Abstract

This work describes our discovery of the dominant role of highly charged interfaces on the electrothermal transport properties of PbS, along with a method to reduce the barrier potential for charge carriers by an order of magnitude. High temperature thermoelectrics such as PbS are inevitably exposed to elevated temperatures during postsynthesis treatment as well as operation. However, we observed that as the material was heated, large concentrations of sulfur vacancy (VS̈) sites were formed at temperatures as low as 266 °C. This loss of sulfur doped the PbS n-type and increased the carrier concentration, where these excess electrons were trapped and immobilized at interfacial defect sites in polycrystalline PbS with an abundance of grain boundaries. Sulfur deficient PbS0.81 exhibited a large barrier potential for charge carriers of 0.352 eV, whereas annealing the material under a sulfur-rich environment prevented VS̈ formation and lowered the barrier by an order of magnitude to 0.046 eV. Through ab initio calculations, the formation of VS̈ was found to be more favorable on the surface compared to the bulk of the material with a 1.72 times lower formation energy barrier. These observations underline the importance of controlling interface-vacancy effects in the preparation of bulk materials comprised of nanoscale constituents.

Highlights

  • This majority carrier type reversal has been observed through changes in the surface condition of (Bi1−xSbx)2Te3 nanoplates.23 Point defects may interact with dopants present in a thermoelectric material;24 the dopant–defect interactions have not been fully understood

  • High temperature thermoelectrics such as PbS are inevitably exposed to elevated temperatures during postsynthesis treatment as well as operation

  • Understanding these interfacial defects is highly relevant to end-use performance since for waste-heat recovery applications, it is more preferable to operate at elevated temperatures from a thermodynamic stand point

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Summary

Introduction

This majority carrier type reversal has been observed through changes in the surface condition of (Bi1−xSbx)2Te3 nanoplates.23 Point defects may interact with dopants present in a thermoelectric material;24 the dopant–defect interactions have not been fully understood. The lower electrical conductivity of the p-type PbS–S–SPS sample can be due to its lower carrier concentration (p = 1.8 × 1018 cm−3) compared to that of the n-type PbS-SPS with a higher carrier concentration (n = 3.7 × 1019 cm−3) [Fig. 4(g)], as well as its higher concentration of grain boundaries.

Results
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