The critical endpoint in the 2d U(1) gauge-Higgs model at topological angle $\theta=\pi$

TL;DR

This paper investigates the phase structure of 2d U(1) gauge-Higgs models with a topological term at θ=π, demonstrating a phase transition in the charge-1 case and a crossover in the charge-2 case, using novel discretization and worldline methods.

Contribution

The authors introduce a mixed group- and algebra-valued discretization scheme and a worldline/worldsheet representation to study the θ=π effects in 2d U(1) gauge-Higgs systems, overcoming complex action issues.

Findings

Charge-1 system exhibits a 2d Ising universality class phase transition.

Charge-2 system shows no true phase transition, only a rapid crossover.

Exact implementation of charge conjugation symmetry at θ=π.

Abstract

We study 2d U(1) gauge Higgs systems with a $\theta$-term. For properly discretizing the topological charge as an integer we introduce a mixed group- and algebra-valued discretization (MGA scheme) for the gauge fields, such that the charge conjugation symmetry at $\theta = \pi$ is implemented exactly. The complex action problem from the $\theta$-term is overcome by exactly mapping the partition sum to a worldline/worldsheet representation. Using Monte Carlo simulation of the worldline/worldsheet representation we study the system at $\theta = \pi$ and show that as a function of the mass parameter the system undergoes a phase transition. Determining the critical exponents from a finite size scaling analysis we show that the transition is in the 2d Ising universality class. We furthermore study the U(1) gauge Higgs systems at $\theta = \pi$ also with charge 2 matter fields, where an additional $Z_2$ symmetry is expected to alter the phase structure. Our results indicate that for charge 2 a true phase transition is absent and only a rapid crossover separates the large and small mass regions.