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P(z)-compatibility subspace and local grading restriction

Definition

Let A be an abelian group, let à contain A as a subgroup, and let V be a strongly A-graded Möbius or conformal vertex algebra. Fix z∈C× and strongly Ã-graded generalized V-modules W1,W2, using the decompositions and operators of def-cft-hlz-strongly-graded-generalized-module. Fix a full category C of strongly Ã-graded generalized V-modules, with morphisms preserving both gradings and, in the Möbius case, all three L(j). For any strongly A~-graded module M, give its restricted dual the grading M′[h](β)=(M[h](−β))∗. A functional in (W1⊗W2)∗ is homogeneous of degree β when it vanishes on every input component except those of total degree −β. For λ∈(W1⊗W2)* define the transported field by

(YP(z)′(v,x1)λ)(w1⊗w2)=λ(w1⊗YW2o(v,x1)w2)+Res⁡x0z−1δ ⁣(x1−1−x0z)λ ⁣(YW1(ex1L(1)(−x1−2)L(0)v,x0)w1⊗w2). The transported action of x0−1δ((x1−1−z)/x0)Yt(v,x1) on λ is the formal series whose evaluation at w1⊗w2 is z−1δ ⁣(x1−1−x0z)λ ⁣(YW1(ex1L(1)(−x1−2)L(0)v,x0)w1⊗w2)+x0−1δ ⁣(z−x1−1−x0)λ(w1⊗YW2o(v,x1)w2), where Yt is the diagonal field and formal delta expansions follow the module conventions. Let COMPP(z) consist of λ for which YP(z)′(v,x1)λ has finitely many negative powers and the transported series equals x0−1δ((x1−1−z)/x0)YP(z)′(v,x1)λ for every v∈V. For j=−1,0,1 define the transported operators by (LP(z)′(j)λ)(w1⊗w2)=λ(w1⊗L(−j)w2)+∑i=01−j(1−ji)ziλ(L(−j−i)w1⊗w2). In the conformal case these are also the corresponding coefficients in YP(z)′(ω,x)=∑j∈ZLP(z)′(j)x−j−2. The P(z)-local grading restriction requires λ to be a finite sum of generalized LP(z)′(0)-eigenvectors, each homogeneous for the A~-grading. Let Wλ be the smallest doubly graded subspace containing λ and stable under every mode of YP(z)′(v,x) and the operators LP(z)′(−1),LP(z)′(0),LP(z)′(1). For every β∈A~ and generalized weight h∈C, require dim⁡(Wλ)[h](β)<∞ and (Wλ)[h+k](β)=0 for all sufficiently negative integers k. For a P(z)-map I with target W, define I′(w′)(w1⊗w2)=⟨w′,I(w1⊗w2)⟩. Define W1 P(z) W2 as the sum of these images I'(W') over all W∈C and all such I; transposed Jacobi and grading conditions put each image in the stated compatibility and local-grading subspace.

Facts & Assumptions

Given: Work over C with the formal-variable, grading, and branch conventions in the linked definitions.

[F1]

Conformal vertex algebra of CFT type: A conformal vertex algebra of CFT type is a complex vertex algebra V in the sense of def-vertex-algebra-state-field, with a specified vector ω∈V and scalar c∈C, such that, writing Y(ω,z)=∑n∈ZL(n)z−n−2, the operators L(n) and scalar central action c satisfy the Virasoro relations of def-virasoro-algebra, and L(−1)=T. In addition, L(0) is diagonalizable, Vn:={v∈V:L(0)v=nv} gives V=⨁n≥0Vn, every Vn is finite dimensional, and V0=C1. Under this page's convention, this is a vertex operator algebra of CFT type. The grading and the CFT-type condition are part of the definition; they do not follow from the vertex-algebra axioms alone. The conformal weight of v∈Vn is n. A conformal vector, a grading, and the nonnegative grading condition are additional data beyond an ordinary vertex algebra.

[F2]

Grading-restricted generalized module: Let V be a conformal vertex algebra of CFT type and M a left V-module. Write LM(0) for the coefficient determined by YM(ω,z)=∑n∈ZLM(n)z−n−2. For h∈C, define the generalized LM(0)-eigenspace M[h]={m∈M:(LM(0)−h)Nm=0 for some integer N≥1}. The module is grading-restricted generalized if M=⨁h∈CM[h], every M[h] is finite dimensional, and the real parts of its nonzero generalized weights are bounded below. The direct sum means each vector has only finitely many generalized-weight components. This convention explicitly adds finite-dimensionality and a lower bound to the generalized-eigenspace decomposition; those conditions are not consequences of the module Jacobi identity.

[F3]

