Superconductivity near a nematic quantum critical point -- the interplay between hot and lukewarm regions
arXiv:1808.08635 · doi:10.1103/PhysRevB.98.220501
Abstract
We present a strong coupling dynamical theory of the superconducting transition in a metal near a QCP towards nematic order. We use a fermion-boson model, in which we treat the ratio of effective boson-fermion coupling and the Fermi energy as a small parameter . We solve, both analytically and numerically, the linearized Eliashberg equation. Our solution takes into account both strong fluctuations at small momentum transfers and weaker fluctuations at large momentum transfers. The strong fluctuations determine , which is of order for both s- and d- wave pairing. The weaker fluctuations determine the angular structure of the superconducting order parameter along the Fermi surface, separating between hot and lukewarm regions. In the hot regions is largest and approximately constant. Beyond the hot region, whose width is , drops by a factor . The s- and d- wave states are not degenerate but the relative difference is small.
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