HgCdTe composition determination using spectroscopic ellipsometry during molecular beam epitaxy growth of near-infrared avalanche photodiode device structures
The application of spectroscopic ellipsometry (SE) for real-time composition determination during molecular beam epitaxy (MBE) growth of Hg^sub 1-x^Cd^sub x^Te alloys with x>0.5 is reported. Techniques previously developed for SE determination of composition in long-wavelength infrared (LWIR) HgC...
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description | The application of spectroscopic ellipsometry (SE) for real-time composition determination during molecular beam epitaxy (MBE) growth of Hg^sub 1-x^Cd^sub x^Te alloys with x>0.5 is reported. Techniques previously developed for SE determination of composition in long-wavelength infrared (LWIR) HgCdTe have been successfully extended to near-infrared HgCdTe avalanche photodiode (APD) device structures with x values in the range of 0.6-0.8. Ellipsometric data collected over a spectral range of 1.7-5 eV were used to measure depth profiles of HgCdTe alloy composition through the use of an optical model of the growth surface. The optical model used a dielectric-function database collected through the growth of a set of HgCdTe calibration samples with x ranging from 0.6 to 0.8. The sensitivity of this SE method of composition determination is estimated to be Δx 0.0002 at x=0.6, which is sufficiently low to sense composition changes arising from flux variations of less than 0.1%. Errors in composition determination because of Hg-flux variations appear to be inconsequential, while substrate-temperature fluctuations have been observed to alter the derived composition at a rate of -0.0004/°C. By comparing the composition inferred from SE and postgrowth 300 K IR transmission measurements on a set of APD device structures, the run-to-run precision of the Se-derived composition (at x=0.6) is estimated to be ±0.0012, which is equivalent to the precision achieved with the same instrumentation during the growth of mid-wavelength infrared (MWIR) HgCdTe alloys in the same MBE system.[PUBLICATION ABSTRACT] |
doi_str_mv | 10.1007/s11664-002-0220-6 |
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J ; OLSON, G. L ; ROTH, J. A ; JENSEN, J. E ; HUNTER, A. T ; JACK ; BAILEY, S. L</creator><creatorcontrib>DE LYON, T. J ; OLSON, G. L ; ROTH, J. A ; JENSEN, J. E ; HUNTER, A. T ; JACK ; BAILEY, S. L</creatorcontrib><description>The application of spectroscopic ellipsometry (SE) for real-time composition determination during molecular beam epitaxy (MBE) growth of Hg^sub 1-x^Cd^sub x^Te alloys with x>0.5 is reported. Techniques previously developed for SE determination of composition in long-wavelength infrared (LWIR) HgCdTe have been successfully extended to near-infrared HgCdTe avalanche photodiode (APD) device structures with x values in the range of 0.6-0.8. Ellipsometric data collected over a spectral range of 1.7-5 eV were used to measure depth profiles of HgCdTe alloy composition through the use of an optical model of the growth surface. The optical model used a dielectric-function database collected through the growth of a set of HgCdTe calibration samples with x ranging from 0.6 to 0.8. The sensitivity of this SE method of composition determination is estimated to be Δx 0.0002 at x=0.6, which is sufficiently low to sense composition changes arising from flux variations of less than 0.1%. Errors in composition determination because of Hg-flux variations appear to be inconsequential, while substrate-temperature fluctuations have been observed to alter the derived composition at a rate of -0.0004/°C. By comparing the composition inferred from SE and postgrowth 300 K IR transmission measurements on a set of APD device structures, the run-to-run precision of the Se-derived composition (at x=0.6) is estimated to be ±0.0012, which is equivalent to the precision achieved with the same instrumentation during the growth of mid-wavelength infrared (MWIR) HgCdTe alloys in the same MBE system.