1.849&lt;br /&gt;
|-&lt;br /&gt;
|110_40_66  || 19.50     ||  1.521     ||  1.622    ||  0.9398    ||  0.9503    ||   1.743     ||  1.275    ||   6.602     ||  1.921&lt;br /&gt;
|-&lt;br /&gt;
|110_50_70  || 19.07     ||  1.618     ||  1.696    ||  0.9336    ||  0.9498    ||   1.751     ||  1.267    ||   4.873     ||  2.085&lt;br /&gt;
|-&lt;br /&gt;
|110_60_73  || 18.32     ||  1.702     ||  1.761    ||  0.9291    ||  0.9507    ||   1.758     ||  1.260    ||   3.471     ||  2.033&lt;br /&gt;
|-&lt;br /&gt;
|110_70_77  || 17.13     ||  1.782     ||  1.816    ||  0.9237    ||  0.9504    ||   1.766     ||  1.252    ||   1.948     ||  1.838&lt;br /&gt;
|-&lt;br /&gt;
|110_80_81  || 15.56     ||  1.853     ||  1.871    ||  0.9192    ||  0.9508    ||   1.773     ||  1.245    ||  0.9878     ||  1.332&lt;br /&gt;
|-&lt;br /&gt;
|110_90_84  || 13.12     ||  1.923     ||  1.926    ||  0.9142    ||  0.9506    ||   1.780     ||  1.238    ||  0.1639     || 0.5301&lt;br /&gt;
|-&lt;br /&gt;
|110_95_86  || 10.73     ||  1.963     ||  1.955    ||  0.9095    ||  0.9486    ||   1.783     ||  1.235    || -0.3746     || 8.1449E-04&lt;br /&gt;
|-&lt;br /&gt;
|110_110_92 || 17.29     ||  2.020     ||  2.055    ||  0.9056    ||  0.9509    ||   1.793     ||  1.225    ||   1.768     ||  2.045&lt;br /&gt;
|-&lt;br /&gt;
|110_120_95 || 17.55     ||  2.048     ||  2.095    ||  0.9014    ||  0.9510    ||   1.799     ||  1.219    ||   2.314     ||  3.774&lt;br /&gt;
|-&lt;br /&gt;
|120_00_57  || 13.14     ||  1.050     ||  1.117    ||  0.9599    ||  0.9497    ||   1.714     ||  1.305    ||   6.304     || 0.4861&lt;br /&gt;
|-&lt;br /&gt;
|120_10_60  || 14.81     ||  1.196     ||  1.268    ||  0.9534    ||  0.9501    ||   1.723     ||  1.295    ||   6.054     || 0.8382&lt;br /&gt;
|-&lt;br /&gt;
|120_20_63  || 17.57     ||  1.323     ||  1.409    ||  0.9458    ||  0.9494    ||   1.732     ||  1.286    ||   6.504     ||  1.409&lt;br /&gt;
|-&lt;br /&gt;
|120_30_67  || 19.50     ||  1.435     ||  1.539    ||  0.9407    ||  0.9503    ||   1.741     ||  1.277    ||   7.263     ||  1.529&lt;br /&gt;
|-&lt;br /&gt;
|120_40_70  || 19.38     ||  1.534     ||  1.621    ||  0.9335    ||  0.9492    ||   1.749     ||  1.269    ||   5.695     ||  1.632&lt;br /&gt;
|-&lt;br /&gt;
|120_50_74  || 18.34     ||  1.621     ||  1.684    ||  0.9294    ||  0.9503    ||   1.756     ||  1.262    ||   3.910     ||  1.864&lt;br /&gt;
|-&lt;br /&gt;
|120_60_77  || 17.24     ||  1.703     ||  1.743    ||  0.9246    ||  0.9507    ||   1.764     ||  1.254    ||   2.381     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|120_70_81  || 16.02     ||  1.780     ||  1.803    ||  0.9197    ||  0.9509    ||   1.771     ||  1.247    ||   1.312     ||  1.511&lt;br /&gt;
|-&lt;br /&gt;
|120_80_84  || 14.49     ||  1.850     ||  1.860    ||  0.9150    ||  0.9509    ||   1.778     ||  1.240    ||  0.5347     ||  1.076&lt;br /&gt;
|-&lt;br /&gt;
|120_90_88  || 12.18     ||  1.918     ||  1.918    ||  0.9096    ||  0.9501    ||   1.785     ||  1.233    || -4.1127E-02 || 0.3613&lt;br /&gt;
|-&lt;br /&gt;
|120_95_90  || 10.06     ||  1.957     ||  1.950    ||  0.9071    ||  0.9499    ||   1.788     ||  1.230    || -0.3241     ||  0.000&lt;br /&gt;
|-&lt;br /&gt;
|120_115_97 || 16.46     ||  2.020     ||  2.066    ||  0.8983    ||  0.9497    ||   1.801     ||  1.216    ||   2.258     ||  2.404&lt;br /&gt;
|-&lt;br /&gt;
|120_120_99 || 17.58     ||  2.008     ||  2.092    ||  0.8967    ||  0.9501    ||   1.804     ||  1.213    ||   4.186     ||  3.647&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Flexibility ==&lt;br /&gt;
&lt;br /&gt;
[[File:Flexibility TJ-II.png|300px|thumb|right|Flexibility diagram of TJ-II magnetic configurations. Several lines of constant rotational transform are highlighted and labelled with the corresponding central &amp;lt;math&amp;gt;\iota/2\pi&amp;lt;/math&amp;gt;-value.]]&lt;br /&gt;
TJ-II has considerable configurational flexibility, as observed in the &#039;flexibility diagram&#039;&amp;lt;ref&amp;gt;E. Ascasíbar, T. Estrada, F. Castejón, A. López-Fraguas, I. Pastor, J. Sánchez, U. Stroth, J. Qin and TJ-II Team, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/45/4/009|Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276–284]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8722</id>
		<title>TJ-II:Magnetic configuration</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8722"/>
		<updated>2026-10-07T13:19:23Z</updated>

		<summary type="html">&lt;p&gt;Admin: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The magnetic configuration of [[TJ-II]] in vacuum is completely determined by the currents flowing through the [[TJ-II:Coil system|external coils]].&lt;br /&gt;
Magnetic configurations are labelled as &#039;xxx_yy_zz&#039;, where&lt;br /&gt;
* &#039;xxx&#039;: 10 times the current (in kA) in the circular coil&lt;br /&gt;
* &#039;yy&#039;: 10 times the current (in kA) in the helical coil&lt;br /&gt;
* &#039;zz&#039;: 10 times the current (in kA) in the vertical field coils&lt;br /&gt;
The current in the toroidal field coils is not specified, as its value is adjusted to guarantee central absorption of the [[TJ-II:Electron Cyclotron Resonant Heating|Electron Cyclotron Resonant Heating]] source (requiring a specific value of the magnetic field on the magnetic axis).&lt;br /&gt;
&lt;br /&gt;
Configuration list:&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;width: 100%&amp;quot; border=&amp;quot;1&amp;quot;||&lt;br /&gt;
|-&lt;br /&gt;
! Configuration &lt;br /&gt;
! &amp;lt;math&amp;gt;r_{av}&amp;lt;/math&amp;gt; (cm) &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(0)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;\iota(a)/2\pi&amp;lt;/math&amp;gt; &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{m,av}&amp;lt;/math&amp;gt;(T) &lt;br /&gt;
! &amp;lt;math&amp;gt;B_{reson}&amp;lt;/math&amp;gt; (T) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(0)&amp;lt;/math&amp;gt; (m) &lt;br /&gt;
! &amp;lt;math&amp;gt;R_{ax}(45)&amp;lt;/math&amp;gt;(m) &lt;br /&gt;
! Shear (%) &lt;br /&gt;
! Well (%)&lt;br /&gt;
|-&lt;br /&gt;
|0_20_13    ||1.139      || 1.185      || 1.194     ||  1.033     || 0.9504     ||  1.644      || 1.374     || 0.7793      ||5.7521E-02&lt;br /&gt;
|-&lt;br /&gt;
|0_30_15    ||4.228      || 1.518      || 1.698     ||  1.019     || 0.9500     ||  1.658      || 1.360     ||  11.85      || 1.050&lt;br /&gt;
|-&lt;br /&gt;
|0_40_18    ||5.903      || 1.756      || 2.003     ||  1.008     || 0.9505     ||  1.671      || 1.347     ||  14.09      || 1.217&lt;br /&gt;
|-&lt;br /&gt;
|0_50_22    ||6.480      || 1.936      || 2.230     || 0.9973     || 0.9502     ||  1.682      || 1.336     ||  15.17      || 2.481&lt;br /&gt;
|-&lt;br /&gt;
|0_60_26    ||8.500      || 2.073      || 2.399     || 0.9885     || 0.9502     ||  1.692      || 1.326     ||  15.70      || 3.218&lt;br /&gt;
|-&lt;br /&gt;
|0_70_29    ||7.147      || 2.187      || 2.434     || 0.9805     || 0.9503     ||  1.701      || 1.317     ||  11.30      || 2.985&lt;br /&gt;
|-&lt;br /&gt;
|0_80_34    ||6.902      || 2.284      || 2.469     || 0.9736     || 0.9506     ||  1.710      || 1.308     ||  8.084      || 2.735&lt;br /&gt;
|-&lt;br /&gt;
|0_90_38    ||6.738      || 2.366      || 2.514     || 0.9663     || 0.9503     ||  1.719      || 1.299     ||  6.269      || 2.534&lt;br /&gt;
|-&lt;br /&gt;
|0_100_42   ||12.59      || 2.436      || 2.667     || 0.9601     || 0.9505     ||  1.727      || 1.291     ||  9.493      || 4.643&lt;br /&gt;
|-&lt;br /&gt;
|0_110_46   ||10.67      || 2.493      || 2.667     || 0.9539     || 0.9503     ||  1.734      || 1.284     ||  6.980      || 4.554&lt;br /&gt;
|-&lt;br /&gt;
|0_120_50   ||12.71      || 2.548      || 2.667     || 0.9482     || 0.9504     ||  1.742      || 1.276     ||  4.683      || 4.272&lt;br /&gt;
|-&lt;br /&gt;
|10_20_18   || 2.557     ||  1.148     ||  1.184    ||   1.024    ||  0.9514    ||   1.652     ||  1.366    ||   3.183     || 0.2469&lt;br /&gt;
|-&lt;br /&gt;
|10_30_20   || 6.083     ||  1.438     ||  1.602    ||   1.010    ||  0.9501    ||   1.666     ||  1.352    ||   11.35     ||  1.398&lt;br /&gt;
|-&lt;br /&gt;
|10_40_24   || 6.921     ||  1.659     ||  1.880    ||   1.000    ||  0.9504    ||   1.678     ||  1.340    ||   13.34     ||  2.751&lt;br /&gt;
|-&lt;br /&gt;
|10_50_27   || 8.140     ||  1.826     ||  1.997    ||  0.9909    ||  0.9504    ||   1.688     ||  1.329    ||   9.321     ||  3.241&lt;br /&gt;
|-&lt;br /&gt;
|10_60_31   || 9.350     ||  1.965     ||  2.183    ||  0.9826    ||  0.9505    ||   1.698     ||  1.319    ||   11.11     ||  3.084&lt;br /&gt;
|-&lt;br /&gt;
|10_70_35   || 10.10     ||  2.077     ||  2.288    ||  0.9750    ||  0.9505    ||   1.707     ||  1.310    ||   10.16     ||  3.597&lt;br /&gt;
|-&lt;br /&gt;
|10_80_38   || 9.810     ||  2.174     ||  2.371    ||  0.9674    ||  0.9502    ||   1.716     ||  1.302    ||   9.037     ||  3.908&lt;br /&gt;
|-&lt;br /&gt;
|10_90_42   || 10.54     ||  2.257     ||  2.434    ||  0.9610    ||  0.9503    ||   1.724     ||  1.294    ||   7.851     ||  4.281&lt;br /&gt;
|-&lt;br /&gt;
|10_100_47  || 10.21     ||  2.327     ||  2.482    ||  0.9546    ||  0.9502    ||   1.732     ||  1.286    ||   6.647     ||  4.236&lt;br /&gt;
|-&lt;br /&gt;
|10_110_51  || 11.11     ||  2.395     ||  2.547    ||  0.9488    ||  0.9501    ||   1.740     ||  1.278    ||   6.331     ||  5.121&lt;br /&gt;
|-&lt;br /&gt;
|10_120_55  || 10.04     ||  2.451     ||  2.565    ||  0.9432    ||  0.9502    ||   1.747     ||  1.271    ||   4.674     ||  4.426&lt;br /&gt;
|-&lt;br /&gt;
|20_10_21   || 1.213     || 0.7902     || 0.7956    ||   1.028    ||  0.9503    ||   1.645     ||  1.373    ||  0.6830     || 3.7624E-02&lt;br /&gt;
|-&lt;br /&gt;
|20_20_22   || 3.952     ||  1.136     ||  1.185    ||   1.014    ||  0.9500    ||   1.661     ||  1.357    ||   4.350     || 0.4717&lt;br /&gt;
|-&lt;br /&gt;
|20_30_25   || 6.779     ||  1.395     ||  1.521    ||   1.003    ||  0.9502    ||   1.673     ||  1.344    ||   9.049     ||  1.550&lt;br /&gt;
|-&lt;br /&gt;
|20_40_28   || 8.475     ||  1.592     ||  1.771    ||  0.9922    ||  0.9498    ||   1.685     ||  1.333    ||   11.25     ||  2.879&lt;br /&gt;
|-&lt;br /&gt;
|20_50_32   || 8.039     ||  1.756     ||  1.906    ||  0.9842    ||  0.9505    ||   1.695     ||  1.323    ||   8.571     ||  3.131&lt;br /&gt;
|-&lt;br /&gt;
|20_60_35   || 11.21     ||  1.884     ||  1.997    ||  0.9755    ||  0.9498    ||   1.705     ||  1.313    ||   5.968     ||  1.980&lt;br /&gt;
|-&lt;br /&gt;
|20_70_39   || 11.08     ||  1.994     ||  2.154    ||  0.9689    ||  0.9504    ||   1.714     ||  1.304    ||   7.982     ||  3.385&lt;br /&gt;
|-&lt;br /&gt;
|20_80_43   || 12.14     ||  2.092     ||  2.255    ||  0.9614    ||  0.9497    ||   1.722     ||  1.296    ||   7.811     ||  4.133&lt;br /&gt;
|-&lt;br /&gt;
|20_90_47   || 12.83     ||  2.174     ||  2.324    ||  0.9558    ||  0.9503    ||   1.730     ||  1.288    ||   6.862     ||  4.713&lt;br /&gt;
|-&lt;br /&gt;
|20_100_51  || 12.68     ||  2.246     ||  2.379    ||  0.9498    ||  0.9503    ||   1.738     ||  1.280    ||   5.945     ||  4.930&lt;br /&gt;
|-&lt;br /&gt;
|20_110_55  || 13.79     ||  2.313     ||  2.434    ||  0.9443    ||  0.9505    ||   1.745     ||  1.273    ||   5.248     ||  5.117&lt;br /&gt;
|-&lt;br /&gt;
|20_120_59  || 13.91     ||  2.368     ||  2.483    ||  0.9386    ||  0.9502    ||   1.752     ||  1.265    ||   4.822     ||  5.418&lt;br /&gt;
|-&lt;br /&gt;
|30_10_25   || 2.709     || 0.8385     || 0.8507    ||   1.018    ||  0.9501    ||   1.654     ||  1.363    ||   1.452     || 0.1431&lt;br /&gt;
|-&lt;br /&gt;
|30_20_27   || 5.443     ||  1.134     ||  1.189    ||   1.007    ||  0.9514    ||   1.669     ||  1.349    ||   4.847     || 0.7001&lt;br /&gt;
|-&lt;br /&gt;
|30_30_30   || 8.180     ||  1.368     ||  1.481    ||  0.9956    ||  0.9506    ||   1.681     ||  1.337    ||   8.332     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|30_40_33   || 9.756     ||  1.550     ||  1.687    ||  0.9860    ||  0.9503    ||   1.692     ||  1.326    ||   8.877     ||  2.798&lt;br /&gt;
|-&lt;br /&gt;
|30_50_37   || 11.16     ||  1.702     ||  1.878    ||  0.9779    ||  0.9503    ||   1.702     ||  1.316    ||   10.37     ||  4.941&lt;br /&gt;
|-&lt;br /&gt;
|30_60_40   || 9.262     ||  1.827     ||  1.936    ||  0.9706    ||  0.9505    ||   1.711     ||  1.307    ||   5.952     ||  3.624&lt;br /&gt;
|-&lt;br /&gt;
|30_70_44   || 12.28     ||  1.937     ||  2.007    ||  0.9631    ||  0.9502    ||   1.720     ||  1.298    ||   3.593     ||  4.431&lt;br /&gt;
|-&lt;br /&gt;
|30_80_48   || 13.28     ||  2.033     ||  2.149    ||  0.9567    ||  0.9502    ||   1.728     ||  1.290    ||   5.702     ||  3.674&lt;br /&gt;
|-&lt;br /&gt;
|30_90_52   || 14.16     ||  2.115     ||  2.231    ||  0.9504    ||  0.9501    ||   1.736     ||  1.282    ||   5.476     ||  4.227&lt;br /&gt;
|-&lt;br /&gt;
|30_100_56  || 14.97     ||  2.187     ||  2.295    ||  0.9448    ||  0.9502    ||   1.743     ||  1.275    ||   4.949     ||  4.755&lt;br /&gt;
|-&lt;br /&gt;
|30_110_59  || 15.76     ||  2.246     ||  2.356    ||  0.9391    ||  0.9500    ||   1.751     ||  1.267    ||   4.920     ||  5.215&lt;br /&gt;
|-&lt;br /&gt;
|30_120_63  || 14.48     ||  2.306     ||  2.389    ||  0.9343    ||  0.9504    ||   1.758     ||  1.260    ||   3.573     ||  5.025&lt;br /&gt;
|-&lt;br /&gt;
|40_00_27   || 1.350     || 0.5464     || 0.5471    ||   1.024    ||  0.9504    ||   1.647     ||  1.371    ||  0.1331     || 2.4768E-02&lt;br /&gt;
|-&lt;br /&gt;
|40_10_29   || 4.111     || 0.8821     || 0.9010    ||   1.010    ||  0.9510    ||   1.663     ||  1.355    ||   2.152     || 0.2456&lt;br /&gt;
|-&lt;br /&gt;
|40_20_31   || 6.646     ||  1.146     ||  1.202    ||  0.9975    ||  0.9501    ||   1.677     ||  1.341    ||   4.928     || 0.8185&lt;br /&gt;
|-&lt;br /&gt;
|40_30_34   || 9.328     ||  1.354     ||  1.452    ||  0.9884    ||  0.9506    ||   1.688     ||  1.330    ||   7.247     ||  1.826&lt;br /&gt;
|-&lt;br /&gt;
|40_40_37   || 11.15     ||  1.523     ||  1.646    ||  0.9788    ||  0.9498    ||   1.699     ||  1.319    ||   8.061     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|40_50_41   || 12.66     ||  1.666     ||  1.797    ||  0.9719    ||  0.9506    ||   1.708     ||  1.310    ||   7.872     ||  4.310&lt;br /&gt;
|-&lt;br /&gt;
|40_60_44   || 12.34     ||  1.786     ||  1.927    ||  0.9637    ||  0.9497    ||   1.717     ||  1.301    ||   7.879     ||  5.834&lt;br /&gt;
|-&lt;br /&gt;
|40_70_48   || 9.734     ||  1.894     ||  1.963    ||  0.9579    ||  0.9504    ||   1.726     ||  1.292    ||   3.625     ||  3.668&lt;br /&gt;
|-&lt;br /&gt;
|40_80_52   || 13.96     ||  1.986     ||  2.067    ||  0.9515    ||  0.9503    ||   1.734     ||  1.284    ||   4.054     ||  3.028&lt;br /&gt;
|-&lt;br /&gt;
|40_90_56   || 15.39     ||  2.062     ||  2.156    ||  0.9457    ||  0.9504    ||   1.741     ||  1.277    ||   4.529     ||  3.841&lt;br /&gt;
|-&lt;br /&gt;
|40_100_60  || 16.40     ||  2.132     ||  2.232    ||  0.9400    ||  0.9502    ||   1.749     ||  1.269    ||   4.683     ||  4.355&lt;br /&gt;
|-&lt;br /&gt;
|40_110_64  || 18.12     ||  2.199     ||  2.288    ||  0.9348    ||  0.9503    ||   1.756     ||  1.262    ||   4.049     ||  4.651&lt;br /&gt;
|-&lt;br /&gt;
|40_120_68  || 16.81     ||  2.256     ||  2.327    ||  0.9295    ||  0.9501    ||   1.763     ||  1.255    ||   3.158     ||  4.904&lt;br /&gt;
|-&lt;br /&gt;
|50_00_31   || 2.818     || 0.6329     || 0.6375    ||   1.013    ||  0.9498    ||   1.657     ||  1.361    ||  0.7286     || 6.1871E-02&lt;br /&gt;
|-&lt;br /&gt;
|50_10_33   || 5.588     || 0.9254     || 0.9532    ||   1.001    ||  0.9506    ||   1.672     ||  1.346    ||   3.003     || 0.3605&lt;br /&gt;
|-&lt;br /&gt;
|50_20_36   || 8.222     ||  1.160     ||  1.216    ||  0.9902    ||  0.9502    ||   1.684     ||  1.334    ||   4.838     ||  1.060&lt;br /&gt;
|-&lt;br /&gt;
|50_30_39   || 10.67     ||  1.352     ||  1.435    ||  0.9815    ||  0.9505    ||   1.695     ||  1.323    ||   6.163     ||  2.008&lt;br /&gt;
|-&lt;br /&gt;
|50_40_42   || 12.44     ||  1.508     ||  1.609    ||  0.9733    ||  0.9504    ||   1.705     ||  1.313    ||   6.719     ||  2.910&lt;br /&gt;
|-&lt;br /&gt;
|50_50_46   || 13.94     ||  1.644     ||  1.758    ||  0.9661    ||  0.9505    ||   1.714     ||  1.303    ||   6.944     ||  4.001&lt;br /&gt;
|-&lt;br /&gt;
|50_60_49   || 15.09     ||  1.757     ||  1.887    ||  0.9587    ||  0.9502    ||   1.723     ||  1.295    ||   7.390     ||  6.217&lt;br /&gt;
|-&lt;br /&gt;
|50_70_53   || 13.03     ||  1.855     ||  1.955    ||  0.9524    ||  0.9502    ||   1.731     ||  1.287    ||   5.353     ||  5.830&lt;br /&gt;
|-&lt;br /&gt;
|50_80_56   || 16.73     ||  1.949     ||  2.004    ||  0.9463    ||  0.9501    ||   1.739     ||  1.279    ||   2.807     ||  4.003&lt;br /&gt;
|-&lt;br /&gt;
|50_90_60   || 16.70     ||  2.011     ||  2.101    ||  0.9407    ||  0.9502    ||   1.747     ||  1.271    ||   4.501     ||  3.444&lt;br /&gt;
|-&lt;br /&gt;
|50_100_64  || 18.15     ||  2.090     ||  2.183    ||  0.9351    ||  0.9500    ||   1.754     ||  1.264    ||   4.434     ||  3.907&lt;br /&gt;
|-&lt;br /&gt;
|50_110_68  || 17.53     ||  2.154     ||  2.223    ||  0.9297    ||  0.9498    ||   1.762     ||  1.256    ||   3.205     ||  4.270&lt;br /&gt;
|-&lt;br /&gt;
|50_120_72  || 19.13     ||  2.213     ||  2.288    ||  0.9250    ||  0.9501    ||   1.768     ||  1.250    ||   3.417     ||  4.378&lt;br /&gt;
|-&lt;br /&gt;
|60_00_35   || 4.247     || 0.7126     || 0.7205    ||   1.003    ||  0.9498    ||   1.667     ||  1.352    ||   1.108     || 0.1270&lt;br /&gt;
|-&lt;br /&gt;
|60_10_37   || 6.862     || 0.9679     ||  1.002    ||  0.9934    ||  0.9509    ||   1.680     ||  1.338    ||   3.520     || 0.4827&lt;br /&gt;
|-&lt;br /&gt;
|60_20_40   || 9.669     ||  1.179     ||  1.240    ||  0.9831    ||  0.9503    ||   1.692     ||  1.326    ||   5.202     ||  1.236&lt;br /&gt;
|-&lt;br /&gt;
|60_30_43   || 12.01     ||  1.354     ||  1.435    ||  0.9747    ||  0.9502    ||   1.702     ||  1.316    ||   5.973     ||  2.132&lt;br /&gt;
|-&lt;br /&gt;
|60_40_46   || 13.48     ||  1.500     ||  1.593    ||  0.9672    ||  0.9503    ||   1.712     ||  1.306    ||   6.170     ||  2.806&lt;br /&gt;
|-&lt;br /&gt;
|60_50_50   || 15.36     ||  1.627     ||  1.732    ||  0.9601    ||  0.9504    ||   1.721     ||  1.297    ||   6.467     ||  3.895&lt;br /&gt;
|-&lt;br /&gt;
|60_60_53   || 16.79     ||  1.734     ||  1.851    ||  0.9528    ||  0.9499    ||   1.729     ||  1.289    ||   6.731     ||  5.666&lt;br /&gt;
|-&lt;br /&gt;
|60_70_57   || 15.88     ||  1.829     ||  1.934    ||  0.9473    ||  0.9502    ||   1.737     ||  1.281    ||   5.736     ||  6.958&lt;br /&gt;
|-&lt;br /&gt;
|60_80_61   || 13.66     ||  1.918     ||  1.968    ||  0.9428    ||  0.9514    ||   1.745     ||  1.273    ||   2.622     ||  4.555&lt;br /&gt;
|-&lt;br /&gt;
|60_90_64   || 17.29     ||  2.009     ||  2.063    ||  0.9359    ||  0.9501    ||   1.753     ||  1.265    ||   2.640     ||  1.637&lt;br /&gt;
|-&lt;br /&gt;
|60_100_68  || 17.62     ||  2.049     ||  2.122    ||  0.9304    ||  0.9497    ||   1.760     ||  1.258    ||   3.560     ||  3.718&lt;br /&gt;
|-&lt;br /&gt;
|60_110_72  || 17.50     ||  2.118     ||  2.177    ||  0.9257    ||  0.9501    ||   1.767     ||  1.251    ||   2.811     ||  4.023&lt;br /&gt;
|-&lt;br /&gt;
|60_120_76  || 17.78     ||  2.174     ||  2.222    ||  0.9217    ||  0.9510    ||   1.774     ||  1.244    ||   2.209     ||  4.211&lt;br /&gt;
|-&lt;br /&gt;
|70_00_39   || 5.731     || 0.7825     || 0.7975    ||  0.9949    ||  0.9497    ||   1.675     ||  1.343    ||   1.908     || 0.2335&lt;br /&gt;
|-&lt;br /&gt;
|70_10_41   || 8.418     ||  1.009     ||  1.048    ||  0.9860    ||  0.9509    ||   1.688     ||  1.330    ||   3.845     || 0.6755&lt;br /&gt;
|-&lt;br /&gt;
|70_20_44   || 11.09     ||  1.201     ||  1.265    ||  0.9767    ||  0.9504    ||   1.699     ||  1.319    ||   5.345     ||  1.317&lt;br /&gt;
|-&lt;br /&gt;
|70_30_47   || 13.41     ||  1.361     ||  1.441    ||  0.9688    ||  0.9504    ||   1.709     ||  1.309    ||   5.859     ||  2.187&lt;br /&gt;
|-&lt;br /&gt;
|70_40_51   || 14.99     ||  1.496     ||  1.591    ||  0.9615    ||  0.9503    ||   1.718     ||  1.300    ||   6.348     ||  2.859&lt;br /&gt;
|-&lt;br /&gt;
|70_50_54   || 16.87     ||  1.617     ||  1.712    ||  0.9543    ||  0.9501    ||   1.727     ||  1.291    ||   5.843     ||  3.756&lt;br /&gt;
|-&lt;br /&gt;
|70_60_57   || 17.89     ||  1.718     ||  1.823    ||  0.9479    ||  0.9500    ||   1.735     ||  1.283    ||   6.140     ||  4.746&lt;br /&gt;
|-&lt;br /&gt;
|70_70_61   || 18.26     ||  1.812     ||  1.928    ||  0.9423    ||  0.9503    ||   1.743     ||  1.275    ||   6.353     ||  6.812&lt;br /&gt;
|-&lt;br /&gt;
|70_80_65   || 16.37     ||  1.896     ||  1.962    ||  0.9363    ||  0.9499    ||   1.751     ||  1.267    ||   3.469     ||  5.948&lt;br /&gt;
|-&lt;br /&gt;
|70_90_68   || 9.135     ||  1.980     ||  1.988    ||  0.9317    ||  0.9506    ||   1.758     ||  1.260    ||  0.3692     || 0.1186&lt;br /&gt;
|-&lt;br /&gt;
|70_100_72  || 18.64     ||  2.007     ||  2.094    ||  0.9267    ||  0.9506    ||   1.765     ||  1.253    ||   4.327     ||  3.356&lt;br /&gt;
|-&lt;br /&gt;
|70_110_76  || 18.23     ||  2.088     ||  2.147    ||  0.9219    ||  0.9507    ||   1.772     ||  1.246    ||   2.792     ||  3.707&lt;br /&gt;
|-&lt;br /&gt;
|70_120_80  || 17.89     ||  2.145     ||  2.184    ||  0.9171    ||  0.9506    ||   1.779     ||  1.239    ||   1.846     ||  4.043&lt;br /&gt;
|-&lt;br /&gt;
|80_00_42   ||7.247      ||0.8436      ||0.8697     || 0.9869     || 0.9497     ||  1.684      || 1.335     ||  3.094      ||0.2402&lt;br /&gt;
|-&lt;br /&gt;
|80_10_45   ||9.865      || 1.049      || 1.095     || 0.9794     || 0.9513     ||  1.695      || 1.323     ||  4.371      ||0.7359&lt;br /&gt;
|-&lt;br /&gt;
|80_20_48   ||12.28      || 1.226      || 1.290     || 0.9697     || 0.9500     ||  1.706      || 1.312     ||  5.206      || 1.327&lt;br /&gt;
|-&lt;br /&gt;
|80_30_51   ||14.38      || 1.370      || 1.454     || 0.9626     || 0.9503     ||  1.715      || 1.303     ||  6.088      || 2.102&lt;br /&gt;
|-&lt;br /&gt;
|80_40_54   ||16.47      || 1.500      || 1.594     || 0.9549     || 0.9497     ||  1.724      || 1.294     ||  6.263      || 2.799&lt;br /&gt;
|-&lt;br /&gt;
|80_50_58   ||17.63      || 1.612      || 1.706     || 0.9492     || 0.9503     ||  1.733      || 1.285     ||  5.842      || 3.329&lt;br /&gt;
|-&lt;br /&gt;
|80_60_61   ||18.84      || 1.712      || 1.814     || 0.9436     || 0.9507     ||  1.741      || 1.277     ||  5.984      || 3.990&lt;br /&gt;
|-&lt;br /&gt;
|80_70_65   ||19.27      || 1.799      || 1.898     || 0.9372     || 0.9501     ||  1.749      || 1.269     ||  5.555      || 4.728&lt;br /&gt;
|-&lt;br /&gt;
|80_80_69   ||17.96      || 1.880      || 1.935     || 0.9321     || 0.9503     ||  1.756      || 1.262     ||  2.921      || 3.774&lt;br /&gt;
|-&lt;br /&gt;
|80_90_73   ||13.42      || 1.957      || 1.982     || 0.9266     || 0.9500     ||  1.764      || 1.254     ||  1.312      ||0.6938&lt;br /&gt;
|-&lt;br /&gt;
|80_100_76  || 18.53     ||  2.008     ||  2.065    ||  0.9220    ||  0.9504    ||   1.770     ||  1.247    ||   2.839     ||  1.773&lt;br /&gt;
|-&lt;br /&gt;
|80_110_80  || 18.41     ||  2.059     ||  2.117    ||  0.9176    ||  0.9507    ||   1.777     ||  1.241    ||   2.847     ||  3.632&lt;br /&gt;
|-&lt;br /&gt;
|80_120_84  || 18.26     ||  2.117     ||  2.157    ||  0.9122    ||  0.9496    ||   1.784     ||  1.234    ||   1.872     ||  3.986&lt;br /&gt;
|-&lt;br /&gt;
|90_00_46   || 8.679     || 0.9022     || 0.9354    ||  0.9802    ||  0.9501    ||   1.691     ||  1.327    ||   3.678     || 0.3981&lt;br /&gt;
|-&lt;br /&gt;
|90_10_49   || 11.45     ||  1.090     ||  1.146    ||  0.9717    ||  0.9502    ||   1.702     ||  1.315    ||   5.148     || 0.8099&lt;br /&gt;
|-&lt;br /&gt;
|90_20_52   || 12.44     ||  1.247     ||  1.323    ||  0.9640    ||  0.9503    ||   1.712     ||  1.305    ||   6.100     ||  1.079&lt;br /&gt;
|-&lt;br /&gt;
|90_30_55   || 16.14     ||  1.383     ||  1.475    ||  0.9571    ||  0.9504    ||   1.722     ||  1.296    ||   6.607     ||  2.158&lt;br /&gt;
|-&lt;br /&gt;
|90_40_58   || 17.45     ||  1.506     ||  1.597    ||  0.9499    ||  0.9501    ||   1.731     ||  1.287    ||   6.012     ||  2.629&lt;br /&gt;
|-&lt;br /&gt;
|90_50_62   || 18.70     ||  1.609     ||  1.706    ||  0.9438    ||  0.9501    ||   1.739     ||  1.279    ||   6.003     ||  2.901&lt;br /&gt;
|-&lt;br /&gt;
|90_60_65   || 18.77     ||  1.703     ||  1.789    ||  0.9381    ||  0.9502    ||   1.747     ||  1.271    ||   5.045     ||  3.047&lt;br /&gt;
|-&lt;br /&gt;
|90_70_69   || 18.43     ||  1.787     ||  1.852    ||  0.9324    ||  0.9500    ||   1.754     ||  1.263    ||   3.623     ||  3.117&lt;br /&gt;
|-&lt;br /&gt;
|90_80_73   || 17.72     ||  1.868     ||  1.909    ||  0.9269    ||  0.9497    ||   1.762     ||  1.256    ||   2.217     ||  2.354&lt;br /&gt;
|-&lt;br /&gt;
|90_90_76   || 14.40     ||  1.940     ||  1.956    ||  0.9221    ||  0.9499    ||   1.769     ||  1.249    ||  0.8079     || 0.8326&lt;br /&gt;
|-&lt;br /&gt;
|90_100_80  || 18.53     ||  2.009     ||  2.038    ||  0.9176    ||  0.9503    ||   1.776     ||  1.242    ||   1.484     ||  1.095&lt;br /&gt;
|-&lt;br /&gt;
|90_110_84  || 18.97     ||  2.021     ||  2.094    ||  0.9129    ||  0.9502    ||   1.783     ||  1.235    ||   3.625     ||  3.669&lt;br /&gt;
|-&lt;br /&gt;
|90_120_88  || 17.79     ||  2.090     ||  2.129    ||  0.9077    ||  0.9494    ||   1.789     ||  1.229    ||   1.827     ||  3.862&lt;br /&gt;
|-&lt;br /&gt;
|100_00_50  || 10.07     || 0.9544     || 0.9970    ||  0.9732    ||  0.9499    ||   1.699     ||  1.319    ||   4.471     || 0.4341&lt;br /&gt;
|-&lt;br /&gt;
|100_10_53  || 12.78     ||  1.127     ||  1.186    ||  0.9649    ||  0.9499    ||   1.710     ||  1.308    ||   5.262     || 0.9629&lt;br /&gt;
|-&lt;br /&gt;
|100_16_55  || 13.69     ||  1.215     ||  1.287    ||  0.9610    ||  0.9501    ||   1.715     ||  1.302    ||   5.901     ||  1.023&lt;br /&gt;
|-&lt;br /&gt;
|100_20_56  || 10.86     ||  1.271     ||  1.324    ||  0.9583    ||  0.9502    ||   1.719     ||  1.299    ||   4.120     || 0.8295&lt;br /&gt;
|-&lt;br /&gt;
|100_22_56  || 15.40     ||  1.309     ||  1.381    ||  0.9412    ||  0.9362    ||   1.722     ||  1.296    ||   5.552     ||  1.648&lt;br /&gt;
|-&lt;br /&gt;
|100_24_58  || 15.90     ||  1.326     ||  1.406    ||  0.9552    ||  0.9499    ||   1.722     ||  1.295    ||   6.105     ||  1.792&lt;br /&gt;
|-&lt;br /&gt;
|100_26_58  || 16.42     ||  1.352     ||  1.435    ||  0.9538    ||  0.9499    ||   1.724     ||  1.293    ||   6.137     ||  1.888&lt;br /&gt;
|-&lt;br /&gt;
|100_28_59  || 17.07     ||  1.375     ||  1.464    ||  0.9527    ||  0.9501    ||   1.726     ||  1.291    ||   6.475     ||  1.983&lt;br /&gt;
|-&lt;br /&gt;
|100_30_59  || 17.29     ||  1.398     ||  1.490    ||  0.9511    ||  0.9500    ||   1.728     ||  1.289    ||   6.561     ||  2.075&lt;br /&gt;
|-&lt;br /&gt;
|100_32_60  || 17.74     ||  1.423     ||  1.517    ||  0.9499    ||  0.9499    ||   1.730     ||  1.288    ||   6.596     ||  2.165&lt;br /&gt;
|-&lt;br /&gt;
|100_36_61  || 18.37     ||  1.467     ||  1.567    ||  0.9475    ||  0.9501    ||   1.733     ||  1.284    ||   6.819     ||  2.183&lt;br /&gt;
|-&lt;br /&gt;
|100_40_63  || 18.77     ||  1.509     ||  1.608    ||  0.9450    ||  0.9500    ||   1.736     ||  1.281    ||   6.553     ||  2.304&lt;br /&gt;
|-&lt;br /&gt;
|100_44_64  || 19.25     ||  1.551     ||  1.653    ||  0.9426    ||  0.9500    ||   1.740     ||  1.278    ||   6.569     ||  2.360&lt;br /&gt;
|-&lt;br /&gt;
|100_48_65  || 19.16     ||  1.591     ||  1.684    ||  0.9400    ||  0.9500    ||   1.743     ||  1.275    ||   5.807     ||  2.555&lt;br /&gt;
|-&lt;br /&gt;
|100_50_65  || 19.11     ||  1.613     ||  1.704    ||  0.9381    ||  0.9501    ||   1.745     ||  1.274    ||   5.628     ||  2.649&lt;br /&gt;
|-&lt;br /&gt;
|100_55_67  || 19.04     ||  1.659     ||  1.739    ||  0.9352    ||  0.9500    ||   1.749     ||  1.270    ||   4.839     ||  2.808&lt;br /&gt;
|-&lt;br /&gt;
|100_56_67  || 18.93     ||  1.667     ||  1.742    ||  0.9347    ||  0.9501    ||   1.750     ||  1.269    ||   4.522     ||  2.692&lt;br /&gt;
|-&lt;br /&gt;
|100_60_68  || 19.04     ||  1.702     ||  1.775    ||  0.9325    ||  0.9500    ||   1.753     ||  1.266    ||   4.326     ||  2.720&lt;br /&gt;
|-&lt;br /&gt;
|100_64_70  || 18.76     ||  1.733     ||  1.799    ||  0.9303    ||  0.9500    ||   1.756     ||  1.263    ||   3.774     ||  2.676&lt;br /&gt;
|-&lt;br /&gt;
|100_68_72  || 18.46     ||  1.771     ||  1.825    ||  0.9279    ||  0.9494    ||   1.759     ||  1.259    ||   3.080     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_70_73  || 18.23     ||  1.784     ||  1.841    ||  0.9277    ||  0.9500    ||   1.760     ||  1.258    ||   3.166     ||  2.452&lt;br /&gt;
|-&lt;br /&gt;
|100_80_77  || 16.73     ||  1.855     ||  1.885    ||  0.9261    ||  0.9532    ||   1.767     ||  1.251    ||   1.617     ||  1.818&lt;br /&gt;
|-&lt;br /&gt;
|100_90_80  || 13.86     ||  1.931     ||  1.936    ||  0.9172    ||  0.9494    ||   1.774     ||  1.244    ||  0.2833     || 0.7382&lt;br /&gt;
|-&lt;br /&gt;
|100_95_82  || 11.27     ||  1.967     ||  1.964    ||  0.9243    ||  0.9582    ||   1.777     ||  1.241    || -0.1435     || 6.8954E-02&lt;br /&gt;
|-&lt;br /&gt;
|100_105_86 || 16.96     ||  2.019     ||  2.045    ||  0.9233    ||  0.9617    ||   1.783     ||  1.235    ||   1.268     ||  1.425&lt;br /&gt;
|-&lt;br /&gt;
|100_110_88 || 18.88     ||  2.020     ||  2.073    ||  0.9229    ||  0.9634    ||   1.786     ||  1.232    ||   2.618     ||  2.366&lt;br /&gt;
|-&lt;br /&gt;
|100_120_92 || 17.63     ||  2.064     ||  2.113    ||  0.9044    ||  0.9501    ||   1.794     ||  1.224    ||   2.379     ||  3.790&lt;br /&gt;
|-&lt;br /&gt;
|110_00_54  || 11.70     ||  1.006     ||  1.060    ||  0.9663    ||  0.9498    ||   1.706     ||  1.312    ||   5.370     || 0.4642&lt;br /&gt;
|-&lt;br /&gt;
|110_10_57  || 13.97     ||  1.160     ||  1.232    ||  0.9593    ||  0.9502    ||   1.716     ||  1.301    ||   6.136     || 0.8247&lt;br /&gt;
|-&lt;br /&gt;
|110_20_60  || 15.75     ||  1.298     ||  1.372    ||  0.9526    ||  0.9504    ||   1.726     ||  1.292    ||   5.739     ||  1.330&lt;br /&gt;
|-&lt;br /&gt;
|110_30_63  || 18.56     ||  1.415     ||  1.516    ||  0.9455    ||  0.9500    ||   1.734     ||  1.284    ||   7.122     ||  1.849&lt;br /&gt;
|-&lt;br /&gt;
|110_40_66  || 19.50     ||  1.521     ||  1.622    ||  0.9398    ||  0.9503    ||   1.743     ||  1.275    ||   6.602     ||  1.921&lt;br /&gt;
|-&lt;br /&gt;
|110_50_70  || 19.07     ||  1.618     ||  1.696    ||  0.9336    ||  0.9498    ||   1.751     ||  1.267    ||   4.873     ||  2.085&lt;br /&gt;
|-&lt;br /&gt;
|110_60_73  || 18.32     ||  1.702     ||  1.761    ||  0.9291    ||  0.9507    ||   1.758     ||  1.260    ||   3.471     ||  2.033&lt;br /&gt;
|-&lt;br /&gt;
|110_70_77  || 17.13     ||  1.782     ||  1.816    ||  0.9237    ||  0.9504    ||   1.766     ||  1.252    ||   1.948     ||  1.838&lt;br /&gt;
|-&lt;br /&gt;
|110_80_81  || 15.56     ||  1.853     ||  1.871    ||  0.9192    ||  0.9508    ||   1.773     ||  1.245    ||  0.9878     ||  1.332&lt;br /&gt;
|-&lt;br /&gt;
|110_90_84  || 13.12     ||  1.923     ||  1.926    ||  0.9142    ||  0.9506    ||   1.780     ||  1.238    ||  0.1639     || 0.5301&lt;br /&gt;
|-&lt;br /&gt;
|110_95_86  || 10.73     ||  1.963     ||  1.955    ||  0.9095    ||  0.9486    ||   1.783     ||  1.235    || -0.3746     || 8.1449E-04&lt;br /&gt;
|-&lt;br /&gt;
|110_110_92 || 17.29     ||  2.020     ||  2.055    ||  0.9056    ||  0.9509    ||   1.793     ||  1.225    ||   1.768     ||  2.045&lt;br /&gt;
|-&lt;br /&gt;
|110_120_95 || 17.55     ||  2.048     ||  2.095    ||  0.9014    ||  0.9510    ||   1.799     ||  1.219    ||   2.314     ||  3.774&lt;br /&gt;
|-&lt;br /&gt;
|120_00_57  || 13.14     ||  1.050     ||  1.117    ||  0.9599    ||  0.9497    ||   1.714     ||  1.305    ||   6.304     || 0.4861&lt;br /&gt;
|-&lt;br /&gt;
|120_10_60  || 14.81     ||  1.196     ||  1.268    ||  0.9534    ||  0.9501    ||   1.723     ||  1.295    ||   6.054     || 0.8382&lt;br /&gt;
|-&lt;br /&gt;
|120_20_63  || 17.57     ||  1.323     ||  1.409    ||  0.9458    ||  0.9494    ||   1.732     ||  1.286    ||   6.504     ||  1.409&lt;br /&gt;
|-&lt;br /&gt;
|120_30_67  || 19.50     ||  1.435     ||  1.539    ||  0.9407    ||  0.9503    ||   1.741     ||  1.277    ||   7.263     ||  1.529&lt;br /&gt;
|-&lt;br /&gt;
|120_40_70  || 19.38     ||  1.534     ||  1.621    ||  0.9335    ||  0.9492    ||   1.749     ||  1.269    ||   5.695     ||  1.632&lt;br /&gt;
|-&lt;br /&gt;
|120_50_74  || 18.34     ||  1.621     ||  1.684    ||  0.9294    ||  0.9503    ||   1.756     ||  1.262    ||   3.910     ||  1.864&lt;br /&gt;
|-&lt;br /&gt;
|120_60_77  || 17.24     ||  1.703     ||  1.743    ||  0.9246    ||  0.9507    ||   1.764     ||  1.254    ||   2.381     ||  1.733&lt;br /&gt;
|-&lt;br /&gt;
|120_70_81  || 16.02     ||  1.780     ||  1.803    ||  0.9197    ||  0.9509    ||   1.771     ||  1.247    ||   1.312     ||  1.511&lt;br /&gt;
|-&lt;br /&gt;
|120_80_84  || 14.49     ||  1.850     ||  1.860    ||  0.9150    ||  0.9509    ||   1.778     ||  1.240    ||  0.5347     ||  1.076&lt;br /&gt;
|-&lt;br /&gt;
|120_90_88  || 12.18     ||  1.918     ||  1.918    ||  0.9096    ||  0.9501    ||   1.785     ||  1.233    || -4.1127E-02 || 0.3613&lt;br /&gt;
|-&lt;br /&gt;
|120_95_90  || 10.06     ||  1.957     ||  1.950    ||  0.9071    ||  0.9499    ||   1.788     ||  1.230    || -0.3241     ||  0.000&lt;br /&gt;
|-&lt;br /&gt;
|120_115_97 || 16.46     ||  2.020     ||  2.066    ||  0.8983    ||  0.9497    ||   1.801     ||  1.216    ||   2.258     ||  2.404&lt;br /&gt;
|-&lt;br /&gt;
|120_120_99 || 17.58     ||  2.008     ||  2.092    ||  0.8967    ||  0.9501    ||   1.804     ||  1.213    ||   4.186     ||  3.647&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Flexibility ==&lt;br /&gt;
&lt;br /&gt;
[[File:Flexibility TJ-II.png|300px|thumb|right|Flexibility diagram of TJ-II magnetic configurations. Several lines of constant rotational transform are highlighted and labelled with the corresponding central &amp;lt;math&amp;gt;\iota/2\pi&amp;lt;/math&amp;gt;-value.]]&lt;br /&gt;
TJ-II has considerable configurational flexibility, as observed in the &#039;flexibility diagram&#039;&amp;lt;ref&amp;gt;E. Ascasíbar, T. Estrada, F. Castejón, A. López-Fraguas, I. Pastor, J. Sánchez, U. Stroth, J. Qin and TJ-II Team, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/45/4/009|Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276–284]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8721</id>
		<title>TJ-II:Magnetic configuration</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8721"/>
		<updated>2026-10-07T12:47:43Z</updated>

