Thermoelectric properties of β-Zn4Sb3 doped with Sn
被引:32
作者:
Koyanagi, T
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Yamaguchi Univ, Fac Engn, Dept Elect & Elect Engn, Ube, Yamaguchi 755, JapanYamaguchi Univ, Fac Engn, Dept Elect & Elect Engn, Ube, Yamaguchi 755, Japan
Koyanagi, T
[1
]
Hino, K
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Yamaguchi Univ, Fac Engn, Dept Elect & Elect Engn, Ube, Yamaguchi 755, JapanYamaguchi Univ, Fac Engn, Dept Elect & Elect Engn, Ube, Yamaguchi 755, Japan
Hino, K
[1
]
Nagamoto, Y
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Yamaguchi Univ, Fac Engn, Dept Elect & Elect Engn, Ube, Yamaguchi 755, JapanYamaguchi Univ, Fac Engn, Dept Elect & Elect Engn, Ube, Yamaguchi 755, Japan
Nagamoto, Y
[1
]
Yoshitake, H
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Yamaguchi Univ, Fac Engn, Dept Elect & Elect Engn, Ube, Yamaguchi 755, JapanYamaguchi Univ, Fac Engn, Dept Elect & Elect Engn, Ube, Yamaguchi 755, Japan
Yoshitake, H
[1
]
Kishimoto, K
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Yamaguchi Univ, Fac Engn, Dept Elect & Elect Engn, Ube, Yamaguchi 755, JapanYamaguchi Univ, Fac Engn, Dept Elect & Elect Engn, Ube, Yamaguchi 755, Japan
Kishimoto, K
[1
]
机构:
[1] Yamaguchi Univ, Fac Engn, Dept Elect & Elect Engn, Ube, Yamaguchi 755, Japan
来源:
PROCEEDINGS ICT'97 - XVI INTERNATIONAL CONFERENCE ON THERMOELECTRICS
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1997年
关键词:
D O I:
10.1109/ICT.1997.667186
中图分类号:
O414.1 [热力学];
学科分类号:
摘要:
We have tried to dope beta-Zn4Sb3 with Sn for the purpose of the p-type doping and the enhancement of phonon scattering, which further improve the thermoelectric properties of beta-Zn4Sb3. Polycrystalline samples doped with Sn were prepared by the spark plasma sintering method Although no other phase was observed except for beta-Zn4Sb3 in Sn-doped samples up to 3%, their lattice constants were not at all changed from that of bulk beta-Zn4Sb3, indicating that Sn was not unfortunately substituted for Sb. These results suggest that microcrystals of Sn is dispersed in grain boundary regions of beta-Zn4Sb3. The Seebeck coefficient was almost unchanged and the electrical conductivity was slightly decreased by doping beta-Zn4Sb3 with Sn, indicating that Sn dose not act as a dopant. On the other hand, the thermal conductivity was lowered from 8.66 mW/cmK of the non-doped sample to 6.88 mW/cmK of the 3% Sn-doped sample at room temperature. This lowering of the thermal conductivity was considered to be due to the point defect phonon scattering induced by inclusions of Sn.