# Orbital selective pairing and superconductivity in iron selenides

## TL;DR

This paper proposes an orbital-selective pairing state, called $s \tau_{3}$, to explain the coexistence of $d$-wave resonance and nodeless gaps in iron selenide superconductors, revealing new insights into multiband superconductivity.

## Contribution

It introduces the $s \tau_{3}$ pairing state as a natural explanation for the unique superconducting properties of iron selenides, highlighting the role of orbital selectivity.

## Key findings

- The $s \tau_{3}$ pairing state explains both resonance mode and nodeless gaps.
- Orbital selectivity favors the $s \tau_{3}$ pairing state energetically.
- Multiband effects lead to unconventional superconducting states.

## Abstract

An important challenge in condensed matter physics is understanding iron-based superconductors. Among these systems, the iron selenides hold the record for highest superconducting transition temperature and pose especially striking puzzles regarding the nature of superconductivity. The pairing state of the alkaline iron selenides appears to be of $d$-wave type based on the observation of a resonance mode in neutron scattering, while it seems to be of $s$-wave type from the nodeless gaps observed everywhere on the Fermi surface (FS). Here we propose an orbital-selective pairing state, dubbed $s \tau_{3}$, as a natural explanation of these disparate properties. The pairing function, containing a matrix $\tau_{3}$ in the basis of $3d$-electron orbitals, does not commute with the kinetic part of the Hamiltonian. This dictates the existence of both intraband and interband pairing terms in the band basis. A spin resonance arises from a $d$-wave-type sign change in the intraband pairing component whereas the quasiparticle excitation is fully gapped on the FS due to an $s$-wave-like form factor associated with the addition in quadrature of the intraband and interband pairing terms. We demonstrate that this pairing state is energetically favored when the electron correlation effects are orbitally selective. More generally, our results illustrate how the multiband nature of correlated electrons affords unusual types of superconducting states, thereby shedding new light not only on the iron-based materials but also on a broad range of other unconventional superconductors such as heavy fermion and organic systems.