Lasing threshold of thresholdless and non-thresholdless metal-semiconductor nanolasers
The recently developed plasmonic and photonic metal-semiconductor nanolasers feature unique properties, such as ultra-small mode volume and footprint, high Purcell factor, and ultra-fast modulation. However, it is often difficult to recognize when the transition to lasing occurs, while the most impo...
Gespeichert in:
Veröffentlicht in: | Optics express 2018-12, Vol.26 (25), p.33473-33483 |
---|---|
Hauptverfasser: | , |
Format: | Artikel |
Sprache: | eng |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
container_end_page | 33483 |
---|---|
container_issue | 25 |
container_start_page | 33473 |
container_title | Optics express |
container_volume | 26 |
creator | Vyshnevyy, Andrey A Fedyanin, Dmitry Yu |
description | The recently developed plasmonic and photonic metal-semiconductor nanolasers feature unique properties, such as ultra-small mode volume and footprint, high Purcell factor, and ultra-fast modulation. However, it is often difficult to recognize when the transition to lasing occurs, while the most important feature of laser radiation, i.e., coherence, is available only above the lasing threshold. Here we systematically study the second-order coherence properties of metal-semiconductor nanolasers at both low- and high-pump rates. We find the lasing threshold using a clear coherence definition and derive a simple expression for the threshold pump current (optical pump power), which can be applied to most thresholdless and non-thresholdless metal-semiconductor nanolasers. |
doi_str_mv | 10.1364/OE.26.033473 |
format | Article |
fullrecord | <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_miscellaneous_2179391172</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2179391172</sourcerecordid><originalsourceid>FETCH-LOGICAL-c329t-b732cbed852120392853c85ba94b001387e005988b1f4407540e4f79761bb5123</originalsourceid><addsrcrecordid>eNpVkDtPwzAURi0EoqWwMaOMDCT4ldgeUVUeUqUuwGrZiUODHLv4JgP_nlYtr-k-dPTp3oPQJcEFYRW_XS0KWhWYMS7YEZoSrHjOsRTHf_oJOgN4x5hwocQpmjBc8ZIrNUWvSwNdeMuGdXKwjr7JYvs7eAeQmdBkIYb8_7Z3g_E5uL6rY2jGeogpCyZEb8AlOEcnrfHgLg51hl7uF8_zx3y5enia3y3zmlE15FYwWlvXyJISipmismS1LK1R3G6vZVI4jEslpSUt51iUHDvebn-oiLUloWyGrve5mxQ_RgeD7juonfcmuDiCpkQopggRO_Rmj9YpAiTX6k3qepM-NcF6Z1KvFppWem9yi18dkkfbu-YH_lbHvgAZBW4T</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2179391172</pqid></control><display><type>article</type><title>Lasing threshold of thresholdless and non-thresholdless metal-semiconductor nanolasers</title><source>DOAJ Directory of Open Access Journals</source><source>Elektronische Zeitschriftenbibliothek - Frei zugängliche E-Journals</source><source>Alma/SFX Local Collection</source><creator>Vyshnevyy, Andrey A ; Fedyanin, Dmitry Yu</creator><creatorcontrib>Vyshnevyy, Andrey A ; Fedyanin, Dmitry Yu</creatorcontrib><description>The recently developed plasmonic and photonic metal-semiconductor nanolasers feature unique properties, such as ultra-small mode volume and footprint, high Purcell factor, and ultra-fast modulation. However, it is often difficult to recognize when the transition to lasing occurs, while the most important feature of laser radiation, i.e., coherence, is available only above the lasing threshold. Here we systematically study the second-order coherence properties of metal-semiconductor nanolasers at both low- and high-pump rates. We find the lasing threshold using a clear coherence definition and derive a simple expression for the threshold pump current (optical pump power), which can be applied to most thresholdless and non-thresholdless metal-semiconductor nanolasers.</description><identifier>ISSN: 1094-4087</identifier><identifier>EISSN: 1094-4087</identifier><identifier>DOI: 10.1364/OE.26.033473</identifier><identifier>PMID: 30645499</identifier><language>eng</language><publisher>United States</publisher><ispartof>Optics express, 2018-12, Vol.26 (25), p.33473-33483</ispartof><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c329t-b732cbed852120392853c85ba94b001387e005988b1f4407540e4f79761bb5123</citedby><cites>FETCH-LOGICAL-c329t-b732cbed852120392853c85ba94b001387e005988b1f4407540e4f79761bb5123</cites><orcidid>0000-0003-1394-4169 ; 0000-0001-7264-0726</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,864,27924,27925</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/30645499$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Vyshnevyy, Andrey A</creatorcontrib><creatorcontrib>Fedyanin, Dmitry Yu</creatorcontrib><title>Lasing threshold of thresholdless and non-thresholdless metal-semiconductor nanolasers</title><title>Optics express</title><addtitle>Opt Express</addtitle><description>The recently developed