Effects of HgCdTe on the Optical Emission of Inductively Coupled Plasmas
Abstract Inductively coupled plasmas (ICP) are the high-density plasmas of choice for processing HgCdTe and related compounds. Real-time examination of the ICP plasmas used to process HgCdTe would be desirable. In this preliminary study, the feasibility of using optical emission spectroscopy (OES) o...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Stoltz, A. J. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2010 |
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| Schlagwörter: |
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| Anmerkung: |
© US Army RDECOM CERDEC NVESD 2010 |
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| Übergeordnetes Werk: |
Enthalten in: Journal of electronic materials - Warrendale, Pa : TMS, 1972, 39(2010), 7 vom: 30. Apr., Seite 958-966 |
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| Übergeordnetes Werk: |
volume:39 ; year:2010 ; number:7 ; day:30 ; month:04 ; pages:958-966 |
| Links: |
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| DOI / URN: |
10.1007/s11664-010-1147-y |
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| Katalog-ID: |
SPR021492778 |
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| 520 | |a Abstract Inductively coupled plasmas (ICP) are the high-density plasmas of choice for processing HgCdTe and related compounds. Real-time examination of the ICP plasmas used to process HgCdTe would be desirable. In this preliminary study, the feasibility of using optical emission spectroscopy (OES) of ICP plasma used for processing HgCdTe has been examined. We have examined the utility of OES as a real-time diagnostic tool for HgCdTe device fabrication. In this preliminary study it has been found that mercury and cadmium can be detected but are dependent on several factors: sample area, material composition, etch rate, sample temperature, photoresist area, and plasma power. Furthermore, we found strong correlation between the amount of hydrogen detected by OES for samples with photoresist versus samples without photoresist while processing with hydrogen-based plasma. Hydrogen emission intensity decreased dramatically in samples with photoresist, contrary to the theory that photoresist adds hydrogen to the plasma effluent. It appears that hydrogen complexes with photoresist, reducing the global amount of hydrogen during the process. Furthermore, this phenomena may help to explain macroloading issues whereby additional photoresist area slowed HgCdTe, CdTe, and photoresist etch rates. | ||
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| 700 | 1 | |a Benson, J. D. |4 aut | |
| 700 | 1 | |a Smith, P. J. |4 aut | |
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10.1007/s11664-010-1147-y doi (DE-627)SPR021492778 (SPR)s11664-010-1147-y-e DE-627 ger DE-627 rakwb eng Stoltz, A. J. verfasserin aut Effects of HgCdTe on the Optical Emission of Inductively Coupled Plasmas 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © US Army RDECOM CERDEC NVESD 2010 Abstract Inductively coupled plasmas (ICP) are the high-density plasmas of choice for processing HgCdTe and related compounds. Real-time examination of the ICP plasmas used to process HgCdTe would be desirable. In this preliminary study, the feasibility of using optical emission spectroscopy (OES) of ICP plasma used for processing HgCdTe has been examined. We have examined the utility of OES as a real-time diagnostic tool for HgCdTe device fabrication. In this preliminary study it has been found that mercury and cadmium can be detected but are dependent on several factors: sample area, material composition, etch rate, sample temperature, photoresist area, and plasma power. Furthermore, we found strong correlation between the amount of hydrogen detected by OES for samples with photoresist versus samples without photoresist while processing with hydrogen-based plasma. Hydrogen emission intensity decreased dramatically in samples with photoresist, contrary to the theory that photoresist adds hydrogen to the plasma effluent. It appears that hydrogen complexes with photoresist, reducing the global amount of hydrogen during the process. Furthermore, this phenomena may help to explain macroloading issues whereby additional photoresist area slowed HgCdTe, CdTe, and photoresist etch rates. Optical characterization (dpeaa)DE-He213 optoelectronic materials (dpeaa)DE-He213 photovoltaic materials (dpeaa)DE-He213 semiconductor processing (dpeaa)DE-He213 II–VI semiconductors (dpeaa)DE-He213 Benson, J. D. aut Smith, P. J. aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 39(2010), 7 vom: 30. Apr., Seite 958-966 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:39 year:2010 number:7 day:30 month:04 pages:958-966 https://dx.doi.org/10.1007/s11664-010-1147-y 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 39 2010 7 30 04 958-966 |
