<TEI xmlns="http://www.tei-c.org/ns/1.0"><teiHeader><fileDesc><titleStmt><title>Episciences.org TEI export of ops:15867 - Open Plasma Science, 2026-01-14, Volume 1</title></titleStmt><publicationStmt><distributor>CCSD - Episciences</distributor><availability status="restricted"><licence target="https://creativecommons.org/licenses/by/4.0">Attribution 4.0 International (CC BY 4.0)</licence></availability><date when="2026-01-14"/></publicationStmt><sourceDesc><p>Episciences.org API platform</p></sourceDesc></fileDesc></teiHeader><text><body><listBibl><biblFull><titleStmt><title xml:lang="en">An adaptive quasi-neutrality solver for full-F flux-driven gyrokinetic simulations of tokamak plasmas in presence of poloidal asymmetries</title><author role="aut"><persName><forename type="first">Peter</forename><surname>Donnel</surname></persName><email/><idno type="ORCID">0000-0002-6669-416X</idno><affiliation ref="#struct-1"/></author><author role="aut"><persName><forename type="first">Kevin</forename><surname>Obrejan</surname></persName><email/><affiliation ref="#struct-1"/></author><author role="aut"><persName><forename type="first">Yanick</forename><surname>Sarazin</surname></persName><email/><idno type="ORCID">0000-0003-2479-563X</idno><affiliation ref="#struct-1"/></author><author role="aut"><persName><forename type="first">Roméo</forename><surname>Bigué</surname></persName><email/><affiliation ref="#struct-1"/><affiliation ref="#struct-2"/></author><author role="aut"><persName><forename type="first">Emily</forename><surname>Bourne</surname></persName><email/><idno type="ORCID">0000-0002-3469-2338</idno><affiliation ref="#struct-0"/></author><author role="aut"><persName><forename type="first">Guillaume</forename><surname>Brochard</surname></persName><email/><idno type="ORCID">0000-0002-3208-3651</idno><affiliation ref="#struct-1"/></author><author role="aut"><persName><forename type="first">Ludovica</forename><surname>de Gianni</surname></persName><email/><affiliation ref="#struct-1"/></author><author role="aut"><persName><forename type="first">Guilhem</forename><surname>Dif-Pradalier</surname></persName><email/><idno type="ORCID">0000-0003-4869-7049</idno><affiliation ref="#struct-1"/></author><author role="aut"><persName><forename type="first">Xavier</forename><surname>Garbet</surname></persName><email/><idno type="ORCID">0000-0001-5730-1259</idno><affiliation ref="#struct-1"/><affiliation ref="#struct-3"/></author><author role="aut"><persName><forename type="first">Virginie</forename><surname>Grandgirard</surname></persName><email/><idno type="ORCID">0000-0001-7821-9107</idno><affiliation ref="#struct-1"/></author><author role="aut"><persName><forename type="first">Philipp</forename><surname>Krah</surname></persName><email/><affiliation ref="#struct-1"/></author><author role="aut"><persName><forename type="first">Yann</forename><surname>Munschy</surname></persName><email/><affiliation ref="#struct-1"/></author><author role="aut"><persName><forename type="first">Protais</forename><surname>Matthieu</surname></persName><email/><idno type="ORCID">0009-0003-5852-7446</idno><affiliation ref="#struct-1"/></author></titleStmt><editionStmt><edition><date type="whenSubmitted">2025-06-13 16:21:03</date><date type="whenProduced">2026-01-14 21:10:11</date><ref type="file" target="http://ops.episciences.org/15867/pdf"/></edition><respStmt><resp>contributor</resp><name key="587150"><persName><forename>Peter</forename><surname>Donnel</surname></persName><email>peter.donnel@cea.fr</email></name></respStmt></editionStmt><publicationStmt><distributor>CCSD</distributor><idno type="id">ops:15867</idno><idno type="url">http://ops.episciences.org/15867</idno><idno type="ref">ops:15867 - Open Plasma Science, 2026-01-14, Volume 1</idno><licence target="https://creativecommons.org/licenses/by/4.0">Attribution 4.0 International (CC BY 4.0)</licence></publicationStmt><sourceDesc><biblStruct><analytic><title xml:lang="en">An adaptive quasi-neutrality solver for full-F flux-driven gyrokinetic simulations of tokamak plasmas in presence of poloidal asymmetries</title><author role="aut"><persName><forename type="first">Peter</forename><surname>Donnel</surname></persName><email/><idno type="ORCID">0000-0002-6669-416X</idno><affiliation ref="#struct-1"/></author><author role="aut"><persName><forename type="first">Kevin</forename><surname>Obrejan</surname></persName><email/><affiliation ref="#struct-1"/></author><author role="aut"><persName><forename type="first">Yanick</forename><surname>Sarazin</surname></persName><email/><idno type="ORCID">0000-0003-2479-563X</idno><affiliation ref="#struct-1"/></author><author role="aut"><persName><forename