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Optimizing residual carriers in undoped InAs/GaSb superlattices for high operating temperature mid-infrared detectors
The mid-infrared 21 Å InAs/24 Å GaSb superlattices (SLs) designed for the 4 μm cutoff wavelength were grown by molecular beam epitaxy at growth temperatures between 370 and 430 °C in order to reduce residual background carriers. The lowest density of 1.8×10 11 cm −2 was obtained from the SLs grown a...
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Published in: | Journal of crystal growth 2009-03, Vol.311 (7), p.1897-1900 |
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container_end_page | 1900 |
container_issue | 7 |
container_start_page | 1897 |
container_title | Journal of crystal growth |
container_volume | 311 |
creator | Haugan, H.J. Elhamri, S. Ullrich, B. Szmulowicz, F. Brown, G.J. Mitchel, W.C. |
description | The mid-infrared 21
Å InAs/24
Å GaSb superlattices (SLs) designed for the 4
μm cutoff wavelength were grown by molecular beam epitaxy at growth temperatures between 370 and 430
°C in order to reduce residual background carriers. The lowest density of 1.8×10
11
cm
−2 was obtained from the SLs grown at 400
°C. With increasing growth temperature, in-plane hole mobility decreased from 8740 to 1400
cm
2/V
s due to increased interfacial roughness, while the photoluminescence (PL) intensity increased due to a decrease in the number of nonstoichiometric nonradiative defects. Further reduction of carrier density to 1×10
11
cm
−2 was achieved by increasing barrier width. As GaSb layer width increases from 24 to 48
Å, the cutoff wavelength decreased from 4.1 to 3.4
μm, which is still in the mid-infrared detection window. More importantly, a dramatic improvement on the PL intensity and the full width at half maximum was achieved from the SL samples with the wider GaSb widths. All mid-infrared SL samples investigated in our studies were residually p-type. |
doi_str_mv | 10.1016/j.jcrysgro.2008.09.141 |
format | article |
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Å InAs/24
Å GaSb superlattices (SLs) designed for the 4
μm cutoff wavelength were grown by molecular beam epitaxy at growth temperatures between 370 and 430
°C in order to reduce residual background carriers. The lowest density of 1.8×10
11
cm
−2 was obtained from the SLs grown at 400
°C. With increasing growth temperature, in-plane hole mobility decreased from 8740 to 1400
cm
2/V
s due to increased interfacial roughness, while the photoluminescence (PL) intensity increased due to a decrease in the number of nonstoichiometric nonradiative defects. Further reduction of carrier density to 1×10
11
cm
−2 was achieved by increasing barrier width. As GaSb layer width increases from 24 to 48
Å, the cutoff wavelength decreased from 4.1 to 3.4
μm, which is still in the mid-infrared detection window. More importantly, a dramatic improvement on the PL intensity and the full width at half maximum was achieved from the SL samples with the wider GaSb widths. All mid-infrared SL samples investigated in our studies were residually p-type.</description><identifier>ISSN: 0022-0248</identifier><identifier>EISSN: 1873-5002</identifier><identifier>DOI: 10.1016/j.jcrysgro.2008.09.141</identifier><identifier>CODEN: JCRGAE</identifier><language>eng</language><publisher>Amsterdam: Elsevier B.V</publisher><subject>A3. Molecular beam epitaxy ; A3. Superlattices ; B1. Antimonides ; B3. Infrared detector ; B3. Semiconductor devices ; Condensed matter: electronic structure, electrical, magnetic, and optical properties ; Cross-disciplinary physics: materials science; rheology ; Exact sciences and technology ; Materials science ; Methods of crystal growth; physics of crystal growth ; Methods of deposition of films and coatings; film growth and epitaxy ; Molecular, atomic, ion, and chemical beam epitaxy ; Optical properties and condensed-matter spectroscopy and other interactions of matter with particles and radiation ; Photoluminescence ; Physics ; Theory and models of crystal growth; physics of crystal growth, crystal morphology and orientation</subject><ispartof>Journal of crystal growth, 2009-03, Vol.311 (7), p.1897-1900</ispartof><rights>2008 Elsevier B.V.