Impact of Crystal Structure on the Thermoelectric Properties of n-Type SrTiO3

09 April 2025, Version 1
This content is a preprint and has not undergone peer review at the time of posting.

Abstract

We present a detailed first-principles study of the electrical and thermal transport, and the thermoelectric figure of merit zT , of the oxide perovskite SrTiO3 in the orthorhombic Pnma, tetragonal I4/mcm and cubic Pm-3m phases. Analysis of the lattice thermal conductivity shows that the “particle-like” contribution, κ_p is highest in the Pm-3m phase due to larger phonon group velocities. We also find that all three phases show significant heat transport through glass-like intraband tunnelling. On the other hand, we predict the cubic and orthorhombic phases to show superior n-type conductivity, due to significantly stronger polar-optic phonon scattering and shorter electron lifetimes in the tetragonal phase. Due to its superior electrical properties, we predict that the Pm-3m phase will attain a 25% larger high-temperature zT than the I4/mcm phase, while we predict the best zT can be obtained for the Pnma phase due to its favourable electrical properties and low κ_latt. This work provides new insight into the impact of structure type on the thermoelectric performance of oxide perovskites, and indicates targeting particular structure types, e.g. through chemical doping, could provide a facile route to optimising the zT of SrTiO3 and related systems.

Keywords

strontium titanate
thermoelectrics
first-principles computational modelling
electronic transport
lattice thermal conductivity

Supplementary materials

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Electronic Supporting Information
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Electronic supporting information: optimised lattice parameters and comparison to experimental measurements; analysis of the “particle-like” contributions to the lattice thermal conductivity at 300 K; anisotropy in the κ_latt at 1000 K; “scattering phase space’; functions for the I4/mcm and Pnma phases of SrTiO3; anisotropy in the electrical transport at 1000 K; analysis of the electron mobility as a function of carrier concentration at 1000 K; and anisotropy in the thermoelectric figure of merit at 400, 600 and 1000 K.
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