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Higher Zhu action on the Omega spaces of an arbitrary weak module
Statement
Let V be a vertex operator algebra with finite-dimensional nonnegative integral state grades, allowing V0 larger than C1, and let M be any weak left V-module. For an integer define For homogeneous a of weight r put , extending linearly in a. Every o(a) preserves , every element of acts by zero, and When V is of CFT type, the linked associative-quotient theorem consequently makes a unital left . The preservation, and multiplicativity identities themselves hold in the full nonnegative scope just stated. No grading, local finiteness or semisimplicity of L(0) on M is assumed. This is the forward action; no converse rationality criterion is asserted.
Facts & Assumptions
Given: The full non-super conformal state-field setup and weak module in the Statement. Here the broader term “vertex operator algebra” means the following data, without the CFT-type condition .
is a complex vector space with vacuum , translation , and state-field map satisfying the lower-truncation, vacuum/creation, translation-covariance, and locality axioms of Vertex algebra in the state–field convention. It has a conformal vector with and central charge , where for all , and . The operator is diagonalizable and , where is finite dimensional. No condition is imposed. A weak left module is a complex vector space with a lower-truncated field map , vacuum action, and the full module Jacobi identity of Module for an ordinary vertex algebra; it has no grading or -semisimplicity assumption. For homogeneous , write .
Taking the two residues of the module Jacobi identity in [F1] gives, for all integers , The first sum is finite by state truncation; on each fixed vector the two terms of the iterate sum are separately finite by rightmost-mode truncation. For negative integer upper indices, . Translation covariance and the conformal-vector residues give , , and when the state product is nonzero. These are consequences of the stated Jacobi axioms; they do not require .
For homogeneous and , and each , the formulas used here are where the circle expression is extended linearly over homogeneous first inputs. This is the full nonnegative-grade convention used locally; in the CFT-type case it agrees with Higher Zhu quotients and candidate products, and Associative structure of the higher Zhu quotients separately proves associativity and descent of the quotient product.
Proof
Let a have weight r and b have weight s. For , commuting past gives terms with coefficient binom(m,j). Their state weight is s+r-j-1 and their mode index is at least this weight plus N. Each kills w in , as does w. The commutator sum is finite by state truncation. Thus o(a) preserves . Vacuum acts identically by the module vacuum identity.
The zero mode of a circle generator is Apply the iterate identity. In every first term the b index is , so that term kills w. In the second terms the b index is the fixed r+s-2-t. Values kill w through . For each remaining , the summed coefficient is a scalar multiple of the finite difference of order r+N of a polynomial in j of degree t. Thus every circle generator acts by zero. All sums can be exchanged here: j ranges over a finite set; in the first iterate sum is zero for all large t, and in the second w is zero for all large t. Also . Therefore . This includes , where the second surviving t range is empty.
Expand using F1 and the iterate identity. For a fixed outer star index p, the second iterate terms again have b index r+s-2-t independent of j. They vanish for , and for their sum over j is the finite difference of the degree-t polynomial binom(j-N-p-1,t), hence zero. In the first terms put the a index . Its b index is r+s-2-k. The Omega cutoff on b eliminates . The inequalities and give . Thus the only possible terms are Write . Then , so their coefficient is exactly This expression accounts for every surviving first term; it uses no cancellation of unknown infinite sums.
The inner sum is the coefficient of in It therefore equals binom(N+a,a-p). Consequently Only o(a)o(b)w remains, proving multiplicativity. Step 1.1 and step 1.2 give the claimed full-scope identities. In the CFT-type case F1 then gives the claimed unital . No existence/induction theorem or nonresonance of conformal-weight differences was used.