Abstract

We numerically study the phase structure of the $CP(1)$ model in the presence of a topological $\ensuremath{\theta}$-term, a regime afflicted by the sign problem for conventional lattice Monte Carlo simulations. Using a bond-weighted tensor renormalization group method, we compute the free energy for inverse couplings ranging from $0\ensuremath{\le}\ensuremath{\beta}\ensuremath{\le}1.1$ and find a $CP$-violating, first-order phase transition at $\ensuremath{\theta}=\ensuremath{\pi}$. In contrast to previous findings, our numerical results provide no evidence for a critical coupling ${\ensuremath{\beta}}_{c}<1.1$ above which a second-order phase transition emerges at $\ensuremath{\theta}=\ensuremath{\pi}$ and/or the first-order transition line bifurcates at $\ensuremath{\theta}\ensuremath{\ne}\ensuremath{\pi}$. If such a critical coupling exists, as suggested by Haldane's conjecture, our study indicates that is larger than ${\ensuremath{\beta}}_{c}>1.1$.

Highlights

  • The CPðN − 1Þ models in 1 þ 1 dimensions share many properties with QCD in 3 þ 1 dimensions, among them confinement, asymptotic freedom, instantons, a 1=N expansion, a topological charge, and a θ-term

  • Using again the tensor renormalization group (TRG) approach, we study the model in a region around θ 1⁄4 π, where we carefully estimate our systematic errors due to the finite values of ðD; kmax; χθ; VÞ

  • We find that the first-order transition at θ 1⁄4 π persists up to β 1⁄4 1.1 without any bifurcation, and we observe no indication that the phase transition at θ 1⁄4 π becomes of second order for β > βc

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Summary

INTRODUCTION

The CPðN − 1Þ models in 1 þ 1 dimensions share many properties with QCD in 3 þ 1 dimensions, among them confinement, asymptotic freedom, instantons, a 1=N expansion, a topological charge, and a θ-term They serve as benchmark models for developing and testing both new numerical techniques and new proposed solutions to open questions of QCD. The θ-term gives rise to an imaginary contribution to the action in the Euclidean formulation of lattice gauge theories This complex action problem, called the sign problem [3], prevents the successful application of Markov chain Monte Carlo (MCMC) methods for large values of the topological vacuum angle θ. The phase diagram of the CPð1Þ model with a θ-term has been studied with a strong coupling analysis [48], Monte Carlo simulations [50], and TRG studies [34,35].

MODEL AND METHODS
RESULTS
CPð1Þ model with θ-term
DISCUSSION AND CONCLUSIONS
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