How statement and proof provenance work
The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.
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These labels describe origin, not correctness: citations and verification chips remain separate evidence.
Zhu quotient algebra and admissible top-level action
Statement
Let be a conformal vertex algebra of CFT type in the state–field convention. For homogeneous , define , , and . Extend and uniquely to bilinear maps over finite homogeneous decompositions. Then is a two-sided ideal for , the product descends to an associative unital product on with unit , and every admissible module has an -module structure on given on homogeneous by . No finite-dimensionality of or is asserted.
Statement references
Facts & Assumptions
Given: V and the admissible module M in the unchanged Statement. All congruences below mean additive difference in the vector subspace O(V); no product on V/O(V) is assumed before ideal stability is proved.
Zhu algebra of a CFT-type vertex operator algebra supplies the finite circle/star mode sums and the vector-space quotient V/O(V).
Conformal vertex algebra of CFT type supplies the conformal grading and .
Admissible module for a vertex operator algebra gives for , with negative grades zero.
Module for an ordinary vertex algebra supplies vacuum and module Jacobi.
The actual Jacobi and residue calculus from the state-field locality axioms public interface states regular-module Jacobi for the fields on V, , the state-product weight rule , and the displayed coefficientwise iterate/residue identities on V and every left V-module. The CFT-type hypotheses here are precisely those of that interface.
Zhu zero-mode identities on singular vectors of an arbitrary module proves coefficientwise that zero modes preserve , annihilate O(V) there, and obey there. It assumes neither an admissible grading nor finiteness or semisimplicity of M.
Proof
For homogeneous set , . We prove each lies in O(V). The case is its defining generator. Integration by parts with F5 gives : differentiate and expand its extra factor 1+z. Thus if all lie in O(V), the same is true at m+1, since m+2 is invertible in C and Ta has weight r+1 when nonzero. Induction gives the assertion for every m. Finally by expanding , and . This proves the full higher-residue relation with no ideal property assumed.
For homogeneous , put , a linear operator on V. Creation gives for every homogeneous a and hence . The derivative property and integration by parts give for , so exactly. We also have the exact derivation identity . To verify it rather than assume it, expand . The L(0)-weight of its ith term is r+s-i, while translation of the same sum is . The elementary identity makes the remaining weight sum cancel that last residue and gives the asserted derivation formula; for the cancellation reads . Finally vacuum and creation give and exactly, since only their constant power-series coefficients contribute to the star residue.
Let and c be homogeneous. Weight bookkeeping in F5 and the finite star sum give Apply F5's residue identity with and . Its first product expands ; the term is . The reversed expansion is , and the minus in the residue identity therefore makes its contribution positive. Define and . Exact coefficient extraction yields These sums are finite: and vanish for large j by truncation. Each summand lies in O(V) by step 1.1, even when are not homogeneous. Hence the associator is in O(V). Bilinearity extends this additive congruence to all inputs.
Right ideal stability follows first, without multiplying an unproved congruence: , where the only congruence is the associator from step 2.1 applied to the actual inputs Da,b,c. Thus . Next the exact derivation relation in step 1.2 gives . Applying step 2.1 to c,Da,b yields , which is in O(V) by the right ideal stability just proved. Thus too. Linearity across circle generators proves both ideal assertions in the Statement. This order of proof avoids assuming either ideal assertion in order to prove the other.
Step 3.1 makes the product on V/O(V) well-defined on both representatives. The associator relation of step 2.1 descends to associativity, and step 1.2 gives its two-sided unit . These conclusions use only finite formal residue identities, not a citation to the algebra-structure theorem.
For and , F3 implies whenever , since its target grade is negative. Hence . F3 also gives . F6 now supplies and , by its explicit circle/star iterate coefficient cancellations. Its vacuum identity makes the action unital. Thus is the stated well-defined representation of the associative algebra from step 4.1. No dimension bound or semisimplicity condition is used.
Depends on
Jacobi and residue calculus from the state-field locality axioms
Zhu zero-mode identities on singular vectors of an arbitrary module
Zhu algebra of a CFT-type vertex operator algebra
Conformal vertex algebra of CFT type
Vertex algebra in the state–field convention
Admissible module for a vertex operator algebra
Module for an ordinary vertex algebra