Broadband dispersion-engineered microresonator on a chip

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dc.contributor.authorYang, Ki Youlko
dc.contributor.authorBeha, Katjako
dc.contributor.authorCole, Daniel C.ko
dc.contributor.authorYi, Xuko
dc.contributor.authorDel'Haye, Pascalko
dc.contributor.authorLee, Hansuekko
dc.contributor.authorLi, Jiangko
dc.contributor.authorOh, Dong Yoonko
dc.contributor.authorDiddams, Scott A.ko
dc.contributor.authorPapp, Scott B.ko
dc.contributor.authorVahala, Kerry J.ko
dc.date.accessioned2016-07-05T07:49:48Z-
dc.date.available2016-07-05T07:49:48Z-
dc.date.created2016-05-27-
dc.date.created2016-05-27-
dc.date.issued2016-05-
dc.identifier.citationNATURE PHOTONICS, v.10, no.5, pp.316 - 316-
dc.identifier.issn1749-4885-
dc.identifier.urihttp://hdl.handle.net/10203/209206-
dc.description.abstractThe control of dispersion in fibre optical waveguides is of critical importance to optical fibre communications systems(1,2) and more recently for continuum generation from the ultraviolet to the mid-infrared(3-5). The wavelength at which the group velocity dispersion crosses zero can be set by varying the fibre core diameter or index step(2,6-8). Moreover, sophisticated methods to manipulate higher-order dispersion so as to shape and even flatten the dispersion over wide bandwidths are possible using multi-cladding fibres(9-11). Here we introduce design and fabrication techniques that allow analogous dispersion control in chip-integrated optical microresonators, and thereby demonstrate higher-order, wide-bandwidth dispersion control over an octave of spectrum. Importantly, the fabrication method we employ for dispersion control simultaneously permits optical Q factors above 100 million, which is critical for the efficient operation of nonlinear optical oscillators. Dispersion control in high-Q systems has become of great importance in recent years with increased interest in chip-integrable optical frequency combs(12-32).-
dc.languageEnglish-
dc.publisherNATURE PUBLISHING GROUP-
dc.titleBroadband dispersion-engineered microresonator on a chip-
dc.typeArticle-
dc.identifier.wosid000374980100013-
dc.identifier.scopusid2-s2.0-84961927545-
dc.type.rimsART-
dc.citation.volume10-
dc.citation.issue5-
dc.citation.beginningpage316-
dc.citation.endingpage316-
dc.citation.publicationnameNATURE PHOTONICS-
dc.identifier.doi10.1038/NPHOTON.2016.36-
dc.contributor.localauthorLee, Hansuek-
dc.contributor.nonIdAuthorYang, Ki Youl-
dc.contributor.nonIdAuthorBeha, Katja-
dc.contributor.nonIdAuthorCole, Daniel C.-
dc.contributor.nonIdAuthorYi, Xu-
dc.contributor.nonIdAuthorDel'Haye, Pascal-
dc.contributor.nonIdAuthorLi, Jiang-
dc.contributor.nonIdAuthorOh, Dong Yoon-
dc.contributor.nonIdAuthorDiddams, Scott A.-
dc.contributor.nonIdAuthorPapp, Scott B.-
dc.contributor.nonIdAuthorVahala, Kerry J.-
dc.description.isOpenAccessN-
dc.type.journalArticleArticle-
dc.subject.keywordPlusFREQUENCY COMB GENERATION-
dc.subject.keywordPlusSINGLE-MODE FIBERS-
dc.subject.keywordPlusMU-M-
dc.subject.keywordPlusRAMAN LASER-
dc.subject.keywordPlusSILICA-
dc.subject.keywordPlusINDEX-
dc.subject.keywordPlusMICROCAVITY-
dc.subject.keywordPlusRESONATOR-
dc.subject.keywordPlusREGION-
dc.subject.keywordPlusSPECTROSCOPY-
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