Redistribution of chromium under annealed sulfur implants into chromium-doped GaAs
The effect of sulfur implant fluence, ion energy, and annealing temperature on the redistribution accumulation of chromium during annealing of GaAs under SiO2 and Si3N4 caps and a capless condition is shown. The variation of the thickness of the heavily damaged or ‘‘amorphized’’ layer with implant f...
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Veröffentlicht in: | Journal of applied physics 1983-01, Vol.54 (12), p.6868-6874 |
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creator | WILSON, R. G EVANS, C. A. JR NORBERG, J. C HOPKINS, C. G PARK, Y. S |
description | The effect of sulfur implant fluence, ion energy, and annealing temperature on the redistribution accumulation of chromium during annealing of GaAs under SiO2 and Si3N4 caps and a capless condition is shown. The variation of the thickness of the heavily damaged or ‘‘amorphized’’ layer with implant fluence is shown and discussed. Three peaks are seen in the Cr accumulation profiles. When their integrated densities are plotted versus inverse annealing temperature, two peaks exhibit an activation energy for breakup of the Cr-defect complexes of 0.56 eV, and the third, of 1.8 eV. The nature or origin of these Cr-defect complexes is discussed. Sulfur migration or ‘‘diffusion’’ versus sulfur density is illustrated and discussed. The correlations of the two Cr peaks observed in 840 °C annealed depth distributions with capping environment and damage depth are discussed. Finally, these Cr accumulation profiles under sulfur implants are compared with those in self-amorphized GaAs. |
doi_str_mv | 10.1063/1.331991 |
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The correlations of the two Cr peaks observed in 840 °C annealed depth distributions with capping environment and damage depth are discussed. Finally, these Cr accumulation profiles under sulfur implants are compared with those in self-amorphized GaAs.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/1.331991</identifier><identifier>CODEN: JAPIAU</identifier><language>eng</language><publisher>Woodbury, NY: American Institute of Physics</publisher><subject>Condensed matter: structure, mechanical and thermal properties ; Defects and impurities in crystals; microstructure ; Exact sciences and technology ; Impurities: concentration, distribution, and gradients ; Physics ; Structure of solids and liquids; crystallography</subject><ispartof>Journal of applied physics, 1983-01, Vol.54 (12), p.6868-6874</ispartof><rights>1984 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c254t-57adc42874e2b1cf80f16f9bab2827c3ee2141c675885e20f639d98f9d5318e3</citedby><cites>FETCH-LOGICAL-c254t-57adc42874e2b1cf80f16f9bab2827c3ee2141c675885e20f639d98f9d5318e3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=9491528$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>WILSON, R. 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Sulfur migration or ‘‘diffusion’’ versus sulfur density is illustrated and discussed. The correlations of the two Cr peaks observed in 840 °C annealed depth distributions with capping environment and damage depth are discussed. Finally, these Cr accumulation profiles under sulfur implants are compared with those in self-amorphized GaAs.</description><subject>Condensed matter: structure, mechanical and thermal properties</subject><subject>Defects and impurities in crystals; microstructure</subject><subject>Exact sciences and technology</subject><subject>Impurities: concentration, distribution, and gradients</subject><subject>Physics</subject><subject>Structure of solids and liquids; crystallography</subject><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1983</creationdate><recordtype>article</recordtype><recordid>eNo90E9LwzAcxvEgCtYp-BJy8OAlM7-kaZLjGDqFgTB2L2n-YKRNS9IefPdOJjs9lw_P4YvQI9A10Ia_wJpz0BquUAVUaSKFoNeoopQBUVrqW3RXyjelAIrrCh0O3sUy59gtcxwTHgO2X3kc4jLgJTmfsUnJm947XJY-LBnHYepNmguOaR4vmLhxOpmd2ZR7dBNMX_zD_67Q8e31uH0n-8_dx3azJ5aJeiZCGmdrpmTtWQc2KBqgCbozHVNMWu49gxpsI4VSwjMaGq6dVkE7wUF5vkLP51ubx1KyD-2U42DyTwu0_UvRQntOcaJPZzqZYk0fskk2lovXtQbBFP8FkWVd6A</recordid><startdate>19830101</startdate><enddate>19830101</enddate><creator>WILSON, R. 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The variation of the thickness of the heavily damaged or ‘‘amorphized’’ layer with implant fluence is shown and discussed. Three peaks are seen in the Cr accumulation profiles. When their integrated densities are plotted versus inverse annealing temperature, two peaks exhibit an activation energy for breakup of the Cr-defect complexes of 0.56 eV, and the third, of 1.8 eV. The nature or origin of these Cr-defect complexes is discussed. Sulfur migration or ‘‘diffusion’’ versus sulfur density is illustrated and discussed. The correlations of the two Cr peaks observed in 840 °C annealed depth distributions with capping environment and damage depth are discussed. Finally, these Cr accumulation profiles under sulfur implants are compared with those in self-amorphized GaAs.</abstract><cop>Woodbury, NY</cop><pub>American Institute of Physics</pub><doi>10.1063/1.331991</doi><tpages>7</tpages></addata></record> |
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subjects | Condensed matter: structure, mechanical and thermal properties Defects and impurities in crystals microstructure Exact sciences and technology Impurities: concentration, distribution, and gradients Physics Structure of solids and liquids crystallography |
title | Redistribution of chromium under annealed sulfur implants into chromium-doped GaAs |
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