The Distribution Tail of LWIR HgCdTe-on-Si FPAs: a Hypothetical Physical Mechanism
A model is proposed to explain disparities found in the operability values and histograms for long-wavelength infrared HgCdTe focal-plane arrays fabricated on Si substrates compared with those fabricated on CdZnTe. The starting point for the model is the close agreement between the aerial density of...
Ausführliche Beschreibung
Autor*in: |
Bubulac, L. O. [verfasserIn] |
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Format: |
E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2011 |
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Schlagwörter: |
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Anmerkung: |
© TMS (outside of the USA) 2011 |
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Übergeordnetes Werk: |
Enthalten in: Journal of electronic materials - Warrendale, Pa : TMS, 1972, 40(2011), 3 vom: 02. Feb., Seite 280-288 |
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Übergeordnetes Werk: |
volume:40 ; year:2011 ; number:3 ; day:02 ; month:02 ; pages:280-288 |
Links: |
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DOI / URN: |
10.1007/s11664-010-1505-9 |
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Katalog-ID: |
SPR021496188 |
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245 | 1 | 4 | |a The Distribution Tail of LWIR HgCdTe-on-Si FPAs: a Hypothetical Physical Mechanism |
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520 | |a A model is proposed to explain disparities found in the operability values and histograms for long-wavelength infrared HgCdTe focal-plane arrays fabricated on Si substrates compared with those fabricated on CdZnTe. The starting point for the model is the close agreement between the aerial density of discrete species (particles, contamination spots, crystalline defects on Si surface) in various interfaces in the HgCdTe/CdTe/Si structure and the density of failed pixels in the array. The density of discrete species is acquired by applying a newly developed variation of the secondary-ion mass spectrometry (SIMS) depth-profiling technique to samples that have been deuterated to enhance detection. A mechanism of selective activation of threading dislocations in a HgCdTe layer on Si is proposed to link discrete species with failed detector pixels. | ||
650 | 4 | |a HgCdTe |7 (dpeaa)DE-He213 | |
650 | 4 | |a discrete species |7 (dpeaa)DE-He213 | |
650 | 4 | |a Si |7 (dpeaa)DE-He213 | |
650 | 4 | |a FPA |7 (dpeaa)DE-He213 | |
650 | 4 | |a dislocation |7 (dpeaa)DE-He213 | |
650 | 4 | |a enhanced diffusion |7 (dpeaa)DE-He213 | |
650 | 4 | |a diffusion pipes |7 (dpeaa)DE-He213 | |
700 | 1 | |a Benson, J.D. |4 aut | |
700 | 1 | |a Jacobs, R.N. |4 aut | |
700 | 1 | |a Stoltz, A.J. |4 aut | |
700 | 1 | |a Jaime-Vasquez, M. |4 aut | |
700 | 1 | |a Almeida, L. A. |4 aut | |
700 | 1 | |a Wang, A. |4 aut | |
700 | 1 | |a Wang, L. |4 aut | |
700 | 1 | |a Hellmer, R. |4 aut | |
700 | 1 | |a Golding, T. |4 aut | |
700 | 1 | |a Dinan, J.H. |4 aut | |
700 | 1 | |a Carmody, M. |4 aut | |
700 | 1 | |a Wijewarnasuriya, P.S. |4 aut | |
700 | 1 | |a Lee, M.F. |4 aut | |
700 | 1 | |a Vilela, M.F. |4 aut | |
700 | 1 | |a Peterson, J. |4 aut | |
700 | 1 | |a Johnson, S.M. |4 aut | |
700 | 1 | |a Lofgreen, D.F. |4 aut | |
700 | 1 | |a Rhiger, D. |4 aut | |
