000837457 001__ 837457
000837457 005__ 20240711113724.0
000837457 0247_ $$2doi$$a10.1016/j.nme.2017.01.010
000837457 0247_ $$2Handle$$a2128/15717
000837457 0247_ $$2WOS$$aWOS:000417293300026
000837457 037__ $$aFZJ-2017-06370
000837457 082__ $$a333.7
000837457 1001_ $$0P:(DE-Juel1)166412$$aReimold, F.$$b0$$eCorresponding author$$ufzj
000837457 245__ $$aThe high field side high density region in SOLPS-modeling of nitrogen-seeded H-modes in ASDEX Upgrade
000837457 260__ $$aAmsterdam [u.a.]$$bElsevier$$c2017
000837457 3367_ $$2DRIVER$$aarticle
000837457 3367_ $$2DataCite$$aOutput Types/Journal article
000837457 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1509093095_17888
000837457 3367_ $$2BibTeX$$aARTICLE
000837457 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000837457 3367_ $$00$$2EndNote$$aJournal Article
000837457 520__ $$aThe understanding of divertor physics and the evolution of divertor detachment is crucial for developing the capability to model power exhaust in current experiments and reliably predict it for future fusion devices. In simulations of ASDEX Upgrade, an experimentally observed region of high density in the high field side scrape-off layer has been recovered. Validated modeling with SOLPS5.0 shows that a detailed match of the high field side scrape-off layer plasma is not only important for local plasma parameters, but can lead to strong changes in global parameters. Drifts play a crucial role in lower-single null discharges with forward toroidal field (-drift pointing down). Their inclusion changes the spatial extent as well as the radial and poloidal gradients of the high field side high density. Adapted transport coefficients that take into account core fueling by plasma diffusion due to the presence of the high field side density and drift-driven radial fluxes now reconcile the modeled deuterium compression ratio, divertor neutral density, neutral radiation levels and deuterium fueling rates with experimental measurements. The onset of strong volume recombination in the simulations now allows to remove the previously necessary increase of perpendicular transport in the inner divertor from the simulations.
000837457 536__ $$0G:(DE-HGF)POF3-174$$a174 - Plasma-Wall-Interaction (POF3-174)$$cPOF3-174$$fPOF III$$x0
000837457 588__ $$aDataset connected to CrossRef
000837457 7001_ $$0P:(DE-HGF)0$$aWischmeier, M.$$b1
000837457 7001_ $$0P:(DE-HGF)0$$aPotzel, S.$$b2
000837457 7001_ $$0P:(DE-HGF)0$$aGuimarais, L.$$b3
000837457 7001_ $$0P:(DE-Juel1)5006$$aReiter, D.$$b4$$ufzj
000837457 7001_ $$0P:(DE-HGF)0$$aBernert, M.$$b5
000837457 7001_ $$0P:(DE-HGF)0$$aDunne, M.$$b6
000837457 7001_ $$0P:(DE-HGF)0$$aLunt, T.$$b7
000837457 773__ $$0PERI:(DE-600)2808888-8$$a10.1016/j.nme.2017.01.010$$gp. S235217911630059X$$p193-199$$tNuclear materials and energy$$v12$$x2352-1791$$y2017
000837457 8564_ $$uhttps://juser.fz-juelich.de/record/837457/files/1-s2.0-S235217911630059X-main.pdf$$yOpenAccess
000837457 8564_ $$uhttps://juser.fz-juelich.de/record/837457/files/1-s2.0-S235217911630059X-main.gif?subformat=icon$$xicon$$yOpenAccess
000837457 8564_ $$uhttps://juser.fz-juelich.de/record/837457/files/1-s2.0-S235217911630059X-main.jpg?subformat=icon-1440$$xicon-1440$$yOpenAccess
000837457 8564_ $$uhttps://juser.fz-juelich.de/record/837457/files/1-s2.0-S235217911630059X-main.jpg?subformat=icon-180$$xicon-180$$yOpenAccess
000837457 8564_ $$uhttps://juser.fz-juelich.de/record/837457/files/1-s2.0-S235217911630059X-main.jpg?subformat=icon-640$$xicon-640$$yOpenAccess
000837457 8564_ $$uhttps://juser.fz-juelich.de/record/837457/files/1-s2.0-S235217911630059X-main.pdf?subformat=pdfa$$xpdfa$$yOpenAccess
000837457 909CO $$ooai:juser.fz-juelich.de:837457$$pdnbdelivery$$pVDB$$pdriver$$popen_access$$popenaire
000837457 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)166412$$aForschungszentrum Jülich$$b0$$kFZJ
000837457 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)5006$$aForschungszentrum Jülich$$b4$$kFZJ
000837457 9131_ $$0G:(DE-HGF)POF3-174$$1G:(DE-HGF)POF3-170$$2G:(DE-HGF)POF3-100$$3G:(DE-HGF)POF3$$4G:(DE-HGF)POF$$aDE-HGF$$bEnergie$$lKernfusion$$vPlasma-Wall-Interaction$$x0
000837457 9141_ $$y2017
000837457 915__ $$0StatID:(DE-HGF)0200$$2StatID$$aDBCoverage$$bSCOPUS
000837457 915__ $$0LIC:(DE-HGF)CCBYNCND4$$2HGFVOC$$aCreative Commons Attribution-NonCommercial-NoDerivs CC BY-NC-ND 4.0
000837457 915__ $$0StatID:(DE-HGF)0501$$2StatID$$aDBCoverage$$bDOAJ Seal
000837457 915__ $$0StatID:(DE-HGF)0112$$2StatID$$aWoS$$bEmerging Sources Citation Index
000837457 915__ $$0StatID:(DE-HGF)0150$$2StatID$$aDBCoverage$$bWeb of Science Core Collection
000837457 915__ $$0StatID:(DE-HGF)0500$$2StatID$$aDBCoverage$$bDOAJ
000837457 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
000837457 915__ $$0StatID:(DE-HGF)0199$$2StatID$$aDBCoverage$$bThomson Reuters Master Journal List
000837457 9201_ $$0I:(DE-Juel1)IEK-4-20101013$$kIEK-4$$lPlasmaphysik$$x0
000837457 9801_ $$aFullTexts
000837457 980__ $$ajournal
000837457 980__ $$aVDB
000837457 980__ $$aUNRESTRICTED
000837457 980__ $$aI:(DE-Juel1)IEK-4-20101013
000837457 981__ $$aI:(DE-Juel1)IFN-1-20101013