Superconducting Chevrel phase PbMo6S8 from first principles

Chevrel ternary superconductors show an intriguing coexistence of molecular aspects, large electron-phonon and electron-electron correlations, which to some extent still impedes their quantitative understanding. We present a first principles study on the prototypical Chevrel compound PbMo6S8, including electronic, structural and vibrational properties at zero and high pressure. We confirm the presence of an extremely strong electron-phonon coupling, linked to the proximity to a R (3) over bar -P (1) over bar structural phase transition, which weakens as the system, upon applied pressures, is driven away from the phase boundary. A detailed description of the superconducting state is obtained by means of fully ab initio superconducting density-functional theory (SCDFT). SCDFT accounts for the role of phase instability, electron-phonon coupling with different intra- and intermolecular phonon modes, and without any empirical parameter, and accurately reproduces the experimental critical temperature and gap. This study provides the conclusive confirmation that Chevrel phases are phonon driven superconductors mitigated, however, by an uncommonly strong Coulomb repulsion. The latter is generated by the combined effect of repulsive Mo states at the Fermi energy and a band gap in close proximity to the Fermi level. This is crucial to rationalize why Chevrel phases, in spite of their extreme electron-phonon coupling, have critical temperatures below 15 K. In addition, we predict the evolution of the superconducting critical temperature as a function of the external pressure, showing an excellent agreement with available experimental data.

Automated summary

Through first-principles study, a strong electron-phonon coupling linked to a structural phase transition and mitigated by Coulomb repulsion is found in Chevrel ternary superconductors. The study provides conclusive evidence explaining why Chevrel phases, despite their extreme electron-phonon coupling, have critical temperatures below 15K. Additionally, the predicted evolution of the superconducting critical temperature with external pressure agrees well with experimental data.