Shastri Shivprasad S, Pandey Sudhir K
School of Engineering, Indian Institute of Technology Mandi, Kamand - 175005, India.
J Phys Condens Matter. 2020 Jun 3;32(35). doi: 10.1088/1361-648X/ab8b9e.
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 gapof ∼0.54 eV. Thisis found to be inadequate to explain the experimental data. The better explanation of experimental Seebeck coefficientis done by consideringof 0.18 eV which suggests the non-stoichiometry and/or disorder in the sample. In the calculation ofand other TE properties temperature dependence on chemical potential is included. In order to look for the possible enhanced TE properties obtainable in ZrNiSn withof ∼0.54 eV, power factor and optimal carrier concentrations are calculated. The optimal electron and hole concentrations required to attain highest power factors are ∼7.6 × 10cmand ∼1.5 × 10cm, respectively. The maximum figure of meritcalculated at 1200 K for n-type and p-type ZrNiSn are ∼0.5 and ∼0.6, respectively. The % efficiency obtained for n-type ZrNiSn is ∼4.2% while for p-type ZrNiSn is ∼5.1%. Theare expected to be further enhanced to ∼1.1 (n-type) and ∼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() of ∼7.8 × 10Kcalculated 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.
在这项工作中,我们尝试通过使用SCAN泛函的密度泛函理论(DFT)和半经典输运计算来理解ZrNiSn样品的实验热电(TE)性质。SCAN和mBJ给出的带隙相同,约为0.54电子伏特。发现这不足以解释实验数据。通过考虑0.18电子伏特能更好地解释实验塞贝克系数,这表明样品中存在非化学计量比和/或无序。在计算以及其他TE性质时,考虑了温度对化学势的依赖性。为了寻找在带隙约为0.54电子伏特的ZrNiSn中可能获得的增强TE性质,计算了功率因子和最佳载流子浓度。获得最高功率因子所需的最佳电子和空穴浓度分别约为7.6×10/cm和1.5×10/cm。在1200K下计算得到的n型和p型ZrNiSn的最大品质因数分别约为0.5和0.6。n型ZrNiSn获得的效率约为4.2%,而p型ZrNiSn为5.1%。通过掺杂重元素以降低热导率,预计在1200K时,品质因数将进一步提高到约1.1(n型)和1.2(p型)。还通过计算色散、态密度总和及部分态密度来研究声子性质。计算得到的382K的德拜温度与398K的实验值吻合良好。在准谐近似下研究了ZrNiSn中的热膨胀行为。我们工作中计算得到的约7.8×10/K的平均线性热膨胀系数与实验值相当接近。计算得到的线性热膨胀系数将有助于设计用于高温应用的热电发电机。