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Trace copper measurements and electrical effects in LPE HgCdTe
Recent improvements in sputter initiated resonance ionization spectroscopy (SIRIS) have now made it possible to measure copper in HgCdTe films into the low 10^sup 13^ cm^sup -3^ range. We have used this technique to show that copper is responsible for type conversion in n-type HgCdTe films. Good n-t...
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Published in: | Journal of electronic materials 1996-08, Vol.25 (8), p.1183-1187 |
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creator | Tower, J P Tobin, S P Norton, P W Bollong, A B |
description | Recent improvements in sputter initiated resonance ionization spectroscopy (SIRIS) have now made it possible to measure copper in HgCdTe films into the low 10^sup 13^ cm^sup -3^ range. We have used this technique to show that copper is responsible for type conversion in n-type HgCdTe films. Good n-type LPE films were found to have less than 1 × 10^sup 14^ cm^sup -3^ copper, while converted p-type samples were found to have copper concentrations approximately equal to the hole concentrations. Some compensated n-type samples with low mobilities have copper concentrations too low to account for the amount of compensation and the presence of a deep acceptor level is suggested. In order to study diffusion of copper from substrates into LPE layers, a CdTe boule was grown intentionally spiked with copper at approximately 3 × 10^sup 16^ cm^sup -3^. Annealing HgCdTe films at 360°C was found to greatly increase the amount of copper that diffuses out of the substrates and a substrate screening technique was developed based on this phenomenon. SIRIS depth profiles showed much greater copper in HgCdTe films than in the substrates, indicating that copper is preferentially attracted to HgCdTe over Cd(Zn)Te. SIRIS spatial mapping showed that copper is concentrated in substrate tellurium inclusions 5-25 times greater than in the surrounding CdZnTe matrix. [PUBLICATION ABSTRACT] |
doi_str_mv | 10.1007/BF02655006 |
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We have used this technique to show that copper is responsible for type conversion in n-type HgCdTe films. Good n-type LPE films were found to have less than 1 × 10^sup 14^ cm^sup -3^ copper, while converted p-type samples were found to have copper concentrations approximately equal to the hole concentrations. Some compensated n-type samples with low mobilities have copper concentrations too low to account for the amount of compensation and the presence of a deep acceptor level is suggested. In order to study diffusion of copper from substrates into LPE layers, a CdTe boule was grown intentionally spiked with copper at approximately 3 × 10^sup 16^ cm^sup -3^. Annealing HgCdTe films at 360°C was found to greatly increase the amount of copper that diffuses out of the substrates and a substrate screening technique was developed based on this phenomenon. SIRIS depth profiles showed much greater copper in HgCdTe films than in the substrates, indicating that copper is preferentially attracted to HgCdTe over Cd(Zn)Te. SIRIS spatial mapping showed that copper is concentrated in substrate tellurium inclusions 5-25 times greater than in the surrounding CdZnTe matrix. [PUBLICATION ABSTRACT]</description><identifier>ISSN: 0361-5235</identifier><identifier>EISSN: 1543-186X</identifier><identifier>DOI: 10.1007/BF02655006</identifier><identifier>CODEN: JECMA5</identifier><language>eng</language><publisher>Warrendale: Springer Nature B.V</publisher><subject>Cadmium zinc telluride ; Copper ; Diffusion ; Mercury cadmium telluride ; Spectrum analysis ; Substrates</subject><ispartof>Journal of electronic materials, 1996-08, Vol.25 (8), p.1183-1187</ispartof><rights>Copyright Minerals, Metals & Materials Society Aug 1996</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c288t-ccbfc05d93896ff52624fcedbb7c3f8e17cf42c06aa12287fb26e11f35ed89b83</citedby><cites>FETCH-LOGICAL-c288t-ccbfc05d93896ff52624fcedbb7c3f8e17cf42c06aa12287fb26e11f35ed89b83</cites></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>Tower, J P</creatorcontrib><creatorcontrib>Tobin, S P</creatorcontrib><creatorcontrib>Norton, P W</creatorcontrib><creatorcontrib>Bollong, A B</creatorcontrib><title>Trace copper measurements and electrical effects in LPE HgCdTe</title><title>Journal of electronic materials</title><description>Recent improvements in sputter initiated resonance ionization spectroscopy (SIRIS) have now made it possible to measure copper in HgCdTe films into the