		<summary type="html">&lt;p&gt;Admin: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The magnetic configuration of [[TJ-II]] in vacuum is completely determined by the currents flowing through the [[TJ-II:Coil system|external coils]].&lt;br /&gt;
Magnetic configurations are labelled as &#039;xxx_yy_zz&#039;, where&lt;br /&gt;
* &#039;xxx&#039;: 10 times the current (in kA) in the circular coil&lt;br /&gt;
* &#039;yy&#039;: 10 times the current (in kA) in the helical coil&lt;br /&gt;
* &#039;zz&#039;: 10 times the current (in kA) in the vertical field coils&lt;br /&gt;
The current in the toroidal field coils is not specified, as its value is adjusted to guarantee central absorption of the [[TJ-II:Electron Cyclotron Resonant Heating|Electron Cyclotron Resonant Heating]] source (requiring a specific value of the magnetic field on the magnetic axis).&lt;br /&gt;
&lt;br /&gt;
Often used configurations are:&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; | Configuration&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; | &amp;lt;math&amp;gt;\iota(0)/2\pi&amp;lt;/math&amp;gt;&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; | Volume (m&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt;)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; | Magnetic well (%)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; | Minor radius &#039;&#039;a&#039;&#039; (m)&lt;br /&gt;
|-&lt;br /&gt;
|100_28_59  || 1.375  || 0.8111 || 1.9   || 0.1760&lt;br /&gt;
|-&lt;br /&gt;
|100_32_60  || 1.423  || 0.934  || 2.0   || 0.1880&lt;br /&gt;
|-&lt;br /&gt;
|100_36_62  || 1.467  || 0.987  || 2.2   || 0.1950&lt;br /&gt;
|-&lt;br /&gt;
|100_40_63  || 1.509  || 1.065  || 2.2   || 0.2030&lt;br /&gt;
|-&lt;br /&gt;
|100_44_64  || 1.551  || 1.287  || 2.4   || 0.2220&lt;br /&gt;
|-&lt;br /&gt;
|100_48_65  || 1.591  || 1.2043 || 2.46  || 0.2160&lt;br /&gt;
|-&lt;br /&gt;
|100_50_65  || 1.614  || 1.260  || 2.5   || 0.2210&lt;br /&gt;
|-&lt;br /&gt;
|100_68_72  || 1.770  || 1.226  || 2.36  || 0.2210&lt;br /&gt;
|-&lt;br /&gt;
| 69_41_51  || 1.515  || 0.580  || 2.5   || 0.1509&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Flexibility ==&lt;br /&gt;
&lt;br /&gt;
[[File:Flexibility TJ-II.png|300px|thumb|right|Flexibility diagram of TJ-II magnetic configurations. Several lines of constant rotational transform are highlighted and labelled with the corresponding central &amp;lt;math&amp;gt;\iota/2\pi&amp;lt;/math&amp;gt;-value.]]&lt;br /&gt;
TJ-II has considerable configurational flexibility, as observed in the &#039;flexibility diagram&#039;&amp;lt;ref&amp;gt;E. Ascasíbar, T. Estrada, F. Castejón, A. López-Fraguas, I. Pastor, J. Sánchez, U. Stroth, J. Qin and TJ-II Team, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/45/4/009|Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276–284]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8720</id>
		<title>TJ-II:Magnetic configuration</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8720"/>
		<updated>2026-10-07T10:43:39Z</updated>

		<summary type="html">&lt;p&gt;Admin: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The magnetic configuration of [[TJ-II]] in vacuum is completely determined by the currents flowing through the [[TJ-II:Coil system|external coils]].&lt;br /&gt;
Magnetic configurations are labelled as &#039;xxx_yy_zz&#039;, where&lt;br /&gt;
* &#039;xxx&#039;: 10 times the current (in kA) in the circular coil&lt;br /&gt;
* &#039;yy&#039;: 10 times the current (in kA) in the helical coil&lt;br /&gt;
* &#039;zz&#039;: 10 times the current (in kA) in the vertical field coils&lt;br /&gt;
The current in the toroidal field coils is not specified, as its value is adjusted to guarantee central absorption of the [[TJ-II:Electron Cyclotron Resonant Heating|Electron Cyclotron Resonant Heating]] source (requiring a specific value of the magnetic field on the magnetic axis).&lt;br /&gt;
&lt;br /&gt;
Often used configurations are:&lt;br /&gt;
* 100_44_64 (a = 0.1925 m, &amp;lt;math&amp;gt;\iota_0/2\pi = 1.55&amp;lt;/math&amp;gt;, V&amp;lt;sub&amp;gt;plasma&amp;lt;/sub&amp;gt; = 1.098 m&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt;) &lt;br /&gt;
* 100_48_65 (a = 0.191 m, &amp;lt;math&amp;gt;\iota_0/2\pi = 1.591&amp;lt;/math&amp;gt;, V&amp;lt;sub&amp;gt;plasma&amp;lt;/sub&amp;gt;= 1.09 m&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
== Flexibility ==&lt;br /&gt;
&lt;br /&gt;
[[File:Flexibility TJ-II.png|300px|thumb|right|Flexibility diagram of TJ-II magnetic configurations. Several lines of constant rotational transform are highlighted and labelled with the corresponding central &amp;lt;math&amp;gt;\iota/2\pi&amp;lt;/math&amp;gt;-value.]]&lt;br /&gt;
TJ-II has considerable configurational flexibility, as observed in the &#039;flexibility diagram&#039;&amp;lt;ref&amp;gt;E. Ascasíbar, T. Estrada, F. Castejón, A. López-Fraguas, I. Pastor, J. Sánchez, U. Stroth, J. Qin and TJ-II Team, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/45/4/009|Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276–284]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8719</id>
		<title>TJ-II:Magnetic configuration</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8719"/>
		<updated>2026-10-07T10:41:35Z</updated>

		<summary type="html">&lt;p&gt;Admin: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The magnetic configuration of [[TJ-II]] in vacuum is completely determined by the currents flowing through the [[TJ-II:Coil system|external coils]].&lt;br /&gt;
Magnetic configurations are labelled as &#039;xxx_yy_zz&#039;, where&lt;br /&gt;
* &#039;xxx&#039;: 10 times the current (in kA) in the circular coil&lt;br /&gt;
* &#039;yy&#039;: 10 times the current (in kA) in the helical coil&lt;br /&gt;
* &#039;zz&#039;: 10 times the current (in kA) in the vertical field coils&lt;br /&gt;
The toroidal field is not specified, as its value is adjusted to guarantee central absorption of the [[TJ-II:Electron Cyclotron Resonant Heating|Electron Cyclotron Resonant Heating]] source.&lt;br /&gt;
&lt;br /&gt;
Often used configurations are:&lt;br /&gt;
* 100_44_64 (a = 0.1925 m, &amp;lt;math&amp;gt;\iota_0/2\pi = 1.55&amp;lt;/math&amp;gt;, V&amp;lt;sub&amp;gt;plasma&amp;lt;/sub&amp;gt; = 1.098 m&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt;) &lt;br /&gt;
* 100_48_65 (a = 0.191 m, &amp;lt;math&amp;gt;\iota_0/2\pi = 1.591&amp;lt;/math&amp;gt;, V&amp;lt;sub&amp;gt;plasma&amp;lt;/sub&amp;gt;= 1.09 m&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt;)&lt;br /&gt;
&lt;br /&gt;
== Flexibility ==&lt;br /&gt;
&lt;br /&gt;
[[File:Flexibility TJ-II.png|300px|thumb|right|Flexibility diagram of TJ-II magnetic configurations. Several lines of constant rotational transform are highlighted and labelled with the corresponding central &amp;lt;math&amp;gt;\iota/2\pi&amp;lt;/math&amp;gt;-value.]]&lt;br /&gt;
TJ-II has considerable configurational flexibility, as observed in the &#039;flexibility diagram&#039;&amp;lt;ref&amp;gt;E. Ascasíbar, T. Estrada, F. Castejón, A. López-Fraguas, I. Pastor, J. Sánchez, U. Stroth, J. Qin and TJ-II Team, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/45/4/009|Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276–284]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=File:Flexibility_TJ-II.png&amp;diff=8718</id>
		<title>File:Flexibility TJ-II.png</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=File:Flexibility_TJ-II.png&amp;diff=8718"/>
		<updated>2026-10-07T10:34:17Z</updated>

		<summary type="html">&lt;p&gt;Admin: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8717</id>
		<title>TJ-II:Magnetic configuration</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8717"/>
		<updated>2026-10-07T10:31:47Z</updated>

		<summary type="html">&lt;p&gt;Admin: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The magnetic configuration of [[TJ-II]] in vacuum is completely determined by the currents flowing through the [[TJ-II:Coil system|external coils]].&lt;br /&gt;
Magnetic configurations are labelled as &#039;xxx_yy_zz&#039;, where&lt;br /&gt;
* &#039;xxx&#039;: 10 times the current (in kA) in the circular coil&lt;br /&gt;
* &#039;yy&#039;: 10 times the current (in kA) in the helical coil&lt;br /&gt;
* &#039;zz&#039;: 10 times the current (in kA) in the vertical field coils&lt;br /&gt;
The toroidal field is not specified, as its value is adjusted to guarantee central absorption of the [[TJ-II:Electron Cyclotron Resonant Heating|Electron Cyclotron Resonant Heating]] source.&lt;br /&gt;
&lt;br /&gt;
Often used configurations are:&lt;br /&gt;
* 100_44_64 (a = 0.1925 m, &amp;lt;math&amp;gt;\iota_0/2\pi = 1.55&amp;lt;/math&amp;gt;, V&amp;lt;sub&amp;gt;plasma&amp;lt;/sub&amp;gt; = 1.098 m&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt;) &lt;br /&gt;
* 100_48_65 (a = 0.191 m, &amp;lt;math&amp;gt;\iota_0/2\pi = 1.591&amp;lt;/math&amp;gt;, V&amp;lt;sub&amp;gt;plasma&amp;lt;/sub&amp;gt;= 1.09 m&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt;)&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8716</id>
		<title>TJ-II:Magnetic configuration</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Magnetic_configuration&amp;diff=8716"/>
		<updated>2026-10-07T10:29:36Z</updated>

