Loading…

Fabry-Perot reflectance modulator for 1.3 μm from (InAlGa)As materials grown at low temperature

We report the first all-semiconductor Fabry–Perot-cavity reflectance modulators operating at wavelengths of 1.32–1.33 μm. These devices were grown on a GaAs substrate using an intermediate, linearly graded InGaAs buffer layer terminating in an In0.33Ga0.67As layer. The Bragg reflector stacks of the...

Full description

Saved in:
Bibliographic Details
Published in:Applied physics letters 1993-03, Vol.62 (9), p.919-921
Main Authors: FRITZ, I. J, HAMMONS, B. E, HOWARD, A. J, BRENNAN, T. M, OLSEN, J. A
Format: Article
Language:English
Subjects:
Citations: Items that this one cites
Items that cite this one
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
cited_by cdi_FETCH-LOGICAL-c254t-7231c7ee0f4374d16cef7a25b1f494a018e400adbddd2aab105e143d3c23e53f3
cites cdi_FETCH-LOGICAL-c254t-7231c7ee0f4374d16cef7a25b1f494a018e400adbddd2aab105e143d3c23e53f3
container_end_page 921
container_issue 9
container_start_page 919
container_title Applied physics letters
container_volume 62
creator FRITZ, I. J
HAMMONS, B. E
HOWARD, A. J
BRENNAN, T. M
OLSEN, J. A
description We report the first all-semiconductor Fabry–Perot-cavity reflectance modulators operating at wavelengths of 1.32–1.33 μm. These devices were grown on a GaAs substrate using an intermediate, linearly graded InGaAs buffer layer terminating in an In0.33Ga0.67As layer. The Bragg reflector stacks of the Fabry–Perot structure are composed of InGaAs and InAlAs layers lattice matched to the buffer, and the active cavity region is an In0.4Ga0.6As/In0.26Al0.35Ga0.39As strained-layer superlattice. The key to obtaining device-quality material was low temperature growth (∼400 °C) of the entire structure. For a device with a 0.38-μm-thick active region and a 4 dB insertion loss, we obtained a contrast ratio of ∼3:1 at 4 V bias.
doi_str_mv 10.1063/1.108519
format article
fullrecord <record><control><sourceid>pascalfrancis_cross</sourceid><recordid>TN_cdi_crossref_primary_10_1063_1_108519</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>4582525</sourcerecordid><originalsourceid>FETCH-LOGICAL-c254t-7231c7ee0f4374d16cef7a25b1f494a018e400adbddd2aab105e143d3c23e53f3</originalsourceid><addsrcrecordid>eNo9kM1KAzEUhYMoWKvgI2Thoi6m5uanM12WYmuhoAtdj3cyN1KZaUqSUvpuPoPPZKTi4nA43I8L5zB2C2IMYqIeIFtlYHrGBiDKslAA1TkbCCFUMZkauGRXMX7maKRSA_a-wCYcixcKPvFAriObcGuJ977dd5h84C4Lxop_f_XcBd_z0Wo765Z4P4u8x0Rhg13kH8EfthwT7_yBJ-p3FDDtA12zC5fvdPPnQ_a2eHydPxXr5-VqPlsXVhqdilIqsCWRcFqVuoWJJVeiNA04PdUooCItBLZN27YSsQFhCLRqlZWKjHJqyEanvzb4GHOTehc2PYZjDaL-XaaG-rRMRu9O6A6jxc6FXHgT_3ltKmmkUT8XBGLG</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Fabry-Perot reflectance modulator for 1.3 μm from (InAlGa)As materials grown at low temperature</title><source>AIP Digital Archive</source><creator>FRITZ, I. J ; HAMMONS, B. E ; HOWARD, A. J ; BRENNAN, T. M ; OLSEN, J. A</creator><creatorcontrib>FRITZ, I. J ; HAMMONS, B. E ; HOWARD, A. J ; BRENNAN, T. M ; OLSEN, J. A</creatorcontrib><description>We report the first all-semiconductor Fabry–Perot-cavity reflectance modulators operating at wavelengths of 1.32–1.33 μm. These devices were grown on a GaAs substrate using an intermediate, linearly graded InGaAs buffer layer terminating in an In0.33Ga0.67As layer. The Bragg reflector stacks of the Fabry–Perot structure are composed of InGaAs and InAlAs layers lattice matched to the buffer, and the active cavity region is an In0.4Ga0.6As/In0.26Al0.35Ga0.39As strained-layer superlattice. The key to obtaining device-quality material was low temperature growth (∼400 °C) of the entire structure. For a device with a 0.38-μm-thick active region and a 4 dB insertion loss, we obtained a contrast ratio of ∼3:1 at 4 V bias.