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10.1007/s11664-010-1505-9 doi (DE-627)SPR021496188 (SPR)s11664-010-1505-9-e DE-627 ger DE-627 rakwb eng Bubulac, L. O. verfasserin aut The Distribution Tail of LWIR HgCdTe-on-Si FPAs: a Hypothetical Physical Mechanism 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © TMS (outside of the USA) 2011 A model is proposed to explain disparities found in the operability values and histograms for long-wavelength infrared HgCdTe focal-plane arrays fabricated on Si substrates compared with those fabricated on CdZnTe. The starting point for the model is the close agreement between the aerial density of discrete species (particles, contamination spots, crystalline defects on Si surface) in various interfaces in the HgCdTe/CdTe/Si structure and the density of failed pixels in the array. The density of discrete species is acquired by applying a newly developed variation of the secondary-ion mass spectrometry (SIMS) depth-profiling technique to samples that have been deuterated to enhance detection. A mechanism of selective activation of threading dislocations in a HgCdTe layer on Si is proposed to link discrete species with failed detector pixels. HgCdTe (dpeaa)DE-He213 discrete species (dpeaa)DE-He213 Si (dpeaa)DE-He213 FPA (dpeaa)DE-He213 dislocation (dpeaa)DE-He213 enhanced diffusion (dpeaa)DE-He213 diffusion pipes (dpeaa)DE-He213 Benson, J.D. aut Jacobs, R.N. aut Stoltz, A.J. aut Jaime-Vasquez, M. aut Almeida, L. A. aut Wang, A. aut Wang, L. aut Hellmer, R. aut Golding, T. aut Dinan, J.H. aut Carmody, M. aut Wijewarnasuriya, P.S. aut Lee, M.F. aut Vilela, M.F. aut Peterson, J. aut Johnson, S.M. aut Lofgreen, D.F. aut Rhiger, D. aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 40(2011), 3 vom: 02. Feb., Seite 280-288 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:40 year:2011 number:3 day:02 month:02 pages:280-288 https://dx.doi.org/10.1007/s11664-010-1505-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 40 2011 3 02 02 280-288 |
spelling |
10.1007/s11664-010-1505-9 doi (DE-627)SPR021496188 (SPR)s11664-010-1505-9-e DE-627 ger DE-627 rakwb eng Bubulac, L. O. verfasserin aut The Distribution Tail of LWIR HgCdTe-on-Si FPAs: a Hypothetical Physical Mechanism 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © TMS (outside of the USA) 2011 A model is proposed to explain disparities found in the operability values and histograms for long-wavelength infrared HgCdTe focal-plane arrays fabricated on Si substrates compared with those fabricated on CdZnTe. The starting point for the model is the close agreement between the aerial density of discrete species (particles, contamination spots, crystalline defects on Si surface) in various interfaces in the HgCdTe/CdTe/Si structure and the density of failed pixels in the array. The density of discrete species is acquired by applying a newly developed variation of the secondary-ion mass spectrometry (SIMS) depth-profiling technique to samples that have been deuterated to enhance detection. A mechanism of selective activation of threading dislocations in a HgCdTe layer on Si is proposed to link discrete species with failed detector pixels. HgCdTe (dpeaa)DE-He213 discrete species (dpeaa)DE-He213 Si (dpeaa)DE-He213 FPA (dpeaa)DE-He213 dislocation (dpeaa)DE-He213 enhanced diffusion (dpeaa)DE-He213 diffusion pipes (dpeaa)DE-He213 Benson, J.D. aut Jacobs, R.N. aut Stoltz, A.J. aut Jaime-Vasquez, M. aut Almeida, L. A. aut Wang, A. aut Wang, L. aut Hellmer, R. aut Golding, T. aut Dinan, J.H. aut Carmody, M. aut Wijewarnasuriya, P.S. aut Lee, M.F. aut Vilela, M.F. aut Peterson, J. aut Johnson, S.M. aut Lofgreen, D.F. aut Rhiger, D. aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 40(2011), 3 vom: 02. Feb., Seite 280-288 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:40 year:2011 number:3 day:02 month:02 pages:280-288 https://dx.doi.org/10.1007/s11664-010-1505-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 40 2011 3 02 02 280-288 |
