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DefinitionDefinition: Literature-sourcedProof: Not applicablePipeline-generatedverified 2026-11-05 (gpt-6.1-sol)
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VOA conformal block and dual fusion product

Definition

Let V be a conformal vertex algebra of CFT type over C, with state-field map Y(v,z)=∑n∈Zv(n)z−n−1, conformal vector, and Virasoro operators as in the supplied definitions. Let (C;p1,…,pN;z1,…,zN) be a pointed compact analytic worldsheet, and let Wi be grading-restricted generalized left V-modules at the marked points. Here each Wi is the algebraic direct sum of its finite-dimensional generalized L(0)-eigenspaces, with the real parts of its weights bounded below; set W=W1⊗C⋯⊗CWN.

For clarity, a grading-restricted generalized V⊗k-module in this page means a vector space with commuting component actions Yi(v,z) of V, with the actions for distinct i commuting, and commuting grading operators Li(0). It has a joint generalized-weight decomposition M=⨁λ∈CkM[λ]; each joint generalized-weight space is finite dimensional, each vector has finite support in the direct sum, and the real parts of the weights are bounded below in each coordinate. The component fields use the state-field convention fixed above.

For a coordinate chart η:U→C on C, the sheaf of VOA states is locally V⊗COU. On an overlap of charts η,μ, glue these trivializations by the formal-coordinate operator U(ρη∣μ), where

ρη∣μ,p(t)=η ⁣(μ−1(t+μ(p)))−η(p).

The composition identity in that supplier is the cocycle condition for these transition maps. Write ωC for the holomorphic cotangent line bundle, whose local sections are f(z) dz and whose coordinate changes use the chain rule. Write ωC(∗P)=⋃k≥0ωC(k∑ipi) for meromorphic one-forms with poles of finite order only at the marked points.

A global section σ of VC⊗ωC(∗P) acts on W by the sum of its residue actions. In the coordinate zi at pi, write its state-valued differential as ∑kvi,kzik dzi; its ith action on w1⊗⋯⊗wN is

∑kw1⊗⋯⊗(vi,k)(k)wi⊗⋯⊗wN,

and the global action is the sum over i. The coinvariant space is the quotient of W by the linear span of all such global actions. The space of conformal blocks is the algebraic dual of this quotient, equivalently the set of linear functionals on W that vanish on every global residue action. For an analytic family, use the same construction fiberwise with the relative cotangent line bundle and the sheaf of VOA states on the total family.

For an (M,N)-pointed surface X with N incoming points, M outgoing points, and a grading-restricted generalized V⊗N-module W at the incoming points, a dual fusion product is a grading-restricted generalized V⊗M-module DX(W) together with a conformal block γX∈CBX(W⊗DX(W)) such that, for every grading-restricted generalized V⊗M-module M0 and every Γ∈CBX(W⊗M0), there is a unique V⊗M-module homomorphism T:M0→DX(W) satisfying Γ=γX∘(idW⊗T). This is a definition of the representing property when such an object exists; existence is a separate theorem.

Remarks

The source's conformal-block spaces depend on the analytic coordinate convention through the formal-coordinate action above. The universal property does not assert that DX(W) exists; it also does not assert finite-dimensionality or semisimplicity. The separate existence item records the C2-cofinite case. The local finite-weight state-sheaf cocycle is supplied by Formal coordinate-change action of a conformal vertex algebra. The formal field identity, finite-pole residue action, coordinate covariance and compatibility with arbitrary module maps are supplied by Formal field and residue covariance for generalized VOA modules. The marked local coordinates are part of the data here; the family construction uses its specified vertical coordinates. The supplier distinguishes its branch-free integral normalization from the conformal LM(0) dilation, so it makes no substitution of the normalized generator in later Ward identities or geometric connections. Outgoing factors use the stated left-module and contragredient conventions; no additional sign is inserted in the sum of local residues.

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