Growth and shrinkage of stacking faults by gold diffusion in silicon
Abstract Gold atoms were indiffused at 1150 ‡C into a silicon crystal containing nuclei for point defects, and then annealed at 1000 ‡C. Growth and shrinkage of the stacking faults induced by the gold diffusion has been investigated. In the indiffusion process, the faults grow homogeneously in propo...
Ausführliche Beschreibung
Autor*in: |
Morooka, M. [verfasserIn] |
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Format: |
Artikel |
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Sprache: |
Englisch |
Erschienen: |
1996 |
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Schlagwörter: |
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Anmerkung: |
© Chapman & Hall 1996 |
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Übergeordnetes Werk: |
Enthalten in: Journal of materials science / Materials in electronics - Kluwer Academic Publishers, 1990, 7(1996), 3 vom: Juni, Seite 221-225 |
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Übergeordnetes Werk: |
volume:7 ; year:1996 ; number:3 ; month:06 ; pages:221-225 |
Links: |
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DOI / URN: |
10.1007/BF00133119 |
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Katalog-ID: |
OLC2026237344 |
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10.1007/BF00133119 doi (DE-627)OLC2026237344 (DE-He213)BF00133119-p DE-627 ger DE-627 rakwb eng 600 670 620 VZ Morooka, M. verfasserin aut Growth and shrinkage of stacking faults by gold diffusion in silicon 1996 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Chapman & Hall 1996 Abstract Gold atoms were indiffused at 1150 ‡C into a silicon crystal containing nuclei for point defects, and then annealed at 1000 ‡C. Growth and shrinkage of the stacking faults induced by the gold diffusion has been investigated. In the indiffusion process, the faults grow homogeneously in proportion to the square root of substitutional gold concentration, but the volume density of the faults is limited at the very beginning of the gold diffusion and does not depend on the gold concentration. In the annealing, the faults shrink inhomogeneously and disappear in turn in proportion to the decrease of substitutional gold, keeping the same mean size as before annealing. The difference between behaviours in the growth and shrinkage is caused by the differences during absorption and discharge of silicon atoms by the faults, due to a distortion around the fault edge. Silicon Gold Shrinkage Material Processing Point Defect Enthalten in Journal of materials science / Materials in electronics Kluwer Academic Publishers, 1990 7(1996), 3 vom: Juni, Seite 221-225 (DE-627)130863289 (DE-600)1030929-9 (DE-576)023106719 0957-4522 nnns volume:7 year:1996 number:3 month:06 pages:221-225 https://doi.org/10.1007/BF00133119 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_23 GBV_ILN_24 GBV_ILN_30 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_62 GBV_ILN_65 GBV_ILN_70 GBV_ILN_2004 GBV_ILN_2006 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2027 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4316 GBV_ILN_4319 GBV_ILN_4323 GBV_ILN_4700 AR 7 1996 3 06 221-225 |
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10.1007/BF00133119 doi (DE-627)OLC2026237344 (DE-He213)BF00133119-p DE-627 ger DE-627 rakwb eng 600 670 620 VZ Morooka, M. verfasserin aut Growth and shrinkage of stacking faults by gold diffusion in silicon 1996 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Chapman & Hall 1996 Abstract Gold atoms were indiffused at 1150 ‡C into a silicon crystal containing nuclei for point defects, and then annealed at 1000 ‡C. Growth and shrinkage of the stacking faults induced by the gold diffusion has been investigated. In the indiffusion process, the faults grow homogeneously in proportion to the square root of substitutional gold concentration, but the volume density of the faults is limited at the very beginning of the gold diffusion and does not depend on the gold concentration. In the annealing, the faults shrink inhomogeneously and disappear in turn in proportion to the decrease of substitutional gold, keeping the same mean size as before annealing. The difference between behaviours in the growth and shrinkage is caused by the differences during absorption and discharge of silicon atoms by the faults, due to a distortion around the fault edge. Silicon Gold Shrinkage Material Processing Point Defect Enthalten in Journal of materials science / Materials in electronics Kluwer Academic Publishers, 1990 7(1996), 3 vom: Juni, Seite 221-225 (DE-627)130863289 (DE-600)1030929-9 (DE-576)023106719 0957-4522 nnns volume:7 year:1996 number:3 month:06 pages:221-225 https://doi.org/10.1007/BF00133119 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_23 GBV_ILN_24 GBV_ILN_30 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_62 GBV_ILN_65 GBV_ILN_70 GBV_ILN_2004 GBV_ILN_2006 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2027 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4316 GBV_ILN_4319 GBV_ILN_4323 GBV_ILN_4700 AR 7 1996 3 06 221-225 |
