scholarly journals On mirror symmetry in three dimensional Abelian gauge theories

1999 ◽  
Vol 1999 (04) ◽  
pp. 021-021 ◽  
Author(s):  
Anton Kapustin ◽  
Matthew J Strassler
2014 ◽  
Vol 29 (32) ◽  
pp. 1530004 ◽  
Author(s):  
Heng-Yu Chen ◽  
Hsiao-Yi Chen ◽  
Jun-Kai Ho

We explicitly apply localization results to study the interpolation between three- and two-dimensional mirror symmetries for Abelian gauge theories with four supercharges. We first use the ellipsoid [Formula: see text] partition functions to verify the mirror symmetry between a pair of general three-dimensional 𝒩 = 2 Abelian Chern–Simons quiver gauge theories. These expressions readily factorize into holomorphic blocks and their antiholomorphic copies, so we can also obtain the partition functions on S1×S2 via fusion procedure. We then demonstrate S1×S2 partition functions for the three-dimensional Abelian gauge theories can be dimensionally reduced to the S2 partition functions of 𝒩 = (2, 2) GLSM and Landau–Ginzburg model for the corresponding two-dimensional mirror pair, as anticipated previously in M. Aganagic et al., J. High Energy Phys.0107, 022 (2001). We also comment on the analogous interpolation for the non-Abelian gauge theories and compute the K-theory vortex partition function for a simple limit to verify the prediction from holomorphic block.


2020 ◽  
Vol 2020 (11) ◽  
Author(s):  
Andrés Collinucci ◽  
Roberto Valandro

Abstract We propose a string theory realization of three-dimensional $$ \mathcal{N} $$ N = 4 quiver gauge theories with special unitary gauge groups. This is most easily understood in type IIA string theory with D4-branes wrapped on holomorphic curves in local K3’s, by invoking the Stückelberg mechanism. From the type IIB perspective, this is understood as simply compactifying the familiar Hanany-Witten (HW) constructions on a T3. The mirror symmetry duals are easily derived. We illustrate this with various examples of mirror pairs.


1997 ◽  
Vol 490 (1-2) ◽  
pp. 107-120 ◽  
Author(s):  
Massimo Porrati ◽  
Alberto Zaffaroni

2009 ◽  
Vol 70 (12) ◽  
pp. 4402-4421 ◽  
Author(s):  
Vieri Benci ◽  
Donato Fortunato

1997 ◽  
Vol 493 (1-2) ◽  
pp. 101-147 ◽  
Author(s):  
Jan de Boer ◽  
Kentaro Hori ◽  
Hirosi Ooguri ◽  
Yaron Oz

1997 ◽  
Vol 493 (1-2) ◽  
pp. 148-176 ◽  
Author(s):  
Jan de Boer ◽  
Kentaro Hori ◽  
Hirosi Ooguri ◽  
Yaron Oz ◽  
Zheng Yin

1996 ◽  
Vol 387 (3) ◽  
pp. 513-519 ◽  
Author(s):  
K. Intriligator ◽  
N. Seiberg

2021 ◽  
Vol 2021 (7) ◽  
Author(s):  
Anindya Dey

Abstract Mirror symmetry, a three dimensional $$ \mathcal{N} $$ N = 4 IR duality, has been studied in detail for quiver gauge theories of the ADE-type (as well as their affine versions) with unitary gauge groups. The A-type quivers (also known as linear quivers) and the associated mirror dualities have a particularly simple realization in terms of a Type IIB system of D3-D5-NS5-branes. In this paper, we present a systematic field theory prescription for constructing 3d mirror pairs beyond the ADE quiver gauge theories, starting from a dual pair of A-type quivers with unitary gauge groups. The construction involves a certain generalization of the S and the T operations, which arise in the context of the SL(2, ℤ) action on a 3d CFT with a U(1) 0-form global symmetry. We implement this construction in terms of two supersymmetric observables — the round sphere partition function and the superconformal index on S2 × S1. We discuss explicit examples of various (non-ADE) infinite families of mirror pairs that can be obtained in this fashion. In addition, we use the above construction to conjecture explicit 3d $$ \mathcal{N} $$ N = 4 Lagrangians for 3d SCFTs, which arise in the deep IR limit of certain Argyres-Douglas theories compactified on a circle.


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