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Clifford and Weyl algebras in symmetric tensor categories

Published 18 Jul 2026 in math.RT, math.CT, math.QA, and math.RA | (2607.16910v1)

Abstract: Let C\mathcal C be a symmetric tensor category over an algebraically closed field k\mathbf k of characteristic ≠2\ne 2. We study Clifford and Weyl algebras of objects of C\mathcal C with a (skew-)symmetric bilinear form. When the form is non-degenerate, we establish simplicity and the Azumaya property for such algebras under suitable assumptions. We also compute Clifford and Weyl algebras in the Verlinde category Verp{\rm Ver}_p and use them to prove that if C\mathcal C is Frobenius exact then the Weyl algebra of a symplectic object of C\mathcal C with finite symmetric algebra is Azumaya. Using this, we introduce the symplectic Witt group SW(C)\mathcal S\mathcal W(\mathcal C), the subgroup of the Brauer group Br(C){\rm Br}(\mathcal C) consisting of Morita classes of such Azumaya algebras, and when C=Rep(G)⊠sVec\mathcal C={\rm Rep}(G)\boxtimes{\rm sVec} for a finite group GG of order coprime to char(k){\rm char}(\mathbf k), express SW(C)\mathcal S\mathcal W(\mathcal C) in terms of second Stiefel-Whitney classes of orthogonal representations of GG.

Authors (1)

Summary

  • The paper constructs Clifford and Weyl algebras internally to symmetric tensor categories and proves PBW theorems using contraction operators and finite Moyal–Weyl products.
  • It establishes simplicity and the Azumaya property under finite-length or characteristic-dependent symmetric-power conditions, then classifies key examples in the Verlinde category.
  • The paper defines a symplectic Witt group within the Brauer group and relates its classes for representation categories to second Stiefel–Whitney classes, with surjectivity for abelian groups but failures for some metacyclic groups.

Overview

This paper develops a theory of Clifford and Weyl algebras internal to an arbitrary symmetric tensor category C\mathcal{C} over an algebraically closed field kk of characteristic ≠2\ne 2. The author constructs these algebras as quotients of enveloping algebras of Heisenberg (super)algebras, proves a PBW theorem, establishes simplicity and the Azumaya property under suitable hypotheses, computes explicit examples in the Verlinde category Verp\mathrm{Ver}_p, and uses the resulting Azumaya algebras to define a symplectic Witt group SW(C)\mathcal{SW}(\mathcal{C}) inside the Brauer group. The final main result identifies this group for C=Rep(G)⊠sVec\mathcal{C} = \mathrm{Rep}(G) \boxtimes \mathrm{sVec} with data built from second Stiefel–Whitney classes of orthogonal representations of GG.

Definitions and basic structure

For an object V∈CV \in \mathcal{C} with a symmetric or skew-symmetric bilinear form BB, the object V⊕1V \oplus \mathbf{1} carries the structure of a Lie superalgebra in kk0: the Heisenberg algebra when kk1 is skew-symmetric (purely even), and the Heisenberg superalgebra when kk2 is symmetric (kk3 even, kk4 odd). The associated algebra is

kk5

called the Weyl algebra in the skew case and the Clifford algebra in the symmetric case; for kk6 this recovers the classical definitions (with the normalization kk7).

Two structural facts organize the theory. First, twisting by a super-line kk8 exchanges symmetry types: there is a natural isomorphism kk9, so in any category containing a super-line the Weyl and Clifford theories are equivalent. Second, for objects ≠2\ne 20 carrying forms of the same type one has ≠2\ne 21, with the super-tensor product in the Clifford case.

Contraction operators and the PBW theorem

The proof machinery rests on bicontraction maps ≠2\ne 22 built from the coproduct components of the Hopf algebra ≠2\ne 23 and the form ≠2\ne 24. Iterated contractions satisfy ≠2\ne 25; consequently, if ≠2\ne 26, then ≠2\ne 27, a fact that governs all positive-characteristic phenomena in the paper.

