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Grading restriction of finitely generated C2-cofinite weak joint modules

Statement

Let V be a C2-cofinite conformal vertex algebra of CFT type over C, and let k≥1. Let W have k left V-module actions whose component modes commute whenever their component indices differ. Suppose W is generated by finitely many vectors under all these component modes. No grading, local finiteness, or semisimplicity of the conformal operators is assumed. Then the commuting conformal operators Li(0) have an algebraic direct-sum decomposition into joint generalized-weight spaces

W=⨁λ∈CkW[λ],W[λ]={w:for every i, (Li(0)−λi)niw=0 for some ni≥1}.

Each joint space is finite dimensional. For some finite set R⊂Ck and some integer vector D∈Zk, every occurring weight belongs to R+D+Nk. In particular its real parts have coordinatewise lower bounds, and the total conformal operator ∑iLi(0) has finite-dimensional generalized-weight spaces and real parts bounded below. The module has a compatible Nk grading with finite-dimensional pieces. Any already specified Nk grading compatible with component mode degrees also has finite-dimensional pieces; the same is true of any specified N grading in which each component mode changes degree by its integer operator degree. Thus it belongs to the full generalized joint-module class used for dual fusion products, including modules that do not split into tensor factors. The assertions apply in particular to finitely generated admissible modules, with no assumption that their specified grading pieces were finite dimensional.

Facts & Assumptions

[F1]

Difference-one spanning and finite degree spans for cyclic weak modules proves, without a module grading or conformal local finiteness assumption, strict-index spanning for a cyclic weak module using a fixed finite positive-weight representative set A and a generator cutoff N. Its degree spans Hd(w) are finite dimensional and vanish below a fixed integer bound. It proves the explicit bound d≥ℓ(ℓ−1)/2−ℓ(N−1) for every normal string.

[F2]

Jacobi and residue calculus from the state-field locality axioms supplies the module mode identities and state weights. The conformal commutator is [Li(0),a(n)(j)]=δij(wt(a)−n−1)a(n)(j). To see the needed module derivative explicitly, use its iterate identity with b=1,m=−2: creation gives a(−2)1=Ta and the vacuum modes give (Ta)(n)M=−na(n−1)M; the conformal commutator then follows from its commutator identity.

[F3]

The component modes commute across components by hypothesis. The Li(0) are their conformal modes, so also commute. A joint generalized-weight space uses possibly nonzero nilpotent parts of all these operators.

[F4]

Admissible module for a vertex operator algebra defines an admissible single-component module by a nonnegative direct-sum grading compatible with integer mode degrees; it does not assume finite-dimensional grading pieces. The analogous multigrading here uses one degree coordinate for each component. Morphisms are not part of the assertions proved in this item.

Proof

Given: The C2-cofinite algebra, commuting component actions, and finite generating set.

1.1F1F3algebra

First take a module cyclic under all components, with generator w. For d∈Zk, define Hd as the span of all words of total component multidegree d applied to w. Component commutativity reorders every word into k consecutive component blocks. For each component choose its generator cutoff Ni≥1 on the finite representative set A. Each block may be reduced by [F1] on the cyclic module of that component generated by w: commute all other blocks to the left, apply the finite linear relation on w, then multiply those other blocks back. Cross-component commutation makes this operation preserve all other multidegrees. Applying this successively to the k blocks gives strict-index block strings with the same total multidegree. The coefficients and truncations may depend on the particular block word; only the final representative cutoff Ni is uniform, precisely as in [F1].

2.1F1F3step 1.1algebra

For each component the bound in [F1] bounds its normal-string length in terms of the actual integer di, independently of initial filtration. For each bounded length there are finitely many state choices and, with largest index less than Ni and fixed index sum, finitely many index choices. Products of these finite choices across the finitely many components give a finite spanning set for Hd. There are integer lower bounds Di such that Hd=0 if any di<Di. Furthermore W=∑dHd, initially an algebraic sum rather than a direct grading. Each Li(0) preserves Hd: its mode has multidegree zero, and left multiplication by it is a permissible additional mode in the definition of the same degree span. Thus every Hd is a finite-dimensional invariant space for all the conformal operators.

