Linear response results for phonons and electron-phonon coupling in hcp Sc - spin fluctuations and implications for superconductivity

TL;DR

This study investigates the electronic, phononic, and electron-phonon interactions in hcp scandium under pressure, revealing strong spin fluctuations that likely suppress superconductivity in the hcp phase but suggest possible superconductivity in the Sc-II phase.

Contribution

It provides detailed calculations of phonon frequencies, electron-phonon coupling, and spin fluctuations in hcp Sc under pressure, highlighting their implications for superconductivity.

Findings

Electron-phonon coupling increases with pressure in hcp Sc.

Spin fluctuations are strong enough to suppress superconductivity in hcp Sc.

Sc-II phase is predicted to be superconducting.

Abstract

We present a study of the electronic structure, phonon frequencies and electron-phonon coupling in hcp Sc under pressure. The electron-phonon coupling constant is found to increase steadily with pressure in the hcp phase, until the pressure reaches a value where the hcp phase becomes unstable. Calculations for the normal pressure $c/a$ ratio predict a phase change somewhere between calculated pressures of 22 and 30 GPa. The calculated frequencies for the equilibrium hcp lattice parameters are in good agreement with the inelastic neutron scattering results. From the measured value of the electronic specific heat constant and the calculated values of the Fermi level density of states and electron-phonon coupling constant, we conclude that the electron-paramagnon coupling constant in hcp Sc should be comparable to the electron-phonon coupling constant. This indicates that the spin fluctuation effects are strong enough to suppress superconductivity completely in hcp Sc. Based on estimates of the electron-paramagnon coupling constants and the calculated or estimated electron-phonon coupling constants, we argue that the hcp phase may become superconducting with a very low transition temperature immediately prior to the transition to the Sc-II phase and that the Sc-II phase should indeed be superconducting.