“…Here, we start by assuming that the propagated thermal field satisfies the plane wave solution T = T ( x , ω) e − i ω t + T 0 , where T ( x , ω), t , ω, and T 0 denotes the complex amplitude, time, oscillation frequency, and reference temperature, respectively. [ 40,41 ] Then the wavevector can be derived accordingly, which helps describe the evanescent characteristics of thermal waves. For v ≠ 0, the wavevector is split into k + and k − (Figure 1c), depending on whether it travels with or against the convection (Figure S1, Supporting Information).…”