The PBW theorem states that the natural surjection ≠2\ne 28 (respectively ≠2\ne 29) is an isomorphism, so Verp\mathrm{Ver}_p0 is a filtered quantization of the Poisson algebra Verp\mathrm{Ver}_p1 (or super-Poisson algebra Verp\mathrm{Ver}_p2). The proof reduces to Weyl algebras via the super-line trick and defines an explicit Moyal–Weyl product on Verp\mathrm{Ver}_p3 by Verp\mathrm{Ver}_p4 with Verp\mathrm{Ver}_p5; associativity follows from the identity Verp\mathrm{Ver}_p6. In characteristic zero this recovers Verp\mathrm{Ver}_p7; in characteristic Verp\mathrm{Ver}_p8 the sum terminates because Verp\mathrm{Ver}_p9, which is what makes the formula valid without division issues beyond the factors SW(C)\mathcal{SW}(\mathcal{C})0 (permissible since SW(C)\mathcal{SW}(\mathcal{C})1). A shorter alternative proof via the schematic Heisenberg group SW(C)\mathcal{SW}(\mathcal{C})2 and known PBW results for group schemes in symmetric tensor categories is also given.

Simplicity and the Azumaya property

The central simplicity result concerns SW(C)\mathcal{SW}(\mathcal{C})3 for a simple (ind-)algebra SW(C)\mathcal{SW}(\mathcal{C})4 in SW(C)\mathcal{SW}(\mathcal{C})5. Two cases are established:

  • Skew case: if SW(C)\mathcal{SW}(\mathcal{C})6 whenever SW(C)\mathcal{SW}(\mathcal{C})7, then SW(C)\mathcal{SW}(\mathcal{C})8 is simple.
  • Hyperbolic case: for SW(C)\mathcal{SW}(\mathcal{C})9 with the canonical pairing, if C=Rep(G)⊠sVec\mathcal{C} = \mathrm{Rep}(G) \boxtimes \mathrm{sVec}0, then C=Rep(G)⊠sVec\mathcal{C} = \mathrm{Rep}(G) \boxtimes \mathrm{sVec}1 is simple.

Both proofs are filtration arguments: commutators with generators produce contractions that strictly lower degree, and injectivity of the relevant maps C=Rep(G)⊠sVec\mathcal{C} = \mathrm{Rep}(G) \boxtimes \mathrm{sVec}2 below degree C=Rep(G)⊠sVec\mathcal{C} = \mathrm{Rep}(G) \boxtimes \mathrm{sVec}3 forces any nonzero ideal to meet C=Rep(G)⊠sVec\mathcal{C} = \mathrm{Rep}(G) \boxtimes \mathrm{sVec}4, hence to be everything. A corollary extends this to orthogonal direct sums of such summands.

The main application is to Frobenius exact categories. If C=Rep(G)⊠sVec\mathcal{C} = \mathrm{Rep}(G) \boxtimes \mathrm{sVec}5 is Frobenius exact and C=Rep(G)⊠sVec\mathcal{C} = \mathrm{Rep}(G) \boxtimes \mathrm{sVec}6 has finite length, then:

  1. C=Rep(G)⊠sVec\mathcal{C} = \mathrm{Rep}(G) \boxtimes \mathrm{sVec}7 is simple for symplectic C=Rep(G)⊠sVec\mathcal{C} = \mathrm{Rep}(G) \boxtimes \mathrm{sVec}8;
  2. the natural map C=Rep(G)⊠sVec\mathcal{C} = \mathrm{Rep}(G) \boxtimes \mathrm{sVec}9 is an isomorphism;
  3. GG0 is a central Azumaya algebra.

The key input is a lemma showing that a category tensor-generated by GG1 with GG2 (or GG3) of finite length has moderate growth; in characteristic zero it is then super-Tannakian by Deligne's theorem, while in characteristic GG4 it admits a fiber functor to GG5. The positive-characteristic argument analyzes the decomposition of GG6 into simples GG7: since GG8 for GG9 and V∈CV \in \mathcal{C}0 (finite length of V∈CV \in \mathcal{C}1), the situation decomposes into copies of V∈CV \in \mathcal{C}2 (even V∈CV \in \mathcal{C}3) and hyperbolic planes V∈CV \in \mathcal{C}4 (odd V∈CV \in \mathcal{C}5, reducing to the previously established cases. The Azumaya property follows from the observation that V∈CV \in \mathcal{C}6 is isometric to V∈CV \in \mathcal{C}7 hyperbolic, so the left-right action map identifies with V∈CV \in \mathcal{C}8.

Top symmetric powers and queer algebras

For a symplectic object V∈CV \in \mathcal{C}9 with BB0 of finite length in a Frobenius exact category, writing BB1 for the top degree with BB2, the object BB3 is invertible, and natural duality isomorphisms BB4 hold, together with BB5. Moreover BB6, so BB7 is a super-line precisely when BB8 is odd. This is proved by reducing along fiber functors to BB9 and V⊕1V \oplus \mathbf{1}0, using that V⊕1V \oplus \mathbf{1}1 is Frobenius via the Verlinde fiber functor.

