“…Optimizing the performance of a thermoelectric material is relatively difficult due to its adversely interdependent transport parameters [12][13][14][15]. Specifically, the performance of a thermoelectric material depends on the dimensionless figure of merit, zT, which is defined as zT = σS 2 T/ðκ e + κ L Þ, where σ, S, κ e , κ L , and T are the electrical conductivity, Seebeck coefficient, electrical thermal conductivity, lattice thermal conductivity, and absolute temperature, respectively [16]. Thus, in order to improve thermoelectric performance, these transport parameters should be synergistically optimized.…”