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dc.creatorWynn, A.es
dc.creatorLipschultz, B.es
dc.creatorCziegler, I.es
dc.creatorHarrison, J.es
dc.creatorJaervinen, A.es
dc.creatorJet Contributorses
dc.creatorGarcía Muñoz, Manueles
dc.date.accessioned2020-07-17T14:06:30Z
dc.date.available2020-07-17T14:06:30Z
dc.date.issued2018
dc.identifier.citationWynn, A., Lipschultz, B., Cziegler, I., Harrison, J., Jaervinen, A., Jet Contributors, y García Muñoz, M. (2018). Investigation into the formation of the scrape-off layer density shoulder in JET ITER-like wall L-mode and H-mode plasmas. Nuclear Fusion, 58 (5), 1-22.
dc.identifier.issn1741-4326es
dc.identifier.urihttps://hdl.handle.net/11441/99621
dc.description.abstractThe low temperature boundary layer plasma (scrape-off layer or SOL) between the hot core and the surrounding vessel determines the level of power loading, erosion and implantation of material surfaces, and thus the viability of tokamak-based fusion as an energy source. This study explores mechanisms affecting the formation of flattened density profiles, so-called ‘density shoulders’, in the low-field side (LFS) SOL, which modify ion and neutral fluxes to surfaces—and subsequent erosion. There is evidence against local enhancement of ionization inducing shoulder formation. We find that increases in SOL parallel resistivity, Λdiv (=[L||νeiΩi]/csΩe), postulated to lead to shoulder growth through changes in SOL turbulence characteristics, correlates with increases in SOL shoulder amplitude, As, but only under a subset of conditions (D2-fuelled L-mode density scans with outer strike point on the horizontal target). Λdiv fails to correlate with As for cases of N2 seeding or during sweeping of the strike point across the horizontal target. The limited correlation of Λdiv and As is also found for H-mode discharges. Thus, while it may be necessary for Λdiv to be above a threshold of ~1 for shoulder formation and/or growth, another mechanism is required. More significantly, we find that in contrast to parallel resistivity, outer divertor recycling, as quantified by the total outer divertor Balmer Dα emission, I–Dα, does scale with As where Λdiv does and even where Λdiv does not. Divertor recycling could lead to SOL density shoulder formation through: (a) reducing the parallel to the field flow (loss) of ions out of the SOL to the divertor; and (b) changes in radial electric fields which lead to E × B poloidal flows as well as potentially affecting SOL turbulence birth characteristics. Thus, changes in divertor recycling may be the sole process involved in bringinges
dc.description.sponsorshipEURATOM 633053es
dc.description.sponsorshipEPSRC EP/L01663X/1es
dc.description.sponsorshipEPSRC EP/K504178/1es
dc.description.sponsorshipRCUK Energy EP/I501045es
dc.formatapplication/pdfes
dc.format.extent22 p.es
dc.language.isoenges
dc.publisherIOP Publishinges
dc.relation.ispartofNuclear Fusion, 58 (5), 1-22.
dc.rightsAttribution-NonCommercial-NoDerivatives 4.0 Internacional*
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/4.0/*
dc.subjectTokamakses
dc.subjectScrapeoff layer transportes
dc.subjectDivertor recyclinges
dc.subjectDivertor geometryes
dc.subjectSOL shoulderes
dc.titleInvestigation into the formation of the scrape-off layer density shoulder in JET ITER-like wall L-mode and H-mode plasmases
dc.typeinfo:eu-repo/semantics/articlees
dcterms.identifierhttps://ror.org/03yxnpp24
dc.type.versioninfo:eu-repo/semantics/publishedVersiones
dc.rights.accessRightsinfo:eu-repo/semantics/openAccesses
dc.contributor.affiliationUniversidad de Sevilla. Departamento de Física Atómica, Molecular y Nucleares
dc.relation.projectID633053es
dc.relation.projectIDEP/L01663X/1es
dc.relation.projectIDEP/K504178/1es
dc.relation.projectIDEP/I501045es
dc.relation.publisherversionhttps://doi.org/10.1088/1741-4326/aaad78es
dc.identifier.doi10.1088/1741-4326/aaad78es
dc.contributor.groupUniversidad de Sevilla. RNM138: Física Nuclear Aplicadaes
dc.journaltitleNuclear Fusiones
dc.publication.volumen58es
dc.publication.issue5es
dc.publication.initialPage1es
dc.publication.endPage22es

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