Thermodynamics of $s_{\pm}-to-s_{++}$ transition in iron pnictides in the vicinity of the Born limit

TL;DR

This paper investigates the thermodynamic nature of the disorder-induced transition between $s_{ ext{±}}$ and $s_{ ext{++}}$ superconducting states in iron pnictides, revealing a first-order transition near the Born limit with hysteresis and a phase diagram.

Contribution

It provides a detailed thermodynamic analysis of the $s_{ ext{±}}$ to $s_{ ext{++}}$ transition, demonstrating the first-order nature and mapping the phase diagram with a critical end point.

Findings

The transition is first-order with hysteresis near the Born limit.

A phase diagram with a critical end point is constructed.

Above the critical point, the transition becomes a crossover.

Abstract

To study thermodynamical properties of the disorder-induced transition between $s_{\pm}$ and $s_{++}$ superconducting gap functions, we calculate the grand thermodynamic potential $\Omega$ in the normal and the superconducting states. Expression for the difference between the two, $\Delta\Omega$, is derived for a two-band model for Fe-based systems with nonmagnetic impurities. The disorder is considered in a $\mathcal{T}$-matrix approximation within the multiband Eliashberg theory. In the vicinity of the Born limit near the $s_{\pm}$-to-$s_{++}$ transition, we find two solutions obtained for opposite directions of the system's evolution with respect to the impurity scattering rate. By calculating the change in entropy $\Delta S$ and the change in electronic specific heat $\Delta C$ from $\Delta\Omega$, we show that such a hysteresis is not due to the time-reversal symmetry breaking state, but it rather points out to the first order phase transition induced by the nonmagnetic disorder. Based on the $\Delta\Omega$ calculations, phase diagram is plotted representing the energetically favourable $s_{\pm}$ and $s_{++}$ states and the transition between them. At finite temperature, a first order phase transition line there is limited by a critical end point. Above that point, the sharp $s_{\pm} \to s_{++}$ transition transforms to a crossover between $s_{\pm}$ and $s_{++}$ states.