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The study of structural, electronic and thermoelectric properties of Ca1−xYbxZn2Sb2 (x = 0, 0.25, 0.5, 0.75, 1) Zintl compounds
International Journal of Modern Physics B ( IF 2.6 ) Pub Date : 2021-03-24 , DOI: 10.1142/s0217979221501009 I. Mili 1, 2 , H. Latelli 1, 2 , T. Ghellab 1, 2 , Z. Charifi 1, 2 , H. Baaziz 1, 2 , F. Soyalp 3
International Journal of Modern Physics B ( IF 2.6 ) Pub Date : 2021-03-24 , DOI: 10.1142/s0217979221501009 I. Mili 1, 2 , H. Latelli 1, 2 , T. Ghellab 1, 2 , Z. Charifi 1, 2 , H. Baaziz 1, 2 , F. Soyalp 3
Affiliation
Based on the electronic structure, the physical properties of Ca 1 − x Yb x Zn 2 Sb 2 (x = 0 , 0.25, 0.5, 0.75, 1) Zintl compounds are studied. The transport properties can be significantly changed by varying the composition x . The materials under study are more metallic with increasing x and behaves like a semiconductor when x decreases. It is found that CaZn 2 Sb 2 exhibits a larger thermopower magnitude (S = 2 4 1 μ V/K at T = 7 0 0 K ) and the Seebeck coefficient decreases as x increases. The calculated figure of merit factor of YbZn 2 Sb 2 is found to be low, this is explained by the fact that its structure is very compact and its bandgap is small which lead to high electrical and thermal conductivity due to high carrier concentration (n = 1 . 2 5 ⋅ 1 0 2 0 cm − 3 at T = 3 0 0 K ). On other hand a narrow-gap (0.46 eV for CaZn 2 Sb 2 ), provides a balance between a high Seebeck coefficient and low electronic thermal conductivity, with a slight increase in the carrier concentration when the temperature increases (3 . 8 7 ⋅ 1 0 1 9 cm − 3 at 600 K). As a consequence, CaZn 2 Sb 2 compound is predicted to have good performance for thermoelectric applications. The electrical ( σ ) and the thermal ( K ) conductivity for CaZn 2 Sb 2 compound in both directions (along x and z -axes) are calculated. It is obtained that ( σ x x ) is 120% of ( σ z z ) at high-temperature, whereas S z z Seebeck coefficient was higher than S x x especially at T = 3 0 0 K (S z z = 2 4 6 μ V/K , S x x = 2 1 3 μ V/K ) . The large value of S z z showed that the transport is dominated by zz -axis.
中文翻译:
Ca1−xYbxZn2Sb2 (x = 0, 0.25, 0.5, 0.75, 1) Zintl 化合物的结构、电子和热电特性研究
根据电子结构,物理性质钙 1 - X 镱 X 锌 2 锑 2 (X = 0 , 0.25, 0.5, 0.75, 1) 研究了 Zintl 化合物。通过改变成分可以显着改变传输特性X . 正在研究的材料随着增加而更具金属性X 并且表现得像一个半导体,当X 减少。发现钙锌 2 锑 2 表现出更大的热电势(小号 = 2 4 1 μ V/K 在吨 = 7 0 0 ķ ) 塞贝克系数随着X 增加。计算的品质因数镱锌 2 锑 2 被发现很低,这是因为它的结构非常紧凑,带隙很小,由于高载流子浓度导致高电导率和热导率(n = 1 . 2 5 ⋅ 1 0 2 0 厘米 - 3 在吨 = 3 0 0 ķ )。另一方面,窄间隙(0.46 eV钙锌 2 锑 2 ),在高塞贝克系数和低电子热导率之间提供平衡,当温度升高时载流子浓度略有增加(3 . 8 7 ⋅ 1 0 1 9 厘米 - 3 在 600 K)。作为结果,钙锌 2 锑 2 预计该化合物在热电应用中具有良好的性能。电气( σ ) 和热( ķ ) 电导率钙锌 2 锑 2 双向复合(沿X 和z -轴)计算。得到的是( σ X X ) 是 120%( σ z z ) 在高温下,而小号 z z 塞贝克系数高于小号 X X 特别是在吨 = 3 0 0 ķ (小号 z z = 2 4 6 μ V/K , 小号 X X = 2 1 3 μ V/K ) . 大的价值小号 z z 表明运输主要由Z Z -轴。
更新日期:2021-03-24
中文翻译:
Ca1−xYbxZn2Sb2 (x = 0, 0.25, 0.5, 0.75, 1) Zintl 化合物的结构、电子和热电特性研究
根据电子结构,物理性质