“…[15][16][17][18][19] Generally, the MC method follows a time-splitting algorithm, namely, the dynamics of a simulated particle is decoupled into advection and scattering processes, and thus the time step used is less than the relaxation time, and the grid size is less than the phonon mean-free-path. 20 Consequently, the computational costs of MC method are expensive in the acoustic thick regime, which prohibit its applications for multiscale problems with diffusive region, although it can be quite efficient for ballistic transport. It is also noted that an improved MC method has been developed recently by simulating only the deviation from equilibrium such that the variance can be efficiently reduced in simulating systems with small temperature variations.…”