Ab initio lattice dynamics and electron-phonon coupling of Bi(111)

TL;DR

This study uses ab initio methods to analyze the lattice dynamics and electron-phonon interactions of Bi(111), revealing surface-specific behaviors and the importance of slab thickness in calculations.

Contribution

It provides a detailed ab initio analysis of Bi(111) surface properties, including electron-phonon coupling, with a focus on convergence and relativistic effects.

Findings

Lattice dynamics are robust and converge at 6 bilayers.

Surface states exhibit moderate electron-phonon coupling (~0.45).

Surface electron-phonon interactions deviate from simple models.

Abstract

We present a comprehensive ab initio study of structural, electronic, lattice dynamical and electron-phonon coupling properties of the Bi(111) surface within density functional perturbation theory. Relativistic corrections due to spin-orbit coupling are consistently taken into account. As calculations are carried out in a periodic slab geometry, special attention is given to the convergence with respect to the slab thickness. Although the electronic structure of Bi(111) thin films varies significantly with thickness, we found that the lattice dynamics of Bi(111) is quite robust and appears converged already for slabs as thin as 6 bilayers. Changes of interatomic couplings are confined mostly to the first two bilayers, resulting in super-bulk modes with frequencies higher than the optic bulk spectrum, and in an enhanced density of states at lower frequencies for atoms in the first bilayer. Electronic states of the surface band related to the outer part of the hole Fermi surfaces exhibit a moderate electron-phonon coupling of about 0.45, which is larger than the coupling constant of bulk Bi. States at the inner part of the hole surface as well as those forming the electron pocket close to the zone center show much increased couplings due to transitions into bulk projected states near Gamma_bar. For these cases, the state dependent Eliashberg functions exhibit pronounced peaks at low energy and strongly deviate in shape from a Debye-like spectrum, indicating that an extraction of the coupling strength from measured electronic self-energies based on this simple model is likely to fail.