Thermo-electronic properties of the copper-oxide $ Cu_{6} %$ O_{8} %$ YCI_{1−x} %$ Br_{x} $
Abstract We report the thermal conductivity and the Seebeck coefficient of polycrystalline samples of $ Cu_{6} %$ O_{8} %$ YCl_{1−x} %$ Br_{x} $. The lattice constant a linearly increases with increasing $ Br^{−} $ concentration x, indicating an expansion of the $ Cu_{6} %$ O_{8} $ cage. At 350 K, t...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Kawashima, Kenji [verfasserIn] Takeda, Hiroki [verfasserIn] Tozawa, Hazuki [verfasserIn] Akimitsu, Jun [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2013 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Journal of the Korean Physical Society - Berlin : Springer, 1968, 63(2013), 3 vom: Aug., Seite 420-422 |
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| Übergeordnetes Werk: |
volume:63 ; year:2013 ; number:3 ; month:08 ; pages:420-422 |
| Links: |
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| DOI / URN: |
10.3938/jkps.63.420 |
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| Katalog-ID: |
SPR032704720 |
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| 100 | 1 | |a Kawashima, Kenji |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a Thermo-electronic properties of the copper-oxide $ Cu_{6} %$ O_{8} %$ YCI_{1−x} %$ Br_{x} $ |
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| 520 | |a Abstract We report the thermal conductivity and the Seebeck coefficient of polycrystalline samples of $ Cu_{6} %$ O_{8} %$ YCl_{1−x} %$ Br_{x} $. The lattice constant a linearly increases with increasing $ Br^{−} $ concentration x, indicating an expansion of the $ Cu_{6} %$ O_{8} $ cage. At 350 K, the thermal conductivity κ is small and undergoes very little change with x, suggesting the existence of an anharmonic vibration. On the other hand, the Seebeck coefficient S is enhanced by substituting $ Br^{−} $ for $ Cl^{−} $. These facts indicate that the thermoelectronic properties are sensitive to the $ Cu_{6} %$ O_{8} $ cage size in the $ Cu_{6} %$ O_{8} $YCl system. | ||
| 650 | 4 | |a Copper-oxide |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Thermoelectronic property |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Cu |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a O |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a YCl |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Br |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Takeda, Hiroki |e verfasserin |4 aut | |
| 700 | 1 | |a Tozawa, Hazuki |e verfasserin |4 aut | |
| 700 | 1 | |a Akimitsu, Jun |e verfasserin |4 aut | |
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| 856 | 4 | 0 | |u https://dx.doi.org/10.3938/jkps.63.420 |z lizenzpflichtig |3 Volltext |
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10.3938/jkps.63.420 doi (DE-627)SPR032704720 (SPR)jkps.63.420-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Kawashima, Kenji verfasserin aut Thermo-electronic properties of the copper-oxide $ Cu_{6} %$ O_{8} %$ YCI_{1−x} %$ Br_{x} $ 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We report the thermal conductivity and the Seebeck coefficient of polycrystalline samples of $ Cu_{6} %$ O_{8} %$ YCl_{1−x} %$ Br_{x} $. The lattice constant a linearly increases with increasing $ Br^{−} $ concentration x, indicating an expansion of the $ Cu_{6} %$ O_{8} $ cage. At 350 K, the thermal conductivity κ is small and undergoes very little change with x, suggesting the existence of an anharmonic vibration. On the other hand, the Seebeck coefficient S is enhanced by substituting $ Br^{−} $ for $ Cl^{−} $. These facts indicate that the thermoelectronic properties are sensitive to the $ Cu_{6} %$ O_{8} $ cage size in the $ Cu_{6} %$ O_{8} $YCl system. Copper-oxide (dpeaa)DE-He213 Thermoelectronic property (dpeaa)DE-He213 Cu (dpeaa)DE-He213 O (dpeaa)DE-He213 YCl (dpeaa)DE-He213 Br (dpeaa)DE-He213 Takeda, Hiroki verfasserin aut Tozawa, Hazuki verfasserin aut Akimitsu, Jun verfasserin aut Enthalten in Journal of the Korean Physical Society Berlin : Springer, 1968 63(2013), 3 vom: Aug., Seite 420-422 (DE-627)328820865 (DE-600)2046361-3 1976-8524 nnns volume:63 year:2013 number:3 month:08 pages:420-422 https://dx.doi.org/10.3938/jkps.63.420 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_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 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 33.00 ASE AR 63 2013 3 08 420-422 |
