Gyrokinetic simulations: Difference between revisions
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The gyrokinetic formalism <ref>[http://pof.aip.org/pfldas/v31/i9/p2670_s1?isAuthorized=no T. S. Hahm. Nonlinear gyrokinetic equations for tokamak microturbulence. Physics of Fluids 31, 2670, 1988.]</ref><ref>[http://rmp.aps.org/abstract/RMP/v79/i2/p421_1 A. J. Brizard and T. S. Hahm. Foundations of nonlinear gyrokinetic theory. Reviews of Modern Physics 2, 421, 2007.]</ref> is based on first principles and provides a valuable tool for investigating low frequency turbulence in fusion plasmas. | The gyrokinetic formalism <ref>[http://pof.aip.org/pfldas/v31/i9/p2670_s1?isAuthorized=no T. S. Hahm. Nonlinear gyrokinetic equations for tokamak microturbulence. Physics of Fluids 31, 2670, 1988.]</ref><ref>[http://rmp.aps.org/abstract/RMP/v79/i2/p421_1 A. J. Brizard and T. S. Hahm. Foundations of nonlinear gyrokinetic theory. Reviews of Modern Physics 2, 421, 2007.]</ref> is based on first principles and provides a valuable tool for investigating low frequency turbulence in fusion plasmas. | ||
The Theory group in the Laboratorio Nacional de Fusión collaborates with the Barcelona Supercomputing Center and the Max Planck IPP at Greifswald for the development and exploitation of the EUTERPE<ref>[EUTERPE EUTERPE]</ref> global gyrokinetic code. | |||
==References== | ==References== | ||
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Revision as of 17:20, 29 April 2010
The gyrokinetic formalism [1][2] is based on first principles and provides a valuable tool for investigating low frequency turbulence in fusion plasmas. The Theory group in the Laboratorio Nacional de Fusión collaborates with the Barcelona Supercomputing Center and the Max Planck IPP at Greifswald for the development and exploitation of the EUTERPE[3] global gyrokinetic code.