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Finite mode windows for a nonnegative C2-cofinite VOA

Statement

Let V be a vertex operator algebra with finite-dimensional nonnegative integral state grades, vacuum, translation and conformal Jacobi axioms, and suppose V/C2(V) is finite dimensional. The space V0 is allowed to be larger than C1. Choose a finite homogeneous set A, together with the vacuum, representing V/C2(V), including its nonvacuum weight-zero representatives. If a weak module is generated by w and amw=0 for a in A and m≥N, it is spanned, in every total operator degree d, by a1(i1)...al(il)w,i1<...<il<N, and these strings satisfy d≥l(l−1)/2−Nl. Hence every degree span is finite dimensional and vanishes for sufficiently negative d; no L0 grading of the weak module is assumed.

For every N≥0, the vector quotient V/ON(V), with the usual higher-circle and T+L0 relations, is finite dimensional. The common zero-mode operators on ΩN of all weak modules form a finite-dimensional unital associative algebra ZN; every ΩN is a module for ZN and o(omega)=L0. This image algebra suffices here; no identification with a higher-Zhu bimodule or reverse rationality criterion is asserted.

Facts & Assumptions

Given: Work over C in the non-super state-field convention. In this item the broader phrase “vertex operator algebra” means a complex vertex algebra with vacuum 1∈V0 and conformal vector ω∈V2, with modes Y(ω,z)=∑j∈ZL(j)z−j−2, central charge c∈C, and L(−1)=T, where [L(m),L(n)]=(m−n)L(m+n)+c12(m3−m)δm+n,0id⁡V for all m,n∈Z, and for which L(0) is diagonalizable and V=⨁r≥0Vr with each Vr finite dimensional. No assumption V0=C1 is made. Each weak module has the lower-truncated fields, vacuum, and full module Jacobi identity specified below, with no grading assumed.

[F1]

Vertex algebra in the state–field convention defines the state-field data (V,1,T,Y) by truncation, vacuum/creation, translation covariance, and locality. The conformal-vector data above adds the Virasoro action and the grading; for homogeneous a∈Vr, wt(a)=r.

[F2]

Module for an ordinary vertex algebra gives the weak-module Jacobi identity. Its coefficient residues give, with generalized binomial coefficients for every integer m, [a(m)M,b(n)M]=∑j≥0(mj)(a(j)b)(m+n−j)M,(a(m)b)(n)M=∑t≥0(−1)t(mt)(a(m−t)Mb(n+t)M−(−1)mb(m+n−t)Ma(t)M). The commutator sum is finite by state truncation; each iterate sum is finite on a fixed vector by rightmost-mode truncation. Translation gives (Tja)(m)M=(−1)jm(m−1)⋯(m−j+1)a(m−j)M, and conformal weight covariance gives wt(a(m)b)=wt(a)+wt(b)−m−1 whenever the product is nonzero.

[F3]

C2-cofiniteness defines C2(V)=span⁡C{a(−2)b:a,b∈V}; the hypothesis in the Statement is that the vector quotient V/C2(V) is finite dimensional.

[F4]

Higher Zhu action on the Omega spaces of an arbitrary weak module proves the preservation, ON(V)-annihilation, and o(a∗Nb)=o(a)o(b) identities in precisely this full nonnegative-grade scope for arbitrary weak modules. Its exact formulas are, for homogeneous a∈Vr, a∘Nb=∑j=0r+N(r+Nj)a(j−2N−2)b,a∗Nb=∑p=0N(−1)p(N+pN)∑j=0r+N(r+Nj)a(j−N−p−1)b, Da=(T+L(0))a=Ta+ra,ON(V)=span⁡C{a∘Nb,  Da:a,b∈V}. These are the “higher-circle” and T+L(0) relations used in Step 5.1; no CFT-type or associative-quotient assertion is imported for this broader case.

Proof

1.1givenF2F3algebra

Fix the total operator degree d, and induct on total state weight p≥0, then on word length l. Replacing a homogeneous state by a representative plus C2-products lowers p in every iterate term, since wt⁡(a−2b)=wt⁡(a)+wt⁡(b)+1 while the two replacement states have total wt(a)+wt(b). The replacement is finite on its fixed tail by the mode truncations in F1 and F2. A vacuum mode either vanishes or removes a letter, lowering length. Nonvacuum weight-zero representatives remain in A; they are NOT silently discarded. At p=0 there are no C2 replacement terms, since those would have positive weight, and the same length and tuple induction below applies.

