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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] | 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]]</ref> global gyrokinetic code. | ||
==References== | ==References== | ||
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