Study of end of range loop interactions with B+ implant damage using a boron doped diffusion layer
A boron doped epilayer was used to investigate the interaction between end of range dislocation loops (formed from Ge+ implantation) and excess point defects generated from a low dose 1014/cm2 B+ implant into silicon. The boron doping spike was grown in by chemical vapor deposition at a depth of 800...
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Veröffentlicht in: | Journal of applied physics 1995-08, Vol.78 (4), p.2298-2302 |
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container_title | Journal of applied physics |
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creator | Listebarger, J. K. Robinson, H. G. Jones, K. S. Law, M. E. Sieloff, D. D. Slinkman, J. A. Sedgwick, T. O. |
description | A boron doped epilayer was used to investigate the interaction between end of range dislocation loops (formed from Ge+ implantation) and excess point defects generated from a low dose 1014/cm2 B+ implant into silicon. The boron doping spike was grown in by chemical vapor deposition at a depth of 8000 Å below the surface. The intrinsic diffusivity of the boron in the doped epilayer was determined by simply annealing the as-grown layer. The end of range (type II) dislocation loops were created using two overlapping room-temperature Ge+ implants of 75 and 190 keV each at a dose of 1×1015/cm2. Upon annealing the amorphous layer regrew and a layer of type II dislocation loops formed ∼2300 Å deep at a density of ∼8×1010/cm2. The enhancement in the buried boron layer diffusivity due to the type II loop forming Ge+ implant was observed to increase approximately between 2.5 and 5 min from 1500× to a value 2500× above the intrinsic diffusivity before dropping back to intrinsic levels after 30 min at 800 °C. A low-energy (8 keV) 1×1014/cm2 B+ (Rp=320 Å) implant into material without loops resulted in an average enhancement of 1540× in boron epilayer diffusivity after 2.5 min at 800 °C. The enhancement dropped down to intrinsic diffusivity levels after 5 min at 800 °C. When a layer of loops was introduced and annealed prior to and deeper than a subsequent low-energy B+ implant, annealing of the B+ implant produced no measurable enhancement in the buried B layer diffusivity. Taken together this imples that the interaction kinetics between the dislocation loop layer and the damage induced interstitials are primarily diffusion limited and the loops are absorbing a significant fraction of the interstitials produced by the low-energy B+ implant. |
doi_str_mv | 10.1063/1.360147 |
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K. ; Robinson, H. G. ; Jones, K. S. ; Law, M. E. ; Sieloff, D. D. ; Slinkman, J. A. ; Sedgwick, T. O.</creator><creatorcontrib>Listebarger, J. K. ; Robinson, H. G. ; Jones, K. S. ; Law, M. E. ; Sieloff, D. D. ; Slinkman, J. A. ; Sedgwick, T. O.</creatorcontrib><description>A boron doped epilayer was used to investigate the interaction between end of range dislocation loops (formed from Ge+ implantation) and excess point defects generated from a low dose 1014/cm2 B+ implant into silicon. The boron doping spike was grown in by chemical vapor deposition at a depth of 8000 Å below the surface. The intrinsic diffusivity of the boron in the doped epilayer was determined by simply annealing the as-grown layer. The end of range (type II) dislocation loops were created using two overlapping room-temperature Ge+ implants of 75 and 190 keV each at a dose of 1×1015/cm2. Upon annealing the amorphous layer regrew and a layer of type II dislocation loops formed ∼2300 Å deep at a density of ∼8×1010/cm2. The enhancement in the buried boron layer diffusivity due to the type II loop forming Ge+ implant was observed to increase approximately between 2.5 and 5 min from 1500× to a value 2500× above the intrinsic diffusivity before dropping back to intrinsic levels after 30 min at 800 °C. A low-energy (8 keV) 1×1014/cm2 B+ (Rp=320 Å) implant into material without loops resulted in an average enhancement of 1540× in boron epilayer diffusivity after 2.5 min at 800 °C. The enhancement dropped down to intrinsic diffusivity levels after 5 min at 800 °C. When a layer of loops was introduced and annealed prior to and deeper than a subsequent low-energy B+ implant, annealing of the B+ implant produced no measurable enhancement in the buried B layer diffusivity. Taken together this imples that the interaction kinetics between the dislocation loop layer and the damage induced interstitials are primarily diffusion limited and the loops are absorbing a significant fraction of the interstitials produced by the low-energy B+ implant.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/1.360147</identifier><language>eng</language><ispartof>Journal of applied physics, 1995-08, Vol.78 (4), p.2298-2302</ispartof><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c261t-197146dc5bdc5895d831062d257813d27a69213b086c7ffb37c9e79abd74661c3</citedby><cites>FETCH-LOGICAL-c261t-197146dc5bdc5895d831062d257813d27a69213b086c7ffb37c9e79abd74661c3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>315,782,786,27931,27932</link.rule.ids></links><search><creatorcontrib>Listebarger, J. 