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纤锌矿氧化锌热导率的第一性原理晶格动力学研究——与氮化镓的对比研究

Thermal Conductivity of Wurtzite Zinc-Oxide from First-Principles Lattice Dynamics--a Comparative Study with Gallium Nitride.

作者信息

Wu Xufei, Lee Jonghoon, Varshney Vikas, Wohlwend Jennifer L, Roy Ajit K, Luo Tengfei

机构信息

Aerospace and Mechanical Engineering, University of Notre Dame, Notre Dame, IN 46530.

Materials and Manufacturing Directorate, Air Force Research Laboratory, Wright-Patterson Air Force Base, OH 45433.

出版信息

Sci Rep. 2016 Mar 1;6:22504. doi: 10.1038/srep22504.

DOI:10.1038/srep22504
PMID:26928396
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC4772549/
Abstract

Wurtzite Zinc-Oxide (w-ZnO) is a wide bandgap semiconductor that holds promise in power electronics applications, where heat dissipation is of critical importance. However, large discrepancies exist in the literature on the thermal conductivity of w-ZnO. In this paper, we determine the thermal conductivity of w-ZnO using first-principles lattice dynamics and compare it to that of wurtzite Gallium-Nitride (w-GaN)--another important wide bandgap semiconductor with the same crystal structure and similar atomic masses as w-ZnO. However, the thermal conductivity values show large differences (400 W/mK of w-GaN vs. 50 W/mK of w-ZnO at room temperature). It is found that the much lower thermal conductivity of ZnO originates from the smaller phonon group velocities, larger three-phonon scattering phase space and larger anharmonicity. Compared to w-GaN, w-ZnO has a smaller frequency gap in phonon dispersion, which is responsible for the stronger anharmonic phonon scattering, and the weaker interatomic bonds in w-ZnO leads to smaller phonon group velocities. The thermal conductivity of w-ZnO also shows strong size effect with nano-sized grains or structures. The results from this work help identify the cause of large discrepancies in w-ZnO thermal conductivity and will provide in-depth understanding of phonon dynamics for the design of w-ZnO-based electronics.

摘要

纤锌矿型氧化锌(w-ZnO)是一种宽带隙半导体,在功率电子应用中具有广阔前景,其中散热至关重要。然而,关于w-ZnO热导率的文献存在很大差异。在本文中,我们使用第一性原理晶格动力学确定了w-ZnO的热导率,并将其与纤锌矿型氮化镓(w-GaN)的热导率进行比较——w-GaN是另一种重要的宽带隙半导体,具有与w-ZnO相同的晶体结构和相似的原子质量。然而,热导率值显示出很大差异(室温下w-GaN为400 W/mK,w-ZnO为50 W/mK)。研究发现,ZnO的热导率低得多源于声子群速度较小、三声子散射相空间较大以及非谐性较大。与w-GaN相比,w-ZnO在声子色散方面的频率间隙较小,这导致了更强的非谐声子散射,并且w-ZnO中较弱的原子间键导致声子群速度较小。w-ZnO的热导率在纳米尺寸的晶粒或结构中也表现出强烈的尺寸效应。这项工作的结果有助于确定w-ZnO热导率存在巨大差异的原因,并将为基于w-ZnO的电子器件设计提供对声子动力学的深入理解。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a7fe/4772549/323fb82d0eec/srep22504-f8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a7fe/4772549/46114fc911f7/srep22504-f1.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a7fe/4772549/e1704da1e60c/srep22504-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a7fe/4772549/242f3b6179e9/srep22504-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a7fe/4772549/eb76c776e297/srep22504-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a7fe/4772549/7c9330822552/srep22504-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a7fe/4772549/323fb82d0eec/srep22504-f8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a7fe/4772549/46114fc911f7/srep22504-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a7fe/4772549/3af14a3e757a/srep22504-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a7fe/4772549/1cd2d36bd7a4/srep22504-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a7fe/4772549/e1704da1e60c/srep22504-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a7fe/4772549/242f3b6179e9/srep22504-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a7fe/4772549/eb76c776e297/srep22504-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a7fe/4772549/7c9330822552/srep22504-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a7fe/4772549/323fb82d0eec/srep22504-f8.jpg

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