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10.1007/s11664-010-1147-y doi (DE-627)SPR021492778 (SPR)s11664-010-1147-y-e DE-627 ger DE-627 rakwb eng Stoltz, A. J. verfasserin aut Effects of HgCdTe on the Optical Emission of Inductively Coupled Plasmas 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © US Army RDECOM CERDEC NVESD 2010 Abstract Inductively coupled plasmas (ICP) are the high-density plasmas of choice for processing HgCdTe and related compounds. Real-time examination of the ICP plasmas used to process HgCdTe would be desirable. In this preliminary study, the feasibility of using optical emission spectroscopy (OES) of ICP plasma used for processing HgCdTe has been examined. We have examined the utility of OES as a real-time diagnostic tool for HgCdTe device fabrication. In this preliminary study it has been found that mercury and cadmium can be detected but are dependent on several factors: sample area, material composition, etch rate, sample temperature, photoresist area, and plasma power. Furthermore, we found strong correlation between the amount of hydrogen detected by OES for samples with photoresist versus samples without photoresist while processing with hydrogen-based plasma. Hydrogen emission intensity decreased dramatically in samples with photoresist, contrary to the theory that photoresist adds hydrogen to the plasma effluent. It appears that hydrogen complexes with photoresist, reducing the global amount of hydrogen during the process. Furthermore, this phenomena may help to explain macroloading issues whereby additional photoresist area slowed HgCdTe, CdTe, and photoresist etch rates. Optical characterization (dpeaa)DE-He213 optoelectronic materials (dpeaa)DE-He213 photovoltaic materials (dpeaa)DE-He213 semiconductor processing (dpeaa)DE-He213 II–VI semiconductors (dpeaa)DE-He213 Benson, J. D. aut Smith, P. J. aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 39(2010), 7 vom: 30. Apr., Seite 958-966 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:39 year:2010 number:7 day:30 month:04 pages:958-966 https://dx.doi.org/10.1007/s11664-010-1147-y 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 39 2010 7 30 04 958-966 |
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10.1007/s11664-010-1147-y doi (DE-627)SPR021492778 (SPR)s11664-010-1147-y-e DE-627 ger DE-627 rakwb eng Stoltz, A. J. verfasserin aut Effects of HgCdTe on the Optical Emission of Inductively Coupled Plasmas 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © US Army RDECOM CERDEC NVESD 2010 Abstract Inductively coupled plasmas (ICP) are the high-density plasmas of choice for processing HgCdTe and related compounds. Real-time examination of the ICP plasmas used to process HgCdTe would be desirable. In this preliminary study, the feasibility of using optical emission spectroscopy (OES) of ICP plasma used for processing HgCdTe has been examined. We have examined the utility of OES as a real-time diagnostic tool for HgCdTe device fabrication. In this preliminary study it has been found that mercury and cadmium can be detected but are dependent on several factors: sample area, material composition, etch rate, sample temperature, photoresist area, and plasma power. Furthermore, we found strong correlation between the amount of hydrogen detected by OES for samples with photoresist versus samples without photoresist while processing with hydrogen-based plasma. Hydrogen emission intensity decreased dramatically in samples with photoresist, contrary to the theory that photoresist adds hydrogen to the plasma effluent. It appears that hydrogen complexes with photoresist, reducing the global amount of hydrogen during the process. Furthermore, this phenomena may help to explain macroloading issues whereby additional photoresist area slowed HgCdTe, CdTe, and photoresist etch rates. Optical characterization (dpeaa)DE-He213 optoelectronic materials (dpeaa)DE-He213 photovoltaic materials (dpeaa)DE-He213 semiconductor processing (dpeaa)DE-He213 II–VI semiconductors (dpeaa)DE-He213 Benson, J. D. aut Smith, P. J. aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 39(2010), 7 vom: 30. Apr., Seite 958-966 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:39 year:2010 number:7 day:30 month:04 pages:958-966 https://dx.doi.org/10.1007/s11664-010-1147-y 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 39 2010 7 30 04 958-966 |
