Non-BCS behavior of the pairing susceptibility near the onset of superconductivity in a quantum-critical metal

TL;DR

This paper investigates the unique behavior of pairing susceptibility in quantum-critical metals, revealing non-BCS features and a multi-critical transition with multiple superconducting states emerging simultaneously.

Contribution

It provides a detailed analysis of the dynamical pairing susceptibility in quantum-critical metals, highlighting non-BCS behavior and the multi-critical nature of the superconducting transition.

Findings

Pairing susceptibility diverges only for certain initial conditions.

Below the transition, susceptibility becomes non-unique and depends on a continuous parameter.

Multiple superconducting states emerge simultaneously near the transition.

Abstract

We analyze the dynamical pairing susceptibility $\chi_{pp} (\omega_m)$ at $T=0$ in a quantum-critical metal, where superconductivity emerges out of a non-Fermi liquid ground state once the pairing interaction exceeds a certain threshold. We obtain $\chi_{pp} (\omega_m)$ as the ratio of the fully dressed dynamical pairing vertex $\Phi (\omega_m)$ and the bare $\Phi_0 (\omega_m)$ (both infinitesimally small). For superconductivity out of a Fermi liquid, the pairing susceptibility is positive above $T_c$, diverges at $T_c$, and becomes negative below it. For superconductivity out of a non-Fermi liquid, the behavior of $\chi_{pp} (\omega_m)$ is different in two aspects: (i) it diverges at the onset of pairing at $T=0$ only for a certain subclass of bare $\Phi_0 (\omega_m)$ and remains non-singular for other $\Phi_0 (\omega_m)$, and (ii) below the instability, it becomes a non-unique function of a continuous parameter $\phi$ for an arbitrary $\Phi_0 (\omega_m)$. The susceptibility is negative in some range of $\phi$ and diverges at the boundary of this range. We argue that this behavior of the susceptibility reflects a multi-critical nature of a superconducting transition in a quantum-critical metal when immediately below the instability an infinite number of superconducting states emerges simultaneously with different amplitudes of the order parameter down to an infinitesimally small one.