“…The relevant first principles are the properly formulated axioms of chiral conformal field theory. The situation is thus reminiscent of the one with the ordinary (semisimple) Verlinde formula, whose proof could be attacked only after those axioms had been formulated [22] (see also [23,24]) for rational conformal field theory. In the semisimple case, the structure constants are expressed through the defining data of the representation category, which is a modular tensor category, and thus through the matrices of the basic B and F operations of [22] as…”
ABSTRACT. We find a nonsemisimple fusion algebra F p associated with each (1, p) Virasoro model. We present a nonsemisimple generalization of the Verlinde formula which allows us to derive F p from modular transformations of characters.
“…The relevant first principles are the properly formulated axioms of chiral conformal field theory. The situation is thus reminiscent of the one with the ordinary (semisimple) Verlinde formula, whose proof could be attacked only after those axioms had been formulated [22] (see also [23,24]) for rational conformal field theory. In the semisimple case, the structure constants are expressed through the defining data of the representation category, which is a modular tensor category, and thus through the matrices of the basic B and F operations of [22] as…”
ABSTRACT. We find a nonsemisimple fusion algebra F p associated with each (1, p) Virasoro model. We present a nonsemisimple generalization of the Verlinde formula which allows us to derive F p from modular transformations of characters.
“…There is a canonical Lie algebra U ′ (V ) which can be attached to a vertex algebra V , see [FBZ,Section 4.1]. U ′ (V ) is generated from the expansion coefficients A n introduced in (2.4).…”
Section: Vertex Algebrasmentioning
confidence: 99%
“…Representations M of the vertex algebra V must in particular be representations of the Lie-algebra U ′ (V ) generated from the coefficients A n , see [FBZ,Section 5] for more details.…”
Section: Representations Of Vertex Algebrasmentioning
confidence: 99%
“…, z n , respectively. It can then be shown that the spaces F (X, R) and F (X ′ , R ′ ) are canonically isomorphic [FBZ,Theorem 10.3.1]. The isomorphism is defined by demanding that…”
Section: Insertions Of the Vacuum Representationmentioning
“…These series are also called fields. They play a crucial role in the theory of vertex operator algebras (see [15,22,3]). We will need the field which corresponds to the highest root θ of g. Namely, let e θ ∈ g be a highest weight vector in the adjoint representation.…”
Abstract. Let L be the basic (level one vacuum) representation of the affine Kac-Moody Lie algebra g. The m-th space F m of the PBW filtration on L is a linear span of vectors of the form x 1 · · · x l v 0 , where l ≤ m, x i ∈ g and v 0 is a highest weight vector of L. In this paper we give two descriptions of the associated graded space L gr with respect to the PBW filtration. The "top-down" description deals with a structure of L gr as a representation of the abelianized algebra of generating operators. We prove that the ideal of relations is generated by the coefficients of the squared field e θ (z) 2 , which corresponds to the longest root θ. The "bottom-up" description deals with the structure of L gr as a representation of the current algebra g ⊗ C[t]. We prove that each quotient F m /F m−1 can be filtered by graded deformations of the tensor products of m copies of g.
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