		<summary type="html">&lt;p&gt;Admin: Created page with &amp;quot;The magnetic configuration of TJ-II in vacuum is completely determined by the currents flowing through the external coils. Magnetic configurations are labelled as &amp;#039;xxx_yy_zz&amp;#039;, where * &amp;#039;xxx&amp;#039;: 10 times the current (in kA) in the circular coil * &amp;#039;yy&amp;#039;: 10 times the current (in kA) in the helical coil * &amp;#039;zz&amp;#039;: 10 times the current (in kA) in the vertical field coils  Often used configurations are: * 100_44_64 (a = 0.1925 m, &amp;lt;math&amp;gt;\iota_0/2\pi = 1.55&amp;lt;/...&amp;quot;&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The magnetic configuration of [[TJ-II]] in vacuum is completely determined by the currents flowing through the [[TJ-II:Coil system|external coils]].&lt;br /&gt;
Magnetic configurations are labelled as &#039;xxx_yy_zz&#039;, where&lt;br /&gt;
* &#039;xxx&#039;: 10 times the current (in kA) in the circular coil&lt;br /&gt;
* &#039;yy&#039;: 10 times the current (in kA) in the helical coil&lt;br /&gt;
* &#039;zz&#039;: 10 times the current (in kA) in the vertical field coils&lt;br /&gt;
&lt;br /&gt;
Often used configurations are:&lt;br /&gt;
* 100_44_64 (a = 0.1925 m, &amp;lt;math&amp;gt;\iota_0/2\pi = 1.55&amp;lt;/math&amp;gt;, V&amp;lt;sub&amp;gt;plasma&amp;lt;/sub&amp;gt; = 1.098 m&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt;) &lt;br /&gt;
* 100_48_65 (a = 0.191 m, &amp;lt;math&amp;gt;\iota_0/2\pi = 1.591&amp;lt;/math&amp;gt;, V&amp;lt;sub&amp;gt;plasma&amp;lt;/sub&amp;gt;= 1.09 m&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt;)&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II&amp;diff=8715</id>
		<title>TJ-II</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II&amp;diff=8715"/>
		<updated>2026-10-07T10:18:26Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* Description */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[File:TJII_model.jpg|500px|thumb|right|TJ-II Model]]&lt;br /&gt;
&lt;br /&gt;
TJ-II is a flexible Heliac installed at Spain&#039;s [[Laboratorio Nacional de Fusión|National Fusion Laboratory]]. &lt;br /&gt;
It is one of Spain&#039;s [https://www.ciencia.gob.es/Organismos-y-Centros/Infraestructuras-Cientificas-y-Tecnicas-Singulares-ICTS.html Unique Scientific and Technical Infrastructures].&lt;br /&gt;
It is currently operational.&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
[[File:Foto_grupo_Fusion_1996.jpg|300px|thumb|left|TJ-II and the TJ-II Team in 1996]]&lt;br /&gt;
&lt;br /&gt;
The flexible Heliac TJ-II was designed on the basis of calculations performed by the team of physicists and engineers of [[CIEMAT]], in collaboration with the Oak Ridge National Laboratory ([http://en.wikipedia.org/wiki/ORNL ORNL], USA) and the Institut für PlasmaPhysik at Garching ([http://en.wikipedia.org/wiki/Max-Planck-Institut_f%C3%BCr_Plasmaphysik IPP], Germany).&lt;br /&gt;
&amp;lt;ref&amp;gt;T.C. Hender et al, &#039;&#039;Studies of a flexible heliac configuration&#039;&#039;, [https://www.osti.gov/biblio/6007697-studies-flexible-heliac-configuration Report ORNL/TM-10374 (1987) OSTI ID: 6007697]&amp;lt;/ref&amp;gt;,&lt;br /&gt;
&amp;lt;ref&amp;gt;A. Perea et al., &amp;quot;Physics Issues in the Design of TJ-II, Proc. 12th European Conf. Controlled Fusion and Plasma Physics, Budapest, Hungary, 1985, [http://libero.ipp.mpg.de/libero/PDF/EPS_12_Vol1_1985.pdf ECA Vol. 9F, Part I, p. 433], European Physical Society (1985)&amp;lt;/ref&amp;gt;. &lt;br /&gt;
The TJ-II project received preferential support from [[Euratom]] for phase I (Physics) in 1986&amp;lt;ref&amp;gt;Application for EURATOM preferential support (Phase I) - TJ-II EXPERIMENT, [https://info.fusion.ciemat.es/InternalReport/fusion_1985.pdf Technical report, Asociación EURATOM/CIEMAT, 1985]&amp;lt;/ref&amp;gt; and for phase II (Engineering) in 1990&amp;lt;ref&amp;gt;Application for EURATOM preferential support (Phase II) - TJ-II EXPERIMENT, [https://info.fusion.ciemat.es/InternalReport/fusion_1989b.pdf Technical report, Asociación EURATOM/CIEMAT, 1989]&amp;lt;/ref&amp;gt;. The [[TJ-II:Construction|construction of this flexible Heliac]] was carried out in parts according to its constitutive elements, which were commissioned to various European companies, although 60% of the investments reverted back to Spanish companies.&lt;br /&gt;
&lt;br /&gt;
The first plasma was produced in 1997.&amp;lt;ref&amp;gt;[http://www.ciemat.es/vertices/vertices-292017/Vertices29/pdf/VERTICES29.pdf Special issue of CIEMAT&#039;s magazine &#039;&#039;Vertices&#039;&#039;] commemorating 20 years of experiments (December, 2017)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Precedents ==&lt;br /&gt;
&lt;br /&gt;
TJ-II is the third magnetic confinement device in a series. In 1983, the device [[TJ-I]] was taken into operation.&lt;br /&gt;
The denomination of this device is due to the abbreviation of &amp;quot;Tokamak de la Junta de Energía Nuclear&amp;quot;, this being the former denomination of [[CIEMAT]]. The abbreviation was maintained for successive devices for administrative reasons.&lt;br /&gt;
&lt;br /&gt;
In 1994, the torsatron [[TJ-IU]] was taken into operation. This was the first magnetic confinement device entirely built in Spain. Currently, [[TJ-IU]] is located at the [http://www.ipf.uni-stuttgart.de/index_e.html University of Stuttgart] in Germany under the name of [[TJ-K]] (the &#039;K&#039; stands for Kiel, its first location in Germany, before arriving in Stuttgart).&lt;br /&gt;
&lt;br /&gt;
== Description ==&lt;br /&gt;
&lt;br /&gt;
[[File:TJ-II_3D_perspective.jpg|300px|thumb|right|TJ-II perspective view]]&lt;br /&gt;
&lt;br /&gt;
In TJ-II, the magnetic trap is obtained by means of [[TJ-II:Coil system|various sets of coils]] that completely determine the magnetic surfaces before plasma initiation. The toroidal field is created by 32 coils. The three-dimensional twist of the central axis of the [[TJ-II:Magnetic configuration|configuration]] is generated by means of two central coils: one circular and one helical. The horizontal position of the plasma is controlled by the vertical field coils. The combined action of these magnetic fields generate bean-shaped magnetic surfaces that guide the particles of the plasma so that they do not collide with the [[TJ-II:Vacuum system|vacuum vessel]] wall. &lt;br /&gt;
&lt;br /&gt;
TJ-II discharges last around 0.25 s, with a repetition frequency of about 7 minutes.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Parameter&#039;&#039;                           !!&#039;&#039;Value&#039;&#039;!!&#039;&#039;Unit&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|Major radius, &#039;&#039;R&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;&#039;&#039;:          ||  1.5  || m  &lt;br /&gt;
|-&lt;br /&gt;
|Minor radius, &#039;&#039;a&#039;&#039;:          ||  &amp;lt; 0.22  || m  &lt;br /&gt;
|-&lt;br /&gt;
|Plasma volume, &#039;&#039;V&#039;&#039;:          ||  1  || m&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt;  &lt;br /&gt;
|-&lt;br /&gt;
|Field periods:          ||  4  ||   &lt;br /&gt;
|-&lt;br /&gt;
|[[TJ-II:Coil system|TF coils]]:          ||  32  ||   &lt;br /&gt;
|-&lt;br /&gt;
|Number of ports:          ||  104  ||   &lt;br /&gt;
|-&lt;br /&gt;
|Rotational transform, &#039;&#039;&amp;amp;iota;/2&amp;amp;pi;&#039;&#039;:          ||  0.9 - 2.5  ||   &lt;br /&gt;
|-&lt;br /&gt;
|Magnetic field on axis, &#039;&#039;B&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;&#039;&#039;:          ||  ~1  || T   &lt;br /&gt;
|-&lt;br /&gt;
|ECRH heating power, &#039;&#039;P&amp;lt;sub&amp;gt;ECRH&amp;lt;/sub&amp;gt;&#039;&#039;:          ||  &amp;lt; 600  || kW   &lt;br /&gt;
|-&lt;br /&gt;
|NBI heating power, &#039;&#039;P&amp;lt;sub&amp;gt;NBI&amp;lt;/sub&amp;gt;&#039;&#039;:          ||  &amp;lt; 2  || MW   &lt;br /&gt;
|-&lt;br /&gt;
|Pulse length:          ||  &amp;lt; 200  || ms   &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Goals and Research ==&lt;br /&gt;
&lt;br /&gt;
The objective of the experimental program of TJ-II is to investigate the physics of a device with a helical magnetic axis having a great flexibility in its magnetic configuration, and to contribute to the international effort regarding the study of magnetic confinement devices for fusion. &lt;br /&gt;
&lt;br /&gt;
Also refer to [[LNF:Plasma Physics]].&lt;br /&gt;
&lt;br /&gt;
== Operation ==&lt;br /&gt;
&lt;br /&gt;
* A [[TJ-II:Vacuum system|vacuum system]] controls the pressure inside the vacuum vessel.&lt;br /&gt;
* The electric energy required for a TJ-II discharge is obtained from a [[TJ-II:Power supply|flywheel generator]].&lt;br /&gt;
* The [[TJ-II:Coil system|coils]] are cooled by means of a [[TJ-II:Cooling system|cooling system]].&lt;br /&gt;
* An extensive set of systems is available to perform [[TJ-II:Plasma Wall Interaction|plasma wall conditioning]].&lt;br /&gt;
* Two movable [[TJ-II:Limiter|limiters]] can be used to limit the plasma.&lt;br /&gt;
* A [[TJ-II:Biasing probe|biasing probe]] can be used to apply a bias potential at the edge.&lt;br /&gt;
* A [[TJ-II:Paddle|mechanical paddle]] is used to suppress runaway electrons during current ramp-up and ramp-down.&lt;br /&gt;
&lt;br /&gt;
== Heating and fuelling ==&lt;br /&gt;
&lt;br /&gt;
In order to fuel and heat the TJ-II plasma, the following systems are used: &lt;br /&gt;
* [[TJ-II:Gas puff|Gas puff]]&lt;br /&gt;
* [[TJ-II:Electron Cyclotron Resonant Heating|Electron Cyclotron Resonant Heating]] (ECRH)&lt;br /&gt;
* [[TJ-II:Neutral Beam Injection|Neutral Beam Injection]] (NBI)&lt;br /&gt;
* [[TJ-II:Electron Bernstein Wave Heating|Electron Bernstein Wave Heating]] (EBWH)&lt;br /&gt;
* [[TJ-II:Pellet injector|Pellet injector]] (PI)&lt;br /&gt;
&lt;br /&gt;
== Control and data acquisition ==&lt;br /&gt;
&lt;br /&gt;
The [[TJ-II:Control and data acquisition systems|Control and data acquisition systems]] were designed end developed at CIEMAT.&lt;br /&gt;
&lt;br /&gt;
== Diagnostics ==&lt;br /&gt;
&lt;br /&gt;
[[File:TJ-II_top_view.jpg|400px|thumb|right|TJ-II in 2012; front left: [[TJ-II:Thomson Scattering|Thomson Scattering]]; left and bottom right: [[TJ-II:Neutral Beam Injection|NBI]]; top: the inclined structures are two [[TJ-II:Heavy Ion Beam Probe|HIBP]] systems. Also visible on top, up front, is the reciprocating [[TJ-II:Langmuir Probes|Langmuir Probe]].]]&lt;br /&gt;
&lt;br /&gt;
TJ-II is fitted with an extensive set of diagnostic systems installed in its 96 access [[TJ-II:Ports|ports]] &amp;lt;ref&amp;gt;K. McCarthy and TJ-II team. &#039;&#039;Plasma diagnostic systems and methods used on the stellarator TJ-II&#039;&#039;. [[doi:10.1088/1748-0221/16/12/C12026|Journal of Instrumentation, 16(12):C12026, 2021]].&amp;lt;/ref&amp;gt;. For information on the magnetic coordinate system (required for cross-diagnostic comparisons), see [[TJ-II:Magnetic_coordinates|TJ-II magnetic coordinates]].&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;Passive diagnostics&#039;&#039;&lt;br /&gt;
* [[TJ-II:Magnetics|Magnetics]]&lt;br /&gt;
* [[TJ-II:Halpha monitors|Halpha monitors]]&lt;br /&gt;
* [[TJ-II:Electron Cyclotron Emission|Electron Cyclotron Emission]]&lt;br /&gt;
* [[TJ-II:Soft X-rays|Soft X-rays]]&lt;br /&gt;
* [[TJ-II:Multifilter electron temperature diagnostic|Multifilter electron temperature diagnostic]] &lt;br /&gt;
* [[TJ-II:Bolometry|Bolometry]]&lt;br /&gt;
* [[TJ-II:Spectroscopy|Spectroscopy]]&lt;br /&gt;
* [[TJ-II:Charge exchange spectroscopy|Charge exchange spectroscopy]]&lt;br /&gt;
* [[TJ-II:Compact Neutral Particle Analyzer|Compact Neutral Particle Analyzer]]&lt;br /&gt;
* [[TJ-II:Fast ion loss probe|Fast ion loss probe]]&lt;br /&gt;
* [[TJ-II:Retarding Field Analyzer|Retarding Field Analyzer]]&lt;br /&gt;
* [[TJ-II:Fast camera|Fast camera]]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;Active diagnostics&#039;&#039;&lt;br /&gt;
* [[TJ-II:Interferometry|Interferometry]]&lt;br /&gt;
* [[TJ-II:Reflectometry|Reflectometry]]&lt;br /&gt;
* [[TJ-II:Heavy Ion Beam Probe|Heavy Ion Beam Probe]]&lt;br /&gt;
* [[TJ-II:Langmuir Probes|Langmuir Probes]]&lt;br /&gt;
* [[TJ-II:Thomson Scattering|Thomson Scattering]]&lt;br /&gt;
* [[TJ-II:Diagnostic neutral beam|Diagnostic neutral beam]]&lt;br /&gt;
* [[TJ-II:Helium Beam|Helium Beam]]&lt;br /&gt;
* [[TJ-II:Lithium Beam|Lithium Beam]]&lt;br /&gt;
&lt;br /&gt;
[https://info.fusion.ciemat.es/cgi-bin/TJII_data.cgi Interactive on-line data visualization]&lt;br /&gt;
&lt;br /&gt;
[https://info.fusion.ciemat.es/InternalReport/IR1532.pdf TJ-II Web Services] for remote data access&lt;br /&gt;
&lt;br /&gt;
== Numerical resources ==&lt;br /&gt;
&lt;br /&gt;
=== Simulation codes ===&lt;br /&gt;
* [[VMEC]] - 3D Plasma equilibrium, assuming nested flux surfaces&lt;br /&gt;
* [[PIES]] - 3D Plasma equilibrium&lt;br /&gt;
* [[HL]] - Field line following code&lt;br /&gt;
* [[ASTRA]] - Plasma transport&lt;br /&gt;
* [[PROCTR]] - Plasma transport&lt;br /&gt;
* [[EUTERPE]] - Gyrokinetic code&lt;br /&gt;
* [[EIRENE]] - A Monte Carlo neutral gas transport code&lt;br /&gt;
* [[FAFNER]]&lt;br /&gt;
* [[CUTIE]] - Full-tokamak fluid turbulence&lt;br /&gt;
* [[MOCA]] - Monte Carlo [[Neoclassical transport]] code&lt;br /&gt;
* [[DKES]] - [[Neoclassical transport]] code&lt;br /&gt;
* [[KNOSOS]] - [[Neoclassical transport]] code&lt;br /&gt;
* [[TRECE]] - Microwave ray tracing&lt;br /&gt;
* [[TRUBA]]- Microwave beam/ray tracing including electron Bernstein wave calculations.&lt;br /&gt;
&lt;br /&gt;
=== Data analysis ===&lt;br /&gt;
* [[Wave_ana]] - Linear and non-linear data analysis, spectral analysis using Fourier and Wavelets&lt;br /&gt;
* [[EBITA]] - Tomographic reconstruction&lt;br /&gt;
* [[TJ-II:Tomography|Tomography]] - Tomographic reconstruction based on mode decomposition in flux surface geometry&lt;br /&gt;
&lt;br /&gt;
=== Software tools ===&lt;br /&gt;
* [[MDSplus]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Category:Toroidal confinement devices]]&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Coil_system&amp;diff=8714</id>
		<title>TJ-II:Coil system</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Coil_system&amp;diff=8714"/>
		<updated>2026-10-07T10:17:39Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* See also */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[File:TJ-II_Helical_coil.jpg|400px|thumb|right|The core coil pack consists of three coils: the circular core (CC), the helix 1 (HX1), and the helix 2 (HX2).]] &lt;br /&gt;
&lt;br /&gt;
The [[TJ-II]] coil system is listed in the table below (in [[Toroidal coordinates|cylindrical coordinates]]).&lt;br /&gt;
All coils are circular, except the helical coil. &lt;br /&gt;
They are directly [[TJ-II:Cooling system|cooled]] by water flowing trough longitudinal holes in the conductors. &lt;br /&gt;
All coils have a reinforced structure to avoid mechanical deformations.&amp;lt;ref&amp;gt;M. Medrano, M. Blaumoser, J. Alonso, G. Barrera, M. Pastor, C. Rubio, F. Pedrazo, and O. Heusmann, &#039;&#039;Strength considerations on the magnetic field coils of the Spanish Stellarator TJ-II&#039;&#039;, [[doi:10.1109/FUSION.1993.518529| Fusion Engineering, 15th IEEE/NPSS Symposium (1993)]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Coil&#039;&#039; !! &#039;&#039;Number&#039;&#039; !!&#039;&#039;Size (m)&#039;&#039;!! &#039;&#039;Position (m) &#039;&#039; !! &#039;&#039;Turns&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|Circular (CC) || 1 || &#039;&#039;R&#039;&#039; = 1.5 || &#039;&#039;Z&#039;&#039; = 0 || 24&lt;br /&gt;
|-&lt;br /&gt;
|Helical (HX)&amp;lt;ref&amp;gt;J. Alonso and M. Blaumoser, &#039;&#039;Design and feasibility of the TJ-II hard core&#039;&#039;, [[doi:10.1109/FUSION.1991.218810|Fusion Engineering,  14th IEEE/NPSS Symposium (1991)]]&amp;lt;/ref&amp;gt; || 1 || &#039;&#039;R&#039;&#039; = 1.5 &amp;lt;br&amp;gt; swing = 0.07 || &#039;&#039;Z&#039;&#039; = 0 || 24&lt;br /&gt;
|-&lt;br /&gt;
|Toroidal (TF) || 28 || &#039;&#039;r&#039;&#039; = 0.425 || &#039;&#039;R&#039;&#039; = 1.5 + 0.2825 cos(4&amp;amp;phi;) &amp;lt;/br&amp;gt; &#039;&#039;Z&#039;&#039; = -0.2825 sin(4&amp;amp;phi;) || 8&lt;br /&gt;
|-&lt;br /&gt;
|Toroidal (TF) || 4 || &#039;&#039;r&#039;&#039; = 0.475 || &#039;&#039;R&#039;&#039; = 1.5 + 0.3325 cos(4&amp;amp;phi;) &amp;lt;/br&amp;gt; &#039;&#039;Z&#039;&#039; = -0.3325 sin(4&amp;amp;phi;) &amp;lt;/br&amp;gt; &amp;amp;phi; = 0, 90, 180, 270&amp;amp;deg;|| 9&lt;br /&gt;
|-&lt;br /&gt;
|Vertical (VF) || 2 || &#039;&#039;R&#039;&#039; = 2.25 || &#039;&#039;Z&#039;&#039; = &amp;amp;pm; 0.75 || 16&lt;br /&gt;
|-&lt;br /&gt;
|Compensation (OH) || 2 || &#039;&#039;R&#039;&#039; = 0.78 || &#039;&#039;Z&#039;&#039; = &amp;amp;pm; 0.75 || 20&lt;br /&gt;
|-&lt;br /&gt;
|Compensation (OH) || 2 || &#039;&#039;R&#039;&#039; = 2.29 || &#039;&#039;Z&#039;&#039; = &amp;amp;pm; 0.75 || 1&lt;br /&gt;
|-&lt;br /&gt;
|Radial (R) || 2 || &#039;&#039;R&#039;&#039; = 0.74 || &#039;&#039;Z&#039;&#039; = &amp;amp;pm; 0.75 || 7&lt;br /&gt;
|-&lt;br /&gt;
|Radial (R) || 2 || &#039;&#039;R&#039;&#039; = 2.24 || &#039;&#039;Z&#039;&#039; = &amp;amp;pm; 0.75 || 5&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
The main helical field is produced by the CC, HX, and TF coils.&lt;br /&gt;
The vertical field coils (VF) allow positioning the magnetic axis.&lt;br /&gt;
The ohmic coils (OH) can generate a loop voltage of 0.1 V, intended to cancel spurious toroidal currents.&lt;br /&gt;
The radial coils (R) produce a trimming radial field of up to 100 G, intended to compensate stray fields.&lt;br /&gt;
&lt;br /&gt;
Currents in the coil sets can be controlled in Autonomous Mode (or `A Mode&#039;) or Controlled Mode (or `C mode&#039;)&amp;lt;ref&amp;gt;A. de la Peña, L. Pacios, R. Carrasco, F. Lapayese,&#039;&#039;A real-time current driving control system for the TJ-II coils&#039;&#039;, [[doi:10.1016/j.fusengdes.2008.12.010|Fusion Engineering and Design &#039;&#039;&#039;84&#039;&#039;&#039;, Issues 2–6 (2009) 676-680]]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
[[File:TJ-II_Coils.png|800px|thumb|Center|TJ-II Coils. Red: central. Yellow: helical. Blue: toroidal. Green: vertical. Brown and green: radial.]]&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
* [[TJ-II:Power supply]]&lt;br /&gt;
* [[TJ-II:Magnetic field]]&lt;br /&gt;
* [[TJ-II:Magnetic configuration]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Ports&amp;diff=8713</id>
		<title>TJ-II:Ports</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Ports&amp;diff=8713"/>
		<updated>2026-10-01T08:53:24Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* Segment D8 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The listing below specifies which diagnostics and devices are connected to each port of [[TJ-II]].&lt;br /&gt;
__NOTOC__&lt;br /&gt;
== [[TJ-II:Sectors|Sector A]] ==&lt;br /&gt;
&lt;br /&gt;
90 &amp;amp;le; &amp;amp;phi; &amp;amp;le; 180 &amp;amp;deg;&lt;br /&gt;
&lt;br /&gt;
=== Segment A1 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|A1TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|A1SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|A1BOT|| ||&lt;br /&gt;
|-&lt;br /&gt;
|A1TANG|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment A2 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|A2TOP|| [[TJ-II:Soft_X-rays| Soft X-ray tomography]] ||&lt;br /&gt;
|-&lt;br /&gt;
|A2SIDE|| [[TJ-II:Soft_X-rays| Soft X-ray tomography]] ||&lt;br /&gt;
|-&lt;br /&gt;
|A2BOT|| [[TJ-II:Soft_X-rays| Soft X-ray tomography]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment A3 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|A3SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|A3BOT|| [[TJ-II:Limiter|Limiter]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment A4 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|A4TOP|| [[TJ-II:Reflectometry|AM reflectometer]] (profiles)&amp;lt;br&amp;gt;[[TJ-II:Heavy Ion Beam Probe|Heavy Ion Beam Probe 2]] (injection) ||&lt;br /&gt;
|-&lt;br /&gt;
|A4SIDE|| [[TJ-II:Heavy Ion Beam Probe|Heavy Ion Beam Probe 2]] (spectrometer) ||&lt;br /&gt;
|-&lt;br /&gt;
|A4BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment A5 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|A5TOP|| Vacuum feedthrough connector for the A5 [[TJ-II:Magnetics|Rogowski coil and diamagnetic loop ]]|| &lt;br /&gt;
|-&lt;br /&gt;
|A5SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|A5BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment A6 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|A6TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|A6SIDE|| [[TJ-II:Electron Cyclotron Resonant Heating|ECRH]] (QTL2) ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment A7 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|A7TOP|| [[TJ-II:Biasing probe|Biasing probe]]||&lt;br /&gt;
|-&lt;br /&gt;
|A7SIDE|| [[TJ-II:Charge_exchange_spectroscopy|Charge exchange spectroscopy]] &amp;lt;br&amp;gt; [[TJ-II:Diagnostic neutral beam|Diagnostic neutral beam]]||&lt;br /&gt;
|-&lt;br /&gt;
|A7BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment A8 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|A8TOP||  ||&lt;br /&gt;
|-&lt;br /&gt;
|A8SIDE||  ||&lt;br /&gt;
|-&lt;br /&gt;
|A8BOT||  ||&lt;br /&gt;
|-&lt;br /&gt;
|A8TANG|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== [[TJ-II:Sectors|Sector B]] ==&lt;br /&gt;
&lt;br /&gt;
180 &amp;amp;le; &amp;amp;phi; &amp;amp;le; 270 &amp;amp;deg;&lt;br /&gt;
&lt;br /&gt;
=== Segment B1 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|B1TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|B1SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|B1BOT|| ||&lt;br /&gt;
|-&lt;br /&gt;
|B1TANG|| [[TJ-II:Compact Neutral Particle Analyzer|Compact Neutral Particle Analyzer]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment B2 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|B2TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|B2SIDE|| [[TJ-II:Pellet injector|Pellet injector]] ||&lt;br /&gt;
|-&lt;br /&gt;
|B2BOT|| [[TJ-II:Langmuir Probes|Langmuir Probes]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment B3 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|B3SIDE|| [[TJ-II:Electron Cyclotron Resonant Heating|ECRH]] (QTL1) ||&lt;br /&gt;
|-&lt;br /&gt;
|B3BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment B4 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|B4TOP|| [[TJ-II:Heavy Ion Beam Probe|Heavy Ion Beam Probe 1]] (injection)||&lt;br /&gt;
|-&lt;br /&gt;
|B4SIDE|| [[TJ-II:Heavy Ion Beam Probe|Heavy Ion Beam Probe 1]] (spectrometer) &amp;lt;br&amp;gt;Vacuum feedthrough connector for the B4 [[TJ-II:Magnetics|Rogowski coil and diamagnetic loop]] ||&lt;br /&gt;
|-&lt;br /&gt;
|B4BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment B5 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|B5TOP|| Vacuum feedthrough connector for the second [[TJ-II:Magnetics|Mirnov coil straight vertical array]] ||&lt;br /&gt;
|-&lt;br /&gt;
|B5SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|B5BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment B6 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|B6TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|B6SIDE|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment B7 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|B7TOP|| [[TJ-II:Bolometry|Multichannel Bolometry]] ||&lt;br /&gt;
|-&lt;br /&gt;
|B7SIDE|| [[TJ-II:Bolometry|Multichannel Bolometry]] ||&lt;br /&gt;
|-&lt;br /&gt;
|B7BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment B8 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|B8TOP|| [[TJ-II:Interferometry|Microwave interferometer]] ||&lt;br /&gt;
|-&lt;br /&gt;
|B8SIDE|| [[TJ-II:Spectroscopy|Spectroscopy]] (toroidal rotation) ||&lt;br /&gt;
|-&lt;br /&gt;
|B8BOT|| [[TJ-II:Interferometry|Microwave interferometer]] ||&lt;br /&gt;
|-&lt;br /&gt;
|B8TANG|| [[TJ-II:Fast camera|Fast camera]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== [[TJ-II:Sectors|Sector C]] ==&lt;br /&gt;
&lt;br /&gt;
270 &amp;amp;le; &amp;amp;phi; &amp;amp;le; 360 &amp;amp;deg;&lt;br /&gt;
&lt;br /&gt;
=== Segment C1 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|C1TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|C1SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|C1BOT|| ||&lt;br /&gt;
|-&lt;br /&gt;
|C1TANG|| [[TJ-II:Neutral Beam Injection|NBI 2]]||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment C2 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|C2TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|C2SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|C2BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment C3 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|C3SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|C3BOT|| [[TJ-II:Limiter|Limiter]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment C4 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|C4TOP|| Vacuum feedthrough connector for the first [[TJ-II:Magnetics|Mirnov coil straight vertical array]] ||&lt;br /&gt;
|-&lt;br /&gt;
|C4SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|C4BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment C5 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|C5TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|C5SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|C5BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment C6 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|C6TOP|| [[TJ-II:Reflectometry#Doppler_Reflectometer|Doppler Reflectometer]] (Mirror) || &lt;br /&gt;
|-&lt;br /&gt;
|C6SIDE|| [[TJ-II:Reflectometry#Doppler_Reflectometer|Doppler Reflectometer]] (Antenna) || &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment C7 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|C7TOP|| [[TJ-II:Lithium Beam|Lithium Beam]]||&lt;br /&gt;
|-&lt;br /&gt;
|C7SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|C7BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment C8 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|C8TOP|| [[TJ-II:Helium Beam|Helium Beam]] ||&lt;br /&gt;
|-&lt;br /&gt;
|C8SIDE|| [[TJ-II:Helium Beam|Helium Beam]] ||&lt;br /&gt;
|-&lt;br /&gt;
|C8BOT|| [[TJ-II:Helium Beam|Helium Beam]] ||&lt;br /&gt;
|-&lt;br /&gt;
|C8TANG|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== [[TJ-II:Sectors|Sector D]] ==&lt;br /&gt;
&lt;br /&gt;
0 &amp;amp;le; &amp;amp;phi; &amp;amp;le; 90 &amp;amp;deg;&lt;br /&gt;
&lt;br /&gt;
=== Segment D1 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|D1TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D1SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D1BOT|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D1TANG|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment D2 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|D2TOP|| [[TJ-II:Thomson Scattering|Thomson Scattering]] (laser view dump) ||&lt;br /&gt;
|-&lt;br /&gt;
|D2SIDE|| [[TJ-II:Thomson Scattering|Thomson Scattering]] (polychromator) ||&lt;br /&gt;
|-&lt;br /&gt;
|D2BOT|| [[TJ-II:Thomson Scattering|Thomson Scattering]] (laser entry)||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment D3 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|D3SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D3BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment D4 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|D4TOP|| [[TJ-II:Langmuir Probes|Langmuir probe]] ||&lt;br /&gt;
|-&lt;br /&gt;
|D4SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D4BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment D5 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|D5TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D5SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D5BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment D6 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|D6TOP|| [[TJ-II:Electron_Bernstein_Wave_Heating|Bernstein Wave Heating]] (mirror) ||&lt;br /&gt;
|-&lt;br /&gt;
|D6SIDE|| [[TJ-II:Electron_Bernstein_Wave_Heating|Bernstein Wave Heating]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment D7 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|D7TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D7SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D7BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment D8 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|D8TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D8SIDE|| [[TJ-II:Spectroscopy|Spectroscopy]] (toroidal rotation) ||&lt;br /&gt;
|-&lt;br /&gt;
|D8BOT|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D8TANG|| [[TJ-II:Neutral Beam Injection|NBI 1]]||&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Ports&amp;diff=8712</id>
		<title>TJ-II:Ports</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Ports&amp;diff=8712"/>
		<updated>2026-10-01T08:53:06Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* Segment C1 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The listing below specifies which diagnostics and devices are connected to each port of [[TJ-II]].&lt;br /&gt;
__NOTOC__&lt;br /&gt;
== [[TJ-II:Sectors|Sector A]] ==&lt;br /&gt;
&lt;br /&gt;
90 &amp;amp;le; &amp;amp;phi; &amp;amp;le; 180 &amp;amp;deg;&lt;br /&gt;
&lt;br /&gt;
=== Segment A1 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|A1TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|A1SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|A1BOT|| ||&lt;br /&gt;
|-&lt;br /&gt;
|A1TANG|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment A2 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|A2TOP|| [[TJ-II:Soft_X-rays| Soft X-ray tomography]] ||&lt;br /&gt;
|-&lt;br /&gt;
|A2SIDE|| [[TJ-II:Soft_X-rays| Soft X-ray tomography]] ||&lt;br /&gt;
|-&lt;br /&gt;
|A2BOT|| [[TJ-II:Soft_X-rays| Soft X-ray tomography]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment A3 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|A3SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|A3BOT|| [[TJ-II:Limiter|Limiter]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment A4 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|A4TOP|| [[TJ-II:Reflectometry|AM reflectometer]] (profiles)&amp;lt;br&amp;gt;[[TJ-II:Heavy Ion Beam Probe|Heavy Ion Beam Probe 2]] (injection) ||&lt;br /&gt;
|-&lt;br /&gt;
|A4SIDE|| [[TJ-II:Heavy Ion Beam Probe|Heavy Ion Beam Probe 2]] (spectrometer) ||&lt;br /&gt;
|-&lt;br /&gt;
|A4BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment A5 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|A5TOP|| Vacuum feedthrough connector for the A5 [[TJ-II:Magnetics|Rogowski coil and diamagnetic loop ]]|| &lt;br /&gt;
|-&lt;br /&gt;
|A5SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|A5BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment A6 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|A6TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|A6SIDE|| [[TJ-II:Electron Cyclotron Resonant Heating|ECRH]] (QTL2) ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment A7 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|A7TOP|| [[TJ-II:Biasing probe|Biasing probe]]||&lt;br /&gt;
|-&lt;br /&gt;
|A7SIDE|| [[TJ-II:Charge_exchange_spectroscopy|Charge exchange spectroscopy]] &amp;lt;br&amp;gt; [[TJ-II:Diagnostic neutral beam|Diagnostic neutral beam]]||&lt;br /&gt;
|-&lt;br /&gt;
|A7BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment A8 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|A8TOP||  ||&lt;br /&gt;
|-&lt;br /&gt;
|A8SIDE||  ||&lt;br /&gt;
|-&lt;br /&gt;
|A8BOT||  ||&lt;br /&gt;
|-&lt;br /&gt;
|A8TANG|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== [[TJ-II:Sectors|Sector B]] ==&lt;br /&gt;
&lt;br /&gt;
180 &amp;amp;le; &amp;amp;phi; &amp;amp;le; 270 &amp;amp;deg;&lt;br /&gt;
&lt;br /&gt;
=== Segment B1 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|B1TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|B1SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|B1BOT|| ||&lt;br /&gt;
|-&lt;br /&gt;
|B1TANG|| [[TJ-II:Compact Neutral Particle Analyzer|Compact Neutral Particle Analyzer]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment B2 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|B2TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|B2SIDE|| [[TJ-II:Pellet injector|Pellet injector]] ||&lt;br /&gt;
|-&lt;br /&gt;
|B2BOT|| [[TJ-II:Langmuir Probes|Langmuir Probes]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment B3 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|B3SIDE|| [[TJ-II:Electron Cyclotron Resonant Heating|ECRH]] (QTL1) ||&lt;br /&gt;
|-&lt;br /&gt;
|B3BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment B4 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|B4TOP|| [[TJ-II:Heavy Ion Beam Probe|Heavy Ion Beam Probe 1]] (injection)||&lt;br /&gt;
|-&lt;br /&gt;
|B4SIDE|| [[TJ-II:Heavy Ion Beam Probe|Heavy Ion Beam Probe 1]] (spectrometer) &amp;lt;br&amp;gt;Vacuum feedthrough connector for the B4 [[TJ-II:Magnetics|Rogowski coil and diamagnetic loop]] ||&lt;br /&gt;
|-&lt;br /&gt;
|B4BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment B5 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|B5TOP|| Vacuum feedthrough connector for the second [[TJ-II:Magnetics|Mirnov coil straight vertical array]] ||&lt;br /&gt;
|-&lt;br /&gt;
|B5SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|B5BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment B6 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|B6TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|B6SIDE|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment B7 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|B7TOP|| [[TJ-II:Bolometry|Multichannel Bolometry]] ||&lt;br /&gt;
|-&lt;br /&gt;
|B7SIDE|| [[TJ-II:Bolometry|Multichannel Bolometry]] ||&lt;br /&gt;
|-&lt;br /&gt;
|B7BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment B8 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|B8TOP|| [[TJ-II:Interferometry|Microwave interferometer]] ||&lt;br /&gt;
|-&lt;br /&gt;
|B8SIDE|| [[TJ-II:Spectroscopy|Spectroscopy]] (toroidal rotation) ||&lt;br /&gt;
|-&lt;br /&gt;
|B8BOT|| [[TJ-II:Interferometry|Microwave interferometer]] ||&lt;br /&gt;
|-&lt;br /&gt;
|B8TANG|| [[TJ-II:Fast camera|Fast camera]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== [[TJ-II:Sectors|Sector C]] ==&lt;br /&gt;
&lt;br /&gt;
270 &amp;amp;le; &amp;amp;phi; &amp;amp;le; 360 &amp;amp;deg;&lt;br /&gt;
&lt;br /&gt;
=== Segment C1 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|C1TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|C1SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|C1BOT|| ||&lt;br /&gt;
|-&lt;br /&gt;
|C1TANG|| [[TJ-II:Neutral Beam Injection|NBI 2]]||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment C2 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|C2TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|C2SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|C2BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment C3 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|C3SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|C3BOT|| [[TJ-II:Limiter|Limiter]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment C4 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|C4TOP|| Vacuum feedthrough connector for the first [[TJ-II:Magnetics|Mirnov coil straight vertical array]] ||&lt;br /&gt;
|-&lt;br /&gt;
|C4SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|C4BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment C5 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|C5TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|C5SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|C5BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment C6 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|C6TOP|| [[TJ-II:Reflectometry#Doppler_Reflectometer|Doppler Reflectometer]] (Mirror) || &lt;br /&gt;
|-&lt;br /&gt;
|C6SIDE|| [[TJ-II:Reflectometry#Doppler_Reflectometer|Doppler Reflectometer]] (Antenna) || &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment C7 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|C7TOP|| [[TJ-II:Lithium Beam|Lithium Beam]]||&lt;br /&gt;
|-&lt;br /&gt;
|C7SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|C7BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment C8 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|C8TOP|| [[TJ-II:Helium Beam|Helium Beam]] ||&lt;br /&gt;
|-&lt;br /&gt;
|C8SIDE|| [[TJ-II:Helium Beam|Helium Beam]] ||&lt;br /&gt;
|-&lt;br /&gt;
|C8BOT|| [[TJ-II:Helium Beam|Helium Beam]] ||&lt;br /&gt;
|-&lt;br /&gt;
|C8TANG|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== [[TJ-II:Sectors|Sector D]] ==&lt;br /&gt;
&lt;br /&gt;
0 &amp;amp;le; &amp;amp;phi; &amp;amp;le; 90 &amp;amp;deg;&lt;br /&gt;
&lt;br /&gt;
=== Segment D1 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|D1TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D1SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D1BOT|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D1TANG|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment D2 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|D2TOP|| [[TJ-II:Thomson Scattering|Thomson Scattering]] (laser view dump) ||&lt;br /&gt;
|-&lt;br /&gt;
|D2SIDE|| [[TJ-II:Thomson Scattering|Thomson Scattering]] (polychromator) ||&lt;br /&gt;
|-&lt;br /&gt;
|D2BOT|| [[TJ-II:Thomson Scattering|Thomson Scattering]] (laser entry)||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment D3 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|D3SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D3BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment D4 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|D4TOP|| [[TJ-II:Langmuir Probes|Langmuir probe]] ||&lt;br /&gt;
|-&lt;br /&gt;
|D4SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D4BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment D5 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|D5TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D5SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D5BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment D6 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|D6TOP|| [[TJ-II:Electron_Bernstein_Wave_Heating|Bernstein Wave Heating]] (mirror) ||&lt;br /&gt;
|-&lt;br /&gt;
|D6SIDE|| [[TJ-II:Electron_Bernstein_Wave_Heating|Bernstein Wave Heating]] ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment D7 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|D7TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D7SIDE|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D7BOT|| ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== Segment D8 ===&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Port&#039;&#039; !!&#039;&#039;Diagnostic or device&#039;&#039;!!&#039;&#039;Comment&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|D8TOP|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D8SIDE|| [[TJ-II:Spectroscopy|Spectroscopy]] (toroidal rotation) ||&lt;br /&gt;
|-&lt;br /&gt;
|D8BOT|| ||&lt;br /&gt;
|-&lt;br /&gt;
|D8TANG|| [[TJ-II:Neutral Beam Injection|NBI 2]]||&lt;br /&gt;
|}&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=User:Admin&amp;diff=8711</id>
		<title>User:Admin</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=User:Admin&amp;diff=8711"/>
		<updated>2026-09-29T07:32:19Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* &amp;amp;ge; 2020 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[File:BvM.jpg|right|]]&lt;br /&gt;
== Personal information ==&lt;br /&gt;
__NOTOC__&lt;br /&gt;
* Boudewijn van Milligen (Admin)&lt;br /&gt;
* Researcher at: &amp;lt;br&amp;gt;[[Laboratorio Nacional de Fusión]] - [[CIEMAT]] &amp;lt;br&amp;gt;Avda. Complutense 40, Edif. 66&amp;lt;br&amp;gt;28040 Madrid, España - Spain&lt;br /&gt;
* Tel. +34 - 914 962 682&lt;br /&gt;
* Email boudewijn.vanmilligen (at) ciemat.es&lt;br /&gt;
User profiles:&lt;br /&gt;
* [https://publons.com/researcher/1248698/boudewijn-ph-van-milligen/ Publons] (ResearcherID H-5121-2015)&lt;br /&gt;
* [http://orcid.org/0000-0001-5344-6274 ORCID 0000-0001-5344-6274]&lt;br /&gt;
* [https://www.scopus.com/authid/detail.uri?authorId=35476190300 Scopus AuthorID 35476190300]&lt;br /&gt;
* [http://scholar.google.com/citations?user=7z9Cr9oAAAAJ Google Scholar]&lt;br /&gt;
* [https://www.researchgate.net/profile/Boudewijn_Van_Milligen/ ResearchGate]&lt;br /&gt;
&lt;br /&gt;
== Interests ==&lt;br /&gt;
&lt;br /&gt;
* Fusion and plasma physics&lt;br /&gt;
** [[H-mode|L-H transition]], Zonal Flows&lt;br /&gt;
** [[Magnetic island]]s, MHD activity&lt;br /&gt;
* [[Anomalous transport]]&lt;br /&gt;
** Turbulence&lt;br /&gt;
** Continuous Time Random Walks&lt;br /&gt;
* Data analysis&lt;br /&gt;
** [[Causality detection]]&lt;br /&gt;
** [[Intermittence]]&lt;br /&gt;
** [[:Wikipedia:Rescaled range|Rescaled range]] or [[:Wikipedia:Hurst exponent|Hurst]] analysis&lt;br /&gt;
** [[Bayesian data analysis]]&lt;br /&gt;
** [[Biorthogonal decomposition]]&lt;br /&gt;
** [[Bicoherence]]&lt;br /&gt;
** [[TJ-II:Tomography|Tomography]]&lt;br /&gt;
&lt;br /&gt;
== Book ==&lt;br /&gt;
&lt;br /&gt;
B.Ph. van Milligen and R. Sánchez, &#039;&#039;Analysis of Turbulence in Fusion Plasmas&#039;&#039;, [[doi:10.1088/978-0-7503-4856-0|IOP Publishing (2022)]], {{ISBN|978-0-7503-4854-6}}&lt;br /&gt;
&lt;br /&gt;
== Selected publications ==&lt;br /&gt;
&lt;br /&gt;
(inverse chronological order)&lt;br /&gt;
=== &amp;amp;ge; 2020 ===&lt;br /&gt;
* Boudewijn Ph. van Milligen, Isabel García-Cortés, Kieran J. McCarthy, et al. &#039;&#039;The pump-out effect as a trigger for the electron to ion root transition in TJ-II&#039;&#039;. [[doi:10.3390/plasma9040039|Plasma, 9(4), 2026]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. van Milligen, I. Voldiner, E. de la Cal, A. Alonso Alvarez, I. Luiz Caldas and Z. Guimarães Filho, &#039;&#039;Turbulence analysis with the spectroscopic gas puff imaging diagnostic in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/1361-6587/ae92b5|Plasma Phys. Control. Fusion &#039;&#039;&#039;68&#039;&#039;&#039; (2026) 085018]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* A. Alonso Alvarez, B. P. Van Milligen, I. Voldiner, I. L. Caldas, Z. Guimarães Filho, O. Kozachok, and A. Chmyga. &#039;&#039;Edge turbulence dynamics across electron–ion root transitions during ECRH modulation experiments in the TJ-II stellarator&#039;&#039;. [[doi:10.1088/1361-6587/ae7470|Plasma Phys. Control. Fusion, &#039;&#039;&#039;68&#039;&#039;&#039; (2026) 065019]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. van Milligen, I. García-Cortés, K.J. McCarthy, et al, &#039;&#039;The rotational transform and enhanced confinement in the TJ-II stellarator&#039;&#039;, [[doi:10.1017/S0022377825100433|Journal of Plasma Physics &#039;&#039;&#039;91&#039;&#039;&#039;, 4 (2025) E98]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* Boudewijn Philip van Milligen, Teresa Estrada, Benjamin Carreras, Luis García, and TJ-II Team. &#039;&#039;Importance of the Rotational Transform for L–H Transitions in the TJ-II Stellarator&#039;&#039; [[doi:10.3390/plasma7020024|Plasma &#039;&#039;&#039;7&#039;&#039;&#039;, no. 2 (2024) 446-464]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. van Milligen, I. Voldiner, B.A. Carreras, L. García, M.A. Ochando and The TJ-II Team, &#039;&#039;Rational surfaces, flows and radial structure in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/1741-4326/aca688|Nucl. Fusion &#039;&#039;&#039;63&#039;&#039;&#039; (2023) 016027]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. Van Milligen, B.A. Carreras, L. Garcia, G. Grenfell, I. Voldiner and C. Hidalgo, &#039;&#039;The impact of radial electric fields and plasma rotation on intermittence in TJ-II&#039;&#039;, [[doi:10.1088/1361-6587/ac54e9|Plasma Phys. Control. Fusion &#039;&#039;&#039;64&#039;&#039;&#039;, 5 (2022) 055006]] ([http://documenta.ciemat.es/handle/123456789/2290 repository])&lt;br /&gt;
* B. van Milligen, A. Melnikov, B. Carreras, L. Garcia, A. Kozachek, C. Hidalgo, J. de Pablos, Ph. Khabanov, L. Eliseev, M. Drabinskij, A. Chmyga, L. Krupnik, the HIBP Team, the TJ-II Team, &#039;&#039;Topology of 2-D turbulent structures based on intermittence in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/1741-4326/ac27c9|Nucl. Fusion &#039;&#039;&#039;61&#039;&#039;&#039;, 11 (2021) 116063]] ([http://documenta.ciemat.es/handle/123456789/2281 repository])&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras, I. Voldiner, U. Losada, C. Hidalgo, and the TJ-II Team, &#039;&#039;Causality, intermittence and crossphase evolution during confinement transitions in the TJ-II stellarator&#039;&#039;, [[doi:10.1063/5.0057791|Phys. Plasmas &#039;&#039;&#039;28&#039;&#039;&#039; (2021) 092302]] ([http://documenta.ciemat.es/handle/123456789/2289 repository])&lt;br /&gt;
* B.Ph. van Milligen, B. Carreras, L. García and C. Hidalgo, &#039;&#039;The localization of low order rational surfaces based on the intermittence parameter in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/1741-4326/ab79cc|Nucl. Fusion &#039;&#039;&#039;60&#039;&#039;&#039; (2020) 056010]] ([http://documenta.ciemat.es/handle/123456789/2291 repository])&lt;br /&gt;
&lt;br /&gt;
=== 2010-2019 ===&lt;br /&gt;
* B.Ph. van Milligen, B. Carreras, L. García and J. Nicolau, &#039;&#039;The radial propagation of heat in strongly driven non-equilibrium fusion plasmas&#039;&#039;, [[doi:10.3390/e21020148|Entropy, &#039;&#039;&#039;21&#039;&#039;&#039;, 2 (2019) 148]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. van Milligen, B. Carreras, E. de la Luna and E. Solano, &#039;&#039;Radial variation of heat transport in L-mode JET discharges&#039;&#039; [[doi:10.1088/1741-4326/ab03e1|Nucl. Fusion, &#039;&#039;&#039;59&#039;&#039;&#039; (2019) 056006]] ([http://documenta.ciemat.es/handle/123456789/2292 repository])&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras, C. Hidalgo, Á. Cappa and the TJ-II Team, &#039;&#039;A possible mechanism for confinement power degradation in the TJ-II stellarator&#039;&#039;, [[doi:10.1063/1.5029881|Phys. Plasmas &#039;&#039;&#039;25&#039;&#039;&#039; (2018) 062503]] ([http://documenta.ciemat.es/handle/123456789/2308 repository])&lt;br /&gt;
* B.Ph. van Milligen, U. Hoefel, J. Nicolau, M. Hirsch, L. García, B. Carreras, C. Hidalgo and the W7-X Team, &#039;&#039;Study of radial heat transport in W7-X using the transfer entropy&#039;&#039;, [[doi:10.1088/1741-4326/aabf5d|Nucl. Fusion &#039;&#039;&#039;58&#039;&#039;&#039; (2018) 076002]] ([http://hdl.handle.net/10016/32565 repository])&lt;br /&gt;
* B.Ph. van Milligen, J. Hernández Nicolau, B. Liu, G. Grenfell, U. Losada, B. Carreras, L. Garcia and C. Hidalgo, &#039;&#039;Filaments in the edge confinement region of TJ-II&#039;&#039;, [[doi:10.1088/1741-4326/aa9db6|Nucl. Fusion &#039;&#039;&#039;58&#039;&#039;&#039; (2018) 026030]] ([http://hdl.handle.net/10016/32563 repository])&lt;br /&gt;
* B.Ph. van Milligen, J.H. Nicolau, L. García, B.A. Carreras, C. Hidalgo and the TJ-II Team, &#039;&#039;The impact of rational surfaces on radial heat transport in TJ-II&#039;&#039;, [[doi:10.1088/1741-4326/aa611f|Nucl. Fusion &#039;&#039;&#039;57&#039;&#039;&#039;, 5 (2017) 056028]], [https://arxiv.org/abs/1701.04574 arxiv:1701.04574]&lt;br /&gt;
* B.Ph. van Milligen, T. Estrada, B.A. Carreras, E. Ascasíbar, C. Hidalgo, I. Pastor, J.M. Fontdecaba, R. Balbín and the TJ-II Team, &#039;&#039;The causal impact of magnetic fluctuations in slow and fast L–H transitions at TJ-II&#039;&#039;, [[doi:10.1063/1.4958807|Phys. Plasmas &#039;&#039;&#039;23&#039;&#039;&#039; (2016) 072305]], [https://arxiv.org/abs/1512.06525 arxiv:1512.06525]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras, L. García, A. Martín de Aguilera, C. Hidalgo, J.H. Nicolau and the TJ-II Team, &#039;&#039;The causal relation between turbulent particle flux and density gradient&#039;&#039;, [[doi:10.1063/1.4958806|Phys. Plasmas &#039;&#039;&#039;23&#039;&#039;&#039; (2016) 072307]]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras and D.E. Newman, &#039;&#039;Constructing criteria to diagnose the likelihood of extreme events in the case of the electric power grid&#039;&#039;, [[doi:10.1063/1.4943569|Chaos &#039;&#039;&#039;26&#039;&#039;&#039; (2016) 033109]]&lt;br /&gt;
* B.Ph. van Milligen, T. Estrada, L. García, D. López-Bruna, B. Carreras, Y. Xu, M. Ochando, C. Hidalgo, J. Reynolds-Barredo and A. López-Fraguas, &#039;&#039;The role of magnetic islands in modifying long range temporal correlations of density fluctuations and local heat transport&#039;&#039;, [[doi:10.1088/0029-5515/56/1/016013|Nucl. Fusion, &#039;&#039;&#039;56&#039;&#039;&#039;, 1 (2016) 016013]], [https://arxiv.org/abs/1506.06890 arxiv:1506.06890]&lt;br /&gt;
* B.Ph. van Milligen, E. Sánchez, A. Alonso, M.A. Pedrosa, C. Hidalgo, A. Martín de Aguilera, A. López Fraguas, &#039;&#039;The use of the Biorthogonal Decomposition for the identification of zonal flows at TJ-II&#039;&#039;, [[doi:10.1088/0741-3335/57/2/025005|Plasma Phys. Control. Fusion &#039;&#039;&#039;57&#039;&#039;&#039;, 2 (2015) 025005]], [https://arxiv.org/abs/1408.1845 arxiv:1408.1845]&lt;br /&gt;
* B.Ph. van Milligen, P.D. Bons, &#039;&#039;Simplified numerical model for clarifying scaling behavior in the intermediate dispersion regime in homogeneous porous media&#039;&#039;, [[doi:10.1016/j.cpc.2014.09.006|Comput. Phys. Commun. &#039;&#039;&#039;185&#039;&#039;&#039; (2014) 3291]], [https://arxiv.org/abs/1409.2724 arxiv:1409.2724]&lt;br /&gt;
* B.Ph. van Milligen, G. Birkenmeier, M. Ramisch, T. Estrada, C. Hidalgo and A. Alonso, &#039;&#039;Causality detection and turbulence in fusion plasmas&#039;&#039;, [[doi:10.1088/0029-5515/54/2/023011|Nucl. Fusion &#039;&#039;&#039;54&#039;&#039;&#039; (2014), 023011]], [https://arxiv.org/abs/1309.7769 arxiv:1309.7769]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Parallel and perpendicular turbulence correlation length in the TJ-II Stellarator&#039;&#039;, [[doi:10.1088/0029-5515/53/9/093025|Nucl. Fusion &#039;&#039;&#039;53&#039;&#039;&#039; (2013) 093025]], [https://arxiv.org/abs/1306.1395 arxiv:1306.1395]&lt;br /&gt;
* P.D. Bons, B.Ph. van Milligen, P. Blum, &#039;&#039;A general unified expression for solute and heat dispersion in homogeneous porous media&#039;&#039;, [[doi:10.1002/wrcr.20488|Water Resour. Res. &#039;&#039;&#039;49&#039;&#039;&#039; (2013) 1]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Spatiotemporal and wavenumber resolved bicoherence at the low to high confinement transition in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/53/11/113034|Nucl. Fusion &#039;&#039;&#039;53&#039;&#039;&#039; (2013) 113034]], [https://arxiv.org/abs/1211.0420 arxiv:1211.0420]&lt;br /&gt;
* B. Ph. van Milligen, R. Sánchez and C. Hidalgo, &#039;&#039;Relevance of Uncorrelated Lorentzian Pulses for the Interpretation of Turbulence in the Edge of Magnetically Confined Toroidal Plasmas&#039;&#039;, [[doi:10.1103/PhysRevLett.109.105001|Phys. Rev. Lett. &#039;&#039;&#039;109&#039;&#039;&#039; (2012) 105001]], [https://arxiv.org/abs/1204.6185 arxiv:1204.6185]&lt;br /&gt;
* B.Ph. van Milligen, P.D. Bons, &#039;&#039;Analytical model for tracer dispersion in porous media&#039;&#039;, [[doi:10.1103/PhysRevE.85.011306|Phys. Rev. E 85 (2012) 011306]], [https://arxiv.org/abs/1111.6512 arxiv:1111.6512]&lt;br /&gt;
* B.Ph. van Milligen, L. García, B.A. Carreras, M.A. Pedrosa, C. Hidalgo, J.A. Alonso, T. Estrada and E. Ascasíbar, &#039;&#039;MHD mode activity and the velocity shear layer at TJ-II&#039;&#039;, [[doi:10.1088/0029-5515/52/1/013006|Nucl. Fusion &#039;&#039;&#039;52&#039;&#039;&#039; (2012) 013006]]&lt;br /&gt;
* B.Ph. van Milligen, T. Estrada, E. Ascasíbar, et al, &#039;&#039;Integrated data analysis at TJ-II: the density profile&#039;&#039;, [[doi:10.1063/1.3608551|Rev. Sci. Instrum. &#039;&#039;&#039;82&#039;&#039;&#039; (2011) 073503]]&lt;br /&gt;
* B.A. Carreras et al., &#039;&#039;Reconstruction of intermittent waveforms associated with the zonal flow at the transition leading to the edge shear flow layer&#039;&#039;, [[doi:10.1088/0029-5515/51/5/053022|Nucl. Fusion &#039;&#039;&#039;51&#039;&#039;&#039; (2011) 053022]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;A global resonance phenomenon at the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/51/1/013005|Nucl. Fusion &#039;&#039;&#039;51&#039;&#039;&#039; (2011) 013005]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;The dynamics of the formation of the edge particle transport barrier at TJ-II&#039;&#039;, [[doi:10.1088/0029-5515/51/11/113002|Nucl. Fusion &#039;&#039;&#039;51&#039;&#039;&#039; (2011) 113002]]&lt;br /&gt;
&lt;br /&gt;
=== 2000-2009 ===&lt;br /&gt;
* B.Ph. van Milligen, I. Calvo and R. Sánchez, &#039;&#039;Continuous time random walks in finite domains and general boundary conditions: some formal considerations&#039;&#039;, [[doi:10.1088/1751-8113/41/21/215004|J. Phys. A: Math. Theor. &#039;&#039;&#039;41&#039;&#039;&#039; (2008) 215004]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Quantifying profile stiffness&#039;&#039;, [http://www.jspf.or.jp/PFR/PFR_articles/pfr2008S1/pfr2008_03-S1070.html Plasma and Fusion Research, &#039;&#039;&#039;3&#039;&#039;&#039; (2008) S1070]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Bicoherence during confinement transitions in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/48/11/115003|Nucl. Fusion &#039;&#039;&#039;48&#039;&#039;&#039; (2008) 115003]]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras, V.E. Lynch and R. Sánchez, &#039;&#039;Pulse propagation in a simple probabilistic transport model&#039;&#039;, [[doi:10.1088/0029-5515/47/3/004|Nucl. Fusion &#039;&#039;&#039;47&#039;&#039;&#039; (2007) 189]]&lt;br /&gt;
* B.Ph. van Milligen, P.D. Bons, B.A. Carreras and R. Sánchez, &#039;&#039;On the applicability of Fick&#039;s Law to diffusion in inhomogeneous systems&#039;&#039;, [[doi:10.1088/0143-0807/26/5/023|Eur. J. Phys. &#039;&#039;&#039;26&#039;&#039;&#039; (2005) 913]]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras and R. Sánchez, &#039;&#039;The foundations of diffusion revisited&#039;&#039;, [[doi:10.1088/0741-3335/47/12B/S56|Plasma Phys. Control. Fusion &#039;&#039;&#039;47&#039;&#039;&#039; (2005) B743]]&lt;br /&gt;
* B.Ph. Van Milligen et al, &#039;&#039;Additional evidence for the universality of turbulent fluctuations and fluxes in the scrape-off layer region of fusion plasmas&#039;&#039;, [[doi:10.1063/1.1884615|Phys. Plasmas &#039;&#039;&#039;12&#039;&#039;&#039; (2005) 052507]]&lt;br /&gt;
* B.Ph. van Milligen, R. Sánchez and B.A. Carreras, &#039;&#039;Probabilistic finite-size transport models for fusion: anomalous transport and scaling laws&#039;&#039;, [[doi:10.1063/1.1701893|Phys. Plasmas &#039;&#039;&#039;11&#039;&#039;&#039;, 5 (2004) 2272]]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras and R. Sánchez, &#039;&#039;Uphill transport and the probabilistic transport model&#039;&#039;, [[doi:10.1063/1.1763915|Phys. Plasmas &#039;&#039;&#039;11&#039;&#039;&#039;, 3787 (2004)]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Revision of TV Thomson scattering data analysis and detection of profile structure&#039;&#039;, [[doi:10.1063/1.1597951|Rev. Sci. Instrum. &#039;&#039;&#039;74&#039;&#039;&#039; (2003) 3998]]&lt;br /&gt;
* B.Ph. van Milligen, E. de la Luna, F.L. Tabarés, et al., &#039;&#039;Ballistic transport phenomena in TJ-II&#039;&#039;, [[doi:10.1088/0029-5515/42/7/301|Nucl. Fusion &#039;&#039;&#039;42&#039;&#039;&#039; (2002) 787]]&lt;br /&gt;
=== 1990 - 1999 ===&lt;br /&gt;
* B.A. Carreras, B.Ph. van Milligen, et al, &#039;&#039;Experimental evidence of long-range correlation and self-similarity in plasma fluctuations&#039;&#039;, [[doi:10.1063/1.873490|Phys. Plasmas &#039;&#039;&#039;6&#039;&#039;&#039;, 5 (1999) 1885]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Statistically robust linear and non-linear wavelet analysis applied to plasma edge turbulence&#039;&#039;, [[doi:10.1063/1.1147727|Rev. Sci. Instrum. &#039;&#039;&#039;68&#039;&#039;&#039; (1997) 967]]&lt;br /&gt;
* B.Ph. van Milligen, V. Tribaldos, J.A. Jiménez, &#039;&#039;A neural network differential equation and plasma equilibrium solver&#039;&#039;, [[doi:10.1103/PhysRevLett.75.3594|Phys. Rev. Lett. &#039;&#039;&#039;75&#039;&#039;&#039; (1995) 3594]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Nonlinear phenomena and intermittency in plasma turbulence&#039;&#039;, [[doi:10.1103/PhysRevLett.74.395|Phys. Rev. Lett. &#039;&#039;&#039;74&#039;&#039;&#039;, 3 (1995) 395]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Wavelet bicoherence: a new turbulence analysis tool&#039;&#039;, [[doi:10.1063/1.871199|Phys. Plasmas &#039;&#039;&#039;2&#039;&#039;&#039;, 8 (1995) 3017]]&lt;br /&gt;
* B.Ph. van Milligen and A. Lopez Fraguas, &#039;&#039;Expansion of vacuum magnetic fields in toroidal harmonics&#039;&#039;, [[doi:10.1016/0010-4655(94)90112-0|Comput. Phys. Commun. &#039;&#039;&#039;81&#039;&#039;&#039;, Issues 1-2 (1994) 74-90]]&lt;br /&gt;
* B.Ph. van Milligen, A.C.A.P. van Lammeren, N.J. Lopes Cardozo, F.C. Schüller and M. Verreck, &#039;&#039;Gradients of electron temperature and density across m=2 islands in RTP&#039;&#039;, [[doi:10.1088/0029-5515/33/8/I03|Nucl. Fusion &#039;&#039;&#039;33&#039;&#039;&#039; (1993) 1119]]&lt;br /&gt;
* B.Ph. van Milligen, N.J. Lopes Cardozo, &#039;&#039;Function Parametrization: a fast inverse mapping method&#039;&#039;, [[doi:10.1016/0010-4655(91)90073-T|Comput. Phys. Commun. &#039;&#039;&#039;66&#039;&#039;&#039; (1991) 243]]&lt;br /&gt;
* B.Ph. van Milligen et al., &#039;&#039;Application of Function Parametrization to the analysis of polarimetry and interferometry data in TEXTOR&#039;&#039;, [[doi:10.1088/0029-5515/31/2/007|Nucl. Fusion &#039;&#039;&#039;31&#039;&#039;&#039; (1991) 309]]&lt;br /&gt;
* B.Ph. van Milligen, &#039;&#039;Exact relations between multipole moments of the flux and moments of the toroidal current density in tokamaks&#039;&#039;, [[doi:10.1088/0029-5515/30/1/012|Nucl. Fusion &#039;&#039;&#039;30&#039;&#039;&#039; (1990) 157]]&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=EBITA&amp;diff=8710</id>
		<title>EBITA</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=EBITA&amp;diff=8710"/>
		<updated>2026-09-24T08:27:06Z</updated>