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10.1007/s11664-010-1505-9 doi (DE-627)SPR021496188 (SPR)s11664-010-1505-9-e DE-627 ger DE-627 rakwb eng Bubulac, L. O. verfasserin aut The Distribution Tail of LWIR HgCdTe-on-Si FPAs: a Hypothetical Physical Mechanism 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © TMS (outside of the USA) 2011 A model is proposed to explain disparities found in the operability values and histograms for long-wavelength infrared HgCdTe focal-plane arrays fabricated on Si substrates compared with those fabricated on CdZnTe. The starting point for the model is the close agreement between the aerial density of discrete species (particles, contamination spots, crystalline defects on Si surface) in various interfaces in the HgCdTe/CdTe/Si structure and the density of failed pixels in the array. The density of discrete species is acquired by applying a newly developed variation of the secondary-ion mass spectrometry (SIMS) depth-profiling technique to samples that have been deuterated to enhance detection. A mechanism of selective activation of threading dislocations in a HgCdTe layer on Si is proposed to link discrete species with failed detector pixels. HgCdTe (dpeaa)DE-He213 discrete species (dpeaa)DE-He213 Si (dpeaa)DE-He213 FPA (dpeaa)DE-He213 dislocation (dpeaa)DE-He213 enhanced diffusion (dpeaa)DE-He213 diffusion pipes (dpeaa)DE-He213 Benson, J.D. aut Jacobs, R.N. aut Stoltz, A.J. aut Jaime-Vasquez, M. aut Almeida, L. A. aut Wang, A. aut Wang, L. aut Hellmer, R. aut Golding, T. aut Dinan, J.H. aut Carmody, M. aut Wijewarnasuriya, P.S. aut Lee, M.F. aut Vilela, M.F. aut Peterson, J. aut Johnson, S.M. aut Lofgreen, D.F. aut Rhiger, D. aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 40(2011), 3 vom: 02. Feb., Seite 280-288 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:40 year:2011 number:3 day:02 month:02 pages:280-288 https://dx.doi.org/10.1007/s11664-010-1505-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 40 2011 3 02 02 280-288 |
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10.1007/s11664-010-1505-9 doi (DE-627)SPR021496188 (SPR)s11664-010-1505-9-e DE-627 ger DE-627 rakwb eng Bubulac, L. O. verfasserin aut The Distribution Tail of LWIR HgCdTe-on-Si FPAs: a Hypothetical Physical Mechanism 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © TMS (outside of the USA) 2011 A model is proposed to explain disparities found in the operability values and histograms for long-wavelength infrared HgCdTe focal-plane arrays fabricated on Si substrates compared with those fabricated on CdZnTe. The starting point for the model is the close agreement between the aerial density of discrete species (particles, contamination spots, crystalline defects on Si surface) in various interfaces in the HgCdTe/CdTe/Si structure and the density of failed pixels in the array. The density of discrete species is acquired by applying a newly developed variation of the secondary-ion mass spectrometry (SIMS) depth-profiling technique to samples that have been deuterated to enhance detection. A mechanism of selective activation of threading dislocations in a HgCdTe layer on Si is proposed to link discrete species with failed detector pixels. HgCdTe (dpeaa)DE-He213 discrete species (dpeaa)DE-He213 Si (dpeaa)DE-He213 FPA (dpeaa)DE-He213 dislocation (dpeaa)DE-He213 enhanced diffusion (dpeaa)DE-He213 diffusion pipes (dpeaa)DE-He213 Benson, J.D. aut Jacobs, R.N. aut Stoltz, A.J. aut Jaime-Vasquez, M. aut Almeida, L. A. aut Wang, A. aut Wang, L. aut Hellmer, R. aut Golding, T. aut Dinan, J.H. aut Carmody, M. aut Wijewarnasuriya, P.S. aut Lee, M.F. aut Vilela, M.F. aut Peterson, J. aut Johnson, S.M. aut Lofgreen, D.F. aut Rhiger, D. aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 40(2011), 3 vom: 02. Feb., Seite 280-288 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:40 year:2011 number:3 day:02 month:02 pages:280-288 https://dx.doi.org/10.1007/s11664-010-1505-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 40 2011 3 02 02 280-288 |
