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基于杂化密度泛函理论的p型CuO、CuO和NiO的热电性质

Thermoelectric Properties of p-Type CuO, CuO, and NiO from Hybrid Density Functional Theory.

作者信息

Linnera Jarno, Sansone Giuseppe, Maschio Lorenzo, Karttunen Antti J

机构信息

Department of Chemistry and Materials Science, Aalto University, Kemistintie 1, 02150 Espoo, Finland.

Dipartimento di Chimica and Dipartimento di Chimica, C3S Centre, NIS Centre, Università di Torino, Via P. Giuria 5, 10125 Torino, Italy.

出版信息

J Phys Chem C Nanomater Interfaces. 2018 Jul 12;122(27):15180-15189. doi: 10.1021/acs.jpcc.8b04281. Epub 2018 Jun 15.

DOI:10.1021/acs.jpcc.8b04281
PMID:30258523
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6150688/
Abstract

The electronic transport coefficients of three Earth-abundant metal oxides CuO, CuO, and NiO were investigated using hybrid density functional theory (DFT). Hybrid DFT methods combined with local Gaussian-type basis sets enabled band structure studies on both non-magnetic and magnetic p-type metal oxides without empirical corrections. The CRYSTAL code was used for obtaining the wavefunction, and the transport properties were calculated with two different methodologies to benchmark their accuracy: a numerical approach as implemented in the BoltzTraP code and an analytical approach recently implemented in CRYSTAL17. Both computational methods produce identical results in good agreement with experimental measurements of the Seebeck coefficient. The predicted electrical conductivities are overestimated, owing likely to the used approximation of a constant electronic relaxation time in the calculations, as explicit electron scattering is neglected and relaxation time is considered only as a free parameter. The obtained results enable us to critically review and complement the available theoretical and experimental literature on the studied p-type thermoelectric metal oxide materials.

摘要

使用杂化密度泛函理论(DFT)研究了三种地球上储量丰富的金属氧化物CuO、Cu₂O和NiO的电子输运系数。杂化DFT方法与局部高斯型基组相结合,能够在无需经验校正的情况下对非磁性和磁性p型金属氧化物进行能带结构研究。使用CRYSTAL代码获取波函数,并采用两种不同方法计算输运性质以检验其准确性:一种是BoltzTraP代码中实现的数值方法,另一种是CRYSTAL17中最近实现的解析方法。两种计算方法得出的结果相同,与塞贝克系数的实验测量结果吻合良好。预测的电导率被高估了,这可能是由于计算中使用了恒定电子弛豫时间的近似,因为忽略了显式电子散射,且弛豫时间仅被视为一个自由参数。所得结果使我们能够批判性地回顾和补充有关所研究的p型热电金属氧化物材料的现有理论和实验文献。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1d33/6150688/77f4a7297f11/jp-2018-04281b_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1d33/6150688/f03a92e8cf29/jp-2018-04281b_0006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1d33/6150688/79813d771c4f/jp-2018-04281b_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1d33/6150688/c93eaae836f2/jp-2018-04281b_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1d33/6150688/9c034cad54ee/jp-2018-04281b_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1d33/6150688/77f4a7297f11/jp-2018-04281b_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1d33/6150688/f03a92e8cf29/jp-2018-04281b_0006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1d33/6150688/79813d771c4f/jp-2018-04281b_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1d33/6150688/c93eaae836f2/jp-2018-04281b_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1d33/6150688/9c034cad54ee/jp-2018-04281b_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1d33/6150688/77f4a7297f11/jp-2018-04281b_0005.jpg

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