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These instabilities are well-correlated with intermittent RE losses in the beginning of RE current formation. The runaway current phase is not observed when the power of instabilities exceeds a threshold. Novel measurements of the RE distribution function during the CQ indicate that the instabilities appear when RE energy (E-RE ) exceeds 2.5-3 MeV, the number of modes grows linearly with E-RE , and their frequencies lie in the range 0.1-3 MHz, below the ion cyclotron frequency. Possible plasma waves exciting by REs in this region are proposed. Increase of the amount of injected argon decreases the E-RE and increases the success rate of the runaway current formation, while increase of the pre-disruption plasma current acts in the opposite direction. No dependence on the pre-disruption core electron temperature is found.", "subjects" : [ { "otype" : "Classification", "mtid" : 10154, "link" : "/api/classification/10154", "label" : "Physical sciences", "published" : true, "snippet" : true } ], "keywords" : [ { "otype" : "Keyword", "mtid" : 1398979, "link" : "/api/keyword/1398979", "label" : "RUNAWAY ELECTRONS", "published" : true, "oldId" : 1398979, "snippet" : true }, { "otype" : "Keyword", "mtid" : 1675921, "link" : "/api/keyword/1675921", "label" : "kinetic instabilities", "published" : true, "snippet" : true }, { "otype" : "Keyword", "mtid" : 1675922, "link" : "/api/keyword/1675922", "label" : "tokamak disruptions", "published" : true, "snippet" : true }, { "otype" : "Keyword", "mtid" : 1675923, "link" : "/api/keyword/1675923", "label" : "massive gas injection", "published" : true, "snippet" : true } ], "digital" : null, "printed" : null, "sourceYear" : 2019, "foreignEdition" : true, "foreignLanguage" : true, "fullPublication" : true, "conferencePublication" : false, "nationalOrigin" : null, "missingAuthor" : false, "oaType" : "NONE", "oaCheckDate" : "2023-10-30", "oaFree" : false, "citationCount" : 0, "citationCountUnpublished" : 0, "citationCountWoOther" : 0, "independentCitCountWoOther" : 0, "doiCitationCount" : 0, "wosCitationCount" : 0, "scopusCitationCount" : 0, "independentCitationCount" : 0, "unhandledCitationCount" : 0, "citingPubCount" : 0, "independentCitingPubCount" : 0, "unhandledCitingPubCount" : 0, "citedPubCount" : 4, "citedCount" : 4, "ratings" : [ { "otype" : "SjrRating", "mtid" : 11001567, "link" : "/api/sjrrating/11001567", "label" : "sjr:D1 (2018) Scopus - Condensed Matter Physics PLASMA PHYSICS AND CONTROLLED FUSION 0741-3335 1361-6587", "listPos" : 34, "rankValue" : 0.1, "type" : "journal", "ratingType" : { "otype" : "RatingType", "mtid" : 10002, "link" : "/api/ratingtype/10002", "label" : "sjr", "code" : "sjr", "published" : true, "snippet" : true }, "subject" : { "otype" : "ClassificationExternal", "mtid" : 3104, "link" : "/api/classificationexternal/3104", "label" : "Scopus - Condensed Matter Physics", "published" : true, "oldId" : 3104, "snippet" : true }, "ranking" : "D1", "calculation" : "DIRECT", "published" : true, "snippet" : true } ], "ratingsForSort" : "D1", "hasCitationDuplums" : false, "userChangeableUntil" : "2020-03-11T02:11:47.842+0000", "directInstitutesForSort" : "", "ownerAuthorCount" : 10, "ownerInstituteCount" : 37, "directInstituteCount" : 0, "authorCount" : 15, "contributorCount" : 0, "hasQualityFactor" : true, "link" : "/api/publication/30565356", "label" : "Lvovskiy A. et al. 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