The dynamical pairing susceptibility in a quantum-critical metal remains finite and positive exactly at the superconducting instability for a constant source, then becomes a non-unique function of a free parameter below it.
Instability of metals with respect to strong electron-phonon interaction
1 Pith paper cite this work. Polarity classification is still indexing.
abstract
We show that thermal equilibrium between conduction electrons and phonons becomes kinetically unstable when the renormalized electron-phonon coupling exceeds a certain threshold. We prove that negative electronic specific heat, $C_\mathrm{el} < 0$, is sufficient to trigger the instability. Specifically, the instability sets in as soon as the quasiparticle weight becomes negative over a range of energies, even before $C_\mathrm{el}$ turns negative. This is an inherently nonequilibrium phenomenon, occurring prior to the formation of any equilibrium phase. Depending on the system, it can proceed along different pathways, ultimately resulting in a structural transition to an insulating or metallic state.
fields
cond-mat.supr-con 1years
2024 1verdicts
CONDITIONAL 1representative citing papers
citing papers explorer
-
Non-BCS behavior of the pairing susceptibility near the onset of superconductivity in a quantum-critical metal
The dynamical pairing susceptibility in a quantum-critical metal remains finite and positive exactly at the superconducting instability for a constant source, then becomes a non-unique function of a free parameter below it.