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10.1007/s11664-010-1147-y doi (DE-627)SPR021492778 (SPR)s11664-010-1147-y-e DE-627 ger DE-627 rakwb eng Stoltz, A. J. verfasserin aut Effects of HgCdTe on the Optical Emission of Inductively Coupled Plasmas 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © US Army RDECOM CERDEC NVESD 2010 Abstract Inductively coupled plasmas (ICP) are the high-density plasmas of choice for processing HgCdTe and related compounds. Real-time examination of the ICP plasmas used to process HgCdTe would be desirable. In this preliminary study, the feasibility of using optical emission spectroscopy (OES) of ICP plasma used for processing HgCdTe has been examined. We have examined the utility of OES as a real-time diagnostic tool for HgCdTe device fabrication. In this preliminary study it has been found that mercury and cadmium can be detected but are dependent on several factors: sample area, material composition, etch rate, sample temperature, photoresist area, and plasma power. Furthermore, we found strong correlation between the amount of hydrogen detected by OES for samples with photoresist versus samples without photoresist while processing with hydrogen-based plasma. Hydrogen emission intensity decreased dramatically in samples with photoresist, contrary to the theory that photoresist adds hydrogen to the plasma effluent. It appears that hydrogen complexes with photoresist, reducing the global amount of hydrogen during the process. Furthermore, this phenomena may help to explain macroloading issues whereby additional photoresist area slowed HgCdTe, CdTe, and photoresist etch rates. Optical characterization (dpeaa)DE-He213 optoelectronic materials (dpeaa)DE-He213 photovoltaic materials (dpeaa)DE-He213 semiconductor processing (dpeaa)DE-He213 II–VI semiconductors (dpeaa)DE-He213 Benson, J. D. aut Smith, P. J. aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 39(2010), 7 vom: 30. Apr., Seite 958-966 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:39 year:2010 number:7 day:30 month:04 pages:958-966 https://dx.doi.org/10.1007/s11664-010-1147-y 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 39 2010 7 30 04 958-966 |
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10.1007/s11664-010-1147-y doi (DE-627)SPR021492778 (SPR)s11664-010-1147-y-e DE-627 ger DE-627 rakwb eng Stoltz, A. J. verfasserin aut Effects of HgCdTe on the Optical Emission of Inductively Coupled Plasmas 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © US Army RDECOM CERDEC NVESD 2010 Abstract Inductively coupled plasmas (ICP) are the high-density plasmas of choice for processing HgCdTe and related compounds. Real-time examination of the ICP plasmas used to process HgCdTe would be desirable. In this preliminary study, the feasibility of using optical emission spectroscopy (OES) of ICP plasma used for processing HgCdTe has been examined. We have examined the utility of OES as a real-time diagnostic tool for HgCdTe device fabrication. In this preliminary study it has been found that mercury and cadmium can be detected but are dependent on several factors: sample area, material composition, etch rate, sample temperature, photoresist area, and plasma power. Furthermore, we found strong correlation between the amount of hydrogen detected by OES for samples with photoresist versus samples without photoresist while processing with hydrogen-based plasma. Hydrogen emission intensity decreased dramatically in samples with photoresist, contrary to the theory that photoresist adds hydrogen to the plasma effluent. It appears that hydrogen complexes with photoresist, reducing the global amount of hydrogen during the process. Furthermore, this phenomena may help to explain macroloading issues whereby additional photoresist area slowed HgCdTe, CdTe, and photoresist etch rates. Optical characterization (dpeaa)DE-He213 optoelectronic materials (dpeaa)DE-He213 photovoltaic materials (dpeaa)DE-He213 semiconductor processing (dpeaa)DE-He213 II–VI semiconductors (dpeaa)DE-He213 Benson, J. D. aut Smith, P. J. aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 39(2010), 7 vom: 30. Apr., Seite 958-966 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:39 year:2010 number:7 day:30 month:04 pages:958-966 https://dx.doi.org/10.1007/s11664-010-1147-y 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 39 2010 7 30 04 958-966 |
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Stoltz, A. J. |
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Stoltz, A. J. misc Optical characterization misc optoelectronic materials misc photovoltaic materials misc semiconductor processing misc II–VI semiconductors Effects of HgCdTe on the Optical Emission of Inductively Coupled Plasmas |
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Effects of HgCdTe on the Optical Emission of Inductively Coupled Plasmas Optical characterization (dpeaa)DE-He213 optoelectronic materials (dpeaa)DE-He213 photovoltaic materials (dpeaa)DE-He213 semiconductor processing (dpeaa)DE-He213 II–VI semiconductors (dpeaa)DE-He213 |
