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dc.creatorCruz Zabala, Diego Josées
dc.creatorViezzer, Eleonoraes
dc.creatorCano Megías, Pilares
dc.creatorCavedon, Marcoes
dc.creatorDux, Ralphes
dc.creatorPlank, Ulrikees
dc.creatorPütterich, Thomases
dc.creatorMcKay, Kiera Annees
dc.creatorRodríguez González, Alfonsoes
dc.creatorGarcía Muñoz, Manueles
dc.date.accessioned2024-07-18T15:49:49Z
dc.date.available2024-07-18T15:49:49Z
dc.date.issued2024-06-12
dc.identifier.citationCruz Zabala, D.J., Viezzer, E., Cano Megías, P., Cavedon, M., Dux, R., Plank, U.,...,García Muñoz, M. (2024). Poloidal structure of the edge parallel flow in H-mode, L-mode and I-mode confinement regimes. Nuclear Fusion, 64 (7), 076051. https://doi.org/10.1088/1741-4326/ad518f.
dc.identifier.issn0029-5515es
dc.identifier.issn1741-4326es
dc.identifier.urihttps://hdl.handle.net/11441/161529
dc.description.abstractImpurity profiles have been measured with the edge high field side (HFS) and low field side (LFS) charge exchange recombination spectroscopy suite at ASDEX Upgrade enabling the study of the poloidal structure of the edge parallel flow in H-mode, L-mode and I-mode. In H-mode, asymmetries in the impurity density, toroidal and poloidal rotations are found. In I-mode, only toroidal rotation asymmetries have been measured while in L-mode no asymmetries have been observed. The measured parallel flow can be divided in two components, the Pfirsch-Schlüter (PS) flow and the symmetric flow. Two different methods have been followed to determine both contributions to the parallel flow. The first method is based on the calculation of the PS flow at the HFS and LFS from the radial electric field. The second method directly provides the symmetric flow from the flux surface average (FSA) of the parallel flow. In H-mode, the methods provide different results, while in L-mode and I-mode they agree. The differences observed in H-mode between the two methods could be explained by the existence of asymmetries in the impurity density, by the non-negligible particle sources and radial losses, or by the approximations made in the calculation of the FSA of the parallel flow from measurements in two poloidal positions (midplane HFS and LFS) only.es
dc.description.sponsorshipMinisterio de Ciencia e Innovación PID2020-116822RB-I00es
dc.description.sponsorshipEuropean Research Council (ERC) 805162es
dc.formatapplication/pdfes
dc.format.extent8 p.es
dc.language.isoenges
dc.publisherInstitute of Physics Publishinges
dc.relation.ispartofNuclear Fusion, 64 (7), 076051.
dc.rightsAtribución 4.0 Internacional*
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/*
dc.subjectAsymmetryes
dc.subjectCXRSes
dc.subjectFlowses
dc.subjectImpurityes
dc.titlePoloidal structure of the edge parallel flow in H-mode, L-mode and I-mode confinement regimeses
dc.typeinfo:eu-repo/semantics/articlees
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.projectIDPID2020-116822RB-I00es
dc.relation.projectID805162es
dc.relation.publisherversionhttps://doi.org/10.1088/1741-4326/ad518fes
dc.identifier.doi10.1088/1741-4326/ad518fes
dc.journaltitleNuclear Fusiones
dc.publication.volumen64es
dc.publication.issue7es
dc.publication.initialPage076051es
dc.contributor.funderMinisterio de Ciencia e Innovación (MICIN). Españaes
dc.contributor.funderEuropean Research Council (ERC)es

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