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Ultra-high modulation depth exceeding 2,400% in optically controlled topological surface plasmons

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dc.contributor.authorSim, Sangwan-
dc.contributor.authorJang, Houk-
dc.contributor.authorKoirala, Nikesh-
dc.contributor.authorBrahlek, Matthew-
dc.contributor.authorMoon, Jisoo-
dc.contributor.authorSung, Ji Ho-
dc.contributor.authorPark, Jun-
dc.contributor.authorCha, Soonyoung-
dc.contributor.authorOh, Seongshik-
dc.contributor.authorJo, Moon-Ho-
dc.contributor.authorAhn, Jong-Hyun-
dc.contributor.authorChoi, Hyunyong-
dc.date.accessioned2021-06-22T19:03:14Z-
dc.date.available2021-06-22T19:03:14Z-
dc.date.created2021-01-21-
dc.date.issued2015-10-
dc.identifier.issn2041-1723-
dc.identifier.urihttps://scholarworks.bwise.kr/erica/handle/2021.sw.erica/17007-
dc.description.abstractModulating light via coherent charge oscillations in solids is the subject of intense research topics in opto-plasmonics. Although a variety of methods are proposed to increase such modulation efficiency, one central challenge is to achieve a high modulation depth ( defined by a ratio of extinction with/without light) under small photon-flux injection, which becomes a fundamental trade-off issue both in metals and semiconductors. Here, by fabricating simple micro-ribbon arrays of topological insulator Bi2Se3, we report an unprecedentedly large modulation depth of 2,400% at 1.5 THz with very low optical fluence of 45 mu J cm(-2). This was possible, first because the extinction spectrum is nearly zero due to the Fano-like plasmon-phonon-destructive interference, thereby contributing an extremely small denominator to the extinction ratio. Second, the numerator of the extinction ratio is markedly increased due to the photoinduced formation of massive two-dimensional electron gas below the topological surface states, which is another contributor to the ultra-high modulation depth.-
dc.language영어-
dc.language.isoen-
dc.publisherNature Publishing Group-
dc.titleUltra-high modulation depth exceeding 2,400% in optically controlled topological surface plasmons-
dc.typeArticle-
dc.contributor.affiliatedAuthorSim, Sangwan-
dc.identifier.doi10.1038/ncomms9814-
dc.identifier.scopusid2-s2.0-84946142721-
dc.identifier.wosid000209871200001-
dc.identifier.bibliographicCitationNature Communications, v.6, pp.1 - 7-
dc.relation.isPartOfNature Communications-
dc.citation.titleNature Communications-
dc.citation.volume6-
dc.citation.startPage1-
dc.citation.endPage7-
dc.type.rimsART-
dc.type.docTypeArticle-
dc.description.journalClass1-
dc.description.isOpenAccessY-
dc.description.journalRegisteredClassscie-
dc.description.journalRegisteredClassscopus-
dc.relation.journalResearchAreaScience & Technology - Other Topics-
dc.relation.journalWebOfScienceCategoryMultidisciplinary Sciences-
dc.subject.keywordPlusDIRAC FERMIONS-
dc.subject.keywordPlusRESONANCES-
dc.subject.keywordPlusDYNAMICS-
dc.subject.keywordPlusSYSTEMS-
dc.subject.keywordPlusSTATE-
dc.identifier.urlhttps://www.nature.com/articles/ncomms9814-
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