The effect of Ti adhesion layer on the thermoelectric noise of a high resolution thermopile for nanowatt heat flux sensor
Abstract The effect of Ti adhesion layer on the thermoelectric noise of Microelectromechanical system (MEMS) thermopile sensor is investigated in this study. Although the adhesion layer does not affect the thermoelectric voltage through the Seebeck effect, it can influence the thermoelectric noise....
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Nam, Sung-Ki [verfasserIn] Lee, Sun-Kyu [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2014 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: International journal of precision engineering and manufacturing - Sŏul : KSPE, 2009, 15(2014), 11 vom: Nov., Seite 2391-2396 |
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| Übergeordnetes Werk: |
volume:15 ; year:2014 ; number:11 ; month:11 ; pages:2391-2396 |
| Links: |
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| DOI / URN: |
10.1007/s12541-014-0605-5 |
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| Katalog-ID: |
SPR026094088 |
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| 245 | 1 | 4 | |a The effect of Ti adhesion layer on the thermoelectric noise of a high resolution thermopile for nanowatt heat flux sensor |
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| 520 | |a Abstract The effect of Ti adhesion layer on the thermoelectric noise of Microelectromechanical system (MEMS) thermopile sensor is investigated in this study. Although the adhesion layer does not affect the thermoelectric voltage through the Seebeck effect, it can influence the thermoelectric noise. Two kinds of samples are prepared, both with and without Ti adhesion layers between the contact junctions of thermopile which are patterned with the 30-array of Au and Cr (Gold-chromium). The Ti layer is used to provide adhesion to the gold film. The surface contact resistance is evaluated by the geometric resistance obtained from a FEM model. These experiments show that the adhesion contact thermopile results in total resistance of 32.64 kΩ and noise amplitude of 313 μV, whereas the direct contact thermopile results in 24.49 kΩ and 187 μV, respectively. The surface of the contact junction are inspected with scanning electron microscopy(SEM), and atomic force microscopy(AFM) to investigate how the Ti adhesion layer affects the increment of the surface contact resistance. Furthermore, a heat flux sensor fabricated with the direct contact junctions of the thermopile achieves sensitivity of 62.9 mV/nW and resolution of 1 nW. | ||
| 650 | 4 | |a Nanowatt heat flux sensor |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Thermopile |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Thermoelectric noise |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Surface contact resistance |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Lee, Sun-Kyu |e verfasserin |4 aut | |
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10.1007/s12541-014-0605-5 doi (DE-627)SPR026094088 (SPR)s12541-014-0605-5-e DE-627 ger DE-627 rakwb eng 600 ASE Nam, Sung-Ki verfasserin aut The effect of Ti adhesion layer on the thermoelectric noise of a high resolution thermopile for nanowatt heat flux sensor 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The effect of Ti adhesion layer on the thermoelectric noise of Microelectromechanical system (MEMS) thermopile sensor is investigated in this study. Although the adhesion layer does not affect the thermoelectric voltage through the Seebeck effect, it can influence the thermoelectric noise. Two kinds of samples are prepared, both with and without Ti adhesion layers between the contact junctions of thermopile which are patterned with the 30-array of Au and Cr (Gold-chromium). The Ti layer is used to provide adhesion to the gold film. The surface contact resistance is evaluated by the geometric resistance obtained from a FEM model. These experiments show that the adhesion contact thermopile results in total resistance of 32.64 kΩ and noise amplitude of 313 μV, whereas the direct contact thermopile results in 24.49 kΩ and 187 μV, respectively. The surface of the contact junction are inspected with scanning