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Associative structure of the higher Zhu quotients
Statement
For each integer , let and be as in the higher Zhu definition. Then is a two-sided ideal for , and descends to an associative unital product on with unit . No finite-dimensionality of is asserted.
Statement references
Facts & Assumptions
Given: The CFT-type conformal vertex algebra and the arbitrary integer in the Statement. Write , and . All congruences below are additive congruences in the vector space ; neither ideal stability nor associativity is assumed when manipulating them. Set
Higher Zhu quotients and candidate products defines the finite circle and star residues, with included in . For a homogeneous state , write , so .
Conformal vertex algebra of CFT type supplies the nonnegative integer weights and . Vertex algebra in the state–field convention gives vectorwise truncation, vacuum/creation and translation covariance.
Jacobi and residue calculus from the state-field locality axioms proves the actual regular-module Jacobi identity, , and . Its Laurent-polynomial residue identity, used on , is Here is a Laurent polynomial and is any integer; the two symbols mean the indicated binomial expansions. This is a proved local supplier, not an invocation of the higher-Zhu algebra theorem.
Proof
For homogeneous and arbitrary define Every such vector lies in the span of circle generators, without using any ideal property. Indeed . Integration by parts and [F3] give If , the same equality holds with left side zero. Induction on , simultaneously for all homogeneous first inputs, therefore gives , since is nonzero. Expanding the extra factor then gives , with every . All these residues are finite sums by truncation and the nonnegative exponents.
Two exact identities will later convert this residue information into both ideal properties. For homogeneous , For the first, integrate against and add . The result is For , ; all adjacent coefficients cancel and the sum is exactly . This proves the first identity. For the second let , use and , the latter being the weight rule of [F3]. Integration by parts gives On the other hand shows that is the same residue with replaced by ; adding proves the identity. Linearity extends both formulas to arbitrary inputs, with the circle operation extended linearly in its first input.
We prove the associator belongs to before using any product of congruence classes. Let , and be homogeneous. Expanding the two star products and using the actual weight of each gives the exact expression Apply [F3] with and . The forward expansion uses and the reversed expansion uses Every reversed-product residue lies in : after extracting the residue its outer -residue has numerator and denominator , so it is , where . Here . Every forward residue with also lies in : after extracting its residue its outer -residue is , where . Both conclusions use only step 1.1. All sums are actually finite on the fixed : the finite polynomial numerators make and sums of modes whose indices tend to with , so truncation kills them for large . Thus the additive congruence left after discarding these residues is No ideal assertion was used in discarding any term.
The finite kernel in step 2.1 equals the kernel of . Explicitly, as a Laurent polynomial in with coefficients in , For a fixed , its left coefficient is The factorial identity giving this equality is valid at every displayed index. The binomial theorem makes the final sum , so the coefficient is exactly . Substitution in step 2.1 proves . Bilinearity extends this independently proved associator congruence to arbitrary triples.
Right ideal stability now follows without multiplying a prior congruence by an arbitrary state. The generators satisfy by step 1.2. The other generators satisfy where the only congruence is the associator of step 3.1 applied to the actual states . Hence . The exact derivation formula of step 1.2 next gives . Finally The last inclusion uses the already proved right ideal stability on the actual element . These statements establish as well. This order avoids circular use of left and right ideal properties.
The vacuum is a two-sided identity modulo . On the left, and give since the polynomial has no coefficient in degree for , and its degree- coefficient is . For the right identity let . The relations give, by induction, Thus coefficientwise modulo . Only finitely many creation coefficients enter any of the star residues, so substitution into is an ordinary finite linear congruence. It gives the same scalar residue as on the left, hence . Step 4.1 makes the quotient product independent of both representatives; step 3.1 then gives associativity and the two vacuum identities give unit . All calculations hold also for and weight . No dimension assertion or representation-theoretic classification is used.