LNF:Fuelling and Impurity Control Studies in the stellarators TJ-II and W7-X using Cryogenic Pellets and Tracer-Encapsulated Solid Pellets (TESPEL): Difference between revisions

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The goal of this project, which falls within the realm of magnetic confinement nuclear fusion, is to continue research initiated in projects ENE2013-48679-R and FIS2017-89326-R on fuelling and impurity control in plasmas created in the stellarators TJ-II (Ciemat, Madrid) and W7-X (Greifswald, Germany). Further research to resolve these issues is critical to demonstrate steady-state operation of helical-type fusion reactors, in particular to identify operational scenarios that ensure adequate plasma fuelling and avoidance of impurity accumulation. This project will contribute to the development and scientific exploitation of stellarators, a priority highlighted in the document "Fusion Electricity: a roadmap to the realization of fusion energy" (EFDA 2012).
The goal of this project, which falls within the realm of magnetic confinement nuclear fusion, is to continue research initiated in projects ENE2013-48679-R and FIS2017-89326-R on fuelling and impurity control in plasmas created in the stellarators TJ-II (Ciemat, Madrid) and W7-X (Greifswald, Germany). Further research to resolve these issues is critical to demonstrate steady-state operation of helical-type fusion reactors, in particular to identify operational scenarios that ensure adequate plasma fuelling and avoidance of impurity accumulation. This project will contribute to the development and scientific exploitation of stellarators, a priority highlighted in the document "Fusion Electricity: a roadmap to the realization of fusion energy" (EFDA 2012).


The first aim is to investigate aspects of plasma fuelling that are still not fully understood and the effects of fuel pellets on plasma magnetic activity, plasma turbulence and plasma performance. For this, the medium-sized heliac TJ-II will be used. It is equipped with a cryogenic pellet injector (PI) for producing solid hydrogen pellets that can be injected at high velocity into the plasma. It is intended to investigate pellet fuelling as a means to enhance plasma confinement (higher stored energy, longer particle confinement) and to identify and explore new pellet phenomena. While TJ-II is equipped with a large number of modern diagnostics, it is proposed to develop a new system to measure pellet cloud density and temperature to extend knowledge of pellet physics.
1. The first aim is to investigate aspects of plasma fuelling that are still not fully understood and the effects of fuel pellets on plasma magnetic activity, plasma turbulence and plasma performance. For this, the medium-sized heliac TJ-II will be used. It is equipped with a cryogenic pellet injector (PI) for producing solid hydrogen pellets that can be injected at high velocity into the plasma. It is intended to investigate pellet fuelling as a means to enhance plasma confinement (higher stored energy, longer particle confinement) and to identify and explore new pellet phenomena. While TJ-II is equipped with a large number of modern diagnostics, it is proposed to develop a new system to measure pellet cloud density and temperature to extend knowledge of pellet physics.


The second aim is to continue to support impurity transport and accumulation studies in TJ-II and W7-X. Under the umbrella of a trilateral collaboration (2020-2029) with the National Institute for Fusion Science (Japan) and IPP-Max-Planck (Greifswald, Germany), Tracer-Encapsulated Solid Pellet (TESPEL) injections systems hare now operated on both TJ-II and W7-X. TESPELs are polystyrene spheres (diameter <1 mm) loaded with impurity tracers (atomic elements other than fuel). This allows delivering a precise quantify of tracer to a preselected location in the plasma core, after which its transport and confinement can be studied. An important aspect of the collaboration has been the establishment of a laboratory to fabricate TESPELs at Ciemat for both devices (project FIS2017- 89326-R). Key parts of this current project are to continue TESPEL fabrication for TJ-II and W7-X at this laboratory, thereby allowing Ciemat to maintain this fruitful collaboration, and to upgrade a vacuum ultraviolet spectrometer on TJ-II to provide important spectral line data for impurity identification in W7-X.
2. The second aim is to continue to support impurity transport and accumulation studies in TJ-II and W7-X. Under the umbrella of a trilateral collaboration (2020-2029) with the National Institute for Fusion Science (Japan) and IPP-Max-Planck (Greifswald, Germany), Tracer-Encapsulated Solid Pellet (TESPEL) injections systems hare now operated on both TJ-II and W7-X. TESPELs are polystyrene spheres (diameter <1 mm) loaded with impurity tracers (atomic elements other than fuel). This allows delivering a precise quantify of tracer to a preselected location in the plasma core, after which its transport and confinement can be studied. An important aspect of the collaboration has been the establishment of a laboratory to fabricate TESPELs at Ciemat for both devices (project FIS2017- 89326-R). Key parts of this current project are to continue TESPEL fabrication for TJ-II and W7-X at this laboratory, thereby allowing Ciemat to maintain this fruitful collaboration, and to upgrade a vacuum ultraviolet spectrometer on TJ-II to provide important spectral line data for impurity identification in W7-X.


The PI and TESPEL systems on TJ-II share a common injection guide lines. This unique set-up allows direct comparative studies of ablation, deposition and plasma response to be made thereby facilitating the understanding of common physics. Given that fuelling and impurity control are critical issues for stellarator steady-state operation, the project will allow us to continue to contribute to, and participate in, research programmes on W7-X, the stellarator of reference. Finally, team members have significant experience in the formation of young researchers at Master and PhD levels and in disseminating research to second level students and to the general public. A PhD student will undertake research in these areas during the project.
The PI and TESPEL systems on TJ-II share a common injection guide lines. This unique set-up allows direct comparative studies of ablation, deposition and plasma response to be made thereby facilitating the understanding of common physics. Given that fuelling and impurity control are critical issues for stellarator steady-state operation, the project will allow us to continue to contribute to, and participate in, research programmes on W7-X, the stellarator of reference. Finally, team members have significant experience in the formation of young researchers at Master and PhD levels and in disseminating research to second level students and to the general public. A PhD student will undertake research in these areas during the project.
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== Main Results ==
== Main Results ==


1. A pellet-induced enhanced confinement regime (or PiEC) has been identified in Neutral Beam Injection (NBI) heated discharges made in TJ-II after the injection of a single cryogenic fuel pellet into its plasma core [1]. In addition to the expected increase in core electron density, the plasma diamagnetic energy content, as determined using a diamagnetic loop, is seen to rise by up to 40%, with respect to reference discharges without pellet injection. Furthermore, the energy confinement time is significantly enhanced when compared to predictions obtained using the 2004 International Stellarator Scaling law, ISS04. Indeed, the operational regimes of other stellarator devices, such as LHD and W7-X, can be similarly extended to performance well beyond those obtainable with gas puffing alone.
1. A pellet-induced enhanced confinement regime (or PiEC) has been identified in Neutral Beam Injection (NBI) heated discharges made in TJ-II after the injection of a single cryogenic fuel pellet into its plasma core <ref>1</ref>. In addition to the expected increase in core electron density, the plasma diamagnetic energy content, as determined using a diamagnetic loop, is seen to rise by up to 40%, with respect to reference discharges without pellet injection. Furthermore, the energy confinement time is significantly enhanced when compared to predictions obtained using the 2004 International Stellarator Scaling law, ISS04. Indeed, the operational regimes of other stellarator devices, such as LHD and W7-X, can be similarly extended to performance well beyond those obtainable with gas puffing alone.