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10.1007/s11664-010-1505-9 doi (DE-627)SPR021496188 (SPR)s11664-010-1505-9-e DE-627 ger DE-627 rakwb eng Bubulac, L. O. verfasserin aut The Distribution Tail of LWIR HgCdTe-on-Si FPAs: a Hypothetical Physical Mechanism 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © TMS (outside of the USA) 2011 A model is proposed to explain disparities found in the operability values and histograms for long-wavelength infrared HgCdTe focal-plane arrays fabricated on Si substrates compared with those fabricated on CdZnTe. The starting point for the model is the close agreement between the aerial density of discrete species (particles, contamination spots, crystalline defects on Si surface) in various interfaces in the HgCdTe/CdTe/Si structure and the density of failed pixels in the array. The density of discrete species is acquired by applying a newly developed variation of the secondary-ion mass spectrometry (SIMS) depth-profiling technique to samples that have been deuterated to enhance detection. A mechanism of selective activation of threading dislocations in a HgCdTe layer on Si is proposed to link discrete species with failed detector pixels. HgCdTe (dpeaa)DE-He213 discrete species (dpeaa)DE-He213 Si (dpeaa)DE-He213 FPA (dpeaa)DE-He213 dislocation (dpeaa)DE-He213 enhanced diffusion (dpeaa)DE-He213 diffusion pipes (dpeaa)DE-He213 Benson, J.D. aut Jacobs, R.N. aut Stoltz, A.J. aut Jaime-Vasquez, M. aut Almeida, L. A. aut Wang, A. aut Wang, L. aut Hellmer, R. aut Golding, T. aut Dinan, J.H. aut Carmody, M. aut Wijewarnasuriya, P.S. aut Lee, M.F. aut Vilela, M.F. aut Peterson, J. aut Johnson, S.M. aut Lofgreen, D.F. aut Rhiger, D. aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 40(2011), 3 vom: 02. Feb., Seite 280-288 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:40 year:2011 number:3 day:02 month:02 pages:280-288 https://dx.doi.org/10.1007/s11664-010-1505-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 40 2011 3 02 02 280-288 |
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English |
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Enthalten in Journal of electronic materials 40(2011), 3 vom: 02. Feb., Seite 280-288 volume:40 year:2011 number:3 day:02 month:02 pages:280-288 |
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Enthalten in Journal of electronic materials 40(2011), 3 vom: 02. Feb., Seite 280-288 volume:40 year:2011 number:3 day:02 month:02 pages:280-288 |
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HgCdTe discrete species Si FPA dislocation enhanced diffusion diffusion pipes |
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Bubulac, L. O. @@aut@@ Benson, J.D. @@aut@@ Jacobs, R.N. @@aut@@ Stoltz, A.J. @@aut@@ Jaime-Vasquez, M. @@aut@@ Almeida, L. A. @@aut@@ Wang, A. @@aut@@ Wang, L. @@aut@@ Hellmer, R. @@aut@@ Golding, T. @@aut@@ Dinan, J.H. @@aut@@ Carmody, M. @@aut@@ Wijewarnasuriya, P.S. @@aut@@ Lee, M.F. @@aut@@ Vilela, M.F. @@aut@@ Peterson, J. @@aut@@ Johnson, S.M. @@aut@@ Lofgreen, D.F. @@aut@@ Rhiger, D. @@aut@@ |
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Bubulac, L. O. |
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Bubulac, L. O. misc HgCdTe misc discrete species misc Si misc FPA misc dislocation misc enhanced diffusion misc diffusion pipes The Distribution Tail of LWIR HgCdTe-on-Si FPAs: a Hypothetical Physical Mechanism |
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The Distribution Tail of LWIR HgCdTe-on-Si FPAs: a Hypothetical Physical Mechanism HgCdTe (dpeaa)DE-He213 discrete species (dpeaa)DE-He213 Si (dpeaa)DE-He213 FPA (dpeaa)DE-He213 dislocation (dpeaa)DE-He213 enhanced diffusion (dpeaa)DE-He213 diffusion pipes (dpeaa)DE-He213 |
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distribution tail of lwir hgcdte-on-si fpas: a hypothetical physical mechanism |
