Alphabeta Math
How statement and proof provenance work

The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.

  • Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.

These labels describe origin, not correctness: citations and verification chips remain separate evidence.

Higher Categorical Symmetries and Defect Algebras

1 · Prerequisites

2 · Summary

This page develops the algebraic structure behind higher symmetries and defect composition. It defines weak linear and fusion 2-categories, constructs the finite-group model 2VectGω, proves its 4-cocycle coherence and identity-on-grading cochain gauge, and gives a separability-projector construction of relative tensor products for bimodules. The general Mod⁡(C) theorem is proved for braided fusion categories over algebraically closed fields of characteristic zero, with AC through the stated classical algebraic geometry suppliers. Its local chain constructs nonpivotal canonical-algebra separability, Eilenberg–Watts, finite semisimple hom categories, adjoints, monad splittings, both object duals, relative products and coherence, explicit fusion-data rank bounds, normalized deformation contraction, and finite-type open-orbit finiteness. All carriers remain draft.

Reading prerequisite

The plan places this page after modular-categories-verlinde-and-tqft. That is a reading route. The finite-group 2-vector-space model is independent of modularity. The algebraic Mod⁡(C) construction applies to a braided fusion category C; it uses braiding to define the tensor product. The batch manifest records the actual item dependencies separately.

Composition and anomaly data

In a selected 2+1D defect theory, surface labels may be modeled by objects, line junctions by 1-morphisms, and point junctions by 2-morphisms. Tensor product of objects and categorical composition of 1-morphisms have different source and target types. A braided fusion 2-category concerns additional data in a specified 3+1D setting; the 2+1D algebraic construction here does not classify those theories.

For finite G, the scalar class [ω]∈H4(G;C×) obstructs removing the pentagonator by the identity-on-grading cochain gauge defined on this page. This is an algebraic obstruction for the stated model. It is distinct from the Maslov/framing correction in the PA-47 surgery construction, and neither alone classifies physical anomalies.

Weighted RT background

The full PA-47 weighted state-space, bordism-map and factorization interface is recorded in Weighted RT background interface for Mod(C). Its actual supplier The weighted Reshetikhin–Turaev TQFT and modular-functor factorization proves the complete marked weighted RT functor, with positive weight action, exact cap-reference correction and both geometric sewing inverses. The algebraic Mod(C) theorem above has no logical dependency on RT data; this separate background supplies no canonical physical realization or phase classification.

Modeling boundary

The October 2, 2026 preprint Kobayashi, Prem, and Yu is retained as dated research context only. Its abstract claims a general construction; its introduction restricts the main realization result to two stated families, says the proposed mixed-state Ansatz is not proved, and disclaims a classification of mixed-state phases. This batch has read only the abstract and introduction, not the proofs, and uses none of the claims as a premise. A physical identification of algebraic objects with defects requires a specified field theory, boundary interpretation, and dimensional setting. A unitary refinement likewise needs compatible dagger data, positive traces, and unitary coherence maps; the general complex-linear results here do not assert those extra structures.

Companion worked examples: higher-categorical-symmetry-and-defect-algebras-examples.

The algebra model uses left algebra modules. An A-B bimodule acts from left B-modules to left A-modules, so the model identifies the module 2-category with the 1-morphism-opposite of the stated algebra bicategory. Tensor multiplication uses the positive middle braiding; the right-to-left action conversion uses its specified inverse. The negative opposite gives a left algebra-bicategory dual and the positive opposite gives a right dual, with their roles exchanged after reversing 1-morphisms. No pivotal or unitary enhancement is assumed.

3 · Logical flowchart

4 · Definitions, theorems and proofs

DefinitionDefinition: AI-adaptedProof: Not applicableOpen item page →

Finite semisimple module category over a fusion category

Definition

Let C be a fusion category over k. A finite semisimple right C-module category consists of a k-linear abelian category M, semisimple in the sense of Semisimple objects and semisimple abelian categories, with finitely many isomorphism classes of simple objects and finite-dimensional k-vector spaces Hom⁡M(m,n) for all m,n∈M, together with a bilinear action functor ⊙:M×C→M and natural isomorphisms αm,X,Y:(m⊙X)⊙Y⟶m⊙(X⊗Y),ρm:m⊙1⟶m, which satisfy the module pentagon and triangle equations obtained from the associator and unitors of C. The left-action convention is defined by reversing the order of the action factors.

A module functor F:M→N is a linear functor with natural action comparisons F(m⊙X)≅F(m)⊙X satisfying the module associativity and unit equations. A module-natural transformation is a natural transformation commuting with those comparisons. These objects, functors, and transformations form a 2-category denoted Mod⁡(C) with ordinary composition of module functors and horizontal and vertical composition of module-natural transformations. The action comparison for a composite is the composite of the two action comparisons; identity functors have identity comparisons.

This definition alone does not assert that there are finitely many equivalence classes of simple module categories, nor that Mod⁡(C) is a fusion 2-category.

DefinitionDefinition: AI-adaptedProof: Not applicablejudge pass (gpt-6-luna)Open item page →

G-graded finite semisimple 2-vector space

Definition

Fix an algebraically closed field k of characteristic zero and a finite group G (Group and abelian group). A finite semisimple category is understood in the sense of Semisimple objects and semisimple abelian categories, with simple objects as in Simple object. A finite semisimple G-graded k-linear category is a finite semisimple k-linear category A together with a direct-sum decomposition A=⨁g∈GAg. An object in Ag is homogeneous of degree g. A grading-preserving linear functor sends each Ag into the corresponding degree-g summand, and its 2-morphisms are natural transformations. Such categories, functors, and natural transformations form the underlying 2-category denoted 2VectG.

For finite semisimple categories A,B with simple-label sets S,T, their finite semisimple tensor product A⊠B has simple labels S×T and Hom⁡(s⊠t,s′⊠t′)=Hom⁡A(s,s′)⊗kHom⁡B(t,t′), extended to direct sums. For a concrete skeleton, choose finite sets Sg of simple labels and replace Ag by the category of finite-dimensional k-vector-space families indexed by Sg. A linear functor is represented by a finite matrix of finite-dimensional vector spaces within each grade. This skeleton fixes the meaning of “finite” and the homogeneous components; it does not assert any physical realization.

DefinitionDefinition: Literature-sourcedProof: Not applicableOpen item page →

Weighted RT background interface for Mod(C)

Definition

Suppose a modular ribbon fusion category C satisfies the hypotheses of The weighted Reshetikhin–Turaev TQFT and modular-functor factorization, including its weighted-Lagrangian bordism convention and proved state-space, composition, and factorization maps. The weighted RT background interface for the present page means using those TQFT state spaces and bordism maps as a separate 2+1-dimensional mathematical background alongside the algebraic defect 2-category Mod⁡(C). The interface asserts no canonical functor from a module category, module functor, or module-natural transformation to a physical defect, and no classification of 3+1-dimensional phases.

Remarks

The actual supplier The weighted Reshetikhin–Turaev TQFT and modular-functor factorization now proves the full marked weighted-Lagrangian RT functor and geometric factorization, including presentation/coupon independence, exact cap normalization, signature–Maslov composition, cylinders, duality, disconnected and empty cases, and both sewing inverses. Its weight action is κ+n for the prescribed +μW composition, with the actual cap-reference correction for arbitrary real object Lagrangians. This establishes the background used in the Definition for every category satisfying the stated modular hypotheses. Full AC enters through the boundary duality/topology suppliers and countable choice through framed coupon evaluation. The algebraic Mod⁡(C) construction remains independently defined; no canonical physical realization or phase classification is inferred.

DefinitionDefinition: AI-adaptedProof: Not applicablejudge pass (gpt-6-luna)Open item page →

Separable algebra objects and bimodules in a fusion category

Definition

In a monoidal category C, an algebra object is an object A with multiplication mA:A⊗A→A and unit ηA:1→A satisfying associativity and unit equations with the associator and unitors of C. It is separable if there is an A-bimodule morphism σA:A→A⊗A with mAσA=1A. The composite eA=σAηA:1→A⊗A is its separability element. It satisfies mAeA=ηA and the centrality equation (mA⊗1A)∘(1A⊗eA)=(1A⊗mA)∘(eA⊗1A):A⟶A⊗A, with associators inserted. In element notation these are ∑ixiyi=1A and ∑iaxi⊗yi=∑ixi⊗yia.

A left A-module is an object M∈C with an associative unital action lM:A⊗M→M; a right A-module has an associative unital action rM:M⊗A→M. Write Mod⁡Cl(A) and Mod⁡Cr(A) for their categories and module morphisms. The category of left A-modules is a right C-module category by M⊙X:=M⊗X, with left A-action obtained by associating A⊗(M⊗X) to (A⊗M)⊗X and applying lM⊗1X, and the inherited associator and unitor. An A-B bimodule is an object X∈C with commuting left and right actions A⊗X→X and X⊗B→X, each associative and unital. A bimodule morphism preserves both actions.

The regular A-A bimodule is the object A with both actions given by mA.

Given an A-B bimodule X and a B-D bimodule Y, a morphism q:X⊗Y→Z is balanced over B if q∘(rX⊗1Y)=q∘(1X⊗lY):X⊗B⊗Y⟶Z. A relative tensor product X⊗BY, when it exists, is an object with a balanced map qB:X⊗Y→X⊗BY universal among balanced maps. Existence is not part of this definition.

DefinitionDefinition: AI-adaptedProof: Not applicablejudge pass (gpt-6-luna)Open item page →

Weak linear 2-category

Definition

Fix a field k. A weak linear 2-category B consists of a class of objects and, for each ordered pair (A,B), a k-linear category B(A,B). Its objects are called 1-morphisms and its morphisms are called 2-morphisms. Each triple A,B,C has a k-bilinear composition functor B(B,C)×B(A,B)⟶B(A,C),(g,f)⟼g∘f, and each A has an identity 1-morphism 1A∈B(A,A). A k-linear category here means that every hom set is a k-vector space and composition is bilinear.

For composable f:A→B, g:B→C, and h:C→D, there is a natural invertible 2-morphism ah,g,f:(h∘g)∘f⟹h∘(g∘f). For each f:A→B there are natural invertible unit 2-morphisms ℓf:1B∘f⟹f,rf:f∘1A⟹f. The associators satisfy the pentagon equation on every fourfold composite; the two unitors and associator satisfy the triangle equation on every pair of composable 1-morphisms. These equations are equalities of 2-morphisms between the indicated parallel 1-morphisms. Vertical composition is composition in each hom category. Horizontal composition is the displayed functor, so functoriality gives the interchange equation between horizontal and vertical composition.

When the associators and unitors are identities, this is a strict 2-category in the sense of Strict 2-category. No strictness is imposed in the weak definition.

Remarks

The source and target of every 2-morphism lie in one hom category. Associators change only the parentheses of a composable string; they do not change its endpoints. No monoidal product on the objects is part of this definition.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

The canonical algebra of a fusion category is Frobenius

Statement

Let C be a fusion category over an algebraically closed field. Write D=C⊠Crev, acting on C by (X⊠Y)⋅V=X⊗V⊗Y. Choose duals with ev⁡i:i⊗i∗→1 and coev⁡i:1→i∗⊗i. The canonical algebra K=End⁡‾D(1) is ⨁ii⊠i∗, with multiplication induced by composition of evaluations and unit the inclusion of the unit summand. Projection λ:K→1⊠1 to that summand makes β=λμ a nondegenerate pairing. Its inverse c:1→K⊗K defines a Frobenius comultiplication Δ=(μ⊗id)(id⊗c)=(id⊗μ)(c⊗id). This comultiplication is coassociative, is a K-bimodule morphism, and has counit λ, with λη=1. No nonvanishing dimension or pivotal structure is assumed.

Proof

Given: The action, duality convention, and field hypotheses in the statement. Associators and unitors are suppressed using coherence.

1.1givenconstructalgebra

The direct sum K represents (X,Y)↦Hom⁡C(X⊗Y,1) by semisimplicity and duality. Evaluation K⋅1→1 therefore induces a unit and multiplication by composition. To specify multiplication without an implicit diagram, choose split matrix units qar:r→i⊗j and par:i⊗j→r with parqbs=δrsδabidr and ∑r,aqarpar=idi⊗j. The (i,j)-to-r component of μ is ∑apar⊠(qar)∗. This expression is independent of matrix units. In either iterated triple multiplication the inserted sums of matrix units are identities, so both products are composition of the same three evaluations. This proves associativity; the unit is inclusion of the unit summand.

