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High power (> 5 W) lambda similar to 9.6 mu m tapered quantum cascade lasers grown by OMVPE
AlInAs/GaInAs superlattices (SLs) with barrier and well layers of various thicknesses were grown by organometallic vapor phase epitaxy to optimize growth of quantum cascade lasers (QCLs). High-resolution x-ray diffraction data of nominally lattice-matched SLs show a systematic shift toward more comp...
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Published in: | Journal of crystal growth 2013-05, Vol.370, p.212-216 |
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container_title | Journal of crystal growth |
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creator | Wang, CA Goyal, A K Menzel, S Calawa, DR Spencer, M Connors, M K McNulty, D Sanchez, A Turner, G W Capasso, F |
description | AlInAs/GaInAs superlattices (SLs) with barrier and well layers of various thicknesses were grown by organometallic vapor phase epitaxy to optimize growth of quantum cascade lasers (QCLs). High-resolution x-ray diffraction data of nominally lattice-matched SLs show a systematic shift toward more compressively strained SLs as the barrier/well layer thicknesses are decreased below about 10 nm. This shift is attributed to In surface segregation in both AlInAs and GaInAs. This shift is compensated for in the growth of ultra-thin layers in QCL structures. QCLs with tapered gain regions and emitting at 9.6 mu m are demonstrated with peak power as high as 5.3 W from one facet at 20 degree C. |
doi_str_mv | 10.1016/j.jcrysgro.2012.11.045 |
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High-resolution x-ray diffraction data of nominally lattice-matched SLs show a systematic shift toward more compressively strained SLs as the barrier/well layer thicknesses are decreased below about 10 nm. This shift is attributed to In surface segregation in both AlInAs and GaInAs. This shift is compensated for in the growth of ultra-thin layers in QCL structures. QCLs with tapered gain regions and emitting at 9.6 mu m are demonstrated with peak power as high as 5.3 W from one facet at 20 degree C.</description><identifier>ISSN: 0022-0248</identifier><identifier>DOI: 10.1016/j.jcrysgro.2012.11.045</identifier><language>eng</language><subject>Barriers ; Crystal growth ; Diffraction ; Gain ; Phase shift ; Quantum cascade lasers ; Vapor phase epitaxy ; X-rays</subject><ispartof>Journal of crystal growth, 2013-05, Vol.370, p.212-216</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Wang, CA</creatorcontrib><creatorcontrib>Goyal, A K</creatorcontrib><creatorcontrib>Menzel, S</creatorcontrib><creatorcontrib>Calawa, DR</creatorcontrib><creatorcontrib>Spencer, M</creatorcontrib><creatorcontrib>Connors, M K</creatorcontrib><creatorcontrib>McNulty, D</creatorcontrib><creatorcontrib>Sanchez, A</creatorcontrib><creatorcontrib>Turner, G W</creatorcontrib><creatorcontrib>Capasso, F</creatorcontrib><title>High power (> 5 W) lambda similar to 9.6 mu m tapered quantum cascade lasers grown by OMVPE</title><title>Journal of crystal growth</title><description>AlInAs/GaInAs superlattices (SLs) with barrier and well layers of various thicknesses were grown by organometallic vapor phase epitaxy to optimize growth of quantum cascade lasers (QCLs). 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QCLs with tapered gain regions and emitting at 9.6 mu m are demonstrated with peak power as high as 5.3 W from one facet at 20 degree C.