Lasing action in single subwavelength particles supporting supercavity modes

buir.contributor.authorDemir, Hilmi Volkan
buir.contributor.orcidDemir, Hilmi Volkan|0000-0003-1793-112X
dc.citation.epage7346en_US
dc.citation.issueNumber6en_US
dc.citation.spage7338en_US
dc.citation.volumeNumber14en_US
dc.contributor.authorMylnikov, V.
dc.contributor.authorHa, S. T.
dc.contributor.authorPan, Z.
dc.contributor.authorValuckas, V.
dc.contributor.authorPaniagua-Domínguez, R.
dc.contributor.authorDemir, Hilmi Volkan
dc.contributor.authorKuznetsov, A. I.
dc.date.accessioned2021-02-12T12:41:36Z
dc.date.available2021-02-12T12:41:36Z
dc.date.issued2020-05
dc.departmentDepartment of Electrical and Electronics Engineeringen_US
dc.departmentDepartment of Physicsen_US
dc.departmentInstitute of Materials Science and Nanotechnology (UNAM)en_US
dc.description.abstractOn-chip light sources are critical for the realization of fully integrated photonic circuitry. So far, semiconductor miniaturized lasers have been mainly limited to sizes on the order of a few microns. Further reduction of sizes is challenging fundamentally due to the associated radiative losses. While using plasmonic metals helps to reduce radiative losses and sizes, they also introduce Ohmic losses hindering real improvements. In this work, we show that, making use of quasibound states in the continuum, or supercavity modes, we circumvent these fundamental issues and realize one of the smallest purely semiconductor nanolasers thus far. Here, the nanolaser structure is based on a single semiconductor nanocylinder that intentionally takes advantage of the destructive interference between two supported optical modes, namely Fabry–Perot and Mie modes, to obtain a significant enhancement in the quality factor of the cavity. We experimentally demonstrate the concept and obtain optically pumped lasing action using GaAs at cryogenic temperatures. The optimal nanocylinder size is as small as 500 nm in diameter and only 330 nm in height with a lasing wavelength around 825 nm, corresponding to a size-to-wavelength ratio as low as 0.6.en_US
dc.description.provenanceSubmitted by Evrim Ergin (eergin@bilkent.edu.tr) on 2021-02-12T12:41:36Z No. of bitstreams: 1 Lasing_action_in_single_subwavelength_particles_supporting_supercavity_modes.pdf: 2652133 bytes, checksum: c42856a0e54e7341e1f6fc59711f4f81 (MD5)en
dc.description.provenanceMade available in DSpace on 2021-02-12T12:41:36Z (GMT). No. of bitstreams: 1 Lasing_action_in_single_subwavelength_particles_supporting_supercavity_modes.pdf: 2652133 bytes, checksum: c42856a0e54e7341e1f6fc59711f4f81 (MD5) Previous issue date: 2020-05en
dc.identifier.doi10.1021/acsnano.0c02730en_US
dc.identifier.issn1936-0851
dc.identifier.urihttp://hdl.handle.net/11693/55120
dc.language.isoEnglishen_US
dc.publisherAmerican Chemical Societyen_US
dc.relation.isversionofhttps://dx.doi.org/10.1021/acsnano.0c02730en_US
dc.source.titleACS Nanoen_US
dc.subjectDielectric nanoantennasen_US
dc.subjectLaseren_US
dc.subjectNanolaseren_US
dc.subjectBound state in the continuumen_US
dc.subjectMie resonanceen_US
dc.subjectGallium arsenideen_US
dc.titleLasing action in single subwavelength particles supporting supercavity modesen_US
dc.typeArticleen_US

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