Closure of the entanglement gap at quantum criticality: The case of the Quantum Spherical Model

TL;DR

This paper investigates how the entanglement gap behaves at a quantum critical point in the quantum spherical model, revealing it vanishes logarithmically and reflecting universal critical behavior.

Contribution

It analytically demonstrates the logarithmic vanishing of the entanglement gap at criticality and links this to changes in the eigenvector structure of the correlator.

Findings

Entanglement gap vanishes as π²/ln(L) at criticality

Rescaled gap δξ·ln(L) crosses at the transition for different sizes

Eigenvector structure of the correlator signals phase change

Abstract

The study of entanglement spectra is a powerful tool to detect or elucidate universal behaviour in quantum many-body systems. We investigate the scaling of the entanglement (or Schmidt) gap $\delta\xi$, i.e., the lowest laying gap of the entanglement spectrum, at a two-dimensional quantum critical point. We focus on the paradigmatic quantum spherical model, which exhibits a second-order transition, and is mappable to free bosons with an additional external constraint. We analytically show that the Schmidt gap vanishes at the critical point, although only logarithmically. For a system on a torus and the half-system bipartition, the entanglement gap vanishes as $\pi^2/\ln(L)$, with $L$ the linear system size. The entanglement gap is nonzero in the paramagnetic phase and exhibits a faster decay in the ordered phase. The rescaled gap $\delta\xi\ln(L)$ exhibits a crossing for different system sizes at the transition, although logarithmic corrections prevent a precise verification of the finite-size scaling. Interestingly, the change of the entanglement gap across the phase diagram is reflected in the zero-mode eigenvector of the spin-spin correlator. At the transition quantum fluctuations give rise to a non-trivial structure of the eigenvector, whereas in the ordered phase it is flat. We also show that the vanishing of the entanglement gap at criticality can be qualitatively but not quantitatively captured by neglecting the structure of the zero-mode eigenvector.