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Thermoelectric Property of A-Site Deficient Zn0.5Rh2O4

机译:A现场缺乏Zn0.5RH2O4的热电性能

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@@ Introduction Thermoelectric materials have been attracted for recycling energy in exhausting heat by thermal-electric conversion effect, which can be closely used and be considered as a new energy resource in human lives. The thermal-electric conversion efficiency is represented by a dimensionless figure of merit: ZT=S2a T/K, where S, a and K are Seebeck coefficient, electrical conductivity, and thermal conductivity, respectively. Accordingly, thermoelectric materials should be designed with higher S, a and lower K. According to the classical semiconductor theory, heavily doped semiconductors having carrier concentrations (n) of ~ 1019 cm3 are candidates for high-ZT materials [1], but metallic materials are not. Thus the discovery of large S (~ 100 |JY/K at 300 K) in NaxCoO2, showing metallic a with n of ~ 1021 cm3, has attracted much attention for its origin of high ZT [2].
机译:@@简介热电材料被吸引用于通过热电转换效果排出耗尽的能量,这可以密切使用,并被视为人类生活中的新能源资源。热电转换效率由无量纲的优点图表示:Zt = S2a T / K,其中S,A和K分别是塞贝克系数,导电性和导热率。因此,热电材料应设计有更高的S,A和下部K.根据经典的半导体理论,具有载载体浓度(N)的掺杂半导体为〜1019cm 3是高ZT材料的候选物[1],但金属材料不是。因此,在纳克苏2中发现大的S(〜100 | JY / K),显示含有N的金属A,其〜1021cm3,对其高ZT的起源引起了很多关注。

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