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In, Yongkyoon
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dc.citation.number 11 -
dc.citation.startPage 112501 -
dc.citation.title PHYSICS OF PLASMAS -
dc.citation.volume 27 -
dc.contributor.author Kim, Minwoo -
dc.contributor.author Lee, J. -
dc.contributor.author Ko, W. H. -
dc.contributor.author Hahn, S. -H. -
dc.contributor.author In, Yongkyoon -
dc.contributor.author Jeon, Y. M. -
dc.contributor.author Suttrop, W. -
dc.contributor.author Kim, S. K. -
dc.contributor.author Park, G. Y. -
dc.contributor.author Juhn, J. -W. -
dc.contributor.author Lee, J. H. -
dc.date.accessioned 2023-12-21T16:43:17Z -
dc.date.available 2023-12-21T16:43:17Z -
dc.date.created 2020-11-30 -
dc.date.issued 2020-11 -
dc.description.abstract Excellent reproducibility of KSTAR resonant magnetic perturbation (RMP)-driven, edge-localized mode (ELM)-crash suppression enables us to construct a database reliably for the study of ELM-crash suppression conditions. To establish a high-fidelity database, we have selected one of the frequently used RMP configurations in KSTAR, n=1, + 90 degrees phasing RMP-coil configuration. A series of fitting curves based on edge profile diagnostics data is used for normalized electron collisionality ( nu e *) and plasma toroidal rotation ( V tor) at pedestal top. Since ITER is expected to employ slowly rotating, low-collisionality, high-density plasmas whose conditions are not readily accessible in the existing devices, the exploration and understanding of these two parameters would be important not only for RMP-driven, ELM-crash-suppression physics but also for the success of ITER. The data points for the ELM-crash suppression phase are in the range of 0.2 < e , ped * <1.1 with Z eff=2 assumption and V tor , ped >40km/s. Suppression thresholds or boundaries in nu e , ped * or V tor , ped are not confirmed in the investigated parameter ranges so far. The KSTAR database still needs additional experimental datasets in ITER-relevant conditions ( nu e , ped * similar to 0.1 and low-torque low-rotation) to confirm the boundary of the ELM-crash suppression window in KSTAR and reduce the uncertainties of the RMP ELM-crash control technique in ITER. In both nu e , ped * and V tor , ped parameters, the phase-space distribution of the ELM-crash suppression has no clear distinction from that of the ELM-crash mitigation. Linear discriminant analysis provides a linear combination of parameters relevant to ELM-crash suppression, best separating two data categories. Recursive feature elimination indicates that n e , ped and I RMP, as well as nu e , ped * and V tor , ped, are critical variables in the separation of the data groups. -
dc.identifier.bibliographicCitation PHYSICS OF PLASMAS, v.27, no.11, pp.112501 -
dc.identifier.doi 10.1063/5.0024055 -
dc.identifier.issn 1070-664X -
dc.identifier.scopusid 2-s2.0-85095722694 -
dc.identifier.uri https://scholarworks.unist.ac.kr/handle/201301/48848 -
dc.identifier.url https://aip.scitation.org/doi/10.1063/5.0024055 -
dc.identifier.wosid 000588468900001 -
dc.language 영어 -
dc.publisher AMER INST PHYSICS -
dc.title Pedestal electron collisionality and toroidal rotation during ELM-crash suppression phase under n=1 RMP in KSTAR -
dc.type Article -
dc.description.isOpenAccess TRUE -
dc.relation.journalWebOfScienceCategory Physics, Fluids & Plasmas -
dc.relation.journalResearchArea Physics -
dc.type.docType Article -
dc.description.journalRegisteredClass scie -
dc.description.journalRegisteredClass scopus -

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