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Strong generators generate the lowest space of a cyclic module
Pure mathematics; no physical premises or physical claim.
Statement
Let be a conformal vertex algebra with , strongly generated by homogeneous positive-weight states , meaning where the word is . Let be an admissible -module, so a homogeneous satisfies . If is cyclic on , meaning where the word is , then Moreover, for each homogeneous state , a noncommutative polynomial in the generator zero modes, depending only on and a fixed strong spanning expression for it, equals 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 , irreducibility, -cofiniteness, the existence of a universal induced module, or the general Zhu correspondence.
Statement references
Facts & Assumptions
Given: The objects, hypotheses and conventions in the Statement.
The CFT-type grading, nonnegative admissible module grading, strong generating set , and cyclic vector are precisely the hypotheses of the Statement.
Conformal vertex algebra of CFT type gives the nonnegative integer state weights and vacuum line.
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.
Admissible module for a vertex operator algebra specifies the degree shift and the vanishing of negative module degrees. Strong generation here means that is spanned by finite words of strictly negative modes of states in applied to .
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
Give a mode of homogeneous degree . The commutator identity in [A2] and its state-product weight rule show every term in has degree . The sum is finite by state truncation. Thus mode commutators preserve total degree.
Let be homogeneous of weights , with , and define the inhomogeneous states for . Extend linearly over homogeneous components. For the summand indexed by , put and , the zero-mode index of . The iterate identity in [A2] gives The first term has rightmost mode of degree .
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 : 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 , a rightmost negative-degree mode kills by admissibility. A word containing only nonnegative modes and at least one positive-degree mode has positive total degree. Since is cyclic on , its degree-zero space is therefore spanned by words in , , applied to .
Because , this first term kills for every . For it can survive only at , when it is exactly . In the second term kills for . For each fixed , the mode is independent of . Its coefficient after summing over is, up to the fixed sign , Indeed is a polynomial of degree , so its th 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 and for on .
Induct on state weight to express every on as a noncommutative polynomial in . Weight zero gives the identity. A strong spanning monomial of positive weight is with , , and a shorter strong monomial. For , expand : its first term is , while every other term has weight , strictly below the target weight; also has lower weight because . The identity in step 2.2 expresses its zero mode using and those lower-weight zero modes. For , expand ; its first term is , and each remaining term has weight , strictly lower than the target. The identity gives the reduction. Negative-weight terms vanish because for . Fix a strong spanning expression for each state: the induction decreases weight and each is finite, so it terminates and yields a polynomial independent of . Combining with step 2.1 proves both assertions.