Acoustic Deformation Potentials of $n$-Type PbTe from First Principles

Abstract

We calculate the uniaxial and dilatation acoustic deformation potentials, ${\Xi }_u^{\text{L}}$ and ${\Xi }_d^{\text{L}}$, of the conduction band L valleys of PbTe from first principles, using the local density approximation (LDA) and hybrid functional (HSE03) exchange-correlation functionals. We find that the choice of a functional does not substantially affect the effective band masses and deformation potentials as long as a physically correct representation of the conduction band states near the band gap has been obtained. Fitting of the electron-phonon matrix elements obtained in density functional perturbation theory (DFPT) with the LDA excluding spin orbit interaction (SOI) gives ${\Xi }_u^{\text{L}}=7.0$~eV and ${\Xi }_d^{\text{L}}=0.4$~eV. Computing the relative shifts of the L valleys induced by strain with the HSE03 functional including SOI gives ${\Xi }_u^{\text{L}}=5.5$~eV and ${\Xi }_d^{\text{L}}=0.8$~eV, in good agreement with the DFPT values. Our calculated values of ${\Xi }_u^{\text{L}}$ agree fairly well with experiment ($\sim 3-4.5$~eV). The computed values of ${\Xi }_d^{\text{L}}$ are substantially smaller than those obtained by fitting electronic transport measurements ($\sim 17-22$~eV), indicating that intravalley acoustic phonon scattering in PbTe is much weaker than previously thought.

arXiv comment13 pages, 4 figures

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