</rights><rights>2009 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c373t-97958deca635676716432920425448922dca7fd252a63f39f9bed85797cb31753</citedby><cites>FETCH-LOGICAL-c373t-97958deca635676716432920425448922dca7fd252a63f39f9bed85797cb31753</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>309,310,314,780,784,789,790,23930,23931,25140,27924,27925</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=21432543$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Haugan, H.J.</creatorcontrib><creatorcontrib>Elhamri, S.</creatorcontrib><creatorcontrib>Ullrich, B.</creatorcontrib><creatorcontrib>Szmulowicz, F.</creatorcontrib><creatorcontrib>Brown, G.J.</creatorcontrib><creatorcontrib>Mitchel, W.C.</creatorcontrib><title>Optimizing residual carriers in undoped InAs/GaSb superlattices for high operating temperature mid-infrared detectors</title><title>Journal of crystal growth</title><description>The mid-infrared 21
Å InAs/24
Å GaSb superlattices (SLs) designed for the 4
μm cutoff wavelength were grown by molecular beam epitaxy at growth temperatures between 370 and 430
°C in order to reduce residual background carriers. The lowest density of 1.8×10
11
cm
−2 was obtained from the SLs grown at 400
°C. With increasing growth temperature, in-plane hole mobility decreased from 8740 to 1400
cm
2/V
s due to increased interfacial roughness, while the photoluminescence (PL) intensity increased due to a decrease in the number of nonstoichiometric nonradiative defects. Further reduction of carrier density to 1×10
11
cm
−2 was achieved by increasing barrier width. As GaSb layer width increases from 24 to 48
Å, the cutoff wavelength decreased from 4.1 to 3.4
μm, which is still in the mid-infrared detection window. More importantly, a dramatic improvement on the PL intensity and the full width at half maximum was achieved from the SL samples with the wider GaSb widths. All mid-infrared SL samples investigated in our studies were residually p-type.</description><subject>A3. Molecular beam epitaxy</subject><subject>A3. Superlattices</subject><subject>B1. Antimonides</subject><subject>B3. Infrared detector</subject><subject>B3. Semiconductor devices</subject><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties</subject><subject>Cross-disciplinary physics: materials science; rheology</subject><subject>Exact sciences and technology</subject><subject>Materials science</subject><subject>Methods of crystal growth; physics of crystal growth</subject><subject>Methods of deposition of films and coatings; film growth and epitaxy</subject><subject>Molecular, atomic, ion, and chemical beam epitaxy</subject><subject>Optical properties and condensed-matter spectroscopy and other interactions of matter with particles and radiation</subject><subject>Photoluminescence</subject><subject>Physics</subject><subject>Theory and models of crystal growth; physics of crystal growth, crystal morphology and orientation</subject><issn>0022-0248</issn><issn>1873-5002</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2009</creationdate><recordtype>article</recordtype><recordid>eNqFkE1v1DAQhi0EEkvhLyBf4JbUX4njG1UFpVKlHoCz5bUnW6_yxUyCVH59vWzhysX24Xnf8TyMvZeilkK2l8f6GPGRDjjXSoiuFq6WRr5gO9lZXTVCqJdsV05VCWW61-wN0VGIkpRix7b7Zc1j_p2nA0egnLYw8BgQMyDxPPFtSvMCid9OV3R5E77tOW0L4BDWNUcg3s_IH_LhgRcKw3rqWWH8894Q-JhTlaceA5aOBCvEdUZ6y171YSB493xfsB9fPn-__lrd3d_cXl_dVVFbvVbOuqZLEEOrm9a2VrZGK6eEUY0xnVMqxWD7pBpViF673u0hdY11Nu61tI2-YB_PvQvOPzeg1Y-ZIgxDmGDeyGujpe6MK2B7BiPORAi9XzCPAR-9FP5k2R_9X8v-ZNkL54vlEvzwPCFQDENZdIqZ_qWVLD9ujC7cpzMHZd1fRa6nmGGKkDIWJz7N-X-jngAxZ5hN</recordid><startdate>20090315</startdate><enddate>20090315</enddate><creator>Haugan, H.J.</creator><creator>Elhamri, S.</creator><creator>Ullrich, B.</creator><creator>Szmulowicz, F.</creator><creator>Brown, G.J.</creator><creator>Mitchel, W.C.</creator><general>Elsevier B.V</general><general>Elsevier</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope></search><sort><creationdate>20090315</creationdate><title>Optimizing residual carriers in undoped InAs/GaSb superlattices for high operating temperature mid-infrared detectors</title><author>Haugan, H.J. ; Elhamri, S. ; Ullrich, B. ; Szmulowicz, F. ; Brown, G.J. ; Mitchel, W.C.