Black phosphorus frequency mixer for infrared optoelectronic signal processing

Black phosphorus possesses several attractive properties for optoelectronics, notably a direct and layer dependent bandgap that varies from the visible to mid-infrared and the ability to transfer the material to nearly arbitrary substrates. A less utilized property of black phosphorus for optoelectr...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:APL photonics 2019-03, Vol.4 (3), p.034502-034502-6
Hauptverfasser: Suess, Ryan J., Hart, Joseph D., Leong, Edward, Mittendorff, Martin, Murphy, Thomas E.
Format: Artikel
Sprache:eng
Online-Zugang:Volltext
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
container_end_page 034502-6
container_issue 3
container_start_page 034502
container_title APL photonics
container_volume 4
creator Suess, Ryan J.
Hart, Joseph D.
Leong, Edward
Mittendorff, Martin
Murphy, Thomas E.
description Black phosphorus possesses several attractive properties for optoelectronics, notably a direct and layer dependent bandgap that varies from the visible to mid-infrared and the ability to transfer the material to nearly arbitrary substrates. A less utilized property of black phosphorus for optoelectronics is the nonlinear photoresponse. The photocarrier lifetime in black phosphorus exhibits a strong nonlinear dependence on the excitation density that is utilized in the present work for optoelectronic mixing. In this scheme, two telecommunications-band lasers are intensity-modulated by a radio frequency (RF) and local oscillator (LO) frequency and focused onto a black phosphorus photoconductive detector. Above the saturation carrier density, the photocurrent is proportional to the square root of the optical power which produces photocurrents at the sum and difference frequencies of the input beams. The bandwidth of the mixing process increases from 10 to 100 MHz for incident powers of 0.01 to 1 mW, respectively. An excess carrier model accurately describes the power dependence of the cutoff frequency and mixing conversion, which are both limited by photocarrier recombination. Optimizing our device geometry to support larger bias fields and decreased carrier transit times could increase the maximum RF/LO frequency beyond a GHz by reducing the excess carrier lifetime. Frequency mixing based on the photocarrier nonlinearity in multilayer black phosphorus demonstrated here can be readily extended to mid-infrared wavelengths as long as 4 µm.
doi_str_mv 10.1063/1.5046732
format Article
fullrecord <record><control><sourceid>scitation_cross</sourceid><recordid>TN_cdi_crossref_primary_10_1063_1_5046732</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><doaj_id>oai_doaj_org_article_21f94cd08d744bb38b3ee1d152f289f2</doaj_id><sourcerecordid>app</sourcerecordid><originalsourceid>FETCH-LOGICAL-c400t-2c3ad93c38124bb1ea18729286417f27ed544310f81cc194b0e5afc0593eb043</originalsourceid><addsrcrecordid>eNqdkE1LAzEQhoMoWLQH_0GuCq2ZJLvJHrX4USh66T1k81FTt5s12Yr99662qGcPwwzDwzPDi9AFkCmQkl3DtCC8FIweoRFlQk5IVYrjP_MpGue8JoRAKaDixQg93TbavOLuJeah0jZjn9zb1rVmhzfhwyXsY8Kh9UknZ3Hs-ugaZ_oU22BwDqtWN7hL0bicQ7s6RydeN9mND_0MLe_vlrPHyeL5YT67WUwMJ6SfUMO0rZhhEiiva3AapKAVlSUH4alwtuCcAfESjBkerYkrtDekqJirCWdnaL7X2qjXqktho9NORR3U9yKmldKpD6ZxioKvuLFEWsGHU0zWzDmwUFBPZeXp4Lrcu0yKOSfnf3xA1FesCtQh1oG92rPZhF73Ibb_g99j-gVVZz37BKpMhjU</addsrcrecordid><sourcetype>Open Website</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Black phosphorus frequency mixer for infrared optoelectronic signal processing</title><source>DOAJ Directory of Open Access Journals</source><source>EZB-FREE-00999 freely available EZB journals</source><creator>Suess, Ryan J. ; Hart, Joseph D. ; Leong, Edward ; Mittendorff, Martin ; Murphy, Thomas E.</creator><creatorcontrib>Suess, Ryan J. ; Hart, Joseph D. ; Leong, Edward ; Mittendorff, Martin ; Murphy, Thomas E.</creatorcontrib><description>Black phosphorus possesses several attractive properties for optoelectronics, notably a direct and layer dependent bandgap that varies from the visible to mid-infrared and the ability to transfer the material to nearly arbitrary substrates. A less utilized property of black phosphorus for optoelectronics is the nonlinear photoresponse. The photocarrier lifetime in black phosphorus exhibits a strong nonlinear dependence on the excitation density that is utilized in the present work for optoelectronic mixing. In this scheme, two telecommunications-band lasers are intensity-modulated by a radio frequency (RF) and local oscillator (LO) frequency and focused onto a black