Nematic chiral Superconductivity driven by chiral loop current order in kagome metals

TL;DR

This paper proposes a mechanism for nematic chiral d-wave superconductivity in kagome metals driven by loop-current order, explaining experimental observations of chirality, nematicity, and topological properties in these materials.

Contribution

It introduces a novel theoretical model linking loop-current order to chiral d-wave superconductivity with topological features in kagome metals.

Findings

Chiral d-wave SC state exhibits nontrivial topological properties.

Nematicity arises when loop-current order coexists with charge-density-wave.

The mechanism explains the emergence of 2x2 pair-density-wave components.

Abstract

The sequence of unconventional quantum phases in the kagome metal AV3Sb5 (A = Cs, Rb, K), including charge-density-wave and loop-current order, gives rise to exotic chiral electronic states that lack time-reversal symmetry (TRS). These unusual low-symmetry electronic states give rise to novel nonreciprocal transport and chiral quasiparticle-interference patterns. Especially, recent experiments have discovered pronounced nematicity and chirality in the superconducting (SC) state. The observed SC state exhibits high sensitively to external magnetic fields, strongly suggesting the breaking of TRS. Furthermore, a small amount of disorders leads to an isotropic s-wave state. In this study, we propose the mechanism of nematic chiral d-wave superconductivity in the presence of loop-current order, emerging from the attractive charge-channel pairing interaction that exists in real kagome metals. An chiral d-wave SC state, which has a nontrivial topological properties, is driven by the TRS breaking pair-hopping mechanism under a sole loop-current order. Notably, chiral SC state exhibits pronounced nematicity when the loop-current order and the Star-of-David charge-density-wave coexist, in spite of the fact that the Fermi surfaces possess almost perfect $C_6$ symmetry. The chiral superconducting state arising from this mechanism is easily switched to conventional s-wave SC by introducing a small amount of impurities. Furthermore, the present mechanism yields a prominent 2x2 pair-density-wave component, consistent with experimental observations. The present study provides insights into the fundamental nature of exotic SC states arising from the loop-current phase in kagome metals.