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c373t-97958deca635676716432920425448922dca7fd252a63f39f9bed85797cb31753</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2009</creationdate><topic>A3. Molecular beam epitaxy</topic><topic>A3. Superlattices</topic><topic>B1. Antimonides</topic><topic>B3. Infrared detector</topic><topic>B3. Semiconductor devices</topic><topic>Condensed matter: electronic structure, electrical, magnetic, and optical properties</topic><topic>Cross-disciplinary physics: materials science; rheology</topic><topic>Exact sciences and technology</topic><topic>Materials science</topic><topic>Methods of crystal growth; physics of crystal growth</topic><topic>Methods of deposition of films and coatings; film growth and epitaxy</topic><topic>Molecular, atomic, ion, and chemical beam epitaxy</topic><topic>Optical properties and condensed-matter spectroscopy and other interactions of matter with particles and radiation</topic><topic>Photoluminescence</topic><topic>Physics</topic><topic>Theory and models of crystal growth; physics of crystal growth, crystal morphology and orientation</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Haugan, H.J.</creatorcontrib><creatorcontrib>Elhamri, S.</creatorcontrib><creatorcontrib>Ullrich, B.</creatorcontrib><creatorcontrib>Szmulowicz, F.</creatorcontrib><creatorcontrib>Brown, G.J.</creatorcontrib><creatorcontrib>Mitchel, W.C.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><jtitle>Journal of crystal growth</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Haugan, H.J.</au><au>Elhamri, S.</au><au>Ullrich, B.</au><au>Szmulowicz, F.</au><au>Brown, G.J.</au><au>Mitchel, W.C.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Optimizing residual carriers in undoped InAs/GaSb superlattices for high operating temperature mid-infrared detectors</atitle><jtitle>Journal of crystal growth</jtitle><date>2009-03-15</date><risdate>2009</risdate><volume>311</volume><issue>7</issue><spage>1897</spage><epage>1900</epage><pages>1897-1900</pages><issn>0022-0248</issn><eissn>1873-5002</eissn><coden>JCRGAE</coden><abstract>The mid-infrared 21
Å InAs/24
Å GaSb superlattices (SLs) designed for the 4
μm cutoff wavelength were grown by molecular beam epitaxy at growth temperatures between 370 and 430
°C in order to reduce residual background carriers. The lowest density of 1.8×10
11
cm
−2 was obtained from the SLs grown at 400
°C. With increasing growth temperature, in-plane hole mobility decreased from 8740 to 1400
cm
2/V
s due to increased interfacial roughness, while the photoluminescence (PL) intensity increased due to a decrease in the number of nonstoichiometric nonradiative defects. Further reduction of carrier density to 1×10
11
cm
−2 was achieved by increasing barrier width. As GaSb layer width increases from 24 to 48
Å, the cutoff wavelength decreased from 4.1 to 3.4
μm, which is still in the mid-infrared detection window. More importantly, a dramatic improvement on the PL intensity and the full width at half maximum was achieved from the SL samples with the wider GaSb widths. All mid-infrared SL samples investigated in our studies were residually p-type.</abstract><cop>Amsterdam</cop><pub>Elsevier B.V</pub><doi>10.1016/j.jcrysgro.2008.09.141</doi><tpages>4</tpages></addata></record> |
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subjects | A3. Molecular beam epitaxy A3. Superlattices B1. Antimonides B3. Infrared detector B3. Semiconductor devices Condensed matter: electronic structure, electrical, magnetic, and optical properties Cross-disciplinary physics: materials science rheology Exact sciences and technology Materials science Methods of crystal growth physics of crystal growth Methods of deposition of films and coatings film growth and epitaxy Molecular, atomic, ion, and chemical beam epitaxy Optical properties and condensed-matter spectroscopy and other interactions of matter with particles and radiation Photoluminescence Physics Theory and models of crystal growth physics of crystal growth, crystal morphology and orientation |
title | Optimizing residual carriers in undoped InAs/GaSb superlattices for high operating temperature mid-infrared detectors |
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