Thermal response functions and second sound in graphene

TL;DR

This paper investigates second sound and ballistic heat transport in graphene using molecular dynamics simulations and compares results with Boltzmann transport theory, revealing insights into phonon decoherence and temperature oscillations.

Contribution

It introduces a simulation approach based on thermal-response functions for analyzing second sound in graphene, highlighting differences from traditional Boltzmann transport predictions.

Findings

Strong second-sound signal predicted at 300K for lengths ≥68.1nm

Second-sound dissipation mainly due to phonon decoherence from band structure

Decay time of second sound varies with thermal excitation length scale

Abstract

The propagation of second sound, and more broadly the ballistic transport of heat, is of central importance in heat dissipation from electronic devices at very short length and time scales. Specifically, there is an interest in the practical implications of violations of Fourier's law. Recently, we have developed a simulation approach based on thermal-response functions that is appropriate for elucidating physics beyond the diffusive regime, including time-dependent sources and second-sound propagation. The methods are applied to free-standing graphene simulated using molecular-dynamics (MD) with empirical potentials. The simulations predict a strong second-sound signal at T=300K for length scales of at least L=68.1nm. It is demonstrated that the second-sound dissipation time is determined primarily by decoherence that emerges from the details of the phonon band structure. It is also shown that the decay time for second sound depends sensitively on the length scale that characterizes the thermal excitation. This is in contrast with theories based on the Boltzmann transport equation (BTE), where second-sound dissipation is determined primarily by the resistive anharmonic phonon scattering rate. Calculations using the linearized BTE are also presented, along with analysis of second sound based on the BTE. This approach results in significantly longer lifetimes for second sound in comparison to our MD simulation results. Predictions for the response due to time-dependent sources are also presented, including insight into how time-dependent sources could be tuned to result in weak or strong temperature oscillations, and how time-dependent experiments might probe the spectra associated with second sound. Results are discussed in the context of second sound in graphite in the temperature range from 100-200K.