2.1step 1.1constructalgebra∎

The pairing β=λμ has no component between the i and j summands unless j is dual to i. For a dual pair, the displayed multiplication shows its component is the tensor product of a nonzero projection i⊗j→1 with the dual of its splitting 1→i⊗j. These are perfect evaluation pairings between dual simple objects, by rigidity. Hence every simple block of the induced map from K to its dual is invertible, proving nondegeneracy. Let c:1→K⊗K be its inverse pairing, so (β⊗id)(id⊗c)=idK=(id⊗β)(c⊗id). Associativity gives β(μ⊗id)=β(id⊗μ), and taking its mates gives Δ=(μ⊗id)(id⊗c)=(id⊗μ)(c⊗id). Taking mates once more gives (μ⊗id)(id⊗Δ)=Δμ=(id⊗μ)(Δ⊗id) and coassociativity; the inverse-pairing equations and β=λμ give (λ⊗id)Δ=id=(id⊗λ)Δ. These mate calculations are justified by composing with the perfect pairing; each resulting equality is respectively the associative triple product or one of the two inverse-pairing identities.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Surjective orbit tangents give finitely many open orbits

Statement

Assume the Axiom of Choice. Let k be algebraically closed of characteristic zero, let G be a finite product of general linear groups, and let X be a reduced affine variety of finite type with an algebraic G-action. If the differential of fx:G→X, g↦gx, is surjective onto TxX at the identity for every x∈X, then every orbit is open and there are finitely many orbits. Empty products and the empty variety are allowed.

Facts & Assumptions

Given: The field, group, variety and tangent-surjectivity hypothesis.

[F1]

Under AC, a morphism has constructible image, and a dense constructible subset of an irreducible variety contains a nonempty open (Chevalley: images of constructible sets are constructible, Dense constructible subsets contain an open).

[F2]

Under AC in characteristic zero, a dominant map of irreducible varieties has a surjective differential at some point mapping to the regular locus of the target (A dominant map has a surjective differential on a dense source open).

[F3]

Classical varieties are Noetherian with finitely many components; their open subsets are quasi-compact (Classical varieties have finite irreducible decompositions).

[F4]

At a closed point of a reduced finite-type variety the local dimension is the maximum of dimensions of its components through that point; the regularity criterion is equality of local dimension and tangent dimension (Local dimension for a reducible classical algebraic set, Jacobian rank detects regularity at closed points); local dimension is at most embedding dimension (dimension at most embedding dimension). Regular local rings are domains (regular local domain induction).

[F5]

A proper closed subvariety of an irreducible variety has strictly smaller dimension (Nonempty opens preserve irreducible dimension).

[F6]

AC is assumed because the classical algebraic geometry suppliers [F1]–[F5] carry that assumption (The Axiom of Choice).

Proof

1.1F1givenconstruct

Fix x and write O=Gx, Z=O‾ with reduced structure. The group G is irreducible: it is the principal open defined by the product of determinants in an affine space, whose polynomial coordinate ring is a domain. Its image and closure are therefore irreducible. By [F1] the orbit is constructible and contains a nonempty open U of Z. Every g∈G preserves Z, since it preserves O and is a homeomorphism. Transitivity gives O=⋃g∈GgU, so O is open in Z and consequently is a locally closed subvariety of X.

2.1F2step 1.1givenalgebra

The orbit map factors through Z: on an affine chart every function vanishing on Z pulls back to a function zero at every point of the reduced variety G, so it is zero. Apply [F2] to the dominant map G→Z. At some g its differential has rank dim⁡Z, since the image point is regular. The differential of the closed immersion Z↪X is injective, as the map on cotangent spaces is a quotient map. Thus dgfx, considered as mapping into TgxX, has rank dim⁡Z. The identity fx∘Lg=(g⋅−)∘fx shows that this rank is the same as the rank at the identity, since left translation and the action of g induce tangent isomorphisms. By the hypothesis it follows that dim⁡TxX=dim⁡Z.

3.1F4F5step 2.1algebra

Since x∈Z⊆X, local dimension obeys dim⁡Z≤dim⁡xX≤dim⁡TxX; the last inequality is the embedding-dimension bound in [F4]. Step 2.1 makes both inequalities equalities. Hence OX,x is regular and therefore a domain by [F4]. There is exactly one irreducible component C of X through x: distinct components through x give distinct minimal primes in this local ring, since localization at x preserves the prime-ideal inclusion correspondence. The irreducible closed subset Z lies in a component through x, hence in C, and has dim⁡Z=dim⁡xX=dim⁡C. By [F5] it follows that Z=C.

4.1F3F6step 1.1step 3.1construct∎

Remove from X the finitely many components other than C. This gives an open neighbourhood V of x contained in C. Since O is open in C by step 1.1, V∩O is an open neighbourhood of x in X contained in O. Translating this neighbourhood by elements of G proves that all of O is open in X. All orbits being open, they form a disjoint open cover of the Noetherian, hence quasi-compact, variety X. A finite subcover exists by [F3], and disjointness means it lists every nonempty orbit. The empty variety has no orbits; if G is the trivial group the argument says each point is open and quasi-compactness still gives finiteness. AC enters through [F1]–[F5], and no extra infinite choices are made.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

A separability element contracts the normalized categorical Hochschild complex in positive degrees

Statement

Let A be an algebra object in a k-linear monoidal category and B an A-bimodule. Suppose e:1→A⊗A satisfies μe=η,(μ⊗id)(id⊗e)=(id⊗μ)(e⊗id). Set Cn=Hom⁡(A⊗n,B), with the Hochschild differential given by the alternating sum of the left action, adjacent multiplications, and the right action. Its normalized subcomplex consists of maps vanishing whenever any input is the unit η. For every n≥1, define hn(f)=λB(idA⊗f)(e⊗idA⊗(n−1)), where λB denotes the left A-action. Then h preserves the normalized subcomplex and dh+hd=id in every positive degree.

Proof

Given: The two separability identities and the commuting left and right A-actions on B. We suppress coherent associators. The formal notation e=∑rxr⊗yr denotes a morphism composite; it does not assume that objects have elements.

1.1givenalgebra

Write the differential explicitly as (df)(a1,…,an+1)=a1f(a2,…,an+1)+∑j=1n(−1)jf(a1,…,ajaj+1,…,an+1)+(−1)n+1f(a1,…,an)an+1. Each pair of successive faces occurs twice with opposite signs in d2, by associativity of multiplication and the bimodule axioms; hence d2=0. At a unit input, the two faces adjoining that input cancel, and all other faces vanish for a normalized cochain. Thus normalization defines a subcomplex. The formula hnf=∑rxrf(yr,−) preserves normalization because every original input is still an input of f.

2.1givenstep 1.1algebra∎

For n≥1, expansion gives (hn+1df)(a1,…,an)=f(a1,…,an)−∑rxrf(yra1,a2,…,an)+∑j=1n−1(−1)j+1∑rxrf(yr,a1,…,ajaj+1,…,an)+(−1)n+1∑rxrf(yr,a1,…,an−1)an. The first term uses ∑rxryr=1. The other expansion is (dhnf)(a1,…,an)=∑ra1xrf(yr,a2,…,an)+∑j=1n−1(−1)j∑rxrf(yr,a1,…,ajaj+1,…,an)+(−1)n∑rxrf(yr,a1,…,an−1)an. Centrality of e identifies the first term of the second expansion with ∑rxrf(yra1,a2,…,an). All remaining terms cancel in pairs, proving hn+1d+dhn=idCn, including n=1 where the interior sums are empty. This identity restricts to the normalized subcomplex by the preceding step.

In degree zero the corresponding identity is h1d=id−P, where P(b)=∑rxrbyr projects onto the bimodule-invariant part. No degree-zero vanishing is asserted.

DefinitionDefinition: AI-adaptedProof: Not applicableOpen item page →

Finite semisimple 2-category

Definition

Let B be a weak linear 2-category. A monad on A in B is a 1-morphism T:A→A with 2-morphisms η:1A⇒T and μ:T∘T⇒T satisfying μ⋅(μ∗1T)=μ⋅(1T∗μ),μ⋅(η∗1T)=1T=μ⋅(1T∗η), where ⋅ is vertical composition, ∗ is horizontal composition, and the associator and unitors of B are inserted. Equivalently it is an algebra object in the monoidal endomorphism category B(A,A). This extends the ordinary-category definition in Monad on a category. It is separable if there is a 2-morphism σ:T⇒T∘T with μ⋅σ=1T,σ⋅μ=(μ∗1T)⋅(1T∗σ)=(1T∗μ)⋅(σ∗1T), again with coherent associators. The last two equalities say that σ is a map of regular T-bimodules.

An adjunction L⊣U in B, for L:A→B and U:B→A, consists of 2-morphisms η:1A⇒UL and ε:LU⇒1B with (ε∗1L)⋅(1L∗η)=1L,(1U∗ε)⋅(η∗1U)=1U, with associators and unitors inserted. These are the same triangle equations as in Adjunction by unit, counit, and the triangle identities, now for 1- and 2-morphisms of B. Its induced monad is (UL,η,1U∗ε∗1L).

A finite semisimple linear 2-category is a weak linear 2-category in which:

  • every hom category is a finite semisimple k-linear category (it has finitely many simple isomorphism classes, finite-dimensional hom spaces, and every object is a finite direct sum of simples);
  • there is a zero object, and each pair A,B has a biproduct A⊕B with inclusions and projections ιA,ιB,πA,πB satisfying πi∘ιj≅0 for i≠j, πi∘ιi≅1, and ιA∘πA⊕ιB∘πB≅1A⊕B; finite biproducts are preserved by composition;
  • every 1-morphism has both a left and a right adjoint (Adjunction by unit, counit, and the triangle identities), with unit and counit 2-morphisms satisfying the two triangle identities;
  • every separable monad has a separable splitting: a separable monad T:A→A is represented by an object AT and an adjunction L⊣U, where L:A→AT and U:AT→A, in the sense of Adjunction by unit, counit, and the triangle identities. Its induced monad UL is isomorphic to T as a monad, and its counit ε:LU⇒1AT has a section s:1AT⇒LU as a 2-morphism in B(AT,AT), with ε∘s=11AT (in a bimodule presentation this section is a bimodule map);
  • there are finitely many equivalence classes of simple objects, where an object A is simple when its identity 1-morphism is simple in B(A,A).

The splitting condition concerns monads in the 2-category; it is stronger than the existence of finite direct sums in each hom category. A choice of separable splitting is not part of the property.

DefinitionDefinition: Literature-sourcedProof: Not applicableOpen item page →

Relative Deligne product in the braided module 2-category

Definition

Let C be a braided fusion category and let M,N be finite semisimple right C-module categories. A relative Deligne product M⊠CN in Mod⁡(C) means a finite semisimple right C-module category P equipped with an exact bilinear functor b:M×N→P that is balanced over the middle C-action and compatible with the outer right C-action, and is universal among such functors: for every finite semisimple right C-module category D, composition with b gives an equivalence between right C-module functors P→D and exact bilinear middle-balanced right C-module functors M×N→D.

For the balancing convention, a right module category N is regarded as a left module category by X▹n:=n⊙X. Its left module associator (X⊗Y)▹n→X▹(Y▹n) is the composite of n⊙cY,X−1 with the inverse right-module associator. “Balanced” means that b(m⊙X,n)≅b(m,X▹n) naturally in all variables, compatibly with the unit and associativity constraints. This definition fixes the universal property and the braiding convention; it does not assert that a product exists.

DefinitionDefinition: Literature-sourcedProof: Not applicablejudge pass (gpt-6-luna)Open item page →

Weak monoidal 2-category

Definition

A weak monoidal 2-category is a weak 2-category B together with the following data.

  1. A bilinear tensor pseudofunctor ⊗:B×B→B. On 1- and 2-morphisms it has invertible comparison 2-morphisms for composition and identities, natural in each variable and satisfying the pseudofunctor composition and unit equations.
  2. A unit object I.
  3. Pseudonatural equivalences aA,B,C:(A⊗B)⊗C→A⊗(B⊗C) and ℓA:I⊗A→A, rA:A⊗I→A. A pseudonatural transformation has a 1-morphism component at every object and an invertible naturality 2-morphism for every 1-morphism; the naturality squares for composites and identities commute. A modification between pseudonatural transformations has a 2-morphism component at every object, and its naturality square for each 1-morphism commutes. “Equivalence” means that an inverse pseudonatural transformation and invertible unit and counit modifications are supplied.
  4. An invertible pentagonator modification ΠA,B,C,D from the composite aA,B,C⊗D∘aA⊗B,C,D to (1A⊗aB,C,D)∘aA,B⊗C,D∘(aA,B,C⊗1D). There are three invertible unit modifications, with sources and targets λA,B:ℓA⊗B∘aI,A,B⟹ℓA⊗1B, ρA,B:rA⊗B⟹(1A⊗rB)∘aA,B,I, τA,B:(1A⊗ℓB)∘aA,I,B⟹rA⊗1B.

All pseudofunctor comparison maps, transformations, and modifications are natural in their object, 1-morphism, and 2-morphism inputs. Their equations are part of the structure: the pentagonator obeys the five-object coherence equation (the two pastings between the endpoints of the 4-dimensional associahedron agree); the three unit modifications obey the triangle and double-unit equations; and inserting a unit in the five-object equation agrees with those unit equations. The tensor pseudofunctor comparisons satisfy their composition, unit, and naturality equations. These are equalities of parallel 2-morphisms; they are not consequences of object-level associativity.

The ordinary associator pentagon is represented schematically below. In a weak monoidal 2-category its two boundary composites are compared by Π, rather than required to be literally equal.

diagram failed to render:
& (A\otimes B)\otimes(C\otimes D) \arrow[rr,"a_{A,B,C\otimes D}"] & & A\otimes(B\otimes(C\otimes D)) \\
((A\otimes B)\otimes C)\otimes D \arrow[ur,"a_{A\otimes B,C,D}"] \arrow[dr,"a_{A,B,C}\otimes 1_D"'] & & & \\
& (A\otimes(B\otimes C))\otimes D \arrow[r,"a_{A,B\otimes C,D}"'] & A\otimes((B\otimes C)\otimes D) \arrow[ur,"1_A\otimes a_{B,C,D}"'] &

This definition uses the weak presentation directly. It invokes no global strictification theorem.

