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    Electron-phonon coupling in magnetic materials using the local spin density approximation

    Álvaro Adrián Carrasco Álvarez1,*, Matteo Giantomassi1, Jae-Mo Lihm1, Guillaume E. Allemand2, Maxime Mignolet3, Matthieu Verstraete3,4, and Samuel Poncé1,5,†

    • 1European Theoretical Spectroscopy Facility, Institute of Condensed Matter and Nanosciences, Université catholique de Louvain, Chemin des Étoiles 8, B-1348 Louvain-la-Neuve, Belgium
    • 2European Theoretical Spectroscopy Facility, Nanomat/Q-Mat, Université de Liège (B5), B-4000 Liège, Belgium
    • 3European Theoretical Spectroscopy Facility, Nanomat Q-Mat, University of Liège, 4000 Liège, Belgium
    • 4ITP Department of Physics, University of Utrecht, 3508 TA Utrecht, The Netherlands
    • 5WEL Research Institute, avenue Pasteur 6, 1300 Wavre, Belgium

    • *Contact author: alvaro.carrasco@uclouvain.be
    • †Contact author: samuel.ponce@uclouvain.be

    Phys. Rev. B 114, 074411 – Published 10 August, 2026

    DOI: https://doi.org/10.1103/gpf5-p4sn

    Abstract

    Magnetic materials are crucial for manipulating electron spin and magnetic fields, enabling applications in data storage, spintronics, charge transport, and energy conversion; they also provide insight into fundamental quantum phenomena. In numerous applications, the interaction between electrons and lattice vibrations, known as electron-phonon coupling, can be of significant importance. In that regard, we extend the epw package to be able to interpolate the electron-phonon matrix elements combining perturbation theory and maximally localized Wannier functions. This enables the use of dense momentum grids at a reasonable computational cost when computing electron-phonon related quantities and physical properties. We validate our implementation considering ferromagnetic iron and nickel, where we explore the phonon induced mass enhancement and Eliashberg spectral function finding different importance of each spin channel for both compounds. Furthermore, we evaluate the carrier resistivity at finite temperatures for both systems, considering the role of the magnetic phase in carrier transport. Our findings indicate that in the case of Fe, the primary contributor to resistivity is electron-phonon scattering. In contrast, for Ni, electron-phonon scattering constitutes less than one-third of the resistivity, underscoring a fundamental difference in the transport properties of the two systems.

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