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10.1007/BF00133119 doi (DE-627)OLC2026237344 (DE-He213)BF00133119-p DE-627 ger DE-627 rakwb eng 600 670 620 VZ Morooka, M. verfasserin aut Growth and shrinkage of stacking faults by gold diffusion in silicon 1996 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Chapman & Hall 1996 Abstract Gold atoms were indiffused at 1150 ‡C into a silicon crystal containing nuclei for point defects, and then annealed at 1000 ‡C. Growth and shrinkage of the stacking faults induced by the gold diffusion has been investigated. In the indiffusion process, the faults grow homogeneously in proportion to the square root of substitutional gold concentration, but the volume density of the faults is limited at the very beginning of the gold diffusion and does not depend on the gold concentration. In the annealing, the faults shrink inhomogeneously and disappear in turn in proportion to the decrease of substitutional gold, keeping the same mean size as before annealing. The difference between behaviours in the growth and shrinkage is caused by the differences during absorption and discharge of silicon atoms by the faults, due to a distortion around the fault edge. Silicon Gold Shrinkage Material Processing Point Defect Enthalten in Journal of materials science / Materials in electronics Kluwer Academic Publishers, 1990 7(1996), 3 vom: Juni, Seite 221-225 (DE-627)130863289 (DE-600)1030929-9 (DE-576)023106719 0957-4522 nnns volume:7 year:1996 number:3 month:06 pages:221-225 https://doi.org/10.1007/BF00133119 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_23 GBV_ILN_24 GBV_ILN_30 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_62 GBV_ILN_65 GBV_ILN_70 GBV_ILN_2004 GBV_ILN_2006 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2027 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4316 GBV_ILN_4319 GBV_ILN_4323 GBV_ILN_4700 AR 7 1996 3 06 221-225 |
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10.1007/BF00133119 doi (DE-627)OLC2026237344 (DE-He213)BF00133119-p DE-627 ger DE-627 rakwb eng 600 670 620 VZ Morooka, M. verfasserin aut Growth and shrinkage of stacking faults by gold diffusion in silicon 1996 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Chapman & Hall 1996 Abstract Gold atoms were indiffused at 1150 ‡C into a silicon crystal containing nuclei for point defects, and then annealed at 1000 ‡C. Growth and shrinkage of the stacking faults induced by the gold diffusion has been investigated. In the indiffusion process, the faults grow homogeneously in proportion to the square root of substitutional gold concentration, but the volume density of the faults is limited at the very beginning of the gold diffusion and does not depend on the gold concentration. In the annealing, the faults shrink inhomogeneously and disappear in turn in proportion to the decrease of substitutional gold, keeping the same mean size as before annealing. The difference between behaviours in the growth and shrinkage is caused by the differences during absorption and discharge of silicon atoms by the faults, due to a distortion around the fault edge. Silicon Gold Shrinkage Material Processing Point Defect Enthalten in Journal of materials science / Materials in electronics Kluwer Academic Publishers, 1990 7(1996), 3 vom: Juni, Seite 221-225 (DE-627)130863289 (DE-600)1030929-9 (DE-576)023106719 0957-4522 nnns volume:7 year:1996 number:3 month:06 pages:221-225 https://doi.org/10.1007/BF00133119 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_23 GBV_ILN_24 GBV_ILN_30 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_62 GBV_ILN_65 GBV_ILN_70 GBV_ILN_2004 GBV_ILN_2006 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2027 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4316 GBV_ILN_4319 GBV_ILN_4323 GBV_ILN_4700 AR 7 1996 3 06 221-225 |
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10.1007/BF00133119 doi (DE-627)OLC2026237344 (DE-He213)BF00133119-p DE-627 ger DE-627 rakwb eng 600 670 620 VZ Morooka, M. verfasserin aut Growth and shrinkage of stacking faults by gold diffusion in silicon 1996 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Chapman & Hall 1996 Abstract Gold atoms were indiffused at 1150 ‡C into a silicon crystal containing nuclei for point defects, and then annealed at 1000 ‡C. Growth and shrinkage of the stacking faults induced by the gold diffusion has been investigated. In the indiffusion process, the faults grow homogeneously in proportion to the square root of substitutional gold concentration, but the volume density of the faults is limited at the very beginning of the gold diffusion and does not depend on the gold concentration. In the annealing, the faults shrink inhomogeneously and disappear in turn in