| spelling |
10.3938/jkps.63.420 doi (DE-627)SPR032704720 (SPR)jkps.63.420-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Kawashima, Kenji verfasserin aut Thermo-electronic properties of the copper-oxide $ Cu_{6} %$ O_{8} %$ YCI_{1−x} %$ Br_{x} $ 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We report the thermal conductivity and the Seebeck coefficient of polycrystalline samples of $ Cu_{6} %$ O_{8} %$ YCl_{1−x} %$ Br_{x} $. The lattice constant a linearly increases with increasing $ Br^{−} $ concentration x, indicating an expansion of the $ Cu_{6} %$ O_{8} $ cage. At 350 K, the thermal conductivity κ is small and undergoes very little change with x, suggesting the existence of an anharmonic vibration. On the other hand, the Seebeck coefficient S is enhanced by substituting $ Br^{−} $ for $ Cl^{−} $. These facts indicate that the thermoelectronic properties are sensitive to the $ Cu_{6} %$ O_{8} $ cage size in the $ Cu_{6} %$ O_{8} $YCl system. Copper-oxide (dpeaa)DE-He213 Thermoelectronic property (dpeaa)DE-He213 Cu (dpeaa)DE-He213 O (dpeaa)DE-He213 YCl (dpeaa)DE-He213 Br (dpeaa)DE-He213 Takeda, Hiroki verfasserin aut Tozawa, Hazuki verfasserin aut Akimitsu, Jun verfasserin aut Enthalten in Journal of the Korean Physical Society Berlin : Springer, 1968 63(2013), 3 vom: Aug., Seite 420-422 (DE-627)328820865 (DE-600)2046361-3 1976-8524 nnns volume:63 year:2013 number:3 month:08 pages:420-422 https://dx.doi.org/10.3938/jkps.63.420 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_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 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 33.00 ASE AR 63 2013 3 08 420-422 |
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10.3938/jkps.63.420 doi (DE-627)SPR032704720 (SPR)jkps.63.420-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Kawashima, Kenji verfasserin aut Thermo-electronic properties of the copper-oxide $ Cu_{6} %$ O_{8} %$ YCI_{1−x} %$ Br_{x} $ 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We report the thermal conductivity and the Seebeck coefficient of polycrystalline samples of $ Cu_{6} %$ O_{8} %$ YCl_{1−x} %$ Br_{x} $. The lattice constant a linearly increases with increasing $ Br^{−} $ concentration x, indicating an expansion of the $ Cu_{6} %$ O_{8} $ cage. At 350 K, the thermal conductivity κ is small and undergoes very little change with x, suggesting the existence of an anharmonic vibration. On the other hand, the Seebeck coefficient S is enhanced by substituting $ Br^{−} $ for $ Cl^{−} $. These facts indicate that the thermoelectronic properties are sensitive to the $ Cu_{6} %$ O_{8} $ cage size in the $ Cu_{6} %$ O_{8} $YCl system. Copper-oxide (dpeaa)DE-He213 Thermoelectronic property (dpeaa)DE-He213 Cu (dpeaa)DE-He213 O (dpeaa)DE-He213 YCl (dpeaa)DE-He213 Br (dpeaa)DE-He213 Takeda, Hiroki verfasserin aut Tozawa, Hazuki verfasserin aut Akimitsu, Jun verfasserin aut Enthalten in Journal of the Korean Physical Society Berlin : Springer, 1968 63(2013), 3 vom: Aug., Seite 420-422 (DE-627)328820865 (DE-600)2046361-3 1976-8524 nnns volume:63 year:2013 number:3 month:08 pages:420-422 https://dx.doi.org/10.3938/jkps.63.420 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_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 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 33.00 ASE AR 63 2013 3 08 420-422 |
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10.3938/jkps.63.420 doi (DE-627)SPR032704720 (SPR)jkps.63.420-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Kawashima, Kenji verfasserin aut Thermo-electronic properties of the copper-oxide $ Cu_{6} %$ O_{8} %$ YCI_{1−x} %$ Br_{x} $ 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We report the thermal conductivity and the Seebeck coefficient of polycrystalline samples of $ Cu_{6} %$ O_{8} %$ YCl_{1−x} %$ Br_{x} $. The lattice constant a linearly increases with increasing $ Br^{−} $ concentration x, indicating an expansion of the $ Cu_{6} %$ O_{8} $ cage. At 350 K, the thermal conductivity κ is small and undergoes very little change with x, suggesting the existence of an anharmonic vibration. On the other hand, the Seebeck coefficient S is enhanced by substituting $ Br^{−} $ for $ Cl^{−} $. These facts indicate that the thermoelectronic