electron microscopy(SEM), and atomic force microscopy(AFM) to investigate how the Ti adhesion layer affects the increment of the surface contact resistance. Furthermore, a heat flux sensor fabricated with the direct contact junctions of the thermopile achieves sensitivity of 62.9 mV/nW and resolution of 1 nW. Nanowatt heat flux sensor (dpeaa)DE-He213 Thermopile (dpeaa)DE-He213 Thermoelectric noise (dpeaa)DE-He213 Surface contact resistance (dpeaa)DE-He213 Lee, Sun-Kyu verfasserin aut Enthalten in International journal of precision engineering and manufacturing Sŏul : KSPE, 2009 15(2014), 11 vom: Nov., Seite 2391-2396 (DE-627)609403109 (DE-600)2515436-9 2005-4602 nnns volume:15 year:2014 number:11 month:11 pages:2391-2396 https://dx.doi.org/10.1007/s12541-014-0605-5 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 15 2014 11 11 2391-2396 |
| spelling |
10.1007/s12541-014-0605-5 doi (DE-627)SPR026094088 (SPR)s12541-014-0605-5-e DE-627 ger DE-627 rakwb eng 600 ASE Nam, Sung-Ki verfasserin aut The effect of Ti adhesion layer on the thermoelectric noise of a high resolution thermopile for nanowatt heat flux sensor 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The effect of Ti adhesion layer on the thermoelectric noise of Microelectromechanical system (MEMS) thermopile sensor is investigated in this study. Although the adhesion layer does not affect the thermoelectric voltage through the Seebeck effect, it can influence the thermoelectric noise. Two kinds of samples are prepared, both with and without Ti adhesion layers between the contact junctions of thermopile which are patterned with the 30-array of Au and Cr (Gold-chromium). The Ti layer is used to provide adhesion to the gold film. The surface contact resistance is evaluated by the geometric resistance obtained from a FEM model. These experiments show that the adhesion contact thermopile results in total resistance of 32.64 kΩ and noise amplitude of 313 μV, whereas the direct contact thermopile results in 24.49 kΩ and 187 μV, respectively. The surface of the contact junction are inspected with scanning electron microscopy(SEM), and atomic force microscopy(AFM) to investigate how the Ti adhesion layer affects the increment of the surface contact resistance. Furthermore, a heat flux sensor fabricated with the direct contact junctions of the thermopile achieves sensitivity of 62.9 mV/nW and resolution of 1 nW. Nanowatt heat flux sensor (dpeaa)DE-He213 Thermopile (dpeaa)DE-He213 Thermoelectric noise (dpeaa)DE-He213 Surface contact resistance (dpeaa)DE-He213 Lee, Sun-Kyu verfasserin aut Enthalten in International journal of precision engineering and manufacturing Sŏul : KSPE, 2009 15(2014), 11 vom: Nov., Seite 2391-2396 (DE-627)609403109 (DE-600)2515436-9 2005-4602 nnns volume:15 year:2014 number:11 month:11 pages:2391-2396 https://dx.doi.org/10.1007/s12541-014-0605-5 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 15 2014 11 11 2391-2396 |
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10.1007/s12541-014-0605-5 doi (DE-627)SPR026094088 (SPR)s12541-014-0605-5-e DE-627 ger DE-627 rakwb eng 600 ASE Nam, Sung-Ki verfasserin aut The effect of Ti adhesion layer on the thermoelectric noise of a high resolution thermopile for nanowatt heat flux sensor 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The effect of Ti adhesion layer on the thermoelectric noise of Microelectromechanical system (MEMS) thermopile sensor is investigated in this study. Although the adhesion layer does not affect the thermoelectric voltage through the Seebeck effect, it can influence the thermoelectric noise. Two kinds of samples are prepared, both with and without Ti adhesion layers between the contact junctions of thermopile which are patterned with the 30-array of Au and Cr (Gold-chromium). The Ti layer is used to provide adhesion to the gold film. The surface contact resistance is evaluated by the geometric resistance obtained from a FEM model. These experiments show that the adhesion contact thermopile results in total resistance of 32.64 kΩ and noise amplitude of 313 μV, whereas the direct contact thermopile results in 24.49 kΩ and 187 μV, respectively. The surface of the contact junction are inspected with scanning