2. New studies, performed with multiple pellet injections, have extended the TJ-II operational regime well beyond limits previously achieved in this device using NBI heating and gas puff [2, 3]. In order to achieve best results, it has been determined that the plasma target electron density should to be in the range 1x10^19 m^-3 to 2.5x10^19 m^-3 and time separations between pellets should be close to energy confinement times, around 10 ms. It is also found, using a Charge Exchange Recombination Spectroscopy diagnostic, that while the plasma electron temperature is almost unaffected by such pellet injections, the majority ion temperature irises significantly due to reduced ion radial heat fluxes during the PiEC phase. It is also found that enhanced performance is independent of whether co- or counter-NBI heating beam is employed. Finally, record stored diamagnetic energy content and plasma beta values are achieved when the largest available pellets are employed. The results indicate that pellet injections extend the operational regime well beyond limits previously achieved in TJ-II without pellets. An important inter-machine study of cryogenic-pellet fueling in helical devices has also been made [4]. This was done to evaluate controlling performance bifurcations in stellarators.
2. New studies, performed with multiple pellet injections, have extended the TJ-II operational regime well beyond limits previously achieved in this device using NBI heating and gas puff<ref>2</ref>,<ref>3</ref>. In order to achieve best results, it has been determined that the plasma target electron density should to be in the range <math>1 \times 10^{19} {\mathrm m}^{-3}</math> to <math>2.5 \times 10^{19} {\mathrm m}^{-3}</math> and time separations between pellets should be close to energy confinement times, around 10 ms. It is also found, using a Charge Exchange Recombination Spectroscopy diagnostic, that while the plasma electron temperature is almost unaffected by such pellet injections, the majority ion temperature irises significantly due to reduced ion radial heat fluxes during the PiEC phase. It is also found that enhanced performance is independent of whether co- or counter-NBI heating beam is employed. Finally, record stored diamagnetic energy content and plasma beta values are achieved when the largest available pellets are employed. The results indicate that pellet injections extend the operational regime well beyond limits previously achieved in TJ-II without pellets. An important inter-machine study of cryogenic-pellet fueling in helical devices has also been made<ref>4</ref>. This was done to evaluate controlling performance bifurcations in stellarators.


3. As noted above, improvement confinement associated with the injection of pellets has been observed in TJ-II during NBI phase of its plasmas. Using a simple model, the modification of turbulent transport by a pellet injection and how this modification affects particle confinement time has been studied [5]. The results indicate a relationship between improved confinement and the evolution of shear flows due to turbulence, especially near low order rational surfaces. Furthermore, experiments show that an additional pellet, or pellets, may enhance the confinement improvement produced by the first. This effect is reproduced in the model when the second density pellet is launched soon after the first one. For this to occur, the second pellet must be injected in the transient period, before the plasma returns to the steady state. In a separate new study on enhanced confinement for a specific magnetic configuration, 100-48-65 (comparison with with and without pellets), it is found that enhanced confinement can depend strongly on plasma currents, which in turn, indicates a dependence on rotational transform (location of low-order rational surfaces in gradient region) [6].
3. As noted above, improvement confinement associated with the injection of pellets has been observed in TJ-II during NBI phase of its plasmas. Using a simple model, the modification of turbulent transport by a pellet injection and how this modification affects particle confinement time has been studied<ref>5</ref>. The results indicate a relationship between improved confinement and the evolution of shear flows due to turbulence, especially near low order rational surfaces. Furthermore, experiments show that an additional pellet, or pellets, may enhance the confinement improvement produced by the first. This effect is reproduced in the model when the second density pellet is launched soon after the first one. For this to occur, the second pellet must be injected in the transient period, before the plasma returns to the steady state. In a separate new study on enhanced confinement for a specific magnetic configuration, 100-48-65 (comparison with with and without pellets), it is found that enhanced confinement can depend strongly on plasma currents, which in turn, indicates a dependence on rotational transform (location of low-order rational surfaces in gradient region<ref>6</ref>.


4. Pellet injection experiments have been performed for a range of magnetic configurations of TJ-II in order to increase our understanding of pellet deposition profiles and of the role of rational surfaces in plasmoid drift in stellarators [7, 8, 9]. In a first instance, it is found that fast-electron impacts on a pellet can lead to ice destruction, this leading to enhanced fuelling efficiency. It is considered that a sudden pellet destruction inhibits the development of normal outward drifting of plasmoids that occurs when pellets are ablated by thermal electrons only [7]. In a separate study, plasmoid drifting is found to be significantly reduced, as is observed in tokamaks, in the vicinity of rational surfaces (rational surfaces have magnetic field lines that are periodic; i.e., the magnetic field lines close back on themselves) [8]. This is attributed to the fact that plasmoid external charge reconnection lengths shorten when close to rational surfaces, resulting in more effective damping of plasmoid drift. Although in stellarators, the effect of plasmoid external currents on drift is expected to be negligible, compared with plasmoid internal currents, this latter effect is clearly measurable in TJ-II. In addition, code simulations reveal that enhanced drift reductions near rational surfaces lead to significantly different deposition profiles for standard magnetic configurations in TJ-II. This implies that it should be possible to identify magnetic configurations that will result in more efficient pellet fuelling. In a further study in the area, a comparison was made on the influence of plasmoid-drift mechanisms on plasma fuelling by cryogenic pellets in ITER and Wendelstein 7-X [9].
4. Pellet injection experiments have been performed for a range of magnetic configurations of TJ-II in order to increase our understanding of pellet deposition profiles and of the role of rational surfaces in plasmoid drift in stellarators<ref>7</ref>. In a first instance, it is found that fast-electron impacts on a pellet can lead to ice destruction, this leading to enhanced fuelling efficiency. In a previous study, it was found that sudden pellet destruction by fast electrons inhibits the development of normal outward drifting of plasmoids that occurs when pellets are ablated by thermal electrons only. In a separate study, plasmoid drifting is found to be significantly reduced, as is observed in tokamaks, in the vicinity of rational surfaces (rational surfaces have magnetic field lines that are periodic; i.e., the magnetic field lines close back on themselves)<ref>8</ref>. This is attributed to the fact that plasmoid external charge reconnection lengths shorten when close to rational surfaces, resulting in more effective damping of plasmoid drift. Although in stellarators, the effect of plasmoid external currents on drift is expected to be negligible, compared with plasmoid internal currents, this latter effect is clearly measurable in TJ-II. In addition, code simulations reveal that enhanced drift reductions near rational surfaces lead to significantly different deposition profiles for standard magnetic configurations in TJ-II. This implies that it should be possible to identify magnetic configurations that will result in more efficient pellet fuelling. In a further study in the area, a comparison was made on the influence of plasmoid-drift mechanisms on plasma fuelling by cryogenic pellets in ITER and Wendelstein 7-X<ref>9</ref>.


5. A tracer-encapsulated solid pellet (TESPEL) system was commissioned successfully for the stellarator Wendelstein 7-X (W7-X) during its OP1.2b experimental campaign [10, 11, 12, 13]. TESPELs are polystyrene encapsulated solid pellets loaded with a single tracer or multiple tracers that are employed for impurity transport studies. During the OP1.2b campaign approximately 140 pellet injections were performed with successful delivery rate of 89%, this result showing that TESPEL production is very reliable. A significant fraction of those TESPELs were fabricated at Ciemat. A large number of TESPELs have been produced for the 2024 SOII experimental campaign on W7-X and for the 2024 campaign on the Large Helical Device (LHD) stellarator. The results for these experiments will be published in the near future.
5. A tracer-encapsulated solid pellet (TESPEL) system was commissioned successfully for the stellarator Wendelstein 7-X (W7-X) during its OP1.2b experimental campaign<ref>10</ref>,<ref>11</ref>,<ref>12</ref>,<ref>13</ref>. TESPELs are polystyrene encapsulated solid pellets loaded with a single tracer or multiple tracers that are employed for impurity transport studies. During the OP1.2b campaign approximately 140 pellet injections were performed with successful delivery rate of 89%, this result showing that TESPEL production is very reliable. A significant fraction of those TESPELs were fabricated at Ciemat. A large number of TESPELs have been produced for the 2024 SOII experimental campaign on W7-X and for the 2024 campaign on the Large Helical Device (LHD) stellarator. The results for these experiments will be published in the near future.


