Abstract

We study two-dimensional $\mathcal{N}{=}(0,2)$ supersymmetric gauged linear sigma models (GLSMs) using supersymmetric localization. We consider $\mathcal{N}{=}(0,2)$ theories with an $R$-symmetry, which can always be defined on curved space by a pseudo-topological twist while preserving one of the two supercharges of flat space. For GLSMs which are deformations of $\mathcal{N}{=}(2,2)$ GLSMs and retain a Coulomb branch, we consider the $A/2$-twist and compute the genus-zero correlation functions of certain pseudo-chiral operators, which generalize the simplest twisted chiral ring operators away from the $\mathcal{N}{=}(2,2)$ locus. These correlation functions can be written in terms of a certain residue operation on the Coulomb branch, generalizing the Jeffrey-Kirwan residue prescription relevant for the $\mathcal{N}{=}(2,2)$ locus. For abelian GLSMs, we reproduce existing results with new formulas that render the quantum sheaf cohomology relations and other properties manifest. For non-abelian GLSMs, our methods lead to new results. As an example, we briefly discuss the quantum sheaf cohomology of the Grassmannian manifold.

Highlights

  • Supersymmetric localization of the two-dimensional gauged linear sigma model (GLSM) has proven an extremely useful tool in the study of two-dimensional superconformal theories and of string compactifications — see e.g. [1,2,3,4,5,6,7,8] for some of the most important recent progress in that direction

  • We study two-dimensional N =(0, 2) supersymmetric gauged linear sigma models (GLSMs) using supersymmetric localization

  • We focus on the case of an N =(0, 2) GLSM with an N =(2, 2) locus — that is, the theory is a continuous deformation of an N =(2, 2) theory, to which it reduces at a special locus in parameter space

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Summary

Introduction

Supersymmetric localization of the two-dimensional gauged linear sigma model (GLSM) has proven an extremely useful tool in the study of two-dimensional superconformal theories and of string compactifications — see e.g. [1,2,3,4,5,6,7,8] for some of the most important recent progress in that direction. The GLSMs that we consider provide simple ultraviolet (UV) completions of non-linear sigma models (NLSM) on Kahler varieties X endowed with an holomorphic vector bundle (more generally, a locally free sheaf) E which is a deformation of the tangent bundle T X, and reduces to it on the N =(2, 2) locus. We consider the N =(0, 2) GLSM for the Grassmannian manifold with a deformed tangent bundle and compute the A/2-twisted correlation functions. This leads to a prediction for the quantum sheaf cohomology of this model, which will be studied further in [43, 44]. We refer to appendix A for a summary of our curvedspace conventions, and for a review of N =(0, 2) supersymmetry in flat space

Background supergravity and the pseudo-topological twist
Supersymmetry multiplets
General multiplet
Chiral multiplets
Fermi multiplets
A Fermi multiplet ΛI of R-charge rI has components
Vector multiplet
Charged chiral and Fermi multiplets
Conserved current and background vector multiplet
Kinetic terms
Superpotential terms
Fayet-Iliopoulos terms
GLSM field content and anomalies
Pseudo-topological observables
Supersymmetric locus and zero-modes on the sphere
Quantum sheaf cohomology relations
The Jeffrey-Kirwan-Grothendieck residue
Derivation of the JKG residue formula
Generalities
The rank-one case
Comparison to previous results
Some properties of the correlation functions
Abelian examples
The quintic
Non-abelian examples
Generalizations
General multiplet The general multiplet S corresponds to a superfield
Full Text
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