plasmonic and photonic metal-semiconductor nanolasers feature unique properties, such as ultra-small mode volume and footprint, high Purcell factor, and ultra-fast modulation. However, it is often difficult to recognize when the transition to lasing occurs, while the most important feature of laser radiation, i.e., coherence, is available only above the lasing threshold. Here we systematically study the second-order coherence properties of metal-semiconductor nanolasers at both low- and high-pump rates. We find the lasing threshold using a clear coherence definition and derive a simple expression for the threshold pump current (optical pump power), which can be applied to most thresholdless and non-thresholdless metal-semiconductor nanolasers.</description><issn>1094-4087</issn><issn>1094-4087</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><recordid>eNpVkDtPwzAURi0EoqWwMaOMDCT4ldgeUVUeUqUuwGrZiUODHLv4JgP_nlYtr-k-dPTp3oPQJcEFYRW_XS0KWhWYMS7YEZoSrHjOsRTHf_oJOgN4x5hwocQpmjBc8ZIrNUWvSwNdeMuGdXKwjr7JYvs7eAeQmdBkIYb8_7Z3g_E5uL6rY2jGeogpCyZEb8AlOEcnrfHgLg51hl7uF8_zx3y5enia3y3zmlE15FYwWlvXyJISipmismS1LK1R3G6vZVI4jEslpSUt51iUHDvebn-oiLUloWyGrve5mxQ_RgeD7juonfcmuDiCpkQopggRO_Rmj9YpAiTX6k3qepM-NcF6Z1KvFppWem9yi18dkkfbu-YH_lbHvgAZBW4T</recordid><startdate>20181210</startdate><enddate>20181210</enddate><creator>Vyshnevyy, Andrey A</creator><creator>Fedyanin, Dmitry Yu</creator><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><orcidid>https://orcid.org/0000-0003-1394-4169</orcidid><orcidid>https://orcid.org/0000-0001-7264-0726</orcidid></search><sort><creationdate>20181210</creationdate><title>Lasing threshold of thresholdless and non-thresholdless metal-semiconductor nanolasers</title><author>Vyshnevyy, Andrey A ; Fedyanin, Dmitry Yu</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c329t-b732cbed852120392853c85ba94b001387e005988b1f4407540e4f79761bb5123</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Vyshnevyy, Andrey A</creatorcontrib><creatorcontrib>Fedyanin, Dmitry Yu</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><jtitle>Optics express</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Vyshnevyy, Andrey A</au><au>Fedyanin, Dmitry Yu</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Lasing threshold of thresholdless and non-thresholdless metal-semiconductor nanolasers</atitle><jtitle>Optics express</jtitle><addtitle>Opt Express</addtitle><date>2018-12-10</date><risdate>2018</risdate><volume>26</volume><issue>25</issue><spage>33473</spage><epage>33483</epage><pages>33473-33483</pages><issn>1094-4087</issn><eissn>1094-4087</eissn><abstract>The recently developed plasmonic and photonic metal-semiconductor nanolasers feature unique properties, such as ultra-small mode volume and footprint, high Purcell factor, and ultra-fast modulation. However, it is often difficult to recognize when the transition to lasing occurs, while the most important feature of laser radiation, i.e., coherence, is available only above the lasing threshold. Here we systematically study the second-order coherence properties of metal-semiconductor nanolasers at both low- and high-pump rates. We find the lasing threshold using a clear coherence definition and derive a simple expression for the threshold pump current (optical pump power), which can be applied to most thresholdless and non-thresholdless metal-semiconductor nanolasers.</abstract><cop>United States</cop><pmid>30645499</pmid><doi>10.1364/OE.26.033473</doi><tpages>11</tpages><orcidid>https://orcid.org/0000-0003-1394-4169</orcidid><orcidid>https://orcid.org/0000-0001-7264-0726</orcidid><oa>free_for_read</oa></addata></record> |
fulltext | fulltext |
identifier | ISSN: 1094-4087 |
ispartof | Optics express, 2018-12, Vol.26 (25), p.33473-33483 |
issn | 1094-4087 1094-4087 |
language | eng |
recordid | cdi_proquest_miscellaneous_2179391172 |
source | DOAJ Directory of Open Access Journals; Elektronische Zeitschriftenbibliothek - Frei zugängliche E-Journals; Alma/SFX Local Collection |
title | Lasing threshold of thresholdless and non-thresholdless metal-semiconductor nanolasers |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-06T10%3A56%3A21IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Lasing%20threshold%20of%20thresholdless%20and%20non-thresholdless%20metal-semiconductor%20nanolasers&rft.jtitle=Optics%20express&rft.au=Vyshnevyy,%20Andrey%20A&rft.date=2018-12-10&rft.volume=26&rft.issue=25&rft.spage=33473&rft.epage=33483&rft.pages=33473-33483&rft.issn=1094-4087&rft.eissn=1094-4087&rft_id=info:doi/10.1364/OE.26.033473&rft_dat=%3Cproquest_cross%3E2179391172%3C/proquest_cross%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=2179391172&rft_id=info:pmid/30645499&rfr_iscdi=true |