Semistrict presentation

A Gray-monoid presentation is an alternative set of specified data; no strictification assertion is needed here. Its underlying linear 2-category is strict. It has an object I, strict linear 2-functors LA=A□− and RA=−□A for every object A, and invertible 2-cells ϕf,g:(f□B′)∘(A□g)⟹(A′□g)∘(f□B) for f:A→A′ and g:B→B′. Write a dot for vertical composition, with the rightmost factor applied first, and ∘ for horizontal composition and whiskering. The complete semistrict equations are as follows.

  1. LAB=RBA, denoted A□B.
  2. LI=RI=id, LALB=LA□B, RBRA=RA□B, and LARB=RBLA, as equalities of 2-functors.
  3. ϕf,1B=1f□B and ϕ1A,g=1A□g.
  4. For composable f,f′ and g,g′, ϕf′∘f,g=(ϕf′,g∘(f□B))⋅((f′□B′)∘ϕf,g), ϕf,g′∘g=((A′□g′)∘ϕf,g)⋅(ϕf,g′∘(A□g)).
  5. For α:f⇒f′ and β:g⇒g′, ϕf′,g⋅((α□B′)∘(A□g))=((A′□g)∘(α□B))⋅ϕf,g, ϕf,g′⋅((f□B′)∘(A□β))=((A′□β)∘(f□B))⋅ϕf,g.
  6. ϕA□g,h=A□ϕg,h, ϕf□B,h=ϕf,B□h, and ϕf,g□C=ϕf,g□C.

Thus even in this semistrict presentation the two tensors of 1-morphisms are compared by the specified interchanger; it is not discarded. The weak presentation above is used directly for the module-category and graded-vector-space constructions on this page.

DefinitionDefinition: Literature-sourcedProof: Not applicablejudge pass (gpt-6-luna)Open item page →

Opposite algebra induced by a braiding

Definition

Let (C,⊗,1,c) be a braided monoidal category and let (A,m,η) be an algebra object (Separable algebra objects and bimodules in a fusion category). Define the monoidal opposite Cmp to have the same objects and morphisms, tensor product X⊗mpY:=Y⊗X, associator αX,Y,Zmp:=αZ,Y,X−1, and unitors λXmp:=ρX, ρXmp:=λX. The braiding defines a strong monoidal equivalence J:Cmp→C that is the identity on the underlying category and has tensorator cY,X−1:X⊗Y→Y⊗X.

Regard A as an algebra in Cmp with the same unit and multiplication m:A⊗mpA=A⊗A→A. Its transport along J is the opposite algebra Aop in C; its multiplication is mAop=m∘cA,A−1:A⊗A→A, and its unit is η. This convention fixes the braiding direction. The hexagon identities are the tensorator coherence of J, and its unit coherence follows from the braiding unit equations.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Canonical algebra modules and coherent tensor sliding

Statement

Use the canonical algebra K in D=C⊠Crev from The canonical algebra of a fusion category is Frobenius. Without a separability or characteristic-zero assumption, the functor J:C→Mod⁡D(K) given by J(V)=(V⊠1)⊗K is an equivalence. There are natural right K-module isomorphisms ρV:(V⊠1)K⟶(1⊠V)K. They obey ρ1=id and the sliding equation: ρV⊗W is the composite of idV⊠1⊗ρW, the interchange of the two separate Deligne factors, and id1⊠W⊗ρV. In particular any right K-linear map J(V)→J(W) uniquely equals f⊗idK for f:V→W.

Proof

Given: The canonical algebra and its multiplication from the cited Frobenius construction. Only finite semisimplicity and rigidity of C are used.

1.1givenconstructalgebra

Put LV=(V⊠1)K and RV=(1⊠V)K. For every X⊠Y, evaluation identifies both Hom⁡D(X⊠Y,LV) and Hom⁡D(X⊠Y,RV) with Hom⁡C(X⊗Y,V). Explicitly the first is ⨁iHom⁡(X,V⊗i)⊗Hom⁡(Y,i∗), evaluated by idV⊗ev⁡i, and the second is ⨁iHom⁡(X,i)⊗Hom⁡(Y,i∗⊗V), evaluated by ev⁡i⊗idV. Their inverses are the duality adjunction followed by the simple-object decomposition; the identity ∑qp=id verifies both inverse equations. Thus they are isomorphisms natural in X,Y,V. These two representations respect the right K-actions: the internal-Hom right action is composition with K on the source 1, and the free right action inserts exactly that further evaluation, by the definition of multiplication. Yoneda therefore gives a natural right K-linear isomorphism ρV:LV→RV identifying these two representations.

2.1step 1.1algebra

To check sliding, apply the preceding adjunction to an arbitrary map X⊠Y→((V⊗W)⊠1)K. The proposed iterated slide inserts one simple decomposition in the W adjunction and one in the V adjunction. Applying their evaluations erases both insertions by ∑qp=id, leaving the original map X⊗Y→V⊗W. The direct map ρV⊗W has the same image by its definition. The adjunction is injective and natural, so Yoneda proves the sliding identity. The unit identity follows by the same calculation with the identity unit constraints. The interchange in this identity is between different Deligne factors and requires no braiding on C.

3.1step 1.1step 2.1algebra

Free-module adjunction gives Hom⁡K(J(X),J(Y))=Hom⁡D(X⊠1,(Y⊠1)K)=Hom⁡C(X,Y): in the sum K=⨁ii⊠i∗ only i=1 contributes to the second equality. The resulting map sends f exactly to f⊗idK, proving full faithfulness. By sliding, every free module (X⊠Y)K is isomorphic to J(X⊗Y); additivity gives the same conclusion for a free module on any object of D.

4.1step 3.1constructalgebra∎

The category of right K-modules is abelian with kernels and cokernels computed in D: tensoring with K is exact, so these inherit unique actions and satisfy the module universal properties. Every module U has a finite free presentation: its action U⊗K→U is epic, since it is split in D by idU⊗η, and the same construction supplies a free epimorphism onto its kernel. By the preceding step the presenting free modules are J(X),J(Y); full faithfulness lifts the presenting map to f:X→Y. The functor J, whose underlying functor is tensoring with the fixed object K, is exact. Hence the presentation identifies U with J(coker⁡f). This proves essential surjectivity and the claimed equivalence without any separability assumption.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Right module internal ends and Eilenberg–Watts equivalence

Statement

Let C be a fusion category over an algebraically closed field k and M a finite semisimple right C-module category. There is an algebra A and a right module equivalence M≃Mod⁡Cl(A). This assertion does not yet assert separability. Fix the convention Hom⁡C(X,[m,n])=Hom⁡M(m⊙X,n). One can take A=[m,m] whenever m is a module generator, meaning every object of M is a quotient of m⊙X for some X∈C. In particular the direct sum of the simple representatives is such a generator. The multiplication is specified below. For any such algebras A,B, a right exact right module functor from left A-modules to left B-modules is uniquely, up to canonical isomorphism, P↦Q⊗AP for a B-A bimodule Q. The equivalence identifies module-natural transformations with bimodule maps. No braiding is assumed.

For a finite semisimple left C-module category and a generator m with every n a quotient of X⊙m, the left-action version is Hom⁡C(X,[m,n])=Hom⁡M(X⊙m,n) and n↦[m,n] is an equivalence to right modules over A=[m,m], with [m,X⊙n]≅X⊗[m,n]. This version likewise does not require or assert separability.

Facts & Assumptions

[F1]

The right module action and its associativity and unit equations are as in Finite semisimple module category over a fusion category. All functors in the statement are k-linear.

[F2]

Algebra objects, left modules and bimodules are as in Separable algebra objects and bimodules in a fusion category. Relative tensors below are cokernels of the difference of the two action maps; they exist in the finite semisimple abelian category C, whether or not the algebra is separable.

Proof

Given: C,M,m as stated. Parentheses in composites stand for the specified associators and action associators. Every comparison is constructed by the displayed adjunctions, so coherence is checked with those associators.

1.1F1construct

Write I for representatives of the simple objects of C. The object [m,n]=⨁i∈IHom⁡M(m⊙i,n)⊗ki represents the stated functor: the decomposition X=⨁iHom⁡(i,X)⊗i identifies both Hom spaces, naturally in X. Evaluation vn:m⊙[m,n]→n is the corresponding universal morphism. The adjunction T⊣R, T(X)=m⊙X, R(n)=[m,n], is thus explicit, and R is exact since each coefficient Hom⁡(m⊙i,−) is exact in a semisimple category. It is faithful by the generator hypothesis: if h:n→n′ is nonzero, precomposing with an epimorphism TX→n gives a nonzero map, and adjunction identifies its image under R as nonzero.

1.2F1F2construct

Let F:Mod⁡l(A)→Mod⁡l(B) be right exact and a right module functor, and put Q=F(A). It has its given left B-action. Apply F to the left A-linear map μ:A⊗A→A and use F(A⊗A)≅Q⊗A to obtain rQ:Q⊗A→Q. The algebra identities for μ and coherence of the module comparison give the right action identities for rQ; since F(μ) is a left B-map, the two actions commute. For a left A-module P, define Q⊗AP as the cokernel of rQ⊗1−1⊗lP on Q⊗A⊗P; the commuting left B-action descends. Tensoring and cokernels are right exact, so this is a right exact right module functor.

2.1step 1.1F1construct

For any X, choose its dual X∨ with evaluation X⊗X∨→1 and coevaluation 1→X∨⊗X. Rigidity gives natural bijections Hom⁡(Y,R(n⊙X))=Hom⁡(m⊙Y,n⊙X)=Hom⁡(m⊙(Y⊗X∨),n)=Hom⁡(Y,R(n)⊗X). Yoneda gives R(n⊙X)≅R(n)⊗X. Applying this construction successively to X,Y and applying it once to X⊗Y give the same bijection: the evaluation of a tensor product is the composite of the two evaluations in reverse order, and their units and counits satisfy the two zigzag identities. This proves the module pentagon for this comparison; evaluation against 1 proves its triangle. Evaluation and the adjunction unit are module-natural by the same representing bijections.

2.2step 1.2F2construct

The two maps A⊗A⊗U(P)⇉A⊗U(P), namely μ⊗1 and 1⊗lP, have coequalizer lP:A⊗U(P)→P in left A-modules. Indeed, if h equalizes them, its unique factor is h(η⊗1); the equalizing identity says both that this is left A-linear and that its composite with lP equals h. Since F is right exact, applying it preserves this coequalizer. Using F(A⊗X)≅Q⊗X, the resulting parallel maps are exactly rQ⊗1 and 1⊗lP. Thus their universal maps give a natural isomorphism Q⊗AP≅F(P). Its module compatibility follows on the free source from the module comparison of F, and follows on P by composing with the epimorphism from that free source.

3.1step 1.1step 2.1F2construct

Set A=R(m). Its unit η:1→A represents 1m and its multiplication μ:A⊗A→A represents m⊙(A⊗A)≅(m⊙A)⊙A→vm⊙1m⊙A→vmm. Associativity follows because both triple composites represent evaluation three times, with equality given by the module pentagon; the two unit identities represent evaluation with an identity inserted. In particular on Hom⁡(1,A)=End⁡(m) this multiplication is a⋅b=b∘a. The action A⊗R(n)→R(n) represents m⊙(A⊗R(n))→m⊙R(n)→n, first using vm, then vn. The same triple-evaluation computation proves that it is a left action. Equivalently it is the action of the monad RT=A⊗− obtained from the adjunction, so its associativity and unit also follow by applying the two adjunction triangles. The resulting comparison K:n↦R(n) is a right module functor to left A-modules; K(TX)=A⊗X with its free left action.

3.2step 1.2step 2.2construct

A module-natural transformation F→F′ evaluated at A is a B-A bimodule map: B-linearity is automatic and A-linearity follows by naturality at μ and module-naturality. Conversely a bimodule map Q→Q′ induces maps of the two coequalizer diagrams of step 2.2 and hence a module-natural transformation. Evaluation at A recovers it, using Q⊗AA≅Q by the action. Every transformation is determined by its component on A: the module constraint determines it on A⊗X, and naturality along the free epimorphism determines it on P. These operations are inverse and preserve identities and composition. This proves the full Eilenberg–Watts equivalence, with source algebra on the right of Q and target algebra on its left.

4.1step 3.1F2construct

Kernels and cokernels of maps of A-modules are their kernels and cokernels in C, with induced actions: tensoring by A is exact, hence preserves the defining kernel and cokernel diagrams. Thus the forgetful functor is exact and faithful. Every left module P has a free presentation A⊗Y→A⊗X→P→0: take the action A⊗U(P)→P, whose underlying map is split by η⊗1; its kernel is another module and is likewise the quotient of a free module. For a free source, the map on Hom spaces induced by K is the bijection Hom⁡A(A⊗X,Rn)=Hom⁡C(X,Rn)=Hom⁡M(TX,n).