electron microscopy(SEM), and atomic force microscopy(AFM) to investigate how the Ti adhesion layer affects the increment of the surface contact resistance. Furthermore, a heat flux sensor fabricated with the direct contact junctions of the thermopile achieves sensitivity of 62.9 mV/nW and resolution of 1 nW. Nanowatt heat flux sensor (dpeaa)DE-He213 Thermopile (dpeaa)DE-He213 Thermoelectric noise (dpeaa)DE-He213 Surface contact resistance (dpeaa)DE-He213 Lee, Sun-Kyu verfasserin aut Enthalten in International journal of precision engineering and manufacturing Sŏul : KSPE, 2009 15(2014), 11 vom: Nov., Seite 2391-2396 (DE-627)609403109 (DE-600)2515436-9 2005-4602 nnns volume:15 year:2014 number:11 month:11 pages:2391-2396 https://dx.doi.org/10.1007/s12541-014-0605-5 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 15 2014 11 11 2391-2396 |
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10.1007/s12541-014-0605-5 doi (DE-627)SPR026094088 (SPR)s12541-014-0605-5-e DE-627 ger DE-627 rakwb eng 600 ASE Nam, Sung-Ki verfasserin aut The effect of Ti adhesion layer on the thermoelectric noise of a high resolution thermopile for nanowatt heat flux sensor 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The effect of Ti adhesion layer on the thermoelectric noise of Microelectromechanical system (MEMS) thermopile sensor is investigated in this study. Although the adhesion layer does not affect the thermoelectric voltage through the Seebeck effect, it can influence the thermoelectric noise. Two kinds of samples are prepared, both with and without Ti adhesion layers between the contact junctions of thermopile which are patterned with the 30-array of Au and Cr (Gold-chromium). The Ti layer is used to provide adhesion to the gold film. The surface contact resistance is evaluated by the geometric resistance obtained from a FEM model. These experiments show that the adhesion contact thermopile results in total resistance of 32.64 kΩ and noise amplitude of 313 μV, whereas the direct contact thermopile results in 24.49 kΩ and 187 μV, respectively. The surface of the contact junction are inspected with scanning electron microscopy(SEM), and atomic force microscopy(AFM) to investigate how the Ti adhesion layer affects the increment of the surface contact resistance. Furthermore, a heat flux sensor fabricated with the direct contact junctions of the thermopile achieves sensitivity of 62.9 mV/nW and resolution of 1 nW. Nanowatt heat flux sensor (dpeaa)DE-He213 Thermopile (dpeaa)DE-He213 Thermoelectric noise (dpeaa)DE-He213 Surface contact resistance (dpeaa)DE-He213 Lee, Sun-Kyu verfasserin aut Enthalten in International journal of precision engineering and manufacturing Sŏul : KSPE, 2009 15(2014), 11 vom: Nov., Seite 2391-2396 (DE-627)609403109 (DE-600)2515436-9 2005-4602 nnns volume:15 year:2014 number:11 month:11 pages:2391-2396 https://dx.doi.org/10.1007/s12541-014-0605-5 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 15 2014 11 11 2391-2396 |
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10.1007/s12541-014-0605-5 doi (DE-627)SPR026094088 (SPR)s12541-014-0605-5-e DE-627 ger DE-627 rakwb eng 600 ASE Nam, Sung-Ki verfasserin aut The effect of Ti adhesion layer on the thermoelectric noise of a high resolution thermopile for nanowatt heat flux sensor 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The effect of Ti adhesion layer on the thermoelectric noise of Microelectromechanical system (MEMS) thermopile sensor is investigated in this study. Although the adhesion layer does not affect the thermoelectric voltage through the Seebeck effect, it can influence the thermoelectric noise. Two kinds of samples are prepared, both with and without Ti adhesion layers between the contact junctions of thermopile which are patterned with the 30-array of Au and Cr (Gold-chromium). The Ti layer is used to provide adhesion to the gold film. The surface contact resistance is evaluated by the geometric resistance obtained from a FEM model. These experiments show that the adhesion contact thermopile results in total resistance of 32.64 kΩ and noise amplitude of 313 μV, whereas the direct contact thermopile results in 24.49 kΩ and 187 μV, respectively. The surface of the