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Thermoelectric properties, efficiency and thermal expansion of ZrNiSn half-Heusler by first-principles calculations

机译:通过第一原理计算,Zrnisn Half-Heusler的热电性能,效率和热膨胀

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In this work, we try to understand the experimental thermoelectric (TE) properties of a ZrNiSn sample with DFT and semiclassical transport calculations using SCAN functional. SCAN and mBJ provide the same band gap E-g of similar to 0.54 eV. This E-g is found to be inadequate to explain the experimental data. The better explanation of experimental Seebeck coefficient S is done by considering E-g of 0.18 eV which suggests the non-stoichiometry and/or disorder in the sample. In the calculation of S and other TE properties temperature dependence on chemical potential is included. In order to look for the possible enhanced TE properties obtainable in ZrNiSn with E-g of similar to 0.54 eV, power factor and optimal carrier concentrations are calculated. The optimal electron and hole concentrations required to attain highest power factors are similar to 7.6 x 10(19) cm(-3) and similar to 1.5 x 10(21) cm(-3), respectively. The maximum figure of merit ZT calculated at 1200 K for n-type and p-type ZrNiSn are similar to 0.5 and similar to 0.6, respectively. The % efficiency obtained for n-type ZrNiSn is similar to 4.2% while for p-type ZrNiSn is similar to 5.1%. The ZT are expected to be further enhanced to similar to 1.1 (n-type) and similar to 1.2 (p-type) at 1200 K by doping with heavy elements for thermal conductivity reduction. The phonon properties are also studied by calculating dispersion, total and partial density of states. The calculated Debye temperature of 382 K is in good agreement with experimental value of 398 K. The thermal expansion behaviour in ZrNiSn is studied under quasi-harmonic approximation. The average linear thermal expansion coefficient alpha(ave)(T) of similar to 7.8 x 10(-6) K-1 calculated in our work is quite close to the experimental values. The calculated linear thermal expansion coefficient will be useful in designing the thermoelectric generators for high temperature applications.
机译:在这项工作中,我们试图了解与使用扫描功能DFT和半经典输运计算一个ZrNiSn样品的实验热电(TE)的特性。 SCAN和MBJ提供相同的带隙E-克类似于0.54电子伏特。此E-克被发现是不足以解释实验数据。实验塞贝克系数S的更好的解释是通过考虑E-克0.18电子伏特这表明在样品中的非化学计量和/或病症的完成。在S和化学势其他TE特性的温度依赖性的计算被包括。为了寻找可能的增强TE在ZrNiSn可获得具有类似E-g至0.54电子伏特,功率因数和最优载流子浓度的属性进行计算。以获得最高的功率因数所需的最佳电子和空穴浓度分别类似于7.6×10(19)厘米(-3)和类似1.5×10(21)厘米(-3),。在1200 K中的n型和p型ZrNiSn计算性能指数ZT的最大数字分别类似于0.5和类似〜0.6,。对于n型ZrNiSn获得的%的效率是相似至4.2%,而对于p型ZrNiSn类似于5.1%。的ZT预计可进一步由掺杂与重元素用于热导率降低到增强在1200ķ类似于1.1(n型)和类似1.2(p型)。声子属性也通过计算分散,总和状态的部分密度的研究。 382 K的计算德拜温度与在ZrNiSn的热膨胀特性下准谐波近似研究398 K的实验值吻合。的平均线性热膨胀系数α(AVE)(T)类似7.8×10(-6)K-1在我们的工作计算是相当接近的实验值。计算出的线性热膨胀系数将是在设计用于高温应用的热电发生器是有用的。

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