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通过快淬-机械球磨-放电等离子烧结工艺制备了p型(Bi0.25Sb0.75)2Te3块体热电材料.在300~523K温度范围内对其电导率、Seebeck系数和热导率进行了测试,并系统研究了快淬后球磨时间对合金热电性能的影响.研究结果表明,随着球磨时间的延长,样品的电导率呈先降后升的趋势,Seebeck系数变化并不明显,而热导率随球磨时间的延长逐渐下降.球磨20h的样品在室温下具有最高的热电优值,最大值达到0.96,机械抗弯强度达到91MPa.

参考文献

[1] Mahan Gerald,Sales Brian,Sharp Jeff.Thermoelectric materials:new approaches to an old problem.Physics Today,1997,50(3):42-47.
[2] Ni H L,Zhu T J,Zhao X B.Thermoelectric properties of hydro-thermally synthesized and hot pressed n-type Bi2Te3 alloys with different contents of Te.Materials Science & Engineering B,2005,117(2):119-122.
[3] Su T C,Zhu P W,Ma H A,et al.Electrical transport and thermoelectric properties of PbTe doped with Sb2Te3 prepared by high-pressure and high-temperature.J.Alloys Compd.,2006,422(1/2):328-331.
[4] Hillhouse Hugh W,Tuominen Mark T.Modeling the thermoelectric transport properties of nanowires embedded in oriented mi-croporous and mesoporous films.Microp.Mesop.Mater.,2001,47(1):39-50.
[5] Dauscher A,Lenoir B,Boffoue O,et al.Thermoelectric films prepared by pulsed laser deposition.ALT01 international conference on advanced laser technologies.Proceedings of SPIE,2002,4762:52-63.
[6] 马秋花,孙亚光.Bi-Te基热电材料的研究进展.稀有金属快报,2007,26(6):7-10.
[7] Tang X F,Xie W J,Li H,et al.Preparation and thermoelectric transport properties of high-performance p-type Bi2Te3 with layered nanostructure.Applied physics letters,2007,90(1):12102-12105.
[8] Cui J L,Mao L D,Yang W,et al.Thermoelectric properties of Cu-doped n-type (Bi2Te3)0.9-(Bi2-xCuxSe3)0.1(x=0-0.2) alloys.Journal of Solid State Chemistry,2007,180(12):3583-3587.
[9] 刘思科,朱秉升,罗普生,等.半导体物理学,4版.北京:国防工业出版社,2008:85-86.
[10] 李佳,张忻,路清梅,等.球磨时间对P型Bi2Te3基热电材料性能的影响.功能材料,2007,38:1338-1340.
[11] 余柏林,祁琼,唐新峰,等(YU Bo-Lin,et al).晶粒尺寸对CoSb3化合物热电性能的影响.物理学报(Acta Physica Siaica),2005,54(12):5763-5768.
[12] Orihashi M,NodaY,Kaibe H T,et al.Evaluation of thermoelectric properties of impurity doped PbTe.Materials Transactions,1998,39(6):672-678.
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