low 10^sup 13^ cm^sup -3^ range. We have used this technique to show that copper is responsible for type conversion in n-type HgCdTe films. Good n-type LPE films were found to have less than 1 × 10^sup 14^ cm^sup -3^ copper, while converted p-type samples were found to have copper concentrations approximately equal to the hole concentrations. Some compensated n-type samples with low mobilities have copper concentrations too low to account for the amount of compensation and the presence of a deep acceptor level is suggested. In order to study diffusion of copper from substrates into LPE layers, a CdTe boule was grown intentionally spiked with copper at approximately 3 × 10^sup 16^ cm^sup -3^. Annealing HgCdTe films at 360°C was found to greatly increase the amount of copper that diffuses out of the substrates and a substrate screening technique was developed based on this phenomenon. SIRIS depth profiles showed much greater copper in HgCdTe films than in the substrates, indicating that copper is preferentially attracted to HgCdTe over Cd(Zn)Te. SIRIS spatial mapping showed that copper is concentrated in substrate tellurium inclusions 5-25 times greater than in the surrounding CdZnTe matrix. [PUBLICATION ABSTRACT]</description><subject>Cadmium zinc telluride</subject><subject>Copper</subject><subject>Diffusion</subject><subject>Mercury cadmium telluride</subject><subject>Spectrum analysis</subject><subject>Substrates</subject><issn>0361-5235</issn><issn>1543-186X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1996</creationdate><recordtype>article</recordtype><recordid>eNpdkM1KxDAYRYMoOI5ufILgRhCq-WnSdCPoMOMIBV2M4C6kX79Ih_6ZtAvf3soIgqt7F4fL5RByydktZyy7e9wwoZViTB-RBVepTLjR78dkwaTmiRJSnZKzGPeMccUNX5D7XXCAFPphwEBbdHEK2GI3Ruq6imKDMIYaXEPR-7lHWne0eF3T7ceq2uE5OfGuiXjxm0vytlnvVtukeHl6Xj0UCQhjxgSg9MBUlUuTa--V0CL1gFVZZiC9QZ6BTwUw7RwXwmS-FBo591JhZfLSyCW5PuwOof-cMI62rSNg07gO-ynaLJVKikyKmbz6R-77KXTzOStYalKjcjVDNwcIQh9jQG-HULcufFnO7I9I-ydSfgNge2P9</recordid><startdate>19960801</startdate><enddate>19960801</enddate><creator>Tower, J P</creator><creator>Tobin, S P</creator><creator>Norton, P W</creator><creator>Bollong, A B</creator><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>3V.</scope><scope>7XB</scope><scope>88I</scope><scope>8AF</scope><scope>8AO</scope><scope>8FE</scope><scope>8FG</scope><scope>8FK</scope><scope>8G5</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>D1I</scope><scope>DWQXO</scope><scope>GNUQQ</scope><scope>GUQSH</scope><scope>HCIFZ</scope><scope>KB.</scope><scope>L6V</scope><scope>M2O</scope><scope>M2P</scope><scope>M7S</scope><scope>MBDVC</scope><scope>P5Z</scope><scope>P62</scope><scope>PDBOC</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>Q9U</scope><scope>S0X</scope><scope>7QQ</scope><scope>7SP</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>19960801</creationdate><title>Trace copper measurements and electrical effects in LPE HgCdTe</title><author>Tower, J P ; 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We have used this technique to show that copper is responsible for type conversion in n-type HgCdTe films. Good n-type LPE films were found to have less than 1 × 10^sup 14^ cm^sup -3^ copper, while converted p-type samples were found to have copper concentrations approximately equal to the hole concentrations. Some compensated n-type samples with low mobilities have copper concentrations too low to account for the amount of compensation and the presence of a deep acceptor level is suggested. In order to study diffusion of copper from substrates into LPE layers, a CdTe boule was grown intentionally spiked with copper at approximately 3 × 10^sup 16^ cm^sup -3^. Annealing HgCdTe films at 360°C was found to greatly increase the amount of copper that diffuses out of the substrates and a substrate screening technique was developed based on this phenomenon. SIRIS depth profiles showed much greater copper in HgCdTe films than in the substrates, indicating that copper is preferentially attracted to HgCdTe over Cd(Zn)Te. SIRIS spatial mapping showed that copper is concentrated in substrate tellurium inclusions 5-25 times greater than in the surrounding CdZnTe matrix. [PUBLICATION ABSTRACT]</abstract><cop>Warrendale</cop><pub>Springer Nature B.V</pub><doi>10.1007/BF02655006</doi><tpages>5</tpages></addata></record> |
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subjects | Cadmium zinc telluride Copper Diffusion Mercury cadmium telluride Spectrum analysis Substrates |
title | Trace copper measurements and electrical effects in LPE HgCdTe |
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