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LemmaStatement: AI-adaptedProof: AI-generatedPipeline-generatedprecheck passverified 2026-11-05 (gpt-6.1-sol)
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Strong generators generate the lowest space of a cyclic module

Physical scope

Pure mathematics; no physical premises or physical claim.

Statement

Let V=⨁d≥0Vd be a conformal vertex algebra with V0=C1, strongly generated by homogeneous positive-weight states S, meaning V=span⁡{s(−k1)1⋯s(−kℓ)ℓ1:ℓ≥0, si∈S, ki≥1}, where the ℓ=0 word is 1. Let M=⨁r≥0M(r) be an admissible V-module, so a homogeneous a∈Vd satisfies a(m)M(r)⊂M(r+d−m−1). If M is cyclic on u∈M(0), meaning M=span⁡{a(m1)1⋯a(mk)ku:k≥0, ai∈V, mi∈Z}, where the k=0 word is u, then M(0)=span⁡{o(s1)⋯o(sk)u:k≥0, si∈S},o(a)=a(wt⁡a−1). Moreover, for each homogeneous state a, a noncommutative polynomial in the generator zero modes, depending only on a and a fixed strong spanning expression for it, equals o(a) on the lowest space of every admissible module. Thus the same generator zero-mode matrices determine the same full lowest-space zero-mode action. The statement does not require semisimple L(0), irreducibility, C2-cofiniteness, the existence of a universal induced module, or the general Zhu correspondence.

Facts & Assumptions

Given: The objects, hypotheses and conventions in the Statement.

[A1]

The CFT-type grading, nonnegative admissible module grading, strong generating set S, and cyclic vector u are precisely the hypotheses of the Statement.

[F1]

Conformal vertex algebra of CFT type gives the nonnegative integer state weights and vacuum line.

[F2]

Module for an ordinary vertex algebra supplies the full module Jacobi identity; taking its formal coefficients gives the commutator and iterate identities displayed in the proof.

[F3]

Admissible module for a vertex operator algebra specifies the degree shift and the vanishing of negative module degrees. Strong generation here means that V is spanned by finite words of strictly negative modes of states in S applied to 1.

[A2]

Jacobi and residue calculus from the state-field locality axioms proves the homogeneous state-product weight rule and the module commutator and iterate coefficient identities used below. Its complete current proof supplies exactly these formal identities.

Proof

1.1givenA2F1algebra

Give a mode a(m) of homogeneous a degree wt⁡(a)−m−1. The commutator identity in [A2] and its state-product weight rule show every term in [a(m),b(n)] has degree wt⁡(a)−m−1+wt⁡(b)−n−1. The sum is finite by state truncation. Thus mode commutators preserve total degree.

1.2A2algebra

Let a,b be homogeneous of weights d,e, with d≥1, and define the inhomogeneous states Ck(a,b)=∑i=0d(di)a(i−k)b for k≥1. Extend o linearly over homogeneous components. For the summand indexed by i, put n=i−k and m=d+e−n−2, the zero-mode index of a(n)b. The iterate identity in [A2] gives (a(n)b)(m)=∑j≥0(−1)j(nj)(a(n−j)b(m+j)−(−1)nb(m+n−j)a(j)). The first term has rightmost mode b(m+j) of degree n−d+1−j=i−k−d+1−j.

2.1givenA1F3step 1.1algebra

Reorder a finite word of modes so positive-degree modes lie left, zero-degree modes middle, and negative-degree modes right. Swap any adjacent factors in the wrong order using AB=BA+[A,B]: the swapped word has one fewer inversion, and every commutator term has shorter length. Induction on length and then inversion count terminates. On applying the reordered word to u∈M(0), a rightmost negative-degree mode kills u by admissibility. A word containing only nonnegative modes and at least one positive-degree mode has positive total degree. Since M is cyclic on u, its degree-zero space is therefore spanned by words in o(a)=a(wt⁡(a)−1), a∈V, applied to u.

2.2givenF2F3A2step 1.2algebra

Because i≤d, this first term kills M(0) for every k≥2. For k=1 it can survive only at i=d,j=0, when it is exactly o(a)o(b). In the second term a(j) kills M(0) for j≥d. For each fixed 0≤j<d, the mode b(m+n−j)=b(d+e−2−j) is independent of i. Its coefficient after summing over i is, up to the fixed sign (−1)j−k+1, ∑i=0d(−1)i(di)(i−kj)=0. Indeed i↦(i−kj) is a polynomial of degree j<d, so its dth finite difference vanishes; this remains true for negative upper entries by the polynomial definition of the binomial coefficient. Module truncation makes the original iterate sums finite on each vector. Therefore o(C1(a,b))=o(a)o(b) and o(Ck(a,b))=0 for k≥2 on M(0).

3.1givenA1F1F3A2step 2.1step 2.2algebra∎

Induct on state weight to express every o(v) on M(0) as a noncommutative polynomial in o(S). Weight zero gives the identity. A strong spanning monomial of positive weight is s(−k)b with s∈S, k≥1, and b a shorter strong monomial. For k=1, expand C1(s,b): its first term is s(−1)b, while every other term s(i−1)b has weight wt⁡(s)+wt⁡(b)−i, strictly below the target weight; also b has lower weight because wt⁡(s)≥1. The identity in step 2.2 expresses its zero mode using o(s)o(b) and those lower-weight zero modes. For k≥2, expand Ck(s,b); its first term is s(−k)b, and each remaining term s(i−k)b has weight wt⁡(s)+wt⁡(b)+k−1−i, strictly lower than the target. The identity o(Ck)=0 gives the reduction. Negative-weight terms vanish because Vd=0 for d<0. Fix a strong spanning expression for each state: the induction decreases weight and each Ck is finite, so it terminates and yields a polynomial independent of M. Combining with step 2.1 proves both assertions.

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