2023
DOI: 10.7498/aps.72.20221981
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Mixed mismatch model predicted interfacial thermal conductance of metal/semiconductor interface

Abstract: The acoustic mismatch model and diffuse mismatch model are widely used in the calculation of interfacial thermal conductance. These two models are respectively based on the assumption of extremely smooth and rough interfaces. Due to the great difference between the actual interface structure and the two hypotheses, the prediction of these two models deviate greatly from the actual interfacial thermal conductance. The recently proposed mixed mismatch model considers the effect of interface structure on the rati… Show more

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Cited by 11 publications
(8 citation statements)
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“…4(d). Based on the theoretical model, 13,58 the OH groups situated on the surface of modified silicon display a higher degree of matching with PVDF, resulting in an increased supply of thermal transport channels and thus enhanced ITC. However, the impact of VDOS recombination on the enhancement of ITC is relatively limited.…”
Section: Resultsmentioning
confidence: 99%
“…4(d). Based on the theoretical model, 13,58 the OH groups situated on the surface of modified silicon display a higher degree of matching with PVDF, resulting in an increased supply of thermal transport channels and thus enhanced ITC. However, the impact of VDOS recombination on the enhancement of ITC is relatively limited.…”
Section: Resultsmentioning
confidence: 99%
“…Oil molecules are modeled using the polymer consistent force field, which has been widely used to simulate a broad range of organic compounds. The Tersoff potential is employed to model the interactions between carbon atoms in the graphene substrates . The non-bond interactions between the atoms are simulated by the Lennard–Jones (L–J) potential: E = 4 ε [ ( σ r i j ) 12 ( σ r i j ) 6 ] where ε and σ are the energy and length constants, respectively, and r ij is the distance between two atoms i and j . For cross-species pairwise L–J interactions, the Lorentz–Berthelot rule is used: , ε i j = ε i i ε j j , σ i j = σ i i + σ j j 2 where σ ij and ε ij are the distance parameters and energy constants of the L–J potential between type i and type j atoms, respectively.…”
Section: Methods and Simulation Modelmentioning
confidence: 99%
“…近些年来,低维纳米材料的蓬勃发展为热电 输运研究注入了新的活力 [18,19] . 研究人员发现相比于传统体材料, 低维纳米材料 的量子尺寸将会使费米面附近的 Seebeck 系数增加很多 [20] , 而同时声子界面散射 增加以及量子限制效应将导致热导率减少 [21] ,从而提升热电性能.受此启发, 纳米线 [22][23][24] 、纳米管 [25][26][27][28] 、纳米带 [29][30][31][32] 等体系中的热电性质陆续被报道. 另外, 纳米复合材料也被预测是提高热电性能的有效途径 [33][34][35] . 在纳米热电研究领域, 石墨烯凭借迷人的物理性质已受到许多研究人员的青 睐.…”
Section: 引 言 随着全球能源危机和环境污染问题的日益严重, 热电材料越来越引起了人们unclassified