Effects of Si/Ge superlattice structure with intermixed interfaces on phonon thermal conductivity

IF 2.9 3区 物理与天体物理 Q3 NANOSCIENCE & NANOTECHNOLOGY Physica E-low-dimensional Systems & Nanostructures Pub Date : 2024-09-20 DOI:10.1016/j.physe.2024.116108
Alexander L. Khamets , Igor V. Safronov , Andrew B. Filonov , Dmitri B. Migas
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Abstract

By means of the Monte-Carlo/Molecular Dynamics and the non-equilibrium Molecular Dynamics methods we investigate the cross- and in-plane thermal conductivities of the (001)-, (110)- and (111)-oriented Si/Ge films (2 − 20 nm) and bulk superlattices with an intermixing at interfaces in comparison with the corresponding alloy structures at 300 K. For the first time the anomalous conductivity reduction of the in-plane thermal transport with respect to the film thickness has been revealed. This effect can be caused by interplay of three phonon scattering mechanisms: the phonon-alloy scattering mechanism, which is dominant, and competing phonon-phonon and phonon-surface scatterings due to the phonon depletion and the surface phonon localization, respectively. In general, the estimated minimal in-plane thermal conductivity values are found to be of 1.7 W/(m∙K) for the SiGe alloy thin films. It is established that the cross-plane thermal conductivity in the Si/Ge film superlattices crucially depends on intermixing at interfaces displaying even smaller values (less 1.5 W/(m∙K)) than in the corresponding SiGe alloy structures. We also show Si/SiGe superlattices in comparison with Ge/SiGe ones to provide up to 9 % gain in decreasing of both cross and in-plane thermal conductivities due to specific redistribution of peak weights in phonon density of states, which affect the thermal transport. These results reveal the insights into the application of SiGe-based superlattices and alloys for the cross- and in-plane thermoelectrics from the thermal transport minimization viewpoint.

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具有混合界面的硅/锗超晶格结构对声子热导率的影响
通过蒙特卡洛/分子动力学和非平衡分子动力学方法,我们研究了(001)-、(110)-和(111)-取向硅/锗薄膜(2 - 20 nm)的横向和面内热传导率,以及与相应合金结构在 300 K 下的界面互混体超晶格的比较。这种效应可能是由三种声子散射机制相互作用造成的:占主导地位的声子-合金散射机制,以及分别由声子耗竭和表面声子定位造成的竞争性声子-声子散射和声子-表面散射。总体而言,硅锗合金薄膜的最小面内热导率估计值为 1.7 W/(m∙K)。研究发现,硅/锗薄膜超晶格的跨面热导率主要取决于界面上的混合情况,其值甚至比相应的硅锗合金结构还要小(小于 1.5 W/(m∙K))。我们还发现,与 Ge/SiGe 超晶格相比,Si/SiGe 超晶格由于声子态密度峰值权重的特定重新分布而降低了横向和面内热导率,最高可提高 9%,从而影响热传输。这些结果从热传输最小化的角度揭示了基于硅锗的超晶格和合金在跨面和面内热电半导体中的应用。
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来源期刊
CiteScore
7.30
自引率
6.10%
发文量
356
审稿时长
65 days
期刊介绍: Physica E: Low-dimensional systems and nanostructures contains papers and invited review articles on the fundamental and applied aspects of physics in low-dimensional electron systems, in semiconductor heterostructures, oxide interfaces, quantum wells and superlattices, quantum wires and dots, novel quantum states of matter such as topological insulators, and Weyl semimetals. Both theoretical and experimental contributions are invited. Topics suitable for publication in this journal include spin related phenomena, optical and transport properties, many-body effects, integer and fractional quantum Hall effects, quantum spin Hall effect, single electron effects and devices, Majorana fermions, and other novel phenomena. Keywords: • topological insulators/superconductors, majorana fermions, Wyel semimetals; • quantum and neuromorphic computing/quantum information physics and devices based on low dimensional systems; • layered superconductivity, low dimensional systems with superconducting proximity effect; • 2D materials such as transition metal dichalcogenides; • oxide heterostructures including ZnO, SrTiO3 etc; • carbon nanostructures (graphene, carbon nanotubes, diamond NV center, etc.) • quantum wells and superlattices; • quantum Hall effect, quantum spin Hall effect, quantum anomalous Hall effect; • optical- and phonons-related phenomena; • magnetic-semiconductor structures; • charge/spin-, magnon-, skyrmion-, Cooper pair- and majorana fermion- transport and tunneling; • ultra-fast nonlinear optical phenomena; • novel devices and applications (such as high performance sensor, solar cell, etc); • novel growth and fabrication techniques for nanostructures
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