“…Figure 6(e) shows how thermal conductivity varies with temperature (κ c ). In the case of narrow bandgap materials, i.e., Sb 2 Te 3 and Bi 2 Te 3 , the total thermal conductivity is the sum of carrier (κ c ), phonon (κ p ), and bipolar thermal conductivity (κ b ), i.e., it can be expressed as κ T = κ c + κ p + κ b [39][40][41]44]. At low temperature, below 423 K, κ b is negligible.…”