6. Experiments in the LHD with continuous lithium power dropping have allowed the creation of a reactor-relevant high-density plasma regime [14, 15]. This is characterized by increased energy confinement as well as surpressed turbulence and reduced impurity confinement. The transition to this regime is driven by the continuous dropping of Li-powder grains into the plasma. When such plasmas are compared to plasmas without Li-powder the achieved high-performance characteristics include: increased plasma energy & core electron temperature, reduced plasma-wall interaction, and an up to one order of magnitude reduction in plasma turbulence across the whole plasma radius in the frequency range 5 to 500 kHz. In addition, and contrary to expectations for high-density plasmas in stellarators, it is seen, when injecting TESPELs to deposit tracers in the core of this high-performance phase, that impurity confinement is significantly reduced for plasmas with Li powder when compared to confinement in discharges without Li-powder. These new results demonstrate the potential of continuous dropping of Li-powder into stellarator plasmas for simultaneously accessing enhanced confinement regimes while avoiding impurity accumulation.
6. Experiments in the LHD with continuous lithium power dropping have allowed the creation of a reactor-relevant high-density plasma regime<ref>14</ref>,<ref>15</ref>. This is characterized by increased energy confinement as well as suppressed turbulence and reduced impurity confinement. The transition to this regime is driven by the continuous dropping of Li-powder grains into the plasma. When such plasmas are compared to plasmas without Li-powder the achieved high-performance characteristics include: increased plasma energy & core electron temperature, reduced plasma-wall interaction, and an up to one order of magnitude reduction in plasma turbulence across the whole plasma radius in the frequency range 5 to 500 kHz. In addition, and contrary to expectations for high-density plasmas in stellarators, it is seen, when injecting TESPELs to deposit tracers in the core of this high-performance phase, that impurity confinement is significantly reduced for plasmas with Li powder when compared to confinement in discharges without Li-powder. These new results demonstrate the potential of continuous dropping of Li-powder into stellarator plasmas for simultaneously accessing enhanced confinement regimes while avoiding impurity accumulation.


== References ==
== References ==
PEER-REVIEWED ARTICLES ASSOCIATED TO THIS PROJECT (SINCE 2021)


[1] Enhanced confinement induced by pellet injection in the stellarator TJ-II, I. García-Cortes, K. J. McCarthy, T. Estrada, V. Tribaldos, B. van Milligen, E. Ascasíbar, R. Carrasco, A. A. Chmyga, R. García, J. Hernández-Sánchez, C. Hidalgo, S. Kozachek, F. Medina, D. Medina-Roque, M. A. Ochando, J. L. de Pablos, N. Panadero, I. Pastor and TJ-II Team, Phys. Plasmas 30 (2023) 072506. https://doi.org/10.1063/5.0151395
[1] Enhanced confinement induced by pellet injection in the stellarator TJ-II, I. García-Cortes, K. J. McCarthy, T. Estrada, V. Tribaldos, B. van Milligen, E. Ascasíbar, R. Carrasco, A. A. Chmyga, R. García, J. Hernández-Sánchez, C. Hidalgo, S. Kozachek, F. Medina, D. Medina-Roque, M. A. Ochando, J. L. de Pablos, N. Panadero, I. Pastor and TJ-II Team, Phys. Plasmas 30 (2023) 072506. https://doi.org/10.1063/5.0151395
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[6] Impact of the rotational transform on enhanced confinement in the TJ-II stellarator. Part 1: experimental results, B. Ph. van Milligen, I. García-Cortés, K. J. McCarthy, T. Estrada, A. Cappa, P. Pons-Villalonga, B. A. Carreras, L. García, O. S. Kozachok, O. O. Chmyga, J. L. de Pablos, J. M. Barcala, A Molinero, D. Tafalla, I. Pastor, A. de la Peña, F. Lapayese, (...) and the TJ-II Team, in preparation for Nucl. Fusion.
[6] Impact of the rotational transform on enhanced confinement in the TJ-II stellarator. Part 1: experimental results, B. Ph. van Milligen, I. García-Cortés, K. J. McCarthy, T. Estrada, A. Cappa, P. Pons-Villalonga, B. A. Carreras, L. García, O. S. Kozachok, O. O. Chmyga, J. L. de Pablos, J. M. Barcala, A Molinero, D. Tafalla, I. Pastor, A. de la Peña, F. Lapayese, (...) and the TJ-II Team, in preparation for Nucl. Fusion.


[7] Using rational surfaces to improve pellet fuelling efficiency in stellarators, N. Panadero, K. J. McCarthy, B. Pégourié, R. Carrasco, I. García-Cortés, R. García, J. Hernández-Sánchez, F. Köchl, J. Mártinez-Fernández, and R. Sakamoto, J. Plasma Phys. 89 (2023) 955890601. https://doi:10.1017/S0022377823001010.
[7] Overview of the TJ-II stellarator research programme towards model validation in fusion plasmas, C. Hidalgo, ..., I. García-Cortés, ..., J. Hernández-Sánchez, ..., B. López-Miranda, ..., K. J. McCarthy, ..., P. Méndez, ..., N. Panadero, ..., N. Tamura, ..., et al., Nucl. Fusion 62 (2022) 042025, https://doi.org/10.1088/1741-4326/ac2ca1
 
[8] Using rational surfaces to improve pellet fuelling efficiency in stellarators, N. Panadero, K. J. McCarthy, B. Pégourié, R. Carrasco, I. García-Cortés, R. García, J. Hernández-Sánchez, F. Köchl, J. Mártinez-Fernández, and R. Sakamoto, J. Plasma Phys. 89 (2023) 955890601. https://doi:10.1017/S0022377823001010.
 
[9] A comparison of the influence of plasmoid-drift mechanisms on plasma fuelling by cryogenic pellets in ITER and Wendelstein 7-X, N. Panadero, F. Koechl, A. R. Polevoi, J. Baldzuhn, C. D. Beidler, P. Lang, A. Loarte, A. Matsuyama, K. J. McCarthy, B. Pégourié, and Y. Turkin, Nucl. Fusion 63, 046022 (2023). https://doi.org/10.1088/1741-4326/acbc34
 
[10] Commissioning of the Tracer-Encapsulated Solid Pellet (TESPEL) Injection system for Wendelstein 7-X and first results, R. Bussiahn, N. Tamura, K. J. McCarthy, B. Buttenschön, C. Brandt, A. Dinklage, A. Langenberg and the W7-X team, Plasma Phys. Control. Fusion, 66 (2024) 115020. https://doi.org/10.1088/1741-4326/ac2cf5.
 
[11] Additional ECRH mitigates thermal quenches induced by tungsten TESPEL injection in LHD , H. Bouvain, A. Dinklage, N. Tamura, H. Igami, H. Kasahara, K. J. McCarthy, D. Medina Roque, I. García-Cortés and the LHD Experiment Group, sent to Nuclear Fusion for publication, NF-106861.
 
[12] Experimental confirmation of efficient island divertor operation and successful neoclassical transport optimization in Wendelstein 7-X, T. S. Pedersen, ..., I. García-Cortés, K. J. McCarthy, …, N. Panadero Alvarez, ..., N. Tamura, ..., Nucl Fusion 62, 042022 (2022). DOI: 10.1088/1741-4326/ac2cf5.
 
[13] Overview of the first Wendelstein 7-X long pulse campaign with fully water-cooled plasma facing components, O. Grulke, …, R. Bussiahn, ..., I. García-Cortés, ..., K. J. McCarthy, ..., D. Medina Roque, …, N. Panadero Alvarez, ..., N. Tamura, et al., Nucl Fusion 62 (2024) 112002. https://doi.org/10.1088/1741-4326/ad2f4d.
 
[14] Overview of Large Helical Device experiments of basic plasma physics for solving crucial issues in reaching burning plasma conditions , K. Ida, ..., D. Medina-Roque, ..., I. García-Córtes, ... K. J. McCarthy, …, et al., Nucl. Fusion 64, 112009 (2024). https://doi.org/10.1088/1741-4326/ad3a7a
 
[15] Reduction of impurity confinement times in lithium-powder induced reduced-turbulence plasmas in the LHD, D. Medina-Roque, F. Nespoli, I. García-Cortés, K. J. McCarthy, N. Tamura, C. Suzuki, M. Goto, T. Kawate, Y. Kawamoto, M. Yoshinuma, K. Ida, K. Tanaka, T. Tokuzawa, H. Funaba, I. Yamada and the LHD team, in preparation for Nucl. Fusion Lett.
 
