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通过(镧、镝和氮)共掺杂改善钛酸锶的热电性能:密度泛函理论方法

Improved Thermoelectric Properties of SrTiO via (La, Dy and N) Co-Doping: DFT Approach.

作者信息

Sikam Pornsawan, Thirayatorn Ruhan, Kaewmaraya Thanayut, Thongbai Prasit, Moontragoon Pairot, Ikonic Zoran

机构信息

Research Center for Quantum Technology, Faculty of Science, Chiang Mai University, Chiang Mai 50200, Thailand.

Office of Research Administration, Chiang Mai University, Chiang Mai 50200, Thailand.

出版信息

Molecules. 2022 Nov 16;27(22):7923. doi: 10.3390/molecules27227923.

Abstract

This work considers the enhancement of the thermoelectric figure of merit, ZT, of SrTiO (STO) semiconductors by (La, Dy and N) co-doping. We have focused on SrTiO because it is a semiconductor with a high Seebeck coefficient compared to that of metals. It is expected that SrTiO can provide a high power factor, because the capability of converting heat into electricity is proportional to the Seebeck coefficient squared. This research aims to improve the thermoelectric performance of SrTiO by replacing host atoms by La, Dy and N atoms based on a theoretical approach performed with the Vienna Ab Initio Simulation Package (VASP) code. Here, undoped SrTiO, SrLaTiO, SrDyTiO, SrTiON, SrLaDyTiO and SrLaTiON are studied to investigate the influence of La, Dy and N doping on the thermoelectric properties of the SrTiO semiconductor. The undoped and La-, Dy- and N-doped STO structures are optimized. Next, the density of states (DOS), band structures, Seebeck coefficient, electrical conductivity per relaxation time, thermal conductivity per relaxation time and figure of merit (ZT) of all the doped systems are studied. From first-principles calculations, STO exhibits a high Seebeck coefficient and high figure of merit. However, metal and nonmetal doping, i.e., (La, N) co-doping, can generate a figure of merit higher than that of undoped STO. Interestingly, La, Dy and N doping can significantly shift the Fermi level and change the DOS of SrTiO around the Fermi level, leading to very different thermoelectric properties than those of undoped SrTiO. All doped systems considered here show greater electrical conductivity per relaxation time than undoped STO. In particular, (La, N) co-doped STO exhibits the highest ZT of 0.79 at 300 K, and still a high value of 0.77 at 1000 K, as well as high electrical conductivity per relaxation time. This renders it a viable candidate for high-temperature applications.

摘要

本研究通过(镧、镝和氮)共掺杂来提高钛酸锶(STO)半导体的热电优值ZT。我们专注于钛酸锶,因为与金属相比,它是一种具有高塞贝克系数的半导体。预计钛酸锶能提供高功率因数,因为将热转化为电的能力与塞贝克系数的平方成正比。本研究旨在基于使用维也纳从头算模拟包(VASP)代码进行的理论方法,通过用镧、镝和氮原子取代主体原子来改善钛酸锶的热电性能。在此,对未掺杂的钛酸锶、SrLaTiO、SrDyTiO、SrTiON、SrLaDyTiO和SrLaTiON进行研究,以考察镧、镝和氮掺杂对钛酸锶半导体热电性能的影响。对未掺杂以及镧、镝和氮掺杂的STO结构进行了优化。接下来,研究了所有掺杂体系的态密度(DOS)、能带结构、塞贝克系数、每弛豫时间的电导率、每弛豫时间的热导率和优值(ZT)。基于第一性原理计算,STO表现出高塞贝克系数和高优值。然而,金属和非金属掺杂,即(镧、氮)共掺杂,能产生比未掺杂的STO更高的优值。有趣的是,镧、镝和氮掺杂能显著移动费米能级并改变钛酸锶在费米能级附近的DOS,导致其热电性能与未掺杂的钛酸锶有很大不同。这里考虑的所有掺杂体系每弛豫时间的电导率都比未掺杂的STO更高。特别是,(镧、氮)共掺杂的STO在300 K时表现出最高的ZT值0.79,在1000 K时仍有0.77的高值,以及高的每弛豫时间电导率。这使其成为高温应用的可行候选材料。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3c90/9693972/af6b64c74bf1/molecules-27-07923-g001.jpg

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