001     835981
005     20240711113518.0
024 7 _ |a 10.1088/1741-4326/aa69c4
|2 doi
024 7 _ |a 0029-5515
|2 ISSN
024 7 _ |a 1741-4326
|2 ISSN
024 7 _ |a WOS:000399878400002
|2 WOS
024 7 _ |a altmetric:19194889
|2 altmetric
037 _ _ |a FZJ-2017-05106
041 _ _ |a English
082 _ _ |a 530
100 1 _ |a Hakola, A.
|0 P:(DE-HGF)0
|b 0
|e Corresponding author
245 _ _ |a Plasma-wall interaction studies in the full-W ASDEX upgrade during helium plasma discharges
260 _ _ |a Vienna
|c 2017
|b IAEA
336 7 _ |a article
|2 DRIVER
336 7 _ |a Output Types/Journal article
|2 DataCite
336 7 _ |a Journal Article
|b journal
|m journal
|0 PUB:(DE-HGF)16
|s 1500988131_25564
|2 PUB:(DE-HGF)
336 7 _ |a ARTICLE
|2 BibTeX
336 7 _ |a JOURNAL_ARTICLE
|2 ORCID
336 7 _ |a Journal Article
|0 0
|2 EndNote
520 _ _ |a Plasma-wall interactions have been studied in the full-W ASDEX Upgrade during its dedicated helium campaign. Relatively clean plasmas with a He content of  >80% could be obtained by applying ion cyclotron wall conditioning (ICWC) discharges upon changeover from D to He. However, co-deposited layers with significant amounts of He and D were measured on W samples exposed to ICWC plasmas at the low-field side (outer) midplane. This is a sign of local migration and accumulation of materials and residual fuel in regions shadowed from direct plasma exposure albeit globally D was removed from the vessel. When exposing W samples to ELMy H-mode helium plasmas in the outer strike-point region, no net erosion was observed but the surfaces had been covered with co-deposited layers mainly consisting of W, B, C, and D and being the thickest on rough and modified surfaces. This is different from the typical erosion-deposition patterns in D plasmas, where usually sharp net-erosion peaks surrounded by prominent net-deposition maxima for W are observed close to the strike point. Moreover, no clear signs of W nanostructure growth or destruction could be seen. The growth of deposited layers may impact the operation of future fusion reactors and is attributed to strong sources in the main chamber that under suitable conditions may switch the balance from net erosion into net deposition, even close to the strike points. In addition, the absence of noticeable chemical erosion in helium plasmas may have affected the thickness of the deposited layers. Retention of He, for its part, remained small and uniform throughout the strike-point region although our results indicate that samples with smooth surfaces can contain an order of magnitude less He than their rough counterparts.
536 _ _ |a 174 - Plasma-Wall-Interaction (POF3-174)
|0 G:(DE-HGF)POF3-174
|c POF3-174
|f POF III
|x 0
588 _ _ |a Dataset connected to CrossRef
700 1 _ |a Brezinsek, S.
|0 P:(DE-Juel1)129976
|b 1
700 1 _ |a Douai, D.
|0 P:(DE-HGF)0
|b 2
700 1 _ |a Balden, M.
|0 P:(DE-HGF)0
|b 3
700 1 _ |a Bobkov, V.
|0 P:(DE-HGF)0
|b 4
700 1 _ |a Carralero, D.
|0 P:(DE-HGF)0
|b 5
700 1 _ |a Greuner, H.
|0 P:(DE-HGF)0
|b 6
700 1 _ |a Elgeti, S.
|0 P:(DE-HGF)0
|b 7
700 1 _ |a Kallenbach, A.
|0 P:(DE-HGF)0
|b 8
700 1 _ |a Krieger, K.
|0 P:(DE-HGF)0
|b 9
700 1 _ |a Meisl, G.
|0 P:(DE-HGF)0
|b 10
700 1 _ |a Oberkofler, M.
|0 P:(DE-HGF)0
|b 11
700 1 _ |a Rohde, V.
|0 P:(DE-HGF)0
|b 12
700 1 _ |a Schneider, P.