contact junction are inspected with scanning electron microscopy(SEM), and atomic force microscopy(AFM) to investigate how the Ti adhesion layer affects the increment of the surface contact resistance. Furthermore, a heat flux sensor fabricated with the direct contact junctions of the thermopile achieves sensitivity of 62.9 mV/nW and resolution of 1 nW. Nanowatt heat flux sensor (dpeaa)DE-He213 Thermopile (dpeaa)DE-He213 Thermoelectric noise (dpeaa)DE-He213 Surface contact resistance (dpeaa)DE-He213 Lee, Sun-Kyu verfasserin aut Enthalten in International journal of precision engineering and manufacturing Sŏul : KSPE, 2009 15(2014), 11 vom: Nov., Seite 2391-2396 (DE-627)609403109 (DE-600)2515436-9 2005-4602 nnns volume:15 year:2014 number:11 month:11 pages:2391-2396 https://dx.doi.org/10.1007/s12541-014-0605-5 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 15 2014 11 11 2391-2396 |
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Enthalten in International journal of precision engineering and manufacturing 15(2014), 11 vom: Nov., Seite 2391-2396 volume:15 year:2014 number:11 month:11 pages:2391-2396 |
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International journal of precision engineering and manufacturing |
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Nam, Sung-Ki @@aut@@ Lee, Sun-Kyu @@aut@@ |
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Although the adhesion layer does not affect the thermoelectric voltage through the Seebeck effect, it can influence the thermoelectric noise. Two kinds of samples are prepared, both with and without Ti adhesion layers between the contact junctions of thermopile which are patterned with the 30-array of Au and Cr (Gold-chromium). The Ti layer is used to provide adhesion to the gold film. The surface contact resistance is evaluated by the geometric resistance obtained from a FEM model. These experiments show that the adhesion contact thermopile results in total resistance of 32.64 kΩ and noise amplitude of 313 μV, whereas the direct contact thermopile results in 24.49 kΩ and 187 μV, respectively. The surface of the contact junction are inspected with scanning electron microscopy(SEM), and atomic force microscopy(AFM) to investigate how the Ti adhesion layer affects the increment of the surface contact resistance. 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Nam, Sung-Ki |
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Nam, Sung-Ki ddc 600 misc Nanowatt heat flux sensor misc Thermopile misc Thermoelectric noise misc Surface contact resistance The effect of Ti adhesion layer on the thermoelectric noise of a high resolution thermopile for nanowatt heat flux sensor |
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600 ASE The effect of Ti adhesion layer on the thermoelectric noise of a high resolution thermopile for nanowatt heat flux sensor Nanowatt heat flux sensor (dpeaa)DE-He213 Thermopile (dpeaa)DE-He213 Thermoelectric noise (dpeaa)DE-He213 Surface contact resistance (dpeaa)DE-He213 |
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ddc 600 misc Nanowatt heat flux sensor misc Thermopile misc Thermoelectric noise misc Surface contact resistance |
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The effect of Ti adhesion layer on the thermoelectric noise of a high resolution thermopile for nanowatt heat flux sensor |
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The effect of Ti adhesion layer on the thermoelectric noise of a high resolution thermopile for nanowatt heat flux sensor |
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Nam, Sung-Ki |
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International journal of precision engineering and manufacturing |
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Nam, Sung-Ki Lee, Sun-Kyu |
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effect of ti adhesion layer on the thermoelectric noise of a high resolution thermopile for nanowatt heat flux sensor |
| title_auth |
The effect of Ti adhesion layer on the thermoelectric noise of a high resolution thermopile for nanowatt heat flux sensor |
| abstract |