type="first">Roméo</forename><surname>Bigué</surname></persName><email/><affiliation ref="#struct-1"/><affiliation ref="#struct-2"/></author><author role="aut"><persName><forename type="first">Emily</forename><surname>Bourne</surname></persName><email/><idno type="ORCID">0000-0002-3469-2338</idno><affiliation ref="#struct-0"/></author><author role="aut"><persName><forename type="first">Guillaume</forename><surname>Brochard</surname></persName><email/><idno type="ORCID">0000-0002-3208-3651</idno><affiliation ref="#struct-1"/></author><author role="aut"><persName><forename type="first">Ludovica</forename><surname>de Gianni</surname></persName><email/><affiliation ref="#struct-1"/></author><author role="aut"><persName><forename type="first">Guilhem</forename><surname>Dif-Pradalier</surname></persName><email/><idno type="ORCID">0000-0003-4869-7049</idno><affiliation ref="#struct-1"/></author><author role="aut"><persName><forename type="first">Xavier</forename><surname>Garbet</surname></persName><email/><idno type="ORCID">0000-0001-5730-1259</idno><affiliation ref="#struct-1"/><affiliation ref="#struct-3"/></author><author role="aut"><persName><forename type="first">Virginie</forename><surname>Grandgirard</surname></persName><email/><idno type="ORCID">0000-0001-7821-9107</idno><affiliation ref="#struct-1"/></author><author role="aut"><persName><forename type="first">Philipp</forename><surname>Krah</surname></persName><email/><affiliation ref="#struct-1"/></author><author role="aut"><persName><forename type="first">Yann</forename><surname>Munschy</surname></persName><email/><affiliation ref="#struct-1"/></author><author role="aut"><persName><forename type="first">Protais</forename><surname>Matthieu</surname></persName><email/><idno type="ORCID">0009-0003-5852-7446</idno><affiliation ref="#struct-1"/></author></analytic><monogr><idno type="HAL">hal-05111064</idno><idno type="issn">3076-1468</idno><title level="j">Open Plasma Science</title><imprint><publisher>Université de Lorraine</publisher><pubPlace>Nancy, France</pubPlace><biblScope unit="volume">Volume 1</biblScope><date type="datePub">2026-01-14T21:10:11+01:00</date></imprint></monogr><idno type="doi">10.46298/ops.15867</idno></biblStruct></sourceDesc><profileDesc><langUsage><language ident="en">English</language></langUsage><textClass><keywords scheme="author"><term>Tokamak</term><term>Gyrokinetic</term><term>Quasi-neutrality</term><term>[PHYS.PHYS.PHYS-PLASM-PH]Physics [physics]/Physics [physics]/Plasma Physics [physics.plasm-ph]</term><term>[PHYS.PHYS.PHYS-COMP-PH]Physics [physics]/Physics [physics]/Computational Physics [physics.comp-ph]</term></keywords></textClass><abstract><p>International audience</p></abstract><abstract xml:lang="en"><p>Gyrokinetic codes are used to simulate transport in tokamak plasmas. In these codes, the distribution functions evolve self consistently with an electromagnetic field. To compute the temporal evolution of the electrostatic potential, a quasi-neutrality equation is solved. In some gyrokinetic codes, the quasi-neutrality solver assumes that the background densities and temperatures are constant in time and on flux surfaces. This assumption, which implicitly uses the so-called δF approach, can break up, in particular at the edge of the plasma which can display large and time evolving poloidal asymmetries.In this paper, a numerical solver of the quasi-neutrality equation accounting for time evolving poloidal asymmetries is presented. This solver is compatible with all electron models (adiabatic, kinetic or hybrid) and written for the long wavelength or the Padé approximations for the polarisation term. The impact of such an improvement is carefully reported on different types of simulations, illustrating when the δF approach forquasi-neutrality is valid and when it fails. A procedure to limit the numerical cost of updating the background profiles in the quasi-neutrality solver is also presented.</p></abstract></profileDesc></biblFull></listBibl></body><back><listOrg><org xml:id="struct-0"><idno type="ROR">https://ror.org/02s376052</idno><orgName>Ecole Polytechnique Fédérale de Lausanne</orgName><orgName acronym="EPFL"/></org><org xml:id="struct-1"><idno type="ROR">https://ror.org/03hffat62</idno><orgName>Institut de Recherche sur la Fusion par confinement Magnétique</orgName><orgName acronym="IRFM"/></org><org xml:id="struct-2"><orgName>Physique des interactions ioniques et moléculaires</orgName></org><org xml:id="struct-3"><idno type="ROR">https://ror.org/02e7b5302</idno><orgName>Nanyang Technological University [Singapour]</orgName><orgName acronym="NTU"/></org></listOrg></back></text></TEI>