		<summary type="html">&lt;p&gt;Admin: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;EBITA is a tomographic reconstruction program.&lt;br /&gt;
&amp;lt;ref&amp;gt;A. P. Navarro, M. A. Ochando and A. Weller, &#039;&#039;Equilibrium-based iterative tomography technique for soft X-ray in stellarators&#039;&#039;, [[doi:10.1109/27.90321|IEEE Trans. Plasma Sci. &#039;&#039;&#039;19&#039;&#039;&#039; (1991) 569]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Software]]&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=File:TJ-II_Helium_beam.png&amp;diff=8709</id>
		<title>File:TJ-II Helium beam.png</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=File:TJ-II_Helium_beam.png&amp;diff=8709"/>
		<updated>2026-09-22T09:10:56Z</updated>

		<summary type="html">&lt;p&gt;Admin: Admin uploaded a new version of File:TJ-II Helium beam.png&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Diagram of the TJ-II Helium beam diagnostic&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Bolometry&amp;diff=8703</id>
		<title>TJ-II:Bolometry</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Bolometry&amp;diff=8703"/>
		<updated>2026-09-19T12:32:38Z</updated>

		<summary type="html">&lt;p&gt;Admin: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[File:TJ-II_Bolometer.png|400px|thumb|right|The TJ-II bolometry system for tomographic reconstruction ([[TJ-II:Sectors|sector]] B7, &amp;amp;phi; = 255.5 &amp;amp;deg;)]]&lt;br /&gt;
&lt;br /&gt;
TJ-II has several bolometry systems&lt;br /&gt;
&amp;lt;ref&amp;gt;M.A. Ochando et al., &#039;&#039;Up-Down and In-Out Asymmetry Monitoring Based on Broadband Radiation Detectors&#039;&#039;, [http://www.new.ans.org/pubs/journals/fst/a_1252 Fusion Sci. Technol. &#039;&#039;&#039;50&#039;&#039;&#039;, 313 (2006)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;B. Zurro et al, &#039;&#039;Method to deduce local impurity transport quantities from the evolution of tomographically reconstructed bolometer signals during tracer injection at TJ-II&#039;&#039;, [[doi:10.1063/1.1787585|Rev. Sci. Instrum. &#039;&#039;&#039;75&#039;&#039;&#039; (2004) 4231]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
:&lt;br /&gt;
* Three 20-channel pinhole cameras in [[TJ-II:Sectors|sector]] B7, monitoring the same poloidal section and used for tomographic reconstructions &amp;lt;ref&amp;gt;[[EBITA]]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;[[TJ-II:Tomography]]&amp;lt;/ref&amp;gt; of the total plasma emissivity. &amp;lt;ref&amp;gt;E. Barrera et al, &#039;&#039;Real-time data acquisition and parallel data processing solution for TJ-II Bolometer arrays diagnostic&#039;&#039;, [[doi:10.1016/j.fusengdes.2006.04.046|Fusion Engineering and Design &#039;&#039;&#039;81&#039;&#039;&#039;, Issues 15-17 (2006) 1863-1867]]&amp;lt;/ref&amp;gt; Signal names in the [[TJ-II:Shot_database|TJ-II database]]: &#039;BO101&#039; ... &#039;BO120&#039;, &#039;BO201&#039; ... &#039;BO220&#039;, &#039;BO301&#039; ... &#039;BO320&#039;.&lt;br /&gt;
* Three 16-channel cameras in [[TJ-II:Sectors|sectors]] A7, C2, D7. Signal names in the [[TJ-II:Shot_database|TJ-II database]]: &#039;ABOL1&#039; ... &#039;ABOL16&#039;, &#039;CBOL1&#039; ... &#039;CBOL16&#039;, &#039;DBOL1&#039; ... &#039;DBOL16&#039;. &lt;br /&gt;
* Six global bolometry monitors. Signal names in the [[TJ-II:Shot_database|TJ-II database]]: &#039;BOL1&#039;, &#039;BOL3&#039;, &#039;BOL6&#039;; &#039;BOL2&#039;, &#039;BOL5&#039;, &#039;BOL7&#039;.&lt;br /&gt;
&lt;br /&gt;
Bolometry has been used to classify radiation profiles into two categories: &#039;bell&#039; and &#039;dome&#039;, related to impurity concentration inside the plasma. &#039;Bell&#039;-type profiles are more robust against radiative collapse&amp;lt;ref&amp;gt;F.L. Tabarés et al, &#039;&#039;Plasma performance and confinement in the TJ-II stellarator with lithium-coated walls&#039;&#039;, [[doi:10.1088/0741-3335/50/12/124051|Plasma Phys. Control. Fusion 50 (2008) 124051]]&amp;lt;/ref&amp;gt; &lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Soft_X-rays&amp;diff=8699</id>
		<title>TJ-II:Soft X-rays</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Soft_X-rays&amp;diff=8699"/>
		<updated>2026-09-12T08:13:50Z</updated>

		<summary type="html">&lt;p&gt;Admin: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Multichannel Soft X-Ray system ==&lt;br /&gt;
&lt;br /&gt;
[[File:TJ-II_Soft-X_array.jpg|400px|thumb|right|TJ-II Soft X-Ray camera array]]&lt;br /&gt;
&lt;br /&gt;
The [[TJ-II]] multichannel soft X-ray system consists of 5 cameras with 16 channels each,&lt;br /&gt;
allowing tomographic reconstruction of the plasma emissions (using the [[EBITA]] code).&lt;br /&gt;
&amp;lt;ref&amp;gt;F. Medina et al, &#039;&#039;X-ray diagnostic systems for the TJ–II flexible heliac&#039;&#039;, [[doi:10.1063/1.1149517|Rev. Sci. Instrum. &#039;&#039;&#039;70&#039;&#039;&#039; (1999) 642]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;F. Medina et al, &#039;&#039;Filamentary current detection in stellarator plasmas&#039;&#039;, [[doi:10.1063/1.1310579|Rev. Sci. Instrum. &#039;&#039;&#039;72&#039;&#039;&#039; (2001) 471]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;F. Medina, M.A. Ochando, A. Baciero, J. Guasp, &#039;&#039;Characterization of ripple-trapped suprathermal electron losses by their bremsstrahlung emission in the soft x-ray range at the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0741-3335/49/4/003|Plasma Phys. Control. Fusion &#039;&#039;&#039;49&#039;&#039;&#039; (2007) 385]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The system is located in [[TJ-II:Sectors|sector]] A2, at &amp;amp;phi; = 104.5&amp;amp;deg;.&lt;br /&gt;
The signals are stored in the [[TJ-II:Shot database|TJ-II database]] with the names &#039;RXxyy&#039;, where &#039;x&#039; = 1,...,5 (corresponding to the five arrays) and &#039;yy&#039; = 01,...,16 (corresponding to the 16 channels).&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[TJ-II:Multifilter electron temperature diagnostic]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=FusionWiki:Current_events&amp;diff=8696</id>
		<title>FusionWiki:Current events</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=FusionWiki:Current_events&amp;diff=8696"/>
		<updated>2026-09-07T11:44:48Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* 2027 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Upcoming Fusion and Plasma events ==&lt;br /&gt;
&lt;br /&gt;
Please feel free to add events.&lt;br /&gt;
&lt;br /&gt;
=== 2026 ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;width: 100%&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | Date (2026)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | Location&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;60%&amp;quot; | Conference/Meeting&lt;br /&gt;
|-&lt;br /&gt;
| February 24-25 || Barcelona, Spain || [https://hpcfusion.bsc.es/2026/about/ Fusion HPC Workshop]&lt;br /&gt;
|-&lt;br /&gt;
| April 20-24 || Córdoba, Spain || [https://ishw2026.com  25&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; International Stellarator and Heliotron Workshop] (ISHW)&lt;br /&gt;
|-&lt;br /&gt;
| June 8-12 || Kudowa-Zdrój, Poland || [http://kudowaschool.ipplm.pl/ 18&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; Kudowa Summer School &#039;Towards Fusion Energy&#039;]&lt;br /&gt;
|-&lt;br /&gt;
| June 15-18 || Prague, Czech Republic || [http://www.plasmaconference.cz/  31&amp;lt;sup&amp;gt;st&amp;lt;/sup&amp;gt; Symposium on Plasma Physics and Technology] (SPPT)&lt;br /&gt;
|-&lt;br /&gt;
| June 29-July 3 || Edinburgh, Scotland (UK) || [https://epsplasma2026.com/ 2026 European Physical Society Conference on Plasma Physics] (EPS-CPP)&lt;br /&gt;
|-&lt;br /&gt;
| September 8-11 || Seoul, Korea || 20&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; International Workshop on H-mode Physics and Transport Barriers (H-Mode Workshop 2026)&lt;br /&gt;
|-&lt;br /&gt;
| September 14-18 || Eindhoven, The Netherlands || [https://www.differ.nl/isla-9 9&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; International Symposium on Liquid Metal Applications for Fusion] (ISLA-9)&lt;br /&gt;
|-&lt;br /&gt;
| October 11-16 || Busan, Korea || [http://aappsdpp.org/AAPPSDPPF/ 10&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; Asia-Pacific Conference on Plasma Physics] (AAPPS-DPP2026)&lt;br /&gt;
|-&lt;br /&gt;
| October 13-15 || Madrid, Spain || [https://ifmif-dones.es/dones-updates/the-4th-dones-users-workshop/ 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; DONES User Workshop]&lt;br /&gt;
|-&lt;br /&gt;
| October 13-15 || Viterbo, Italy || [https://indico.fusenet.eu/event/66/overview FuseNet PhD Event]&lt;br /&gt;
|-&lt;br /&gt;
| October 20-23 || Hefei, China || [https://conferences.iaea.org/event/452/program 3&amp;lt;sup&amp;gt;rd&amp;lt;/sup&amp;gt; technical meeting on long-pulse operation of fusion devices]&lt;br /&gt;
|-&lt;br /&gt;
| November 15-20 || Seville, Spain || [https://istw2026.psft.eu 23&amp;lt;sup&amp;gt;rd&amp;lt;/sup&amp;gt; International Spherical Torus Workshop] (ISTW 2026)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== 2027 ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;width: 100%&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | Date (2026)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | Location&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;60%&amp;quot; | Conference/Meeting&lt;br /&gt;
|-&lt;br /&gt;
| February 15-19 || Nagoya, Japan || [https://lhdws2027.nifs.ac.jp/ International LHD Workshop] (LHDWS 2027)&lt;br /&gt;
|-&lt;br /&gt;
| July 5-9 || Lausanne, Switzerland || [https://epsplasma2027.epfl.ch/ European Physical Society Conference on Plasma Physics] (EPS 2027)&lt;br /&gt;
|-&lt;br /&gt;
| September 7-10 || Tromsø, Norway || [https://uit.no/tavla/artikkel/936431/31th_eu-us_transport_task_force_workshop 31&amp;lt;sup&amp;gt;st&amp;lt;/sup&amp;gt; EU-US Transport Task Force Workshop] (TTF 2027)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Periodic meetings ==&lt;br /&gt;
&lt;br /&gt;
The following FusionWiki entries attempt to both provide a record of historic meetings and direct links to proceedings:&lt;br /&gt;
* The [[IAEA Fusion Energy Conference]] (FEC)&lt;br /&gt;
* The [[European Physical Society Conference on Plasma Physics]] (EPS-CPP)&lt;br /&gt;
* The [[European Conference on Plasma Diagnostics]] (ECPD)&lt;br /&gt;
* The [[International Congress on Plasma Physics]] (ICPP)&lt;br /&gt;
* The [https://engage.aps.org/dpp/meetings/annual-meeting Annual Meeting of the Division of Plasma Physics of the American Physical Society] (APS-DPP)&lt;br /&gt;
* The [[https://www.aappsdpp.org/AAPPSDPPF/Meetings.html  Asia-Pacific Conference on Plasma Physics AAPPS-DPP]&lt;br /&gt;
* The [[International Stellarator and Heliotron Workshop]] (ISHW)&lt;br /&gt;
* The [[European Fusion Theory Conference]] (EFTC)&lt;br /&gt;
* The [[Conference on Plasma Surface Interactions]] (PSI)&lt;br /&gt;
* The [[Symposium on Fusion Technology]] (SOFT)&lt;br /&gt;
* The [[Symposium On Fusion Engineering]] (SOFE)&lt;br /&gt;
* The [[EU-US Transport Task Force Meeting]] (TTF)&lt;br /&gt;
* The [[International Toki Conference]] (ITC)&lt;br /&gt;
* The [[Topical Conference on High Temperature Plasma Diagnostics]] (HTPD)&lt;br /&gt;
* The [http://www.sherwoodtheory.org/ Sherwood Theory Conference]&lt;br /&gt;
* The [[International Conference on Tritium Science and Technology]] (TRITIUM)&lt;br /&gt;
* The [[International Symposium on Fusion Nuclear Technology]] (ISFNT)&lt;br /&gt;
* The [[Coordinated Working Group Meeting]] (CWGM)&lt;br /&gt;
* The [http://varenna-lausanne.epfl.ch/ Theory of Fusion Plasmas: Joint Varenna-Lausanne International Workshop] (Varenna-Lausanne even years)&lt;br /&gt;
* The International Conference on Fusion Reactor Materials (ICFRM)&lt;br /&gt;
&lt;br /&gt;
See also [[:Category:Conferences]].&lt;br /&gt;
&lt;br /&gt;
== Meeting lists at other sites ==&lt;br /&gt;
&lt;br /&gt;
* [http://ieee-npss.org/directory-of-plasma-conferences/ IEEE Nuclear and Plasma Sciences Society Directory of Plasma Conferences].&lt;br /&gt;
* [https://www.iter.org/conferences Calendar maintained at ITER of upcoming conferences on fusion science, fusion technology, plasma physics and energy].&lt;br /&gt;
* [https://www-amdis.iaea.org/w/index.php/Calendar_of_Meetings Calendar maintained by IAEA Atomic and Molecular Data Unit of meetings related to A+M+PMI processes and data for fusion].&lt;br /&gt;
* [http://fusenet.eu/events Calendar maintained by the European Fusion Education Network (FuseNet) of upcoming fusion related events].&lt;br /&gt;
* [http://crpp.epfl.ch/conferences_e Calendar maintained at Centre de Recherches en Physique des Plasmas, EPFL, of conferences on plasma physics research].&lt;br /&gt;
* [http://www.conference-service.com/conferences/plasma-and-gas-discharge-physics.html COMS Conferences and Meetings on Plasma and Gas-discharge Physics].&lt;br /&gt;
* [http://fire.pppl.gov/meetings_fusion.htm Calendar maintained at Fire, PPPL, of fusion meetings].&lt;br /&gt;
* [http://www.jspf.or.jp/calendar/cldrb.html Plasma and Fusion Calendar maintained by the Japan Society of Plasma Science and Nuclear Fusion Research].&lt;br /&gt;
* [https://burningplasma.org/newsandevents/?article=enews&amp;amp;issue=current Calendar maintained by the United States Burning Plasma Organization (USBPO) of fusion energy events].&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=FusionWiki:Current_events&amp;diff=8695</id>
		<title>FusionWiki:Current events</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=FusionWiki:Current_events&amp;diff=8695"/>
		<updated>2026-09-04T17:15:18Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* 2027 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Upcoming Fusion and Plasma events ==&lt;br /&gt;
&lt;br /&gt;
Please feel free to add events.&lt;br /&gt;
&lt;br /&gt;
=== 2026 ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;width: 100%&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | Date (2026)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | Location&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;60%&amp;quot; | Conference/Meeting&lt;br /&gt;
|-&lt;br /&gt;
| February 24-25 || Barcelona, Spain || [https://hpcfusion.bsc.es/2026/about/ Fusion HPC Workshop]&lt;br /&gt;
|-&lt;br /&gt;
| April 20-24 || Córdoba, Spain || [https://ishw2026.com  25&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; International Stellarator and Heliotron Workshop] (ISHW)&lt;br /&gt;
|-&lt;br /&gt;
| June 8-12 || Kudowa-Zdrój, Poland || [http://kudowaschool.ipplm.pl/ 18&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; Kudowa Summer School &#039;Towards Fusion Energy&#039;]&lt;br /&gt;
|-&lt;br /&gt;
| June 15-18 || Prague, Czech Republic || [http://www.plasmaconference.cz/  31&amp;lt;sup&amp;gt;st&amp;lt;/sup&amp;gt; Symposium on Plasma Physics and Technology] (SPPT)&lt;br /&gt;
|-&lt;br /&gt;
| June 29-July 3 || Edinburgh, Scotland (UK) || [https://epsplasma2026.com/ 2026 European Physical Society Conference on Plasma Physics] (EPS-CPP)&lt;br /&gt;
|-&lt;br /&gt;
| September 8-11 || Seoul, Korea || 20&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; International Workshop on H-mode Physics and Transport Barriers (H-Mode Workshop 2026)&lt;br /&gt;
|-&lt;br /&gt;
| September 14-18 || Eindhoven, The Netherlands || [https://www.differ.nl/isla-9 9&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; International Symposium on Liquid Metal Applications for Fusion] (ISLA-9)&lt;br /&gt;
|-&lt;br /&gt;
| October 11-16 || Busan, Korea || [http://aappsdpp.org/AAPPSDPPF/ 10&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; Asia-Pacific Conference on Plasma Physics] (AAPPS-DPP2026)&lt;br /&gt;
|-&lt;br /&gt;
| October 13-15 || Madrid, Spain || [https://ifmif-dones.es/dones-updates/the-4th-dones-users-workshop/ 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; DONES User Workshop]&lt;br /&gt;
|-&lt;br /&gt;
| October 13-15 || Viterbo, Italy || [https://indico.fusenet.eu/event/66/overview FuseNet PhD Event]&lt;br /&gt;
|-&lt;br /&gt;
| October 20-23 || Hefei, China || [https://conferences.iaea.org/event/452/program 3&amp;lt;sup&amp;gt;rd&amp;lt;/sup&amp;gt; technical meeting on long-pulse operation of fusion devices]&lt;br /&gt;
|-&lt;br /&gt;
| November 15-20 || Seville, Spain || [https://istw2026.psft.eu 23&amp;lt;sup&amp;gt;rd&amp;lt;/sup&amp;gt; International Spherical Torus Workshop] (ISTW 2026)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== 2027 ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;width: 100%&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | Date (2026)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | Location&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;60%&amp;quot; | Conference/Meeting&lt;br /&gt;
|-&lt;br /&gt;
| February 15-19 || Nagoya, Japan || [https://lhdws2027.nifs.ac.jp/ International LHD Workshop] (LHDWS 2027)&lt;br /&gt;
|-&lt;br /&gt;
| September 7-10 || Tromsø, Norway || [https://uit.no/tavla/artikkel/936431/31th_eu-us_transport_task_force_workshop 31&amp;lt;sup&amp;gt;st&amp;lt;/sup&amp;gt; EU-US Transport Task Force Workshop] (TTF 2027)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Periodic meetings ==&lt;br /&gt;
&lt;br /&gt;
The following FusionWiki entries attempt to both provide a record of historic meetings and direct links to proceedings:&lt;br /&gt;
* The [[IAEA Fusion Energy Conference]] (FEC)&lt;br /&gt;
* The [[European Physical Society Conference on Plasma Physics]] (EPS-CPP)&lt;br /&gt;
* The [[European Conference on Plasma Diagnostics]] (ECPD)&lt;br /&gt;
* The [[International Congress on Plasma Physics]] (ICPP)&lt;br /&gt;
* The [https://engage.aps.org/dpp/meetings/annual-meeting Annual Meeting of the Division of Plasma Physics of the American Physical Society] (APS-DPP)&lt;br /&gt;
* The [[https://www.aappsdpp.org/AAPPSDPPF/Meetings.html  Asia-Pacific Conference on Plasma Physics AAPPS-DPP]&lt;br /&gt;
* The [[International Stellarator and Heliotron Workshop]] (ISHW)&lt;br /&gt;
* The [[European Fusion Theory Conference]] (EFTC)&lt;br /&gt;
* The [[Conference on Plasma Surface Interactions]] (PSI)&lt;br /&gt;
* The [[Symposium on Fusion Technology]] (SOFT)&lt;br /&gt;
* The [[Symposium On Fusion Engineering]] (SOFE)&lt;br /&gt;
* The [[EU-US Transport Task Force Meeting]] (TTF)&lt;br /&gt;
* The [[International Toki Conference]] (ITC)&lt;br /&gt;
* The [[Topical Conference on High Temperature Plasma Diagnostics]] (HTPD)&lt;br /&gt;
* The [http://www.sherwoodtheory.org/ Sherwood Theory Conference]&lt;br /&gt;
* The [[International Conference on Tritium Science and Technology]] (TRITIUM)&lt;br /&gt;
* The [[International Symposium on Fusion Nuclear Technology]] (ISFNT)&lt;br /&gt;
* The [[Coordinated Working Group Meeting]] (CWGM)&lt;br /&gt;
* The [http://varenna-lausanne.epfl.ch/ Theory of Fusion Plasmas: Joint Varenna-Lausanne International Workshop] (Varenna-Lausanne even years)&lt;br /&gt;
* The International Conference on Fusion Reactor Materials (ICFRM)&lt;br /&gt;
&lt;br /&gt;
See also [[:Category:Conferences]].&lt;br /&gt;
&lt;br /&gt;
== Meeting lists at other sites ==&lt;br /&gt;
&lt;br /&gt;
* [http://ieee-npss.org/directory-of-plasma-conferences/ IEEE Nuclear and Plasma Sciences Society Directory of Plasma Conferences].&lt;br /&gt;
* [https://www.iter.org/conferences Calendar maintained at ITER of upcoming conferences on fusion science, fusion technology, plasma physics and energy].&lt;br /&gt;
* [https://www-amdis.iaea.org/w/index.php/Calendar_of_Meetings Calendar maintained by IAEA Atomic and Molecular Data Unit of meetings related to A+M+PMI processes and data for fusion].&lt;br /&gt;
* [http://fusenet.eu/events Calendar maintained by the European Fusion Education Network (FuseNet) of upcoming fusion related events].&lt;br /&gt;
* [http://crpp.epfl.ch/conferences_e Calendar maintained at Centre de Recherches en Physique des Plasmas, EPFL, of conferences on plasma physics research].&lt;br /&gt;
* [http://www.conference-service.com/conferences/plasma-and-gas-discharge-physics.html COMS Conferences and Meetings on Plasma and Gas-discharge Physics].&lt;br /&gt;
* [http://fire.pppl.gov/meetings_fusion.htm Calendar maintained at Fire, PPPL, of fusion meetings].&lt;br /&gt;
* [http://www.jspf.or.jp/calendar/cldrb.html Plasma and Fusion Calendar maintained by the Japan Society of Plasma Science and Nuclear Fusion Research].&lt;br /&gt;
* [https://burningplasma.org/newsandevents/?article=enews&amp;amp;issue=current Calendar maintained by the United States Burning Plasma Organization (USBPO) of fusion energy events].&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=EU-US_Transport_Task_Force_Meeting&amp;diff=8694</id>
		<title>EU-US Transport Task Force Meeting</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=EU-US_Transport_Task_Force_Meeting&amp;diff=8694"/>
		<updated>2026-09-04T17:13:27Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* List of conferences */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The joint EU-US TTF meeting or workshop is held alternately in the USA and in Europe.&lt;br /&gt;
Its focus is on transport in magnetized plasmas, covering theory, experiment, and modeling aspects.&lt;br /&gt;
&lt;br /&gt;
In the period 2003-2005, the logical enumeration of the workshop was disrupted.&lt;br /&gt;
&lt;br /&gt;
== List of conferences ==&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Number&#039;&#039; !!&#039;&#039;Denomination&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|1|| 1&amp;lt;sup&amp;gt;st&amp;lt;/sup&amp;gt; (1994) Göteborg, Sweden&lt;br /&gt;
|-&lt;br /&gt;
|2|| 2&amp;lt;sup&amp;gt;nd&amp;lt;/sup&amp;gt; (1995) Marina del Rey, USA&lt;br /&gt;
|-&lt;br /&gt;
|3|| 3&amp;lt;sup&amp;gt;rd&amp;lt;/sup&amp;gt; (1996) Varenna, Italy &amp;lt;ref&amp;gt;J.W. Connor, C. Hidalgo, A. Jacchia, F. Romanelli, and U. Stroth, &#039;&#039;EU - US Workshop on Transport in Fusion Plasmas&#039;&#039;, [[doi:10.1088/0741-3335/39/4/007|Plasma Phys. Control. Fusion &#039;&#039;&#039;39&#039;&#039;&#039; (1997) 609]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|4|| 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (1997) Madison, USA&lt;br /&gt;
|-&lt;br /&gt;
|5|| 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (1998) Göteborg, Sweden &amp;lt;ref&amp;gt;J.W. Connor, P. Buratti, J.G. Cordey, C. Hidalgo, A. Jacchia, U. Stroth, and W. Suttrop, &#039;&#039;EU-US workshop on transport in fusion plasmas&#039;&#039;, [[doi:10.1088/0741-3335/41/5/601|Plasma Phys. Control. Fusion &#039;&#039;&#039;41&#039;&#039;&#039; (1999) 693]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|6|| [http://www-internal.psfc.mit.edu/ttf/1999/portland-meeting.html 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (1999) Portland, USA] &amp;lt;ref&amp;gt;Combined with the 12&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; annual US TTF Meeting&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|7|| [http://www.ifp.cnr.it/conference/EU-US_TTF.Varenna.Sept.2000/index.html 7&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2000) Varenna, Italy]&lt;br /&gt;
|-&lt;br /&gt;
|8|| [http://ffden-2.phys.uaf.edu/ttf.2001/index.htm 8&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2001) Fairbanks, Alaska, USA] &amp;lt;ref&amp;gt;Combined with the 14&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; annual US TTF Meeting&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|9|| [https://info.fusion.ciemat.es/ttf2002 9&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2002) Córdoba, Spain] &amp;lt;ref&amp;gt;J.W. Connor, X. Garbet, L. Giannone, M. Greenwald, C. Hidalgo, A. Loarte, and P. Mantica, &#039;&#039;EU-US transport task force workshop on transport in fusion plasmas: transport near operational limits&#039;&#039;, [[doi:10.1088/0741-3335/45/4/310|Plasma Phys. Control. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2003) 455]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|10|| [http://www.psfc.mit.edu/ttf/2003/meeting.html 9&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2003) Madison, USA] &amp;lt;ref&amp;gt;Combined with the 16&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; annual US TTF Meeting&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|11|| [http://www.ifp.cnr.it/conference/TTF04/index.htm 10&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2004) Varenna, Italy] &amp;lt;ref&amp;gt;J.W. Connor, X. Garbet, A.L. Rogister, M. Romanelli, and F. Ryter, &#039;&#039;EU–US workshop on transport in fusion plasmas&#039;&#039;, [[doi:10.1088/0741-3335/47/6/013|Plasma Phys. Control. Fusion &#039;&#039;&#039;47&#039;&#039;&#039; (2005) 941]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|12|| [http://www.mfescience.org/TTF2005/ 10&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2005) Napa, California, USA] &amp;lt;ref&amp;gt;Combined with the 18&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; annual US TTF Meeting&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|13|| [http://www-fusion-magnetique.cea.fr/ttf2006/index.htm 11&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2006) Marseille, France] &amp;lt;ref&amp;gt;J.W. Connor, C. Angioni, P.H. Diamond, G.W. Hammett, C. Hidalgo, A. Loarte, and P. Mantica, &#039;&#039;11th EU-US Transport Task Force workshop on transport in fusion plasmas&#039;&#039;, [[doi:10.1088/0029-5515/47/4/014|Nucl. Fusion &#039;&#039;&#039;47&#039;&#039;&#039; (2007) 361]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|14|| [http://fusion.gat.com/conferences/ttf/ 12&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2007) San Diego, USA]&lt;br /&gt;
|-&lt;br /&gt;
|15|| [http://www.risoe.dk/conferences/EUUS_TtF.aspx 13&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2008) Copenhagen, Denmark] &amp;lt;ref&amp;gt;Combined with the 1&amp;lt;sup&amp;gt;st&amp;lt;/sup&amp;gt; [[EFDA]] Transport Topical Group Meeting&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;J.W. Connor, A. Fasoli, C. Hidalgo, A. Kirk, V. Naulin, A.G. Peeters, and T. Tala, &#039;&#039;13th EU–US Transport Task Force Workshop on transport in fusion plasmas&#039;&#039;, [[doi:10.1088/0029-5515/49/4/047001|Nucl. Fusion &#039;&#039;&#039;49&#039;&#039;&#039; (2009) 047001]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|16|| [http://ttf2009.ucsd.edu/ 14&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2009) San Diego, USA]&lt;br /&gt;
|-&lt;br /&gt;
|17|| [https://info.fusion.ciemat.es/ttg2010 15&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2010) Córdoba, Spain] &amp;lt;ref&amp;gt;Combined with the 3&amp;lt;sup&amp;gt;rd&amp;lt;/sup&amp;gt; [[EFDA]] Transport Topical Group Meeting&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|18|| [http://ttf2011.pppl.gov/ 16&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2011) San Diego, USA]&lt;br /&gt;
|-&lt;br /&gt;
|19|| [http://www.igi.cnr.it/eu_us_ttf_2012/ 17&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2012) Padua, Italy] &amp;lt;ref&amp;gt;Combined with the 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; [[EFDA]] Transport Topical Group Meeting&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|20|| [http://ttf2013.ucsd.edu 18&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2013) Santa Rosa, CA, USA]&lt;br /&gt;
|-&lt;br /&gt;
|21|| [http://www.ttf2014.org/ 19&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2014) Abingdon, UK]&amp;lt;ref&amp;gt;The meeting at [http://ttf2014.ucsd.edu/TTF_2014/Home.html San Antonio, Texas, USA] is a US TTF meeing, not a Joint EU-US meeting - in spite of the announcement!&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;C. Angioni, P. Mantica, V. Naulin et al., &#039;&#039;Summary of the 19th Joint EU-US Transport Task Force Workshop&#039;&#039;, [[doi:10.1088/0029-5515/55/6/067001|Nucl. Fusion &#039;&#039;&#039;55&#039;&#039;&#039;, 6 (2015) 067001]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|22|| [http://www.psfc.mit.edu/TTF2015/index.html 20&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2015) Salem, MA, USA]&lt;br /&gt;
|-&lt;br /&gt;
|23|| [http://spc.epfl.ch/ttf16 21&amp;lt;sup&amp;gt;st&amp;lt;/sup&amp;gt; (2016) Leysin, Switzerland]&lt;br /&gt;
|-&lt;br /&gt;
|24 || [https://fusion.gat.com/conferences/ttf17/ 22&amp;lt;sup&amp;gt;nd&amp;lt;/sup&amp;gt; (2017) Williamsburg, VA, USA]&lt;br /&gt;
|-&lt;br /&gt;
|25 || [http://www.psft.eu/ttf2018/ 23&amp;lt;sup&amp;gt;rd&amp;lt;/sup&amp;gt; (2018) Seville, Spain]&lt;br /&gt;
|-&lt;br /&gt;
|26 || [https://sites.google.com/ucsd.edu/ttf2019/ 24&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2019) Austin, TX, USA]&lt;br /&gt;
|-&lt;br /&gt;
|27 || [https://www.york.ac.uk/physics/ypi/conferencesevents/25thjointeu-ustransporttaskforcemeeting/ 25&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2020) York, UK]&amp;lt;ref&amp;gt;The 2020 Meeting was postponed to 2021 in view of the coronavirus crisis.&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|28 || [https://ttf2023.sciencesconf.org/ 27&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2023) Nancy, France]&lt;br /&gt;
|-&lt;br /&gt;
|29 || [https://ttf2025.ek.hun-ren.hu/ 29&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2025) Budapest, Hungary]&lt;br /&gt;
|-&lt;br /&gt;
|30 || [https://sites.google.com/psfc.mit.edu/usttf2026/home 30&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2026) Salem, MA, USA]&lt;br /&gt;
|-&lt;br /&gt;
|31 || [https://uit.no/tavla/artikkel/936431/31th_eu-us_transport_task_force_workshop 31&amp;lt;sup&amp;gt;st&amp;lt;/sup&amp;gt; (2027) Tromsø, Norway]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Notes and references ==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Category:Conferences]]&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=FusionWiki:Current_events&amp;diff=8693</id>
		<title>FusionWiki:Current events</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=FusionWiki:Current_events&amp;diff=8693"/>
		<updated>2026-09-04T17:04:09Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* 2027 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Upcoming Fusion and Plasma events ==&lt;br /&gt;
&lt;br /&gt;
Please feel free to add events.&lt;br /&gt;
&lt;br /&gt;
=== 2026 ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;width: 100%&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | Date (2026)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | Location&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;60%&amp;quot; | Conference/Meeting&lt;br /&gt;
|-&lt;br /&gt;
| February 24-25 || Barcelona, Spain || [https://hpcfusion.bsc.es/2026/about/ Fusion HPC Workshop]&lt;br /&gt;
|-&lt;br /&gt;
| April 20-24 || Córdoba, Spain || [https://ishw2026.com  25&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; International Stellarator and Heliotron Workshop] (ISHW)&lt;br /&gt;
|-&lt;br /&gt;
| June 8-12 || Kudowa-Zdrój, Poland || [http://kudowaschool.ipplm.pl/ 18&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; Kudowa Summer School &#039;Towards Fusion Energy&#039;]&lt;br /&gt;
|-&lt;br /&gt;
| June 15-18 || Prague, Czech Republic || [http://www.plasmaconference.cz/  31&amp;lt;sup&amp;gt;st&amp;lt;/sup&amp;gt; Symposium on Plasma Physics and Technology] (SPPT)&lt;br /&gt;
|-&lt;br /&gt;
| June 29-July 3 || Edinburgh, Scotland (UK) || [https://epsplasma2026.com/ 2026 European Physical Society Conference on Plasma Physics] (EPS-CPP)&lt;br /&gt;
|-&lt;br /&gt;
| September 8-11 || Seoul, Korea || 20&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; International Workshop on H-mode Physics and Transport Barriers (H-Mode Workshop 2026)&lt;br /&gt;
|-&lt;br /&gt;
| September 14-18 || Eindhoven, The Netherlands || [https://www.differ.nl/isla-9 9&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; International Symposium on Liquid Metal Applications for Fusion] (ISLA-9)&lt;br /&gt;
|-&lt;br /&gt;
| October 11-16 || Busan, Korea || [http://aappsdpp.org/AAPPSDPPF/ 10&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; Asia-Pacific Conference on Plasma Physics] (AAPPS-DPP2026)&lt;br /&gt;
|-&lt;br /&gt;
| October 13-15 || Madrid, Spain || [https://ifmif-dones.es/dones-updates/the-4th-dones-users-workshop/ 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; DONES User Workshop]&lt;br /&gt;
|-&lt;br /&gt;
| October 13-15 || Viterbo, Italy || [https://indico.fusenet.eu/event/66/overview FuseNet PhD Event]&lt;br /&gt;
|-&lt;br /&gt;
| October 20-23 || Hefei, China || [https://conferences.iaea.org/event/452/program 3&amp;lt;sup&amp;gt;rd&amp;lt;/sup&amp;gt; technical meeting on long-pulse operation of fusion devices]&lt;br /&gt;
|-&lt;br /&gt;
| November 15-20 || Seville, Spain || [https://istw2026.psft.eu 23&amp;lt;sup&amp;gt;rd&amp;lt;/sup&amp;gt; International Spherical Torus Workshop] (ISTW 2026)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== 2027 ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;width: 100%&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | Date (2026)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | Location&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;60%&amp;quot; | Conference/Meeting&lt;br /&gt;
|-&lt;br /&gt;
| February 15-19 || Nagoya, Japan || [https://lhdws2027.nifs.ac.jp/ International LHD Workshop] (LHDWS 2027)&lt;br /&gt;
|-&lt;br /&gt;
| September 7-10 || Tromsø, Norway || [https://uit.no/tavla/artikkel/936431/31th_eu-us_transport_task_force_workshop 30&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; EU-US Transport Task Force Workshop] (TTF 2027)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Periodic meetings ==&lt;br /&gt;
&lt;br /&gt;
The following FusionWiki entries attempt to both provide a record of historic meetings and direct links to proceedings:&lt;br /&gt;
* The [[IAEA Fusion Energy Conference]] (FEC)&lt;br /&gt;
* The [[European Physical Society Conference on Plasma Physics]] (EPS-CPP)&lt;br /&gt;
* The [[European Conference on Plasma Diagnostics]] (ECPD)&lt;br /&gt;
* The [[International Congress on Plasma Physics]] (ICPP)&lt;br /&gt;
* The [https://engage.aps.org/dpp/meetings/annual-meeting Annual Meeting of the Division of Plasma Physics of the American Physical Society] (APS-DPP)&lt;br /&gt;
* The [[https://www.aappsdpp.org/AAPPSDPPF/Meetings.html  Asia-Pacific Conference on Plasma Physics AAPPS-DPP]&lt;br /&gt;
* The [[International Stellarator and Heliotron Workshop]] (ISHW)&lt;br /&gt;
* The [[European Fusion Theory Conference]] (EFTC)&lt;br /&gt;
* The [[Conference on Plasma Surface Interactions]] (PSI)&lt;br /&gt;
* The [[Symposium on Fusion Technology]] (SOFT)&lt;br /&gt;
* The [[Symposium On Fusion Engineering]] (SOFE)&lt;br /&gt;
* The [[EU-US Transport Task Force Meeting]] (TTF)&lt;br /&gt;
* The [[International Toki Conference]] (ITC)&lt;br /&gt;
* The [[Topical Conference on High Temperature Plasma Diagnostics]] (HTPD)&lt;br /&gt;
* The [http://www.sherwoodtheory.org/ Sherwood Theory Conference]&lt;br /&gt;
* The [[International Conference on Tritium Science and Technology]] (TRITIUM)&lt;br /&gt;
* The [[International Symposium on Fusion Nuclear Technology]] (ISFNT)&lt;br /&gt;
* The [[Coordinated Working Group Meeting]] (CWGM)&lt;br /&gt;
* The [http://varenna-lausanne.epfl.ch/ Theory of Fusion Plasmas: Joint Varenna-Lausanne International Workshop] (Varenna-Lausanne even years)&lt;br /&gt;
* The International Conference on Fusion Reactor Materials (ICFRM)&lt;br /&gt;
&lt;br /&gt;
See also [[:Category:Conferences]].&lt;br /&gt;
&lt;br /&gt;
== Meeting lists at other sites ==&lt;br /&gt;
&lt;br /&gt;
* [http://ieee-npss.org/directory-of-plasma-conferences/ IEEE Nuclear and Plasma Sciences Society Directory of Plasma Conferences].&lt;br /&gt;
* [https://www.iter.org/conferences Calendar maintained at ITER of upcoming conferences on fusion science, fusion technology, plasma physics and energy].&lt;br /&gt;
* [https://www-amdis.iaea.org/w/index.php/Calendar_of_Meetings Calendar maintained by IAEA Atomic and Molecular Data Unit of meetings related to A+M+PMI processes and data for fusion].&lt;br /&gt;
* [http://fusenet.eu/events Calendar maintained by the European Fusion Education Network (FuseNet) of upcoming fusion related events].&lt;br /&gt;
* [http://crpp.epfl.ch/conferences_e Calendar maintained at Centre de Recherches en Physique des Plasmas, EPFL, of conferences on plasma physics research].&lt;br /&gt;
* [http://www.conference-service.com/conferences/plasma-and-gas-discharge-physics.html COMS Conferences and Meetings on Plasma and Gas-discharge Physics].&lt;br /&gt;
* [http://fire.pppl.gov/meetings_fusion.htm Calendar maintained at Fire, PPPL, of fusion meetings].&lt;br /&gt;
* [http://www.jspf.or.jp/calendar/cldrb.html Plasma and Fusion Calendar maintained by the Japan Society of Plasma Science and Nuclear Fusion Research].&lt;br /&gt;
* [https://burningplasma.org/newsandevents/?article=enews&amp;amp;issue=current Calendar maintained by the United States Burning Plasma Organization (USBPO) of fusion energy events].&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=EU-US_Transport_Task_Force_Meeting&amp;diff=8692</id>
		<title>EU-US Transport Task Force Meeting</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=EU-US_Transport_Task_Force_Meeting&amp;diff=8692"/>
		<updated>2026-09-04T17:03:50Z</updated>

