Abstract
Migdal-Eliashberg theory is one of the state-of-the-art methods for describing conventional superconductors from first principles. However, widely used implementations assume a constant density of states around the Fermi level, which hinders a proper description of materials with distinct features in its vicinity. Here, we present an implementation of the Migdal-Eliashberg theory within the EPW code that considers the full electronic structure and accommodates scattering processes beyond the Fermi surface. To significantly reduce computational costs, we introduce a non-uniform sampling scheme along the imaginary axis. We demonstrate the power of our implementation by applying it to the sodalite-like clathrates YH6 and CaH6, and to the covalently-bonded H3S and D3S. Furthermore, we investigate the effect of maximizing the density of states at the Fermi level in doped H3S and BaSiH8 within the full-bandwidth treatment compared to the constant-density-of-states approximation. Our findings highlight the importance of this advanced treatment in such complex materials.
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CITATION STYLE
Lucrezi, R., Ferreira, P. P., Hajinazar, S., Mori, H., Paudyal, H., Margine, E. R., & Heil, C. (2024). Full-bandwidth anisotropic Migdal-Eliashberg theory and its application to superhydrides. Communications Physics, 7(1). https://doi.org/10.1038/s42005-024-01528-6
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