[PUBLICATION ABSTRACT]</description><identifier>ISSN: 0361-5235</identifier><identifier>EISSN: 1543-186X</identifier><identifier>DOI: 10.1007/s11664-002-0220-6</identifier><identifier>CODEN: JECMA5</identifier><language>eng</language><publisher>New York, NY: Institute of Electrical and Electronics Engineers</publisher><subject>Alloys ; Applied sciences ; Calibration ; Composition and phase identification ; Condensed matter: structure, mechanical and thermal properties ; Cross-disciplinary physics: materials science; rheology ; Electronics ; Exact sciences and technology ; Investigations ; Lasers ; Materials science ; Methods of deposition of films and coatings; film growth and epitaxy ; Molecular beam epitaxy ; Molecular, atomic, ion, and chemical beam epitaxy ; Optoelectronic devices ; Photodiodes; phototransistors; photoresistors ; Physics ; Radiation ; Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices ; Sensors ; Surfaces and interfaces; thin films and whiskers (structure and nonelectronic properties) ; Thin film structure and morphology</subject><ispartof>Journal of electronic materials, 2002-07, Vol.31 (7), p.688-693</ispartof><rights>2002 INIST-CNRS</rights><rights>TMS-The Minerals, Metals and Materials Society 2002</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c332t-2d8ba3a72d874854dbf9d60cc001443d37474c608e602b52cbce96e20cedccb43</citedby><cites>FETCH-LOGICAL-c332t-2d8ba3a72d874854dbf9d60cc001443d37474c608e602b52cbce96e20cedccb43</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=13830392$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>DE LYON, T. J</creatorcontrib><creatorcontrib>OLSON, G. L</creatorcontrib><creatorcontrib>ROTH, J. A</creatorcontrib><creatorcontrib>JENSEN, J. E</creatorcontrib><creatorcontrib>HUNTER, A. T</creatorcontrib><creatorcontrib>JACK</creatorcontrib><creatorcontrib>BAILEY, S. L</creatorcontrib><title>HgCdTe composition determination using spectroscopic ellipsometry during molecular beam epitaxy growth of near-infrared avalanche photodiode device structures</title><title>Journal of electronic materials</title><description>The application of spectroscopic ellipsometry (SE) for real-time composition determination during molecular beam epitaxy (MBE) growth of Hg^sub 1-x^Cd^sub x^Te alloys with x>0.5 is reported. Techniques previously developed for SE determination of composition in long-wavelength infrared (LWIR) HgCdTe have been successfully extended to near-infrared HgCdTe avalanche photodiode (APD) device structures with x values in the range of 0.6-0.8. Ellipsometric data collected over a spectral range of 1.7-5 eV were used to measure depth profiles of HgCdTe alloy composition through the use of an optical model of the growth surface. The optical model used a dielectric-function database collected through the growth of a set of HgCdTe calibration samples with x ranging from 0.6 to 0.8. The sensitivity of this SE method of composition determination is estimated to be Δx 0.0002 at x=0.6, which is sufficiently low to sense composition changes arising from flux variations of less than 0.1%. Errors in composition determination because of Hg-flux variations appear to be inconsequential, while substrate-temperature fluctuations have been observed to alter the derived composition at a rate of -0.0004/°C. By comparing the composition inferred from SE and postgrowth 300 K IR transmission measurements on a set of APD device structures, the run-to-run precision of the Se-derived composition (at x=0.6) is estimated to be ±0.0012, which is equivalent to the precision achieved with the same instrumentation during the growth of mid-wavelength infrared (MWIR) HgCdTe alloys in the same MBE system.[PUBLICATION ABSTRACT]</description><subject>Alloys</subject><subject>Applied sciences</subject><subject>Calibration</subject><subject>Composition and phase identification</subject><subject>Condensed matter: structure, mechanical and thermal properties</subject><subject>Cross-disciplinary physics: materials science; rheology</subject><subject>Electronics</subject><subject>Exact sciences and technology</subject><subject>Investigations</subject><subject>Lasers</subject><subject>Materials science</subject><subject>Methods of deposition of films and coatings; film growth and epitaxy</subject><subject>Molecular beam epitaxy</subject><subject>Molecular, atomic, ion, and chemical beam epitaxy</subject><subject>Optoelectronic devices</subject><subject>Photodiodes; phototransistors; photoresistors</subject><subject>Physics</subject><subject>Radiation</subject><subject>Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices</subject><subject>Sensors</subject><subject>Surfaces and interfaces; thin films and whiskers (structure and nonelectronic properties)</subject><subject>Thin film structure and morphology</subject><issn>0361-5235</issn><issn>1543-186X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2002</creationdate><recordtype>article</recordtype><sourceid>8G5</sourceid><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GNUQQ</sourceid><sourceid>GUQSH</sourceid><sourceid>M2O</sourceid><recordid>eNpdkc2KFDEUhYM4YDv6AO4CorvS_FUqvZTGmREG3Iwwu5C6udWdoapSJqnRfhmfddL2gODqcuG7P-ccQt5x9okz1n3OnGutGsZEw4RgjX5BNrxVsuFG378kGyY1b1oh21fkdc4PjPGWG74hf272O3-HFOK0xBxKiDP1WDBNYXZ_uzWHeU_zglBSzBCXABTHMSw5TljSkfo1nYgpjgjr6BLt0U0Ul1Dc7yPdp_irHGgc6IwuNWEekkvoqXt0o5vhgHQ5xBJ9iB7r5ccASHNJK5Q1YX5DLgY3Znz7XC_Jj6uvd7ub5vb79bfdl9sGpBSlEd70Trqu1k6ZVvl-2HrNAKpOpaSXneoUaGZQM9G3AnrArUbBAD1Ar-Ql-Xjeu6T4c8Vc7BQyVJluxrhmKzquDFOmgu__Ax_imub6m-XVU9EZqVml-JmCallOONglhcmlY4XsKS97zsvWvOwpL6vrzIfnzS6DG6tNM4T8b1AayeRWyCdiv5pe</recordid><startdate>20020701</startdate><enddate>20020701</enddate><creator>DE LYON, T. 