		<summary type="html">&lt;p&gt;Admin: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The joint EU-US TTF meeting or workshop is held alternately in the USA and in Europe.&lt;br /&gt;
Its focus is on transport in magnetized plasmas, covering theory, experiment, and modeling aspects.&lt;br /&gt;
&lt;br /&gt;
In the period 2003-2005, the logical enumeration of the workshop was disrupted.&lt;br /&gt;
&lt;br /&gt;
== List of conferences ==&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;  align=&amp;quot;center&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
!&#039;&#039;Number&#039;&#039; !!&#039;&#039;Denomination&#039;&#039;&lt;br /&gt;
|-&lt;br /&gt;
|1|| 1&amp;lt;sup&amp;gt;st&amp;lt;/sup&amp;gt; (1994) Göteborg, Sweden&lt;br /&gt;
|-&lt;br /&gt;
|2|| 2&amp;lt;sup&amp;gt;nd&amp;lt;/sup&amp;gt; (1995) Marina del Rey, USA&lt;br /&gt;
|-&lt;br /&gt;
|3|| 3&amp;lt;sup&amp;gt;rd&amp;lt;/sup&amp;gt; (1996) Varenna, Italy &amp;lt;ref&amp;gt;J.W. Connor, C. Hidalgo, A. Jacchia, F. Romanelli, and U. Stroth, &#039;&#039;EU - US Workshop on Transport in Fusion Plasmas&#039;&#039;, [[doi:10.1088/0741-3335/39/4/007|Plasma Phys. Control. Fusion &#039;&#039;&#039;39&#039;&#039;&#039; (1997) 609]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|4|| 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (1997) Madison, USA&lt;br /&gt;
|-&lt;br /&gt;
|5|| 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (1998) Göteborg, Sweden &amp;lt;ref&amp;gt;J.W. Connor, P. Buratti, J.G. Cordey, C. Hidalgo, A. Jacchia, U. Stroth, and W. Suttrop, &#039;&#039;EU-US workshop on transport in fusion plasmas&#039;&#039;, [[doi:10.1088/0741-3335/41/5/601|Plasma Phys. Control. Fusion &#039;&#039;&#039;41&#039;&#039;&#039; (1999) 693]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|6|| [http://www-internal.psfc.mit.edu/ttf/1999/portland-meeting.html 5&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (1999) Portland, USA] &amp;lt;ref&amp;gt;Combined with the 12&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; annual US TTF Meeting&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|7|| [http://www.ifp.cnr.it/conference/EU-US_TTF.Varenna.Sept.2000/index.html 7&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2000) Varenna, Italy]&lt;br /&gt;
|-&lt;br /&gt;
|8|| [http://ffden-2.phys.uaf.edu/ttf.2001/index.htm 8&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2001) Fairbanks, Alaska, USA] &amp;lt;ref&amp;gt;Combined with the 14&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; annual US TTF Meeting&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|9|| [https://info.fusion.ciemat.es/ttf2002 9&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2002) Córdoba, Spain] &amp;lt;ref&amp;gt;J.W. Connor, X. Garbet, L. Giannone, M. Greenwald, C. Hidalgo, A. Loarte, and P. Mantica, &#039;&#039;EU-US transport task force workshop on transport in fusion plasmas: transport near operational limits&#039;&#039;, [[doi:10.1088/0741-3335/45/4/310|Plasma Phys. Control. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2003) 455]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|10|| [http://www.psfc.mit.edu/ttf/2003/meeting.html 9&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2003) Madison, USA] &amp;lt;ref&amp;gt;Combined with the 16&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; annual US TTF Meeting&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|11|| [http://www.ifp.cnr.it/conference/TTF04/index.htm 10&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2004) Varenna, Italy] &amp;lt;ref&amp;gt;J.W. Connor, X. Garbet, A.L. Rogister, M. Romanelli, and F. Ryter, &#039;&#039;EU–US workshop on transport in fusion plasmas&#039;&#039;, [[doi:10.1088/0741-3335/47/6/013|Plasma Phys. Control. Fusion &#039;&#039;&#039;47&#039;&#039;&#039; (2005) 941]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|12|| [http://www.mfescience.org/TTF2005/ 10&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2005) Napa, California, USA] &amp;lt;ref&amp;gt;Combined with the 18&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; annual US TTF Meeting&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|13|| [http://www-fusion-magnetique.cea.fr/ttf2006/index.htm 11&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2006) Marseille, France] &amp;lt;ref&amp;gt;J.W. Connor, C. Angioni, P.H. Diamond, G.W. Hammett, C. Hidalgo, A. Loarte, and P. Mantica, &#039;&#039;11th EU-US Transport Task Force workshop on transport in fusion plasmas&#039;&#039;, [[doi:10.1088/0029-5515/47/4/014|Nucl. Fusion &#039;&#039;&#039;47&#039;&#039;&#039; (2007) 361]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|14|| [http://fusion.gat.com/conferences/ttf/ 12&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2007) San Diego, USA]&lt;br /&gt;
|-&lt;br /&gt;
|15|| [http://www.risoe.dk/conferences/EUUS_TtF.aspx 13&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2008) Copenhagen, Denmark] &amp;lt;ref&amp;gt;Combined with the 1&amp;lt;sup&amp;gt;st&amp;lt;/sup&amp;gt; [[EFDA]] Transport Topical Group Meeting&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;J.W. Connor, A. Fasoli, C. Hidalgo, A. Kirk, V. Naulin, A.G. Peeters, and T. Tala, &#039;&#039;13th EU–US Transport Task Force Workshop on transport in fusion plasmas&#039;&#039;, [[doi:10.1088/0029-5515/49/4/047001|Nucl. Fusion &#039;&#039;&#039;49&#039;&#039;&#039; (2009) 047001]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|16|| [http://ttf2009.ucsd.edu/ 14&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2009) San Diego, USA]&lt;br /&gt;
|-&lt;br /&gt;
|17|| [https://info.fusion.ciemat.es/ttg2010 15&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2010) Córdoba, Spain] &amp;lt;ref&amp;gt;Combined with the 3&amp;lt;sup&amp;gt;rd&amp;lt;/sup&amp;gt; [[EFDA]] Transport Topical Group Meeting&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|18|| [http://ttf2011.pppl.gov/ 16&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2011) San Diego, USA]&lt;br /&gt;
|-&lt;br /&gt;
|19|| [http://www.igi.cnr.it/eu_us_ttf_2012/ 17&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2012) Padua, Italy] &amp;lt;ref&amp;gt;Combined with the 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; [[EFDA]] Transport Topical Group Meeting&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|20|| [http://ttf2013.ucsd.edu 18&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2013) Santa Rosa, CA, USA]&lt;br /&gt;
|-&lt;br /&gt;
|21|| [http://www.ttf2014.org/ 19&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2014) Abingdon, UK]&amp;lt;ref&amp;gt;The meeting at [http://ttf2014.ucsd.edu/TTF_2014/Home.html San Antonio, Texas, USA] is a US TTF meeing, not a Joint EU-US meeting - in spite of the announcement!&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;C. Angioni, P. Mantica, V. Naulin et al., &#039;&#039;Summary of the 19th Joint EU-US Transport Task Force Workshop&#039;&#039;, [[doi:10.1088/0029-5515/55/6/067001|Nucl. Fusion &#039;&#039;&#039;55&#039;&#039;&#039;, 6 (2015) 067001]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|22|| [http://www.psfc.mit.edu/TTF2015/index.html 20&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2015) Salem, MA, USA]&lt;br /&gt;
|-&lt;br /&gt;
|23|| [http://spc.epfl.ch/ttf16 21&amp;lt;sup&amp;gt;st&amp;lt;/sup&amp;gt; (2016) Leysin, Switzerland]&lt;br /&gt;
|-&lt;br /&gt;
|24 || [https://fusion.gat.com/conferences/ttf17/ 22&amp;lt;sup&amp;gt;nd&amp;lt;/sup&amp;gt; (2017) Williamsburg, VA, USA]&lt;br /&gt;
|-&lt;br /&gt;
|25 || [http://www.psft.eu/ttf2018/ 23&amp;lt;sup&amp;gt;rd&amp;lt;/sup&amp;gt; (2018) Seville, Spain]&lt;br /&gt;
|-&lt;br /&gt;
|26 || [https://sites.google.com/ucsd.edu/ttf2019/ 24&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2019) Austin, TX, USA]&lt;br /&gt;
|-&lt;br /&gt;
|27 || [https://www.york.ac.uk/physics/ypi/conferencesevents/25thjointeu-ustransporttaskforcemeeting/ 25&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2020) York, UK]&amp;lt;ref&amp;gt;The 2020 Meeting was postponed to 2021 in view of the coronavirus crisis.&amp;lt;/ref&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|28 || [https://ttf2023.sciencesconf.org/ 27&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2023) Nancy, France]&lt;br /&gt;
|-&lt;br /&gt;
|29 || [https://ttf2025.ek.hun-ren.hu/ 29&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2025) Budapest, Hungary]&lt;br /&gt;
|-&lt;br /&gt;
|30 || [https://uit.no/tavla/artikkel/936431/31th_eu-us_transport_task_force_workshop 30&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; (2027) Tromsø, Norway]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Notes and references ==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Category:Conferences]]&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=FusionWiki:Current_events&amp;diff=8691</id>
		<title>FusionWiki:Current events</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=FusionWiki:Current_events&amp;diff=8691"/>
		<updated>2026-09-04T16:59:59Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* 2027 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Upcoming Fusion and Plasma events ==&lt;br /&gt;
&lt;br /&gt;
Please feel free to add events.&lt;br /&gt;
&lt;br /&gt;
=== 2026 ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;width: 100%&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | Date (2026)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | Location&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;60%&amp;quot; | Conference/Meeting&lt;br /&gt;
|-&lt;br /&gt;
| February 24-25 || Barcelona, Spain || [https://hpcfusion.bsc.es/2026/about/ Fusion HPC Workshop]&lt;br /&gt;
|-&lt;br /&gt;
| April 20-24 || Córdoba, Spain || [https://ishw2026.com  25&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; International Stellarator and Heliotron Workshop] (ISHW)&lt;br /&gt;
|-&lt;br /&gt;
| June 8-12 || Kudowa-Zdrój, Poland || [http://kudowaschool.ipplm.pl/ 18&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; Kudowa Summer School &#039;Towards Fusion Energy&#039;]&lt;br /&gt;
|-&lt;br /&gt;
| June 15-18 || Prague, Czech Republic || [http://www.plasmaconference.cz/  31&amp;lt;sup&amp;gt;st&amp;lt;/sup&amp;gt; Symposium on Plasma Physics and Technology] (SPPT)&lt;br /&gt;
|-&lt;br /&gt;
| June 29-July 3 || Edinburgh, Scotland (UK) || [https://epsplasma2026.com/ 2026 European Physical Society Conference on Plasma Physics] (EPS-CPP)&lt;br /&gt;
|-&lt;br /&gt;
| September 8-11 || Seoul, Korea || 20&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; International Workshop on H-mode Physics and Transport Barriers (H-Mode Workshop 2026)&lt;br /&gt;
|-&lt;br /&gt;
| September 14-18 || Eindhoven, The Netherlands || [https://www.differ.nl/isla-9 9&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; International Symposium on Liquid Metal Applications for Fusion] (ISLA-9)&lt;br /&gt;
|-&lt;br /&gt;
| October 11-16 || Busan, Korea || [http://aappsdpp.org/AAPPSDPPF/ 10&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; Asia-Pacific Conference on Plasma Physics] (AAPPS-DPP2026)&lt;br /&gt;
|-&lt;br /&gt;
| October 13-15 || Madrid, Spain || [https://ifmif-dones.es/dones-updates/the-4th-dones-users-workshop/ 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; DONES User Workshop]&lt;br /&gt;
|-&lt;br /&gt;
| October 13-15 || Viterbo, Italy || [https://indico.fusenet.eu/event/66/overview FuseNet PhD Event]&lt;br /&gt;
|-&lt;br /&gt;
| October 20-23 || Hefei, China || [https://conferences.iaea.org/event/452/program 3&amp;lt;sup&amp;gt;rd&amp;lt;/sup&amp;gt; technical meeting on long-pulse operation of fusion devices]&lt;br /&gt;
|-&lt;br /&gt;
| November 15-20 || Seville, Spain || [https://istw2026.psft.eu 23&amp;lt;sup&amp;gt;rd&amp;lt;/sup&amp;gt; International Spherical Torus Workshop] (ISTW 2026)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== 2027 ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;width: 100%&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | Date (2026)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | Location&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;60%&amp;quot; | Conference/Meeting&lt;br /&gt;
|-&lt;br /&gt;
| February 15-19 || Nagoya, Japan || [https://lhdws2027.nifs.ac.jp/ International LHD Workshop] (LHDWS 2027)&lt;br /&gt;
|-&lt;br /&gt;
| September 7-10 || Tromsø, Norway || [https://uit.no/tavla/artikkel/936431/31th_eu-us_transport_task_force_workshop 31&amp;lt;sup&amp;gt;st&amp;lt;/sup&amp;gt; EU-US Transport Task Force Workshop] (TTF 2027)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Periodic meetings ==&lt;br /&gt;
&lt;br /&gt;
The following FusionWiki entries attempt to both provide a record of historic meetings and direct links to proceedings:&lt;br /&gt;
* The [[IAEA Fusion Energy Conference]] (FEC)&lt;br /&gt;
* The [[European Physical Society Conference on Plasma Physics]] (EPS-CPP)&lt;br /&gt;
* The [[European Conference on Plasma Diagnostics]] (ECPD)&lt;br /&gt;
* The [[International Congress on Plasma Physics]] (ICPP)&lt;br /&gt;
* The [https://engage.aps.org/dpp/meetings/annual-meeting Annual Meeting of the Division of Plasma Physics of the American Physical Society] (APS-DPP)&lt;br /&gt;
* The [[https://www.aappsdpp.org/AAPPSDPPF/Meetings.html  Asia-Pacific Conference on Plasma Physics AAPPS-DPP]&lt;br /&gt;
* The [[International Stellarator and Heliotron Workshop]] (ISHW)&lt;br /&gt;
* The [[European Fusion Theory Conference]] (EFTC)&lt;br /&gt;
* The [[Conference on Plasma Surface Interactions]] (PSI)&lt;br /&gt;
* The [[Symposium on Fusion Technology]] (SOFT)&lt;br /&gt;
* The [[Symposium On Fusion Engineering]] (SOFE)&lt;br /&gt;
* The [[EU-US Transport Task Force Meeting]] (TTF)&lt;br /&gt;
* The [[International Toki Conference]] (ITC)&lt;br /&gt;
* The [[Topical Conference on High Temperature Plasma Diagnostics]] (HTPD)&lt;br /&gt;
* The [http://www.sherwoodtheory.org/ Sherwood Theory Conference]&lt;br /&gt;
* The [[International Conference on Tritium Science and Technology]] (TRITIUM)&lt;br /&gt;
* The [[International Symposium on Fusion Nuclear Technology]] (ISFNT)&lt;br /&gt;
* The [[Coordinated Working Group Meeting]] (CWGM)&lt;br /&gt;
* The [http://varenna-lausanne.epfl.ch/ Theory of Fusion Plasmas: Joint Varenna-Lausanne International Workshop] (Varenna-Lausanne even years)&lt;br /&gt;
* The International Conference on Fusion Reactor Materials (ICFRM)&lt;br /&gt;
&lt;br /&gt;
See also [[:Category:Conferences]].&lt;br /&gt;
&lt;br /&gt;
== Meeting lists at other sites ==&lt;br /&gt;
&lt;br /&gt;
* [http://ieee-npss.org/directory-of-plasma-conferences/ IEEE Nuclear and Plasma Sciences Society Directory of Plasma Conferences].&lt;br /&gt;
* [https://www.iter.org/conferences Calendar maintained at ITER of upcoming conferences on fusion science, fusion technology, plasma physics and energy].&lt;br /&gt;
* [https://www-amdis.iaea.org/w/index.php/Calendar_of_Meetings Calendar maintained by IAEA Atomic and Molecular Data Unit of meetings related to A+M+PMI processes and data for fusion].&lt;br /&gt;
* [http://fusenet.eu/events Calendar maintained by the European Fusion Education Network (FuseNet) of upcoming fusion related events].&lt;br /&gt;
* [http://crpp.epfl.ch/conferences_e Calendar maintained at Centre de Recherches en Physique des Plasmas, EPFL, of conferences on plasma physics research].&lt;br /&gt;
* [http://www.conference-service.com/conferences/plasma-and-gas-discharge-physics.html COMS Conferences and Meetings on Plasma and Gas-discharge Physics].&lt;br /&gt;
* [http://fire.pppl.gov/meetings_fusion.htm Calendar maintained at Fire, PPPL, of fusion meetings].&lt;br /&gt;
* [http://www.jspf.or.jp/calendar/cldrb.html Plasma and Fusion Calendar maintained by the Japan Society of Plasma Science and Nuclear Fusion Research].&lt;br /&gt;
* [https://burningplasma.org/newsandevents/?article=enews&amp;amp;issue=current Calendar maintained by the United States Burning Plasma Organization (USBPO) of fusion energy events].&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=FusionWiki:Current_events&amp;diff=8686</id>
		<title>FusionWiki:Current events</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=FusionWiki:Current_events&amp;diff=8686"/>
		<updated>2026-08-26T09:29:28Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* 2026 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Upcoming Fusion and Plasma events ==&lt;br /&gt;
&lt;br /&gt;
Please feel free to add events.&lt;br /&gt;
&lt;br /&gt;
=== 2026 ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;width: 100%&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | Date (2026)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | Location&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;60%&amp;quot; | Conference/Meeting&lt;br /&gt;
|-&lt;br /&gt;
| February 24-25 || Barcelona, Spain || [https://hpcfusion.bsc.es/2026/about/ Fusion HPC Workshop]&lt;br /&gt;
|-&lt;br /&gt;
| April 20-24 || Córdoba, Spain || [https://ishw2026.com  25&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; International Stellarator and Heliotron Workshop] (ISHW)&lt;br /&gt;
|-&lt;br /&gt;
| June 8-12 || Kudowa-Zdrój, Poland || [http://kudowaschool.ipplm.pl/ 18&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; Kudowa Summer School &#039;Towards Fusion Energy&#039;]&lt;br /&gt;
|-&lt;br /&gt;
| June 15-18 || Prague, Czech Republic || [http://www.plasmaconference.cz/  31&amp;lt;sup&amp;gt;st&amp;lt;/sup&amp;gt; Symposium on Plasma Physics and Technology] (SPPT)&lt;br /&gt;
|-&lt;br /&gt;
| June 29-July 3 || Edinburgh, Scotland (UK) || [https://epsplasma2026.com/ 2026 European Physical Society Conference on Plasma Physics] (EPS-CPP)&lt;br /&gt;
|-&lt;br /&gt;
| September 8-11 || Seoul, Korea || 20&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; International Workshop on H-mode Physics and Transport Barriers (H-Mode Workshop 2026)&lt;br /&gt;
|-&lt;br /&gt;
| September 14-18 || Eindhoven, The Netherlands || [https://www.differ.nl/isla-9 9&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; International Symposium on Liquid Metal Applications for Fusion] (ISLA-9)&lt;br /&gt;
|-&lt;br /&gt;
| October 11-16 || Busan, Korea || [http://aappsdpp.org/AAPPSDPPF/ 10&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; Asia-Pacific Conference on Plasma Physics] (AAPPS-DPP2026)&lt;br /&gt;
|-&lt;br /&gt;
| October 13-15 || Madrid, Spain || [https://ifmif-dones.es/dones-updates/the-4th-dones-users-workshop/ 4&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; DONES User Workshop]&lt;br /&gt;
|-&lt;br /&gt;
| October 13-15 || Viterbo, Italy || [https://indico.fusenet.eu/event/66/overview FuseNet PhD Event]&lt;br /&gt;
|-&lt;br /&gt;
| October 20-23 || Hefei, China || [https://conferences.iaea.org/event/452/program 3&amp;lt;sup&amp;gt;rd&amp;lt;/sup&amp;gt; technical meeting on long-pulse operation of fusion devices]&lt;br /&gt;
|-&lt;br /&gt;
| November 15-20 || Seville, Spain || [https://istw2026.psft.eu 23&amp;lt;sup&amp;gt;rd&amp;lt;/sup&amp;gt; International Spherical Torus Workshop] (ISTW 2026)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
=== 2027 ===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;width: 100%&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | Date (2026)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | Location&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;60%&amp;quot; | Conference/Meeting&lt;br /&gt;
|-&lt;br /&gt;
| February 15-19 || Nagoya, Japan || [https://lhdws2027.nifs.ac.jp/ International LHD Workshop] (LHDWS 2027)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Periodic meetings ==&lt;br /&gt;
&lt;br /&gt;
The following FusionWiki entries attempt to both provide a record of historic meetings and direct links to proceedings:&lt;br /&gt;
* The [[IAEA Fusion Energy Conference]] (FEC)&lt;br /&gt;
* The [[European Physical Society Conference on Plasma Physics]] (EPS-CPP)&lt;br /&gt;
* The [[European Conference on Plasma Diagnostics]] (ECPD)&lt;br /&gt;
* The [[International Congress on Plasma Physics]] (ICPP)&lt;br /&gt;
* The [https://engage.aps.org/dpp/meetings/annual-meeting Annual Meeting of the Division of Plasma Physics of the American Physical Society] (APS-DPP)&lt;br /&gt;
* The [[https://www.aappsdpp.org/AAPPSDPPF/Meetings.html  Asia-Pacific Conference on Plasma Physics AAPPS-DPP]&lt;br /&gt;
* The [[International Stellarator and Heliotron Workshop]] (ISHW)&lt;br /&gt;
* The [[European Fusion Theory Conference]] (EFTC)&lt;br /&gt;
* The [[Conference on Plasma Surface Interactions]] (PSI)&lt;br /&gt;
* The [[Symposium on Fusion Technology]] (SOFT)&lt;br /&gt;
* The [[Symposium On Fusion Engineering]] (SOFE)&lt;br /&gt;
* The [[EU-US Transport Task Force Meeting]] (TTF)&lt;br /&gt;
* The [[International Toki Conference]] (ITC)&lt;br /&gt;
* The [[Topical Conference on High Temperature Plasma Diagnostics]] (HTPD)&lt;br /&gt;
* The [http://www.sherwoodtheory.org/ Sherwood Theory Conference]&lt;br /&gt;
* The [[International Conference on Tritium Science and Technology]] (TRITIUM)&lt;br /&gt;
* The [[International Symposium on Fusion Nuclear Technology]] (ISFNT)&lt;br /&gt;
* The [[Coordinated Working Group Meeting]] (CWGM)&lt;br /&gt;
* The [http://varenna-lausanne.epfl.ch/ Theory of Fusion Plasmas: Joint Varenna-Lausanne International Workshop] (Varenna-Lausanne even years)&lt;br /&gt;
* The International Conference on Fusion Reactor Materials (ICFRM)&lt;br /&gt;
&lt;br /&gt;
See also [[:Category:Conferences]].&lt;br /&gt;
&lt;br /&gt;
== Meeting lists at other sites ==&lt;br /&gt;
&lt;br /&gt;
* [http://ieee-npss.org/directory-of-plasma-conferences/ IEEE Nuclear and Plasma Sciences Society Directory of Plasma Conferences].&lt;br /&gt;
* [https://www.iter.org/conferences Calendar maintained at ITER of upcoming conferences on fusion science, fusion technology, plasma physics and energy].&lt;br /&gt;
* [https://www-amdis.iaea.org/w/index.php/Calendar_of_Meetings Calendar maintained by IAEA Atomic and Molecular Data Unit of meetings related to A+M+PMI processes and data for fusion].&lt;br /&gt;
* [http://fusenet.eu/events Calendar maintained by the European Fusion Education Network (FuseNet) of upcoming fusion related events].&lt;br /&gt;
* [http://crpp.epfl.ch/conferences_e Calendar maintained at Centre de Recherches en Physique des Plasmas, EPFL, of conferences on plasma physics research].&lt;br /&gt;
* [http://www.conference-service.com/conferences/plasma-and-gas-discharge-physics.html COMS Conferences and Meetings on Plasma and Gas-discharge Physics].&lt;br /&gt;
* [http://fire.pppl.gov/meetings_fusion.htm Calendar maintained at Fire, PPPL, of fusion meetings].&lt;br /&gt;
* [http://www.jspf.or.jp/calendar/cldrb.html Plasma and Fusion Calendar maintained by the Japan Society of Plasma Science and Nuclear Fusion Research].&lt;br /&gt;
* [https://burningplasma.org/newsandevents/?article=enews&amp;amp;issue=current Calendar maintained by the United States Burning Plasma Organization (USBPO) of fusion energy events].&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=User:Admin&amp;diff=8682</id>
		<title>User:Admin</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=User:Admin&amp;diff=8682"/>
		<updated>2026-08-14T07:35:01Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* &amp;amp;ge; 2020 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[File:BvM.jpg|right|]]&lt;br /&gt;
== Personal information ==&lt;br /&gt;
__NOTOC__&lt;br /&gt;
* Boudewijn van Milligen (Admin)&lt;br /&gt;
* Researcher at: &amp;lt;br&amp;gt;[[Laboratorio Nacional de Fusión]] - [[CIEMAT]] &amp;lt;br&amp;gt;Avda. Complutense 40, Edif. 66&amp;lt;br&amp;gt;28040 Madrid, España - Spain&lt;br /&gt;
* Tel. +34 - 914 962 682&lt;br /&gt;
* Email boudewijn.vanmilligen (at) ciemat.es&lt;br /&gt;
User profiles:&lt;br /&gt;
* [https://publons.com/researcher/1248698/boudewijn-ph-van-milligen/ Publons] (ResearcherID H-5121-2015)&lt;br /&gt;
* [http://orcid.org/0000-0001-5344-6274 ORCID 0000-0001-5344-6274]&lt;br /&gt;
* [https://www.scopus.com/authid/detail.uri?authorId=35476190300 Scopus AuthorID 35476190300]&lt;br /&gt;
* [http://scholar.google.com/citations?user=7z9Cr9oAAAAJ Google Scholar]&lt;br /&gt;
* [https://www.researchgate.net/profile/Boudewijn_Van_Milligen/ ResearchGate]&lt;br /&gt;
&lt;br /&gt;
== Interests ==&lt;br /&gt;
&lt;br /&gt;
* Fusion and plasma physics&lt;br /&gt;
** [[H-mode|L-H transition]], Zonal Flows&lt;br /&gt;
** [[Magnetic island]]s, MHD activity&lt;br /&gt;
* [[Anomalous transport]]&lt;br /&gt;
** Turbulence&lt;br /&gt;
** Continuous Time Random Walks&lt;br /&gt;
* Data analysis&lt;br /&gt;
** [[Causality detection]]&lt;br /&gt;
** [[Intermittence]]&lt;br /&gt;
** [[:Wikipedia:Rescaled range|Rescaled range]] or [[:Wikipedia:Hurst exponent|Hurst]] analysis&lt;br /&gt;
** [[Bayesian data analysis]]&lt;br /&gt;
** [[Biorthogonal decomposition]]&lt;br /&gt;
** [[Bicoherence]]&lt;br /&gt;
** [[TJ-II:Tomography|Tomography]]&lt;br /&gt;
&lt;br /&gt;
== Book ==&lt;br /&gt;
&lt;br /&gt;
B.Ph. van Milligen and R. Sánchez, &#039;&#039;Analysis of Turbulence in Fusion Plasmas&#039;&#039;, [[doi:10.1088/978-0-7503-4856-0|IOP Publishing (2022)]], {{ISBN|978-0-7503-4854-6}}&lt;br /&gt;
&lt;br /&gt;
== Selected publications ==&lt;br /&gt;
&lt;br /&gt;
(inverse chronological order)&lt;br /&gt;
=== &amp;amp;ge; 2020 ===&lt;br /&gt;
* B.Ph. van Milligen, I. Voldiner, E. de la Cal, A. Alonso Alvarez, I. Luiz Caldas and Z. Guimarães Filho, &#039;&#039;Turbulence analysis with the spectroscopic gas puff imaging diagnostic in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/1361-6587/ae92b5|Plasma Phys. Control. Fusion &#039;&#039;&#039;68&#039;&#039;&#039; (2026) 085018]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* A. Alonso Alvarez, B. P. Van Milligen, I. Voldiner, I. L. Caldas, Z. Guimarães Filho, O. Kozachok, and A. Chmyga. &#039;&#039;Edge turbulence dynamics across electron–ion root transitions during ECRH modulation experiments in the TJ-II stellarator&#039;&#039;. [[doi:10.1088/1361-6587/ae7470|Plasma Phys. Control. Fusion, &#039;&#039;&#039;68&#039;&#039;&#039; (2026) 065019]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. van Milligen, I. García-Cortés, K.J. McCarthy, et al, &#039;&#039;The rotational transform and enhanced confinement in the TJ-II stellarator&#039;&#039;, [[doi:10.1017/S0022377825100433|Journal of Plasma Physics &#039;&#039;&#039;91&#039;&#039;&#039;, 4 (2025) E98]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* Boudewijn Philip van Milligen, Teresa Estrada, Benjamin Carreras, Luis García, and TJ-II Team. &#039;&#039;Importance of the Rotational Transform for L–H Transitions in the TJ-II Stellarator&#039;&#039; [[doi:10.3390/plasma7020024|Plasma &#039;&#039;&#039;7&#039;&#039;&#039;, no. 2 (2024) 446-464]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. van Milligen, I. Voldiner, B.A. Carreras, L. García, M.A. Ochando and The TJ-II Team, &#039;&#039;Rational surfaces, flows and radial structure in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/1741-4326/aca688|Nucl. Fusion &#039;&#039;&#039;63&#039;&#039;&#039; (2023) 016027]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. Van Milligen, B.A. Carreras, L. Garcia, G. Grenfell, I. Voldiner and C. Hidalgo, &#039;&#039;The impact of radial electric fields and plasma rotation on intermittence in TJ-II&#039;&#039;, [[doi:10.1088/1361-6587/ac54e9|Plasma Phys. Control. Fusion &#039;&#039;&#039;64&#039;&#039;&#039;, 5 (2022) 055006]] ([http://documenta.ciemat.es/handle/123456789/2290 repository])&lt;br /&gt;
* B. van Milligen, A. Melnikov, B. Carreras, L. Garcia, A. Kozachek, C. Hidalgo, J. de Pablos, Ph. Khabanov, L. Eliseev, M. Drabinskij, A. Chmyga, L. Krupnik, the HIBP Team, the TJ-II Team, &#039;&#039;Topology of 2-D turbulent structures based on intermittence in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/1741-4326/ac27c9|Nucl. Fusion &#039;&#039;&#039;61&#039;&#039;&#039;, 11 (2021) 116063]] ([http://documenta.ciemat.es/handle/123456789/2281 repository])&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras, I. Voldiner, U. Losada, C. Hidalgo, and the TJ-II Team, &#039;&#039;Causality, intermittence and crossphase evolution during confinement transitions in the TJ-II stellarator&#039;&#039;, [[doi:10.1063/5.0057791|Phys. Plasmas &#039;&#039;&#039;28&#039;&#039;&#039; (2021) 092302]] ([http://documenta.ciemat.es/handle/123456789/2289 repository])&lt;br /&gt;
* B.Ph. van Milligen, B. Carreras, L. García and C. Hidalgo, &#039;&#039;The localization of low order rational surfaces based on the intermittence parameter in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/1741-4326/ab79cc|Nucl. Fusion &#039;&#039;&#039;60&#039;&#039;&#039; (2020) 056010]] ([http://documenta.ciemat.es/handle/123456789/2291 repository])&lt;br /&gt;
&lt;br /&gt;
=== 2010-2019 ===&lt;br /&gt;
* B.Ph. van Milligen, B. Carreras, L. García and J. Nicolau, &#039;&#039;The radial propagation of heat in strongly driven non-equilibrium fusion plasmas&#039;&#039;, [[doi:10.3390/e21020148|Entropy, &#039;&#039;&#039;21&#039;&#039;&#039;, 2 (2019) 148]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. van Milligen, B. Carreras, E. de la Luna and E. Solano, &#039;&#039;Radial variation of heat transport in L-mode JET discharges&#039;&#039; [[doi:10.1088/1741-4326/ab03e1|Nucl. Fusion, &#039;&#039;&#039;59&#039;&#039;&#039; (2019) 056006]] ([http://documenta.ciemat.es/handle/123456789/2292 repository])&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras, C. Hidalgo, Á. Cappa and the TJ-II Team, &#039;&#039;A possible mechanism for confinement power degradation in the TJ-II stellarator&#039;&#039;, [[doi:10.1063/1.5029881|Phys. Plasmas &#039;&#039;&#039;25&#039;&#039;&#039; (2018) 062503]] ([http://documenta.ciemat.es/handle/123456789/2308 repository])&lt;br /&gt;
* B.Ph. van Milligen, U. Hoefel, J. Nicolau, M. Hirsch, L. García, B. Carreras, C. Hidalgo and the W7-X Team, &#039;&#039;Study of radial heat transport in W7-X using the transfer entropy&#039;&#039;, [[doi:10.1088/1741-4326/aabf5d|Nucl. Fusion &#039;&#039;&#039;58&#039;&#039;&#039; (2018) 076002]] ([http://hdl.handle.net/10016/32565 repository])&lt;br /&gt;
* B.Ph. van Milligen, J. Hernández Nicolau, B. Liu, G. Grenfell, U. Losada, B. Carreras, L. Garcia and C. Hidalgo, &#039;&#039;Filaments in the edge confinement region of TJ-II&#039;&#039;, [[doi:10.1088/1741-4326/aa9db6|Nucl. Fusion &#039;&#039;&#039;58&#039;&#039;&#039; (2018) 026030]] ([http://hdl.handle.net/10016/32563 repository])&lt;br /&gt;
* B.Ph. van Milligen, J.H. Nicolau, L. García, B.A. Carreras, C. Hidalgo and the TJ-II Team, &#039;&#039;The impact of rational surfaces on radial heat transport in TJ-II&#039;&#039;, [[doi:10.1088/1741-4326/aa611f|Nucl. Fusion &#039;&#039;&#039;57&#039;&#039;&#039;, 5 (2017) 056028]], [https://arxiv.org/abs/1701.04574 arxiv:1701.04574]&lt;br /&gt;
* B.Ph. van Milligen, T. Estrada, B.A. Carreras, E. Ascasíbar, C. Hidalgo, I. Pastor, J.M. Fontdecaba, R. Balbín and the TJ-II Team, &#039;&#039;The causal impact of magnetic fluctuations in slow and fast L–H transitions at TJ-II&#039;&#039;, [[doi:10.1063/1.4958807|Phys. Plasmas &#039;&#039;&#039;23&#039;&#039;&#039; (2016) 072305]], [https://arxiv.org/abs/1512.06525 arxiv:1512.06525]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras, L. García, A. Martín de Aguilera, C. Hidalgo, J.H. Nicolau and the TJ-II Team, &#039;&#039;The causal relation between turbulent particle flux and density gradient&#039;&#039;, [[doi:10.1063/1.4958806|Phys. Plasmas &#039;&#039;&#039;23&#039;&#039;&#039; (2016) 072307]]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras and D.E. Newman, &#039;&#039;Constructing criteria to diagnose the likelihood of extreme events in the case of the electric power grid&#039;&#039;, [[doi:10.1063/1.4943569|Chaos &#039;&#039;&#039;26&#039;&#039;&#039; (2016) 033109]]&lt;br /&gt;
* B.Ph. van Milligen, T. Estrada, L. García, D. López-Bruna, B. Carreras, Y. Xu, M. Ochando, C. Hidalgo, J. Reynolds-Barredo and A. López-Fraguas, &#039;&#039;The role of magnetic islands in modifying long range temporal correlations of density fluctuations and local heat transport&#039;&#039;, [[doi:10.1088/0029-5515/56/1/016013|Nucl. Fusion, &#039;&#039;&#039;56&#039;&#039;&#039;, 1 (2016) 016013]], [https://arxiv.org/abs/1506.06890 arxiv:1506.06890]&lt;br /&gt;
* B.Ph. van Milligen, E. Sánchez, A. Alonso, M.A. Pedrosa, C. Hidalgo, A. Martín de Aguilera, A. López Fraguas, &#039;&#039;The use of the Biorthogonal Decomposition for the identification of zonal flows at TJ-II&#039;&#039;, [[doi:10.1088/0741-3335/57/2/025005|Plasma Phys. Control. Fusion &#039;&#039;&#039;57&#039;&#039;&#039;, 2 (2015) 025005]], [https://arxiv.org/abs/1408.1845 arxiv:1408.1845]&lt;br /&gt;
* B.Ph. van Milligen, P.D. Bons, &#039;&#039;Simplified numerical model for clarifying scaling behavior in the intermediate dispersion regime in homogeneous porous media&#039;&#039;, [[doi:10.1016/j.cpc.2014.09.006|Comput. Phys. Commun. &#039;&#039;&#039;185&#039;&#039;&#039; (2014) 3291]], [https://arxiv.org/abs/1409.2724 arxiv:1409.2724]&lt;br /&gt;
* B.Ph. van Milligen, G. Birkenmeier, M. Ramisch, T. Estrada, C. Hidalgo and A. Alonso, &#039;&#039;Causality detection and turbulence in fusion plasmas&#039;&#039;, [[doi:10.1088/0029-5515/54/2/023011|Nucl. Fusion &#039;&#039;&#039;54&#039;&#039;&#039; (2014), 023011]], [https://arxiv.org/abs/1309.7769 arxiv:1309.7769]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Parallel and perpendicular turbulence correlation length in the TJ-II Stellarator&#039;&#039;, [[doi:10.1088/0029-5515/53/9/093025|Nucl. Fusion &#039;&#039;&#039;53&#039;&#039;&#039; (2013) 093025]], [https://arxiv.org/abs/1306.1395 arxiv:1306.1395]&lt;br /&gt;
* P.D. Bons, B.Ph. van Milligen, P. Blum, &#039;&#039;A general unified expression for solute and heat dispersion in homogeneous porous media&#039;&#039;, [[doi:10.1002/wrcr.20488|Water Resour. Res. &#039;&#039;&#039;49&#039;&#039;&#039; (2013) 1]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Spatiotemporal and wavenumber resolved bicoherence at the low to high confinement transition in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/53/11/113034|Nucl. Fusion &#039;&#039;&#039;53&#039;&#039;&#039; (2013) 113034]], [https://arxiv.org/abs/1211.0420 arxiv:1211.0420]&lt;br /&gt;
* B. Ph. van Milligen, R. Sánchez and C. Hidalgo, &#039;&#039;Relevance of Uncorrelated Lorentzian Pulses for the Interpretation of Turbulence in the Edge of Magnetically Confined Toroidal Plasmas&#039;&#039;, [[doi:10.1103/PhysRevLett.109.105001|Phys. Rev. Lett. &#039;&#039;&#039;109&#039;&#039;&#039; (2012) 105001]], [https://arxiv.org/abs/1204.6185 arxiv:1204.6185]&lt;br /&gt;
* B.Ph. van Milligen, P.D. Bons, &#039;&#039;Analytical model for tracer dispersion in porous media&#039;&#039;, [[doi:10.1103/PhysRevE.85.011306|Phys. Rev. E 85 (2012) 011306]], [https://arxiv.org/abs/1111.6512 arxiv:1111.6512]&lt;br /&gt;
* B.Ph. van Milligen, L. García, B.A. Carreras, M.A. Pedrosa, C. Hidalgo, J.A. Alonso, T. Estrada and E. Ascasíbar, &#039;&#039;MHD mode activity and the velocity shear layer at TJ-II&#039;&#039;, [[doi:10.1088/0029-5515/52/1/013006|Nucl. Fusion &#039;&#039;&#039;52&#039;&#039;&#039; (2012) 013006]]&lt;br /&gt;
* B.Ph. van Milligen, T. Estrada, E. Ascasíbar, et al, &#039;&#039;Integrated data analysis at TJ-II: the density profile&#039;&#039;, [[doi:10.1063/1.3608551|Rev. Sci. Instrum. &#039;&#039;&#039;82&#039;&#039;&#039; (2011) 073503]]&lt;br /&gt;
* B.A. Carreras et al., &#039;&#039;Reconstruction of intermittent waveforms associated with the zonal flow at the transition leading to the edge shear flow layer&#039;&#039;, [[doi:10.1088/0029-5515/51/5/053022|Nucl. Fusion &#039;&#039;&#039;51&#039;&#039;&#039; (2011) 053022]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;A global resonance phenomenon at the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/51/1/013005|Nucl. Fusion &#039;&#039;&#039;51&#039;&#039;&#039; (2011) 013005]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;The dynamics of the formation of the edge particle transport barrier at TJ-II&#039;&#039;, [[doi:10.1088/0029-5515/51/11/113002|Nucl. Fusion &#039;&#039;&#039;51&#039;&#039;&#039; (2011) 113002]]&lt;br /&gt;
&lt;br /&gt;
=== 2000-2009 ===&lt;br /&gt;
* B.Ph. van Milligen, I. Calvo and R. Sánchez, &#039;&#039;Continuous time random walks in finite domains and general boundary conditions: some formal considerations&#039;&#039;, [[doi:10.1088/1751-8113/41/21/215004|J. Phys. A: Math. Theor. &#039;&#039;&#039;41&#039;&#039;&#039; (2008) 215004]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Quantifying profile stiffness&#039;&#039;, [http://www.jspf.or.jp/PFR/PFR_articles/pfr2008S1/pfr2008_03-S1070.html Plasma and Fusion Research, &#039;&#039;&#039;3&#039;&#039;&#039; (2008) S1070]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Bicoherence during confinement transitions in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/48/11/115003|Nucl. Fusion &#039;&#039;&#039;48&#039;&#039;&#039; (2008) 115003]]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras, V.E. Lynch and R. Sánchez, &#039;&#039;Pulse propagation in a simple probabilistic transport model&#039;&#039;, [[doi:10.1088/0029-5515/47/3/004|Nucl. Fusion &#039;&#039;&#039;47&#039;&#039;&#039; (2007) 189]]&lt;br /&gt;
* B.Ph. van Milligen, P.D. Bons, B.A. Carreras and R. Sánchez, &#039;&#039;On the applicability of Fick&#039;s Law to diffusion in inhomogeneous systems&#039;&#039;, [[doi:10.1088/0143-0807/26/5/023|Eur. J. Phys. &#039;&#039;&#039;26&#039;&#039;&#039; (2005) 913]]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras and R. Sánchez, &#039;&#039;The foundations of diffusion revisited&#039;&#039;, [[doi:10.1088/0741-3335/47/12B/S56|Plasma Phys. Control. Fusion &#039;&#039;&#039;47&#039;&#039;&#039; (2005) B743]]&lt;br /&gt;
* B.Ph. Van Milligen et al, &#039;&#039;Additional evidence for the universality of turbulent fluctuations and fluxes in the scrape-off layer region of fusion plasmas&#039;&#039;, [[doi:10.1063/1.1884615|Phys. Plasmas &#039;&#039;&#039;12&#039;&#039;&#039; (2005) 052507]]&lt;br /&gt;
* B.Ph. van Milligen, R. Sánchez and B.A. Carreras, &#039;&#039;Probabilistic finite-size transport models for fusion: anomalous transport and scaling laws&#039;&#039;, [[doi:10.1063/1.1701893|Phys. Plasmas &#039;&#039;&#039;11&#039;&#039;&#039;, 5 (2004) 2272]]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras and R. Sánchez, &#039;&#039;Uphill transport and the probabilistic transport model&#039;&#039;, [[doi:10.1063/1.1763915|Phys. Plasmas &#039;&#039;&#039;11&#039;&#039;&#039;, 3787 (2004)]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Revision of TV Thomson scattering data analysis and detection of profile structure&#039;&#039;, [[doi:10.1063/1.1597951|Rev. Sci. Instrum. &#039;&#039;&#039;74&#039;&#039;&#039; (2003) 3998]]&lt;br /&gt;
* B.Ph. van Milligen, E. de la Luna, F.L. Tabarés, et al., &#039;&#039;Ballistic transport phenomena in TJ-II&#039;&#039;, [[doi:10.1088/0029-5515/42/7/301|Nucl. Fusion &#039;&#039;&#039;42&#039;&#039;&#039; (2002) 787]]&lt;br /&gt;
=== 1990 - 1999 ===&lt;br /&gt;
* B.A. Carreras, B.Ph. van Milligen, et al, &#039;&#039;Experimental evidence of long-range correlation and self-similarity in plasma fluctuations&#039;&#039;, [[doi:10.1063/1.873490|Phys. Plasmas &#039;&#039;&#039;6&#039;&#039;&#039;, 5 (1999) 1885]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Statistically robust linear and non-linear wavelet analysis applied to plasma edge turbulence&#039;&#039;, [[doi:10.1063/1.1147727|Rev. Sci. Instrum. &#039;&#039;&#039;68&#039;&#039;&#039; (1997) 967]]&lt;br /&gt;
* B.Ph. van Milligen, V. Tribaldos, J.A. Jiménez, &#039;&#039;A neural network differential equation and plasma equilibrium solver&#039;&#039;, [[doi:10.1103/PhysRevLett.75.3594|Phys. Rev. Lett. &#039;&#039;&#039;75&#039;&#039;&#039; (1995) 3594]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Nonlinear phenomena and intermittency in plasma turbulence&#039;&#039;, [[doi:10.1103/PhysRevLett.74.395|Phys. Rev. Lett. &#039;&#039;&#039;74&#039;&#039;&#039;, 3 (1995) 395]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Wavelet bicoherence: a new turbulence analysis tool&#039;&#039;, [[doi:10.1063/1.871199|Phys. Plasmas &#039;&#039;&#039;2&#039;&#039;&#039;, 8 (1995) 3017]]&lt;br /&gt;
* B.Ph. van Milligen and A. Lopez Fraguas, &#039;&#039;Expansion of vacuum magnetic fields in toroidal harmonics&#039;&#039;, [[doi:10.1016/0010-4655(94)90112-0|Comput. Phys. Commun. &#039;&#039;&#039;81&#039;&#039;&#039;, Issues 1-2 (1994) 74-90]]&lt;br /&gt;
* B.Ph. van Milligen, A.C.A.P. van Lammeren, N.J. Lopes Cardozo, F.C. Schüller and M. Verreck, &#039;&#039;Gradients of electron temperature and density across m=2 islands in RTP&#039;&#039;, [[doi:10.1088/0029-5515/33/8/I03|Nucl. Fusion &#039;&#039;&#039;33&#039;&#039;&#039; (1993) 1119]]&lt;br /&gt;
* B.Ph. van Milligen, N.J. Lopes Cardozo, &#039;&#039;Function Parametrization: a fast inverse mapping method&#039;&#039;, [[doi:10.1016/0010-4655(91)90073-T|Comput. Phys. Commun. &#039;&#039;&#039;66&#039;&#039;&#039; (1991) 243]]&lt;br /&gt;
* B.Ph. van Milligen et al., &#039;&#039;Application of Function Parametrization to the analysis of polarimetry and interferometry data in TEXTOR&#039;&#039;, [[doi:10.1088/0029-5515/31/2/007|Nucl. Fusion &#039;&#039;&#039;31&#039;&#039;&#039; (1991) 309]]&lt;br /&gt;
* B.Ph. van Milligen, &#039;&#039;Exact relations between multipole moments of the flux and moments of the toroidal current density in tokamaks&#039;&#039;, [[doi:10.1088/0029-5515/30/1/012|Nucl. Fusion &#039;&#039;&#039;30&#039;&#039;&#039; (1990) 157]]&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=CIEMAT&amp;diff=8680</id>
		<title>CIEMAT</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=CIEMAT&amp;diff=8680"/>
		<updated>2026-08-06T08:00:13Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* History */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[File:CIEMAT.jpg|400px|thumb|right|CIEMAT logo]]&lt;br /&gt;
The Centro para Investigaciones Energéticas, Medioambientales y Tecnológicas (Centre for Energy, Environment and Technology Research, CIEMAT), an Organism of the Spanish Ministry of Science and Innovation, is a Public Research Agency that is mainly focused on the energy and the environment, but also conducts studies into many advanced technologies and in various areas of fundamental research. Its staff numbers upward from 1200.&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
The CIEMAT is the successor of the Junta de Energía Nuclear (JEN), founded in 1951 by a Decree (dated October 22, 1951) with the purpose of studying the pacific application of nuclear energy and ionizing radiation.&lt;br /&gt;
&lt;br /&gt;
In 1986, the organization was renamed CIEMAT, and its scope was enhanced to include other forms of alternative energy, to study the environmental impact of energy generation, and to develop associated technologies.&lt;br /&gt;
&amp;lt;ref&amp;gt;A.R. de Pablos, J.M. Sánchez Ron, &#039;&#039;De la JEN al CIEMAT&#039;&#039;, Ediciones Doce Calles S.L. (2001) [http://www.boe.es/diario_boe/txt.php?id=BOE-A-2011-15214 NIPO] 402-01-005-7; [https://catalogo.bne.es/permalink/34BNE_INST/95vni4/alma991007713959708606 Bibilioteca Nacional de España]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Goals ==&lt;br /&gt;
&lt;br /&gt;
CIEMAT focuses on research and technological development projects, serving as a reference for the technical representation of Spain in international forums, and advising government on matters within its field of competence. Its main goals are:&lt;br /&gt;
* To develop alternative energy sources&lt;br /&gt;
* To improve energy efficiency and optimize energy generating systems&lt;br /&gt;
* To improve the efficiency and reduce the environmental impact of fossil fuels&lt;br /&gt;
* To improve the safety of energy generation by nuclear fission&lt;br /&gt;
* To study the feasibility of [[Nuclear fusion|nuclear fusion]] as a future energy option&lt;br /&gt;
* To improve the competitiveness of renewable energy sources in the energy market&lt;br /&gt;
* To develop solutions for improving the environmental quality&lt;br /&gt;
&lt;br /&gt;
== Research centres ==&lt;br /&gt;
&lt;br /&gt;
CIEMAT possesses three research centres:&lt;br /&gt;
* The main establishment is in Madrid (Moncloa), and that is where the [[Laboratorio Nacional de Fusión]] is located.&lt;br /&gt;
* The Solar Platform in Almería &amp;lt;ref&amp;gt;[http://www.psa.es/webeng/index.php The Solar Platform]&amp;lt;/ref&amp;gt; - the largest solar energy plant in Europe, located in the Tabernas Desert.&lt;br /&gt;
* The Centre for Renewable Energy Development in Soria. &amp;lt;ref&amp;gt;[http://www.ciemat.es/CEDERportal/portal.do The Centre for Renewable Energy Development]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== External links ==&lt;br /&gt;
&lt;br /&gt;
* [http://www.ciemat.es CIEMAT web site] &lt;br /&gt;
* [http://es.wikipedia.org/wiki/CIEMAT CIEMAT in the Wikipedia] (Spanish)&lt;br /&gt;
* [http://www.openstreetmap.org/?lat=40.45455&amp;amp;lon=-3.72867&amp;amp;zoom=17&amp;amp;layers=M OpenStreetMap]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=SIESTA&amp;diff=8679</id>
		<title>SIESTA</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=SIESTA&amp;diff=8679"/>
		<updated>2026-07-31T13:23:18Z</updated>

