On the compactification of 5d theories to 4d
Abstract We study general properties of the mapping between 5d and 4d superconformal field theories (SCFTs) under both twisted circle compactification and tuning of local relevant deformation and CB moduli. After elucidating in generality when a 5d SCFT reduces to a 4d one, we identify nearly all N...
Main Authors: | , |
---|---|
Format: | Article |
Language: | English |
Published: |
SpringerOpen
2021-08-01
|
Series: | Journal of High Energy Physics |
Subjects: | |
Online Access: | https://doi.org/10.1007/JHEP08(2021)017 |
id |
doaj-206cde80ff7343e8b07db5797f91ac2d |
---|---|
record_format |
Article |
spelling |
doaj-206cde80ff7343e8b07db5797f91ac2d2021-08-08T11:43:12ZengSpringerOpenJournal of High Energy Physics1029-84792021-08-012021816110.1007/JHEP08(2021)017On the compactification of 5d theories to 4dMario Martone0Gabi Zafrir1C. N. Yang Institute for Theoretical Physics, Stony Brook UniversityDipartimento di Fisica, Università di Milano-Bicocca & INFN — Sezione di Milano-BicoccaAbstract We study general properties of the mapping between 5d and 4d superconformal field theories (SCFTs) under both twisted circle compactification and tuning of local relevant deformation and CB moduli. After elucidating in generality when a 5d SCFT reduces to a 4d one, we identify nearly all N $$ \mathcal{N} $$ = 1 5d SCFT parents of rank-2 4d N $$ \mathcal{N} $$ = 2 SCFTs. We then use this result to map out the mass deformation trajectories among the rank-2 theories in 4d. This can be done by first understanding the mass deformations of the 5d N $$ \mathcal{N} $$ = 1 SCFTs and then map them to 4d. The former task can be easily achieved by exploiting the fact that the 5d parent theories can be obtained as the strong coupling limit of Lagrangian theories, and the latter by understanding the behavior under compactification. Finally we identify a set of general criteria that 4d moduli spaces of vacua have to satisfy when the corresponding SCFTs are related by mass deformations and check that all our RG-flows satisfy them. Many of the mass deformations we find are not visible from the corresponding complex integrable systems.https://doi.org/10.1007/JHEP08(2021)017Conformal Field TheoryExtended SupersymmetryField Theories in Higher Dimensions |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Mario Martone Gabi Zafrir |
spellingShingle |
Mario Martone Gabi Zafrir On the compactification of 5d theories to 4d Journal of High Energy Physics Conformal Field Theory Extended Supersymmetry Field Theories in Higher Dimensions |
author_facet |
Mario Martone Gabi Zafrir |
author_sort |
Mario Martone |
title |
On the compactification of 5d theories to 4d |
title_short |
On the compactification of 5d theories to 4d |
title_full |
On the compactification of 5d theories to 4d |
title_fullStr |
On the compactification of 5d theories to 4d |
title_full_unstemmed |
On the compactification of 5d theories to 4d |
title_sort |
on the compactification of 5d theories to 4d |
publisher |
SpringerOpen |
series |
Journal of High Energy Physics |
issn |
1029-8479 |
publishDate |
2021-08-01 |
description |
Abstract We study general properties of the mapping between 5d and 4d superconformal field theories (SCFTs) under both twisted circle compactification and tuning of local relevant deformation and CB moduli. After elucidating in generality when a 5d SCFT reduces to a 4d one, we identify nearly all N $$ \mathcal{N} $$ = 1 5d SCFT parents of rank-2 4d N $$ \mathcal{N} $$ = 2 SCFTs. We then use this result to map out the mass deformation trajectories among the rank-2 theories in 4d. This can be done by first understanding the mass deformations of the 5d N $$ \mathcal{N} $$ = 1 SCFTs and then map them to 4d. The former task can be easily achieved by exploiting the fact that the 5d parent theories can be obtained as the strong coupling limit of Lagrangian theories, and the latter by understanding the behavior under compactification. Finally we identify a set of general criteria that 4d moduli spaces of vacua have to satisfy when the corresponding SCFTs are related by mass deformations and check that all our RG-flows satisfy them. Many of the mass deformations we find are not visible from the corresponding complex integrable systems. |
topic |
Conformal Field Theory Extended Supersymmetry Field Theories in Higher Dimensions |
url |
https://doi.org/10.1007/JHEP08(2021)017 |
work_keys_str_mv |
AT mariomartone onthecompactificationof5dtheoriesto4d AT gabizafrir onthecompactificationof5dtheoriesto4d |
_version_ |
1721215604284719104 |