2018
DOI: 10.1007/jhep01(2018)085
|View full text |Cite
|
Sign up to set email alerts
|

’t Hooft anomalies and boundaries

Abstract: We argue that there is an obstruction to placing theories with 't Hooft anomalies on manifolds with a boundary, unless the symmetry associated with the anomaly can be represented as a non-invariance under an Abelian transformation. For a two dimensional conformal field theory we further demonstrate that all anomalies except the usual trace anomaly are incompatible on a manifold with a boundary. Our findings extend a known result whereby, under mild assumptions, Lagrangian theories with chiral matter cannot be … Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

2
37
0

Year Published

2018
2018
2023
2023

Publication Types

Select...
7

Relationship

0
7

Authors

Journals

citations
Cited by 31 publications
(39 citation statements)
references
References 45 publications
2
37
0
Order By: Relevance
“…It has important applications in quantum field theory, string theory and condensed matter physics. For interesting developments of BCFT and related topics please see [3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19]. In the spirit of AdS/CFT [20], Takayanagi [21] proposes to extend the d dimensional manifold M to a d + 1 dimensional asymptotically AdS space N so that ∂N = M ∪ Q, where Q is a d dimensional manifold which satisfies ∂Q = ∂M = P .…”
Section: Introductionmentioning
confidence: 99%
“…It has important applications in quantum field theory, string theory and condensed matter physics. For interesting developments of BCFT and related topics please see [3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19]. In the spirit of AdS/CFT [20], Takayanagi [21] proposes to extend the d dimensional manifold M to a d + 1 dimensional asymptotically AdS space N so that ∂N = M ∪ Q, where Q is a d dimensional manifold which satisfies ∂Q = ∂M = P .…”
Section: Introductionmentioning
confidence: 99%
“…In addition to traditional field theory techniques, see, e.g. [48][49][50][51][52][53][54][55], the need of a non-perturbative approach using symmetries or dualities is evident. A non-perturbative holographic dual description to BCFT was initiated by Takayanagi in [56] and later developed for general shape of boundary geometry in [57,58].…”
Section: Introductionmentioning
confidence: 99%
“…In addition to traditional field theory techniques, see, e.g. [63,65,[69][70][71][72][73][74], the need of a non-perturbative approach using symmetries or dualities is evident. A non-perturbative holographic dual description to BCFT was initiated by Takayanagi in [54] and later developed for general shape of boundary geometry in [55,56].…”
Section: Holographic Boundary Conformal Field Theorymentioning
confidence: 99%