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Effects of HgCdTe on the Optical Emission of Inductively Coupled Plasmas |
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Effects of HgCdTe on the Optical Emission of Inductively Coupled Plasmas |
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Stoltz, A. J. Benson, J. D. Smith, P. J. |
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effects of hgcdte on the optical emission of inductively coupled plasmas |
| title_auth |
Effects of HgCdTe on the Optical Emission of Inductively Coupled Plasmas |
| abstract |
Abstract Inductively coupled plasmas (ICP) are the high-density plasmas of choice for processing HgCdTe and related compounds. Real-time examination of the ICP plasmas used to process HgCdTe would be desirable. In this preliminary study, the feasibility of using optical emission spectroscopy (OES) of ICP plasma used for processing HgCdTe has been examined. We have examined the utility of OES as a real-time diagnostic tool for HgCdTe device fabrication. In this preliminary study it has been found that mercury and cadmium can be detected but are dependent on several factors: sample area, material composition, etch rate, sample temperature, photoresist area, and plasma power. Furthermore, we found strong correlation between the amount of hydrogen detected by OES for samples with photoresist versus samples without photoresist while processing with hydrogen-based plasma. Hydrogen emission intensity decreased dramatically in samples with photoresist, contrary to the theory that photoresist adds hydrogen to the plasma effluent. It appears that hydrogen complexes with photoresist, reducing the global amount of hydrogen during the process. Furthermore, this phenomena may help to explain macroloading issues whereby additional photoresist area slowed HgCdTe, CdTe, and photoresist etch rates. © US Army RDECOM CERDEC NVESD 2010 |
| abstractGer |
Abstract Inductively coupled plasmas (ICP) are the high-density plasmas of choice for processing HgCdTe and related compounds. Real-time examination of the ICP plasmas used to process HgCdTe would be desirable. In this preliminary study, the feasibility of using optical emission spectroscopy (OES) of ICP plasma used for processing HgCdTe has been examined. We have examined the utility of OES as a real-time diagnostic tool for HgCdTe device fabrication. In this preliminary study it has been found that mercury and cadmium can be detected but are dependent on several factors: sample area, material composition, etch rate, sample temperature, photoresist area, and plasma power. Furthermore, we found strong correlation between the amount of hydrogen detected by OES for samples with photoresist versus samples without photoresist while processing with hydrogen-based plasma. Hydrogen emission intensity decreased dramatically in samples with photoresist, contrary to the theory that photoresist adds hydrogen to the plasma effluent. It appears that hydrogen complexes with photoresist, reducing the global amount of hydrogen during the process. Furthermore, this phenomena may help to explain macroloading issues whereby additional photoresist area slowed HgCdTe, CdTe, and photoresist etch rates. © US Army RDECOM CERDEC NVESD 2010 |
| abstract_unstemmed |
Abstract Inductively coupled plasmas (ICP) are the high-density plasmas of choice for processing HgCdTe and related compounds. Real-time examination of the ICP plasmas used to process HgCdTe would be desirable. In this preliminary study, the feasibility of using optical emission spectroscopy (OES) of ICP plasma used for processing HgCdTe has been examined. We have examined the utility of OES as a real-time diagnostic tool for HgCdTe device fabrication. In this preliminary study it has been found that mercury and cadmium can be detected but are dependent on several factors: sample area, material composition, etch rate, sample temperature, photoresist area, and plasma power. Furthermore, we found strong correlation between the amount of hydrogen detected by OES for samples with photoresist versus samples without photoresist while processing with hydrogen-based plasma. Hydrogen emission intensity decreased dramatically in samples with photoresist, contrary to the theory that photoresist adds hydrogen to the plasma effluent. It appears that hydrogen complexes with photoresist, reducing the global amount of hydrogen during the process. Furthermore, this phenomena may help to explain macroloading issues whereby additional photoresist area slowed HgCdTe, CdTe, and photoresist etch rates. © US Army RDECOM CERDEC NVESD 2010 |
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Effects of HgCdTe on the Optical Emission of Inductively Coupled Plasmas |
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|
| score |
7.399913 |