|0 P:(DE-HGF)0
|b 13
700 1 _ |a Schwarz-Selinger, T.
|0 P:(DE-HGF)0
|b 14
700 1 _ |a Lahtinen, A.
|0 P:(DE-HGF)0
|b 15
700 1 _ |a De Temmerman, G.
|0 P:(DE-HGF)0
|b 16
700 1 _ |a Caniello, R.
|0 P:(DE-HGF)0
|b 17
700 1 _ |a Ghezzi, F.
|0 P:(DE-HGF)0
|b 18
700 1 _ |a Garcia-Carrasco, A.
|0 P:(DE-HGF)0
|b 19
700 1 _ |a Petersson, P.
|0 P:(DE-HGF)0
|b 20
700 1 _ |a Bogdanovic Radovic, I.
|0 P:(DE-HGF)0
|b 21
700 1 _ |a Siketic, Z.
|0 P:(DE-HGF)0
|b 22
700 1 _ |a Wauters, T.
|0 P:(DE-HGF)0
|b 23
773 _ _ |a 10.1088/1741-4326/aa69c4
|g Vol. 57, no. 6, p. 066015 -
|0 PERI:(DE-600)2037980-8
|n 6
|p 066015
|t Nuclear fusion
|v 57
|y 2017
|x 1741-4326
856 4 _ |u https://juser.fz-juelich.de/record/835981/files/Hakola_2017_Nucl._Fusion_57_066015.pdf
|y Restricted
909 C O |o oai:juser.fz-juelich.de:835981
|p VDB
910 1 _ |a Forschungszentrum Jülich
|0 I:(DE-588b)5008462-8
|k FZJ
|b 1
|6 P:(DE-Juel1)129976
913 1 _ |a DE-HGF
|l Kernfusion
|1 G:(DE-HGF)POF3-170
|0 G:(DE-HGF)POF3-174
|2 G:(DE-HGF)POF3-100
|v Plasma-Wall-Interaction
|x 0
|4 G:(DE-HGF)POF
|3 G:(DE-HGF)POF3
|b Energie
914 1 _ |y 2017
915 _ _ |a Nationallizenz
|0 StatID:(DE-HGF)0420
|2 StatID
915 _ _ |a National-Konsortium
|0 StatID:(DE-HGF)0430
|2 StatID
915 _ _ |a JCR
|0 StatID:(DE-HGF)0100
|2 StatID
|b NUCL FUSION : 2015
915 _ _ |a DBCoverage
|0 StatID:(DE-HGF)0200
|2 StatID
|b SCOPUS
915 _ _ |a DBCoverage
|0 StatID:(DE-HGF)0600
|2 StatID
|b Ebsco Academic Search
915 _ _ |a Peer Review
|0 StatID:(DE-HGF)0030
|2 StatID
|b ASC
915 _ _ |a DBCoverage
|0 StatID:(DE-HGF)0199
|2 StatID
|b Thomson Reuters Master Journal List
915 _ _ |a WoS
|0 StatID:(DE-HGF)0110
|2 StatID
|b Science Citation Index
915 _ _ |a DBCoverage
|0 StatID:(DE-HGF)0150
|2 StatID
|b Web of Science Core Collection
915 _ _ |a WoS
|0 StatID:(DE-HGF)0111
|2 StatID
|b Science Citation Index Expanded
915 _ _ |a DBCoverage
|0 StatID:(DE-HGF)1150
|2 StatID
|b Current Contents - Physical, Chemical and Earth Sciences
915 _ _ |a IF < 5
|0 StatID:(DE-HGF)9900
|2 StatID
920 1 _ |0 I:(DE-Juel1)IEK-4-20101013
|k IEK-4
|l Plasmaphysik
|x 0
980 _ _ |a journal
980 _ _ |a VDB
980 _ _ |a I:(DE-Juel1)IEK-4-20101013
980 _ _ |a UNRESTRICTED
981 _ _ |a I:(DE-Juel1)IFN-1-20101013


LibraryCollectionCLSMajorCLSMinorLanguageAuthor
Marc 21