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YCT(T = O、F、OH)的热电和热力学性质研究。

Investigations on the thermoelectric and thermodynamic properties of YCT (T = O, F, OH).

作者信息

Wang Li, Chang Wen-Li, Sun Zi-Qi, Zhang Zi-Meng

机构信息

The School of Mathematics and Physics, Lanzhou Jiaotong University 88 Anning West Road, Anning District Lanzhou Cit 730070 China

出版信息

RSC Adv. 2022 May 12;12(23):14377-14383. doi: 10.1039/d2ra01077a.

DOI:10.1039/d2ra01077a
PMID:35702233
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9096430/
Abstract

Using the first-principle calculations combined with the Boltzmann transport theory, we studied the thermoelectric properties of YCT (T = O, F, OH) MXenes. Specifically, the Seebeck coefficient, thermal and electrical conductivities under constant relaxation time approximation were calculated. Results show that for p-type carriers, YCO has the largest power factor of up to 0.0017 W m K when the carrier concentration is 4.067 × 10 cm at 900 K, at the same temperature, for n-type carriers, the concentration is 9.376 × 10 cm, the power factor in YC(OH) is 0.0026 W m K. In particular, the figure of merit in YCF is 1.38 at 900 K because of its low thermal conductivity, indicating that it can be considered a potential medium-temperature thermoelectric material. In addition, the thermodynamics properties within 32 GPa and 900 K, such as bulk modulus, heat capacity and thermal expansion, are also estimated using the quasi-harmonic Debye model. Our results may offer some valuable hints for the potential application of YCT (T = O, F, OH) in the thermoelectric field.

摘要

结合第一性原理计算和玻尔兹曼输运理论,我们研究了YCT(T = O、F、OH)MXenes的热电性能。具体而言,计算了在恒定弛豫时间近似下的塞贝克系数、热导率和电导率。结果表明,对于p型载流子,当载流子浓度在900 K时为4.067×10 cm时,YCO具有高达0.0017 W m K的最大功率因数;在相同温度下,对于n型载流子,浓度为9.376×10 cm时,YC(OH)中的功率因数为0.0026 W m K。特别地,由于其低热导率,YCF在900 K时的优值为1.38,表明它可被视为一种潜在的中温热电材料。此外,还使用准谐德拜模型估计了在32 GPa和900 K范围内的热力学性质,如体积模量、热容量和热膨胀。我们的结果可能为YCT(T = O、F、OH)在热电领域的潜在应用提供一些有价值的线索。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/7de1f2b8a1a3/d2ra01077a-f10.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/faa8e9d47ad4/d2ra01077a-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/9efcc3be6cdd/d2ra01077a-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/d7dc2cb3fd14/d2ra01077a-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/c507b75941c8/d2ra01077a-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/160b617ddf19/d2ra01077a-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/07ad54ae8a32/d2ra01077a-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/20542c6785db/d2ra01077a-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/a10e78743e7e/d2ra01077a-f8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/5d371ead5a1d/d2ra01077a-f9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/7de1f2b8a1a3/d2ra01077a-f10.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/faa8e9d47ad4/d2ra01077a-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/9efcc3be6cdd/d2ra01077a-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/d7dc2cb3fd14/d2ra01077a-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/c507b75941c8/d2ra01077a-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/160b617ddf19/d2ra01077a-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/07ad54ae8a32/d2ra01077a-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/20542c6785db/d2ra01077a-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/a10e78743e7e/d2ra01077a-f8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/5d371ead5a1d/d2ra01077a-f9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0ea8/9096430/7de1f2b8a1a3/d2ra01077a-f10.jpg

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