5.1step 1.1step 3.1step 4.1construct

Every object of M is a quotient of T(X) by the module-generator hypothesis (for the sum of simples, take X to be a finite sum of units); applying the same argument to its kernel gives a presentation T(Y)→T(X)→n→0. Exactness of R sends it to a free presentation of K(n). Applying Hom⁡(−,n′) and Hom⁡A(−,K(n′)) identifies the two kernels of the maps out of the free terms by step 4.1. Hence K is fully faithful. Conversely, lift the first map of a free presentation of P uniquely to T(Y)→T(X) by step 4.1 and take its cokernel n in M. Exactness gives K(n)≅P. Thus K is the asserted right module equivalence. The zero category is included by taking m=0 and the zero algebra, whose unit identity holds on the zero object.

6.1step 2.1step 3.1step 5.1F1construct∎

To obtain the left-action version, view a left C-module as a right Crev-module by n◃X=X⊙n. The module pentagon is the same pentagon with the tensor inputs reversed, so all preceding constructions apply. An algebra in Crev gives an algebra A in C with the same underlying multiplication morphism A⊗A→A, reading tensor positions in the order of C; a left module over it in Crev is exactly a right A-module in C. Thus the fully faithful and essentially surjective comparison of step 5.1 becomes the stated equivalence to right modules, and the projection comparison of step 2.1 becomes [m,X⊙n]≅X⊗[m,n]. In this convention the internal-end multiplication represents A⊙(A⊙m)→A⊙m→m, and on ordinary endomorphisms is usual composition. In particular [m,X⊙m]≅X⊗A as right A-modules, with the free right action. No separability assertion entered any of these arguments.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

A uniform rank and action-multiplicity bound for module categories

Statement

For a fixed fusion category C over an algebraically closed field of characteristic zero, there is a finite integer R(C) such that every indecomposable finite semisimple right C-module category has at most R(C) isomorphism classes of simple objects. More explicitly, write I for its simple labels, 0 for the unit, and Nijk for its fusion coefficients. There are positive real numbers di=di∗, determined by these coefficients, with d0=1 and didj=∑kNijkdk. Put D=∑idi2. One may take R(C)=⌊D⌋. For every finite semisimple right module category, indecomposable or otherwise, the multiplicity naib=[ma⊙Xi:mb] satisfies naib≤D/di. Consequently there are finitely many possible action multiplicity arrays at any specified rank, and finitely many indecomposable arrays at all ranks.

The real numbers used here concern the fusion ring, and are not categorical traces. No pivotal structure or positivity of categorical dimensions is assumed.

Facts & Assumptions

Given: The category and module categories in the statement.

[F1]

Fusion categories are finite semisimple and rigid with simple unit (Fusion and multifusion categories).

[F2]

Right module categories have associative unital actions (Finite semisimple module category over a fusion category). Indecomposable means not a direct sum of two nonzero action-stable full semisimple subcategories.

Proof

1.1F1algebra

On the real vector space with orthonormal basis bi=[Xi], rigidity gives Frobenius reciprocity Nijk=Ni∗kj=Nkj∗i, and Nij0=δj,i∗. Indeed the adjunctions Hom⁡(Xi⊗Xj,Xk)≅Hom⁡(Xj,Xi∗⊗Xk) and Hom⁡(Xi⊗Xj,Xk)≅Hom⁡(Xi,Xk⊗Xj∗) give the first equalities by dimensions; simplicity of the unit gives the second. Left and right multiplication matrices Li,Ri therefore have transposes Li∗,Ri∗, respectively, and LiRj=RjLi by associativity. The matrix S=∑iLi is real symmetric and strictly positive entrywise: for any a,b, the nonzero object Xb⊗Xa∗ has a simple summand Xi, and reciprocity then gives Niab>0. The object is nonzero because tensoring by a nonzero rigid object is faithful: the unit is a summand of its dual times itself, so a zero tensor product would force the other factor to be zero.

2.1step 1.1algebra

Here is the required positive-matrix argument without an unproved Perron theorem. A real symmetric strictly positive matrix T has a largest eigenvalue λ by the finite-dimensional spectral theorem, equivalently the maximum of vtTv on the real unit sphere. Replacing a maximizing vector by its coordinatewise absolute value cannot decrease this expression; take a nonnegative maximizer v. The equation Tv=λv implies λ>0 and every coordinate of v is positive. Every maximizing vector has coordinates of one sign: if both signs occur, taking absolute values strictly increases its quadratic form because every cross entry is positive. Hence the top eigenspace is one-dimensional, for an independent top eigenvector could be chosen orthogonal to v and would necessarily have both signs. Apply this to S and normalize its positive top eigenvector v by v0=1.

3.1step 1.1step 2.1algebra

Since Ri commutes with S, Riv=div for a scalar di; it is positive because Ri is nonzero and nonnegative and v is strictly positive. Transposition and the scalar product give di⟨v,v⟩=⟨v,Riv⟩=⟨Ri∗v,v⟩=di∗⟨v,v⟩. The coefficient of b0 in vbi is vi∗, so di=vi∗=vi. Right multiplication by a product now gives didj=∑kNijkdk, and R0=1 gives d0=1. These numbers are fixed by the fusion data, since S and the normalization of its unique positive top eigenvector are fixed. Writing Ω=∑idibi=v, we have Ωbi=diΩ and therefore Ω2=DΩ for D=∑idi2.

4.1F1F2step 3.1algebra

For a module category let Ai have entry (b,a) equal to naib. Adjunction for the action, obtained by applying its associator to the evaluation and coevaluation of Xi, gives Hom⁡(ma⊙Xi,mb)≅Hom⁡(ma,mb⊙Xi∗), hence Ait=Ai∗. The matrices represent the fusion ring in the opposite order, which does not affect the equation for the square of a single element. Thus B=∑idiAi is symmetric, has nonnegative entries, satisfies B2=DB, and has diagonal entries at least one since A0=1. If the category is indecomposable, B is strictly positive: the undirected graph joining simples whenever some Ai has a positive connecting entry is connected, since its connected components are exactly action-stable summands. A path from a to b gives a positive entry in the product of its action matrices. Associativity expands that product as a nonnegative integer sum of the Ai, so some Ai already connects a to b.

5.1step 2.1step 3.1step 4.1algebra∎

Every eigenvalue of symmetric B is either 0 or D, by B2=DB. In the indecomposable case strict positivity and step 2.1 make its top eigenspace one-dimensional; since B≠0, its nonzero eigenvalue is D and it has rank one. Thus r≤tr⁡B=D, as each of its r diagonal entries is at least one. For the multiplicity bound in any module category, no indecomposability is needed: the same polynomial identity and symmetry show that the operator norm of B is D, so 0≤di(Ai)ba≤Bba≤D by applying the norm inequality to the unit coordinate vectors. Each entry is therefore a nonnegative integer bounded by D/di. At rank r there are only ∣I∣r2 entries and finitely many such arrays. For indecomposable arrays 1≤r≤⌊D⌋, so their union is finite. The empty category, if allowed, adds the single rank-zero array and is not indecomposable.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Module functor adjoints and separable-monad splittings in Mod(C)

Statement

Let C be a fusion category over an algebraically closed field of characteristic zero, and let M,N be finite semisimple right C-module categories. Every module functor F:M→N has left and right adjoints whose adjunction units and counits are module-natural. Every separable monad in the 2-category of finite semisimple C-module categories has a separable splitting in that 2-category.

Here a separable monad is (T,μ,η) with a module-natural section σ:T→T2 of μ satisfying Tμ∘σT=σ∘μ=μT∘Tσ. A separable splitting means an adjunction L⊣U inducing this monad whose counit admits a module-natural section.

Facts & Assumptions

[F1]

Right module categories and module functors have the specified associators, unitors and comparisons in Finite semisimple module category over a fusion category.

[F2]

Rigidity in Fusion and multifusion categories supplies evaluation and coevaluation maps satisfying both zigzag identities. For a finite semisimple k-linear category, write V⊗ka for a finite copower.

Proof

Given: C,M,N,F as stated, with comparison fm,X:F(m⊙X)→F(m)⊙X.

1.1F1F2construct

Choose representatives a of the finitely many simple objects of M. Put R(n)=⨁aHom⁡N(F(a),n)⊗ka and L(n)=⨁aHom⁡N(n,F(a))∗⊗ka. Since End⁡(a)=k, decomposition into these simples gives natural bijections Hom⁡M(m,Rn)=Hom⁡N(Fm,n) and Hom⁡M(Ln,m)=Hom⁡N(n,Fm). Define the units and counits to represent the identity maps under these bijections. The two triangle identities follow by applying either bijection: in each case the composite corresponds to the original identity. Thus these are actual ordinary adjunctions, with no exactness or representability assumption left implicit.

1.2F1construct

Let (T,μ,η,σ) be a separable monad on M. Define MT to consist of pairs (x,a) with a:Tx→x, aηx=1 and aT(a)=aμx; its arrows h:(x,a)→(y,b) obey ha=bT(h). The underlying additive functor T is exact because M is semisimple. Thus the kernel and cokernel of h carry induced T-actions, by exactness and the universal properties, satisfying the two algebra equations. They give the categorical kernel and cokernel in MT. The canonical comparison from coimage to image is the underlying isomorphism and preserves actions; its inverse preserves them as well. Therefore MT is abelian and the forgetful functor U is exact and faithful. Its free left adjoint is LT(x)=(Tx,μx), with unit ηx and counit at (x,a) equal to a. The two triangles are respectively μxTηx=1 and aηx=1.

2.1step 1.1F1F2construct

Fix a dual pair X,X∨ with evaluation X⊗X∨→1 and coevaluation 1→X∨⊗X. Define rn,X:R(n⊙X)→Rn⊙X by the following natural bijections in m: Hom⁡M(m,R(n⊙X))≅Hom⁡N(Fm,n⊙X)≅Hom⁡N(F(m⊙X∨),n)≅Hom⁡M(m⊙X∨,Rn)≅Hom⁡M(m,Rn⊙X). The middle identification uses fm,X∨ and the other identifications use the adjunction or the displayed duality. Every arrow is invertible, so Yoneda gives an invertible module comparison. To verify its pentagon, apply Hom⁡(m,−) to the two paths for X,Y. Both paths move Y∨ and then X∨ across Hom, apply f to the resulting action, then move them back. The equality of these composites is exactly the module pentagon for f, since evaluation of the dual of X⊗Y is the consecutive evaluation of Y and X with the associators. For X=1 the same comparison reduces to the module unit equation for f. This proves all module-functor axioms for R.

2.2step 1.2constructalgebra

For (x,a) put s(x,a)=T(a)σxηx:x→Tx. Its composite with a is aT(a)σxηx=aμxσxηx=aηx=1. It is an algebra map to (Tx,μx): indeed sa=T(a)σxηxa=T(a)σxT(a)ηTx=T(a)T2(a)σTxηTx=T(a)T(μx)σTxηTx=T(a)σxμxηTx=T(a)σx, while μxT(s)=μxT2(a)T(σx)T(ηx)=T(a)μTxT(σx)T(ηx)=T(a)σxμxT(ηx)=T(a)σx. Here the middle equalities use, in order, naturality, the algebra equation, the two bimodule equations for σ, and the unit equations. Naturality of s in algebra maps follows by the same naturality of σ,η and ha=bT(h). Thus every algebra is a natural retract of its free algebra.

3.1step 1.1step 2.1F1F2construct

Under the bijections of step 2.1, the image of the adjunction counit ϵn:FRn→n is its tensor translate, so the equality (ϵn⊙1X)fRn,XF(rn,X)=ϵn⊙X holds. This is precisely module-naturality of ϵ. For the unit, apply the adjunction bijection to its two proposed module-naturality composites; both correspond to the identity of F(m⊙X) after f and its inverse cancel. Faithfulness of the bijection proves their equality. Hence both triangles from step 1.1 are identities of module-natural transformations. For L, use the dual pair with evaluation X♭⊗X→1 and coevaluation 1→X⊗X♭ in the identical argument with the Hom adjunction reversed: Hom⁡(L(n⊙X),m)≅Hom⁡(n,Fm⊙X♭)≅Hom⁡(Ln,m⊙X♭)≅Hom⁡(Ln⊙X,m). Its middle comparison is that of F. Evaluation of tensor products gives the module pentagon, the unit pair gives its unit equation, and applying this bijection proves module-naturality of its unit and counit.

3.2step 1.2step 2.2construct

For each x, LT(x) is projective, since Hom⁡MT(LTx,−)=Hom⁡M(x,U−) is exact. Hence all objects are projective by step 2.2. Let g be the sum of the finitely many simples of M. Every object of MT is a quotient of a finite sum of copies of LTg: first its underlying object is a summand of a finite sum of copies of g, and then its action is an epimorphism from its free object. Also End⁡(LTg) is finite dimensional, being a subspace of an underlying Hom space in M. Every object has finite length, since a strict chain of subobjects remains a strict chain after the faithful exact functor U and U(x,a)=x has finite length. With all objects projective, all short exact sequences split, so each object is a finite sum of simples. Each simple is a summand of LTg because its quotient from a finite sum of LTg splits; the finite length of LTg bounds the number of such simples. Thus MT is finite semisimple with finite dimensional Hom spaces.