2.1F2step 1.1algebra

Sort adjacent indices by the commutator. Each commutator state has smaller total state weight by j+1, so the error is already reduced by the p induction. After sorting, a last index ≥N kills the cyclic vector. For fixed p,l,d the surviving sorted tuples have fixed sum p-l-d and every index ≤N−1, hence every index is also at least p-l-d-(l-1)(N-1). There are only finitely many tuples, with a finite lexicographic order.

3.1F2step 1.1step 2.1algebra

At a repeated adjacent index i use (a−1b)(2i+1)=∑t≥0(a(−1−t)b(2i+1+t)+b(2i−t)at). For i<0 the first sum contains exactly one desired repeated pair at t=−i−1; for i≥0 the second contains exactly one reversed pair at t=i. Commute that reversed pair, whose error has smaller p. Every other pair has unequal indices summing to 2i, so after sorting it has a smaller first index and a lexicographically smaller full tuple, or dies by the N cutoff. The collapsed state a−1b has the same p and shorter word length. Its C2 replacement lowers p as before. Induction on this finite tuple set, after the outer p and length inductions, therefore removes all equal indices with coefficient ONE. The argument applies at p=0 as well: commutator states of negative weight are zero, and the collapsed weight-zero representative is handled by shorter length.

4.1step 2.1step 3.1algebra

These reductions cover every finite p and l, not a fixed truncated filtration only. In a resulting strict word, ij≤N−1−(l−j), while wt⁡(aj)≥0. Consequently d=∑j(wt⁡(aj)−ij−1)≥l(l−1)/2−Nl. This quadratic is bounded below and tends to positive infinity. At fixed d it bounds l. For each such l there are finitely many states and their fixed total weight fixes the index sum; step 2.1 bounds all indices. Hence the full unbounded-filtration degree span is finite dimensional and is zero below the quadratic minimum.

5.1F3F4step 4.1algebra

For k≥2 let Ck(V)=span⁡{a−kb}. Apply the spanning result to V generated by its vacuum. Nonnegative modes kill the vacuum, so all surviving indices are negative. A word whose smallest index is -m with m≥k belongs to Ck, because (T(m−k)a)(−k)=k(k+1)...(m−1)a(−m). Otherwise all distinct indices lie in the finite interval -k+1,...,-1; finitely many such words remain. Thus Ck(V) is homogeneous, has finite codimension in V, and contains all sufficiently high state-weight spaces. Modulo ON(V), the circle identity reduces a(−2N−2)b to −∑j≥1binom⁡(wt⁡(a)+N,j)a(j−2N−2)b. Each term has smaller state weight. Induction on nonnegative state weight therefore reduces V/ON to finitely many low grades. This proves its finite dimension, including nonvacuum weight-zero states. No ideal property of ON is used.

6.1F4step 5.1algebra∎

Let F be the free complex vector space on the set ⋃ℓ≥0(V×Z)ℓ of finite mode words, including the empty word, and let Pa,m prepend the letter (a,m). Let K consist of all subspaces K⊆F stable under every Pa,m for which the induced operators on F/K are linear in a and satisfy the weak-module axioms. This is a set, as a subset of the power set of F; it involves no basis or isomorphism-representative choices. For every cyclic weak module generated by w, evaluation of a word on w gives a surjection F→Vw intertwining all prepend operators. Its kernel belongs to K, and the induced isomorphism identifies Vw with that quotient. For fixed N≥0, map a∈V to the family of its zero-mode operators in ∏K∈KEnd⁡C(ΩN(F/K)). By [F4] these operators preserve the indicated spaces, kill ON(V), take the vacuum to the identity family, and multiply according to a∗Nb. The image ZN is therefore an associative unital algebra of dimension at most dim⁡V/ON(V), hence finite. Every w∈ΩN(M) belongs to its cyclic weak submodule, and w∈ΩN(Vw), so this family detects exactly the state zero-mode identities on all weak ΩN spaces. Thus the action on every ΩN(M) factors through ZN. In particular a polynomial annihilating o(ω) in this finite-dimensional algebra annihilates LM(0) on every weak ΩN(M), uniformly in M.

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