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Importance of nonlinear long-range electron-phonon interaction for the carrier mobility of anharmonic halide perovskites

Matthew Houtput1, Ingvar Zappacosta1, William Wenborn1, Serghei Klimin1, Samuel Poncé2,3, Jacques Tempere1, and Cesare Franchini4,5

  • 1Theory of Quantum Systems and Complex Systems, Universiteit Antwerpen, B-2000 Antwerpen, Belgium
  • 2European Theoretical Spectroscopy Facility and Institute of Condensed Matter and Nanosciences, Université Catholique de Louvain, Chemin des Étoiles 8, B-1348 Louvain-la-Neuve, Belgium
  • 3WEL Research Institute, avenue Pasteur 6, 1300 Wavre, Belgium
  • 4Faculty of Physics, Computational Materials Physics, University of Vienna, Kolingasse 14-16, A-1090 Vienna, Austria
  • 5Department of Physics and Astronomy, Alma Mater Studiorum - Università di Bologna, 40127 Bologna, Italy

Phys. Rev. B 114, L200301 – Published 8 October, 2026

DOI: https://doi.org/10.1103/jl6h-yzky

Abstract

The interaction between the electrons and the lattice vibrations in a solid is responsible for various important effects, such as formation of polarons, temperature-dependent band gaps, phonon-limited carrier transport, and conventional superconductivity. Most works assume a linear electron-phonon interaction, where the electron only interacts with one phonon at a time. However, the validity of this assumption has not been verified in polar anharmonic materials, where large ionic displacements may invalidate the assumption of linear interaction. Here, we show that nonlinear electron-phonon interactions contribute significantly to the finite-temperature electron mobility of the inorganic lead halide perovskite CsPbI3. The effect of nonlinear interaction is taken into account using the recently derived expression for the long-range part of the one-electron-two-phonon matrix element. We calculate the electron mobility from first principles within the self-energy relaxation-time approximation, treating the electron-phonon coupling in the long-range approximation. Despite these approximations, the calculated mobilities are in good agreement with the available experimental data, while enabling us to isolate and quantify the contribution of nonlinear electron-phonon interactions relative to the conventional linear coupling. We find that the one-electron-two-phonon interaction modifies the temperature dependence of the mobility in CsPbI3 and reduces its room-temperature value by about 10%. This sizable contribution results from the combined effects of strong lattice anharmonicity and large thermal phonon populations, the latter being enhanced by the low phonon frequencies associated with the heavy constituent atoms. These results identify a regime in which nonlinear electron-phonon interactions become relevant and indicate that they should be explicitly considered for finite-temperature properties of anharmonic halide perovskites.

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