Abstract

Optical absorption edge measurements are performed on I doped PbTe using diffuse reflectance infrared Fourier transform spectroscopy. The Burstein–Moss shift, an increase in the absorption edge (optical band gap) with increasing doping level, is explored. The optical gap increases on the order of 0.1 eV for doping levels ranging from 3 × 1018 to 2 × 1020 cm−3, relevant doping levels for good thermoelectric materials. Chemical potential is estimated from transport measurements—specifically, Hall effect and Seebeck coefficient—using a single band Kane model. In heavily doped semiconductors, it is well-known that the band gap shrinks with increasing doping level. This effect, known as band gap renormalization, is fit here using an n1/3 scaling law which reflects an electron–electron exchange interaction. The renormalization effect in these samples is shown to be more than 0.1 eV, on the same order of magnitude as the band gap itself. Existing models do not explain such large relative changes in band gap and are not entirely self-consistent. An improved theory for the renormalization in narrow gap semiconductors is required.

Highlights

  • Optical absorption edge measurements are performed on I doped PbTe using diffuse reflectance infrared Fourier transform spectroscopy

  • Doped semiconductors, including most good thermoelectric materials, have free carrier contributions to the optical absorption that can complicate the estimate of the band gap

  • While the Diffuse reflectance infrared Fourier transform spectroscopy (DRIFTS) method of measuring the optical absorption has been thoroughly explored in catalysis research and has shown some promise for quantifying chemical reactions [88, 89], as a technique for precisely determining band gaps in semiconductors diffuse reflectance has only proven semi-quantitative (±0.1 eV) [90]

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Summary

Introduction

Optical absorption edge measurements are performed on I doped PbTe using diffuse reflectance infrared Fourier transform spectroscopy. Doped semiconductors, including most good thermoelectric materials, have free carrier contributions to the optical absorption that can complicate the estimate of the band gap.

Results
Conclusion

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