Exact degeneracy of Casimir energy for N $$ \mathcal{N} $$ = 4 supersymmetric Yang-Mills theory on ADE singularities and S-duality

Abstract Classically, the ground states of N $$ \mathcal{N} $$ = 4 supersymmetric Yang-Mills theory on ℝ × S 3/Γ where Γ is a discrete ADE subgroup of SU(2) are represented by flat Wilson lines winding around the ADE singularity. By a duality relating such ground states to WZW conformal blocks, the...

Full description

Saved in:
Bibliographic Details
Main Author: Chao Ju
Format: Article
Language:English
Published: SpringerOpen 2024-08-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP08(2024)037
Tags: Add Tag
No Tags, Be the first to tag this record!
_version_ 1846158838698344448
author Chao Ju
author_facet Chao Ju
author_sort Chao Ju
collection DOAJ
description Abstract Classically, the ground states of N $$ \mathcal{N} $$ = 4 supersymmetric Yang-Mills theory on ℝ × S 3/Γ where Γ is a discrete ADE subgroup of SU(2) are represented by flat Wilson lines winding around the ADE singularity. By a duality relating such ground states to WZW conformal blocks, the ground state degeneracy cannot be lifted by quantum corrections. Using the superconformal index, we compute the supersymmetric Casimir energy of each flat Wilson line for SU(2) SYM on different ADE singularities and find that the flat Wilson lines all have the same supersymmetric Casimir energy. We argue that this exact degeneracy is peculiar to N $$ \mathcal{N} $$ = 4 supersymmetry and show that the degeneracy is lifted when the number of supersymmetry is reduced. In particular, we uncover a surprising result for the ground state structure of the conformal N $$ \mathcal{N} $$ = 2 SU(2) four-flavor theory on S 3/Γ. For N $$ \mathcal{N} $$ = 4 SYM, S-duality maps the ground state Wilson lines to ground state t’ Hooft lines taking values in the Langlands dual group. We show that the supersymmetric Casimir energy of the t’ Hooft line ground states is the same as the Wilson line ground states. This can be viewed as a ground state test of S-duality.
format Article
id doaj-art-c8cd62455df14bc7b1c7dc739775c08d
institution Kabale University
issn 1029-8479
language English
publishDate 2024-08-01
publisher SpringerOpen
record_format Article
series Journal of High Energy Physics
spelling doaj-art-c8cd62455df14bc7b1c7dc739775c08d2024-11-24T12:07:54ZengSpringerOpenJournal of High Energy Physics1029-84792024-08-012024813810.1007/JHEP08(2024)037Exact degeneracy of Casimir energy for N $$ \mathcal{N} $$ = 4 supersymmetric Yang-Mills theory on ADE singularities and S-dualityChao Ju0Berkeley Center for Theoretical Physics and Department of Physics, University of CaliforniaAbstract Classically, the ground states of N $$ \mathcal{N} $$ = 4 supersymmetric Yang-Mills theory on ℝ × S 3/Γ where Γ is a discrete ADE subgroup of SU(2) are represented by flat Wilson lines winding around the ADE singularity. By a duality relating such ground states to WZW conformal blocks, the ground state degeneracy cannot be lifted by quantum corrections. Using the superconformal index, we compute the supersymmetric Casimir energy of each flat Wilson line for SU(2) SYM on different ADE singularities and find that the flat Wilson lines all have the same supersymmetric Casimir energy. We argue that this exact degeneracy is peculiar to N $$ \mathcal{N} $$ = 4 supersymmetry and show that the degeneracy is lifted when the number of supersymmetry is reduced. In particular, we uncover a surprising result for the ground state structure of the conformal N $$ \mathcal{N} $$ = 2 SU(2) four-flavor theory on S 3/Γ. For N $$ \mathcal{N} $$ = 4 SYM, S-duality maps the ground state Wilson lines to ground state t’ Hooft lines taking values in the Langlands dual group. We show that the supersymmetric Casimir energy of the t’ Hooft line ground states is the same as the Wilson line ground states. This can be viewed as a ground state test of S-duality.https://doi.org/10.1007/JHEP08(2024)037Duality in Gauge Field TheoriesSupersymmetric Gauge TheorySupersymmetry and DualityChern-Simons Theories
spellingShingle Chao Ju
Exact degeneracy of Casimir energy for N $$ \mathcal{N} $$ = 4 supersymmetric Yang-Mills theory on ADE singularities and S-duality
Journal of High Energy Physics
Duality in Gauge Field Theories
Supersymmetric Gauge Theory
Supersymmetry and Duality
Chern-Simons Theories
title Exact degeneracy of Casimir energy for N $$ \mathcal{N} $$ = 4 supersymmetric Yang-Mills theory on ADE singularities and S-duality
title_full Exact degeneracy of Casimir energy for N $$ \mathcal{N} $$ = 4 supersymmetric Yang-Mills theory on ADE singularities and S-duality
title_fullStr Exact degeneracy of Casimir energy for N $$ \mathcal{N} $$ = 4 supersymmetric Yang-Mills theory on ADE singularities and S-duality
title_full_unstemmed Exact degeneracy of Casimir energy for N $$ \mathcal{N} $$ = 4 supersymmetric Yang-Mills theory on ADE singularities and S-duality
title_short Exact degeneracy of Casimir energy for N $$ \mathcal{N} $$ = 4 supersymmetric Yang-Mills theory on ADE singularities and S-duality
title_sort exact degeneracy of casimir energy for n mathcal n 4 supersymmetric yang mills theory on ade singularities and s duality
topic Duality in Gauge Field Theories
Supersymmetric Gauge Theory
Supersymmetry and Duality
Chern-Simons Theories
url https://doi.org/10.1007/JHEP08(2024)037
work_keys_str_mv AT chaoju exactdegeneracyofcasimirenergyfornmathcaln4supersymmetricyangmillstheoryonadesingularitiesandsduality