m=+/-1 and m=+/-2 mode helicon wave excitation

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dc.contributor.authorKim, JHko
dc.contributor.authorYun, SMko
dc.contributor.authorChang, Hong-Youngko
dc.date.accessioned2013-03-02T15:39:20Z-
dc.date.available2013-03-02T15:39:20Z-
dc.date.created2012-02-06-
dc.date.created2012-02-06-
dc.date.issued1996-12-
dc.identifier.citationIEEE TRANSACTIONS ON PLASMA SCIENCE, v.24, no.6, pp.1364 - 1370-
dc.identifier.issn0093-3813-
dc.identifier.urihttp://hdl.handle.net/10203/74215-
dc.description.abstractThe characteristics of plasma produced by plane polarized m = +/-1 and m = +/-2 mode helicon waves were investigated for the first time. Plane polarized m = ii and m = +/-2 mode helicon waves were mainly excited using a Nagoya type III antenna and a quadrupole antenna, respectively. Two-dimensional cross-field measurements of ArII optical emission induced by hot electrons were made to investigate the RF power deposition. The components of the wave magnetic field measured with a magnetic probe were compared with the field profiles computed for the m = +/-1 and m = +/-2 modes. Two and four high intensity plasma columns were observed for the m = +/-1 and m = +/-2 modes, respectively. These columns were located at the regions between the antenna legs. The radial profiles of the wave magnetic field were in good agreement with computations.-
dc.languageEnglish-
dc.publisherIEEE-INST ELECTRICAL ELECTRONICS ENGINEERS INC-
dc.subjectPLASMA PRODUCTION-
dc.titlem=+/-1 and m=+/-2 mode helicon wave excitation-
dc.typeArticle-
dc.identifier.wosidA1996VY93600007-
dc.identifier.scopusid2-s2.0-0030418237-
dc.type.rimsART-
dc.citation.volume24-
dc.citation.issue6-
dc.citation.beginningpage1364-
dc.citation.endingpage1370-
dc.citation.publicationnameIEEE TRANSACTIONS ON PLASMA SCIENCE-
dc.contributor.localauthorChang, Hong-Young-
dc.contributor.nonIdAuthorKim, JH-
dc.contributor.nonIdAuthorYun, SM-
dc.type.journalArticleArticle-
dc.subject.keywordPlusPLASMA PRODUCTION-
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