properties are sensitive to the $ Cu_{6} %$ O_{8} $ cage size in the $ Cu_{6} %$ O_{8} $YCl system. Copper-oxide (dpeaa)DE-He213 Thermoelectronic property (dpeaa)DE-He213 Cu (dpeaa)DE-He213 O (dpeaa)DE-He213 YCl (dpeaa)DE-He213 Br (dpeaa)DE-He213 Takeda, Hiroki verfasserin aut Tozawa, Hazuki verfasserin aut Akimitsu, Jun verfasserin aut Enthalten in Journal of the Korean Physical Society Berlin : Springer, 1968 63(2013), 3 vom: Aug., Seite 420-422 (DE-627)328820865 (DE-600)2046361-3 1976-8524 nnns volume:63 year:2013 number:3 month:08 pages:420-422 https://dx.doi.org/10.3938/jkps.63.420 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_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 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 33.00 ASE AR 63 2013 3 08 420-422 |
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10.3938/jkps.63.420 doi (DE-627)SPR032704720 (SPR)jkps.63.420-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Kawashima, Kenji verfasserin aut Thermo-electronic properties of the copper-oxide $ Cu_{6} %$ O_{8} %$ YCI_{1−x} %$ Br_{x} $ 2013 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We report the thermal conductivity and the Seebeck coefficient of polycrystalline samples of $ Cu_{6} %$ O_{8} %$ YCl_{1−x} %$ Br_{x} $. The lattice constant a linearly increases with increasing $ Br^{−} $ concentration x, indicating an expansion of the $ Cu_{6} %$ O_{8} $ cage. At 350 K, the thermal conductivity κ is small and undergoes very little change with x, suggesting the existence of an anharmonic vibration. On the other hand, the Seebeck coefficient S is enhanced by substituting $ Br^{−} $ for $ Cl^{−} $. These facts indicate that the thermoelectronic properties are sensitive to the $ Cu_{6} %$ O_{8} $ cage size in the $ Cu_{6} %$ O_{8} $YCl system. Copper-oxide (dpeaa)DE-He213 Thermoelectronic property (dpeaa)DE-He213 Cu (dpeaa)DE-He213 O (dpeaa)DE-He213 YCl (dpeaa)DE-He213 Br (dpeaa)DE-He213 Takeda, Hiroki verfasserin aut Tozawa, Hazuki verfasserin aut Akimitsu, Jun verfasserin aut Enthalten in Journal of the Korean Physical Society Berlin : Springer, 1968 63(2013), 3 vom: Aug., Seite 420-422 (DE-627)328820865 (DE-600)2046361-3 1976-8524 nnns volume:63 year:2013 number:3 month:08 pages:420-422 https://dx.doi.org/10.3938/jkps.63.420 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_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 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 33.00 ASE AR 63 2013 3 08 420-422 |
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English |
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Enthalten in Journal of the Korean Physical Society 63(2013), 3 vom: Aug., Seite 420-422 volume:63 year:2013 number:3 month:08 pages:420-422 |
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Enthalten in Journal of the Korean Physical Society 63(2013), 3 vom: Aug., Seite 420-422 volume:63 year:2013 number:3 month:08 pages:420-422 |
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findex.gbv.de |
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Copper-oxide Thermoelectronic property Cu O YCl Br |
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Journal of the Korean Physical Society |
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Kawashima, Kenji @@aut@@ Takeda, Hiroki @@aut@@ Tozawa, Hazuki @@aut@@ Akimitsu, Jun @@aut@@ |
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2013-08-01T00:00:00Z |
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328820865 |
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|
| author |
Kawashima, Kenji |
| spellingShingle |
Kawashima, Kenji ddc 530 bkl 33.00 misc Copper-oxide misc Thermoelectronic property misc Cu misc O misc YCl misc Br Thermo-electronic properties of the copper-oxide $ Cu_{6} %$ O_{8} %$ YCI_{1−x} %$ Br_{x} $ |
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Kawashima, Kenji |
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| topic_title |
530 ASE 33.00 bkl Thermo-electronic properties of the copper-oxide $ Cu_{6} %$ O_{8} %$ YCI_{1−x} %$ Br_{x} $ Copper-oxide (dpeaa)DE-He213 Thermoelectronic property (dpeaa)DE-He213 Cu (dpeaa)DE-He213 O (dpeaa)DE-He213 YCl (dpeaa)DE-He213 Br (dpeaa)DE-He213 |
| topic |
ddc 530 bkl 33.00 misc Copper-oxide misc Thermoelectronic property misc Cu misc O misc YCl misc Br |