proportion to the decrease of substitutional gold, keeping the same mean size as before annealing. The difference between behaviours in the growth and shrinkage is caused by the differences during absorption and discharge of silicon atoms by the faults, due to a distortion around the fault edge. Silicon Gold Shrinkage Material Processing Point Defect Enthalten in Journal of materials science / Materials in electronics Kluwer Academic Publishers, 1990 7(1996), 3 vom: Juni, Seite 221-225 (DE-627)130863289 (DE-600)1030929-9 (DE-576)023106719 0957-4522 nnns volume:7 year:1996 number:3 month:06 pages:221-225 https://doi.org/10.1007/BF00133119 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_23 GBV_ILN_24 GBV_ILN_30 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_62 GBV_ILN_65 GBV_ILN_70 GBV_ILN_2004 GBV_ILN_2006 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2027 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4316 GBV_ILN_4319 GBV_ILN_4323 GBV_ILN_4700 AR 7 1996 3 06 221-225 |
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Growth and shrinkage of stacking faults by gold diffusion in silicon |
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Growth and shrinkage of stacking faults by gold diffusion in silicon |
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Morooka, M. |
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Journal of materials science / Materials in electronics |
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Journal of materials science / Materials in electronics |
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1996 |
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Morooka, M. |
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Morooka, M. |
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10.1007/BF00133119 |
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600 670 620 |
title_sort |
growth and shrinkage of stacking faults by gold diffusion in silicon |
title_auth |
Growth and shrinkage of stacking faults by gold diffusion in silicon |
abstract |
Abstract Gold atoms were indiffused at 1150 ‡C into a silicon crystal containing nuclei for point defects, and then annealed at 1000 ‡C. Growth and shrinkage of the stacking faults induced by the gold diffusion has been investigated. In the indiffusion process, the faults grow homogeneously in proportion to the square root of substitutional gold concentration, but the volume density of the faults is limited at the very beginning of the gold diffusion and does not depend on the gold concentration. In the annealing, the faults shrink inhomogeneously and disappear in turn in proportion to the decrease of substitutional gold, keeping the same mean size as before annealing. The difference between behaviours in the growth and shrinkage is caused by the differences during absorption and discharge of silicon atoms by the faults, due to a distortion around the fault edge. © Chapman & Hall 1996 |
abstractGer |
Abstract Gold atoms were indiffused at 1150 ‡C into a silicon crystal containing nuclei for point defects, and then annealed at 1000 ‡C. Growth and shrinkage of the stacking faults induced by the gold diffusion has been investigated. In the indiffusion process, the faults grow homogeneously in proportion to the square root of substitutional gold concentration, but the volume density of the faults is limited at the very beginning of the gold diffusion and does not depend on the gold concentration. In the annealing, the faults shrink inhomogeneously and disappear in turn in proportion to the decrease of substitutional gold, keeping the same mean size as before annealing. The difference between behaviours in the growth and shrinkage is caused by the differences during absorption and discharge of silicon atoms by the faults, due to a distortion around the fault edge. © Chapman & Hall 1996 |
abstract_unstemmed |
Abstract Gold atoms were indiffused at 1150 ‡C into a silicon crystal containing nuclei for point defects, and then annealed at 1000 ‡C. Growth and shrinkage of the stacking faults induced by the gold diffusion has been investigated. In the indiffusion process, the faults grow homogeneously in proportion to the square root of substitutional gold concentration, but the volume density of the faults is limited at the very beginning of the gold diffusion and does not depend on the gold concentration. In the annealing, the faults shrink inhomogeneously and disappear in turn in proportion to the decrease of substitutional gold, keeping the same mean size as before annealing. The difference between behaviours in the growth and shrinkage is caused by the differences during absorption and discharge of silicon atoms by the faults, due to a distortion around the fault edge. © Chapman & Hall 1996 |
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Growth and shrinkage of stacking faults by gold diffusion in silicon |
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