		<summary type="html">&lt;p&gt;Admin: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;SIESTA is an ideal [[MHD equilibrium|MHD 3D-equilibrium]] solver, capable of dealing with [[Magnetic island|magnetic islands]] and stochastic regions in a fast, accurate and scalable manner.&lt;br /&gt;
&amp;lt;ref&amp;gt;S. P. Hirshman, R. Sanchez, and C. R. Cook, &#039;&#039;SIESTA: A scalable iterative equilibrium solver for toroidal applications&#039;&#039;, [[doi:10.1063/1.3597155|Phys. Plasmas 18, 062504 (2011)]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://epsppd.epfl.ch/Hersonissos/pdf/P2_058.pdf S.P. Hirschmann, R. Sánchez, V.E. Lynch, E.F. D&#039;Azevedo, J.C. Hill, &#039;&#039;SIESTA: A Scalable Iterative Equilibrium Solver for Toroidal Applications&#039;&#039;, 35&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; EPS Conference on Plasma Physics, ECA &#039;&#039;&#039;32D&#039;&#039;&#039; (2008) P-2.058] ([https://info.fusion.ciemat.es/OCS/EPS2008/pdf/P2_058.pdf alternative link])&amp;lt;/ref&amp;gt;&lt;br /&gt;
The SIESTA code will complement other existent 3D MHD island solvers and is particularly suited for applications that require not only accuracy but speed of evaluation as well, such as experimental 3D equilibrium reconstruction or stellarator design. SIESTA will also be useful to calculate MHD equilibria at very high spatial resolutions, such as those that might be required for the investigation of NTMs at [[ITER]]-relevant temperature and resistivity conditions. SIESTA is based on a preconditioned, iterative algorithm that takes advantage of a pre-existent [[VMEC]] solution to provide both a background coordinate system that guarantees a compact representation as well as a good initial guess for the iterative procedure.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Software]]&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=SIESTA&amp;diff=8678</id>
		<title>SIESTA</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=SIESTA&amp;diff=8678"/>
		<updated>2026-07-31T13:11:05Z</updated>

		<summary type="html">&lt;p&gt;Admin: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;SIESTA is an ideal [[MHD equilibrium|MHD 3D-equilibrium]] solver, capable of dealing with [[Magnetic island|magnetic islands]] and stochastic regions in a fast, accurate and scalable manner.&lt;br /&gt;
&amp;lt;ref&amp;gt;S. P. Hirshman, R. Sanchez, and C. R. Cook, &#039;&#039;SIESTA: A scalable iterative equilibrium solver for toroidal applications&#039;&#039;, [[doi:10.1063/1.3597155|Phys. Plasmas 18, 062504 (2011)]]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://epsppd.epfl.ch/Hersonissos/pdf/P2_058.pdf S.P. Hirschmann, R. Sánchez, V.E. Lynch, E.F. D&#039;Azevedo, J.C. Hill, &#039;&#039;SIESTA: A Scalable Iterative Equilibrium Solver for Toroidal Applications&#039;&#039;, 25&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; EPS Conference on Plasma Physics, ECA &#039;&#039;&#039;32D&#039;&#039;&#039; (2008) P-2.058] (or [https://info.fusion.ciemat.es/OCS/EPS2008/pdf/P2_058.pdf 35th EPS Conference on Plasma Phys. Hersonissos, 9 - 13 June 2008 ECA Vol.32D, P-2.058 (2008)])&amp;lt;/ref&amp;gt;&lt;br /&gt;
The SIESTA code will complement other existent 3D MHD island solvers and is particularly suited for applications that require not only accuracy but speed of evaluation as well, such as experimental 3D equilibrium reconstruction or stellarator design. SIESTA will also be useful to calculate MHD equilibria at very high spatial resolutions, such as those that might be required for the investigation of NTMs at [[ITER]]-relevant temperature and resistivity conditions. SIESTA is based on a preconditioned, iterative algorithm that takes advantage of a pre-existent [[VMEC]] solution to provide both a background coordinate system that guarantees a compact representation as well as a good initial guess for the iterative procedure.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Software]]&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=SIESTA&amp;diff=8677</id>
		<title>SIESTA</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=SIESTA&amp;diff=8677"/>
		<updated>2026-07-31T13:08:24Z</updated>

		<summary type="html">&lt;p&gt;Admin: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;SIESTA is a new ideal [[MHD equilibrium|MHD 3D-equilibrium]] solver, capable of dealing with [[Magnetic island|magnetic islands]] and stochastic regions in a fast, accurate and scalable manner.&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://epsppd.epfl.ch/Hersonissos/pdf/P2_058.pdf S.P. Hirschmann, R. Sánchez, V.E. Lynch, E.F. D&#039;Azevedo, J.C. Hill, &#039;&#039;SIESTA: A Scalable Iterative Equilibrium Solver for Toroidal Applications&#039;&#039;, 25&amp;lt;sup&amp;gt;th&amp;lt;/sup&amp;gt; EPS Conference on Plasma Physics, ECA &#039;&#039;&#039;32D&#039;&#039;&#039; (2008) P-2.058] (or [https://info.fusion.ciemat.es/OCS/EPS2008/pdf/P2_058.pdf 35th EPS Conference on Plasma Phys. Hersonissos, 9 - 13 June 2008 ECA Vol.32D, P-2.058 (2008)])&amp;lt;/ref&amp;gt;&lt;br /&gt;
The SIESTA code will complement other existent 3D MHD island solvers and is particularly suited for applications that require not only accuracy but speed of evaluation as well, such as experimental 3D equilibrium reconstruction or stellarator design. SIESTA will also be useful to calculate MHD equilibria at very high spatial resolutions, such as those that might be required for the investigation of NTMs at [[ITER]]-relevant temperature and resistivity conditions. SIESTA is based on a preconditioned, iterative algorithm that takes advantage of a pre-existent [[VMEC]] solution to provide both a background coordinate system that guarantees a compact representation as well as a good initial guess for the iterative procedure.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Category:Software]]&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=User:Admin&amp;diff=8676</id>
		<title>User:Admin</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=User:Admin&amp;diff=8676"/>
		<updated>2026-07-31T08:52:59Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* &amp;amp;ge; 2020 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[File:BvM.jpg|right|]]&lt;br /&gt;
== Personal information ==&lt;br /&gt;
__NOTOC__&lt;br /&gt;
* Boudewijn van Milligen (Admin)&lt;br /&gt;
* Researcher at: &amp;lt;br&amp;gt;[[Laboratorio Nacional de Fusión]] - [[CIEMAT]] &amp;lt;br&amp;gt;Avda. Complutense 40, Edif. 66&amp;lt;br&amp;gt;28040 Madrid, España - Spain&lt;br /&gt;
* Tel. +34 - 914 962 682&lt;br /&gt;
* Email boudewijn.vanmilligen (at) ciemat.es&lt;br /&gt;
User profiles:&lt;br /&gt;
* [https://publons.com/researcher/1248698/boudewijn-ph-van-milligen/ Publons] (ResearcherID H-5121-2015)&lt;br /&gt;
* [http://orcid.org/0000-0001-5344-6274 ORCID 0000-0001-5344-6274]&lt;br /&gt;
* [https://www.scopus.com/authid/detail.uri?authorId=35476190300 Scopus AuthorID 35476190300]&lt;br /&gt;
* [http://scholar.google.com/citations?user=7z9Cr9oAAAAJ Google Scholar]&lt;br /&gt;
* [https://www.researchgate.net/profile/Boudewijn_Van_Milligen/ ResearchGate]&lt;br /&gt;
&lt;br /&gt;
== Interests ==&lt;br /&gt;
&lt;br /&gt;
* Fusion and plasma physics&lt;br /&gt;
** [[H-mode|L-H transition]], Zonal Flows&lt;br /&gt;
** [[Magnetic island]]s, MHD activity&lt;br /&gt;
* [[Anomalous transport]]&lt;br /&gt;
** Turbulence&lt;br /&gt;
** Continuous Time Random Walks&lt;br /&gt;
* Data analysis&lt;br /&gt;
** [[Causality detection]]&lt;br /&gt;
** [[Intermittence]]&lt;br /&gt;
** [[:Wikipedia:Rescaled range|Rescaled range]] or [[:Wikipedia:Hurst exponent|Hurst]] analysis&lt;br /&gt;
** [[Bayesian data analysis]]&lt;br /&gt;
** [[Biorthogonal decomposition]]&lt;br /&gt;
** [[Bicoherence]]&lt;br /&gt;
** [[TJ-II:Tomography|Tomography]]&lt;br /&gt;
&lt;br /&gt;
== Book ==&lt;br /&gt;
&lt;br /&gt;
B.Ph. van Milligen and R. Sánchez, &#039;&#039;Analysis of Turbulence in Fusion Plasmas&#039;&#039;, [[doi:10.1088/978-0-7503-4856-0|IOP Publishing (2022)]], {{ISBN|978-0-7503-4854-6}}&lt;br /&gt;
&lt;br /&gt;
== Selected publications ==&lt;br /&gt;
&lt;br /&gt;
(inverse chronological order)&lt;br /&gt;
=== &amp;amp;ge; 2020 ===&lt;br /&gt;
* B.Ph. van Milligen, I. Voldiner, E. de la Cal, A. Alonso Alvarez, I. Luiz Caldas and Z. Guimarães Filho, &#039;&#039;Turbulence analysis with the spectroscopic gas puff imaging diagnostic in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/1361-6587/ae92b5|Plasma Phys. Control. Fusion (2026)]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* A. Alonso Alvarez, B. P. Van Milligen, I. Voldiner, I. L. Caldas, Z. Guimarães Filho, O. Kozachok, and A. Chmyga. &#039;&#039;Edge turbulence dynamics across electron–ion root transitions during ECRH modulation experiments in the TJ-II stellarator&#039;&#039;. [[doi:10.1088/1361-6587/ae7470|Plasma Phys. Control. Fusion, &#039;&#039;&#039;68&#039;&#039;&#039; (2026) 065019]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. van Milligen, I. García-Cortés, K.J. McCarthy, et al, &#039;&#039;The rotational transform and enhanced confinement in the TJ-II stellarator&#039;&#039;, [[doi:10.1017/S0022377825100433|Journal of Plasma Physics &#039;&#039;&#039;91&#039;&#039;&#039;, 4 (2025) E98]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* Boudewijn Philip van Milligen, Teresa Estrada, Benjamin Carreras, Luis García, and TJ-II Team. &#039;&#039;Importance of the Rotational Transform for L–H Transitions in the TJ-II Stellarator&#039;&#039; [[doi:10.3390/plasma7020024|Plasma &#039;&#039;&#039;7&#039;&#039;&#039;, no. 2 (2024) 446-464]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. van Milligen, I. Voldiner, B.A. Carreras, L. García, M.A. Ochando and The TJ-II Team, &#039;&#039;Rational surfaces, flows and radial structure in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/1741-4326/aca688|Nucl. Fusion &#039;&#039;&#039;63&#039;&#039;&#039; (2023) 016027]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. Van Milligen, B.A. Carreras, L. Garcia, G. Grenfell, I. Voldiner and C. Hidalgo, &#039;&#039;The impact of radial electric fields and plasma rotation on intermittence in TJ-II&#039;&#039;, [[doi:10.1088/1361-6587/ac54e9|Plasma Phys. Control. Fusion &#039;&#039;&#039;64&#039;&#039;&#039;, 5 (2022) 055006]] ([http://documenta.ciemat.es/handle/123456789/2290 repository])&lt;br /&gt;
* B. van Milligen, A. Melnikov, B. Carreras, L. Garcia, A. Kozachek, C. Hidalgo, J. de Pablos, Ph. Khabanov, L. Eliseev, M. Drabinskij, A. Chmyga, L. Krupnik, the HIBP Team, the TJ-II Team, &#039;&#039;Topology of 2-D turbulent structures based on intermittence in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/1741-4326/ac27c9|Nucl. Fusion &#039;&#039;&#039;61&#039;&#039;&#039;, 11 (2021) 116063]] ([http://documenta.ciemat.es/handle/123456789/2281 repository])&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras, I. Voldiner, U. Losada, C. Hidalgo, and the TJ-II Team, &#039;&#039;Causality, intermittence and crossphase evolution during confinement transitions in the TJ-II stellarator&#039;&#039;, [[doi:10.1063/5.0057791|Phys. Plasmas &#039;&#039;&#039;28&#039;&#039;&#039; (2021) 092302]] ([http://documenta.ciemat.es/handle/123456789/2289 repository])&lt;br /&gt;
* B.Ph. van Milligen, B. Carreras, L. García and C. Hidalgo, &#039;&#039;The localization of low order rational surfaces based on the intermittence parameter in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/1741-4326/ab79cc|Nucl. Fusion &#039;&#039;&#039;60&#039;&#039;&#039; (2020) 056010]] ([http://documenta.ciemat.es/handle/123456789/2291 repository])&lt;br /&gt;
&lt;br /&gt;
=== 2010-2019 ===&lt;br /&gt;
* B.Ph. van Milligen, B. Carreras, L. García and J. Nicolau, &#039;&#039;The radial propagation of heat in strongly driven non-equilibrium fusion plasmas&#039;&#039;, [[doi:10.3390/e21020148|Entropy, &#039;&#039;&#039;21&#039;&#039;&#039;, 2 (2019) 148]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. van Milligen, B. Carreras, E. de la Luna and E. Solano, &#039;&#039;Radial variation of heat transport in L-mode JET discharges&#039;&#039; [[doi:10.1088/1741-4326/ab03e1|Nucl. Fusion, &#039;&#039;&#039;59&#039;&#039;&#039; (2019) 056006]] ([http://documenta.ciemat.es/handle/123456789/2292 repository])&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras, C. Hidalgo, Á. Cappa and the TJ-II Team, &#039;&#039;A possible mechanism for confinement power degradation in the TJ-II stellarator&#039;&#039;, [[doi:10.1063/1.5029881|Phys. Plasmas &#039;&#039;&#039;25&#039;&#039;&#039; (2018) 062503]] ([http://documenta.ciemat.es/handle/123456789/2308 repository])&lt;br /&gt;
* B.Ph. van Milligen, U. Hoefel, J. Nicolau, M. Hirsch, L. García, B. Carreras, C. Hidalgo and the W7-X Team, &#039;&#039;Study of radial heat transport in W7-X using the transfer entropy&#039;&#039;, [[doi:10.1088/1741-4326/aabf5d|Nucl. Fusion &#039;&#039;&#039;58&#039;&#039;&#039; (2018) 076002]] ([http://hdl.handle.net/10016/32565 repository])&lt;br /&gt;
* B.Ph. van Milligen, J. Hernández Nicolau, B. Liu, G. Grenfell, U. Losada, B. Carreras, L. Garcia and C. Hidalgo, &#039;&#039;Filaments in the edge confinement region of TJ-II&#039;&#039;, [[doi:10.1088/1741-4326/aa9db6|Nucl. Fusion &#039;&#039;&#039;58&#039;&#039;&#039; (2018) 026030]] ([http://hdl.handle.net/10016/32563 repository])&lt;br /&gt;
* B.Ph. van Milligen, J.H. Nicolau, L. García, B.A. Carreras, C. Hidalgo and the TJ-II Team, &#039;&#039;The impact of rational surfaces on radial heat transport in TJ-II&#039;&#039;, [[doi:10.1088/1741-4326/aa611f|Nucl. Fusion &#039;&#039;&#039;57&#039;&#039;&#039;, 5 (2017) 056028]], [https://arxiv.org/abs/1701.04574 arxiv:1701.04574]&lt;br /&gt;
* B.Ph. van Milligen, T. Estrada, B.A. Carreras, E. Ascasíbar, C. Hidalgo, I. Pastor, J.M. Fontdecaba, R. Balbín and the TJ-II Team, &#039;&#039;The causal impact of magnetic fluctuations in slow and fast L–H transitions at TJ-II&#039;&#039;, [[doi:10.1063/1.4958807|Phys. Plasmas &#039;&#039;&#039;23&#039;&#039;&#039; (2016) 072305]], [https://arxiv.org/abs/1512.06525 arxiv:1512.06525]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras, L. García, A. Martín de Aguilera, C. Hidalgo, J.H. Nicolau and the TJ-II Team, &#039;&#039;The causal relation between turbulent particle flux and density gradient&#039;&#039;, [[doi:10.1063/1.4958806|Phys. Plasmas &#039;&#039;&#039;23&#039;&#039;&#039; (2016) 072307]]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras and D.E. Newman, &#039;&#039;Constructing criteria to diagnose the likelihood of extreme events in the case of the electric power grid&#039;&#039;, [[doi:10.1063/1.4943569|Chaos &#039;&#039;&#039;26&#039;&#039;&#039; (2016) 033109]]&lt;br /&gt;
* B.Ph. van Milligen, T. Estrada, L. García, D. López-Bruna, B. Carreras, Y. Xu, M. Ochando, C. Hidalgo, J. Reynolds-Barredo and A. López-Fraguas, &#039;&#039;The role of magnetic islands in modifying long range temporal correlations of density fluctuations and local heat transport&#039;&#039;, [[doi:10.1088/0029-5515/56/1/016013|Nucl. Fusion, &#039;&#039;&#039;56&#039;&#039;&#039;, 1 (2016) 016013]], [https://arxiv.org/abs/1506.06890 arxiv:1506.06890]&lt;br /&gt;
* B.Ph. van Milligen, E. Sánchez, A. Alonso, M.A. Pedrosa, C. Hidalgo, A. Martín de Aguilera, A. López Fraguas, &#039;&#039;The use of the Biorthogonal Decomposition for the identification of zonal flows at TJ-II&#039;&#039;, [[doi:10.1088/0741-3335/57/2/025005|Plasma Phys. Control. Fusion &#039;&#039;&#039;57&#039;&#039;&#039;, 2 (2015) 025005]], [https://arxiv.org/abs/1408.1845 arxiv:1408.1845]&lt;br /&gt;
* B.Ph. van Milligen, P.D. Bons, &#039;&#039;Simplified numerical model for clarifying scaling behavior in the intermediate dispersion regime in homogeneous porous media&#039;&#039;, [[doi:10.1016/j.cpc.2014.09.006|Comput. Phys. Commun. &#039;&#039;&#039;185&#039;&#039;&#039; (2014) 3291]], [https://arxiv.org/abs/1409.2724 arxiv:1409.2724]&lt;br /&gt;
* B.Ph. van Milligen, G. Birkenmeier, M. Ramisch, T. Estrada, C. Hidalgo and A. Alonso, &#039;&#039;Causality detection and turbulence in fusion plasmas&#039;&#039;, [[doi:10.1088/0029-5515/54/2/023011|Nucl. Fusion &#039;&#039;&#039;54&#039;&#039;&#039; (2014), 023011]], [https://arxiv.org/abs/1309.7769 arxiv:1309.7769]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Parallel and perpendicular turbulence correlation length in the TJ-II Stellarator&#039;&#039;, [[doi:10.1088/0029-5515/53/9/093025|Nucl. Fusion &#039;&#039;&#039;53&#039;&#039;&#039; (2013) 093025]], [https://arxiv.org/abs/1306.1395 arxiv:1306.1395]&lt;br /&gt;
* P.D. Bons, B.Ph. van Milligen, P. Blum, &#039;&#039;A general unified expression for solute and heat dispersion in homogeneous porous media&#039;&#039;, [[doi:10.1002/wrcr.20488|Water Resour. Res. &#039;&#039;&#039;49&#039;&#039;&#039; (2013) 1]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Spatiotemporal and wavenumber resolved bicoherence at the low to high confinement transition in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/53/11/113034|Nucl. Fusion &#039;&#039;&#039;53&#039;&#039;&#039; (2013) 113034]], [https://arxiv.org/abs/1211.0420 arxiv:1211.0420]&lt;br /&gt;
* B. Ph. van Milligen, R. Sánchez and C. Hidalgo, &#039;&#039;Relevance of Uncorrelated Lorentzian Pulses for the Interpretation of Turbulence in the Edge of Magnetically Confined Toroidal Plasmas&#039;&#039;, [[doi:10.1103/PhysRevLett.109.105001|Phys. Rev. Lett. &#039;&#039;&#039;109&#039;&#039;&#039; (2012) 105001]], [https://arxiv.org/abs/1204.6185 arxiv:1204.6185]&lt;br /&gt;
* B.Ph. van Milligen, P.D. Bons, &#039;&#039;Analytical model for tracer dispersion in porous media&#039;&#039;, [[doi:10.1103/PhysRevE.85.011306|Phys. Rev. E 85 (2012) 011306]], [https://arxiv.org/abs/1111.6512 arxiv:1111.6512]&lt;br /&gt;
* B.Ph. van Milligen, L. García, B.A. Carreras, M.A. Pedrosa, C. Hidalgo, J.A. Alonso, T. Estrada and E. Ascasíbar, &#039;&#039;MHD mode activity and the velocity shear layer at TJ-II&#039;&#039;, [[doi:10.1088/0029-5515/52/1/013006|Nucl. Fusion &#039;&#039;&#039;52&#039;&#039;&#039; (2012) 013006]]&lt;br /&gt;
* B.Ph. van Milligen, T. Estrada, E. Ascasíbar, et al, &#039;&#039;Integrated data analysis at TJ-II: the density profile&#039;&#039;, [[doi:10.1063/1.3608551|Rev. Sci. Instrum. &#039;&#039;&#039;82&#039;&#039;&#039; (2011) 073503]]&lt;br /&gt;
* B.A. Carreras et al., &#039;&#039;Reconstruction of intermittent waveforms associated with the zonal flow at the transition leading to the edge shear flow layer&#039;&#039;, [[doi:10.1088/0029-5515/51/5/053022|Nucl. Fusion &#039;&#039;&#039;51&#039;&#039;&#039; (2011) 053022]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;A global resonance phenomenon at the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/51/1/013005|Nucl. Fusion &#039;&#039;&#039;51&#039;&#039;&#039; (2011) 013005]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;The dynamics of the formation of the edge particle transport barrier at TJ-II&#039;&#039;, [[doi:10.1088/0029-5515/51/11/113002|Nucl. Fusion &#039;&#039;&#039;51&#039;&#039;&#039; (2011) 113002]]&lt;br /&gt;
&lt;br /&gt;
=== 2000-2009 ===&lt;br /&gt;
* B.Ph. van Milligen, I. Calvo and R. Sánchez, &#039;&#039;Continuous time random walks in finite domains and general boundary conditions: some formal considerations&#039;&#039;, [[doi:10.1088/1751-8113/41/21/215004|J. Phys. A: Math. Theor. &#039;&#039;&#039;41&#039;&#039;&#039; (2008) 215004]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Quantifying profile stiffness&#039;&#039;, [http://www.jspf.or.jp/PFR/PFR_articles/pfr2008S1/pfr2008_03-S1070.html Plasma and Fusion Research, &#039;&#039;&#039;3&#039;&#039;&#039; (2008) S1070]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Bicoherence during confinement transitions in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/48/11/115003|Nucl. Fusion &#039;&#039;&#039;48&#039;&#039;&#039; (2008) 115003]]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras, V.E. Lynch and R. Sánchez, &#039;&#039;Pulse propagation in a simple probabilistic transport model&#039;&#039;, [[doi:10.1088/0029-5515/47/3/004|Nucl. Fusion &#039;&#039;&#039;47&#039;&#039;&#039; (2007) 189]]&lt;br /&gt;
* B.Ph. van Milligen, P.D. Bons, B.A. Carreras and R. Sánchez, &#039;&#039;On the applicability of Fick&#039;s Law to diffusion in inhomogeneous systems&#039;&#039;, [[doi:10.1088/0143-0807/26/5/023|Eur. J. Phys. &#039;&#039;&#039;26&#039;&#039;&#039; (2005) 913]]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras and R. Sánchez, &#039;&#039;The foundations of diffusion revisited&#039;&#039;, [[doi:10.1088/0741-3335/47/12B/S56|Plasma Phys. Control. Fusion &#039;&#039;&#039;47&#039;&#039;&#039; (2005) B743]]&lt;br /&gt;
* B.Ph. Van Milligen et al, &#039;&#039;Additional evidence for the universality of turbulent fluctuations and fluxes in the scrape-off layer region of fusion plasmas&#039;&#039;, [[doi:10.1063/1.1884615|Phys. Plasmas &#039;&#039;&#039;12&#039;&#039;&#039; (2005) 052507]]&lt;br /&gt;
* B.Ph. van Milligen, R. Sánchez and B.A. Carreras, &#039;&#039;Probabilistic finite-size transport models for fusion: anomalous transport and scaling laws&#039;&#039;, [[doi:10.1063/1.1701893|Phys. Plasmas &#039;&#039;&#039;11&#039;&#039;&#039;, 5 (2004) 2272]]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras and R. Sánchez, &#039;&#039;Uphill transport and the probabilistic transport model&#039;&#039;, [[doi:10.1063/1.1763915|Phys. Plasmas &#039;&#039;&#039;11&#039;&#039;&#039;, 3787 (2004)]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Revision of TV Thomson scattering data analysis and detection of profile structure&#039;&#039;, [[doi:10.1063/1.1597951|Rev. Sci. Instrum. &#039;&#039;&#039;74&#039;&#039;&#039; (2003) 3998]]&lt;br /&gt;
* B.Ph. van Milligen, E. de la Luna, F.L. Tabarés, et al., &#039;&#039;Ballistic transport phenomena in TJ-II&#039;&#039;, [[doi:10.1088/0029-5515/42/7/301|Nucl. Fusion &#039;&#039;&#039;42&#039;&#039;&#039; (2002) 787]]&lt;br /&gt;
=== 1990 - 1999 ===&lt;br /&gt;
* B.A. Carreras, B.Ph. van Milligen, et al, &#039;&#039;Experimental evidence of long-range correlation and self-similarity in plasma fluctuations&#039;&#039;, [[doi:10.1063/1.873490|Phys. Plasmas &#039;&#039;&#039;6&#039;&#039;&#039;, 5 (1999) 1885]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Statistically robust linear and non-linear wavelet analysis applied to plasma edge turbulence&#039;&#039;, [[doi:10.1063/1.1147727|Rev. Sci. Instrum. &#039;&#039;&#039;68&#039;&#039;&#039; (1997) 967]]&lt;br /&gt;
* B.Ph. van Milligen, V. Tribaldos, J.A. Jiménez, &#039;&#039;A neural network differential equation and plasma equilibrium solver&#039;&#039;, [[doi:10.1103/PhysRevLett.75.3594|Phys. Rev. Lett. &#039;&#039;&#039;75&#039;&#039;&#039; (1995) 3594]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Nonlinear phenomena and intermittency in plasma turbulence&#039;&#039;, [[doi:10.1103/PhysRevLett.74.395|Phys. Rev. Lett. &#039;&#039;&#039;74&#039;&#039;&#039;, 3 (1995) 395]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Wavelet bicoherence: a new turbulence analysis tool&#039;&#039;, [[doi:10.1063/1.871199|Phys. Plasmas &#039;&#039;&#039;2&#039;&#039;&#039;, 8 (1995) 3017]]&lt;br /&gt;
* B.Ph. van Milligen and A. Lopez Fraguas, &#039;&#039;Expansion of vacuum magnetic fields in toroidal harmonics&#039;&#039;, [[doi:10.1016/0010-4655(94)90112-0|Comput. Phys. Commun. &#039;&#039;&#039;81&#039;&#039;&#039;, Issues 1-2 (1994) 74-90]]&lt;br /&gt;
* B.Ph. van Milligen, A.C.A.P. van Lammeren, N.J. Lopes Cardozo, F.C. Schüller and M. Verreck, &#039;&#039;Gradients of electron temperature and density across m=2 islands in RTP&#039;&#039;, [[doi:10.1088/0029-5515/33/8/I03|Nucl. Fusion &#039;&#039;&#039;33&#039;&#039;&#039; (1993) 1119]]&lt;br /&gt;
* B.Ph. van Milligen, N.J. Lopes Cardozo, &#039;&#039;Function Parametrization: a fast inverse mapping method&#039;&#039;, [[doi:10.1016/0010-4655(91)90073-T|Comput. Phys. Commun. &#039;&#039;&#039;66&#039;&#039;&#039; (1991) 243]]&lt;br /&gt;
* B.Ph. van Milligen et al., &#039;&#039;Application of Function Parametrization to the analysis of polarimetry and interferometry data in TEXTOR&#039;&#039;, [[doi:10.1088/0029-5515/31/2/007|Nucl. Fusion &#039;&#039;&#039;31&#039;&#039;&#039; (1991) 309]]&lt;br /&gt;
* B.Ph. van Milligen, &#039;&#039;Exact relations between multipole moments of the flux and moments of the toroidal current density in tokamaks&#039;&#039;, [[doi:10.1088/0029-5515/30/1/012|Nucl. Fusion &#039;&#039;&#039;30&#039;&#039;&#039; (1990) 157]]&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=LNF:Nationally_Funded_Projects&amp;diff=8671</id>
		<title>LNF:Nationally Funded Projects</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=LNF:Nationally_Funded_Projects&amp;diff=8671"/>
		<updated>2026-07-20T16:45:37Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* Instructions to add a new project to the list */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Nationally funded projects of the [[Laboratorio Nacional de Fusión]].&lt;br /&gt;
&lt;br /&gt;
== LNF - Nationally funded projects ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;categorytree mode=&amp;quot;pages&amp;quot;&amp;gt;LNF Nationally Funded Projects - finished&amp;lt;/categorytree&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;categorytree mode=&amp;quot;pages&amp;quot;&amp;gt;LNF Nationally Funded Projects&amp;lt;/categorytree&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&amp;lt;div align=&amp;quot;center&amp;quot;&amp;gt; &lt;br /&gt;
{|&lt;br /&gt;
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{|&lt;br /&gt;
! &amp;lt;p style=&amp;quot;margin:3px; font-size:120%; font-weight:bold; text-align:center; padding:0.2em 0.4em&amp;quot;&amp;gt; &lt;br /&gt;
[https://www.aei.gob.es/sites/default/files/inline-files/20250331_Guia%20comunicacion%20publicidad%20ayudas_v01.pdf Instrucciones relativas a los requisitos de publicidad en proyectos de los planes nacionales (Marzo/2025)] &amp;lt;/p&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Instructions to add a new project to the list ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;Please read the following brief instructions&#039;&#039;&lt;br /&gt;
# Log in to the FusionWiki. If you don&#039;t have an account, request one by clicking &#039;Create account&#039; in the left-hand menu.&lt;br /&gt;
# &amp;lt;font color=&amp;quot;#FF0000&amp;quot;&amp;gt;&#039;&#039;Type the name of your project page in the field below&#039;&#039;&amp;lt;/font&amp;gt;. The required format is: &#039;LNF:Title of my project&#039; (without the apostrophes). Note the &#039;LNF:&#039; at the beginning!&lt;br /&gt;
# Click &#039;Create new project page&#039;. Your project page will be created. Edit and save (please use &#039;Show preview&#039; before saving the final version).&lt;br /&gt;
# Use the template provided to provide the project information&lt;br /&gt;
# The page can be written in English or Spanish &lt;br /&gt;
# The page must include at the top of the page the logo and the text for the acknowledgement associated with the type of project/year (see the link above)&lt;br /&gt;
&lt;br /&gt;
&amp;lt;inputbox&amp;gt;&lt;br /&gt;
type=create&lt;br /&gt;
placeholder=LNF:Title of my project&lt;br /&gt;
buttonlabel=Create new project page with this title&lt;br /&gt;
preload=LNF:Project_template&lt;br /&gt;
&amp;lt;/inputbox&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Once you save the new project page, it will automatically be included in the list above (&#039;&#039;&#039;provided&#039;&#039;&#039; you don&#039;t delete the relevant lines at the end of your project page).&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=LNF:Project_template&amp;diff=8662</id>
		<title>LNF:Project template</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=LNF:Project_template&amp;diff=8662"/>
		<updated>2026-07-20T09:45:34Z</updated>

