Abstract

In this paper, we introduce a new set of modular-invariant phase factors for orbifolds with trivially-acting subgroups, analogous to discrete torsion and generalizing quantum symmetries. After describing their basic properties, we generalize decomposition to include orbifolds with these new phase factors, making a precise proposal for how such orbifolds are equivalent to disjoint unions of other orbifolds without trivially-acting subgroups or one-form symmetries, which we check in numerous examples.

Highlights

  • In an orbifold, it is an old story that one has the option of adding modular-invariant phases such as discrete torsion, which in a Γ orbifold are classified by H2(Γ, U(1))

  • E-mail: dgrobbins@albany.edu, ersharpe@vt.edu, tvandermeulen@albany.edu Abstract: In this paper, we introduce a new set of modular-invariant phase factors for orbifolds with trivially-acting subgroups, analogous to discrete torsion and generalizing quantum symmetries

  • In appendix A, we review the analogous result for general orbifold groups G, demonstrating that for a quantum symmetry group G = G/[G, G], the orbifold [X/Γ] for Γ = G × Gwith appropriate discrete torsion is equivalent to [X/[G, G]]

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Summary

Introduction

It is an old story that one has the option of adding modular-invariant phases such as discrete torsion, which in a Γ orbifold are classified by H2(Γ, U(1)). It is the purpose of this paper to describe those novel modular-invariant degrees of freedom explicitly These new degrees of freedom generalize quantum symmetries of orbifolds [11, 12], for which reason we use the same nomenclature, and are specific to orbifolds in which a subgroup of the orbifold group acts trivially on the original space. The quantum symmetries we shall be focused on do not always arise from discrete torsion, and so define new modular-invariant phases — but in which the modular invariance is achieved in a novel fashion These new degrees of freedom arise in the case that a subgroup K of the orbifold group Γ acts trivially.

Review of ordinary quantum symmetries
Basics of general construction
Special case of discrete torsion
General case
General conjecture for decomposition
Extension of Z2 to Z4
Extension of Z2 by Zk
Extension of Z3 to Z9 In this section we start with a G = Z3 orbifold, extend G by K = Z3 to Γ = Z9
Extension of Z2 × Z2 to Z2 × Z4
Without discrete torsion
With discrete torsion
Extension of Z2 × Z2 to D4
Extension of Z2 × Z4 to Z4 Z4
Extension of D4 to Z4 Z4
Without discrete torsion From section 3, we predict that
Extension of Z2 × Z2 to D4 × Z2 × Z2
With discrete torsion in Z2 × Z2 ⊂ Γ
With discrete torsion in D4 ⊂ Γ
Summary
Conclusions
A Notes on conventional quantum symmetries in orbifolds
C Open string sector
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