 
POSTERS AND TALKS IN CONFERENCES SINCE 2021
 
 
1) TESPEL: a powerful tool for investigating impurity control in the plasma core of magnetic confinement fusion devices, K. J. McCarthy, N. Tamura, R. Bussiahn, N. Takano, F. Reimold, I. García-Cortés, D. Medina-Roque, LHD team, W7-X team, TJ-II team, Invited talk at the 33rd Symposium on Fusion Technology, Dublin, Ireland (2024).
 
2) Achieving high-performance plasma scenarios in the stellarator TJ-II using cryogenic pellet injection, K. J. McCarthy, I. García-Cortés, J. A. Alonso, A. Baciero, R. Carrasco, O. O. Chmyga, T. Estrada, L. García, R. García, J. Hernández-Sánchez, O. S. Kozachok, B. López Miranda, F. Medina, D. Medina-Roque, B. van Milligen, M. Navarro, J. L. de Pablos, N. Panadero, I. Pastor, J. de la Riva, V. Tribaldos, and TJ-II Team, Invited talk at the 24th International Stellarator Helitotron Workshop, Hiroshima, Japan (2024).
 
3) Validation of pellet deposition physics by simulation/experiment comparisons on helical devices, N. Panadero, K. J. McCarthy, J. Baldzuhn, G. Motojima, R. Sakamoto, K. Nagasaki, F. Köchl and TJ-II, W7-X, LHD and Heliotron J teams, Invited talk at the 49th EPS Conference on Plasma Physics, Bordeaux, France (2023).
 
4) Is core fuelling by pellets in helical devices as straightforward as envisaged? An overview of simulation results with the HPI2 code in helical devices, N. Panadero, K. J. McCarthy, J. Baldzuhn, G. Motojima, R. Sakamoto, K. Nagasaki, and F. Köchl, Invited talk at the 23nd International Stellarator-Heliotron Workshop, Warsaw, Poland (2022).
 
5) Enhanced confinement after multi-pellet injection into neutral beam injection heated plasmas in the stellarator TJ-II, K. J. McCarthy, I. García-Cortés, A. V. Melnikov, N. Panadero, E. Ascasíbar, M. Drabinskiy, L. G. Eliseev, T. Estrada, J. Hernández-Sánchez, P. Khabanov, A. S. Kozachek, M. Liniers, S. E. Lysenko, D. Medina-Roque, P. Medina, M. A. Ochando, J. L. de Pablos, I. Pastor, C. Toledo, B. van Milligen, & TJ-II team, Oral talk at the 48th EPS Conf. Plasma Phys., Maastricht, The Netherlands (2022).
 
6) Pellet injection in the stellarator TJ-II for fuelling and impurity control studies, I. García-Cortés, K. J. McCarthy, D. Medina-Roque, N. Tamura, A. Baciero, R. Carrasco, O. O. Chmyga, T. Estrada, R. García, J. Hernández-Sánchez, O. S. Kozachok, B. López Miranda, F. Medina, B. van Milligen, M. Navarro, J. L. de Pablos, N. Panadero, I. Pastor, J. de la Riva, V. Tribaldos and TJ-II Team, Oral talk at the XXXIX Reunión Bienal de la Real Sociedad Español de Física, Donostia/San Sebastián, Spain (2024).
 
7) Enhanced-performance scenarios in the stellarator TJ-II using pellet injection, I. García-Cortés, K. J. McCarthy, D. Medina-Roque, A. Baciero, R. Carrasco, O. Chmyga, T. Estrada, L. García, J. Hernández-Sánchez, O. S. Kozachok, B. López Miranda, F. Medina, B. van Milligen, N. Panadero, I. Pastor, J. de la Riva, D. Tafalla, V. Tribaldos, and the TJ-II Team, Oral talk at the 50th EPS Conference on Plasma Physics, Salamanca, Spain (2024).
 
8) Controlling performance bifurcations in large stellarators, an intermachine study of cryogenic fueling in helical devices, A. Dinklage, …, A. Alonso, … I. García-Cortés, …, K. McCarthy, … N. Panadero, et al., the TJ-II team, Oral talk at the 29th Fusion Energy Conference, London, England (2023).
 
9) Enhanced plasma performance after pellet injections in the stellarator TJ-II, K. J. McCarthy, I. García-Cortés, V. Tribaldos, T. Estrada, D. Medina Roque, B. van Milligen, N. Panadero, E. Ascasíbar, R. Carrasco, R. García, J. Hernández Sánchez, B. López Miranda, A. S. Kozachek, I. Pastor, A. A. Chmyga, and TJ-II team, 29th IAEA-Fusion Energy Conference, Poster presentation at the 29th Fusion Energy Conference, London, England (2023).
 
10) Physics Studies of Cryogenic Pellet and Tracer-loaded Pellet (TESPEL) injections in the Stellarator TJ-II, K. J. McCarthy, N. Panadero, I. García Cortes, E. Ascasíbar, A. Cappa, J. M. Fontdecaba, J. Hernández Sánchez, M. Liners, I. Pastor, TJ-II Team, N. Tamura, and G. Motojima, Poster presentation at the 28th IAEA-FEC Conference, Nice, France (2021).
 
12) Influence of the magnetic well on pellet fuelling in the TJ-II stellarator, N. Panadero, K. J. McCarthy, I. García Cortés, B. López Miranda, et al., and TJ-II Team, Poster presentation at the 24th International Stellarator Helitotron Workshop, Hiroshima, Japan (2024).
 
13) A study on Z-dependence of impurity confinement and transport in turbulence reduced plasmas via lithium powder injection in LHD, D. Medina-Roque, I. García-Cortés, K. J. McCarthy, N. Tamura, F. Nespoli, C. Suzuki, M. Goto, T. Kawate, Y. Kawamoto, M. Yoshinuma, K. Ida, K. Tanaka, T. Tokuzawa, H. Funaba, I. Yamada and the LHD team, Poster presentation at the 50th EPS Conference on Plasma Physics, Salamanca, Spain (2024).
 
14) Neoclassical analysis of the enhanced-performance scenarios in the stellarator TJ-II after pellet injection, V. Tribaldos, I. García-Cortés, B. Ph. van Milligen, K. J. McCarthy and TJ-II team, Poster presentation at the 50th EPS Conference on Plasma Physics, Salamanca, Spain (2024).
 
15) Impact of low order rationals in the enhanced confinement by pellet injection in TJ-II, L. García, B. A. Carreras, I. García-Cortés, B. Ph. van Milligen, K. J. McCarthy and TJ-II team, Poster presentation at the 50th EPS Conference on Plasma Physics, Salamanca, Spain (2024).
 
16) Characterization of the impact of pellet injections on fast-ion losses in NBI plasmas in the TJ-II stellarator, B. López-Miranda, N. Panadero, C. Salcuni, Á. Cappa, A. Baciero, R. García, I. García-Cortés, J. Hernández-Sánchez, D. Jiménez-Rey, D. López-Bruna, D. Medina, F. Medina, K. J. McCarthy, I. Pastor, J. de la Riva, Poster presentation at the 50th EPS Conference on Plasma Physics, Salamanca, Spain (2024).
 
17) Additional ECRH mitigates thermal quenches induced by tungsten TESPEL injection in LHD, H. Bouvain, A. Dinklage, N. Tamura, H. Kasahara, R. Bussiahn, K. McCarthy, D. Medinaand the LHD Team, Poster presentation at the 29th IAEA Fusion Energy Conference, London, England (2023).
 
18) TESPEL studies on the Z-dependence of impurity transport in different plasma scenarios in LHD, D. Medina, N. Tamura, I. García-Cortés, K. J. McCarthy & LHD team, 49th EPS Conf. Plasma Phys., Bordeaux, France (2023).