		<summary type="html">&lt;p&gt;Admin: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== LNF - Nationally funded project ==&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Title&#039;&#039;&#039;: &#039;&#039;&#039;Enter Title here&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Reference&#039;&#039;&#039;: Referencia Plan Nacional&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Programme and date&#039;&#039;&#039;: Proyectos de ... Año&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Programme type (Modalidad de proyecto)&#039;&#039;&#039;: &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Area/subarea (Área temática / subárea)&#039;&#039;&#039;: &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Principal Investigator(s)&#039;&#039;&#039;: [https://orcid.org/0000-0000-0000-0000 John Doe]&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Project type&#039;&#039;&#039;: Proyecto individual / coordinado&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Start-end dates&#039;&#039;&#039;: dd/mm/yyyy - dd/mm/yyyy&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Financing granted (direct costs)&#039;&#039;&#039;: 0 €&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Acknowledgement&#039;&#039;&#039;: Grant ´´´Referencia del proyecto´´´ funded by MICIU/AEI/ 10.13039/501100011033 and by “ERDF/EU”. &lt;br /&gt;
&lt;br /&gt;
[[File:LogoOficial_PlanNacional_2021.png|500px]] &lt;br /&gt;
&#039;&#039; Este logo y el texto para los agradecimientos en las publicaciones son válidos para proyectos de «Generación de Conocimiento» de 2021, 2022, 2023, 2024 (mas información en el link at final de la pagina)&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
== Description of the project ==&lt;br /&gt;
&lt;br /&gt;
Enter text here&lt;br /&gt;
&lt;br /&gt;
&amp;lt;!-- If applicable: references --&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Project documentation ==&lt;br /&gt;
&lt;br /&gt;
(Optional) Add the project proposal and the final report at the end of the project, and any other information related with the project&lt;br /&gt;
&lt;br /&gt;
== Main results ==&lt;br /&gt;
&lt;br /&gt;
Enter text here (summary of main project results from the final report)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Dissemination of project results (peer-reviewed publications and conference presentations) ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;!-- If applicable: references --&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references /&amp;gt; &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039; DO NOT FORGET TO ADD THE CORRESPONDING LOGO AT THE BOTTOM OF THE PAGE (see the link provided in the main page)&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;!-- DO NOT REMOVE THE FOLLOWING LINES --&amp;gt;&lt;br /&gt;
&amp;lt;hr&amp;gt;&lt;br /&gt;
[[LNF:Nationally Funded Projects|Back to list of nationally funded projects]]&lt;br /&gt;
&lt;br /&gt;
[[Category:LNF Nationally Funded Projects]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;!-- Change category to [[Category:LNF Nationally Funded Projects - finished]] once the project is finished --&amp;gt;&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=Journals&amp;diff=8651</id>
		<title>Journals</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=Journals&amp;diff=8651"/>
		<updated>2026-07-15T07:56:33Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* Computation */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This page is meant to provide an overview of (scientific) journals of relevance for fusion and plasma physics, along with a description of their focus and impact (IF = [[:Wikipedia:Impact factor|Impact factor]]). Such a list could be helpful to choose the optimal forum for a publication. It is in need of expansion (please help).&lt;br /&gt;
&lt;br /&gt;
== Fusion and plasma physics ==&lt;br /&gt;
{|class=&amp;quot;wikitable sortable&amp;quot; style=&amp;quot;width: 100%&amp;quot;&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;35%&amp;quot; | Journal (publisher)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;45%&amp;quot; | Description&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | IF (year)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/0029-5515 Nuclear Fusion] (IOP) &lt;br /&gt;
| The journal covers all aspects of research, theoretical and practical, relevant to controlled thermonuclear fusion.&lt;br /&gt;
| 3.307 (2016) 3.5 (2023)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/0963-0252/ Plasma Sources Science and Technology] (IOP)&lt;br /&gt;
| A single interdisciplinary forum for physicists, engineers and materials scientists working in the increasingly significant field of low-temperature plasma science.&lt;br /&gt;
| 3.302 (2016) 3.3 (2023)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/0741-3335 Plasma Physics and Controlled Fusion] (IOP) &lt;br /&gt;
| Covering all aspects of the physics of hot, highly ionised plasmas in the laboratory, the ionosphere and in space as well as in magnetic and inertial-confinement fusion.&lt;br /&gt;
| 2.392 (2016) 2.1 (2023)&lt;br /&gt;
|-&lt;br /&gt;
| [http://pop.aip.org/ Physics of Plasmas] (AIP) &lt;br /&gt;
| Physics of Plasmas, published by the American Institute of Physics with the cooperation of The American Physical Society, Division of Plasma Physics, is devoted to original experimental and theoretical contributions to the physics of plasmas.&lt;br /&gt;
| 2.115 (2016) 2.0 (2023)&lt;br /&gt;
|-&lt;br /&gt;
| [https://www.journals.elsevier.com/journal-of-nuclear-materials Journal of Nuclear Materials] (Elsevier) &lt;br /&gt;
| The Journal of Nuclear Materials publishes high quality papers in materials research for nuclear applications, primarily fission reactors, fusion reactors, and similar environments including radiation areas of charged particle accelerators.&lt;br /&gt;
| 2.048 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [https://www.mdpi.com/journal/plasma Plasma] (MDPI) &lt;br /&gt;
| Plasma is an international, open access, peer-reviewed journal covering all aspects of plasma science, published quarterly online by MDPI.&lt;br /&gt;
| 1.9 (2023)&lt;br /&gt;
|-&lt;br /&gt;
| [http://onlinelibrary.wiley.com/journal/10.1002/%28ISSN%291521-3986 Contributions to Plasma Physics] (Wiley) &lt;br /&gt;
| Basic physics of low-temperature plasmas; Strongly correlated non-ideal plasmas; Plasma discharges - microplasmas, reactive, and atmospheric pressure plasmas; Plasma diagnostics; Plasma-surface interaction; Plasma technology; Plasma medicine&lt;br /&gt;
| 1.44 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://journals.cambridge.org/action/displayJournal?jid=PLA Journal of Plasma Physics] (Cambridge) &lt;br /&gt;
| JPP aspires to be the intellectual home of those who think of plasma physics as a fundamental discipline. The journal will particularly focus on publishing research on laboratory plasmas, space physics and plasma astrophysics that takes advantage of the rapid ongoing progress in instrumentation and computing to advance fundamental understanding of multiscale plasma physics. The Journal welcomes submissions of analytical, numerical and experimental work: both original research and tutorial- or review-style papers, as well as proposals for its Lecture Notes series.&lt;br /&gt;
| 1.16 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.sciencedirect.com/science/journal/09203796 Fusion Engineering and Design] (Elsevier)&lt;br /&gt;
| The journal accepts papers about experiments (both plasma and technology), theory, models, methods, and designs in areas relating to technology, engineering, and applied science aspects of magnetic and inertial fusion energy. &lt;br /&gt;
| 1.14 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://ieeexplore.ieee.org/servlet/opac?punumber=27 IEEE Transactions on Plasma Science] (IEEE) &lt;br /&gt;
| Plasma science and engineering, including: magnetofluid dynamics and thermionics; plasma dynamics; gaseous electronics and arc technology; controlled thermonuclear fusion; electron, ion, and plasma sources; space plasmas; high-current relativistic electron beams; laser-plasma interactions; diagnostics; plasma chemistry and colloidal and solid-state plasmas. &lt;br /&gt;
| 1.052 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.springer.com/physics/atomic%2C+molecular%2C+optical+%26+plasma+physics/journal/11452 Plasma Physics Reports] (Springer)&lt;br /&gt;
| The journal covers the following topics: high-temperature plasma physics related to the problem of controlled nuclear fusion based on magnetic and inertial confinement; physics of cosmic plasma, including magnetosphere plasma, sun and stellar plasma, etc.; gas discharge plasma and plasma generated by laser and particle beams. The journal also publishes papers on such related topics as plasma electronics, generation of radiation in plasma, and plasma diagnostics.&lt;br /&gt;
| 0.984 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [https://link.springer.com/journal/10894 Journal of Fusion Energy] (Springer)&lt;br /&gt;
| The Journal of Fusion Energy features contributions and review papers pertinent to the development of thermonuclear fusion as a useful power source. Intended to serve as a journal of record for publication of research results, the journal also provides a forum for discussion of the broader policy and planning issues that have played, and will continue to play, a crucial role in the fusion program. &lt;br /&gt;
| 0.858 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/1009-0630/ Plasma Science and Technology] (IOP)&lt;br /&gt;
| PST publishes novel experimental and theoretical results showing progress of interdisciplinary and application sciences in the fields related to plasma physics.&lt;br /&gt;
| 0.83 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://epubs.ans.org/?p=fst Fusion Science and Technology] (ANS)&lt;br /&gt;
| Fusion Science and Technology (FST) is the leading source of information on fusion plasma physics and plasma engineering, fusion plasma enabling science and technology, fusion nuclear technology and material science, fusion applications, fusion design and system studies.&lt;br /&gt;
| 0.578 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [https://www.tandfonline.com/loi/grad20 Radiation Effects and Defects in Solids] (Taylor &amp;amp; Francis)&lt;br /&gt;
| The Journal covers a wide range of topics under radiation and plasma sciences. The range of contributions encompasses: radiation physics; radiochemistry, radiobiology and physical effects of medical irradiation, including research on radiative cell degeneration; optical, electrical and mechanical effects of radiation, and their secondary effects such as diffusion and particle emission from surfaces; plasma techniques and plasma phenomena. On plasma science the Journal covers all areas of fusion, space and low temperature plasmas.&lt;br /&gt;
| 0.443 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.jspf.or.jp/PFR/ Plasma and Fusion Research] (Japan Society of Plasma Science and Nuclear Fusion Research)&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.jspf.or.jp/JPFRS/ Journal of Plasma and Fusion Research SERIES] (Japan Society of Plasma Science and Nuclear Fusion Research)&lt;br /&gt;
|&lt;br /&gt;
| &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Computation ==&lt;br /&gt;
{|class=&amp;quot;wikitable sortable&amp;quot; style=&amp;quot;width: 100%&amp;quot;&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;35%&amp;quot; | Journal (publisher)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;45%&amp;quot; | Description&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | IF (year)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.sciencedirect.com/science/journal/00104655 Computer Physics Communications] (Elsevier) &lt;br /&gt;
| Computer Physics Communications publishes research papers and computer program descriptions in computational physics and physical chemistry: the focus is on computational methods and techniques rather than results. &lt;br /&gt;
| 3.936 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.journals.elsevier.com/journal-of-computational-physics/ Journal of Computational Physics] (Elsevier) &lt;br /&gt;
| Journal of Computational Physics thoroughly treats the computational aspects of physical problems, presenting techniques for the numerical solution of mathematical equations arising in all areas of physics. The journal seeks to emphasize methods that cross disciplinary boundaries. &lt;br /&gt;
| 2.744 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [https://journals.plos.org/ PLoS One]  &lt;br /&gt;
|  &lt;br /&gt;
| See [https://plos.org/metrics/ PLoS One metrics]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== General physics ==&lt;br /&gt;
{|class=&amp;quot;wikitable sortable&amp;quot; style=&amp;quot;width: 100%&amp;quot;&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;35%&amp;quot; | Journal (publisher)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;45%&amp;quot; | Description&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | IF (year)&lt;br /&gt;
|-&lt;br /&gt;
| [http://rmp.aps.org/ Reviews of Modern Physics] (APS) &lt;br /&gt;
| Reviews of Modern Physics (RMP) is the world’s premier physics review journal and the most highly cited Physical Review publication. Written by leading international researchers, RMP’s in-depth essays provide outstanding coverage of a topic and give context and background for current research trends.&lt;br /&gt;
| 36.917 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.nature.com/nphys/ Nature Physics] &lt;br /&gt;
| Nature Physics publishes papers of the highest quality and significance in all areas of physics, pure and applied. The journal&#039;s content reflects core physics disciplines, but is also open to a broad range of topics whose central theme falls within the bounds of physics. Theoretical physics, particularly where it is pertinent to experiment, also features. &lt;br /&gt;
| 22.806 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://prl.aps.org/ Physical Review Letters] (APS)&lt;br /&gt;
| Physical Review Letters (PRL) is the world’s premier physics letter journal and the American Physical Society’s flagship publication. Since 1958 it has contributed to APS’s mission to advance and diffuse the knowledge of physics by publishing seminal research by Nobel Prize–winning and other distinguished researchers in all fields of physics.&lt;br /&gt;
| 8.462 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://pre.aps.org/ Physical Review E] (APS)&lt;br /&gt;
| Physical Review E, interdisciplinary in scope, focuses on many-body phenomena, including recent developments in quantum and classical chaos and soft matter physics. It has sections on statistical physics, equilibrium and transport properties of fluids, liquid crystals, complex fluids, polymers, chaos, fluid dynamics, plasma physics, classical physics, and computational physics. In addition, the journal features sections on two rapidly growing areas: biological physics and granular materials.&lt;br /&gt;
| 2.366 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/0295-5075/ Europhysics Letters] (IOP)&lt;br /&gt;
| EPL publishes original, high-quality Letters in all areas of physics, ranging from condensed matter topics and interdisciplinary research to astrophysics, geophysics, plasma and fusion sciences, including those with application potential. &lt;br /&gt;
| 1.957 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://rsi.aip.org/ Review of Scientific Instruments] (AIP)&lt;br /&gt;
| Review of Scientific Instruments (RSI) publishes novel advancements in scientific instrumentation, apparatuses, techniques of experimental measurement, and related mathematical analysis.&lt;br /&gt;
| 1.515 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.springer.com/physics/atomic%2C+molecular%2C+optical+%26+plasma+physics/journal/10053 European Physical Journal D] (Springer)&lt;br /&gt;
| Atomic, Molecular, Optical and Plasma Physics&lt;br /&gt;
| 1.288 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/1402-4896/ Physica Scripta] (IOP)&lt;br /&gt;
| Physica Scripta, endorsed by The Royal Swedish Academy of Sciences, is an international journal dedicated to presenting novel and accessible research findings across the breadth of theoretical and experimental physics.&lt;br /&gt;
| 1.28 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/0143-0807 European Journal of Physics] (IOP)&lt;br /&gt;
| With a world-wide readership and authors from every continent, European Journal of Physics is a truly international journal dedicated to maintaining and improving the standard of taught physics in universities and other higher education institutes.&lt;br /&gt;
| 0.614 (2016)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== General science ==&lt;br /&gt;
{|class=&amp;quot;wikitable sortable&amp;quot; style=&amp;quot;width: 100%&amp;quot; &lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;35%&amp;quot; | Journal (publisher)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;45%&amp;quot; | Description&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | IF (year)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.nature.com/ Nature] &lt;br /&gt;
|&lt;br /&gt;
| 40.137 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.sciencemag.org/ Science]&lt;br /&gt;
| &lt;br /&gt;
| 37.205 (2016)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Preprint servers ==&lt;br /&gt;
&lt;br /&gt;
{|class=&amp;quot;wikitable sortable&amp;quot; style=&amp;quot;width: 100%&amp;quot; &lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;35%&amp;quot; | Journal (publisher)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;45%&amp;quot; | Description&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | IF (year)&lt;br /&gt;
|-&lt;br /&gt;
| [http://arxiv.org/list/physics.plasm-ph/recent ArXiV] &lt;br /&gt;
| Non-refereed preprint service&lt;br /&gt;
| &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Institutional repositories ==&lt;br /&gt;
&lt;br /&gt;
{|class=&amp;quot;wikitable sortable&amp;quot; style=&amp;quot;width: 100%&amp;quot; &lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;35%&amp;quot; | Repository&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;45%&amp;quot; | Description&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | IF (year)&lt;br /&gt;
|-&lt;br /&gt;
| [http://documenta.ciemat.es CIEMAT] &lt;br /&gt;
| Repository&lt;br /&gt;
| &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Impact factors ==&lt;br /&gt;
&lt;br /&gt;
Older journal impact factors can be found here:&lt;br /&gt;
* [https://info.fusion.ciemat.es/media/IF_1992-2009.zip Impact Factors 1992-2009] (zip file, 23 MB)&lt;br /&gt;
* [https://info.fusion.ciemat.es/media/JCR_1979_1997.zip Impact Factors 1979-1997] (zip file, 115 MB)&lt;br /&gt;
&lt;br /&gt;
== Note ==&lt;br /&gt;
&lt;br /&gt;
Journal abbreviations in citations are standardized. Consult the [http://www.issn.org/2-22660-LTWA.php LTWA].&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Books]]&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=Journals&amp;diff=8650</id>
		<title>Journals</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=Journals&amp;diff=8650"/>
		<updated>2026-07-15T07:50:09Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* Computation */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This page is meant to provide an overview of (scientific) journals of relevance for fusion and plasma physics, along with a description of their focus and impact (IF = [[:Wikipedia:Impact factor|Impact factor]]). Such a list could be helpful to choose the optimal forum for a publication. It is in need of expansion (please help).&lt;br /&gt;
&lt;br /&gt;
== Fusion and plasma physics ==&lt;br /&gt;
{|class=&amp;quot;wikitable sortable&amp;quot; style=&amp;quot;width: 100%&amp;quot;&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;35%&amp;quot; | Journal (publisher)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;45%&amp;quot; | Description&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | IF (year)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/0029-5515 Nuclear Fusion] (IOP) &lt;br /&gt;
| The journal covers all aspects of research, theoretical and practical, relevant to controlled thermonuclear fusion.&lt;br /&gt;
| 3.307 (2016) 3.5 (2023)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/0963-0252/ Plasma Sources Science and Technology] (IOP)&lt;br /&gt;
| A single interdisciplinary forum for physicists, engineers and materials scientists working in the increasingly significant field of low-temperature plasma science.&lt;br /&gt;
| 3.302 (2016) 3.3 (2023)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/0741-3335 Plasma Physics and Controlled Fusion] (IOP) &lt;br /&gt;
| Covering all aspects of the physics of hot, highly ionised plasmas in the laboratory, the ionosphere and in space as well as in magnetic and inertial-confinement fusion.&lt;br /&gt;
| 2.392 (2016) 2.1 (2023)&lt;br /&gt;
|-&lt;br /&gt;
| [http://pop.aip.org/ Physics of Plasmas] (AIP) &lt;br /&gt;
| Physics of Plasmas, published by the American Institute of Physics with the cooperation of The American Physical Society, Division of Plasma Physics, is devoted to original experimental and theoretical contributions to the physics of plasmas.&lt;br /&gt;
| 2.115 (2016) 2.0 (2023)&lt;br /&gt;
|-&lt;br /&gt;
| [https://www.journals.elsevier.com/journal-of-nuclear-materials Journal of Nuclear Materials] (Elsevier) &lt;br /&gt;
| The Journal of Nuclear Materials publishes high quality papers in materials research for nuclear applications, primarily fission reactors, fusion reactors, and similar environments including radiation areas of charged particle accelerators.&lt;br /&gt;
| 2.048 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [https://www.mdpi.com/journal/plasma Plasma] (MDPI) &lt;br /&gt;
| Plasma is an international, open access, peer-reviewed journal covering all aspects of plasma science, published quarterly online by MDPI.&lt;br /&gt;
| 1.9 (2023)&lt;br /&gt;
|-&lt;br /&gt;
| [http://onlinelibrary.wiley.com/journal/10.1002/%28ISSN%291521-3986 Contributions to Plasma Physics] (Wiley) &lt;br /&gt;
| Basic physics of low-temperature plasmas; Strongly correlated non-ideal plasmas; Plasma discharges - microplasmas, reactive, and atmospheric pressure plasmas; Plasma diagnostics; Plasma-surface interaction; Plasma technology; Plasma medicine&lt;br /&gt;
| 1.44 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://journals.cambridge.org/action/displayJournal?jid=PLA Journal of Plasma Physics] (Cambridge) &lt;br /&gt;
| JPP aspires to be the intellectual home of those who think of plasma physics as a fundamental discipline. The journal will particularly focus on publishing research on laboratory plasmas, space physics and plasma astrophysics that takes advantage of the rapid ongoing progress in instrumentation and computing to advance fundamental understanding of multiscale plasma physics. The Journal welcomes submissions of analytical, numerical and experimental work: both original research and tutorial- or review-style papers, as well as proposals for its Lecture Notes series.&lt;br /&gt;
| 1.16 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.sciencedirect.com/science/journal/09203796 Fusion Engineering and Design] (Elsevier)&lt;br /&gt;
| The journal accepts papers about experiments (both plasma and technology), theory, models, methods, and designs in areas relating to technology, engineering, and applied science aspects of magnetic and inertial fusion energy. &lt;br /&gt;
| 1.14 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://ieeexplore.ieee.org/servlet/opac?punumber=27 IEEE Transactions on Plasma Science] (IEEE) &lt;br /&gt;
| Plasma science and engineering, including: magnetofluid dynamics and thermionics; plasma dynamics; gaseous electronics and arc technology; controlled thermonuclear fusion; electron, ion, and plasma sources; space plasmas; high-current relativistic electron beams; laser-plasma interactions; diagnostics; plasma chemistry and colloidal and solid-state plasmas. &lt;br /&gt;
| 1.052 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.springer.com/physics/atomic%2C+molecular%2C+optical+%26+plasma+physics/journal/11452 Plasma Physics Reports] (Springer)&lt;br /&gt;
| The journal covers the following topics: high-temperature plasma physics related to the problem of controlled nuclear fusion based on magnetic and inertial confinement; physics of cosmic plasma, including magnetosphere plasma, sun and stellar plasma, etc.; gas discharge plasma and plasma generated by laser and particle beams. The journal also publishes papers on such related topics as plasma electronics, generation of radiation in plasma, and plasma diagnostics.&lt;br /&gt;
| 0.984 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [https://link.springer.com/journal/10894 Journal of Fusion Energy] (Springer)&lt;br /&gt;
| The Journal of Fusion Energy features contributions and review papers pertinent to the development of thermonuclear fusion as a useful power source. Intended to serve as a journal of record for publication of research results, the journal also provides a forum for discussion of the broader policy and planning issues that have played, and will continue to play, a crucial role in the fusion program. &lt;br /&gt;
| 0.858 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/1009-0630/ Plasma Science and Technology] (IOP)&lt;br /&gt;
| PST publishes novel experimental and theoretical results showing progress of interdisciplinary and application sciences in the fields related to plasma physics.&lt;br /&gt;
| 0.83 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://epubs.ans.org/?p=fst Fusion Science and Technology] (ANS)&lt;br /&gt;
| Fusion Science and Technology (FST) is the leading source of information on fusion plasma physics and plasma engineering, fusion plasma enabling science and technology, fusion nuclear technology and material science, fusion applications, fusion design and system studies.&lt;br /&gt;
| 0.578 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [https://www.tandfonline.com/loi/grad20 Radiation Effects and Defects in Solids] (Taylor &amp;amp; Francis)&lt;br /&gt;
| The Journal covers a wide range of topics under radiation and plasma sciences. The range of contributions encompasses: radiation physics; radiochemistry, radiobiology and physical effects of medical irradiation, including research on radiative cell degeneration; optical, electrical and mechanical effects of radiation, and their secondary effects such as diffusion and particle emission from surfaces; plasma techniques and plasma phenomena. On plasma science the Journal covers all areas of fusion, space and low temperature plasmas.&lt;br /&gt;
| 0.443 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.jspf.or.jp/PFR/ Plasma and Fusion Research] (Japan Society of Plasma Science and Nuclear Fusion Research)&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.jspf.or.jp/JPFRS/ Journal of Plasma and Fusion Research SERIES] (Japan Society of Plasma Science and Nuclear Fusion Research)&lt;br /&gt;
|&lt;br /&gt;
| &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Computation ==&lt;br /&gt;
{|class=&amp;quot;wikitable sortable&amp;quot; style=&amp;quot;width: 100%&amp;quot;&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;35%&amp;quot; | Journal (publisher)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;45%&amp;quot; | Description&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | IF (year)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.sciencedirect.com/science/journal/00104655 Computer Physics Communications] (Elsevier) &lt;br /&gt;
| Computer Physics Communications publishes research papers and computer program descriptions in computational physics and physical chemistry: the focus is on computational methods and techniques rather than results. &lt;br /&gt;
| 3.936 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.journals.elsevier.com/journal-of-computational-physics/ Journal of Computational Physics] (Elsevier) &lt;br /&gt;
| Journal of Computational Physics thoroughly treats the computational aspects of physical problems, presenting techniques for the numerical solution of mathematical equations arising in all areas of physics. The journal seeks to emphasize methods that cross disciplinary boundaries. &lt;br /&gt;
| 2.744 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [https://journals.plos.org/ PLoS One]  &lt;br /&gt;
|  &lt;br /&gt;
| &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== General physics ==&lt;br /&gt;
{|class=&amp;quot;wikitable sortable&amp;quot; style=&amp;quot;width: 100%&amp;quot;&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;35%&amp;quot; | Journal (publisher)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;45%&amp;quot; | Description&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | IF (year)&lt;br /&gt;
|-&lt;br /&gt;
| [http://rmp.aps.org/ Reviews of Modern Physics] (APS) &lt;br /&gt;
| Reviews of Modern Physics (RMP) is the world’s premier physics review journal and the most highly cited Physical Review publication. Written by leading international researchers, RMP’s in-depth essays provide outstanding coverage of a topic and give context and background for current research trends.&lt;br /&gt;
| 36.917 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.nature.com/nphys/ Nature Physics] &lt;br /&gt;
| Nature Physics publishes papers of the highest quality and significance in all areas of physics, pure and applied. The journal&#039;s content reflects core physics disciplines, but is also open to a broad range of topics whose central theme falls within the bounds of physics. Theoretical physics, particularly where it is pertinent to experiment, also features. &lt;br /&gt;
| 22.806 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://prl.aps.org/ Physical Review Letters] (APS)&lt;br /&gt;
| Physical Review Letters (PRL) is the world’s premier physics letter journal and the American Physical Society’s flagship publication. Since 1958 it has contributed to APS’s mission to advance and diffuse the knowledge of physics by publishing seminal research by Nobel Prize–winning and other distinguished researchers in all fields of physics.&lt;br /&gt;
| 8.462 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://pre.aps.org/ Physical Review E] (APS)&lt;br /&gt;
| Physical Review E, interdisciplinary in scope, focuses on many-body phenomena, including recent developments in quantum and classical chaos and soft matter physics. It has sections on statistical physics, equilibrium and transport properties of fluids, liquid crystals, complex fluids, polymers, chaos, fluid dynamics, plasma physics, classical physics, and computational physics. In addition, the journal features sections on two rapidly growing areas: biological physics and granular materials.&lt;br /&gt;
| 2.366 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/0295-5075/ Europhysics Letters] (IOP)&lt;br /&gt;
| EPL publishes original, high-quality Letters in all areas of physics, ranging from condensed matter topics and interdisciplinary research to astrophysics, geophysics, plasma and fusion sciences, including those with application potential. &lt;br /&gt;
| 1.957 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://rsi.aip.org/ Review of Scientific Instruments] (AIP)&lt;br /&gt;
| Review of Scientific Instruments (RSI) publishes novel advancements in scientific instrumentation, apparatuses, techniques of experimental measurement, and related mathematical analysis.&lt;br /&gt;
| 1.515 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.springer.com/physics/atomic%2C+molecular%2C+optical+%26+plasma+physics/journal/10053 European Physical Journal D] (Springer)&lt;br /&gt;
| Atomic, Molecular, Optical and Plasma Physics&lt;br /&gt;
| 1.288 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/1402-4896/ Physica Scripta] (IOP)&lt;br /&gt;
| Physica Scripta, endorsed by The Royal Swedish Academy of Sciences, is an international journal dedicated to presenting novel and accessible research findings across the breadth of theoretical and experimental physics.&lt;br /&gt;
| 1.28 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/0143-0807 European Journal of Physics] (IOP)&lt;br /&gt;
| With a world-wide readership and authors from every continent, European Journal of Physics is a truly international journal dedicated to maintaining and improving the standard of taught physics in universities and other higher education institutes.&lt;br /&gt;
| 0.614 (2016)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== General science ==&lt;br /&gt;
{|class=&amp;quot;wikitable sortable&amp;quot; style=&amp;quot;width: 100%&amp;quot; &lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;35%&amp;quot; | Journal (publisher)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;45%&amp;quot; | Description&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | IF (year)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.nature.com/ Nature] &lt;br /&gt;
|&lt;br /&gt;
| 40.137 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.sciencemag.org/ Science]&lt;br /&gt;
| &lt;br /&gt;
| 37.205 (2016)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Preprint servers ==&lt;br /&gt;
&lt;br /&gt;
{|class=&amp;quot;wikitable sortable&amp;quot; style=&amp;quot;width: 100%&amp;quot; &lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;35%&amp;quot; | Journal (publisher)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;45%&amp;quot; | Description&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | IF (year)&lt;br /&gt;
|-&lt;br /&gt;
| [http://arxiv.org/list/physics.plasm-ph/recent ArXiV] &lt;br /&gt;
| Non-refereed preprint service&lt;br /&gt;
| &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Institutional repositories ==&lt;br /&gt;
&lt;br /&gt;
{|class=&amp;quot;wikitable sortable&amp;quot; style=&amp;quot;width: 100%&amp;quot; &lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;35%&amp;quot; | Repository&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;45%&amp;quot; | Description&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | IF (year)&lt;br /&gt;
|-&lt;br /&gt;
| [http://documenta.ciemat.es CIEMAT] &lt;br /&gt;
| Repository&lt;br /&gt;
| &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Impact factors ==&lt;br /&gt;
&lt;br /&gt;
Older journal impact factors can be found here:&lt;br /&gt;
* [https://info.fusion.ciemat.es/media/IF_1992-2009.zip Impact Factors 1992-2009] (zip file, 23 MB)&lt;br /&gt;
* [https://info.fusion.ciemat.es/media/JCR_1979_1997.zip Impact Factors 1979-1997] (zip file, 115 MB)&lt;br /&gt;
&lt;br /&gt;
== Note ==&lt;br /&gt;
&lt;br /&gt;
Journal abbreviations in citations are standardized. Consult the [http://www.issn.org/2-22660-LTWA.php LTWA].&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Books]]&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=Journals&amp;diff=8649</id>
		<title>Journals</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=Journals&amp;diff=8649"/>
		<updated>2026-07-15T07:41:49Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* On-line publications */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This page is meant to provide an overview of (scientific) journals of relevance for fusion and plasma physics, along with a description of their focus and impact (IF = [[:Wikipedia:Impact factor|Impact factor]]). Such a list could be helpful to choose the optimal forum for a publication. It is in need of expansion (please help).&lt;br /&gt;
&lt;br /&gt;
== Fusion and plasma physics ==&lt;br /&gt;
{|class=&amp;quot;wikitable sortable&amp;quot; style=&amp;quot;width: 100%&amp;quot;&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;35%&amp;quot; | Journal (publisher)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;45%&amp;quot; | Description&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | IF (year)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/0029-5515 Nuclear Fusion] (IOP) &lt;br /&gt;
| The journal covers all aspects of research, theoretical and practical, relevant to controlled thermonuclear fusion.&lt;br /&gt;
| 3.307 (2016) 3.5 (2023)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/0963-0252/ Plasma Sources Science and Technology] (IOP)&lt;br /&gt;
| A single interdisciplinary forum for physicists, engineers and materials scientists working in the increasingly significant field of low-temperature plasma science.&lt;br /&gt;
| 3.302 (2016) 3.3 (2023)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/0741-3335 Plasma Physics and Controlled Fusion] (IOP) &lt;br /&gt;
| Covering all aspects of the physics of hot, highly ionised plasmas in the laboratory, the ionosphere and in space as well as in magnetic and inertial-confinement fusion.&lt;br /&gt;
| 2.392 (2016) 2.1 (2023)&lt;br /&gt;
|-&lt;br /&gt;
| [http://pop.aip.org/ Physics of Plasmas] (AIP) &lt;br /&gt;
| Physics of Plasmas, published by the American Institute of Physics with the cooperation of The American Physical Society, Division of Plasma Physics, is devoted to original experimental and theoretical contributions to the physics of plasmas.&lt;br /&gt;
| 2.115 (2016) 2.0 (2023)&lt;br /&gt;
|-&lt;br /&gt;
| [https://www.journals.elsevier.com/journal-of-nuclear-materials Journal of Nuclear Materials] (Elsevier) &lt;br /&gt;
| The Journal of Nuclear Materials publishes high quality papers in materials research for nuclear applications, primarily fission reactors, fusion reactors, and similar environments including radiation areas of charged particle accelerators.&lt;br /&gt;
| 2.048 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [https://www.mdpi.com/journal/plasma Plasma] (MDPI) &lt;br /&gt;
| Plasma is an international, open access, peer-reviewed journal covering all aspects of plasma science, published quarterly online by MDPI.&lt;br /&gt;
| 1.9 (2023)&lt;br /&gt;
|-&lt;br /&gt;
| [http://onlinelibrary.wiley.com/journal/10.1002/%28ISSN%291521-3986 Contributions to Plasma Physics] (Wiley) &lt;br /&gt;
| Basic physics of low-temperature plasmas; Strongly correlated non-ideal plasmas; Plasma discharges - microplasmas, reactive, and atmospheric pressure plasmas; Plasma diagnostics; Plasma-surface interaction; Plasma technology; Plasma medicine&lt;br /&gt;
| 1.44 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://journals.cambridge.org/action/displayJournal?jid=PLA Journal of Plasma Physics] (Cambridge) &lt;br /&gt;
| JPP aspires to be the intellectual home of those who think of plasma physics as a fundamental discipline. The journal will particularly focus on publishing research on laboratory plasmas, space physics and plasma astrophysics that takes advantage of the rapid ongoing progress in instrumentation and computing to advance fundamental understanding of multiscale plasma physics. The Journal welcomes submissions of analytical, numerical and experimental work: both original research and tutorial- or review-style papers, as well as proposals for its Lecture Notes series.&lt;br /&gt;
| 1.16 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.sciencedirect.com/science/journal/09203796 Fusion Engineering and Design] (Elsevier)&lt;br /&gt;
| The journal accepts papers about experiments (both plasma and technology), theory, models, methods, and designs in areas relating to technology, engineering, and applied science aspects of magnetic and inertial fusion energy. &lt;br /&gt;
| 1.14 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://ieeexplore.ieee.org/servlet/opac?punumber=27 IEEE Transactions on Plasma Science] (IEEE) &lt;br /&gt;
| Plasma science and engineering, including: magnetofluid dynamics and thermionics; plasma dynamics; gaseous electronics and arc technology; controlled thermonuclear fusion; electron, ion, and plasma sources; space plasmas; high-current relativistic electron beams; laser-plasma interactions; diagnostics; plasma chemistry and colloidal and solid-state plasmas. &lt;br /&gt;
| 1.052 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.springer.com/physics/atomic%2C+molecular%2C+optical+%26+plasma+physics/journal/11452 Plasma Physics Reports] (Springer)&lt;br /&gt;
| The journal covers the following topics: high-temperature plasma physics related to the problem of controlled nuclear fusion based on magnetic and inertial confinement; physics of cosmic plasma, including magnetosphere plasma, sun and stellar plasma, etc.; gas discharge plasma and plasma generated by laser and particle beams. The journal also publishes papers on such related topics as plasma electronics, generation of radiation in plasma, and plasma diagnostics.&lt;br /&gt;
| 0.984 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [https://link.springer.com/journal/10894 Journal of Fusion Energy] (Springer)&lt;br /&gt;
| The Journal of Fusion Energy features contributions and review papers pertinent to the development of thermonuclear fusion as a useful power source. Intended to serve as a journal of record for publication of research results, the journal also provides a forum for discussion of the broader policy and planning issues that have played, and will continue to play, a crucial role in the fusion program. &lt;br /&gt;
| 0.858 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/1009-0630/ Plasma Science and Technology] (IOP)&lt;br /&gt;
| PST publishes novel experimental and theoretical results showing progress of interdisciplinary and application sciences in the fields related to plasma physics.&lt;br /&gt;
| 0.83 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://epubs.ans.org/?p=fst Fusion Science and Technology] (ANS)&lt;br /&gt;
| Fusion Science and Technology (FST) is the leading source of information on fusion plasma physics and plasma engineering, fusion plasma enabling science and technology, fusion nuclear technology and material science, fusion applications, fusion design and system studies.&lt;br /&gt;
| 0.578 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [https://www.tandfonline.com/loi/grad20 Radiation Effects and Defects in Solids] (Taylor &amp;amp; Francis)&lt;br /&gt;
| The Journal covers a wide range of topics under radiation and plasma sciences. The range of contributions encompasses: radiation physics; radiochemistry, radiobiology and physical effects of medical irradiation, including research on radiative cell degeneration; optical, electrical and mechanical effects of radiation, and their secondary effects such as diffusion and particle emission from surfaces; plasma techniques and plasma phenomena. On plasma science the Journal covers all areas of fusion, space and low temperature plasmas.&lt;br /&gt;
| 0.443 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.jspf.or.jp/PFR/ Plasma and Fusion Research] (Japan Society of Plasma Science and Nuclear Fusion Research)&lt;br /&gt;
|&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.jspf.or.jp/JPFRS/ Journal of Plasma and Fusion Research SERIES] (Japan Society of Plasma Science and Nuclear Fusion Research)&lt;br /&gt;
|&lt;br /&gt;
| &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Computation ==&lt;br /&gt;
{|class=&amp;quot;wikitable sortable&amp;quot; style=&amp;quot;width: 100%&amp;quot;&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;35%&amp;quot; | Journal (publisher)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;45%&amp;quot; | Description&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | IF (year)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.sciencedirect.com/science/journal/00104655 Computer Physics Communications] (Elsevier) &lt;br /&gt;
| Computer Physics Communications publishes research papers and computer program descriptions in computational physics and physical chemistry: the focus is on computational methods and techniques rather than results. &lt;br /&gt;
| 3.936 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.journals.elsevier.com/journal-of-computational-physics/ Journal of Computational Physics] (Elsevier) &lt;br /&gt;
| Journal of Computational Physics thoroughly treats the computational aspects of physical problems, presenting techniques for the numerical solution of mathematical equations arising in all areas of physics. The journal seeks to emphasize methods that cross disciplinary boundaries. &lt;br /&gt;
| 2.744 (2016)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== General physics ==&lt;br /&gt;
{|class=&amp;quot;wikitable sortable&amp;quot; style=&amp;quot;width: 100%&amp;quot;&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;35%&amp;quot; | Journal (publisher)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;45%&amp;quot; | Description&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | IF (year)&lt;br /&gt;
|-&lt;br /&gt;
| [http://rmp.aps.org/ Reviews of Modern Physics] (APS) &lt;br /&gt;
| Reviews of Modern Physics (RMP) is the world’s premier physics review journal and the most highly cited Physical Review publication. Written by leading international researchers, RMP’s in-depth essays provide outstanding coverage of a topic and give context and background for current research trends.&lt;br /&gt;
| 36.917 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.nature.com/nphys/ Nature Physics] &lt;br /&gt;
| Nature Physics publishes papers of the highest quality and significance in all areas of physics, pure and applied. The journal&#039;s content reflects core physics disciplines, but is also open to a broad range of topics whose central theme falls within the bounds of physics. Theoretical physics, particularly where it is pertinent to experiment, also features. &lt;br /&gt;
| 22.806 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://prl.aps.org/ Physical Review Letters] (APS)&lt;br /&gt;
| Physical Review Letters (PRL) is the world’s premier physics letter journal and the American Physical Society’s flagship publication. Since 1958 it has contributed to APS’s mission to advance and diffuse the knowledge of physics by publishing seminal research by Nobel Prize–winning and other distinguished researchers in all fields of physics.&lt;br /&gt;
| 8.462 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://pre.aps.org/ Physical Review E] (APS)&lt;br /&gt;
| Physical Review E, interdisciplinary in scope, focuses on many-body phenomena, including recent developments in quantum and classical chaos and soft matter physics. It has sections on statistical physics, equilibrium and transport properties of fluids, liquid crystals, complex fluids, polymers, chaos, fluid dynamics, plasma physics, classical physics, and computational physics. In addition, the journal features sections on two rapidly growing areas: biological physics and granular materials.&lt;br /&gt;
| 2.366 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/0295-5075/ Europhysics Letters] (IOP)&lt;br /&gt;
| EPL publishes original, high-quality Letters in all areas of physics, ranging from condensed matter topics and interdisciplinary research to astrophysics, geophysics, plasma and fusion sciences, including those with application potential. &lt;br /&gt;
| 1.957 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://rsi.aip.org/ Review of Scientific Instruments] (AIP)&lt;br /&gt;
| Review of Scientific Instruments (RSI) publishes novel advancements in scientific instrumentation, apparatuses, techniques of experimental measurement, and related mathematical analysis.&lt;br /&gt;
| 1.515 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.springer.com/physics/atomic%2C+molecular%2C+optical+%26+plasma+physics/journal/10053 European Physical Journal D] (Springer)&lt;br /&gt;
| Atomic, Molecular, Optical and Plasma Physics&lt;br /&gt;
| 1.288 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/1402-4896/ Physica Scripta] (IOP)&lt;br /&gt;
| Physica Scripta, endorsed by The Royal Swedish Academy of Sciences, is an international journal dedicated to presenting novel and accessible research findings across the breadth of theoretical and experimental physics.&lt;br /&gt;
| 1.28 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://iopscience.iop.org/0143-0807 European Journal of Physics] (IOP)&lt;br /&gt;
| With a world-wide readership and authors from every continent, European Journal of Physics is a truly international journal dedicated to maintaining and improving the standard of taught physics in universities and other higher education institutes.&lt;br /&gt;
| 0.614 (2016)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== General science ==&lt;br /&gt;
{|class=&amp;quot;wikitable sortable&amp;quot; style=&amp;quot;width: 100%&amp;quot; &lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;35%&amp;quot; | Journal (publisher)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;45%&amp;quot; | Description&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | IF (year)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.nature.com/ Nature] &lt;br /&gt;
|&lt;br /&gt;
| 40.137 (2016)&lt;br /&gt;
|-&lt;br /&gt;
| [http://www.sciencemag.org/ Science]&lt;br /&gt;
| &lt;br /&gt;
| 37.205 (2016)&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Preprint servers ==&lt;br /&gt;
&lt;br /&gt;
{|class=&amp;quot;wikitable sortable&amp;quot; style=&amp;quot;width: 100%&amp;quot; &lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;35%&amp;quot; | Journal (publisher)&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;45%&amp;quot; | Description&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | IF (year)&lt;br /&gt;
|-&lt;br /&gt;
| [http://arxiv.org/list/physics.plasm-ph/recent ArXiV] &lt;br /&gt;
| Non-refereed preprint service&lt;br /&gt;
| &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Institutional repositories ==&lt;br /&gt;
&lt;br /&gt;
{|class=&amp;quot;wikitable sortable&amp;quot; style=&amp;quot;width: 100%&amp;quot; &lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;35%&amp;quot; | Repository&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;45%&amp;quot; | Description&lt;br /&gt;
! scope=&amp;quot;col&amp;quot; width=&amp;quot;20%&amp;quot; | IF (year)&lt;br /&gt;
|-&lt;br /&gt;
| [http://documenta.ciemat.es CIEMAT] &lt;br /&gt;
| Repository&lt;br /&gt;
| &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
== Impact factors ==&lt;br /&gt;
&lt;br /&gt;
Older journal impact factors can be found here:&lt;br /&gt;
* [https://info.fusion.ciemat.es/media/IF_1992-2009.zip Impact Factors 1992-2009] (zip file, 23 MB)&lt;br /&gt;
* [https://info.fusion.ciemat.es/media/JCR_1979_1997.zip Impact Factors 1979-1997] (zip file, 115 MB)&lt;br /&gt;
&lt;br /&gt;
== Note ==&lt;br /&gt;
&lt;br /&gt;
Journal abbreviations in citations are standardized. Consult the [http://www.issn.org/2-22660-LTWA.php LTWA].&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Books]]&lt;/div&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>https://wiki.fusenet.eu/fusionwiki/index.php?title=User:Admin&amp;diff=8628</id>
		<title>User:Admin</title>
		<link rel="alternate" type="text/html" href="https://wiki.fusenet.eu/fusionwiki/index.php?title=User:Admin&amp;diff=8628"/>
		<updated>2026-05-30T15:28:04Z</updated>

