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CsPbX(X = Cl、Br和I)的非谐声子重整化与热电性质:第一性原理计算

Anharmonic phonon renormalization and thermoelectric properties of CsPbX (X = Cl, Br, and I): first-principles calculations.

作者信息

Yao Ziang, Cao Wei, Wang Ziyu, Miao Ling, Shi Jing, Xiong Rui

机构信息

Key Laboratory of Artificial Micro- and Nano-structures of Ministry of Education, School of Physics and Technology, Wuhan University, Wuhan, P. R. China.

The Institute of Technological Sciences, Wuhan University, Wuhan, P. R. China.

出版信息

Phys Chem Chem Phys. 2023 Oct 4;25(38):26236-26244. doi: 10.1039/d3cp03224h.

Abstract

Halide perovskites with ultralow thermal conductivity have emerged as promising candidates for thermoelectric materials. We study the lattice dynamics and thermoelectric properties of cubic all-inorganic lead halide perovskites CsPbX (X = Cl, Br, and I) through first-principles calculations. Combined with self-consistent phonon theory, we have successfully renormalized the phonon frequency using a quartic anharmonic term, allowing us to accurately reproduce the phonon dispersion of the high-temperature cubic phase of CsPbX without any imaginary frequencies. Cubic CsPbX exhibit ultralow lattice thermal conductivities (0.61-1.71 Wm K) at room temperature. Because of the strong quartic anharmonic renormalization and hardening of the soft modes, the lattice thermal conductivities of cubic CsPbX all exhibit weak temperature dependence. Notably, CsPbCl exhibits remarkably high thermal conductivity and a long phonon lifetime. This can be attributed to the smallest atomic mean square displacement and the weakest tilting and distortions of PbCl octahedra, resulting from the strongest Pb-Cl covalent bonding. Furthermore, the maximum value of 0.63 at 900 K is obtained for the n-type CsPbBr.

摘要

具有超低热导率的卤化物钙钛矿已成为热电材料的有前途的候选者。我们通过第一性原理计算研究了立方全无机铅卤化物钙钛矿CsPbX(X = Cl、Br和I)的晶格动力学和热电性能。结合自洽声子理论,我们成功地使用四次非谐项对声子频率进行了重整化,从而能够在没有任何虚频率的情况下准确再现CsPbX高温立方相的声子色散。立方CsPbX在室温下表现出超低的晶格热导率(0.61 - 1.71 Wm K)。由于强烈的四次非谐重整化和软模的硬化,立方CsPbX的晶格热导率均表现出较弱的温度依赖性。值得注意的是,CsPbCl表现出非常高的热导率和声子寿命。这可归因于最小的原子均方位移以及PbCl八面体最弱的倾斜和畸变,这是由最强的Pb - Cl共价键导致的。此外,n型CsPbBr在900 K时获得了0.63的最大值。

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