4.1step 1.2step 2.2step 3.2F1construct∎

Write tx,X:T(x⊙X)→Tx⊙X for the module comparison. Define (x,a)⊙X=(x⊙X,(a⊙1)tx,X). The fact that μ and η are module-natural proves its two algebra equations. The associativity and unit constraints inherited from M are algebra maps by the pentagon and unit equation for t, and obey their own pentagon and triangle because U is faithful. Thus MT is a finite semisimple right module category. The displayed action makes U a module functor, and t gives LT its module structure. Module-naturality of η,μ verifies the adjunction unit and counit. Module-naturality of σ,η and of the action a verifies that s from step 2.2 is module-natural as well. Consequently LT⊣U is a separable adjunction, induces exactly T with its multiplication and unit, and supplies the required splitting.

LemmaStatement: AI-adaptedProof: AI-adaptedOpen item page →

A separability idempotent constructs the balanced relative tensor product

Statement

Let C be a fusion category over an algebraically closed field k, let B be a separable algebra object, and let X be an A-B bimodule and Y a B-D bimodule. Put eB=σBηB:1→B⊗B. The endomorphism pX,Y=(rX⊗lY)∘(1X⊗eB⊗1Y):X⊗Y→X⊗Y is idempotent. Its image, with the induced map qB:X⊗Y→im⁡(pX,Y), is the relative tensor product X⊗BY: for every object Z, composition with qB gives a bijection from morphisms im⁡(pX,Y)→Z to maps X⊗Y→Z balanced over B. The result is independent up to a unique canonical isomorphism of the chosen splitting of pX,Y.

Facts & Assumptions

Given: A fusion category C over an algebraically closed field k, a separable algebra B, and bimodules X,Y as in the statement.

[F1]

Separable algebra objects and bimodules in a fusion category: The separability section is a B-B bimodule map and mBσB=1B; balanced maps equalize the right action on X and the left action on Y.

[F2]

Semisimple objects and semisimple abelian categories: Every object in a semisimple category is a finite direct sum of simple objects.

[F3]

Fusion and multifusion categories: A fusion category is a finite semisimple tensor category over the stated field.

[F4]

Simple object: A simple object is nonzero and has no subobjects other than zero and itself.

Proof

1.1F1given

Since σB is a bimodule map and mBσB=1B, the element eB=σBηB satisfies mBeB=ηB and the centrality equation ((mB⊗1B)∘(1B⊗eB))=((1B⊗mB)∘(eB⊗1B)):B→B⊗B. Associators are inserted in the displayed composite according to source and target. This equation says, in element notation, ∑ibxi⊗yi=∑ixi⊗yib for eB=∑ixi⊗yi.

2.1F1givenstep 1.1algebra

The centrality equation gives pX,Y(rX⊗1Y)=pX,Y(1X⊗lY): on an elementary tensor, both maps apply the equality ∑ibxi⊗yi=∑ixi⊗yib between the middle factors. Thus pX,Y is balanced. If f:X⊗Y→Z is balanced, then fpX,Y(x⊗y)=∑if(xxi⊗yiy)=∑if(x⊗xiyiy)=f(x⊗y), where the first equality is the definition of p, the second is balancing, and the third uses mBeB=ηB, the unit action on Y. This calculation is an equality of composites of action maps, so it does not depend on element notation. Taking f=pX,Y proves pX,Y2=pX,Y.

3.1F2F3F4step 2.1constructalgebra

Write X⊗Y as a finite direct sum of pairwise nonisomorphic simple objects using [F2]. A nonzero morphism between simple objects has kernel either zero or the whole source and image either zero or the whole target by [F4]; nonzero excludes the latter kernel and former image, so the morphism is an isomorphism. Thus distinct simple summands have zero Hom spaces, and End⁡(S) is a finite-dimensional division algebra over k. For any u∈End⁡(S), its minimal polynomial splits over the algebraically closed field k; the equation ∏j(u−λj1)=0 and absence of zero divisors imply u=λj1 for some root λj, so End⁡(S)=k. Therefore pX,Y is a finite block matrix of k-linear idempotents on the multiplicity spaces. For each such idempotent P:V→V, every v∈V is Pv+(v−Pv) with Pv∈im⁡P and v−Pv∈ker⁡P, while im⁡P∩ker⁡P=0; hence V=im⁡P⊕ker⁡P and P splits. Taking these splittings over all blocks gives X⊗Y→qBP→iX⊗Y with iqB=pX,Y and qBi=1P. Since pX,Y equalizes the two action maps, qB does too: apply the monomorphism i to the two composites from X⊗B⊗Y and use step 2.1. Hence qB is balanced.

4.1step 2.1step 3.1algebra

If f:X⊗Y→Z is any balanced map, step 2.1 gives fpX,Y=f. Therefore f~=fi:P→Z satisfies f~qB=fiqB=fpX,Y=f. It is unique because qBi=1P: any g:P→Z with gqB=f must satisfy g=gqBi=fi. Thus P has the balanced universal property.

5.1step 4.1algebra∎

Any other splitting of the same idempotent has the same universal property. The unique maps between the two representing objects that preserve their universal balanced maps are inverse, since each composite preserves that same universal map and uniqueness in step 4.1 forces it to be the identity. This proves canonical independence of the splitting.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Finite semisimplicity for separable algebra modules and bimodules

Statement

Let A,B be separable algebra objects in a fusion category C. The categories of left A-modules, right B-modules and A-B bimodules are finite semisimple. This assertion is valid in any characteristic in which the stated separability sections exist. In particular the left A-modules, with action P⊙X=P⊗X, form a finite semisimple right C-module category.

Facts & Assumptions

[F1]

The separability elements and their centrality equations, and all action conventions, are those of Separable algebra objects and bimodules in a fusion category. Tensoring in the fusion category is exact.

Proof

Given: A,B,C as stated; write eA=∑ixi⊗yi and eB=∑juj⊗vj as symbolic notation for the two separability morphisms, with no element interpretation assumed.

1.1F1construct

The kernel and cokernel of a bimodule map are their underlying kernel and cokernel in C, with induced actions: exactness of A⊗− and −⊗B gives these actions by the universal properties, and their algebra and commuting equations follow after composition with the monomorphism or epimorphism. Therefore the bimodule category is abelian, the forgetful functor is exact and faithful, and its Hom spaces are finite dimensional. The same reasoning applies with either action omitted.

1.2F1constructalgebra

For an underlying morphism t:P→Q between bimodules, define its left and right averages by L(t)(p)=∑ixit(yip) and R(t)(p)=∑jt(puj)vj. Each notation denotes the composite formed from eA or eB, the relevant actions and t. Centrality and associativity give L(t)(ap)=aL(t)(p) and R(t)(pb)=R(t)(p)b. For example ∑ixit(yiap)=∑iaxit(yip) is exactly the centrality equation precomposed with the action and postcomposed with t and the target action. The commuting bimodule actions show that L preserves right linearity and R preserves left linearity; they also give LR(t)=RL(t) by the common expression ∑i,jxit(yipuj)vj. If t respects the averaged action then the average equals t, using ∑xiyi=1 or ∑ujvj=1.

2.1step 1.1step 1.2construct

Given a bimodule epimorphism q:Q→P, choose a section t:P→Q in C, which exists by semisimplicity. Then s=LR(t) is a bimodule map and qs=LR(qt)=LR(1)=1. Thus all bimodule epis split. Every bimodule has finite length, since its strict subobject chains remain strict under the faithful exact forgetful functor and its underlying object has finite length. Splitting of epis then expresses every object as a finite sum of simples by induction on its length.

3.1step 1.1step 2.1F1construct∎

Let g be the sum of representatives of the finitely many simple objects of C. Every bimodule P is a quotient of a finite sum of copies of A⊗g⊗B. Indeed its underlying object is a summand of a finite sum of g; apply A⊗−⊗B to the resulting epimorphism and then apply both actions, whose composite is epi since it has an underlying section given by both units. Each simple bimodule is consequently a summand of a finite sum of A⊗g⊗B, hence a simple constituent of this finite-length object. There are finitely many. Omitting one action gives the same argument for one-sided modules, or use the separable unit algebra for that side. The right action on left modules preserves their action equations and inherits its pentagon and triangle from C. This proves all assertions.

TheoremStatement: Literature-sourcedProof: AI-adaptedOpen item page →

A braiding gives the tensor product algebra structure

Statement

Let C be a braided fusion category with braiding c, and let A,B be algebra objects. The object A⊗B is an algebra with unit ηA⊗ηB and multiplication mA⊗B=(mA⊗mB)∘(1A⊗cB,A⊗1B).

Facts & Assumptions

Given: A braided fusion category C with braiding c and algebra objects A,B.

[F1]

Braided monoidal category: The braiding is natural and invertible and satisfies both hexagon identities.

[F2]

Separable algebra objects and bimodules in a fusion category: An algebra object has multiplication and unit satisfying associativity and the two unit equations.

Proof

1.1F1F2given

The proposed multiplication first moves the middle B⊗A pair to A⊗B by cB,A and then applies mA and mB. With a unit input, naturality of the braiding with the unitors reduces the crossing to the identity, so the left and right unit composites are mA(ηA⊗1A)=1A and mB(ηB⊗1B)=1B, or their right-unit counterparts. Thus ηA⊗ηB is a unit.

2.1F1F2step 1.1algebra∎

On three tensor factors A⊗B⊗A⊗B⊗A⊗B, the left-associated product first crosses B1 past A2, then expands the crossing of B1⊗B2 past A3 into the crossings of B2 and B1 past A3. The right-associated product first crosses B2 past A3, then expands the crossing of B1 past A2⊗A3 into the crossings past A2 and A3. The two expansions use the two hexagons [F1]. The crossing of B1 past A2 and that of B2 past A3 involve disjoint tensor factors and commute by functoriality, so both composites perform the same three crossings in the same resulting order. They then apply respectively mA(mA⊗1A) and mB(mB⊗1B), or mA(1A⊗mA) and mB(1B⊗mB); these agree by the algebra associativity equations in [F2]. Hence mA⊗B is associative.

DefinitionDefinition: Literature-sourcedProof: Not applicablejudge pass (gpt-6-luna)Open item page →

Four-cocycle twisted monoidal structure on 2Vect_G

Definition

Let G be a finite group (Group and abelian group), with identity e. A normalized multiplicative 4-cochain is a function ω:G4→k× equal to 1 whenever any argument is e. It is a group 4-cocycle when, for all g,h,k,l,m∈G, ω(h,k,l,m)ω(g,hk,l,m)ω(g,h,k,lm)=ω(gh,k,l,m)ω(g,h,kl,m)ω(g,h,k,l).

On 2VectG, define the tensor product by convolution: (A⊗B)u=⨁gh=uAg⊠Bh, where ⊠ is the finite semisimple tensor product of linear categories. The unit is Vectk concentrated in degree e. The associator and unitors are the canonical rebracketing and unit equivalences. On four homogeneous inputs of degrees g,h,k,l, prescribe the pentagonator to be multiplication by the scalar ω(g,h,k,l) on every simple summand; extend it by direct sums and naturality. Denote this proposed weak monoidal 2-category structure by 2VectGω.

The scalar is central, so its naturality is componentwise. The displayed group equation is the exact coherence condition to be checked for five homogeneous inputs. This definition includes no braiding and no claim about classification of all fusion 2-categories.

DefinitionDefinition: AI-adaptedProof: Not applicableOpen item page →

Fusion 2-category

Definition

A fusion 2-category is a finite semisimple linear 2-category with a weak monoidal structure, a simple monoidal unit, and left and right duals for every object. For a right dual A# of A, the duality data include 1-morphisms eA:A⊗A#→I,iA:I→A#⊗A, and invertible cusp 2-morphisms from (eA⊗A)∘(A⊗iA) to 1A and from (A#⊗eA)∘(iA⊗A#) to 1A#, with the associator and unitors inserted at the indicated sources and targets.

For a left dual #A of A, the data separately include 1-morphisms eAℓ:#A⊗A→I,iAℓ:I→A⊗#A, and invertible cusp 2-morphisms from (A⊗eAℓ)∘(iAℓ⊗A) to 1A and from (eAℓ⊗#A)∘(#A⊗iAℓ) to 1#A. The associator and unitors are inserted at these sources and targets as well. No identification of the chosen left and right duals is required.

Here “simple unit” means that 1I is a simple 1-morphism. A pivotal or spherical enhancement is extra structure: it requires its own duality coherence and trace axioms. Neither such enhancement nor a spherical trace is included in “fusion 2-category.”

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

The braided tensor product of separable algebras is separable

Statement

Let C be a braided fusion category and let A,B be separable algebra objects, with bimodule sections σA,σB. Give A⊗B the braided tensor-product algebra structure from A braiding gives the tensor product algebra structure. A separability section is σA⊗B=(1A⊗cB,A−1⊗1B)∘(σA⊗σB):A⊗B⟶(A⊗B)⊗(A⊗B). This is an A⊗B-bimodule map and its composite with multiplication is the identity.

Facts & Assumptions

Given: A braided fusion category and separable algebras A,B with the chosen bimodule sections.

