000864167 001__ 864167
000864167 005__ 20240711113848.0
000864167 0247_ $$2doi$$a10.1016/j.nme.2018.05.002
000864167 0247_ $$2Handle$$a2128/22554
000864167 0247_ $$2WOS$$aWOS:000435611400037
000864167 037__ $$aFZJ-2019-04033
000864167 082__ $$a624
000864167 1001_ $$0P:(DE-Juel1)166256$$aSchmitz, J.$$b0$$eCorresponding author
000864167 245__ $$aWCrY smart alloys as advanced plasma-facing materials – Exposure to steady-state pure deuterium plasmas in PSI-2
000864167 260__ $$aAmsterdam [u.a.]$$bElsevier$$c2018
000864167 3367_ $$2DRIVER$$aarticle
000864167 3367_ $$2DataCite$$aOutput Types/Journal article
000864167 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1564646766_5550
000864167 3367_ $$2BibTeX$$aARTICLE
000864167 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000864167 3367_ $$00$$2EndNote$$aJournal Article
000864167 520__ $$aIn this paper the impact of steady state pure D plasma on WCrY smart alloys at ion energies of 120 and 220 eV is reported. For this purpose a comparison with simultaneously exposed pure W samples is drawn. Different analysis techniques employed for pre- and post-plasma sample analysis hint at a significant depletion of Cr and enrichment of W for lower ion energies. Preferential sputtering leads to enhanced volumetric loss at 220 eV. Analysis of redeposited material indicated local redeposition of Cr. Modelling the ion irradiation with SDTrimSP is used to further interpret experimental results. Depending on the sample temperature during plasma exposure and the magnitude of the ion flux, diffusion of Cr towards the surface is a determining factor for erosion of smart alloys for higher ion energies.
000864167 536__ $$0G:(DE-HGF)POF3-174$$a174 - Plasma-Wall-Interaction (POF3-174)$$cPOF3-174$$fPOF III$$x0
000864167 588__ $$aDataset connected to CrossRef
000864167 7001_ $$0P:(DE-Juel1)130090$$aLitnovsky, A.$$b1$$ufzj
000864167 7001_ $$0P:(DE-Juel1)166427$$aKlein, F.$$b2$$ufzj
000864167 7001_ $$0P:(DE-Juel1)161367$$aWegener, T.$$b3
000864167 7001_ $$0P:(DE-Juel1)171237$$aTan, X. Y.$$b4
000864167 7001_ $$0P:(DE-Juel1)162160$$aRasinski, M.$$b5$$ufzj
000864167 7001_ $$0P:(DE-HGF)0$$aMutzke, A.$$b6
000864167 7001_ $$0P:(DE-Juel1)164146$$aHansen, P.$$b7
000864167 7001_ $$0P:(DE-Juel1)130070$$aKreter, A.$$b8$$ufzj
000864167 7001_ $$0P:(DE-Juel1)130122$$aPospieszczyk, A.$$b9$$ufzj
000864167 7001_ $$0P:(DE-Juel1)139534$$aMöller, S.$$b10
000864167 7001_ $$0P:(DE-Juel1)2594$$aCoenen, J. W.$$b11
000864167 7001_ $$0P:(DE-Juel1)157640$$aLinsmeier, Ch.$$b12
000864167 7001_ $$0P:(DE-Juel1)138352$$aBreuer, U.$$b13$$ufzj
000864167 7001_ $$0P:(DE-Juel1)162271$$aGonzalez-Julian, J.$$b14
000864167 7001_ $$0P:(DE-Juel1)129591$$aBram, M.$$b15$$ufzj
000864167 773__ $$0PERI:(DE-600)2808888-8$$a10.1016/j.nme.2018.05.002$$gVol. 15, p. 220 - 225$$p220 - 225$$tNuclear materials and energy$$v15$$x2352-1791$$y2018
000864167 8564_ $$uhttps://juser.fz-juelich.de/record/864167/files/1-s2.0-S2352179117301023-main.pdf$$yOpenAccess
000864167 8564_ $$uhttps://juser.fz-juelich.de/record/864167/files/1-s2.0-S2352179117301023-main.pdf?subformat=pdfa$$xpdfa$$yOpenAccess
000864167 909CO $$ooai:juser.fz-juelich.de:864167$$pdnbdelivery$$pdriver$$pVDB$$popen_access$$popenaire
000864167 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)166256$$aForschungszentrum Jülich$$b0$$kFZJ
000864167 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)130090$$aForschungszentrum Jülich$$b1$$kFZJ
000864167 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)166427$$aForschungszentrum Jülich$$b2$$kFZJ
000864167 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)162160$$aForschungszentrum Jülich$$b5$$kFZJ
000864167 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)164146$$aForschungszentrum Jülich$$b7$$kFZJ
000864167 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)130070$$aForschungszentrum Jülich$$b8$$kFZJ
000864167 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)130122$$aForschungszentrum Jülich$$b9$$kFZJ
000864167 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)139534$$aForschungszentrum Jülich$$b10$$kFZJ
000864167 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)2594$$aForschungszentrum Jülich$$b11$$kFZJ
000864167 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)157640$$aForschungszentrum Jülich$$b12$$kFZJ
000864167 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)138352$$aForschungszentrum Jülich$$b13$$kFZJ
000864167 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)162271$$aForschungszentrum Jülich$$b14$$kFZJ
000864167 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)129591$$aForschungszentrum Jülich$$b15$$kFZJ
000864167 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
000864167 9141_ $$y2019
000864167 915__ $$0StatID:(DE-HGF)0200$$2StatID$$aDBCoverage$$bSCOPUS
000864167 915__ $$0LIC:(DE-HGF)CCBY4$$2HGFVOC$$aCreative Commons Attribution CC BY 4.0
000864167 915__ $$0StatID:(DE-HGF)0501$$2StatID$$aDBCoverage$$bDOAJ Seal
000864167 915__ $$0StatID:(DE-HGF)0112$$2StatID$$aWoS$$bEmerging Sources Citation Index
000864167 915__ $$0StatID:(DE-HGF)0500$$2StatID$$aDBCoverage$$bDOAJ
000864167 915__ $$0StatID:(DE-HGF)0150$$2StatID$$aDBCoverage$$bWeb of Science Core Collection
000864167 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
000864167 915__ $$0StatID:(DE-HGF)0030$$2StatID$$aPeer Review$$bDOAJ : Peer review
000864167 915__ $$0StatID:(DE-HGF)0199$$2StatID$$aDBCoverage$$bClarivate Analytics Master Journal List
000864167 9201_ $$0I:(DE-Juel1)IEK-4-20101013$$kIEK-4$$lPlasmaphysik$$x0
000864167 9201_ $$0I:(DE-Juel1)IEK-1-20101013$$kIEK-1$$lWerkstoffsynthese und Herstellungsverfahren$$x1
000864167 9201_ $$0I:(DE-Juel1)S-OO-20090406$$kS-OO$$lSicherheit und Strahlenschutz;Objektsicherung,Objektsicherungsdienst$$x2
000864167 9801_ $$aFullTexts
000864167 980__ $$ajournal
000864167 980__ $$aVDB
000864167 980__ $$aUNRESTRICTED
000864167 980__ $$aI:(DE-Juel1)IEK-4-20101013
000864167 980__ $$aI:(DE-Juel1)IEK-1-20101013
000864167 980__ $$aI:(DE-Juel1)S-OO-20090406
000864167 981__ $$aI:(DE-Juel1)IFN-1-20101013
000864167 981__ $$aI:(DE-Juel1)IMD-2-20101013