Steady State and Modulated Heat Conduction in Layered Systems Predicted by the Phonon Boltzmann Transport Equation
Jose Ordonez-Miranda, Ronggui Yang, Sebastian Volz, and J. J., Alvarado-Gil

TL;DR
This paper derives analytical expressions for heat conduction in layered systems using the phonon Boltzmann transport equation, revealing regimes where Fourier law applies and providing tools for thermal analysis of thin films.
Contribution
It extends the classical Fourier law approach by incorporating phonon transport physics, offering new formulas and invariants for analyzing heat conduction in layered thin films.
Findings
Heat conduction depends on the ratio of film thickness to phonon mean free path.
Diffusive behavior emerges when the ratio is large, ballistic when small.
Derived a simple formula for cross-plane thermal conductivity of thin films.
Abstract
Based on the phonon Boltzmann transport equation under the relaxation time approximation, analytical expressions for the temperature profiles of both steady state and modulated heat conduction inside a thin film deposited on a substrate are derived and analyzed. It is shown that both steady state and modulated components of the temperature depend strongly on the ratio between the film thickness and the average phonon mean free path, and they exhibit the diffusive behavior as predicted by the Fourier law of heat conduction when this ratio is much larger than the unity. In contrast, in the ballistic regime when this ratio is comparable to or smaller than the unity, the steady-state temperature tends to be independent of position, while the amplitude and the phase of the modulated temperature appear to be lower than those determined by the Fourier law. Furthermore, we derived an invariant…
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