[8] A comparison of the influence of plasmoid-drift mechanisms on plasma fuelling by cryogenic pellets in ITER and Wendelstein 7-X, N. Panadero, F. Koechl, A. R. Polevoi, J. Baldzuhn, C. D. Beidler, P. Lang, A. Loarte, A. Matsuyama, K. J. McCarthy, B. Pégourié, and Y. Turkin, Nucl. Fusion 63, 046022 (2023). https://doi.org/10.1088/1741-4326/acbc34
19) Studying fast-ion losses induced by Alfvén Eigenmodes and by pellet injection in NBI heated plasmas of the stellarator TJ-II, B. López-Miranda, A. Baciero, D. Jiménez-Rey, K. J. McCarthy, I. García-Cortés, N. Panadero, D. Medina-Roque, J. Hernández Sánchez, A. Cappa, P. Pons, F. Medina, and I. Pastor, 49th EPS Conf. Plasma Phys., Bordeaux, France (2023).


[9] Commissioning of the Tracer-Encapsulated Solid Pellet (TESPEL) Injection system for Wendelstein 7-X and first results, R. Bussiahn, N. Tamura, K. J. McCarthy, B. Buttenschön, C. Brandt, A. Dinklage, A. Langenberg and the W7-X team, Plasma Phys. Control. Fusion, 66 (2024) 115020. https://doi.org/10.1088/1741-4326/ac2cf5.
20) Enhanced confinement induced by multi-pellet injection into neutral beam injection heated plasmas in the stellarator TJ-II, I. García-Cortés, K. J. McCarthy, V. Tribaldos, D. Medina-Roque, N. Panadero, E. Ascasíbar, T. Estrada, J. Hernández-Sánchez, A. S. Kozachek, M. Liniers, S. E. Lysenko, D. Medina-Roque, P. Medina, M. A. Ochando, J. L. de Pablos, I. Pastor, B. van Milligen & TJ-II team, Poster presentation at the 49th EPS Conf. Plasma Phys., Bordeaux, France (2023).


[10] Additional ECRH mitigates thermal quenches induced by tungsten TESPEL injection in LHD , H. Bouvain, A. Dinklage, N. Tamura, H. Igami, H. Kasahara, K. J. McCarthy, D. Medina Roque, I. García-Cortés and the LHD Experiment Group, sent to Nuclear Fusion for publication, NF-106861.  
21) On the radial pellet cloud drift in stellarator plasmas, G. Kocsis, J. Baldzuhn, C. Biedermann, R. Bussiahn, A. Buzás, G. Cseh, I. García-Cortés, M. Krause, K. J. McCarthy, D. Medina-Roque, N. Panadero, T. Szepesi, N. Tamura, Th. Wegner, TJ-II team and W7-X team, Poster presentation at the 49th EPS Conf. Plasma Phys., Bordeaux, France (2023).


[11] Experimental confirmation of efficient island divertor operation and successful neoclassical transport optimization in Wendelstein 7-X, T. S. Pedersen, ..., I. García-Cortés, K. J. McCarthy, …, N. Panadero Alvarez, ..., N. Tamura, ..., Nucl Fusion 62, 042022 (2022). DOI: 10.1088/1741-4326/ac2cf5.
22) New Insights into cryogenic and TESPEL pellet physics in TJ-II, D. Medina-Roque, I. García-Cortés, K. J. McCarthy, N. Tamura, N. Panadero, E. Ascasíbar, T. Estrada, J. Hernández-Sánchez, A. S. Kosachek, M. Liniers, P. Medina, M. A. Ochando, J. L. de Pablos, I. Pastor, C. Toledo, B. van Milligen & TJ-II team, Poster presentation at the 48th EPS Conf. Plasma Phys., Maastricht, The Netherlands (2022).


[12] Overview of the first Wendelstein 7-X long pulse campaign with fully water-cooled plasma facing components, O. Grulke, …, R. Bussiahn, ..., I. García-Cortés, ..., K. J. McCarthy, ..., D. Medina Roque, …, N. Panadero Alvarez, ..., N. Tamura, et al., Nucl Fusion 62 (2024) 112002. https://doi.org/10.1088/1741-4326/ad2f4d.
23) Pellet studies with an upgraded fast-camera system in the stellarator TJ-II, N. Panadero, G. Kocsis, T. Szepesi, K. J. McCarthy, G. Motojima, E. de la Cal, J. Hernández Sánchez, A. Ros, and TJ-II Team, Poster presentation at the 47th EPS Conference on Plasma Physics, On-line Event (2020/21).


[13] Overview of Large Helical Device experiments of basic plasma physics for solving crucial issues in reaching burning plasma conditions , K. Ida, ..., D. Medina-Roque, ..., I. García-Córtes, ... K. J. McCarthy, …, et al., Nucl. Fusion 64, 112009 (2024). https://doi.org/10.1088/1741-4326/ad3a7a
24) Impurity transport studies on Wendelstein 7-X by Tracer-Encapsulated Solid Pellets, R. Bussiahn, N. Tamura, K.J. McCarthy and the W7-X team, Poster presentation at the 47th EPS Conference on Plasma Physics, On-line Event (2020/21).


[14] Reduction of impurity confinement times in lithium-powder induced reduced-turbulence plasmas in the LHD, D. Medina-Roque, F. Nespoli, I. García-Cortés, K. J. McCarthy, N. Tamura, C. Suzuki, M. Goto, T. Kawate, Y. Kawamoto, M. Yoshinuma, K. Ida, K. Tanaka, T. Tokuzawa, H. Funaba, I. Yamada and the LHD team, in preparation for Nucl. Fusion Lett.




Latest revision as of 15:09, 11 November 2024

LNF - Nationally funded project

Title: Fuelling and Impurity Control Studies in the stellarators TJ-II and W7-X using Cryogenic Pellets and Tracer-Encapsulated Solid Pellets (TESPEL)e

Reference: PID2020-116599RB-I00

Funding Umbrella: Plan Estatal de Investigación Científica y Técnica y de Innovación 2021-2023

Funding Programme: Proyecto de investigación subvencionado por el Ministerio de Ciencia e Innovación

Subprogramme: Proyectos de I+D+i Retos Investigación

Programme and date: Proyectos I+D+i 2020

Programme type/ Modalidad:

Area/subarea: Physical Sciences / Physics and its applications

Principal Investigator(s): Kieran Joseph McCarthy María Isabel García Cortés

Project type: Investigación Orientada Tipo B

Start-end dates: 01/09/2021 - 31/08/2025

Financing granted (direct costs): 130000 €

Description of the project

The goal of this project, which falls within the realm of magnetic confinement nuclear fusion, is to continue research initiated in projects ENE2013-48679-R and FIS2017-89326-R on fuelling and impurity control in plasmas created in the stellarators TJ-II (Ciemat, Madrid) and W7-X (Greifswald, Germany). Further research to resolve these issues is critical to demonstrate steady-state operation of helical-type fusion reactors, in particular to identify operational scenarios that ensure adequate plasma fuelling and avoidance of impurity accumulation. This project will contribute to the development and scientific exploitation of stellarators, a priority highlighted in the document "Fusion Electricity: a roadmap to the realization of fusion energy" (EFDA 2012).

1. The first aim is to investigate aspects of plasma fuelling that are still not fully understood and the effects of fuel pellets on plasma magnetic activity, plasma turbulence and plasma performance. For this, the medium-sized heliac TJ-II will be used. It is equipped with a cryogenic pellet injector (PI) for producing solid hydrogen pellets that can be injected at high velocity into the plasma. It is intended to investigate pellet fuelling as a means to enhance plasma confinement (higher stored energy, longer particle confinement) and to identify and explore new pellet phenomena. While TJ-II is equipped with a large number of modern diagnostics, it is proposed to develop a new system to measure pellet cloud density and temperature to extend knowledge of pellet physics.

