Stokes phenomena in 3d N $$ \mathcal{N} $$ = 2 SQED2 and CP $$ \mathbbm{CP} $$ 1 models

Abstract We propose a novel approach of uncovering Stokes phenomenon exhibited by the holomorphic blocks of CP $$ \mathbbm{CP} $$ 1 model by considering it as a specific decoupling limit of SQED2 model. This approach involves using a ℤ 3 symmetry that leaves the supersymmetric parameter space of SQE...

Full description

Bibliographic Details
Main Authors: Dharmesh Jain, Arkajyoti Manna
Format: Article
Language:English
Published: SpringerOpen 2021-09-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP09(2021)112
id doaj-2d1e98bb396844afb7c3883955daa11c
record_format Article
spelling doaj-2d1e98bb396844afb7c3883955daa11c2021-09-26T11:53:32ZengSpringerOpenJournal of High Energy Physics1029-84792021-09-012021913110.1007/JHEP09(2021)112Stokes phenomena in 3d N $$ \mathcal{N} $$ = 2 SQED2 and CP $$ \mathbbm{CP} $$ 1 modelsDharmesh Jain0Arkajyoti Manna1Department of Theoretical Sciences, S.N. Bose National Centre for Basic SciencesInstitute of Mathematical Sciences, Homi Bhabha National Institute (HBNI)Abstract We propose a novel approach of uncovering Stokes phenomenon exhibited by the holomorphic blocks of CP $$ \mathbbm{CP} $$ 1 model by considering it as a specific decoupling limit of SQED2 model. This approach involves using a ℤ 3 symmetry that leaves the supersymmetric parameter space of SQED2 model invariant to transform a pair of SQED2 holomorphic blocks to get two new pairs of blocks. The original pair obtained by solving the line operator identities of the SQED2 model and the two new transformed pairs turn out to be related by Stokes-like matrices. These three pairs of holomorphic blocks can be reduced to the known triplet of CP $$ \mathbbm{CP} $$ 1 blocks in a particular decoupling limit where two of the chiral multiplets in the SQED2 model are made infinitely massive. This reduction then correctly reproduces the Stokes regions and matrices of the CP $$ \mathbbm{CP} $$ 1 blocks. Along the way, we find six pairs of SQED2 holomorphic blocks in total, which lead to six Stokes-like regions covering uniquely the full parameter space of the SQED2 model.https://doi.org/10.1007/JHEP09(2021)112Chern-Simons TheoriesSupersymmetric Gauge TheoryNonperturbative Effects
collection DOAJ
language English
format Article
sources DOAJ
author Dharmesh Jain
Arkajyoti Manna
spellingShingle Dharmesh Jain
Arkajyoti Manna
Stokes phenomena in 3d N $$ \mathcal{N} $$ = 2 SQED2 and CP $$ \mathbbm{CP} $$ 1 models
Journal of High Energy Physics
Chern-Simons Theories
Supersymmetric Gauge Theory
Nonperturbative Effects
author_facet Dharmesh Jain
Arkajyoti Manna
author_sort Dharmesh Jain
title Stokes phenomena in 3d N $$ \mathcal{N} $$ = 2 SQED2 and CP $$ \mathbbm{CP} $$ 1 models
title_short Stokes phenomena in 3d N $$ \mathcal{N} $$ = 2 SQED2 and CP $$ \mathbbm{CP} $$ 1 models
title_full Stokes phenomena in 3d N $$ \mathcal{N} $$ = 2 SQED2 and CP $$ \mathbbm{CP} $$ 1 models
title_fullStr Stokes phenomena in 3d N $$ \mathcal{N} $$ = 2 SQED2 and CP $$ \mathbbm{CP} $$ 1 models
title_full_unstemmed Stokes phenomena in 3d N $$ \mathcal{N} $$ = 2 SQED2 and CP $$ \mathbbm{CP} $$ 1 models
title_sort stokes phenomena in 3d n $$ \mathcal{n} $$ = 2 sqed2 and cp $$ \mathbbm{cp} $$ 1 models
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2021-09-01
description Abstract We propose a novel approach of uncovering Stokes phenomenon exhibited by the holomorphic blocks of CP $$ \mathbbm{CP} $$ 1 model by considering it as a specific decoupling limit of SQED2 model. This approach involves using a ℤ 3 symmetry that leaves the supersymmetric parameter space of SQED2 model invariant to transform a pair of SQED2 holomorphic blocks to get two new pairs of blocks. The original pair obtained by solving the line operator identities of the SQED2 model and the two new transformed pairs turn out to be related by Stokes-like matrices. These three pairs of holomorphic blocks can be reduced to the known triplet of CP $$ \mathbbm{CP} $$ 1 blocks in a particular decoupling limit where two of the chiral multiplets in the SQED2 model are made infinitely massive. This reduction then correctly reproduces the Stokes regions and matrices of the CP $$ \mathbbm{CP} $$ 1 blocks. Along the way, we find six pairs of SQED2 holomorphic blocks in total, which lead to six Stokes-like regions covering uniquely the full parameter space of the SQED2 model.
topic Chern-Simons Theories
Supersymmetric Gauge Theory
Nonperturbative Effects
url https://doi.org/10.1007/JHEP09(2021)112
work_keys_str_mv AT dharmeshjain stokesphenomenain3dnmathcaln2sqed2andcpmathbbmcp1models
AT arkajyotimanna stokesphenomenain3dnmathcaln2sqed2andcpmathbbmcp1models
_version_ 1716867681341145088