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dc.creatorCavedon, M.es
dc.creatorPütterich, T.es
dc.creatorViezzer, Eleonoraes
dc.creatorLaggner, F. M.es
dc.creatorBurckhart, A.es
dc.creatorDunne, M. G.es
dc.creatorFischer, R.es
dc.creatorLebschy, A.es
dc.creatorMink, F.es
dc.creatorStroth, U.es
dc.creatorWillensdorfer, M.es
dc.creatorWolfrum, E.es
dc.date.accessioned2018-09-17T08:12:01Z
dc.date.available2018-09-17T08:12:01Z
dc.date.issued2017
dc.identifier.citationCavedon, M., Pütterich, T., Viezzer, E., Laggner, F.M., Burckhart, A., Dunne, M.G.,...,Wolfrum, E. (2017). Pedestal and Er profile evolution during an edge localized mode cycle at ASDEX Upgrade. Plasma Physics and Controlled Fusion, 59, 105007 (8pp). https://doi.org/10.1088/1361-6587/aa7ad0.
dc.identifier.issn1361-6587es
dc.identifier.urihttps://hdl.handle.net/11441/78538
dc.description.abstractThe upgrade of the edge charge exchange recombination spectroscopy diagnostic at ASDEX Upgrade has enabled highly spatially resolved me asurements of the impurity ion dynamics during an edge-localized mode cycle ( ELM ) with unprecedented temp oral resolution, i.e. 65 μ s. The increase of transport during an ELM induces a relaxation of the ion, electron edge gradients in impurity density and fl ows. Detailed characterization of the recovery of the edge temperature gradients reveals a difference in the ion and electron channe l: the maximum ion temperature gradient T i  is re-established on similar timescales as n e  , which is faster than the recovery of T e  .Afterthe clamping of the maximum gradient, T i and T e at the pedestal top continue to rise up to the next ELM while n e stays constant which means that the temperatur e pedestal and the resu lting pedestal pressure widen until the next ELM. The edge radial electric fi eld E r at the ELM crash is found to reduce to typical L-mode values and its ma ximum recovers to its pre-ELM conditions on a similar time scale as for n e and T i . Within the uncertainties, the measurements of E r align with their neoclassical predictions E r,neo for most of the ELM cycle, thus indicating that E r is dominated by collisional processes. However, between 2 and 4 ms af ter the ELM crash, other contributions to E B ́ fl ow, e.g. zonal fl ows or ion orbit effects, could not be excluded within the uncertainties.es
dc.description.sponsorshipEuropean Commission (EUROfusion 633053)es
dc.formatapplication/pdfes
dc.language.isoenges
dc.publisherIOP Publishinges
dc.relation.ispartofPlasma Physics and Controlled Fusion, 59, 105007 (8pp).
dc.rightsAttribution-NonCommercial-NoDerivatives 4.0 Internacional*
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/4.0/*
dc.subjectEdge localised modeses
dc.subjectIon temperaturees
dc.subjectEdge gradient recoveryes
dc.subjectRadial electric fieldes
dc.titlePedestal and Er profile evolution during an edge localized mode cycle at ASDEX Upgradees
dc.typeinfo:eu-repo/semantics/articlees
dcterms.identifierhttps://ror.org/03yxnpp24
dc.type.versioninfo:eu-repo/semantics/submittedVersiones
dc.rights.accessRightsinfo:eu-repo/semantics/openAccesses
dc.contributor.affiliationUniversidad de Sevilla. Departamento de Física Atómica, Molecular y Nucleares
dc.relation.projectIDEUROfusion 633053es
dc.relation.publisherversionhttp://iopscience.iop.org/article/10.1088/1361-6587/aa7ad0es
dc.identifier.doi10.1088/1361-6587/aa7ad0es
idus.format.extent8es
dc.journaltitlePlasma Physics and Controlled Fusiones
dc.publication.volumen59es
dc.publication.initialPage105007 (8pp)es
dc.contributor.funderEuropean Commission (EC)

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