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研究新型p型半赫斯勒合金的电子结构和热电功率因子。

Inspecting the electronic structure and thermoelectric power factor of novel p-type half-Heuslers.

作者信息

Khandy Shakeel Ahmad

机构信息

Department of Physics, National Taiwan University, Taipei, 10617, Taiwan, ROC.

出版信息

Sci Rep. 2021 Oct 21;11(1):20756. doi: 10.1038/s41598-021-00314-6.

DOI:10.1038/s41598-021-00314-6
PMID:34675306
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC8531014/
Abstract

In line for semiconducting electronic properties, we systematically scrutinize the likely to be grown half-Heusler compounds XTaZ (X = Pd, Pt and Z = Al, Ga, In) for their stability and thermoelectric properties. The energetically favored F-43m configuration of XTaZ alloys at equilibrium lattice constant is a promising non-magnetic semiconductor reflected from its total valence electron count (N = 18) and electronic structure calculations. Alongside mechanical stability, the dynamic stability is guaranteed from lattice vibrations and the phonon studies. The energy gaps of these stable Ta-based materials with Z = Ga are estimated to reach as high as 0.46 eV when X = Pd and 0.95 eV when X = Pt; however, this feature is reduced when Z = Al/In and X = Pd/Pt, respectively. Lattice thermal conductivity calculations are achieved to predict the smallest room temperature value of K = 33.6 W/K (PdTaGa) and 38.0 W/mK (for PtAlGa) among the proposed group of Heusler structures. In the end, we investigated the plausible thermoelectric performance of XTaZ alloys, which announces a comparable difference for the n-type and p-type doping regions. Among the six alloys, PtTaAl, PtTaGa and PtTaIn are predicted to be the most efficient materials where the power factor (PF) elevates up to ~ 90.5, 106.7, 106.5 mW/(Km), respectively at 900 K; however the lower values are recorded for PdTaAl (~ 66.5), PdTaGa (~ 76.5) and PdTaIn (~ 73.4) alloys. While this reading unlocks avenues for additional assessment of this new class of Half Heuslers, the project approach used here is largely appropriate for possible collection of understandings to realize novel stable materials with potential high temperature applications.

摘要

为了研究半导体电子特性,我们系统地研究了可能生长的半赫斯勒化合物XTaZ(X = Pd、Pt,Z = Al、Ga、In)的稳定性和热电性能。XTaZ合金在平衡晶格常数下能量上有利的F-43m构型是一种有前途的非磁性半导体,这从其总价电子数(N = 18)和电子结构计算中可以看出。除了机械稳定性外,晶格振动和声子研究保证了动态稳定性。当X = Pd且Z = Ga时,这些稳定的Ta基材料的能隙估计高达0.46 eV;当X = Pt且Z = Ga时,能隙估计高达0.95 eV;然而,当Z = Al/In且X = Pd/Pt时,这一特性会降低。通过晶格热导率计算预测,在所提出的赫斯勒结构组中,室温下K的最小值分别为33.6 W/K(PdTaGa)和38.0 W/mK(PtAlGa)。最后,我们研究了XTaZ合金可能的热电性能,结果表明n型和p型掺杂区域存在相当的差异。在这六种合金中,PtTaAl、PtTaGa和PtTaIn预计是最有效的材料,在900 K时功率因数(PF)分别高达约90.5、106.7、106.5 mW/(Km);然而,PdTaAl(约66.5)、PdTaGa(约76.5)和PdTaIn(约73.4)合金的功率因数较低。虽然这一结果为进一步评估这类新型半赫斯勒化合物开辟了道路,但这里采用的项目方法在很大程度上适用于收集可能的认识,以实现具有潜在高温应用的新型稳定材料。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f77e/8531014/d7bd4669f182/41598_2021_314_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f77e/8531014/1c86a18c9878/41598_2021_314_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f77e/8531014/6752b4cc4883/41598_2021_314_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f77e/8531014/405b0d770c94/41598_2021_314_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f77e/8531014/d84168381b53/41598_2021_314_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f77e/8531014/e8171b79ba0d/41598_2021_314_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f77e/8531014/08c7f2c2267b/41598_2021_314_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f77e/8531014/6fdf3fbb8894/41598_2021_314_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f77e/8531014/d7bd4669f182/41598_2021_314_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f77e/8531014/1c86a18c9878/41598_2021_314_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f77e/8531014/6752b4cc4883/41598_2021_314_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f77e/8531014/405b0d770c94/41598_2021_314_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f77e/8531014/d84168381b53/41598_2021_314_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f77e/8531014/e8171b79ba0d/41598_2021_314_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f77e/8531014/08c7f2c2267b/41598_2021_314_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f77e/8531014/6fdf3fbb8894/41598_2021_314_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f77e/8531014/d7bd4669f182/41598_2021_314_Fig8_HTML.jpg

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