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ddc 530 bkl 33.00 misc Copper-oxide misc Thermoelectronic property misc Cu misc O misc YCl misc Br |
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ddc 530 bkl 33.00 misc Copper-oxide misc Thermoelectronic property misc Cu misc O misc YCl misc Br |
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Elektronische Aufsätze Aufsätze Elektronische Ressource |
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Journal of the Korean Physical Society |
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Thermo-electronic properties of the copper-oxide $ Cu_{6} %$ O_{8} %$ YCI_{1−x} %$ Br_{x} $ |
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(DE-627)SPR032704720 (SPR)jkps.63.420-e |
| title_full |
Thermo-electronic properties of the copper-oxide $ Cu_{6} %$ O_{8} %$ YCI_{1−x} %$ Br_{x} $ |
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Kawashima, Kenji |
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Journal of the Korean Physical Society |
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2013 |
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420 |
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Kawashima, Kenji Takeda, Hiroki Tozawa, Hazuki Akimitsu, Jun |
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10.3938/jkps.63.420 |
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verfasserin |
| title_sort |
thermo-electronic properties of the copper-oxide $ cu_{6} %$ o_{8} %$ yci_{1−x} %$ br_{x} $ |
| title_auth |
Thermo-electronic properties of the copper-oxide $ Cu_{6} %$ O_{8} %$ YCI_{1−x} %$ Br_{x} $ |
| abstract |
Abstract We report the thermal conductivity and the Seebeck coefficient of polycrystalline samples of $ Cu_{6} %$ O_{8} %$ YCl_{1−x} %$ Br_{x} $. The lattice constant a linearly increases with increasing $ Br^{−} $ concentration x, indicating an expansion of the $ Cu_{6} %$ O_{8} $ cage. At 350 K, the thermal conductivity κ is small and undergoes very little change with x, suggesting the existence of an anharmonic vibration. On the other hand, the Seebeck coefficient S is enhanced by substituting $ Br^{−} $ for $ Cl^{−} $. These facts indicate that the thermoelectronic properties are sensitive to the $ Cu_{6} %$ O_{8} $ cage size in the $ Cu_{6} %$ O_{8} $YCl system. |
| abstractGer |
Abstract We report the thermal conductivity and the Seebeck coefficient of polycrystalline samples of $ Cu_{6} %$ O_{8} %$ YCl_{1−x} %$ Br_{x} $. The lattice constant a linearly increases with increasing $ Br^{−} $ concentration x, indicating an expansion of the $ Cu_{6} %$ O_{8} $ cage. At 350 K, the thermal conductivity κ is small and undergoes very little change with x, suggesting the existence of an anharmonic vibration. On the other hand, the Seebeck coefficient S is enhanced by substituting $ Br^{−} $ for $ Cl^{−} $. These facts indicate that the thermoelectronic properties are sensitive to the $ Cu_{6} %$ O_{8} $ cage size in the $ Cu_{6} %$ O_{8} $YCl system. |
| abstract_unstemmed |
Abstract We report the thermal conductivity and the Seebeck coefficient of polycrystalline samples of $ Cu_{6} %$ O_{8} %$ YCl_{1−x} %$ Br_{x} $. The lattice constant a linearly increases with increasing $ Br^{−} $ concentration x, indicating an expansion of the $ Cu_{6} %$ O_{8} $ cage. At 350 K, the thermal conductivity κ is small and undergoes very little change with x, suggesting the existence of an anharmonic vibration. On the other hand, the Seebeck coefficient S is enhanced by substituting $ Br^{−} $ for $ Cl^{−} $. These facts indicate that the thermoelectronic properties are sensitive to the $ Cu_{6} %$ O_{8} $ cage size in the $ Cu_{6} %$ O_{8} $YCl system. |
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3 |
| title_short |
Thermo-electronic properties of the copper-oxide $ Cu_{6} %$ O_{8} %$ YCI_{1−x} %$ Br_{x} $ |
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https://dx.doi.org/10.3938/jkps.63.420 |
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Takeda, Hiroki Tozawa, Hazuki Akimitsu, Jun |
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Takeda, Hiroki Tozawa, Hazuki Akimitsu, Jun |
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10.3938/jkps.63.420 |
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2024-07-03T14:17:50.190Z |
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|
| score |
7.39884 |