The Seebeck Coefficient of Insulators: Electrochemical Potential
Abstract We discuss the theory behind low-temperature measurement of the Seebeck coefficient in materials with few electrons, such as insulators and lightly doped semiconductors. The Seebeck coefficient is defined thermodynamically as being related to the electrochemical potential. However, the meas...
Ausführliche Beschreibung
Autor*in: |
Mahan, G.D. [verfasserIn] |
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Format: |
Artikel |
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Sprache: |
Englisch |
Erschienen: |
2015 |
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Schlagwörter: |
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Anmerkung: |
© The Minerals, Metals & Materials Society 2015 |
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Übergeordnetes Werk: |
Enthalten in: Journal of electronic materials - Springer US, 1972, 45(2015), 3 vom: 28. Aug., Seite 1257-1259 |
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Übergeordnetes Werk: |
volume:45 ; year:2015 ; number:3 ; day:28 ; month:08 ; pages:1257-1259 |
Links: |
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DOI / URN: |
10.1007/s11664-015-3986-z |
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Katalog-ID: |
OLC2042343390 |
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10.1007/s11664-015-3986-z doi (DE-627)OLC2042343390 (DE-He213)s11664-015-3986-z-p DE-627 ger DE-627 rakwb eng 670 VZ Mahan, G.D. verfasserin aut The Seebeck Coefficient of Insulators: Electrochemical Potential 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © The Minerals, Metals & Materials Society 2015 Abstract We discuss the theory behind low-temperature measurement of the Seebeck coefficient in materials with few electrons, such as insulators and lightly doped semiconductors. The Seebeck coefficient is defined thermodynamically as being related to the electrochemical potential. However, the measurement is of the voltage for a material with no current, which is not the same as the gradient of the electrochemical potential. Seebeck transport Rayleigh electrochemical Enthalten in Journal of electronic materials Springer US, 1972 45(2015), 3 vom: 28. Aug., Seite 1257-1259 (DE-627)129398233 (DE-600)186069-0 (DE-576)014781387 0361-5235 nnns volume:45 year:2015 number:3 day:28 month:08 pages:1257-1259 https://doi.org/10.1007/s11664-015-3986-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_70 AR 45 2015 3 28 08 1257-1259 |
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10.1007/s11664-015-3986-z doi (DE-627)OLC2042343390 (DE-He213)s11664-015-3986-z-p DE-627 ger DE-627 rakwb eng 670 VZ Mahan, G.D. verfasserin aut The Seebeck Coefficient of Insulators: Electrochemical Potential 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © The Minerals, Metals & Materials Society 2015 Abstract We discuss the theory behind low-temperature measurement of the Seebeck coefficient in materials with few electrons, such as insulators and lightly doped semiconductors. The Seebeck coefficient is defined thermodynamically as being related to the electrochemical potential. However, the measurement is of the voltage for a material with no current, which is not the same as the gradient of the electrochemical potential. Seebeck transport Rayleigh electrochemical Enthalten in Journal of electronic materials Springer US, 1972 45(2015), 3 vom: 28. Aug., Seite 1257-1259 (DE-627)129398233 (DE-600)186069-0 (DE-576)014781387 0361-5235 nnns volume:45 year:2015 number:3 day:28 month:08 pages:1257-1259 https://doi.org/10.1007/s11664-015-3986-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_70 AR 45 2015 3 28 08 1257-1259 |
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10.1007/s11664-015-3986-z doi (DE-627)OLC2042343390 (DE-He213)s11664-015-3986-z-p DE-627 ger DE-627 rakwb eng 670 VZ Mahan, G.D. verfasserin aut The Seebeck Coefficient of Insulators: Electrochemical Potential 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © The Minerals, Metals & Materials Society 2015 Abstract We discuss the theory behind low-temperature measurement of the Seebeck coefficient in materials with few electrons, such as insulators and lightly doped semiconductors. The Seebeck coefficient is defined thermodynamically as being related to the electrochemical potential. However, the measurement is of the voltage for a material with no current, which is not the same as the gradient of the electrochemical potential. Seebeck transport Rayleigh electrochemical Enthalten in Journal of electronic materials Springer US, 1972 45(2015), 3 vom: 28. Aug., Seite 1257-1259 (DE-627)129398233 (DE-600)186069-0 (DE-576)014781387 0361-5235 nnns volume:45 year:2015 number:3 day:28 month:08 pages:1257-1259 https://doi.org/10.1007/s11664-015-3986-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_70 AR 45 2015 3 28 08 1257-1259 |