</description><subject>Barriers</subject><subject>Crystal growth</subject><subject>Diffraction</subject><subject>Gain</subject><subject>Phase shift</subject><subject>Quantum cascade lasers</subject><subject>Vapor phase epitaxy</subject><subject>X-rays</subject><issn>0022-0248</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><recordid>eNotjTtPwzAUhT2ARCn8BXTHMiTc6zixsyChqjykojLwGBgqO7ktqZImtRNV_fdEgumc4TvfEeKGMCak7G4X7wp_ClvfxhJJxkQxqvRMTBCljFAqcyEuQ9ghjjThRHw_V9sf6Noje5jdQwpft1DbxpUWQtVUtfXQt5DHGTQDNNDbjj2XcBjsvh8aKGwobMnjJLAPMP4e9-BOsHr9fFtcifONrQNf_-dUfDwu3ufP0XL19DJ_WEYdkekjli7dSOmkTjSypSQnRVqyMWyKUlOixp6VjjGTzulcU5qZwlkkk-iUMZmK2Z-38-1h4NCvmyoUXNd2z-0Q1qQylSqDOSa_8tlUbA</recordid><startdate>20130501</startdate><enddate>20130501</enddate><creator>Wang, CA</creator><creator>Goyal, A K</creator><creator>Menzel, S</creator><creator>Calawa, DR</creator><creator>Spencer, M</creator><creator>Connors, M K</creator><creator>McNulty, D</creator><creator>Sanchez, A</creator><creator>Turner, G W</creator><creator>Capasso, F</creator><scope>7SP</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20130501</creationdate><title>High power (> 5 W) lambda similar to 9.6 mu m tapered quantum cascade lasers grown by OMVPE</title><author>Wang, CA ; Goyal, A K ; Menzel, S ; Calawa, DR ; Spencer, M ; Connors, M K ; McNulty, D ; Sanchez, A ; Turner, G W ; Capasso, F</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p118t-e2b5f22b27370ea13914172e88e8cd71342e86dbe062bb7971568cba018375e03</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2013</creationdate><topic>Barriers</topic><topic>Crystal growth</topic><topic>Diffraction</topic><topic>Gain</topic><topic>Phase shift</topic><topic>Quantum cascade lasers</topic><topic>Vapor phase epitaxy</topic><topic>X-rays</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Wang, CA</creatorcontrib><creatorcontrib>Goyal, A K</creatorcontrib><creatorcontrib>Menzel, S</creatorcontrib><creatorcontrib>Calawa, DR</creatorcontrib><creatorcontrib>Spencer, M</creatorcontrib><creatorcontrib>Connors, M K</creatorcontrib><creatorcontrib>McNulty, D</creatorcontrib><creatorcontrib>Sanchez, A</creatorcontrib><creatorcontrib>Turner, G W</creatorcontrib><creatorcontrib>Capasso, F</creatorcontrib><collection>Electronics & Communications Abstracts</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of crystal growth</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Wang, CA</au><au>Goyal, A K</au><au>Menzel, S</au><au>Calawa, DR</au><au>Spencer, M</au><au>Connors, M K</au><au>McNulty, D</au><au>Sanchez, A</au><au>Turner, G W</au><au>Capasso, F</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>High power (> 5 W) lambda similar to 9.6 mu m tapered quantum cascade lasers grown by OMVPE</atitle><jtitle>Journal of crystal growth</jtitle><date>2013-05-01</date><risdate>2013</risdate><volume>370</volume><spage>212</spage><epage>216</epage><pages>212-216</pages><issn>0022-0248</issn><abstract>AlInAs/GaInAs superlattices (SLs) with barrier and well layers of various thicknesses were grown by organometallic vapor phase epitaxy to optimize growth of quantum cascade lasers (QCLs). High-resolution x-ray diffraction data of nominally lattice-matched SLs show a systematic shift toward more compressively strained SLs as the barrier/well layer thicknesses are decreased below about 10 nm. This shift is attributed to In surface segregation in both AlInAs and GaInAs. This shift is compensated for in the growth of ultra-thin layers in QCL structures. QCLs with tapered gain regions and emitting at 9.6 mu m are demonstrated with peak power as high as 5.3 W from one facet at 20 degree C.</abstract><doi>10.1016/j.jcrysgro.2012.11.045</doi><tpages>5</tpages></addata></record> |
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source | Elsevier |
subjects | Barriers Crystal growth Diffraction Gain Phase shift Quantum cascade lasers Vapor phase epitaxy X-rays |
title | High power (> 5 W) lambda similar to 9.6 mu m tapered quantum cascade lasers grown by OMVPE |
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