</description><identifier>ISSN: 0003-6951</identifier><identifier>EISSN: 1077-3118</identifier><identifier>DOI: 10.1063/1.108519</identifier><identifier>CODEN: APPLAB</identifier><language>eng</language><publisher>Melville, NY: American Institute of Physics</publisher><subject>Exact sciences and technology ; Fundamental areas of phenomenology (including applications) ; Optical elements, devices, and systems ; Optical processors, correlators, and modulators ; Optics ; Physics</subject><ispartof>Applied physics letters, 1993-03, Vol.62 (9), p.919-921</ispartof><rights>1993 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c254t-7231c7ee0f4374d16cef7a25b1f494a018e400adbddd2aab105e143d3c23e53f3</citedby><cites>FETCH-LOGICAL-c254t-7231c7ee0f4374d16cef7a25b1f494a018e400adbddd2aab105e143d3c23e53f3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27903,27904</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&amp;idt=4582525$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>FRITZ, I. J</creatorcontrib><creatorcontrib>HAMMONS, B. E</creatorcontrib><creatorcontrib>HOWARD, A. J</creatorcontrib><creatorcontrib>BRENNAN, T. M</creatorcontrib><creatorcontrib>OLSEN, J. A</creatorcontrib><title>Fabry-Perot reflectance modulator for 1.3 μm from (InAlGa)As materials grown at low temperature</title><title>Applied physics letters</title><description>We report the first all-semiconductor Fabry–Perot-cavity reflectance modulators operating at wavelengths of 1.32–1.33 μm. These devices were grown on a GaAs substrate using an intermediate, linearly graded InGaAs buffer layer terminating in an In0.33Ga0.67As layer. The Bragg reflector stacks of the Fabry–Perot structure are composed of InGaAs and InAlAs layers lattice matched to the buffer, and the active cavity region is an In0.4Ga0.6As/In0.26Al0.35Ga0.39As strained-layer superlattice. The key to obtaining device-quality material was low temperature growth (∼400 °C) of the entire structure. For a device with a 0.38-μm-thick active region and a 4 dB insertion loss, we obtained a contrast ratio of ∼3:1 at 4 V bias.</description><subject>Exact sciences and technology</subject><subject>Fundamental areas of phenomenology (including applications)</subject><subject>Optical elements, devices, and systems</subject><subject>Optical processors, correlators, and modulators</subject><subject>Optics</subject><subject>Physics</subject><issn>0003-6951</issn><issn>1077-3118</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1993</creationdate><recordtype>article</recordtype><recordid>eNo9kM1KAzEUhYMoWKvgI2Thoi6m5uanM12WYmuhoAtdj3cyN1KZaUqSUvpuPoPPZKTi4nA43I8L5zB2C2IMYqIeIFtlYHrGBiDKslAA1TkbCCFUMZkauGRXMX7maKRSA_a-wCYcixcKPvFAriObcGuJ977dd5h84C4Lxop_f_XcBd_z0Wo765Z4P4u8x0Rhg13kH8EfthwT7_yBJ-p3FDDtA12zC5fvdPPnQ_a2eHydPxXr5-VqPlsXVhqdilIqsCWRcFqVuoWJJVeiNA04PdUooCItBLZN27YSsQFhCLRqlZWKjHJqyEanvzb4GHOTehc2PYZjDaL-XaaG-rRMRu9O6A6jxc6FXHgT_3ltKmmkUT8XBGLG</recordid><startdate>19930301</startdate><enddate>19930301</enddate><creator>FRITZ, I. J</creator><creator>HAMMONS, B. E</creator><creator>HOWARD, A. J</creator><creator>BRENNAN, T. M</creator><creator>OLSEN, J. A</creator><general>American Institute of Physics</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>19930301</creationdate><title>Fabry-Perot reflectance modulator for 1.3 μm from (InAlGa)As materials grown at low temperature</title><author>FRITZ, I. J ; HAMMONS, B. E ; HOWARD, A. J ; BRENNAN, T. M ; OLSEN, J. A</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c254t-7231c7ee0f4374d16cef7a25b1f494a018e400adbddd2aab105e143d3c23e53f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1993</creationdate><topic>Exact sciences and technology</topic><topic>Fundamental areas of phenomenology (including applications)</topic><topic>Optical elements, devices, and systems</topic><topic>Optical processors, correlators, and modulators</topic><topic>Optics</topic><topic>Physics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>FRITZ, I. J</creatorcontrib><creatorcontrib>HAMMONS, B. E</creatorcontrib><creatorcontrib>HOWARD, A. J</creatorcontrib><creatorcontrib>BRENNAN, T. M</creatorcontrib><creatorcontrib>OLSEN, J. A</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><jtitle>Applied physics letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>FRITZ, I. J</au><au>HAMMONS, B. E</au><au>HOWARD, A. J</au><au>BRENNAN, T. M</au><au>OLSEN, J. A</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Fabry-Perot reflectance modulator for 1.3 μm from (InAlGa)As materials grown at low temperature</atitle><jtitle>Applied physics letters</jtitle><date>1993-03-01</date><risdate>1993</risdate><volume>62</volume><issue>9</issue><spage>919</spage><epage>921</epage><pages>919-921</pages><issn>0003-6951</issn><eissn>1077-3118</eissn><coden>APPLAB</coden><abstract>We report the first all-semiconductor Fabry–Perot-cavity reflectance modulators operating at wavelengths of 1.32–1.33 μm. These devices were grown on a GaAs substrate using an intermediate, linearly graded InGaAs buffer layer terminating in an In0.33Ga0.67As layer. The Bragg reflector stacks of the Fabry–Perot structure are composed of InGaAs and InAlAs layers lattice matched to the buffer, and the active cavity region is an In0.4Ga0.6As/In0.26Al0.35Ga0.39As strained-layer superlattice. The key to obtaining device-quality material was low temperature growth (∼400 °C) of the entire structure. For a device with a 0.38-μm-thick active region and a 4 dB insertion loss, we obtained a contrast ratio of ∼3:1 at 4 V bias.</abstract><cop>Melville, NY</cop><pub>American Institute of Physics</pub><doi>10.1063/1.108519</doi><tpages>3</tpages></addata></record>
fulltext fulltext
identifier ISSN: 0003-6951
ispartof Applied physics letters, 1993-03, Vol.62 (9), p.919-921
issn 0003-6951
1077-3118
language eng
recordid cdi_crossref_primary_10_1063_1_108519
source AIP Digital Archive
subjects Exact sciences and technology
Fundamental areas of phenomenology (including applications)
Optical elements, devices, and systems
Optical processors, correlators, and modulators
Optics
Physics
title Fabry-Perot reflectance modulator for 1.3 μm from (InAlGa)As materials grown at low temperature
url http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-25T23%3A15%3A00IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-pascalfrancis_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Fabry-Perot%20reflectance%20modulator%20for%201.3%20%CE%BCm%20from%20(InAlGa)As%20materials%20grown%20at%20low%20temperature&rft.jtitle=Applied%20physics%20letters&rft.au=FRITZ,%20I.%20J&rft.date=1993-03-01&rft.volume=62&rft.issue=9&rft.spage=919&rft.epage=921&rft.pages=919-921&rft.issn=0003-6951&rft.eissn=1077-3118&rft.coden=APPLAB&rft_id=info:doi/10.1063/1.108519&rft_dat=%3Cpascalfrancis_cross%3E4582525%3C/pascalfrancis_cross%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-c254t-7231c7ee0f4374d16cef7a25b1f494a018e400adbddd2aab105e143d3c23e53f3%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_id=info:pmid/&rfr_iscdi=true