3.1F2F3step 2.1algebra

In particular T=H0 is finite dimensional, contains w, and is invariant under all Li(0). Commuting endomorphisms of a finite-dimensional complex vector space have a finite joint generalized-eigenspace decomposition: decompose for the first operator using its split minimal polynomial and pairwise coprime primary factors; every other commuting operator preserves each primary space, so repeat on each space for the remaining operators. Let R⊂Ck be the resulting finite joint spectral set, and write w=∑ρ∈Rwρ accordingly. Each projection is a polynomial in the commuting operators on T, so wρ∈H0. The commutator [F2] implies that a component word of multidegree d sends wρ into joint generalized weight ρ+d. This also puts it in Hd, because wρ is a finite linear combination of multidegree-zero words on w.

4.1step 2.1step 3.1algebra

Consequently Hd is spanned by its joint generalized-weight vectors at the finite weights in R+d, and W=∑dHd is spanned by joint generalized-weight vectors. Distinct joint weights are linearly independent: any proposed linear relation uses finitely many weights and finitely many vectors, and polynomial primary projections in the commuting operators isolate each weight on the finite-dimensional space spanned by their finite nilpotent orbits. This proves the asserted algebraic direct sum. At a fixed weight λ, only the finitely many multidegrees d=λ−ρ∈Zk, ρ∈R, can contribute. Hence W[λ] lies in the finite sum of those finite-dimensional Hd and is finite dimensional. Its support lies in R+D+Nk by step 2.1. These conclusions were derived from finite degree spans; they were not assumed in defining them.

5.1step 4.1algebra

For finitely many generators, form the finite direct sum of their cyclic joint submodules and map it onto W by addition. The preceding arguments give a finite joint spectral set, coordinate lower bounds, and finite joint spaces for that finite direct sum. Its kernel is stable under the conformal operators and decomposes into its joint components: for any vector of the kernel, finitely many polynomial primary projections isolate its finitely many joint components and remain in the kernel. The quotient therefore inherits the joint decomposition, finite joint-space dimensions, and support within the same finite union of shifted nonnegative lattices. Taking coordinatewise minima of the finitely many integer bounds gives one D and a finite set R as in the Statement.

6.1F2step 5.1construct

Within each of the finitely many distinct joint lattice cosets choose a representative α, and for each coordinate take the minimum integer shift mi among occurring weights α+n. These minima exist by the proved coordinatewise lower bounds. Put β=α+m; it need not itself occur. The sum of W[β+n] over those distinct cosets defines finite-dimensional pieces indexed by n∈Nk. Their direct sum is W, and [F2] gives exactly the component mode-degree rule. These auxiliary semisimple degree operators do not replace the original conformal operators. Finally at fixed total weight, or below a fixed upper bound on its real part, the finite-coset support and the coordinatewise lower bounds leave finitely many joint weights; all corresponding joint spaces are finite dimensional. The total conformal generalized-weight space is exactly their direct sum, since on each joint space the sum of the commuting nilpotent parts is nilpotent.

7.1F4step 1.1step 2.1step 5.1algebra∎

If a compatible grading is already specified, enlarge the finite generating set by all its finitely many graded components, obtaining finitely many homogeneous generators. For any such generator at multidegree m, the proof of steps 1.1–2.1 gives finite-dimensional operator-multidegree spans Hd with di≥Di. A fixed specified multigrading piece of degree n is spanned by terms with d=n−m, so is finite dimensional. For a single specified total grading, its degree-n piece is spanned by terms with ∑idi=n−m; the coordinate lower bounds leave finitely many such integer tuples, and each corresponding Hd is finite dimensional. Summing over the finite homogeneous generating set proves the assertion for the original pieces. This proves all remaining assertions without replacing a specified grading by an assumed conformal grading.

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