Please use this identifier to cite or link to this item: http://hdl.handle.net/2067/48945
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dc.contributor.authorLabit, B.it
dc.contributor.authorEich, T.it
dc.contributor.authorHarrer, G. F.it
dc.contributor.authorWolfrum, E.it
dc.contributor.authorBernert, M.it
dc.contributor.authorDunne, M. G.it
dc.contributor.authorFrassinetti, L.it
dc.contributor.authorHennequin, P.it
dc.contributor.authorMaurizio, R.it
dc.contributor.authorMerle, A.it
dc.contributor.authorMeyer, H.it
dc.contributor.authorSaarelma, S.it
dc.contributor.authorSheikh, U.it
dc.contributor.authorAdamek, J.it
dc.contributor.authorAgostini, M.it
dc.contributor.authorAguiam, D.it
dc.contributor.authorAkers, R.it
dc.contributor.authorAlbanese, R.it
dc.contributor.authorAlbert, C.it
dc.contributor.authorAlessi, E.it
dc.contributor.authorAmbrosino, R.it
dc.contributor.authorAndr be, Y.it
dc.contributor.authorAngioni, C.it
dc.contributor.authorApruzzese, G.it
dc.contributor.authorAradi, M.it
dc.contributor.authorArnichand, H.it
dc.contributor.authorAuriemma, F.it
dc.contributor.authorAvdeeva, G.it
dc.contributor.authorAyllon-Guerola, J. M.it
dc.contributor.authorBagnato, F.it
dc.contributor.authorBandaru, V. K.it
dc.contributor.authorBarnes, M.it
dc.contributor.authorBarrera-Orte, L.it
dc.contributor.authorBettini, P.it
dc.contributor.authorBilato, R.it
dc.contributor.authorBiletskyi, O.it
dc.contributor.authorBilkova, P.it
dc.contributor.authorBin, W.it
dc.contributor.authorBlanchard, P.it
dc.contributor.authorBlanken, T.it
dc.contributor.authorBobkov, V.it
dc.contributor.authorBock, A.it
dc.contributor.authorBoeyaert, D.it
dc.contributor.authorBogar, K.it
dc.contributor.authorBogar, O.it
dc.contributor.authorBohm, P.it
dc.contributor.authorBolzonella, T.it
dc.contributor.authorBombarda, F.it
dc.contributor.authorBoncagni, L.it
dc.contributor.authorBouquey, F.it
dc.contributor.authorBowman, C.it
dc.contributor.authorBrezinsek, S.it
dc.contributor.authorBrida, D.it
dc.contributor.authorBrunetti, D.it
dc.contributor.authorBucalossi, J.it
dc.contributor.authorBuchanan, J.it
dc.contributor.authorBuermans, J.it
dc.contributor.authorBufferand, H.it
dc.contributor.authorBuller, S.it
dc.contributor.authorBuratti, P.it
dc.contributor.authorBurckhart, A.it
dc.contributor.authorCalabr, G.it
dc.contributor.authorCalacci, L.it
dc.contributor.authorCamenen, Y.it
dc.contributor.authorCannas, B.it
dc.contributor.authorCano Megías, P.it
dc.contributor.authorCarnevale, D.it
dc.contributor.authorCarpanese, F.it
dc.contributor.authorCarr, M.it
dc.contributor.authorCarralero, D.it
dc.contributor.authorCarraro, L.it
dc.contributor.authorCasolari, A.it
dc.contributor.authorCathey, A.it
dc.contributor.authorCausa, F.it
dc.contributor.authorCavedon, M.it
dc.contributor.authorCecconello, M.it
dc.contributor.authorCeccuzzi, S.it
dc.contributor.authorCerovsky, J.it
dc.contributor.authorChapman, S.it
dc.contributor.authorChmielewski, P.it
dc.contributor.authorChoi, D.it
dc.contributor.authorCianfarani, C.it
dc.contributor.authorCiraolo, G.it
dc.contributor.authorCoda, S.it
dc.contributor.authorCoelho, R.it
dc.contributor.authorColas, L.it
dc.contributor.authorColette, D.it
dc.contributor.authorCordaro, L.it
dc.contributor.authorCordella, F.it
dc.contributor.authorCostea, S.it
dc.contributor.authorCoster, D.it
dc.contributor.authorCruz Zabala, D. J.it
dc.contributor.authorCseh, G.it
dc.contributor.authorCzarnecka, A.it
dc.contributor.authorCziegler, I.it
dc.contributor.authorD'Arcangelo, O.it
dc.contributor.authorDal Molin, A.it
dc.contributor.authorDavid, P.it
dc.contributor.authorDe Carolis, G.it
dc.contributor.authorDe Oliveira, H.it
dc.contributor.authorMastrostefano, Stefanoit
dc.date.accessioned2023-01-24T00:08:13Z-
dc.date.available2023-01-24T00:08:13Z-
dc.date.issued2019it
dc.identifier.issn00295515it
dc.identifier.urihttp://hdl.handle.net/2067/48945-
dc.description.abstractWithin the EUROfusion MST1 work package, a series of experiments has been conducted on AUG and TCV devices to disentangle the role of plasma fueling and plasma shape for the onset of small ELM regimes. On both devices, small ELM regimes with high confinement are achieved if and only if two conditions are fulfilled at the same time. Firstly, the plasma density at the separatrix must be large enough (ne,sep/nG ∼ 0.3), leading to a pressure profile flattening at the separatrix, which stabilizes type-I ELMs. Secondly, the magnetic configuration has to be close to a double null (DN), leading to a reduction of the magnetic shear in the extreme vicinity of the separatrix. As a consequence, its stabilizing effect on ballooning modes is weakened.it
dc.titleDependence on plasma shape and plasma fueling for small edge-localized mode regimes in TCV and ASDEX Upgradeit
dc.typearticle*
dc.identifier.doi10.1088/1741-4326/ab2211it
dc.identifier.scopus2-s2.0-85070909412it
dc.identifier.urlhttps://api.elsevier.com/content/abstract/scopus_id/85070909412it
dc.relation.journalNUCLEAR FUSIONit
dc.relation.firstpage086020it
dc.relation.volume59it
dc.relation.issue8it
dc.type.miur262*
item.fulltextWith Fulltext-
item.openairetypearticle-
item.cerifentitytypePublications-
item.grantfulltextrestricted-
item.openairecristypehttp://purl.org/coar/resource_type/c_18cf-
crisitem.journal.journalissn0029-5515-
crisitem.journal.anceE122730-
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