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The end of range (type II) dislocation loops were created using two overlapping room-temperature Ge+ implants of 75 and 190 keV each at a dose of 1×1015/cm2. Upon annealing the amorphous layer regrew and a layer of type II dislocation loops formed ∼2300 Å deep at a density of ∼8×1010/cm2. The enhancement in the buried boron layer diffusivity due to the type II loop forming Ge+ implant was observed to increase approximately between 2.5 and 5 min from 1500× to a value 2500× above the intrinsic diffusivity before dropping back to intrinsic levels after 30 min at 800 °C. A low-energy (8 keV) 1×1014/cm2 B+ (Rp=320 Å) implant into material without loops resulted in an average enhancement of 1540× in boron epilayer diffusivity after 2.5 min at 800 °C. The enhancement dropped down to intrinsic diffusivity levels after 5 min at 800 °C. When a layer of loops was introduced and annealed prior to and deeper than a subsequent low-energy B+ implant, annealing of the B+ implant produced no measurable enhancement in the buried B layer diffusivity. Taken together this imples that the interaction kinetics between the dislocation loop layer and the damage induced interstitials are primarily diffusion limited and the loops are absorbing a significant fraction of the interstitials produced by the low-energy B+ implant.</description><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1995</creationdate><recordtype>article</recordtype><recordid>eNotUEtLxDAYDKJgXQV_Qo6CdM3XtHkcdXFVWPCgnkuaxxppk5J0kf57u6yHYZhhGJhB6BbIGgijD7CmjEDNz1ABRMiSNw05RwUhFZRCcnmJrnL-IQRAUFmg7mM6mBlHh20wR0oq7C3uYxyxD5NNSk8-hox__fSNn-6xH8ZehQkbNagleMg-7LHCXUwxYBNHa7Dxzi3-ons123SNLpzqs7355xX62j5_bl7L3fvL2-ZxV-qKwVSC5FAzo5tugZCNEXQZVJmq4QKoqbhisgLaEcE0d66jXEvLpeoMrxkDTVfo7tSrU8w5WdeOyQ8qzS2Q9vhNC-3pG_oHXwxV1w</recordid><startdate>19950815</startdate><enddate>19950815</enddate><creator>Listebarger, J. K.</creator><creator>Robinson, H. G.</creator><creator>Jones, K. S.</creator><creator>Law, M. 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E.</creatorcontrib><creatorcontrib>Sieloff, D. D.</creatorcontrib><creatorcontrib>Slinkman, J. A.</creatorcontrib><creatorcontrib>Sedgwick, T. O.</creatorcontrib><collection>CrossRef</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Listebarger, J. K.</au><au>Robinson, H. G.</au><au>Jones, K. S.</au><au>Law, M. E.</au><au>Sieloff, D. D.</au><au>Slinkman, J. A.</au><au>Sedgwick, T. O.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Study of end of range loop interactions with B+ implant damage using a boron doped diffusion layer</atitle><jtitle>Journal of applied physics</jtitle><date>1995-08-15</date><risdate>1995</risdate><volume>78</volume><issue>4</issue><spage>2298</spage><epage>2302</epage><pages>2298-2302</pages><issn>0021-8979</issn><eissn>1089-7550</eissn><abstract>A boron doped epilayer was used to investigate the interaction between end of range dislocation loops (formed from Ge+ implantation) and excess point defects generated from a low dose 1014/cm2 B+ implant into silicon. The boron doping spike was grown in by chemical vapor deposition at a depth of 8000 Å below the surface. The intrinsic diffusivity of the boron in the doped epilayer was determined by simply annealing the as-grown layer. The end of range (type II) dislocation loops were created using two overlapping room-temperature Ge+ implants of 75 and 190 keV each at a dose of 1×1015/cm2. Upon annealing the amorphous layer regrew and a layer of type II dislocation loops formed ∼2300 Å deep at a density of ∼8×1010/cm2. The enhancement in the buried boron layer diffusivity due to the type II loop forming Ge+ implant was observed to increase approximately between 2.5 and 5 min from 1500× to a value 2500× above the intrinsic diffusivity before dropping back to intrinsic levels after 30 min at 800 °C. A low-energy (8 keV) 1×1014/cm2 B+ (Rp=320 Å) implant into material without loops resulted in an average enhancement of 1540× in boron epilayer diffusivity after 2.5 min at 800 °C. The enhancement dropped down to intrinsic diffusivity levels after 5 min at 800 °C. When a layer of loops was introduced and annealed prior to and deeper than a subsequent low-energy B+ implant, annealing of the B+ implant produced no measurable enhancement in the buried B layer diffusivity. Taken together this imples that the interaction kinetics between the dislocation loop layer and the damage induced interstitials are primarily diffusion limited and the loops are absorbing a significant fraction of the interstitials produced by the low-energy B+ implant.</abstract><doi>10.1063/1.360147</doi><tpages>5</tpages><oa>free_for_read</oa></addata></record> |
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title | Study of end of range loop interactions with B+ implant damage using a boron doped diffusion layer |
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