[F1]

Separable algebra objects and bimodules in a fusion category gives the two bimodule-section equations and the section identity.

[F2]

A braiding gives the tensor product algebra structure gives the positive braided tensor-product multiplication; naturality and both braiding hexagons hold.

Proof

1.1F1F2givenalgebra

Let D=C⊠C, whose objects needed here are pairs, with componentwise tensor. Define T(U,V)=U⊗V and strong tensorator t_{(U,V),(U',V')}=1_U⊗c_{V,U'}⊗1_{V'} : UVU'V'→UU'VV'.

1.2F1F2givenalgebra

The tensorator pentagon compares three such pairs. Expanding crossings past products by the two hexagons leaves crossings V1 past U2,U3 and V2 past U3; the two crossings on disjoint slots commute. Thus the two composites coincide. Unit coherence follows from the braiding unit equation. This proves T strong monoidal without a strictification theorem: insert the given associations and its pentagon throughout.

1.3F1F2givenalgebra

For R=(A,B), put mu=(m_A,m_B), s=(sigma_A,sigma_B). In D, mu s=id and s mu=(mu⊗id)(id⊗s)=(id⊗mu)(s⊗id), componentwise. Put K=T(R), m=T(mu)t, sigma=t^{-1}T(s). Naturality of t and its just-proved coherence transport the THREE equations to m sigma=id_K, sigma m=(m⊗id_K)(id_K⊗sigma), sigma m=(id_K⊗m)(sigma⊗id_K).

2.1F1F2givenalgebra∎

For clarity the first left-linearity transport starts with t^{-1} T(s mu)t; replace s mu by (mu⊗id)(id⊗s), use naturality to move T(s) to the last two inputs, and use the tensorator pentagon to replace the two intervening tensorators by (t⊗id)(id⊗t^{-1}). This is exactly (T(mu)t⊗id)(id⊗t^{-1}T(s)). The right-linearity calculation replaces s mu by (id⊗mu)(s⊗id) and gives (id⊗T(mu)t)(t^{-1}T(s)⊗id) in the same way. These are both linearity composites, not merely a multiplication/section cancellation. Expanding t gives exactly the candidate sigma=(1_A⊗c_{B,A}^{-1}⊗1_B)(sigma_A⊗sigma_B).

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Nonzero global dimension and the canonical Frobenius scalar

Statement

Let C be a fusion category over an algebraically closed field k of characteristic zero. Use left duals i∗ with ev⁡i:i⊗i∗→1 and coev⁡i:1→i∗⊗i. For each simple i, choose an isomorphism ai:i→i∗∗ and put di=ev⁡i∗(idi∗⊗ai)coev⁡i,ei=ev⁡i(ai−1⊗idi∗)coev⁡i∗,∣i∣2=diei. The scalar ∣i∣2 is independent of ai. The global dimension Dim⁡(C)=∑i∣i∣2 is nonzero. Over C, every ∣i∣2 is a strictly positive real number. For the canonical Frobenius algebra (K,μ,η,Δ,λ) of The canonical algebra of a fusion category is Frobenius, λμΔη=Dim⁡(C)≠0. No pivotal or unitary structure on C is assumed.

Facts & Assumptions

[F1]

The canonical Frobenius algebra and its explicit multiplication, perfect pairing β=λμ, inverse pairing c=Δη, and normalization λη=1 are supplied by The canonical algebra of a fusion category is Frobenius.

[F2]

The equivalence from the regular category to canonical-algebra modules and its coherent tensor-sliding maps, without assuming separability, are supplied by Canonical algebra modules and coherent tensor sliding.

Proof

Given: k,C as stated. Associators, tensor constraints of duality, and unitors in the following composites are the specified coherent ones. The symbol ∗ retains the statement's left-dual convention. For the cyclic-transpose construction only, write ∨ for right duality, with evaluation X∨⊗X→1 and coevaluation 1→X⊗X∨.

1.1givenalgebra

Left and right duals of a simple i are isomorphic. Indeed, rigidity identifies the unique simple j with Hom⁡(1,i⊗j)≠0 as one dual, and the unique simple j with Hom⁡(i⊗j,1)≠0 as the other; semisimplicity makes both dimensions the multiplicity of the unit in i⊗j, so these simple labels coincide. Thus i≅i∗∗. Each of the two loops defining di,ei is nonzero: it is a nonzero inclusion of the multiplicity-one unit summand in a product of dual simples followed by a nonzero projection to that summand. Multiplicity one follows from End⁡(i)=k and rigidity. Any two ai differ by a scalar t≠0; this multiplies di by t and ei by t−1. Hence ∣i∣2 is well-defined and nonzero.

1.2F1F2construct

Put D=C⊠Crev. The object 1∈C is a generator for its regular left D-module action, since (V⊠1)⋅1=V. By F2, H(V)=Hom⁡‾(1,V) is an equivalence from C to right K-modules. Rigidity and representability identify both LV=(V⊠1)K and RV=(1⊠V)K with H(V): applying Hom⁡D(X⊠Y,−) in each case gives Hom⁡C(X⊗Y,V), by moving V across the Hom using the appropriate dual. These identifications preserve the right action because both actions are composition of the representing evaluations. Thus J:V↦LV is fully faithful, and the identity on the represented Hom functor defines a right K-linear natural isomorphism ρV:LV→RV.

1.3F1constructalgebra

We prove the algebraic mate calculation needed to dualize sliding. In any rigid category, let A be a Frobenius algebra with b=ϵm, and let ℓ:A→A∨ be its perfect right-curried pairing, so b=ev⁡A(ℓ⊗id). Put F=(−)∨∨, q=(ℓ−1)∨ℓ:A→F(A) and bR=ev⁡A∨(idF(A)⊗ℓ). Then ℓ∨q=ℓ, hence bR(q⊗id)=b. For t:U⊗V→1 define its cyclic transpose, of source F(V)⊗U, by RU,V(t)=ev⁡V∨(idF(V)⊗[(t⊗idV∨)(idU⊗coev⁡V)]). The two snake identities make this operation invertible. Direct substitution proves naturality in U and the rule RU,W(t(idU⊗h))=RU,V(t)(F(h)⊗idU) for h:W→V. It also proves that two successive last-factor rotations equal rotation of their last-two-factor block: substitute the nested coevaluation formula for V⊗W and the reverse-order evaluation formula, obtaining the same nested composite.

2.1step 1.2F1construct

The sliding equation for ρ says that on (V⊠1)(W⊠1)K, sliding W and then V, commuting the distinct exterior factors between these operations, equals sliding V⊗W. To verify it without a diagram, apply Hom⁡D(X⊠Y,−) and the identifications of step 1.2. In either order the two adjunctions represent the same map X⊗Y→V⊗W. If intermediate simple decompositions are inserted, their inclusion/projection sum is ∑qapa=id, so erasing these sums gives the original map in both orders. The reverse-order tensor-dual evaluation is exactly the composite of the two evaluations, and the module associator equation identifies their parentheses. The unit case is evaluation against 1. Yoneda proves the sliding and unit equations.

2.2step 1.3algebra

Define τn(t)=RA⊗(n−1),A(t)(q⊗id) on Hom⁡(A⊗n,1), and set t3=b(m⊗id)=b(id⊗m). Using the first expression and naturality in the first argument gives τ3(t3)=bR(q⊗m)=b(id⊗m)=t3. Thus τ32(t3)=t3. On the other hand, the two-factor rotation rule gives τ32(t3)=RA,A⊗A(t3)(q⊗q⊗id). Using t3=b(id⊗m) and naturality in the last argument makes this bR(F(m)(q⊗q)⊗id). The nondegenerate pairing makes h↦bR(h⊗id) injective on Hom⁡(A⊗A,F(A)), and t3=bR(qm⊗id). Therefore qm=F(m)(q⊗q). Similarly rotating b(id⊗η)=ϵ=b(η⊗id) gives bR(F(η)⊗id)=bR(qη⊗id), so qη=F(η). Thus q is an algebra isomorphism. Every expression above is typed: both inputs to F(m) lie in F(A), and no product of an A input and an F(A) input is used.

2.3F1step 1.1construct

We compute the canonical Frobenius scalar directly, rather than using a trace characterization of δ. Fix a simple i and write j=i∗, transporting across a chosen representative isomorphism if necessary. With d=di,e=ei,a=ai, choose the following projections and sections of the unit summands: pij=ev⁡i,qij=(a−1⊗idi∗)coev⁡i∗/e,pji=ev⁡i∗(idi∗⊗a),qji=coev⁡i/d. Then pijqij=pjiqji=1. The explicit multiplication in F1 gives βij=pij⊠qij∗. Write the corresponding inverse-pairing component as cij=Aiqij⊠pij∗; this is its general form because the relevant two Hom spaces from the unit are one-dimensional. On Ki=i⊠i∗, the first exterior factor in (id⊗β)(c⊗id) is Ai(idi⊗pji)(qij⊗idi); the second is (qji∗⊗idi∗)(idi∗⊗pij∗), which is the left dual of (pij⊗idi)(idi⊗qji). No other summand contributes.

3.1step 1.2step 2.1step 2.2construct

Apply this construction to K∈D and its Frobenius pairing. The twice-right-dual of ρV is a map (F(V)⊠1)K∨∨→(1⊠F−1(V))K∨∨, because right duality in the reversed second factor is left duality in C. It is right K∨∨-linear by twice dualizing the action square. Transport through the algebra isomorphism q:K→K∨∨ gives a right K-linear map ρ~V:(F(V)⊠1)K→(1⊠F−1(V))K. Compose with ρF−1(V)−1. Full faithfulness of J gives a unique isomorphism δV:F(V)→F−1(V) whose image is this composite. The twice-dual sliding equation, transported through q, is the sliding equation for ρ~: internal q−1,q pairs cancel, and the multiplication and unit vertices agree by step 2.2. Combining it with the inverse sliding equation for ρ proves the tensor equation for δ; full faithfulness reflects it in C. Thus gV=δF(V)−1:V→F2(V) is a monoidal natural isomorphism.

4.1step 3.1constructalgebra

Monoidal natural isomorphisms of rigid tensor functors preserve duality. Here this follows directly by applying naturality and the monoidal equation for g to evaluation and coevaluation: the resulting two equations say that gX∨ is the inverse dual of gX, under the canonical dual constraints. Uniqueness of a dual mate follows from the snake identities, so gX∨=(gX∨)−1. Applying this twice gives gF(X)=F(gX). Define C~ to have objects (V,f) with f:V→F(V) invertible and F(f)f=gV, and arrows h with F(h)f=f′h. Tensor using f⊗f′ and the tensor constraint of F; monoidality of g proves closure. The inverse-dual identity just proved gives dual objects and their evaluation and coevaluation. The tautological map f:(V,f)→(F(V),F(f)) is an arrow, with its target an object by F(gV)=gF(V), and it is natural and monoidal. Hence it is a pivotal structure.

5.1step 1.1step 4.1constructalgebra

This cover is finite semisimple. Every simple i is F-stable by step 1.1. Choose bi:i→F(i); there is ci≠0 with F(bi)bi=cigi. Choose ti with ti2ci=1. There are exactly two simple lifts (i,±tibi). On any multiplicity space of i, an arbitrary lift has the form tibi⊗T, and its equation is T2=id. Characteristic zero gives the two projections (id±T)/2, so every lift is a direct sum of these two simple lifts. Their endomorphisms are k, and Hom between opposite lifts vanishes. There are exactly twice as many simple labels, the tensor unit has endomorphism ring k, and rigidity was proved in step 4.1. Thus C~ is a pivotal fusion category, and its forgetful tensor functor to C preserves every evaluation/coevaluation composite, hence squared norms.

6.1step 1.1step 5.1algebra

Over C, squared norms in any pivotal fusion category are strictly positive. Indeed let Di be the pivotal trace of a simple i; substituting tensor-product evaluations and coevaluations and the monoidal pivotal equation proves DiDj=∑rNijrDr, and duality gives ∣i∣2=DiDi∗. Let (Mi)j,r=Nijr and D=(Dj)j≠0, since D1=1. Then MiD=DiD. Rigidity gives Nijr=Ni∗rj, so Mi∗=Mit and MiMitD=∣i∣2D. Since Mi is real, ∣i∣2=D∗MiMitDD∗D=∥MitD∥2∥D∥2≥0. Step 1.1 excludes zero. A pivotal structure for right double duality also supplies one for left double duality by inversion and reindexing, so this calculation applies to the cover in step 5.1 with the statement's trace convention. Each simple of C lifts to a simple of the cover, and forgetting preserves its two trace loops. Thus ∣i∣2>0 in C and ∑i∣i∣2>0. No positivity or reality of Di was used.

7.1step 6.1constructalgebra

For arbitrary k, choose a finite skeletal presentation: simple labels, bases for their finite multiplicity spaces, matrices of associators, unitors, evaluations and coevaluations, their needed inverses, and the finitely many ai±1. Their entries generate a finitely generated characteristic-zero subfield k0⊂k. It embeds into C by choosing an algebraically independent complex image of a finite transcendence basis and extending the remaining finite algebraic extension. The split semisimple skeletal category over k0 with these matrices has the same simple labels and remains split semisimple after this embedding. Its pentagon, triangle and snake equations are finite matrix identities over k0, hence still hold. The two trace loops and their sum are elements of k0 given by these same matrix expressions. A zero sum in k would therefore give a zero sum in the complex fusion category, contradicting step 6.1. Hence Dim⁡(C)≠0.