The paper also classifies simple algebras in V⊕1V \oplus \mathbf{1}2: they are exactly V⊕1V \oplus \mathbf{1}3 and the queer algebras V⊕1V \oplus \mathbf{1}4 for nonzero V⊕1V \oplus \mathbf{1}5. This follows from the classification of indecomposable exact module categories over V⊕1V \oplus \mathbf{1}6 (corresponding to the ADET graphs V⊕1V \oplus \mathbf{1}7 and V⊕1V \oplus \mathbf{1}8) plus standard reconstruction. A concrete identification connects this to classical representation theory: for V⊕1V \oplus \mathbf{1}9, the Weyl algebra kk00 is isomorphic to kk01, where kk02 is the image of the spin representation of kk03 in kk04 — obtained by transporting the classical isomorphism kk05 through the Verlinde fiber functor.

The symplectic Witt group

For Frobenius exact kk06, the classes kk07 of symplectic objects with kk08 of finite length, modulo those with kk09, form an elementary abelian 2-group kk10, the symplectic Witt group. Since kk11, the Azumaya property gives kk12, so every class is 2-torsion, and the assignment kk13 defines an inclusion

kk14

the 2-torsion subgroup of the Brauer group. Injectivity holds because Brauer-triviality of kk15 reconstructs kk16 as kk17 for some kk18.

Computation for Rep(G) ⊠ sVec

Let kk19 be finite of order coprime to kk20 and kk21. By Carnovale's theorem, kk22, where kk23 denotes cohomology with the modified multiplication kk24. For an orthogonal representation kk25 of kk26, stabilizing to kk27 yields a class kk28 as the pullback of the Clifford-group extension. The main computation gives

kk29

so kk30, where kk31 is generated by the kk32. The proof identifies kk33 with the classical Clifford superalgebra kk34, computes its Picard restriction to kk35 as kk36, and constructs explicit twisted-adjoint lifts kk37 realizing the multiplier kk38. A subsequent remark refines this: under the Künneth decomposition, kk39 versus kk40, so the raw pullback requires correction by the mixed cocycle kk41 in odd dimension.

Stiefel–Whitney classes over ℂ

Over kk42, writing kk43 for the Stiefel–Whitney classes of an orthogonal representation, one has kk44 and kk45. The Whitney sum formula shows the modified multiplication on kk46 corresponds to kk47, and the key vanishing kk48 holds since kk49 is a coboundary. Defining the Stiefel–Whitney subgroup

kk50

one obtains kk51 as sets, where kk52, and this is a subgroup for ordinary multiplication as well. Notably, kk53 need not be a subgroup for kk54 — for kk55 the class kk56 of two coordinate characters is nonzero.

The resulting surjectivity criterion is sharp:

Statement Condition / example
kk57 surjective iff kk58
kk59 surjective whenever kk60 is abelian
kk61 not always surjective type-1 split metacyclic groups

For abelian kk62, kk63, so cup products of characters exhaust the 2-torsion. For non-surjectivity, the metacyclic examples of Gunarwardena–Kahn–Thomas supply a degree-two class outside the span of second Stiefel–Whitney classes; the argument uses that kk64 consists of Kummer classes of complex characters, themselves realizable as kk65 of oriented real two-planes, so no correction can rescue the class.

Limitations and open questions

Several hypotheses are essential and their removal is not addressed. Simplicity and the Azumaya property require kk66 (or finite length of kk67); the behavior of kk68 when symmetric powers grow indefinitely, e.g., for negligible objects, is not treated. The symplectic Witt group is defined only within Frobenius exact categories, and the explicit Stiefel–Whitney computation requires kk69 with kk70; the non-semisimple or non-super-Tannakian analogues are open. The classification of simple algebras is specific to kk71 and relies on the known module-category classification there. Finally, the failure of surjectivity of kk72 for general finite groups leaves open a precise characterization of which 2-torsion Brauer classes arise from symplectic objects beyond the abelian and metacyclic cases considered here.

Conclusion

The paper supplies a categorical framework in which Clifford and Weyl algebras behave as in classical algebra — PBW, simplicity, Azumaya — provided symmetric powers vanish above the characteristic, and demonstrates that Frobenius exactity converts finite-length hypotheses into verifiable fiber-functor computations in kk73. The resulting symplectic Witt group links the Brauer 2-torsion of super-representation categories to Stiefel–Whitney theory, with a complete answer for abelian groups and a concrete obstruction class for the general case.

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