2019
DOI: 10.1007/jhep01(2019)160
|View full text |Cite
|
Sign up to set email alerts
|

Vertex algebras at the corner

Abstract: We introduce a class of Vertex Operator Algebras which arise at junctions of supersymmetric interfaces in N = 4 Super Yang Mills gauge theory. These vertex algebras satisfy non-trivial duality relations inherited from S-duality of the four-dimensional gauge theory. The gauge theory construction equips the vertex algebras with collections of modules labelled by supersymmetric interface line defects. We discuss in detail the simplest class of algebras Y L,M,N , which generalizes W N algebras. We uncover tantaliz… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

10
327
0

Year Published

2019
2019
2022
2022

Publication Types

Select...
9

Relationship

4
5

Authors

Journals

citations
Cited by 127 publications
(337 citation statements)
references
References 49 publications
10
327
0
Order By: Relevance
“…N for 3d hypermultiplet so that it is compatible with the H-twist (mirror Rozansky-Witten twist). The resulting deformed boundary condition supports the VOA Sb of symplectic bosons X(z) and Y (z) of conformal dimension 1 2 which obey the OPE [39,36]…”
Section: D Matter Multipletssupporting
confidence: 55%
“…N for 3d hypermultiplet so that it is compatible with the H-twist (mirror Rozansky-Witten twist). The resulting deformed boundary condition supports the VOA Sb of symplectic bosons X(z) and Y (z) of conformal dimension 1 2 which obey the OPE [39,36]…”
Section: D Matter Multipletssupporting
confidence: 55%
“…There are various intertwined relations between supersymmetric gauge theories and Vertex Operator Algebras [1][2][3][4][5][6][7][8][9][10][11]. In many of these constructions the VOA emerges as the local operator algebra of some QFT which is topological away from some special two-dimensional location or defect and holomorphic at the defect.…”
Section: Contentsmentioning
confidence: 99%
“…There is a nice combinatorial description of the truncation in terms of plane partitions (box-counting) which is discussed in [72,73]. The free field representation of Y N 1 ,N 2 ,N 3 was constructed in [67].…”
Section: Other Triality Framesmentioning
confidence: 99%