Interplay between superconductivity and non-Fermi liquid at a quantum-critical point in a metal. I: The -model and its phase diagram at . The case
arXiv:2004.13220 · doi:10.1103/PhysRevB.102.024524
Abstract
We analyze a class of quantum-critical models, in which momentum integration and the selection of a particular pairing symmetry can be done explicitly, and the competition between non-Fermi liquid and pairing can be analyzed within an effective model with dynamical electron-electron interaction (the -model). In this paper, the first in the series, we consider the case and . We argue that tendency to pairing is stronger, and the ground state is a superconductor. We argue, however, that superconducting state is highly non-trivial as there exists a discrete set of topologically distinct solutions for the pairing gap (). All solutions have the same spatial pairing symmetry, but differ in the time domain: changes sign times as a function of Matsubara frequency . The solution is sign-preserving and tends to a finite value at , like in BCS theory. The solution corresponds to an infinitesimally small . As a proof, we obtain the exact solution of the linearized gap equation at on the entire frequency axis for all , and an approximate solution of the non-linear gap equation.We argue that the presence of an infinite set of solutions opens up a new channel of gap fluctuations. We extend the analysis to the case where the pairing component of the interaction has additional factor and show that there exists a critical , above which superconductivity disappears, and the ground state becomes a non-Fermi liquid.We show that all solutions develop simultaneously once gets smaller than .
arXiv commentReplaced with the published version
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