EUTERPE: Difference between revisions

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The EUTERPE gyrokinetic code was created at the CRPP in Lausanne as a global linear particle in cell code for studying electrostatic plasma instabilities <ref>[http://www.ispp.it/Courses_and_Workshops.html G. Jost, T. M. Tran, K. Appert, W. A. Cooper, and L. Villard, in Theory of Fusion Plasmas, International Workshop, Varenna, September 1998 (Editrice Compositori, Società Italiana di Fisica, Bologna, 1999), p. 419.]</ref>. It allows three-dimensional turbulence simulations using a plasma equilibrium calculated with the [[VMEC]] code as a starting point. EUTERPE was further developed at the Max Planck IPP and several linear calculations of ion temperature gradient (ITG) driven turbulence in [[Tokamak|tokamak]] and [[Stellarator|stellarator]] geometry have been carried out using it  
The EUTERPE gyrokinetic code was created at the CRPP in Lausanne as a global linear particle in cell code for studying electrostatic plasma instabilities <ref>G. Jost, T. M. Tran, K. Appert, W. A. Cooper, and L. Villard, [http://www.ispp.it/Courses_and_Workshops.html in Theory of Fusion Plasmas, International Workshop, Varenna, September 1998 (Editrice Compositori, Società Italiana di Fisica, Bologna, 1999), p. 419.]</ref>. It allows three-dimensional turbulence simulations using a plasma equilibrium calculated with the [[VMEC]] code as a starting point. EUTERPE was further developed at the Max Planck IPP and several linear calculations of ion temperature gradient (ITG) driven turbulence in [[Tokamak|tokamak]] and [[Stellarator|stellarator]] geometry have been carried out using it  
<ref>[http://pop.aip.org/phpaen/v8/i7/p3321_s1 G. Jost, T. M. Tran, W. Cooper, and K. Appert. Phys. Plasmas '''8''': 3321 (2001)]</ref>
<ref>G. Jost, T. M. Tran, W. Cooper, and K. Appert. [[doi:10.1063/1.1374585|Phys. Plasmas '''8''': 3321 (2001)]]</ref>
<ref>[http://pop.aip.org/phpaen/v11/i6/p3196_s1 V. Kornilov, R. Kleiber, R. Hatzky, L. Villard, and G. Jost. Phys. Plasmas '''11''': 3196 (2004)]</ref>
<ref>V. Kornilov, R. Kleiber, R. Hatzky, L. Villard, and G. Jost. [[doi:10.1063/1.1737393|Phys. Plasmas '''11''': 3196 (2004)]]</ref>
<ref>[http://iopscience.iop.org/0029-5515/45/4/003 V. Kornilov, R. Kleiber, and R. Hatzky, Nucl. Fusion '''45''': 238 (2005)]</ref>
<ref>V. Kornilov, R. Kleiber, and R. Hatzky, [[doi:10.1088/0029-5515/45/4/003|Nucl. Fusion '''45''': 238 (2005)]]</ref>
<ref>[http://link.aip.org/link/?APCPCS/871/136/1 R. Kleiber, ''Global linear gyrokinetic simulations for stellarator and axisymmetric equilibria'', Joint Varenna-Lausanne International Workshop. AIP Conference Proceedings, 871, p. 136, 2006]</ref>.  
<ref>R. Kleiber, ''Global linear gyrokinetic simulations for stellarator and axisymmetric equilibria'', Joint Varenna-Lausanne International Workshop. [[doi:10.1063/1.2404546|AIP Conference Proceedings, 871, p. 136, 2006]]</ref>.  
Afterwards, the code has been  heavily optimized and improved. The perturbation to the magnetic field, a third species (in adition to electrons and ions) and the non-linear dynamics have been included.  
Afterwards, the code has been  heavily optimized and improved. The perturbation to the magnetic field, a third species (in adition to electrons and ions) and the non-linear dynamics have been included.  


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An equilibrium state calculated with the code VMEC is used as a starting point. The equilibrium quantities computed by VMEC are mapped onto the spatial grid using an intermediate program.  
An equilibrium state calculated with the code VMEC is used as a starting point. The equilibrium quantities computed by VMEC are mapped onto the spatial grid using an intermediate program.  


EUTERPE features several techniques for the noise control: the filtering of Fourier modes (square and diagonal filters can be used) and the optimized loading <ref>[http://pop.aip.org/phpaen/v9/i3/p898_s1 Hatzky, R Tran, TM Konies, A Kleiber, R Allfrey, SJ .Energy conservation in a nonlinear gyrokinetic particle-in-cell code for ion-temperature-gradient-driven modes in theta-pinch geometry. PHYSICS OF PLASMAS, 9- 3,p. 912,2002.]</ref>.  
EUTERPE features several techniques for the noise control: the filtering of Fourier modes (square and diagonal filters can be used) and the optimized loading <ref>Hatzky, R Tran, TM Konies, A Kleiber, R Allfrey, SJ .Energy conservation in a nonlinear gyrokinetic particle-in-cell code for ion-temperature-gradient-driven modes in theta-pinch geometry. [[doi:10.1063/1.1449889|Phys. Plasmas, 9- 3, p. 898, 2002.]]</ref>.  


==References==
==References==