Pomeranchuk instability in the nematic phase of two monolayer FeSe/SrTiO3

TL;DR

This paper provides direct evidence that Pomeranchuk instability drives nematicity in two monolayer FeSe/SrTiO3, revealing momentum-dependent electronic order and its potential link to superconductivity.

Contribution

The study demonstrates, through ARPES measurements, that nematicity in FeSe/SrTiO3 originates from Pomeranchuk instability, clarifying its nature in a system without magnetic order.

Findings

Degeneracy of dxz and dyz bands at the Brillouin zone center

Significant band separation at the zone corner

Momentum-dependent nematicity indicating Pomeranchuk instability

Abstract

Nematicity, where electrons break rotational symmetry while preserving translational symmetry, is ubiquitous in strongly correlated quantum matters, including high-Tc cuprates and iron-based superconductors. A central question in nematicity is whether it is driven by Pomeranchuk instability in momentum space or orbital order (polarization) in real space, especially as nematicity intertwines with superconductivity. FeSe/SrTiO3 (STO), where nematicity occurs without long-range magnetic order, is an ideal platform for studying the nature and origin of the electronic nematicity. Here we present direct evidence of Pomeranchuk nematic order in two monolayer FeSe/STO using angle-resolved photoemission spectroscopy, revealing a remarkable degeneracy of dxz and dyz bands at the Brillouin zone center, but a significant band separation at the zone corner. This momentum-dependent nematicity demonstrates that nematicity in FeSe/STO originates from the Pomeranchuk instability, offering insights into the relationship between nematicity and superconductivity. Our results establish two-dimensional FeSe thin film as a powerful platform for investigating quantum physics under complex intertwinement.