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Understanding the transport behaviour of PbSe: A combined experimental and computational study

Published 7 Aug 2024 in cond-mat.mtrl-sci | (2408.03786v2)

Abstract: Lead chalcogenides are the promising thermoelectric (TE) materials having narrow band gap. The present work investigates the TE behaviour of PbSe in the temperature range 300-500 K. The transport properties of the sample have been studied using the Abinit and BoltzTrap code. The experimentally observed value of \textit{S} at 300 and 500 K is found to be ∼\sim 198 and 266 μ\muV K<sup>−1<sup>{-1}, respectively. The rate of increase in \emph{S} from 300 to 460 (460 to 500) K is found to be ∼\sim 0.4 (0.09). The temperature dependent electrical conductivity \textit{(σ\sigma)} shows the increasing trend, with values of ∼\sim 0.35 ×\times 10<sup>3<sup>{3} and ∼\sim 0.58 ×\times 10<sup>3<sup>{3} Ω\Omega{-1}</sup>m</sup> m{-1}$</sup> at 300 and 500 K, respectively. Further, the value of thermal conductivity \textit{($\kappa$)} at 300 (500) K is found to be 0.74 (1.07) W m${-1}</sup>K</sup> K{-1}$.</sup> The value of \textit{$\kappa$} is found to be increasing upto 460 K and then starts decreasing. The dispersion plot indicates that PbSe is a direct band gap semiconductor with band gap value of 0.16 (0.27) eV considering spin-orbit coupling (without SOC). The partial density of states (PDOS) plot shows that Pb 6p and Se 4p states have a major contribution in the transport properties. The observed and calculated values of \textit{S} gives a good match for SOC case. The calculated \textit{$\sigma$} and electronic part of thermal conductivity (\textit{$\kappa{_e}$}) gives good match with the experimental data. The maximum power factor (PF) value of $\sim$ 4.3 $\times$ 10${-5}</sup>W/mK</sup> W/mK{2}$ is observed at 500 K. This work helps in understanding the TE behaviour of PbSe through a novel and insightful alliance of experimental measurements and DFT approach.

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