		<summary type="html">&lt;p&gt;Admin: /* Selected publications */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[File:BvM.jpg|right|]]&lt;br /&gt;
== Personal information ==&lt;br /&gt;
__NOTOC__&lt;br /&gt;
* Boudewijn van Milligen (Admin)&lt;br /&gt;
* Researcher at: &amp;lt;br&amp;gt;[[Laboratorio Nacional de Fusión]] - [[CIEMAT]] &amp;lt;br&amp;gt;Avda. Complutense 40, Edif. 66&amp;lt;br&amp;gt;28040 Madrid, España - Spain&lt;br /&gt;
* Tel. +34 - 914 962 682&lt;br /&gt;
* Email boudewijn.vanmilligen (at) ciemat.es&lt;br /&gt;
User profiles:&lt;br /&gt;
* [https://publons.com/researcher/1248698/boudewijn-ph-van-milligen/ Publons] (ResearcherID H-5121-2015)&lt;br /&gt;
* [http://orcid.org/0000-0001-5344-6274 ORCID 0000-0001-5344-6274]&lt;br /&gt;
* [https://www.scopus.com/authid/detail.uri?authorId=35476190300 Scopus AuthorID 35476190300]&lt;br /&gt;
* [http://scholar.google.com/citations?user=7z9Cr9oAAAAJ Google Scholar]&lt;br /&gt;
* [https://www.researchgate.net/profile/Boudewijn_Van_Milligen/ ResearchGate]&lt;br /&gt;
&lt;br /&gt;
== Interests ==&lt;br /&gt;
&lt;br /&gt;
* Fusion and plasma physics&lt;br /&gt;
** [[H-mode|L-H transition]], Zonal Flows&lt;br /&gt;
** [[Magnetic island]]s, MHD activity&lt;br /&gt;
* [[Anomalous transport]]&lt;br /&gt;
** Turbulence&lt;br /&gt;
** Continuous Time Random Walks&lt;br /&gt;
* Data analysis&lt;br /&gt;
** [[Causality detection]]&lt;br /&gt;
** [[Intermittence]]&lt;br /&gt;
** [[:Wikipedia:Rescaled range|Rescaled range]] or [[:Wikipedia:Hurst exponent|Hurst]] analysis&lt;br /&gt;
** [[Bayesian data analysis]]&lt;br /&gt;
** [[Biorthogonal decomposition]]&lt;br /&gt;
** [[Bicoherence]]&lt;br /&gt;
** [[TJ-II:Tomography|Tomography]]&lt;br /&gt;
&lt;br /&gt;
== Book ==&lt;br /&gt;
&lt;br /&gt;
B.Ph. van Milligen and R. Sánchez, &#039;&#039;Analysis of Turbulence in Fusion Plasmas&#039;&#039;, [[doi:10.1088/978-0-7503-4856-0|IOP Publishing (2022)]], {{ISBN|978-0-7503-4854-6}}&lt;br /&gt;
&lt;br /&gt;
== Selected publications ==&lt;br /&gt;
&lt;br /&gt;
(inverse chronological order)&lt;br /&gt;
=== &amp;amp;ge; 2020 ===&lt;br /&gt;
* A. Alonso Alvarez, B. P. Van Milligen, I. Voldiner, I. L. Caldas, Z. Guimarães Filho, O. Kozachok, and A. Chmyga. &#039;&#039;Edge turbulence dynamics across electron–ion root transitions during ECRH modulation experiments in the TJ-II stellarator&#039;&#039;. [[doi:10.1088/1361-6587/ae7470|Plasma Phys. Control. Fusion, 2026]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. van Milligen, I. García-Cortés, K.J. McCarthy, et al, &#039;&#039;The rotational transform and enhanced confinement in the TJ-II stellarator&#039;&#039;, [[doi:10.1017/S0022377825100433|Journal of Plasma Physics &#039;&#039;&#039;91&#039;&#039;&#039;, 4 (2025) E98]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* Boudewijn Philip van Milligen, Teresa Estrada, Benjamin Carreras, Luis García, and TJ-II Team. &#039;&#039;Importance of the Rotational Transform for L–H Transitions in the TJ-II Stellarator&#039;&#039; [[doi:10.3390/plasma7020024|Plasma &#039;&#039;&#039;7&#039;&#039;&#039;, no. 2 (2024) 446-464]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. van Milligen, I. Voldiner, B.A. Carreras, L. García, M.A. Ochando and The TJ-II Team, &#039;&#039;Rational surfaces, flows and radial structure in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/1741-4326/aca688|Nucl. Fusion &#039;&#039;&#039;63&#039;&#039;&#039; (2023) 016027]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. Van Milligen, B.A. Carreras, L. Garcia, G. Grenfell, I. Voldiner and C. Hidalgo, &#039;&#039;The impact of radial electric fields and plasma rotation on intermittence in TJ-II&#039;&#039;, [[doi:10.1088/1361-6587/ac54e9|Plasma Phys. Control. Fusion &#039;&#039;&#039;64&#039;&#039;&#039;, 5 (2022) 055006]] ([http://documenta.ciemat.es/handle/123456789/2290 repository])&lt;br /&gt;
* B. van Milligen, A. Melnikov, B. Carreras, L. Garcia, A. Kozachek, C. Hidalgo, J. de Pablos, Ph. Khabanov, L. Eliseev, M. Drabinskij, A. Chmyga, L. Krupnik, the HIBP Team, the TJ-II Team, &#039;&#039;Topology of 2-D turbulent structures based on intermittence in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/1741-4326/ac27c9|Nucl. Fusion &#039;&#039;&#039;61&#039;&#039;&#039;, 11 (2021) 116063]] ([http://documenta.ciemat.es/handle/123456789/2281 repository])&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras, I. Voldiner, U. Losada, C. Hidalgo, and the TJ-II Team, &#039;&#039;Causality, intermittence and crossphase evolution during confinement transitions in the TJ-II stellarator&#039;&#039;, [[doi:10.1063/5.0057791|Phys. Plasmas &#039;&#039;&#039;28&#039;&#039;&#039; (2021) 092302]] ([http://documenta.ciemat.es/handle/123456789/2289 repository])&lt;br /&gt;
* B.Ph. van Milligen, B. Carreras, L. García and C. Hidalgo, &#039;&#039;The localization of low order rational surfaces based on the intermittence parameter in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/1741-4326/ab79cc|Nucl. Fusion &#039;&#039;&#039;60&#039;&#039;&#039; (2020) 056010]] ([http://documenta.ciemat.es/handle/123456789/2291 repository])&lt;br /&gt;
&lt;br /&gt;
=== 2010-2019 ===&lt;br /&gt;
* B.Ph. van Milligen, B. Carreras, L. García and J. Nicolau, &#039;&#039;The radial propagation of heat in strongly driven non-equilibrium fusion plasmas&#039;&#039;, [[doi:10.3390/e21020148|Entropy, &#039;&#039;&#039;21&#039;&#039;&#039;, 2 (2019) 148]] [[File:Open Access Icon.png|10px|link=:Wikipedia:Open_access_(publishing)|Open access]]&lt;br /&gt;
* B.Ph. van Milligen, B. Carreras, E. de la Luna and E. Solano, &#039;&#039;Radial variation of heat transport in L-mode JET discharges&#039;&#039; [[doi:10.1088/1741-4326/ab03e1|Nucl. Fusion, &#039;&#039;&#039;59&#039;&#039;&#039; (2019) 056006]] ([http://documenta.ciemat.es/handle/123456789/2292 repository])&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras, C. Hidalgo, Á. Cappa and the TJ-II Team, &#039;&#039;A possible mechanism for confinement power degradation in the TJ-II stellarator&#039;&#039;, [[doi:10.1063/1.5029881|Phys. Plasmas &#039;&#039;&#039;25&#039;&#039;&#039; (2018) 062503]] ([http://documenta.ciemat.es/handle/123456789/2308 repository])&lt;br /&gt;
* B.Ph. van Milligen, U. Hoefel, J. Nicolau, M. Hirsch, L. García, B. Carreras, C. Hidalgo and the W7-X Team, &#039;&#039;Study of radial heat transport in W7-X using the transfer entropy&#039;&#039;, [[doi:10.1088/1741-4326/aabf5d|Nucl. Fusion &#039;&#039;&#039;58&#039;&#039;&#039; (2018) 076002]] ([http://hdl.handle.net/10016/32565 repository])&lt;br /&gt;
* B.Ph. van Milligen, J. Hernández Nicolau, B. Liu, G. Grenfell, U. Losada, B. Carreras, L. Garcia and C. Hidalgo, &#039;&#039;Filaments in the edge confinement region of TJ-II&#039;&#039;, [[doi:10.1088/1741-4326/aa9db6|Nucl. Fusion &#039;&#039;&#039;58&#039;&#039;&#039; (2018) 026030]] ([http://hdl.handle.net/10016/32563 repository])&lt;br /&gt;
* B.Ph. van Milligen, J.H. Nicolau, L. García, B.A. Carreras, C. Hidalgo and the TJ-II Team, &#039;&#039;The impact of rational surfaces on radial heat transport in TJ-II&#039;&#039;, [[doi:10.1088/1741-4326/aa611f|Nucl. Fusion &#039;&#039;&#039;57&#039;&#039;&#039;, 5 (2017) 056028]], [https://arxiv.org/abs/1701.04574 arxiv:1701.04574]&lt;br /&gt;
* B.Ph. van Milligen, T. Estrada, B.A. Carreras, E. Ascasíbar, C. Hidalgo, I. Pastor, J.M. Fontdecaba, R. Balbín and the TJ-II Team, &#039;&#039;The causal impact of magnetic fluctuations in slow and fast L–H transitions at TJ-II&#039;&#039;, [[doi:10.1063/1.4958807|Phys. Plasmas &#039;&#039;&#039;23&#039;&#039;&#039; (2016) 072305]], [https://arxiv.org/abs/1512.06525 arxiv:1512.06525]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras, L. García, A. Martín de Aguilera, C. Hidalgo, J.H. Nicolau and the TJ-II Team, &#039;&#039;The causal relation between turbulent particle flux and density gradient&#039;&#039;, [[doi:10.1063/1.4958806|Phys. Plasmas &#039;&#039;&#039;23&#039;&#039;&#039; (2016) 072307]]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras and D.E. Newman, &#039;&#039;Constructing criteria to diagnose the likelihood of extreme events in the case of the electric power grid&#039;&#039;, [[doi:10.1063/1.4943569|Chaos &#039;&#039;&#039;26&#039;&#039;&#039; (2016) 033109]]&lt;br /&gt;
* B.Ph. van Milligen, T. Estrada, L. García, D. López-Bruna, B. Carreras, Y. Xu, M. Ochando, C. Hidalgo, J. Reynolds-Barredo and A. López-Fraguas, &#039;&#039;The role of magnetic islands in modifying long range temporal correlations of density fluctuations and local heat transport&#039;&#039;, [[doi:10.1088/0029-5515/56/1/016013|Nucl. Fusion, &#039;&#039;&#039;56&#039;&#039;&#039;, 1 (2016) 016013]], [https://arxiv.org/abs/1506.06890 arxiv:1506.06890]&lt;br /&gt;
* B.Ph. van Milligen, E. Sánchez, A. Alonso, M.A. Pedrosa, C. Hidalgo, A. Martín de Aguilera, A. López Fraguas, &#039;&#039;The use of the Biorthogonal Decomposition for the identification of zonal flows at TJ-II&#039;&#039;, [[doi:10.1088/0741-3335/57/2/025005|Plasma Phys. Control. Fusion &#039;&#039;&#039;57&#039;&#039;&#039;, 2 (2015) 025005]], [https://arxiv.org/abs/1408.1845 arxiv:1408.1845]&lt;br /&gt;
* B.Ph. van Milligen, P.D. Bons, &#039;&#039;Simplified numerical model for clarifying scaling behavior in the intermediate dispersion regime in homogeneous porous media&#039;&#039;, [[doi:10.1016/j.cpc.2014.09.006|Comput. Phys. Commun. &#039;&#039;&#039;185&#039;&#039;&#039; (2014) 3291]], [https://arxiv.org/abs/1409.2724 arxiv:1409.2724]&lt;br /&gt;
* B.Ph. van Milligen, G. Birkenmeier, M. Ramisch, T. Estrada, C. Hidalgo and A. Alonso, &#039;&#039;Causality detection and turbulence in fusion plasmas&#039;&#039;, [[doi:10.1088/0029-5515/54/2/023011|Nucl. Fusion &#039;&#039;&#039;54&#039;&#039;&#039; (2014), 023011]], [https://arxiv.org/abs/1309.7769 arxiv:1309.7769]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Parallel and perpendicular turbulence correlation length in the TJ-II Stellarator&#039;&#039;, [[doi:10.1088/0029-5515/53/9/093025|Nucl. Fusion &#039;&#039;&#039;53&#039;&#039;&#039; (2013) 093025]], [https://arxiv.org/abs/1306.1395 arxiv:1306.1395]&lt;br /&gt;
* P.D. Bons, B.Ph. van Milligen, P. Blum, &#039;&#039;A general unified expression for solute and heat dispersion in homogeneous porous media&#039;&#039;, [[doi:10.1002/wrcr.20488|Water Resour. Res. &#039;&#039;&#039;49&#039;&#039;&#039; (2013) 1]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Spatiotemporal and wavenumber resolved bicoherence at the low to high confinement transition in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/53/11/113034|Nucl. Fusion &#039;&#039;&#039;53&#039;&#039;&#039; (2013) 113034]], [https://arxiv.org/abs/1211.0420 arxiv:1211.0420]&lt;br /&gt;
* B. Ph. van Milligen, R. Sánchez and C. Hidalgo, &#039;&#039;Relevance of Uncorrelated Lorentzian Pulses for the Interpretation of Turbulence in the Edge of Magnetically Confined Toroidal Plasmas&#039;&#039;, [[doi:10.1103/PhysRevLett.109.105001|Phys. Rev. Lett. &#039;&#039;&#039;109&#039;&#039;&#039; (2012) 105001]], [https://arxiv.org/abs/1204.6185 arxiv:1204.6185]&lt;br /&gt;
* B.Ph. van Milligen, P.D. Bons, &#039;&#039;Analytical model for tracer dispersion in porous media&#039;&#039;, [[doi:10.1103/PhysRevE.85.011306|Phys. Rev. E 85 (2012) 011306]], [https://arxiv.org/abs/1111.6512 arxiv:1111.6512]&lt;br /&gt;
* B.Ph. van Milligen, L. García, B.A. Carreras, M.A. Pedrosa, C. Hidalgo, J.A. Alonso, T. Estrada and E. Ascasíbar, &#039;&#039;MHD mode activity and the velocity shear layer at TJ-II&#039;&#039;, [[doi:10.1088/0029-5515/52/1/013006|Nucl. Fusion &#039;&#039;&#039;52&#039;&#039;&#039; (2012) 013006]]&lt;br /&gt;
* B.Ph. van Milligen, T. Estrada, E. Ascasíbar, et al, &#039;&#039;Integrated data analysis at TJ-II: the density profile&#039;&#039;, [[doi:10.1063/1.3608551|Rev. Sci. Instrum. &#039;&#039;&#039;82&#039;&#039;&#039; (2011) 073503]]&lt;br /&gt;
* B.A. Carreras et al., &#039;&#039;Reconstruction of intermittent waveforms associated with the zonal flow at the transition leading to the edge shear flow layer&#039;&#039;, [[doi:10.1088/0029-5515/51/5/053022|Nucl. Fusion &#039;&#039;&#039;51&#039;&#039;&#039; (2011) 053022]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;A global resonance phenomenon at the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/51/1/013005|Nucl. Fusion &#039;&#039;&#039;51&#039;&#039;&#039; (2011) 013005]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;The dynamics of the formation of the edge particle transport barrier at TJ-II&#039;&#039;, [[doi:10.1088/0029-5515/51/11/113002|Nucl. Fusion &#039;&#039;&#039;51&#039;&#039;&#039; (2011) 113002]]&lt;br /&gt;
&lt;br /&gt;
=== 2000-2009 ===&lt;br /&gt;
* B.Ph. van Milligen, I. Calvo and R. Sánchez, &#039;&#039;Continuous time random walks in finite domains and general boundary conditions: some formal considerations&#039;&#039;, [[doi:10.1088/1751-8113/41/21/215004|J. Phys. A: Math. Theor. &#039;&#039;&#039;41&#039;&#039;&#039; (2008) 215004]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Quantifying profile stiffness&#039;&#039;, [http://www.jspf.or.jp/PFR/PFR_articles/pfr2008S1/pfr2008_03-S1070.html Plasma and Fusion Research, &#039;&#039;&#039;3&#039;&#039;&#039; (2008) S1070]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Bicoherence during confinement transitions in the TJ-II stellarator&#039;&#039;, [[doi:10.1088/0029-5515/48/11/115003|Nucl. Fusion &#039;&#039;&#039;48&#039;&#039;&#039; (2008) 115003]]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras, V.E. Lynch and R. Sánchez, &#039;&#039;Pulse propagation in a simple probabilistic transport model&#039;&#039;, [[doi:10.1088/0029-5515/47/3/004|Nucl. Fusion &#039;&#039;&#039;47&#039;&#039;&#039; (2007) 189]]&lt;br /&gt;
* B.Ph. van Milligen, P.D. Bons, B.A. Carreras and R. Sánchez, &#039;&#039;On the applicability of Fick&#039;s Law to diffusion in inhomogeneous systems&#039;&#039;, [[doi:10.1088/0143-0807/26/5/023|Eur. J. Phys. &#039;&#039;&#039;26&#039;&#039;&#039; (2005) 913]]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras and R. Sánchez, &#039;&#039;The foundations of diffusion revisited&#039;&#039;, [[doi:10.1088/0741-3335/47/12B/S56|Plasma Phys. Control. Fusion &#039;&#039;&#039;47&#039;&#039;&#039; (2005) B743]]&lt;br /&gt;
* B.Ph. Van Milligen et al, &#039;&#039;Additional evidence for the universality of turbulent fluctuations and fluxes in the scrape-off layer region of fusion plasmas&#039;&#039;, [[doi:10.1063/1.1884615|Phys. Plasmas &#039;&#039;&#039;12&#039;&#039;&#039; (2005) 052507]]&lt;br /&gt;
* B.Ph. van Milligen, R. Sánchez and B.A. Carreras, &#039;&#039;Probabilistic finite-size transport models for fusion: anomalous transport and scaling laws&#039;&#039;, [[doi:10.1063/1.1701893|Phys. Plasmas &#039;&#039;&#039;11&#039;&#039;&#039;, 5 (2004) 2272]]&lt;br /&gt;
* B.Ph. van Milligen, B.A. Carreras and R. Sánchez, &#039;&#039;Uphill transport and the probabilistic transport model&#039;&#039;, [[doi:10.1063/1.1763915|Phys. Plasmas &#039;&#039;&#039;11&#039;&#039;&#039;, 3787 (2004)]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Revision of TV Thomson scattering data analysis and detection of profile structure&#039;&#039;, [[doi:10.1063/1.1597951|Rev. Sci. Instrum. &#039;&#039;&#039;74&#039;&#039;&#039; (2003) 3998]]&lt;br /&gt;
* B.Ph. van Milligen, E. de la Luna, F.L. Tabarés, et al., &#039;&#039;Ballistic transport phenomena in TJ-II&#039;&#039;, [[doi:10.1088/0029-5515/42/7/301|Nucl. Fusion &#039;&#039;&#039;42&#039;&#039;&#039; (2002) 787]]&lt;br /&gt;
=== 1990 - 1999 ===&lt;br /&gt;
* B.A. Carreras, B.Ph. van Milligen, et al, &#039;&#039;Experimental evidence of long-range correlation and self-similarity in plasma fluctuations&#039;&#039;, [[doi:10.1063/1.873490|Phys. Plasmas &#039;&#039;&#039;6&#039;&#039;&#039;, 5 (1999) 1885]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Statistically robust linear and non-linear wavelet analysis applied to plasma edge turbulence&#039;&#039;, [[doi:10.1063/1.1147727|Rev. Sci. Instrum. &#039;&#039;&#039;68&#039;&#039;&#039; (1997) 967]]&lt;br /&gt;
* B.Ph. van Milligen, V. Tribaldos, J.A. Jiménez, &#039;&#039;A neural network differential equation and plasma equilibrium solver&#039;&#039;, [[doi:10.1103/PhysRevLett.75.3594|Phys. Rev. Lett. &#039;&#039;&#039;75&#039;&#039;&#039; (1995) 3594]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Nonlinear phenomena and intermittency in plasma turbulence&#039;&#039;, [[doi:10.1103/PhysRevLett.74.395|Phys. Rev. Lett. &#039;&#039;&#039;74&#039;&#039;&#039;, 3 (1995) 395]]&lt;br /&gt;
* B.Ph. van Milligen et al, &#039;&#039;Wavelet bicoherence: a new turbulence analysis tool&#039;&#039;, [[doi:10.1063/1.871199|Phys. Plasmas &#039;&#039;&#039;2&#039;&#039;&#039;, 8 (1995) 3017]]&lt;br /&gt;
* B.Ph. van Milligen and A. Lopez Fraguas, &#039;&#039;Expansion of vacuum magnetic fields in toroidal harmonics&#039;&#039;, [[doi:10.1016/0010-4655(94)90112-0|Comput. Phys. Commun. &#039;&#039;&#039;81&#039;&#039;&#039;, Issues 1-2 (1994) 74-90]]&lt;br /&gt;
* B.Ph. van Milligen, A.C.A.P. van Lammeren, N.J. Lopes Cardozo, F.C. Schüller and M. Verreck, &#039;&#039;Gradients of electron temperature and density across m=2 islands in RTP&#039;&#039;, [[doi:10.1088/0029-5515/33/8/I03|Nucl. Fusion &#039;&#039;&#039;33&#039;&#039;&#039; (1993) 1119]]&lt;br /&gt;
* B.Ph. van Milligen, N.J. Lopes Cardozo, &#039;&#039;Function Parametrization: a fast inverse mapping method&#039;&#039;, [[doi:10.1016/0010-4655(91)90073-T|Comput. Phys. Commun. &#039;&#039;&#039;66&#039;&#039;&#039; (1991) 243]]&lt;br /&gt;
* B.Ph. van Milligen et al., &#039;&#039;Application of Function Parametrization to the analysis of polarimetry and interferometry data in TEXTOR&#039;&#039;, [[doi:10.1088/0029-5515/31/2/007|Nucl. Fusion &#039;&#039;&#039;31&#039;&#039;&#039; (1991) 309]]&lt;br /&gt;
* B.Ph. van Milligen, &#039;&#039;Exact relations between multipole moments of the flux and moments of the toroidal current density in tokamaks&#039;&#039;, [[doi:10.1088/0029-5515/30/1/012|Nucl. Fusion &#039;&#039;&#039;30&#039;&#039;&#039; (1990) 157]]&lt;/div&gt;</summary>
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