8.1step 2.3step 7.1algebra∎

Substitution gives (idi⊗pji)(qij⊗idi)=e−1idi: its numerator is a−1(idi∗∗⊗ev⁡i∗)(coev⁡i∗⊗idi∗∗)a=idi by the snake identity. The other first-factor composite is (pij⊗idi)(idi⊗qji)=d−1idi, by (ev⁡i⊗idi)(idi⊗coev⁡i)=idi. The inverse-pairing equation is therefore Ai/(de)=1, so Ai=de=∣i∣2. Finally βijcij=Ai(pijqij)⊠(qij∗pij∗)=∣i∣2. Summing all simple blocks and using c=Δη gives λμΔη=βc=∑i∣i∣2, which is nonzero by step 7.1.

TheoremStatement: AI-adaptedProof: AI-adaptedOpen item page →

Relative tensor product gives associative composition of separable bimodules

Statement

For separable algebra objects in a finite semisimple monoidal category, take objects to be separable algebras, 1-morphisms A→B to be A-B bimodules, and 2-morphisms to be bimodule maps. Composition is X∘Y=X⊗BY with order fixed so X:A→B and Y:B→D compose as X⊗BY:A→D. This composition has canonical associators and unitors satisfying the bicategory pentagon and interchange equations; its units are the regular bimodules AAA.

Facts & Assumptions

Given: Separable algebras and bimodules as in Separable algebra objects and bimodules in a fusion category.

[F1]

A separability idempotent constructs the balanced relative tensor product constructs relative tensor products by a separability idempotent when the ambient category is fusion over an algebraically closed field. Step 1.1 below gives the construction under the present, more general hypotheses.

[F2]

Separable algebra objects and bimodules in a fusion category: Bimodule morphisms preserve the left and right actions, and the regular A-A bimodule has multiplication actions.

[F3]

Semisimple objects and semisimple abelian categories: The ambient category is abelian and semisimple. In an abelian category every idempotent p:V→V splits through its image: if p=iq with i monic and q epic, then p2=p implies qi=1.

Proof

1.1F1F2F3givenconstructalgebra

We prove the projector construction directly under the present hypotheses, extending the construction of [F1]. For each composable pair X:A→B, Y:B→D, set p=(rX⊗lY)(1X⊗eB⊗1Y) on X⊗Y, where eB=σBηB. Suppress coherent associators and write eB=∑ibi⊗ci only as notation for this morphism insertion. Centrality of eB gives p(xb,y)=p(x,by). Any balanced f satisfies fp(x,y)=∑if(xbi,ciy)=f(x,(∑ibici)y)=f(x,y) by mBeB=ηB. These are equalities of action-map composites, independent of elements. Taking f=p gives p2=p. Split p=iq through its image P using [F3], with qi=1P. The map q is balanced because i is monic and p is balanced. Every balanced f factors as (fi)q=f, uniquely since q is split epic. Commutativity of the outer A,D actions with the middle B actions makes p an outer bimodule endomorphism; the induced actions on its image satisfy their axioms after precomposition with the split epimorphism q and its tensor translates. Thus P=X⊗BY is an A-D bimodule with the required universal property, without rigidity, algebraic closedness or a simple tensor unit.

2.1step 1.1givenconstruct

Let X:A→B, Y:B→D, and Z:D→E. Both (X⊗BY)⊗DZ and X⊗B(Y⊗DZ) receive a map from X⊗Y⊗Z that is balanced in the B- and D-slots. Conversely, a map from X⊗Y⊗Z balanced in both slots factors uniquely through either parenthesization: first apply the universal property in step 1.1 to one slot, then to the other. Tensoring preserves its split epimorphic universal maps; the two balancing projectors commute because the two actions on Y commute. Hence either iterated factorization retains balancing in the other slot. The two iterated products therefore represent the same functor of the target object.

3.1step 2.1algebra

The representing property in step 2.1 gives a unique isomorphism aX,Y,Z:(X⊗BY)⊗DZ⟶X⊗B(Y⊗DZ) preserving the universal three-balanced map; applying the same property in reverse gives its inverse. For four composable bimodules, both composites around the pentagon preserve the same universal four-balanced map. Uniqueness therefore makes the two composites equal, which is the pentagon equation.

3.2F2step 1.1step 2.1algebra

The regular bimodule A is a left and right unit. The action maps A⊗AX→X and X⊗AA→X are balanced. Their inverses are induced by the algebra unit ηA and the relevant unitors. The action and unit laws show the two composites are identities; the triangle equation for these unitors follows because its two paths agree on the universal balanced map, so step 2.1 forces equality.

4.1step 1.1step 2.1step 3.1step 3.2algebra∎

Bimodule maps f:X→X′ and g:Y→Y′ induce the unique map f⊗Bg preserving the universal balanced map. For composable triples of bimodule maps, either horizontal-then-vertical or vertical-then-horizontal composition has the same composite with that universal map, since each is the ordinary composite of f,g on the tensor factors. Uniqueness from step 1.1 gives equality; this is interchange. Thus these data form the stated bicategory.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

The canonical algebra of a characteristic-zero fusion category is separable

Statement

Let C be a fusion category over an algebraically closed field of characteristic zero. For the canonical Frobenius algebra (K,μ,η,Δ,λ) constructed in The canonical algebra of a fusion category is Frobenius, set t=λμΔη. Then t≠0 and s=t−1Δ is a K-bimodule section of multiplication. In particular K is separable, and e=sη satisfies μe=η,(μ⊗id)(id⊗e)=(id⊗μ)(e⊗id).

Facts & Assumptions

[F1]

The canonical Frobenius algebra and its displayed bimodule identities are supplied by The canonical algebra of a fusion category is Frobenius.

[F2]

The squared-norm computation in Nonzero global dimension and the canonical Frobenius scalar identifies λμΔη with the nonzero global dimension of C; no pivotal structure is assumed.

Proof

Given: The Frobenius algebra and field hypotheses in the statement.

1.1F1givenalgebra

The bimodule equations imply that u=μΔ is a K-bimodule endomorphism and u=μ(id⊗uη). Because Hom⁡D(1,K)=kη, write uη=tη. Thus u=tidK; applying λ gives t=λμΔη since λη=1.

2.1F1F2step 1.1algebra∎

Fact [F2] gives t≠0. Therefore s=t−1Δ is a bimodule map and μs=idK. Its value e=sη obeys μe=η. Applying the left and right bimodule equations for s to the unit identifies (μ⊗id)(id⊗e) and (id⊗μ)(e⊗id) with s, proving centrality.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Object duals in the separable-algebra model of Mod(C)

Statement

For a separable algebra object A in a braided fusion category C, the object represented by A in the separable-algebra/bimodule monoidal 2-category has a left dual represented by the opposite algebra Aop of Opposite algebra induced by a braiding. There are evaluation Aop⊗A→1 and coevaluation 1→A⊗Aop bimodules, with invertible cusp 2-morphisms identifying both snake composites with the respective regular bimodules. It also has a right dual represented by the positive opposite algebra Aop,+ with multiplication mAcA,A; left and right opposites are not identified.

Facts & Assumptions

Given: A separable algebra A in a braided fusion category.

[F1]

Opposite algebra induced by a braiding fixes the negative opposite, and The braided tensor product of separable algebras is separable gives the admissible tensor-algebra objects.

[F2]

Relative tensor product gives associative composition of separable bimodules and Separable algebra objects and bimodules in a fusion category give the balanced universal products, split-epimorphic universal maps, action equations and unit equations.

Proof

1.1F1F2givenalgebra

Use the algebra-bimodule orientation: a 1-morphism R→S is an R-S bimodule, and composition is relative tensoring in the displayed order. For an R-S bimodule X and a T-U bimodule Y, their tensor X⊗Y is an (R⊗T)-(S⊗U) bimodule. Its left action is (lX⊗lY)(1R⊗cT,X⊗1Y) and its right action is (rX⊗rY)(1X⊗cY,S⊗1U); both shuffles are positive. These exact actions are used in each seven-strand calculation below. Write O=Aop with multiplication m c^-1. It is separable with section σO=cA,AσA: regard A and its section in the monoidal opposite, then transport through the strong monoidal functor of [F1]. Its tensorator is cY,X−1, so multiplication transports by c−1 and the section by c. The multiplication/section composite is mc−1cσA=1A. Both section-linearity diagrams transport by tensorator naturality and its inverse-hexagon coherence, precisely as the transport calculation in the tensor-separability lemma. Thus K=A⊗O and L=O⊗A are separable, both with positive braided tensor multiplication. All associations below are the canonical ones of C; the ordinary associator pentagon ensures the displayed expressions with brackets restored are equal. Denote the iterated multiplication of A by μ_r. For a permutation π let n_π mean its negative permutation braid: interchange adjacent U,V by c_{V,U}^{-1}: UV→VU, using any reduced expression for π. Independence of reduced expression follows from commuting disjoint crossings and the inverse braid relation, itself obtained by naturality and the two inverse hexagons. No symmetric-braiding relation is used. The construction supplies a left dual with e:O⊗A→1 and i:1→A⊗O. Take e to be underlying A with left action λ:L⊗A=(O⊗A)⊗A→A, and i to be underlying A with right action ρ:A⊗K=A⊗(A⊗O)→A. On these three underlying A factors their formulas, with coherent reassociation, are λ=μ3(1A⊗cA,A−1)(cA,A−1⊗1A) and ρ=μ3(cA,A−1⊗1A)(1A⊗cA,A−1). Thus λ moves the first (opposite) input through the last two inputs, whereas ρ moves the last (opposite) input through the first two. These are exactly the block inverse crossings cA⊗A,A−1 and cA,A⊗A−1 after reassociation, not crossings of the whole algebra L or K with the module.

1.2F1F2givenalgebra

Thus the opposite input moves to the far right in λ and to the far left in ρ. These actions are associative: expand the product of L or K, expand the two inverse crossings past products by the inverse hexagons, and use naturality to move crossings before multiplication. In each action equation the positive crossing in the tensor product algebra cancels the adjacent inverse crossing introduced by the opposite multiplication. What remains is the same negative permutation followed by μ_5. In ordinary word notation both sides for λ on (a,b,c,d,x) have word b d x c a, and both sides for ρ on (x,a,b,c,d) have word d b x a c; these words specify the resulting permutation, not an elementwise assumption about C. All residual crossings are negative and have precisely the inversions of these permutations. Units cancel by braiding naturality with η and the unit equations. This proves that the displayed maps really are bimodules. The first snake is (i⊗1_A)⊗_{A⊗O⊗A}(1_A⊗e). Its raw underlying tensor has four A slots (u,v;w,z). Define the cusp to the regular A-bimodule by P_A=μ_4 n_[2,4,1,3], that is u v w z→v u w z→v u z w→v z u w, all three interchanges negative. Its inverse is the composite A→A^4→snake inserting (η,1_A;η,η). Check balance on the seven slots (u,v,a,b,c,w,z): acting on the right of i⊗1_A or on the left of 1_A⊗e and then applying P_A both yield μ_7 n_[2,5,7,4,1,3,6], with resulting word v c z b u a w. To verify this equality, expand the tensor-bimodule action's positive shuffle, λ, ρ, and the opposite product, use naturality to move every crossing before μ, and cancel adjacent positive/inverse pairs. The remaining negative crossings are, respectively, the pairs (u,v),(u,b),(a,b),(u,c),(a,c),(b,c),(u,z),(a,z),(b,z),(w,z), exactly the ten inversions of the displayed permutation. Source and target A-linearity similarly reduce to the negative shuffles with words a v z u w and v z u w a; no crossing with the external action survives. Hence P_A descends to an A-A-bimodule map.

1.3F1F2givenalgebra

The two inverse equations are actual balanced-map equations. P_A after unit insertion is 1_A. Conversely, on q(u,v;w,z), transfer the first algebra slot w from the second bimodule through the balancing relation, then transfer the resulting first slot uw through the middle opposite algebra, then transfer the resulting second evaluation slot zuw through the last algebra. The outcome is q(1,vzuw;1,1). In C these three transfers mean exactly the three inverse crossings defining n_[2,4,1,3]; multiplication naturality and the unit identities supply the displayed word order. Thus q equals s_A P_A q; q is a split epimorphism by the separability-idempotent construction, so s_A P_A=id. This proves the first cusp is invertible, not merely a surjection on generators. The second snake is (1_O⊗i)⊗_{O⊗A⊗O}(e⊗1_O). On its raw four slots (u,v;w,z) define P_O=μ_4 n_[4,2,3,1], whose word is z v w u, with all five inversion crossings negative. The inverse inserts (η,η;η,1_A). On seven slots (u,v,b,c,d,w,z) both middle-action composites reduce to μ_7 n_[7,5,2,4,6,3,1], with word z d v c w b u. The sixteen remaining negative crossings are the inversions of that permutation: z crosses u,v,b,c,d,w; d crosses u,v,b,c; v crosses u; c crosses u,b; w crosses u,b; b crosses u (sixteen in total). The source and target O-actions reduce to μ_5 with the corresponding negative crossing from m_O, proving O-O-linearity. P_O s_O=id follows from units. For the reverse composite, use successively balance in the first O-slot, the central A-slot, and the last O-slot: the word representatives become (1,v;wu,z), (1,vwu;1,z), (1,1;1,zvwu). Restoring the negative crossings gives exactly n_[4,2,3,1]; hence s_O P_O q=q, and split epimorphy of q yields the inverse equation.

