Predicting the Thermal Boundary Resistance of Isolated and Closely-Spaced Si/Si1−XGeX Interfaces With Molecular Dynamics Simulations

Author(s):  
E. S. Landry ◽  
T. Matsuura ◽  
A. J. H. McGaughey

Phonon scattering at an interface between two materials results in a thermal boundary resistance R, given by [1] R=ΔTq,(1) where ΔT and q are the temperature drop and heat flux across the interface. Predicting the thermal boundary resistance of semiconductor/semiconductor interfaces is important in devices where phonon interface scattering is a significant contributor to the overall thermal resistance (e.g., computer chips with high component density). Such predictions will also lead to improvements in the design of nanocomposite materials (e.g., superlattices) with low thermal conductivity, desirable in thermoelectric energy conversion applications [2].

Author(s):  
E. S. Landry ◽  
A. J. H. McGaughey

Phonon scattering at the interface between two materials results in a thermal resistance, R [1]. An ability to accurately predict the thermal resistance of semiconductor interfaces is important in devices where phonon interface scattering is a significant contributor to the overall thermal resistance (e.g., computer chips with high component density). This ability will also lead to improvements in the design of semiconductor superlattices with low thermal conductivity, desirable in thermoelectric energy conversion applications [2].


Author(s):  
Ruijie Zhao ◽  
Yunfei Chen ◽  
Kedong Bi ◽  
Meihui Lin ◽  
Zan Wang

A modified lattice-dynamical model is proposed to calculate the thermal boundary resistance at the interface between two fcc lattices. The nonequilibrium molecular dynamics (MD) simulation is employed to verify the theoretical calculations. In our physical model, solid crystal argon is set at the left side and the right side structure properties are tunable by setting the atomic mass and the interactive energy strength among atoms with different values. In the case of mass mismatch, the predictions of the lattice-dynamical (LD) model agree well at low temperature while the calculations of the diffuse mismatch model (DMM) based on the detailed phonon dispersion agree well at high temperature with the MD simulations. The modified LD model, considering a partially specular and partially diffuse phonon scattering, can explain the simulations reasonably in the whole temperature rage. The good agreement between the theoretical calculations and the simulations may be attributed to that phonon scattering mechanisms are dominated by elastic scattering at the perfect interfaces. In the case of interactive energy strength mismatch, the simulations are under the predictions of both the theoretical models, which may be attributed to the fact that this mismatch can bring about an outstanding contribution to opening up an inelastic channel for heat transfer at the interfaces.


2018 ◽  
Vol 20 (35) ◽  
pp. 22623-22628
Author(s):  
Riccardo Rurali ◽  
Xavier Cartoixà ◽  
Dick Bedeaux ◽  
Signe Kjelstrup ◽  
Luciano Colombo

We critically readdress the definition of thermal boundary resistance at an interface between two semiconductors.


Author(s):  
Luciano Colombo

I describe a set of computational experiments using molecular dynamics simulations, showing that the interface between two solid materials can be described as an autonomous thermodynamical system. By making use of the Gibbs description for such an interface, I discuss a robust nonequilibrium thermodynamics theoretical framework providing information about its corresponding thermal boundary resistance. In particular, I show that the termal resistance of a junction between two pure solid materials can be regarded as an interface property, depending solely on the interface temperature.


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