2017
DOI: 10.48550/arxiv.1711.05343
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On Infinite Order Simple Current Extensions of Vertex Operator Algebras

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Cited by 3 publications
(4 citation statements)
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“…The up-shot of correctness of these Conjectures is the knowledge of the complete vertex tensor category of finite-dimensional weight modules of the singlet VOA and especially this is a rigid and braided tensor category so that all the results of [56] apply. We also would like to mention that the subtleties of passing to a completion of the category due to infinite order simple current extensions are discussed in both [46,62].…”
Section: The Singlet M(p)mentioning
confidence: 99%
“…The up-shot of correctness of these Conjectures is the knowledge of the complete vertex tensor category of finite-dimensional weight modules of the singlet VOA and especially this is a rigid and braided tensor category so that all the results of [56] apply. We also would like to mention that the subtleties of passing to a completion of the category due to infinite order simple current extensions are discussed in both [46,62].…”
Section: The Singlet M(p)mentioning
confidence: 99%
“…Simple Current Extensions. The process of extending a vertex operator algebra by (tensor powers of) modules whose tensor product is invertible (such extentions are called simple current extentions) has a long history in the conformal field theory and vertex operator algebra literature for both finite order extensions [42] and more recently also infinite ones [33,43]. At a categorical level, extensions (not necessarily the simple current type) correspond to algebra objects in a braided monoidal category [31,44,45].…”
Section: Examplementioning
confidence: 99%
“…43) Here Y( )Y( ) and Y(Y( )) denote the obvious product and iterate of intertwining operators and we have suppressed the objects labelling the natural transformations ϕ 2 , α C , α D . The left triangle commutes by the definition (see Theorem 2.12) of associativity for intertwining operators.…”
mentioning
confidence: 99%
“…As L − 3 2 (sl 3 ) is a simple current extension in this direct limit completion [CMY20a,AR18], it now follows from [CKL20a, CKM17] that D is the category of local modules for L − 3 2 (sl 3 ), viewed as a commutative algebra object in the direct limit completion. There is therefore an induction functor that maps any module V in the completion that centralises the algebra object L − 3 2 (sl 3 ) to an object Ind V in D. Moreover, this functor is a vertex tensor functor [CKM17], meaning that it respects the fusion products of the completion and D:…”
Section: Reconstructingmentioning
confidence: 99%