phosphorus photoconductive detector. Above the saturation carrier density, the photocurrent is proportional to the square root of the optical power which produces photocurrents at the sum and difference frequencies of the input beams. The bandwidth of the mixing process increases from 10 to 100 MHz for incident powers of 0.01 to 1 mW, respectively. An excess carrier model accurately describes the power dependence of the cutoff frequency and mixing conversion, which are both limited by photocarrier recombination. Optimizing our device geometry to support larger bias fields and decreased carrier transit times could increase the maximum RF/LO frequency beyond a GHz by reducing the excess carrier lifetime. Frequency mixing based on the photocarrier nonlinearity in multilayer black phosphorus demonstrated here can be readily extended to mid-infrared wavelengths as long as 4 µm.</description><identifier>ISSN: 2378-0967</identifier><identifier>EISSN: 2378-0967</identifier><identifier>DOI: 10.1063/1.5046732</identifier><identifier>CODEN: APPHD2</identifier><language>eng</language><publisher>AIP Publishing LLC</publisher><ispartof>APL photonics, 2019-03, Vol.4 (3), p.034502-034502-6</ispartof><rights>Author(s)</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c400t-2c3ad93c38124bb1ea18729286417f27ed544310f81cc194b0e5afc0593eb043</citedby><cites>FETCH-LOGICAL-c400t-2c3ad93c38124bb1ea18729286417f27ed544310f81cc194b0e5afc0593eb043</cites><orcidid>0000-0002-8286-3832 ; 0000-0003-3998-2518 ; 0000-0003-1516-9186 ; 0000-0002-9396-0574</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,864,2102,27924,27925</link.rule.ids></links><search><creatorcontrib>Suess, Ryan J.</creatorcontrib><creatorcontrib>Hart, Joseph D.</creatorcontrib><creatorcontrib>Leong, Edward</creatorcontrib><creatorcontrib>Mittendorff, Martin</creatorcontrib><creatorcontrib>Murphy, Thomas E.</creatorcontrib><title>Black phosphorus frequency mixer for infrared optoelectronic signal processing</title><title>APL photonics</title><description>Black phosphorus possesses several attractive properties for optoelectronics, notably a direct and layer dependent bandgap that varies from the visible to mid-infrared and the ability to transfer the material to nearly arbitrary substrates. A less utilized property of black phosphorus for optoelectronics is the nonlinear photoresponse. The photocarrier lifetime in black phosphorus exhibits a strong nonlinear dependence on the excitation density that is utilized in the present work for optoelectronic mixing. In this scheme, two telecommunications-band lasers are intensity-modulated by a radio frequency (RF) and local oscillator (LO) frequency and focused onto a black phosphorus photoconductive detector. Above the saturation carrier density, the photocurrent is proportional to the square root of the optical power which produces photocurrents at the sum and difference frequencies of the input beams. The bandwidth of the mixing process increases from 10 to 100 MHz for incident powers of 0.01 to 1 mW, respectively. An excess carrier model accurately describes the power dependence of the cutoff frequency and mixing conversion, which are both limited by photocarrier recombination. Optimizing our device geometry to support larger bias fields and decreased carrier transit times could increase the maximum RF/LO frequency beyond a GHz by reducing the excess carrier lifetime. Frequency mixing based on the photocarrier nonlinearity in multilayer black phosphorus demonstrated here can be readily extended to mid-infrared wavelengths as long as 4 µm.</description><issn>2378-0967</issn><issn>2378-0967</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><sourceid>DOA</sourceid><recordid>eNqdkE1LAzEQhoMoWLQH_0GuCq2ZJLvJHrX4USh66T1k81FTt5s12Yr99662qGcPwwzDwzPDi9AFkCmQkl3DtCC8FIweoRFlQk5IVYrjP_MpGue8JoRAKaDixQg93TbavOLuJeah0jZjn9zb1rVmhzfhwyXsY8Kh9UknZ3Hs-ugaZ_oU22BwDqtWN7hL0bicQ7s6RydeN9mND_0MLe_vlrPHyeL5YT67WUwMJ6SfUMO0rZhhEiiva3AapKAVlSUH4alwtuCcAfESjBkerYkrtDekqJirCWdnaL7X2qjXqktho9NORR3U9yKmldKpD6ZxioKvuLFEWsGHU0zWzDmwUFBPZeXp4Lrcu0yKOSfnf3xA1FesCtQh1oG92rPZhF73Ibb_g99j-gVVZz37BKpMhjU</recordid><startdate>20190301</startdate><enddate>20190301</enddate><creator>Suess, Ryan J.</creator><creator>Hart, Joseph D.</creator><creator>Leong, Edward</creator><creator>Mittendorff, Martin</creator><creator>Murphy, Thomas E.