EUTERPE: Difference between revisions
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<ref>[http://iopscience.iop.org/0029-5515/45/4/003 V. Kornilov, R. Kleiber, and R. Hatzky, Nucl. Fusion '''45''': 238 (2005)]</ref><ref>[http://scitation.aip.org/getabs/servlet/GetabsServlet?prog=normal&id=APCPCS000871000001000136000001 R. Kleiber. Global linear gyrokinetic simulations for stellarator and | <ref>[http://iopscience.iop.org/0029-5515/45/4/003 V. Kornilov, R. Kleiber, and R. Hatzky, Nucl. Fusion '''45''': 238 (2005)]</ref><ref>[http://scitation.aip.org/getabs/servlet/GetabsServlet?prog=normal&id=APCPCS000871000001000136000001 R. Kleiber. Global linear gyrokinetic simulations for stellarator and | ||
axisymmetric equilibria. Joint Varenna-Lausanne International Workshop. | axisymmetric equilibria. Joint Varenna-Lausanne International Workshop. | ||
AIP Conference Proceedings, 871, p. 136, 2006]</ref>. Afterwards, the code has been heavily optimized and improved and non-linear dynamics have been included. | 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. | ||
The EUTERPE code solves the gyroaveraged Vlasov equation for the distribution function of ions | The EUTERPE code solves the gyroaveraged Vlasov equation for the distribution function of ions | ||