2. The second aim is to continue to support impurity transport and accumulation studies in TJ-II and W7-X. Under the umbrella of a trilateral collaboration (2020-2029) with the National Institute for Fusion Science (Japan) and IPP-Max-Planck (Greifswald, Germany), Tracer-Encapsulated Solid Pellet (TESPEL) injections systems hare now operated on both TJ-II and W7-X. TESPELs are polystyrene spheres (diameter <1 mm) loaded with impurity tracers (atomic elements other than fuel). This allows delivering a precise quantify of tracer to a preselected location in the plasma core, after which its transport and confinement can be studied. An important aspect of the collaboration has been the establishment of a laboratory to fabricate TESPELs at Ciemat for both devices (project FIS2017- 89326-R). Key parts of this current project are to continue TESPEL fabrication for TJ-II and W7-X at this laboratory, thereby allowing Ciemat to maintain this fruitful collaboration, and to upgrade a vacuum ultraviolet spectrometer on TJ-II to provide important spectral line data for impurity identification in W7-X.

The PI and TESPEL systems on TJ-II share a common injection guide lines. This unique set-up allows direct comparative studies of ablation, deposition and plasma response to be made thereby facilitating the understanding of common physics. Given that fuelling and impurity control are critical issues for stellarator steady-state operation, the project will allow us to continue to contribute to, and participate in, research programmes on W7-X, the stellarator of reference. Finally, team members have significant experience in the formation of young researchers at Master and PhD levels and in disseminating research to second level students and to the general public. A PhD student will undertake research in these areas during the project.

Main Results

1. A pellet-induced enhanced confinement regime (or PiEC) has been identified in Neutral Beam Injection (NBI) heated discharges made in TJ-II after the injection of a single cryogenic fuel pellet into its plasma core [1]. In addition to the expected increase in core electron density, the plasma diamagnetic energy content, as determined using a diamagnetic loop, is seen to rise by up to 40%, with respect to reference discharges without pellet injection. Furthermore, the energy confinement time is significantly enhanced when compared to predictions obtained using the 2004 International Stellarator Scaling law, ISS04. Indeed, the operational regimes of other stellarator devices, such as LHD and W7-X, can be similarly extended to performance well beyond those obtainable with gas puffing alone.

2. New studies, performed with multiple pellet injections, have extended the TJ-II operational regime well beyond limits previously achieved in this device using NBI heating and gas puff[2],[3]. In order to achieve best results, it has been determined that the plasma target electron density should to be in the range to and time separations between pellets should be close to energy confinement times, around 10 ms. It is also found, using a Charge Exchange Recombination Spectroscopy diagnostic, that while the plasma electron temperature is almost unaffected by such pellet injections, the majority ion temperature irises significantly due to reduced ion radial heat fluxes during the PiEC phase. It is also found that enhanced performance is independent of whether co- or counter-NBI heating beam is employed. Finally, record stored diamagnetic energy content and plasma beta values are achieved when the largest available pellets are employed. The results indicate that pellet injections extend the operational regime well beyond limits previously achieved in TJ-II without pellets. An important inter-machine study of cryogenic-pellet fueling in helical devices has also been made[4]. This was done to evaluate controlling performance bifurcations in stellarators.

3. As noted above, improvement confinement associated with the injection of pellets has been observed in TJ-II during NBI phase of its plasmas. Using a simple model, the modification of turbulent transport by a pellet injection and how this modification affects particle confinement time has been studied[5]. The results indicate a relationship between improved confinement and the evolution of shear flows due to turbulence, especially near low order rational surfaces. Furthermore, experiments show that an additional pellet, or pellets, may enhance the confinement improvement produced by the first. This effect is reproduced in the model when the second density pellet is launched soon after the first one. For this to occur, the second pellet must be injected in the transient period, before the plasma returns to the steady state. In a separate new study on enhanced confinement for a specific magnetic configuration, 100-48-65 (comparison with with and without pellets), it is found that enhanced confinement can depend strongly on plasma currents, which in turn, indicates a dependence on rotational transform (location of low-order rational surfaces in gradient region[6].

4. Pellet injection experiments have been performed for a range of magnetic configurations of TJ-II in order to increase our understanding of pellet deposition profiles and of the role of rational surfaces in plasmoid drift in stellarators[7]. In a first instance, it is found that fast-electron impacts on a pellet can lead to ice destruction, this leading to enhanced fuelling efficiency. In a previous study, it was found that sudden pellet destruction by fast electrons inhibits the development of normal outward drifting of plasmoids that occurs when pellets are ablated by thermal electrons only. In a separate study, plasmoid drifting is found to be significantly reduced, as is observed in tokamaks, in the vicinity of rational surfaces (rational surfaces have magnetic field lines that are periodic; i.e., the magnetic field lines close back on themselves)[8]. This is attributed to the fact that plasmoid external charge reconnection lengths shorten when close to rational surfaces, resulting in more effective damping of plasmoid drift. Although in stellarators, the effect of plasmoid external currents on drift is expected to be negligible, compared with plasmoid internal currents, this latter effect is clearly measurable in TJ-II. In addition, code simulations reveal that enhanced drift reductions near rational surfaces lead to significantly different deposition profiles for standard magnetic configurations in TJ-II. This implies that it should be possible to identify magnetic configurations that will result in more efficient pellet fuelling. In a further study in the area, a comparison was made on the influence of plasmoid-drift mechanisms on plasma fuelling by cryogenic pellets in ITER and Wendelstein 7-X[9].

5. A tracer-encapsulated solid pellet (TESPEL) system was commissioned successfully for the stellarator Wendelstein 7-X (W7-X) during its OP1.2b experimental campaign[10],[11],[12],[13]. TESPELs are polystyrene encapsulated solid pellets loaded with a single tracer or multiple tracers that are employed for impurity transport studies. During the OP1.2b campaign approximately 140 pellet injections were performed with successful delivery rate of 89%, this result showing that TESPEL production is very reliable. A significant fraction of those TESPELs were fabricated at Ciemat. A large number of TESPELs have been produced for the 2024 SOII experimental campaign on W7-X and for the 2024 campaign on the Large Helical Device (LHD) stellarator. The results for these experiments will be published in the near future.

6. Experiments in the LHD with continuous lithium power dropping have allowed the creation of a reactor-relevant high-density plasma regime[14],[15]. This is characterized by increased energy confinement as well as suppressed turbulence and reduced impurity confinement. The transition to this regime is driven by the continuous dropping of Li-powder grains into the plasma. When such plasmas are compared to plasmas without Li-powder the achieved high-performance characteristics include: increased plasma energy & core electron temperature, reduced plasma-wall interaction, and an up to one order of magnitude reduction in plasma turbulence across the whole plasma radius in the frequency range 5 to 500 kHz. In addition, and contrary to expectations for high-density plasmas in stellarators, it is seen, when injecting TESPELs to deposit tracers in the core of this high-performance phase, that impurity confinement is significantly reduced for plasmas with Li powder when compared to confinement in discharges without Li-powder. These new results demonstrate the potential of continuous dropping of Li-powder into stellarator plasmas for simultaneously accessing enhanced confinement regimes while avoiding impurity accumulation.

References

PEER-REVIEWED ARTICLES ASSOCIATED TO THIS PROJECT (SINCE 2021)

[1] Enhanced confinement induced by pellet injection in the stellarator TJ-II, I. García-Cortes, K. J. McCarthy, T. Estrada, V. Tribaldos, B. van Milligen, E. Ascasíbar, R. Carrasco, A. A. Chmyga, R. García, J. Hernández-Sánchez, C. Hidalgo, S. Kozachek, F. Medina, D. Medina-Roque, M. A. Ochando, J. L. de Pablos, N. Panadero, I. Pastor and TJ-II Team, Phys. Plasmas 30 (2023) 072506. https://doi.org/10.1063/5.0151395

[2] Multi-pellet injection into the NBI-heated phase of TJ-II plasmas, K. J. McCarthy, I. García-Cortés, 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. Herranz, 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, Nucl. Fusion 64 (2024) 066019, https://doi.org/10.1088/1741-4326/ad4047.