Module for an ordinary vertex algebra: Let V be a vertex algebra over C in the ordinary, non-super convention of def-vertex-algebra-state-field. A left V-module is a complex vector space M and a linear map YM(−,z):V⟶{formal fields on M},a⟼YM(a,z)=∑n∈Za(n)Mz−n−1, with the following properties: 1. Lower truncation. For every a∈V and m∈M, a(n)Mm=0 for all sufficiently large integers n, so YM(a,z)m∈M((z)) in the support convention of def-formal-distribution-on-a-vector-space. 2. Vacuum. YM(1,z)=id⁡M. 3. Module Jacobi identity. For every a,b∈V, z0−1δ ⁣(z1−z2z0)YM(a,z1)YM(b,z2)−z0−1δ ⁣(z2−z1−z0)YM(b,z2)YM(a,z1)=z2−1δ ⁣(z1−z0z2)YM(Y(a,z0)b,z2). Here δ(x)=∑r∈Zxr; the first expansion is in nonnegative powers of z2, the second in nonnegative powers of z1, and the right-hand expansion is in nonnegative powers of z0. They use the formal binomial conventions of def-formal-distribution-on-a-vector-space. The Y inside the right-hand side is the state-field map of V; it is not the action map YM. A V-module homomorphism f:M→N is a linear map such that fYM(a,z)=YN(a,z)f for every a∈V. This definition does not impose a conformal grading, finite-dimensional weight spaces, semisimplicity of L0, a right-module convention, or a twist by an automorphism. For a conformal vertex algebra, write YM(ω,z)=∑n∈ZLM(n)z−n−2 when a conformal vector ω is specified. A V-submodule of M is a linear subspace stable under every mode a(n)M. A module is simple (or irreducible) if it is nonzero and has no proper nonzero V-submodule. A module is completely reducible (or semisimple) if it is an internal direct sum of simple V-submodules; the empty direct sum is the zero module.

[F4]

Contragredient module of a generalized module: For a grading-restricted generalized module M over a conformal vertex algebra V, its contragredient candidate is M′=⊕h∈CM[h]∗, with action defined by ⟨YM′(v,x)w′,w⟩=⟨w′,YMo(v,x)w⟩, where YMo(v,x)=YM(exL(1)(−x−2)L(0)v,x−1). On homogeneous integer-weight vectors, (−x−2)L(0) contributes (−1)wt(v)x−2wt(v). Whether this formula satisfies all module axioms and gives M''≅M is a separate theorem; this definition alone does not assert it. V is self-contragredient when V≅V' as V-modules.

[F5]

P(z)-intertwining map: Let z∈C× and W1,W2,W3 be generalized V-modules. A P(z)-intertwining map of type (W3;W1,W2) is a linear map I:W1⊗W2→Wˉ3=∏h∈CW3[h] whose Ã-degrees add, for which πh−mI(w1⊗w2)=0 for all sufficiently large integers m for each fixed h,w1,w2, and which satisfies the P(z)-Jacobi identity and, for j=−1,0,1,L(j)I(w1⊗w2)=I(w1⊗L(j)w2)+∑i=0j+1(j+1i)ziI((L(j−i)w1)⊗w2). There is no L(-1)-derivative axiom for I. Formal variables x0,x1 are independent; z is a fixed complex number.

[F6]

Strongly graded generalized module in the HLZ setting: Let V be an ordinary non-super vertex algebra in the sense of def-vertex-algebra-state-field. A Möbius vertex algebra is V with operators L(-1),L(0),L(1) representing sl(2), with L(-1) equal to translation, and satisfying [L(j),Y(v,x)]=∑i=0j+1(j+1i)xiY(L(j−i)v,x) for j=−1,0,1. A Möbius module has the corresponding sl(2)-action and field commutator identities. A conformal vertex algebra supplies these operators through its Virasoro field. For a generalized module write L(0)s for the diagonal operator acting by h on W[h]; the nilpotent part is L(0)−L(0)s. Let A be an abelian group and suppose V has compatible integer-weight and A-gradings V=⊕n∈Z,α∈AV(n)(α), each component finite dimensional and lower truncated in n for each α, 1∈V(0)(0),vmV(β)⊂V(α+β), and L(j)V(α)⊂V(α) for j=−1,0,1. In the conformal case require ω∈V(2)(0). For an abelian group Ã⊃A, a generalized module W=⊕h∈C,β∈A~W[h](β) is strongly Ã-graded when the gradings are compatible, each W[h](β) is finite dimensional, W[h+k](β)=0 for all sufficiently negative integers k for each h,β, vmW(β)⊂W(α+β), and L(j)W(β)⊂W(β) for j=−1,0,1. Morphisms preserve both gradings and the V-action.

[F7]

Strongly graded contragredient duality for Möbius and conformal modules proves the opposite-field restricted dual and double-dual evaluation for arbitrary strongly graded generalized modules over strongly graded Möbius or conformal vertex algebras. Its lower truncation uses a fixed auxiliary-degree integer weight string, and does not assume a globally bounded grading or CFT type.

Proof

1.1givenF1F2F3F4F6algebra

The residue action is the transpose of the diagonal vertex action together with the opposite second-input field; module truncation and the finite L(1)-sum make its coefficients defined on homogeneous inputs.

2.1givenF1F2F3F4F5F6F7step 1.1algebra∎

Let I:W1⊗W2→W‾ be a P(z)-map with W∈C, and define I′:W′→(W1⊗W2)∗ by transposition. Transposing its P(z)-Jacobi identity gives the defining transported compatibility identity, while the three L(j) identities give compatibility with the transported LP(z)′(j). The transposed field identity makes I′ intertwine the contragredient action on W′ with the transported action on its image. The strong grading of W then gives finite-dimensional components and lower truncation for W'. Since every w′∈W′ is a finite sum of doubly homogeneous generalized-weight vectors, I′(w′) is a finite sum of homogeneous generalized LP(z)′(0)-eigenvectors. The subspace generated from I′(w′) by the transported modes is the image under I′ of the submodule generated by w′ in W′. Its doubly graded components therefore remain finite dimensional and lower truncated. Thus each image lies in the stated compatibility and local-grading subspace, so their sum does also.

Depends on

Dependency tree · 2 levels

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