Abstract

We study the dependence of supersymmetric partition functions on continuous parameters for the flavor symmetry group, GF, for 2d mathcal{N} = (0, 2) and 4d mathcal{N} = 1 supersymmetric quantum field theories. In any diffeomorphism-invariant scheme and in the presence of GF ’t Hooft anomalies, the supersymmetric Ward identities imply that the partition function has a non-holomorphic dependence on the flavor parameters. We show this explicitly for the 2d torus partition function, {Z}_{T^2} , and for a large class of 4d partition functions on half-BPS four-manifolds, {Z}_{{mathcal{M}}^4} — in particular, for mathcal{M} 4 = S3 × S1 and mathcal{M} 4 = Σg × T2. We propose a new expression for {Z}_{{mathcal{M}}_{d-1}times {S}^1} , which differs from earlier holomorphic results by the introduction of a non-holomorphic “Casimir” pre-factor. The latter is fixed by studying the “high temperature” limit of the partition function. Our proposal agrees with the supersymmetric Ward identities, and with explicit calculations of the absolute value of the partition function using a gauge-invariant zeta-function regularization.

Highlights

  • In this paper, we explore intriguing properties of supersymmetric partition functions in even space-time dimensions.1 In two dimensions, we consider the T 2 partition function of2d N = (0, 2) supersymmetric theories, or elliptic genus [2]

  • We study the dependence of supersymmetric partition functions on continuous parameters for the flavor symmetry group, GF, for 2d N = (0, 2) and 4d N = 1 supersymmetric quantum field theories

  • For simplicity, we focus on the flavor sector and, on the consequences of the flavor ’t Hooft anomalies in the presence of supersymmetry

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Summary

Introduction

We explore intriguing properties of supersymmetric partition functions in even space-time dimensions. In two dimensions, we consider the T 2 partition function of. The relation (1.7) is modified, and the partition function acquires a non-holomorphic dependence on the flavor parameters, that is precisely as required to make its absolute value gauge-invariant These quantum corrections to supersymmetric Ward identities, referred to as “supersymmetry anomalies,” were studied long ago in [14, 15], and more recently in [16,17,18,19,20,21,22]. As an interesting warm-up to the four-dimensional case, let us study the partition function of a 2d N = (0, 2) supersymmetric theory on the torus, in the presence of flat connections for background gauge fields coupling to the flavor symmetry — this is known as the flavored N = (0, 2) elliptic genus

The free fermion and the Quillen anomaly
The elliptic genus and the torus partition function
Non-holomorphy of the supersymmetric partition function ZT 2
Anomalous supersymmetry variation from WZ gauge-fixing
Half-BPS Hermitian geometry
Background vector multiplet and minimal coupling
M4 supersymmetric partition functions and holomorphy
Supersymmetry variation of the effective action
Non-holomorphy of the supersymmetric partition function ZM4
R-symmetry contributions to δζW
The small-βS1 limit and the 3d functional W3d
The holomorphic supersymmetric partition function
The “gauge-invariant” supersymmetric partition function
Four-dimensional conventions
Three-dimensional conventions and dimensional reduction from 4d
Two-dimensional and one-dimensional conventions
C One-loop determinants and ζ-function regularization
Free fermions on T 2
D Large-gauge transformations and the anomaly polynomial
Large gauge transformations for the 4d partition function
Full Text
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