Designing whispering gallery modes via transformation optics

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dc.contributor.authorKim, Yushinko
dc.contributor.authorLee, Soo-Youngko
dc.contributor.authorRyu, Jung-Wanko
dc.contributor.authorKim, Inboko
dc.contributor.authorHan, Jae-Hyungko
dc.contributor.authorTae, Heung-Sikko
dc.contributor.authorChoi, Muhanko
dc.contributor.authorMin, Bumkiko
dc.date.accessioned2016-11-29T05:07:46Z-
dc.date.available2016-11-29T05:07:46Z-
dc.date.created2016-11-08-
dc.date.created2016-11-08-
dc.date.issued2016-10-
dc.identifier.citationNATURE PHOTONICS, v.10, no.10, pp.647 - 652-
dc.identifier.issn1749-4885-
dc.identifier.urihttp://hdl.handle.net/10203/214105-
dc.description.abstractIn dielectric cavities with a rotational symmetry, whispering gallery modes (WGMs) with an extremely long lifetime (that is, a very high Q factor) can be formed by total internal reflection of light around the rim of the cavities. The ultrahigh Q factor of WGMs has enabled a variety of impressive photonic systems, such as ultralow threshold microlasers(1-3), biosensors with unprecedented sensitivity(4,5) and cavity optomechanical devices(6). However, the isotropic emission of WGMs, which is due to the rotational symmetry, is a serious drawback in applications that require directional light sources. Considerable efforts have thus been devoted to achieving directional emission by intentionally breaking the rotational symmetry(7-9). However, all of the methods proposed so far have suffered from substantial Q-spoiling. Here, we show how the mode properties of dielectric whispering gallery cavities, such as the Q factor and emission directionality, can be tailored at will using transformation optics. The proposed scheme will open a new horizon of applications beyond the conventional WGMs-
dc.languageEnglish-
dc.publisherNATURE PUBLISHING GROUP-
dc.subjectDIRECTIONAL EMISSION-
dc.subjectCLOAK-
dc.subjectMICROCAVITY-
dc.subjectFREQUENCIES-
dc.subjectRESONATORS-
dc.subjectSYSTEMS-
dc.subjectLASERS-
dc.titleDesigning whispering gallery modes via transformation optics-
dc.typeArticle-
dc.identifier.wosid000384951900010-
dc.identifier.scopusid2-s2.0-84988733643-
dc.type.rimsART-
dc.citation.volume10-
dc.citation.issue10-
dc.citation.beginningpage647-
dc.citation.endingpage652-
dc.citation.publicationnameNATURE PHOTONICS-
dc.identifier.doi10.1038/NPHOTON.2016.184-
dc.contributor.localauthorMin, Bumki-
dc.contributor.nonIdAuthorLee, Soo-Young-
dc.contributor.nonIdAuthorRyu, Jung-Wan-
dc.contributor.nonIdAuthorKim, Inbo-
dc.contributor.nonIdAuthorHan, Jae-Hyung-
dc.contributor.nonIdAuthorTae, Heung-Sik-
dc.contributor.nonIdAuthorChoi, Muhan-
dc.type.journalArticleArticle-
dc.subject.keywordPlusDIRECTIONAL EMISSION-
dc.subject.keywordPlusCLOAK-
dc.subject.keywordPlusMICROCAVITY-
dc.subject.keywordPlusFREQUENCIES-
dc.subject.keywordPlusRESONATORS-
dc.subject.keywordPlusSYSTEMS-
dc.subject.keywordPlusLASERS-
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