Abstract The effect of Ti adhesion layer on the thermoelectric noise of Microelectromechanical system (MEMS) thermopile sensor is investigated in this study. Although the adhesion layer does not affect the thermoelectric voltage through the Seebeck effect, it can influence the thermoelectric noise. Two kinds of samples are prepared, both with and without Ti adhesion layers between the contact junctions of thermopile which are patterned with the 30-array of Au and Cr (Gold-chromium). The Ti layer is used to provide adhesion to the gold film. The surface contact resistance is evaluated by the geometric resistance obtained from a FEM model. These experiments show that the adhesion contact thermopile results in total resistance of 32.64 kΩ and noise amplitude of 313 μV, whereas the direct contact thermopile results in 24.49 kΩ and 187 μV, respectively. The surface of the contact junction are inspected with scanning electron microscopy(SEM), and atomic force microscopy(AFM) to investigate how the Ti adhesion layer affects the increment of the surface contact resistance. Furthermore, a heat flux sensor fabricated with the direct contact junctions of the thermopile achieves sensitivity of 62.9 mV/nW and resolution of 1 nW. |
| abstractGer |
Abstract The effect of Ti adhesion layer on the thermoelectric noise of Microelectromechanical system (MEMS) thermopile sensor is investigated in this study. Although the adhesion layer does not affect the thermoelectric voltage through the Seebeck effect, it can influence the thermoelectric noise. Two kinds of samples are prepared, both with and without Ti adhesion layers between the contact junctions of thermopile which are patterned with the 30-array of Au and Cr (Gold-chromium). The Ti layer is used to provide adhesion to the gold film. The surface contact resistance is evaluated by the geometric resistance obtained from a FEM model. These experiments show that the adhesion contact thermopile results in total resistance of 32.64 kΩ and noise amplitude of 313 μV, whereas the direct contact thermopile results in 24.49 kΩ and 187 μV, respectively. The surface of the contact junction are inspected with scanning electron microscopy(SEM), and atomic force microscopy(AFM) to investigate how the Ti adhesion layer affects the increment of the surface contact resistance. Furthermore, a heat flux sensor fabricated with the direct contact junctions of the thermopile achieves sensitivity of 62.9 mV/nW and resolution of 1 nW. |
| abstract_unstemmed |
Abstract The effect of Ti adhesion layer on the thermoelectric noise of Microelectromechanical system (MEMS) thermopile sensor is investigated in this study. Although the adhesion layer does not affect the thermoelectric voltage through the Seebeck effect, it can influence the thermoelectric noise. Two kinds of samples are prepared, both with and without Ti adhesion layers between the contact junctions of thermopile which are patterned with the 30-array of Au and Cr (Gold-chromium). The Ti layer is used to provide adhesion to the gold film. The surface contact resistance is evaluated by the geometric resistance obtained from a FEM model. These experiments show that the adhesion contact thermopile results in total resistance of 32.64 kΩ and noise amplitude of 313 μV, whereas the direct contact thermopile results in 24.49 kΩ and 187 μV, respectively. The surface of the contact junction are inspected with scanning electron microscopy(SEM), and atomic force microscopy(AFM) to investigate how the Ti adhesion layer affects the increment of the surface contact resistance. Furthermore, a heat flux sensor fabricated with the direct contact junctions of the thermopile achieves sensitivity of 62.9 mV/nW and resolution of 1 nW. |
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| title_short |
The effect of Ti adhesion layer on the thermoelectric noise of a high resolution thermopile for nanowatt heat flux sensor |
| url |
https://dx.doi.org/10.1007/s12541-014-0605-5 |
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| author2 |
Lee, Sun-Kyu |
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Lee, Sun-Kyu |
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| doi_str |
10.1007/s12541-014-0605-5 |
| up_date |
2024-07-03T18:51:02.821Z |
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