000906935 001__ 906935
000906935 005__ 20240711113953.0
000906935 0247_ $$2doi$$a10.1002/ctpp.202100172
000906935 0247_ $$2ISSN$$a0005-8025
000906935 0247_ $$2ISSN$$a0863-1042
000906935 0247_ $$2ISSN$$a1521-3986
000906935 0247_ $$2Handle$$a2128/33999
000906935 0247_ $$2WOS$$aWOS:000768307900001
000906935 037__ $$aFZJ-2022-01760
000906935 082__ $$a570
000906935 1001_ $$0P:(DE-Juel1)181062$$aRode, Sebastian$$b0$$eCorresponding author$$ufzj
000906935 245__ $$aImplementation and validation of guiding centre approximation into ERO2 .0
000906935 260__ $$aWeinheim$$bWiley-VCH$$c2022
000906935 3367_ $$2DRIVER$$aarticle
000906935 3367_ $$2DataCite$$aOutput Types/Journal article
000906935 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1679044303_15787
000906935 3367_ $$2BibTeX$$aARTICLE
000906935 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000906935 3367_ $$00$$2EndNote$$aJournal Article
000906935 520__ $$aThe Monte-Carlo code ERO2.0 uses full orbit resolution to follow impurity particles throughout the plasma volume to determine the local erosion and deposition fluxes on the plasma-facing components of fusion devices in magnetic confinement fusion. To have direct comparisons to other transport codes (e.g., ASCOT and DIVIMP) and to accelerate the code, guiding centre approximation (GCA) was implemented into ERO2.0. In addition, a hybrid simulation mode for ERO2.0 was developed, in which the advantages of both full orbit resolution and guiding centre approximation are used. In typical scenarios in this simulation mode, full orbit resolution is applied exclusively near the wall region, while GCA is used everywhere else along a particle's trajectory. Special emphasis was put on the validation of the implementation by an inner-code benchmarking to pure full orbit simulations. Analysed scenarios included test plasmas with simplified geometry and a realistic test case corresponding to a deuterium limiter plasma used in JET pulse #80319. The results of simulations performed in the hybrid simulation mode are in very good agreement to corresponding pure full orbit simulations, while a significant code speed-up was achieved.
000906935 536__ $$0G:(DE-HGF)POF4-134$$a134 - Plasma-Wand-Wechselwirkung (POF4-134)$$cPOF4-134$$fPOF IV$$x0
000906935 588__ $$aDataset connected to CrossRef, Journals: juser.fz-juelich.de
000906935 7001_ $$0P:(DE-Juel1)165905$$aRomazanov, Juri$$b1$$ufzj
000906935 7001_ $$aReiser, Dirk$$b2
000906935 7001_ $$0P:(DE-Juel1)129976$$aBrezinsek, Sebastijan$$b3$$ufzj
000906935 7001_ $$0P:(DE-Juel1)157640$$aLinsmeier, Christian$$b4$$ufzj
000906935 7001_ $$0P:(DE-HGF)0$$aPukhov, Alexander$$b5
000906935 773__ $$0PERI:(DE-600)2018082-2$$a10.1002/ctpp.202100172$$n5-6$$pe202100172$$tContributions to plasma physics$$v62$$x0005-8025$$y2022
000906935 8564_ $$uhttps://juser.fz-juelich.de/record/906935/files/Contributions%20to%20Plasma%20Physics%20-%202022%20-%20Rode%20-%20Implementation%20and%20validation%20of%20guiding%20centre%20approximation%20into%20ERO2%200.pdf$$yOpenAccess
000906935 8767_ $$d2022-02-15$$eHybrid-OA$$jDEAL
000906935 909CO $$ooai:juser.fz-juelich.de:906935$$pdnbdelivery$$popenCost$$pVDB$$pdriver$$pOpenAPC_DEAL$$popen_access$$popenaire
000906935 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)181062$$aForschungszentrum Jülich$$b0$$kFZJ
000906935 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)165905$$aForschungszentrum Jülich$$b1$$kFZJ
000906935 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)129976$$aForschungszentrum Jülich$$b3$$kFZJ
000906935 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)157640$$aForschungszentrum Jülich$$b4$$kFZJ
000906935 9131_ $$0G:(DE-HGF)POF4-134$$1G:(DE-HGF)POF4-130$$2G:(DE-HGF)POF4-100$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Energie$$lFusion$$vPlasma-Wand-Wechselwirkung$$x0
000906935 9141_ $$y2022
000906935 915pc $$0PC:(DE-HGF)0000$$2APC$$aAPC keys set
000906935 915pc $$0PC:(DE-HGF)0120$$2APC$$aDEAL: Wiley 2019
000906935 915__ $$0StatID:(DE-HGF)0200$$2StatID$$aDBCoverage$$bSCOPUS$$d2021-01-30
000906935 915__ $$0LIC:(DE-HGF)CCBY4$$2HGFVOC$$aCreative Commons Attribution CC BY 4.0
000906935 915__ $$0StatID:(DE-HGF)0600$$2StatID$$aDBCoverage$$bEbsco Academic Search$$d2021-01-30
000906935 915__ $$0StatID:(DE-HGF)1150$$2StatID$$aDBCoverage$$bCurrent Contents - Physical, Chemical and Earth Sciences$$d2021-01-30
000906935 915__ $$0StatID:(DE-HGF)3001$$2StatID$$aDEAL Wiley$$d2021-01-30$$wger
000906935 915__ $$0StatID:(DE-HGF)0113$$2StatID$$aWoS$$bScience Citation Index Expanded$$d2021-01-30
000906935 915__ $$0StatID:(DE-HGF)0150$$2StatID$$aDBCoverage$$bWeb of Science Core Collection$$d2021-01-30
000906935 915__ $$0StatID:(DE-HGF)9900$$2StatID$$aIF < 5$$d2021-01-30
000906935 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
000906935 915__ $$0StatID:(DE-HGF)0030$$2StatID$$aPeer Review$$bASC$$d2021-01-30
000906935 915__ $$0StatID:(DE-HGF)0100$$2StatID$$aJCR$$bCONTRIB PLASM PHYS : 2019$$d2021-01-30
000906935 915__ $$0StatID:(DE-HGF)0160$$2StatID$$aDBCoverage$$bEssential Science Indicators$$d2021-01-30
000906935 915__ $$0StatID:(DE-HGF)0420$$2StatID$$aNationallizenz$$d2021-01-30$$wger
000906935 915__ $$0StatID:(DE-HGF)0199$$2StatID$$aDBCoverage$$bClarivate Analytics Master Journal List$$d2021-01-30
000906935 9201_ $$0I:(DE-Juel1)IEK-4-20101013$$kIEK-4$$lPlasmaphysik$$x0
000906935 9801_ $$aAPC
000906935 9801_ $$aFullTexts
000906935 980__ $$ajournal
000906935 980__ $$aVDB
000906935 980__ $$aI:(DE-Juel1)IEK-4-20101013
000906935 980__ $$aAPC
000906935 980__ $$aUNRESTRICTED
000906935 981__ $$aI:(DE-Juel1)IFN-1-20101013