[3] Density profiles in stellarators: an overview of particle transport, fueling and profile shaping studies at TJ-II, J. A. Alonso, …, I. García-Cortés, ..., J. Hernández-Sánchez, ..., B. López-Miranda, ..., K. J. McCarthy, ..., D. Medina-Roque, ..., P. Méndez, ..., N. Panadero, ..., N. Tamura, ..., et al., Nucl. Fusion 64 (2024) 112018. https://doi.org/10.1088/1741-4326/ad67ef

[4] Controlling performance bifurcations in stellarators - an inter-machine study of cryogenic-pellet fueling in helical devices, A. Dinklage, ..., I. García-Cortés, ..., K. McCarthy, D. Medina-Roque, ..., N. Tamura, ..., The Heliotron-J Team, The TJ-II Team, The LHD Experiment Team and the W7-X Team, sent to Nucl. Fusion, NF-107510.

[5] The effect of pellet injection on turbulent transport in TJ-II, L. García, I. García-Cortés, B. A. Carreras, K. J. McCarthy, B. van Milligen and TJ-II team, Phys. Plasmas 30 (2023) 092303. https://doi.org/10.1063/5.0163832

[6] Impact of the rotational transform on enhanced confinement in the TJ-II stellarator. Part 1: experimental results, B. Ph. van Milligen, I. García-Cortés, K. J. McCarthy, T. Estrada, A. Cappa, P. Pons-Villalonga, B. A. Carreras, L. García, O. S. Kozachok, O. O. Chmyga, J. L. de Pablos, J. M. Barcala, A Molinero, D. Tafalla, I. Pastor, A. de la Peña, F. Lapayese, (...) and the TJ-II Team, in preparation for Nucl. Fusion.

[7] Overview of the TJ-II stellarator research programme towards model validation in fusion plasmas, C. Hidalgo, ..., I. García-Cortés, ..., J. Hernández-Sánchez, ..., B. López-Miranda, ..., K. J. McCarthy, ..., P. Méndez, ..., N. Panadero, ..., N. Tamura, ..., et al., Nucl. Fusion 62 (2022) 042025, https://doi.org/10.1088/1741-4326/ac2ca1

[8] Using rational surfaces to improve pellet fuelling efficiency in stellarators, N. Panadero, K. J. McCarthy, B. Pégourié, R. Carrasco, I. García-Cortés, R. García, J. Hernández-Sánchez, F. Köchl, J. Mártinez-Fernández, and R. Sakamoto, J. Plasma Phys. 89 (2023) 955890601. https://doi:10.1017/S0022377823001010.

[9] A comparison of the influence of plasmoid-drift mechanisms on plasma fuelling by cryogenic pellets in ITER and Wendelstein 7-X, N. Panadero, F. Koechl, A. R. Polevoi, J. Baldzuhn, C. D. Beidler, P. Lang, A. Loarte, A. Matsuyama, K. J. McCarthy, B. Pégourié, and Y. Turkin, Nucl. Fusion 63, 046022 (2023). https://doi.org/10.1088/1741-4326/acbc34

[10] Commissioning of the Tracer-Encapsulated Solid Pellet (TESPEL) Injection system for Wendelstein 7-X and first results, R. Bussiahn, N. Tamura, K. J. McCarthy, B. Buttenschön, C. Brandt, A. Dinklage, A. Langenberg and the W7-X team, Plasma Phys. Control. Fusion, 66 (2024) 115020. https://doi.org/10.1088/1741-4326/ac2cf5.

[11] Additional ECRH mitigates thermal quenches induced by tungsten TESPEL injection in LHD , H. Bouvain, A. Dinklage, N. Tamura, H. Igami, H. Kasahara, K. J. McCarthy, D. Medina Roque, I. García-Cortés and the LHD Experiment Group, sent to Nuclear Fusion for publication, NF-106861.

[12] Experimental confirmation of efficient island divertor operation and successful neoclassical transport optimization in Wendelstein 7-X, T. S. Pedersen, ..., I. García-Cortés, K. J. McCarthy, …, N. Panadero Alvarez, ..., N. Tamura, ..., Nucl Fusion 62, 042022 (2022). DOI: 10.1088/1741-4326/ac2cf5.

[13] Overview of the first Wendelstein 7-X long pulse campaign with fully water-cooled plasma facing components, O. Grulke, …, R. Bussiahn, ..., I. García-Cortés, ..., K. J. McCarthy, ..., D. Medina Roque, …, N. Panadero Alvarez, ..., N. Tamura, et al., Nucl Fusion 62 (2024) 112002. https://doi.org/10.1088/1741-4326/ad2f4d.

[14] Overview of Large Helical Device experiments of basic plasma physics for solving crucial issues in reaching burning plasma conditions , K. Ida, ..., D. Medina-Roque, ..., I. García-Córtes, ... K. J. McCarthy, …, et al., Nucl. Fusion 64, 112009 (2024). https://doi.org/10.1088/1741-4326/ad3a7a

[15] Reduction of impurity confinement times in lithium-powder induced reduced-turbulence plasmas in the LHD, D. Medina-Roque, F. Nespoli, I. García-Cortés, K. J. McCarthy, N. Tamura, C. Suzuki, M. Goto, T. Kawate, Y. Kawamoto, M. Yoshinuma, K. Ida, K. Tanaka, T. Tokuzawa, H. Funaba, I. Yamada and the LHD team, in preparation for Nucl. Fusion Lett.


POSTERS AND TALKS IN CONFERENCES SINCE 2021


1) TESPEL: a powerful tool for investigating impurity control in the plasma core of magnetic confinement fusion devices, K. J. McCarthy, N. Tamura, R. Bussiahn, N. Takano, F. Reimold, I. García-Cortés, D. Medina-Roque, LHD team, W7-X team, TJ-II team, Invited talk at the 33rd Symposium on Fusion Technology, Dublin, Ireland (2024).

2) Achieving high-performance plasma scenarios in the stellarator TJ-II using cryogenic pellet injection, K. J. McCarthy, I. García-Cortés, J. A. Alonso, A. Baciero, R. Carrasco, O. O. Chmyga, T. Estrada, L. García, R. García, J. Hernández-Sánchez, O. S. Kozachok, B. López Miranda, F. Medina, D. Medina-Roque, B. van Milligen, M. Navarro, J. L. de Pablos, N. Panadero, I. Pastor, J. de la Riva, V. Tribaldos, and TJ-II Team, Invited talk at the 24th International Stellarator Helitotron Workshop, Hiroshima, Japan (2024).

3) Validation of pellet deposition physics by simulation/experiment comparisons on helical devices, N. Panadero, K. J. McCarthy, J. Baldzuhn, G. Motojima, R. Sakamoto, K. Nagasaki, F. Köchl and TJ-II, W7-X, LHD and Heliotron J teams, Invited talk at the 49th EPS Conference on Plasma Physics, Bordeaux, France (2023).

4) Is core fuelling by pellets in helical devices as straightforward as envisaged? An overview of simulation results with the HPI2 code in helical devices, N. Panadero, K. J. McCarthy, J. Baldzuhn, G. Motojima, R. Sakamoto, K. Nagasaki, and F. Köchl, Invited talk at the 23nd International Stellarator-Heliotron Workshop, Warsaw, Poland (2022).

5) Enhanced confinement after multi-pellet injection into neutral beam injection heated plasmas in the stellarator TJ-II, K. J. McCarthy, I. García-Cortés, A. V. Melnikov, N. Panadero, E. Ascasíbar, M. Drabinskiy, L. G. Eliseev, T. Estrada, J. Hernández-Sánchez, P. Khabanov, A. S. Kozachek, M. Liniers, S. E. Lysenko, D. Medina-Roque, P. Medina, M. A. Ochando, J. L. de Pablos, I. Pastor, C. Toledo, B. van Milligen, & TJ-II team, Oral talk at the 48th EPS Conf. Plasma Phys., Maastricht, The Netherlands (2022).