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Microelectronics. Optoelectronics. Solid state devices</topic><topic>Sensors</topic><topic>Surfaces and interfaces; thin films and whiskers (structure and nonelectronic properties)</topic><topic>Thin film structure and morphology</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>DE LYON, T. J</creatorcontrib><creatorcontrib>OLSON, G. L</creatorcontrib><creatorcontrib>ROTH, J. A</creatorcontrib><creatorcontrib>JENSEN, J. E</creatorcontrib><creatorcontrib>HUNTER, A. T</creatorcontrib><creatorcontrib>JACK</creatorcontrib><creatorcontrib>BAILEY, S. 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J</au><au>OLSON, G. L</au><au>ROTH, J. A</au><au>JENSEN, J. E</au><au>HUNTER, A. T</au><au>JACK</au><au>BAILEY, S. L</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>HgCdTe composition determination using spectroscopic ellipsometry during molecular beam epitaxy growth of near-infrared avalanche photodiode device structures</atitle><jtitle>Journal of electronic materials</jtitle><date>2002-07-01</date><risdate>2002</risdate><volume>31</volume><issue>7</issue><spage>688</spage><epage>693</epage><pages>688-693</pages><issn>0361-5235</issn><eissn>1543-186X</eissn><coden>JECMA5</coden><abstract>The application of spectroscopic ellipsometry (SE) for real-time composition determination during molecular beam epitaxy (MBE) growth of Hg^sub 1-x^Cd^sub x^Te alloys with x>0.5 is reported. Techniques previously developed for SE determination of composition in long-wavelength infrared (LWIR) HgCdTe have been successfully extended to near-infrared HgCdTe avalanche photodiode (APD) device structures with x values in the range of 0.6-0.8. Ellipsometric data collected over a spectral range of 1.7-5 eV were used to measure depth profiles of HgCdTe alloy composition through the use of an optical model of the growth surface. The optical model used a dielectric-function database collected through the growth of a set of HgCdTe calibration samples with x ranging from 0.6 to 0.8. The sensitivity of this SE method of composition determination is estimated to be Δx 0.0002 at x=0.6, which is sufficiently low to sense composition changes arising from flux variations of less than 0.1%. Errors in composition determination because of Hg-flux variations appear to be inconsequential, while substrate-temperature fluctuations have been observed to alter the derived composition at a rate of -0.0004/°C. By comparing the composition inferred from SE and postgrowth 300 K IR transmission measurements on a set of APD device structures, the run-to-run precision of the Se-derived composition (at x=0.6) is estimated to be ±0.0012, which is equivalent to the precision achieved with the same instrumentation during the growth of mid-wavelength infrared (MWIR) HgCdTe alloys in the same MBE system.[PUBLICATION ABSTRACT]</abstract><cop>New York, NY</cop><pub>Institute of Electrical and Electronics Engineers</pub><doi>10.1007/s11664-002-0220-6</doi><tpages>6</tpages></addata></record> |
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subjects | Alloys Applied sciences Calibration Composition and phase identification Condensed matter: structure, mechanical and thermal properties Cross-disciplinary physics: materials science rheology Electronics Exact sciences and technology Investigations Lasers Materials science Methods of deposition of films and coatings film growth and epitaxy Molecular beam epitaxy Molecular, atomic, ion, and chemical beam epitaxy Optoelectronic devices Photodiodes phototransistors photoresistors Physics Radiation Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices Sensors Surfaces and interfaces thin films and whiskers (structure and nonelectronic properties) Thin film structure and morphology |
title | HgCdTe composition determination using spectroscopic ellipsometry during molecular beam epitaxy growth of near-infrared avalanche photodiode device structures |
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