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10.1007/s11664-015-3986-z doi (DE-627)OLC2042343390 (DE-He213)s11664-015-3986-z-p DE-627 ger DE-627 rakwb eng 670 VZ Mahan, G.D. verfasserin aut The Seebeck Coefficient of Insulators: Electrochemical Potential 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © The Minerals, Metals & Materials Society 2015 Abstract We discuss the theory behind low-temperature measurement of the Seebeck coefficient in materials with few electrons, such as insulators and lightly doped semiconductors. The Seebeck coefficient is defined thermodynamically as being related to the electrochemical potential. However, the measurement is of the voltage for a material with no current, which is not the same as the gradient of the electrochemical potential. Seebeck transport Rayleigh electrochemical Enthalten in Journal of electronic materials Springer US, 1972 45(2015), 3 vom: 28. Aug., Seite 1257-1259 (DE-627)129398233 (DE-600)186069-0 (DE-576)014781387 0361-5235 nnns volume:45 year:2015 number:3 day:28 month:08 pages:1257-1259 https://doi.org/10.1007/s11664-015-3986-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_70 AR 45 2015 3 28 08 1257-1259 |
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10.1007/s11664-015-3986-z doi (DE-627)OLC2042343390 (DE-He213)s11664-015-3986-z-p DE-627 ger DE-627 rakwb eng 670 VZ Mahan, G.D. verfasserin aut The Seebeck Coefficient of Insulators: Electrochemical Potential 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © The Minerals, Metals & Materials Society 2015 Abstract We discuss the theory behind low-temperature measurement of the Seebeck coefficient in materials with few electrons, such as insulators and lightly doped semiconductors. The Seebeck coefficient is defined thermodynamically as being related to the electrochemical potential. However, the measurement is of the voltage for a material with no current, which is not the same as the gradient of the electrochemical potential. Seebeck transport Rayleigh electrochemical Enthalten in Journal of electronic materials Springer US, 1972 45(2015), 3 vom: 28. Aug., Seite 1257-1259 (DE-627)129398233 (DE-600)186069-0 (DE-576)014781387 0361-5235 nnns volume:45 year:2015 number:3 day:28 month:08 pages:1257-1259 https://doi.org/10.1007/s11664-015-3986-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_70 AR 45 2015 3 28 08 1257-1259 |
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Abstract We discuss the theory behind low-temperature measurement of the Seebeck coefficient in materials with few electrons, such as insulators and lightly doped semiconductors. The Seebeck coefficient is defined thermodynamically as being related to the electrochemical potential. However, the measurement is of the voltage for a material with no current, which is not the same as the gradient of the electrochemical potential. © The Minerals, Metals & Materials Society 2015 |
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Abstract We discuss the theory behind low-temperature measurement of the Seebeck coefficient in materials with few electrons, such as insulators and lightly doped semiconductors. The Seebeck coefficient is defined thermodynamically as being related to the electrochemical potential. However, the measurement is of the voltage for a material with no current, which is not the same as the gradient of the electrochemical potential. © The Minerals, Metals & Materials Society 2015 |
abstract_unstemmed |
Abstract We discuss the theory behind low-temperature measurement of the Seebeck coefficient in materials with few electrons, such as insulators and lightly doped semiconductors. The Seebeck coefficient is defined thermodynamically as being related to the electrochemical potential. However, the measurement is of the voltage for a material with no current, which is not the same as the gradient of the electrochemical potential. © The Minerals, Metals & Materials Society 2015 |
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