Abstract

We discuss the lattice formulation of the 't Hooft surface, that is, the two-dimensional surface operator of a dual variable. The 't Hooft surface describes the world sheets of topological vortices. We derive the formulas to calculate the expectation value of the 't Hooft surface in the multiple-charge lattice Abelian Higgs model and in the lattice non-Abelian Higgs model. As the first demonstration of the formula, we compute the intervortex potential in the charge-2 lattice Abelian Higgs model.

Highlights

  • Topological orders are quantum phases beyond the Landau theory of symmetry breaking [1]

  • We study the ’t Hooft surface in lattice gauge theory

  • We focus on the lattice gauge Higgs

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Summary

INTRODUCTION

Topological orders are quantum phases beyond the Landau theory of symmetry breaking [1]. The ’t Hooft surface gives the criterion for the confinement of the fractionally charged vortices It plays an essential role in the topological order of Cooper pairs in superconductors [16,22,23] and that of diquarks in color superconductors [17,24,25,26,27]. It might seem impossible to calculate the expectation values of the ’t Hooft operators in a quantitative manner This is possible in lattice gauge theory. It was applied to several lattice simulations [28,29,30,31,32,33,34,35,36,37,38] This can be generalized to higher-dimensional defects, say, the ’t Hooft surface. The Euclidean fourdimensional lattice is considered and the lattice unit is used throughout the paper

DUAL LATTICE AND DUAL VARIABLE
ABELIAN HIGGS MODEL
NON-ABELIAN HIGGS MODEL
SIMULATION
SUMMARY
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