Alphabeta Math
TheoremStatement: Literature-sourcedProof: AI-adaptedPipeline-generatedprecheck passverified 2026-11-05 (gpt-6.1-sol)
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.

  • Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.

These labels describe origin, not correctness: citations and verification chips remain separate evidence.

The restricted dual with opposite action is a contragredient module

Statement

For every grading-restricted generalized module M over a conformal vertex algebra V of CFT type, the restricted dual action defined by the opposite field forms a grading-restricted generalized V-module M′. The componentwise evaluation M→M′′ is a V-module isomorphism.

Facts & Assumptions

Given: Work over C with the formal-variable, grading, and branch conventions in the linked definitions.

[F1]

Contragredient module of a generalized module: For a grading-restricted generalized module M over a conformal vertex algebra V, its contragredient candidate is M′=⊕h∈CM[h]∗, with action defined by ⟨YM′(v,x)w′,w⟩=⟨w′,YMo(v,x)w⟩, where YMo(v,x)=YM(exL(1)(−x−2)L(0)v,x−1). On homogeneous integer-weight vectors, (−x−2)L(0) contributes (−1)wt(v)x−2wt(v). Whether this formula satisfies all module axioms and gives M''≅M is a separate theorem; this definition alone does not assert it. V is self-contragredient when V≅V' as V-modules.

[F2]

Conformal vertex algebra of CFT type: A conformal vertex algebra of CFT type is a complex vertex algebra V in the sense of def-vertex-algebra-state-field, with a specified vector ω∈V and scalar c∈C, such that, writing Y(ω,z)=∑n∈ZL(n)z−n−2, the operators L(n) and scalar central action c satisfy the Virasoro relations of def-virasoro-algebra, and L(−1)=T. In addition, L(0) is diagonalizable, Vn:={v∈V:L(0)v=nv} gives V=⨁n≥0Vn, every Vn is finite dimensional, and V0=C1. Under this page's convention, this is a vertex operator algebra of CFT type. The grading and the CFT-type condition are part of the definition; they do not follow from the vertex-algebra axioms alone. The conformal weight of v∈Vn is n. A conformal vector, a grading, and the nonnegative grading condition are additional data beyond an ordinary vertex algebra.

[F3]

Grading-restricted generalized module: Let V be a conformal vertex algebra of CFT type and M a left V-module. Write LM(0) for the coefficient determined by YM(ω,z)=∑n∈ZLM(n)z−n−2. For h∈C, define the generalized LM(0)-eigenspace M[h]={m∈M:(LM(0)−h)Nm=0 for some integer N≥1}. The module is grading-restricted generalized if M=⨁h∈CM[h], every M[h] is finite dimensional, and the real parts of its nonzero generalized weights are bounded below. The direct sum means each vector has only finitely many generalized-weight components. This convention explicitly adds finite-dimensionality and a lower bound to the generalized-eigenspace decomposition; those conditions are not consequences of the module Jacobi identity.

[F4]

Module for an ordinary vertex algebra: Let V be a vertex algebra over C in the ordinary, non-super convention of def-vertex-algebra-state-field. A left V-module is a complex vector space M and a linear map YM(−,z):V⟶{formal fields on M},a⟼YM(a,z)=∑n∈Za(n)Mz−n−1, with the following properties: 1. Lower truncation. For every a∈V and m∈M, a(n)Mm=0 for all sufficiently large integers n, so YM(a,z)m∈M((z)) in the support convention of def-formal-distribution-on-a-vector-space. 2. Vacuum. YM(1,z)=id⁡M. 3. Module Jacobi identity. For every a,b∈V, z0−1δ ⁣(z1−z2z0)YM(a,z1)YM(b,z2)−z0−1δ ⁣(z2−z1−z0)YM(b,z2)YM(a,z1)=z2−1δ ⁣(z1−z0z2)YM(Y(a,z0)b,z2). Here δ(x)=∑r∈Zxr; the first expansion is in nonnegative powers of z2, the second in nonnegative powers of z1, and the right-hand expansion is in nonnegative powers of z0. They use the formal binomial conventions of def-formal-distribution-on-a-vector-space. The Y inside the right-hand side is the state-field map of V; it is not the action map YM. A V-module homomorphism f:M→N is a linear map such that fYM(a,z)=YN(a,z)f for every a∈V. This definition does not impose a conformal grading, finite-dimensional weight spaces, semisimplicity of L0, a right-module convention, or a twist by an automorphism. For a conformal vertex algebra, write YM(ω,z)=∑n∈ZLM(n)z−n−2 when a conformal vector ω is specified. A V-submodule of M is a linear subspace stable under every mode a(n)M. A module is simple (or irreducible) if it is nonzero and has no proper nonzero V-submodule. A module is completely reducible (or semisimple) if it is an internal direct sum of simple V-submodules; the empty direct sum is the zero module.

[F5]

Opposite fields under formal coordinate inversion proves opposite Jacobi, translation, the three opposite Möbius brackets, the explicit opposite modes and their generalized-weight shifts, and A(x−1)A(x)=1.

Proof

1.1givenF3F5algebra

For v∈Vd the opposite mode vno maps M[h] into M[h+n+1−d]. Thus its transpose sends M[k]∗ into M[k+d−n−1]∗. If Re(h)≥B for all weights of M, the latter space vanishes when Re(k)+d−n−1<B. A restricted-dual vector has finite weight support, so one bound works for that vector. This proves both preservation of M′ by every mode and lower truncation of its field. This bound comes from the lower weight bound on M, rather than from upper truncation of the opposite field on a fixed vector of M.

2.1givenF1F2F4F5step 1.1algebra

Pair each candidate module identity against w∈M. Vacuum follows from opposite vacuum. Transposition reverses the two products in opposite Jacobi, giving exactly the ordinary module Jacobi identity in F4; every matrix coefficient and delta expansion is legitimate by step 1.1 and F5. The derivative identity transposes directly. Since A(x)ω=x−4ω, one has ⟨LM′(j)w′,w⟩=⟨w′,LM(−j)w⟩. The Virasoro bracket is preserved: transposing reverses a commutator and reverses its two indices, so the central term remains c(j3−j)δj+k,0/12. The opposite Möbius brackets likewise transpose to the ordinary module brackets. Hence this is a conformal generalized module.

3.1F3step 2.1algebra

On M[h]∗ the operator LM′(0) is the transpose of LM(0), so its only generalized eigenvalue is h. Distinct generalized eigenspaces remain distinct, and the restricted direct sum is exactly their decomposition. Their dimensions and their common lower real weight bound are the same as for M. Thus M′ is grading restricted.

4.1F1F3F5step 3.1algebra∎

Evaluation identifies M[h] with M[h]∗∗ because each is finite dimensional. Pair the action on its double dual against w′∈M′: twice applying the defining transpose gives the original action with state A(x−1)A(x)v=v. Thus evaluation commutes coefficientwise with every YM(v,x). The direct sum of the finite-dimensional evaluation isomorphisms is therefore a V-module isomorphism M≅M′′.

Depends on

Dependency tree · 2 levels

Sources