6) Pellet injection in the stellarator TJ-II for fuelling and impurity control studies, I. García-Cortés, K. J. McCarthy, D. Medina-Roque, N. Tamura, A. Baciero, R. Carrasco, O. O. Chmyga, T. Estrada, R. García, J. Hernández-Sánchez, O. S. Kozachok, B. López Miranda, F. Medina, B. van Milligen, M. Navarro, J. L. de Pablos, N. Panadero, I. Pastor, J. de la Riva, V. Tribaldos and TJ-II Team, Oral talk at the XXXIX Reunión Bienal de la Real Sociedad Español de Física, Donostia/San Sebastián, Spain (2024).

7) Enhanced-performance scenarios in the stellarator TJ-II using pellet injection, I. García-Cortés, K. J. McCarthy, D. Medina-Roque, A. Baciero, R. Carrasco, O. Chmyga, T. Estrada, L. García, J. Hernández-Sánchez, O. S. Kozachok, B. López Miranda, F. Medina, B. van Milligen, N. Panadero, I. Pastor, J. de la Riva, D. Tafalla, V. Tribaldos, and the TJ-II Team, Oral talk at the 50th EPS Conference on Plasma Physics, Salamanca, Spain (2024).

8) Controlling performance bifurcations in large stellarators, an intermachine study of cryogenic fueling in helical devices, A. Dinklage, …, A. Alonso, … I. García-Cortés, …, K. McCarthy, … N. Panadero, et al., the TJ-II team, Oral talk at the 29th Fusion Energy Conference, London, England (2023).

9) Enhanced plasma performance after pellet injections in the stellarator TJ-II, K. J. McCarthy, I. García-Cortés, V. Tribaldos, T. Estrada, D. Medina Roque, B. van Milligen, N. Panadero, E. Ascasíbar, R. Carrasco, R. García, J. Hernández Sánchez, B. López Miranda, A. S. Kozachek, I. Pastor, A. A. Chmyga, and TJ-II team, 29th IAEA-Fusion Energy Conference, Poster presentation at the 29th Fusion Energy Conference, London, England (2023).

10) Physics Studies of Cryogenic Pellet and Tracer-loaded Pellet (TESPEL) injections in the Stellarator TJ-II, K. J. McCarthy, N. Panadero, I. García Cortes, E. Ascasíbar, A. Cappa, J. M. Fontdecaba, J. Hernández Sánchez, M. Liners, I. Pastor, TJ-II Team, N. Tamura, and G. Motojima, Poster presentation at the 28th IAEA-FEC Conference, Nice, France (2021).

12) Influence of the magnetic well on pellet fuelling in the TJ-II stellarator, N. Panadero, K. J. McCarthy, I. García Cortés, B. López Miranda, et al., and TJ-II Team, Poster presentation at the 24th International Stellarator Helitotron Workshop, Hiroshima, Japan (2024).

13) A study on Z-dependence of impurity confinement and transport in turbulence reduced plasmas via lithium powder injection in LHD, D. Medina-Roque, I. García-Cortés, K. J. McCarthy, N. Tamura, F. Nespoli, C. Suzuki, M. Goto, T. Kawate, Y. Kawamoto, M. Yoshinuma, K. Ida, K. Tanaka, T. Tokuzawa, H. Funaba, I. Yamada and the LHD team, Poster presentation at the 50th EPS Conference on Plasma Physics, Salamanca, Spain (2024).

14) Neoclassical analysis of the enhanced-performance scenarios in the stellarator TJ-II after pellet injection, V. Tribaldos, I. García-Cortés, B. Ph. van Milligen, K. J. McCarthy and TJ-II team, Poster presentation at the 50th EPS Conference on Plasma Physics, Salamanca, Spain (2024).

15) Impact of low order rationals in the enhanced confinement by pellet injection in TJ-II, L. García, B. A. Carreras, I. García-Cortés, B. Ph. van Milligen, K. J. McCarthy and TJ-II team, Poster presentation at the 50th EPS Conference on Plasma Physics, Salamanca, Spain (2024).

16) Characterization of the impact of pellet injections on fast-ion losses in NBI plasmas in the TJ-II stellarator, B. López-Miranda, N. Panadero, C. Salcuni, Á. Cappa, A. Baciero, R. García, I. García-Cortés, J. Hernández-Sánchez, D. Jiménez-Rey, D. López-Bruna, D. Medina, F. Medina, K. J. McCarthy, I. Pastor, J. de la Riva, Poster presentation at the 50th EPS Conference on Plasma Physics, Salamanca, Spain (2024).

17) Additional ECRH mitigates thermal quenches induced by tungsten TESPEL injection in LHD, H. Bouvain, A. Dinklage, N. Tamura, H. Kasahara, R. Bussiahn, K. McCarthy, D. Medinaand the LHD Team, Poster presentation at the 29th IAEA Fusion Energy Conference, London, England (2023).

18) TESPEL studies on the Z-dependence of impurity transport in different plasma scenarios in LHD, D. Medina, N. Tamura, I. García-Cortés, K. J. McCarthy & LHD team, 49th EPS Conf. Plasma Phys., Bordeaux, France (2023).

19) Studying fast-ion losses induced by Alfvén Eigenmodes and by pellet injection in NBI heated plasmas of the stellarator TJ-II, B. López-Miranda, A. Baciero, D. Jiménez-Rey, K. J. McCarthy, I. García-Cortés, N. Panadero, D. Medina-Roque, J. Hernández Sánchez, A. Cappa, P. Pons, F. Medina, and I. Pastor, 49th EPS Conf. Plasma Phys., Bordeaux, France (2023).

20) Enhanced confinement induced by multi-pellet injection into neutral beam injection heated plasmas in the stellarator TJ-II, I. García-Cortés, K. J. McCarthy, V. Tribaldos, D. Medina-Roque, N. Panadero, E. Ascasíbar, T. Estrada, J. Hernández-Sánchez, A. S. Kozachek, M. Liniers, S. E. Lysenko, D. Medina-Roque, P. Medina, M. A. Ochando, J. L. de Pablos, I. Pastor, B. van Milligen & TJ-II team, Poster presentation at the 49th EPS Conf. Plasma Phys., Bordeaux, France (2023).

21) On the radial pellet cloud drift in stellarator plasmas, G. Kocsis, J. Baldzuhn, C. Biedermann, R. Bussiahn, A. Buzás, G. Cseh, I. García-Cortés, M. Krause, K. J. McCarthy, D. Medina-Roque, N. Panadero, T. Szepesi, N. Tamura, Th. Wegner, TJ-II team and W7-X team, Poster presentation at the 49th EPS Conf. Plasma Phys., Bordeaux, France (2023).

22) New Insights into cryogenic and TESPEL pellet physics in TJ-II, D. Medina-Roque, I. García-Cortés, K. J. McCarthy, N. Tamura, N. Panadero, E. Ascasíbar, T. Estrada, J. Hernández-Sánchez, A. S. Kosachek, M. Liniers, P. Medina, M. A. Ochando, J. L. de Pablos, I. Pastor, C. Toledo, B. van Milligen & TJ-II team, Poster presentation at the 48th EPS Conf. Plasma Phys., Maastricht, The Netherlands (2022).

23) Pellet studies with an upgraded fast-camera system in the stellarator TJ-II, N. Panadero, G. Kocsis, T. Szepesi, K. J. McCarthy, G. Motojima, E. de la Cal, J. Hernández Sánchez, A. Ros, and TJ-II Team, Poster presentation at the 47th EPS Conference on Plasma Physics, On-line Event (2020/21).

24) Impurity transport studies on Wendelstein 7-X by Tracer-Encapsulated Solid Pellets, R. Bussiahn, N. Tamura, K.J. McCarthy and the W7-X team, Poster presentation at the 47th EPS Conference on Plasma Physics, On-line Event (2020/21).


Back to list of nationally funded projects

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