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dc.contributor.authorLu, Tien-Changen_US
dc.contributor.authorLai, Ying-Yuen_US
dc.contributor.authorLan, Yu-Pinen_US
dc.contributor.authorHuang, Si-Weien_US
dc.contributor.authorChen, Jun-Rongen_US
dc.contributor.authorWu, Yung-Chien_US
dc.contributor.authorHsieh, Wen-Fengen_US
dc.contributor.authorDeng, Huien_US
dc.date.accessioned2014-12-08T15:21:56Z-
dc.date.available2014-12-08T15:21:56Z-
dc.date.issued2012-02-27en_US
dc.identifier.issn1094-4087en_US
dc.identifier.urihttp://dx.doi.org/10.1364/OE.20.005530en_US
dc.identifier.urihttp://hdl.handle.net/11536/15617-
dc.description.abstractWe report on the room temperature polariton lasing and photon lasing in a ZnO-based hybrid microcavity under optical pumping. A series of experimental studies of the polariton lasing (exciton-photon detunings of delta = -119meV) in the strong-coupling regime are discussed and compared to a photon lasing (delta = -45meV) in the weak-coupling regime obtained in the same structure. The measured threshold power density (31.8kW/cm(2)) of polariton lasing is one order of magnitude lower than that of the photon lasing (318.2kW/cm(2)). In addition, the comparison between polariton lasing and photon lasing is done in terms of the linewidth broadening, blue-shift of the emission peak, and polarization. (C) 2012 Optical Society of Americaen_US
dc.language.isoen_USen_US
dc.titleRoom temperature polariton lasing vs. photon lasing in a ZnO-based hybrid microcavityen_US
dc.typeArticleen_US
dc.identifier.doi10.1364/OE.20.005530en_US
dc.identifier.journalOPTICS EXPRESSen_US
dc.citation.volume20en_US
dc.citation.issue5en_US
dc.citation.spage5530en_US
dc.citation.epage5537en_US
dc.contributor.department光電工程學系zh_TW
dc.contributor.departmentDepartment of Photonicsen_US
dc.identifier.wosnumberWOS:000301053200073-
dc.citation.woscount19-
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