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The Distribution Tail of LWIR HgCdTe-on-Si FPAs: a Hypothetical Physical Mechanism |
abstract |
A model is proposed to explain disparities found in the operability values and histograms for long-wavelength infrared HgCdTe focal-plane arrays fabricated on Si substrates compared with those fabricated on CdZnTe. The starting point for the model is the close agreement between the aerial density of discrete species (particles, contamination spots, crystalline defects on Si surface) in various interfaces in the HgCdTe/CdTe/Si structure and the density of failed pixels in the array. The density of discrete species is acquired by applying a newly developed variation of the secondary-ion mass spectrometry (SIMS) depth-profiling technique to samples that have been deuterated to enhance detection. A mechanism of selective activation of threading dislocations in a HgCdTe layer on Si is proposed to link discrete species with failed detector pixels. © TMS (outside of the USA) 2011 |
abstractGer |
A model is proposed to explain disparities found in the operability values and histograms for long-wavelength infrared HgCdTe focal-plane arrays fabricated on Si substrates compared with those fabricated on CdZnTe. The starting point for the model is the close agreement between the aerial density of discrete species (particles, contamination spots, crystalline defects on Si surface) in various interfaces in the HgCdTe/CdTe/Si structure and the density of failed pixels in the array. The density of discrete species is acquired by applying a newly developed variation of the secondary-ion mass spectrometry (SIMS) depth-profiling technique to samples that have been deuterated to enhance detection. A mechanism of selective activation of threading dislocations in a HgCdTe layer on Si is proposed to link discrete species with failed detector pixels. © TMS (outside of the USA) 2011 |
abstract_unstemmed |
A model is proposed to explain disparities found in the operability values and histograms for long-wavelength infrared HgCdTe focal-plane arrays fabricated on Si substrates compared with those fabricated on CdZnTe. The starting point for the model is the close agreement between the aerial density of discrete species (particles, contamination spots, crystalline defects on Si surface) in various interfaces in the HgCdTe/CdTe/Si structure and the density of failed pixels in the array. The density of discrete species is acquired by applying a newly developed variation of the secondary-ion mass spectrometry (SIMS) depth-profiling technique to samples that have been deuterated to enhance detection. A mechanism of selective activation of threading dislocations in a HgCdTe layer on Si is proposed to link discrete species with failed detector pixels. © TMS (outside of the USA) 2011 |
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container_issue |
3 |
title_short |
The Distribution Tail of LWIR HgCdTe-on-Si FPAs: a Hypothetical Physical Mechanism |
url |
https://dx.doi.org/10.1007/s11664-010-1505-9 |
remote_bool |
true |
author2 |
Benson, J.D. Jacobs, R.N. Stoltz, A.J. Jaime-Vasquez, M. Almeida, L. A. Wang, A. Wang, L. Hellmer, R. Golding, T. Dinan, J.H. Carmody, M. Wijewarnasuriya, P.S. Lee, M.F. Vilela, M.F. Peterson, J. Johnson, S.M. Lofgreen, D.F. Rhiger, D. |
author2Str |
Benson, J.D. Jacobs, R.N. Stoltz, A.J. Jaime-Vasquez, M. Almeida, L. A. Wang, A. Wang, L. Hellmer, R. Golding, T. Dinan, J.H. Carmody, M. Wijewarnasuriya, P.S. Lee, M.F. Vilela, M.F. Peterson, J. Johnson, S.M. Lofgreen, D.F. Rhiger, D. |
ppnlink |
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doi_str |
10.1007/s11664-010-1505-9 |
up_date |
2024-07-03T22:54:58.871Z |
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1803600316465152000 |
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|
score |
7.39787 |