</creator><general>AIP Publishing LLC</general><scope>AJDQP</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>DOA</scope><orcidid>https://orcid.org/0000-0002-8286-3832</orcidid><orcidid>https://orcid.org/0000-0003-3998-2518</orcidid><orcidid>https://orcid.org/0000-0003-1516-9186</orcidid><orcidid>https://orcid.org/0000-0002-9396-0574</orcidid></search><sort><creationdate>20190301</creationdate><title>Black phosphorus frequency mixer for infrared optoelectronic signal processing</title><author>Suess, Ryan J. ; Hart, Joseph D. ; Leong, Edward ; Mittendorff, Martin ; Murphy, Thomas E.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c400t-2c3ad93c38124bb1ea18729286417f27ed544310f81cc194b0e5afc0593eb043</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Suess, Ryan J.</creatorcontrib><creatorcontrib>Hart, Joseph D.</creatorcontrib><creatorcontrib>Leong, Edward</creatorcontrib><creatorcontrib>Mittendorff, Martin</creatorcontrib><creatorcontrib>Murphy, Thomas E.</creatorcontrib><collection>AIP Open Access Journals</collection><collection>CrossRef</collection><collection>DOAJ Directory of Open Access Journals</collection><jtitle>APL photonics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Suess, Ryan J.</au><au>Hart, Joseph D.</au><au>Leong, Edward</au><au>Mittendorff, Martin</au><au>Murphy, Thomas E.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Black phosphorus frequency mixer for infrared optoelectronic signal processing</atitle><jtitle>APL photonics</jtitle><date>2019-03-01</date><risdate>2019</risdate><volume>4</volume><issue>3</issue><spage>034502</spage><epage>034502-6</epage><pages>034502-034502-6</pages><issn>2378-0967</issn><eissn>2378-0967</eissn><coden>APPHD2</coden><abstract>Black phosphorus possesses several attractive properties for optoelectronics, notably a direct and layer dependent bandgap that varies from the visible to mid-infrared and the ability to transfer the material to nearly arbitrary substrates. A less utilized property of black phosphorus for optoelectronics is the nonlinear photoresponse. The photocarrier lifetime in black phosphorus exhibits a strong nonlinear dependence on the excitation density that is utilized in the present work for optoelectronic mixing. In this scheme, two telecommunications-band lasers are intensity-modulated by a radio frequency (RF) and local oscillator (LO) frequency and focused onto a black phosphorus photoconductive detector. Above the saturation carrier density, the photocurrent is proportional to the square root of the optical power which produces photocurrents at the sum and difference frequencies of the input beams. The bandwidth of the mixing process increases from 10 to 100 MHz for incident powers of 0.01 to 1 mW, respectively. An excess carrier model accurately describes the power dependence of the cutoff frequency and mixing conversion, which are both limited by photocarrier recombination. Optimizing our device geometry to support larger bias fields and decreased carrier transit times could increase the maximum RF/LO frequency beyond a GHz by reducing the excess carrier lifetime. Frequency mixing based on the photocarrier nonlinearity in multilayer black phosphorus demonstrated here can be readily extended to mid-infrared wavelengths as long as 4 µm.</abstract><pub>AIP Publishing LLC</pub><doi>10.1063/1.5046732</doi><tpages>6</tpages><orcidid>https://orcid.org/0000-0002-8286-3832</orcidid><orcidid>https://orcid.org/0000-0003-3998-2518</orcidid><orcidid>https://orcid.org/0000-0003-1516-9186</orcidid><orcidid>https://orcid.org/0000-0002-9396-0574</orcidid><oa>free_for_read</oa></addata></record>
fulltext fulltext
identifier ISSN: 2378-0967
ispartof APL photonics, 2019-03, Vol.4 (3), p.034502-034502-6
issn 2378-0967
2378-0967
language eng
recordid cdi_crossref_primary_10_1063_1_5046732
source DOAJ Directory of Open Access Journals; EZB-FREE-00999 freely available EZB journals
title Black phosphorus frequency mixer for infrared optoelectronic signal processing
url https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2024-12-28T16%3A19%3A29IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-scitation_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Black%20phosphorus%20frequency%20mixer%20for%20infrared%20optoelectronic%20signal%20processing&rft.jtitle=APL%20photonics&rft.au=Suess,%20Ryan%20J.&rft.date=2019-03-01&rft.volume=4&rft.issue=3&rft.spage=034502&rft.epage=034502-6&rft.pages=034502-034502-6&rft.issn=2378-0967&rft.eissn=2378-0967&rft.coden=APPHD2&rft_id=info:doi/10.1063/1.5046732&rft_dat=%3Cscitation_cross%3Eapp%3C/scitation_cross%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_id=info:pmid/&rft_doaj_id=oai_doaj_org_article_21f94cd08d744bb38b3ee1d152f289f2&rfr_iscdi=true