1.4F1F2givenalgebra

For the right dual put P=Aop,+ with multiplication mAcA,A. The same monoidal-opposite transport, now with positive tensorator, makes P separable with section cA,A−1σA. Define evaluation eR:A⊗P→1 on underlying A by the left action λR=μ3(1A⊗cA,A), and coevaluation iR:1→P⊗A by the right action ρR=μ3(cA,A⊗1A). Thus their words are axb on inputs (a,b,x) and bxa on inputs (x,b,a). Expanding either associative action equation gives the same positive permutation followed by μ5; the crossings are the inversions of the words acxdb and cbxad, respectively. This follows by the two positive hexagons and multiplication naturality, with the tensor-product positive shuffle and positive opposite multiplication retained. Unit coherence follows by naturality with ηA.

1.5F1F2givenalgebra

Write pπ for the positive permutation braid, using cU,V:UV→VU at each inversion. The first right snake (1A⊗iR)⊗A⊗P⊗A(eR⊗1A) has cusp μ4p[1,3,2,4], word uwvz, with inverse induced by (a,1;1,1). On the seven inputs (u,v,a,b,c,w,z) its two middle-action composites are the same positive permutation with word uawbvcz. The five remaining crossings are (v,a),(v,b),(v,w),(b,w),(c,w). Source and target linearity follow by cancelling the external action crossing against this shuffle; both act by ordinary multiplication on the outside of the word. The inverse equation follows by units in one direction; in the other direction the successive balance transfers give representatives (uw,v;1,z), (uw,vz;1,1), (uw,1;vz,1) and (uwvz,1;1,1). Each displayed transfer means the corresponding positive crossing in p[1,3,2,4], as follows by naturality before multiplication. Thus equality holds after the universal split epimorphism and proves the reverse inverse equation.

1.6F1F2givenalgebra

The second right snake (iR⊗1P)⊗P⊗A⊗P(1P⊗eR) has cusp μ4p[3,1,4,2], word wuzv, with inverse induced by (1,1;a,1). On seven inputs (u,v,b,c,d,w,z) both middle-action composites are the positive permutation with word wbuczdv. The remaining crossings are exactly its inversions: (u,b),(u,w),(v,b),(v,c),(v,d),(v,w),(v,z),(b,w),(c,w),(d,w),(d,z). The external source and target P actions contribute the positive crossings of mP, and the resulting composites on both sides have the same positive permutations; hence this cusp is P-P linear. The unit insertion is a right inverse. For the other inverse, balance successively in the first P, last P, central A, and first P slot, giving (1,v;wu,z), (1,1;wu,zv), (zv,1;wu,1) and (1,1;wuzv,1). Naturality restores precisely the positive crossings of the displayed shuffle. Equality after the universal split epimorphism proves that this cusp too is invertible.

2.1F1F2givenalgebra∎

The four displayed invertible cusp maps give a left and a right object dual with their stated orientations. Unit insertions and action maps commute with reassociation because both preserve the same universal balanced tensor. These are the required object-duality data and equations in the weak monoidal 2-category.

TheoremStatement: Literature-sourcedProof: AI-adaptedOpen item page →

A normalized group 4-cocycle gives a fusion 2-category 2Vect_G^omega

Statement

Let G be a finite group and let ω:G4→C× be a normalized group 4-cocycle. The convolution structure and scalar pentagonator of Four-cocycle twisted monoidal structure on 2Vect_G make 2VectGω a fusion 2-category. Its simple-object equivalence classes are exactly δg for g∈G, where δg is VectC concentrated in grade g. The monoidal unit δe is simple. Every 1-morphism has left and right adjoints, every separable monad splits, and every object has left and right duals.

Facts & Assumptions

Given: A finite group G, the field C, and a normalized multiplicative 4-cocycle ω, so ω(h,k,l,m)ω(g,hk,l,m)ω(g,h,k,lm)=ω(gh,k,l,m)ω(g,h,kl,m)ω(g,h,k,l).

[F1]

Four-cocycle twisted monoidal structure on 2Vect_G: On four homogeneous inputs of degrees (g,h,k,l), the pentagonator is scalar multiplication by ω(g,h,k,l) on each simple summand, extended by direct sums and naturality.

[F2]

G-graded finite semisimple 2-vector space: The concrete skeleton uses finite simple-label sets Sg and finite-dimensional vector-space families; linear functors are represented by finite matrices within each grade.

[F3]

Finite semisimple 2-category: Every hom category is finite semisimple, finite direct sums and zero exist, every 1-morphism has left and right adjoints, every separable monad splits, and there are finitely many simple-object equivalence classes.

[F4]

Fusion 2-category: A fusion 2-category is finite semisimple and weak monoidal, has a simple monoidal unit, and has left and right duals with evaluation, coevaluation, and cusp 2-isomorphisms.

[F5]

Group and abelian group: Group multiplication is associative and has an identity and inverses.

Proof

1.1F1F5given

For homogeneous inputs of grades g,h,k,l,m, the two composites of pentagonators have scalar coefficients ω(h,k,l,m)ω(g,hk,l,m)ω(g,h,k,lm)andω(gh,k,l,m)ω(g,h,kl,m)ω(g,h,k,l). They agree by the 4-cocycle equation in [F1]. On arbitrary objects both pastings are direct sums of these homogeneous components, and their naturality makes the componentwise equality an equality of modifications. Every coherence equation with a unit input reduces to the identity scalar by normalization in [F1].

1.2F2F3algebra

Let A,B have respectively ng,mg simple labels in grade g. A grading-preserving linear functor A→B is a family of matrices of finite-dimensional vector spaces, one mg-by-ng matrix for each g. Consequently its hom category is a finite product of finite matrix categories over VectC. Each matrix category is semisimple: its simple objects have one copy of C in a single matrix entry and zero elsewhere, and every matrix is a finite direct sum of these. Composition is matrix multiplication with direct sums and tensor products of finite-dimensional vector spaces. Object direct sums are concatenation of the finite simple-label sets. This proves the hom-category and direct-sum clauses of [F3].

1.3F2F3algebra

If F:A→B is represented by matrices Vji, define its right adjoint by the transposed matrices (FR)ij=Vji∗, where V∗ is the ordinary finite-dimensional vector-space dual; define its left adjoint using the opposite duality. The unit and counit are the direct sums of the vector-space coevaluation and evaluation maps. Each triangle composite is the identity on every matrix entry by the vector-space dual-basis identities, so these are left and right adjoints.

1.4F2F3algebra

Let S=⨆g∈GSg be the finite simple-label set of A≃VecS. A grading-preserving monad T has finite matrix entries Tt,s, zero unless s,t have the same grade. Its unit and multiplication satisfy the monad unit and associativity laws; these are exactly the identity and composition laws for the finite k-linear category with objects S and morphism spaces Tt,s. Its finite-dimensional category algebra RT=⨁s,t∈STt,s has unit the sum of the object identities, and a T-algebra is exactly a family (Ms)s∈S with compatible left RT-action maps Tt,s⊗Ms→Mt. The separability section σ:T⇒T2 gives E=ση(1)=∑ixi⊗yi∈RT⊗RT; the equations μσ=1T and T-bilinearity of σ say respectively ∑ixiyi=1RT and aE=Ea for every a∈RT, component by component. For a surjective homomorphism p:M→N of finite-dimensional left RT-modules, choose a k-linear section s and set sˉ(n)=∑ixi s(yin). Then psˉ(n)=∑ixiyin=n, while sˉ(an)=∑ixis(yian)=∑i(axi)s(yin)=asˉ(n) by Ea=aE. Thus every module epimorphism splits; every finite-dimensional module is a quotient of a finite direct sum of copies of the regular module, by choosing a finite vector-space generating set, so it is projective and the finite-dimensional module category is semisimple. Every simple module is a quotient of the regular module, which has finite length, so there are finitely many simple classes. Since RT has no entries between different grades, its central grade idempotents split this Eilenberg–Moore category into finitely many finite semisimple grade pieces. The free functor F sends X to (TX,μX) and is left adjoint to the forgetful functor U: the adjunction bijection sends an algebra map f:TX→M to fηX, with inverse g↦aM∘T(g) for a T-algebra action aM. The monad and algebra laws verify that these maps are inverse. Both functors preserve grades, and UF=T with unit η and multiplication μ. Hence the Eilenberg–Moore category and the adjunction F⊣U give the required separable-monad splitting in 2VectGω.

1.5F2F3step 1.4constructalgebra

For completeness the splitting has the required section of its counit. For a T-algebra (x,a) define s(x,a)=T(a)σxηx:x→Tx, as a map to the free algebra (Tx,μx). The algebra law and μσ=1 give as=aT(a)σxηx=aμxσxηx=aηx=1x. To check that s is an algebra map, naturality and the two T-bimodule equations for σ give sa=T(a)σxηxa=T(a)σxT(a)ηTx=T(a)T2(a)σTxηTx=T(a)T(μx)σTxηTx=T(a)σxμxηTx=T(a)σx,μxT(s)=μxT2(a)T(σx)T(ηx)=T(a)μTxT(σx)T(ηx)=T(a)σxμxT(ηx)=T(a)σx. Thus sa=μxT(s). For an algebra map h:(x,a)→(y,b), the identity ha=bT(h) and naturality of σ,η imply T(h)s(x,a)=s(y,b)h. Every component preserves grades, since T,a,σ,η do. Hence s:1⇒FU is a grading-preserving natural section of the counit FU⇒1, an actual 2-morphism in the Eilenberg–Moore endomorphism hom category required by [F3].

2.1F1F2F5step 1.1algebra

Tensoring linear functors on separate factors has the canonical comparison that sends an elementary tensor x⊗y to F(x)⊗G(y). The two sides of each interchange equation therefore agree on elementary tensors and hence on the entire tensor product. The scalar in [F1] commutes with every linear map, so the pentagonator is natural in 1- and 2-morphisms. Thus the prescribed operations satisfy the pseudofunctor and naturality parts of the weak monoidal 2-category definition.

2.2F2F3step 1.2algebra

The identity functor of a finite semisimple category with simple labels s1,…,sn is the direct sum of the n projection-inclusion functors for those labels. Each summand is simple, so the identity is simple exactly when n=1. The only simple objects of 2VectGω are therefore the one-label categories δg, one for each g∈G. In particular δe is the unique simple summand of the monoidal unit and is simple.

3.1F1F2F4step 1.1algebra∎

For an object with simple labels sg,i, put the dual label sg,i# in grade g−1. Evaluation sends (sg,i,sh,j#) to C when h=g and j=i, and to 0 otherwise; coevaluation sends C to the direct sum of sg,i#⊗sg,i over all labels. Each right-dual triangle composite is the identity on every simple label, since only its matching diagonal summand survives; reversing evaluation and coevaluation gives the same check for left duals. Thus both cusp transformations have scalar 1. These composites use only the associator and unitors on at most three object factors; the 4-cocycle enters the four-input pentagonator already checked in step 1.1, and normalized unit cases contribute scalar 1. This supplies duals without asserting a pivotal or spherical enhancement.

TheoremStatement: Literature-sourcedProof: AI-adaptedOpen item page →

A normalized 3-cochain gives the gauge equivalence of 2Vect_G^omega

Statement

Let ω,ω′ be normalized 4-cocycles on a finite group G, and let β:G3→C× be a normalized 3-cochain. Define δβ(g,h,k,l)=β(h,k,l)β(gh,k,l)−1β(g,hk,l)β(g,h,kl)−1β(g,h,k). If ω′=ω δβ, then the identity on the underlying graded 2-category, with identity tensor and unit constraints and triple-input coherence modification β(g,h,k), is a monoidal 2-equivalence 2VectGω≃2VectGω′. Here H4(G;C×) means normalized multiplicative 4-cocycles modulo coboundaries of normalized 3-cochains, with trivial G-action on C×. Within this identity-on-grading gauge family, an untwisting to ω′=1 exists exactly when [ω]=0 in this quotient.

Facts & Assumptions

Given: The structures in Four-cocycle twisted monoidal structure on 2Vect_G and a normalized 3-cochain β with ω′=ω δβ.

[F1]

Four-cocycle twisted monoidal structure on 2Vect_G: A normalized multiplicative 4-cochain is a function ω:G4→k× equal to 1 if any input is e, and it is a 4-cocycle when it satisfies the displayed five-variable equation.

Proof

1.1givenalgebra

The multiplicative coboundary on a normalized 3-cochain is the five-factor expression in the statement. Its coboundary is 1: writing δ=∏idi(−1)i, where d0 drops the first group element, d4 drops the last, and each interior di multiplies adjacent entries, the identities djdi=didj−1 for i<j pair every factor of δ2β with its inverse. The interior identities are exactly associativity in G. Hence ωδβ is a 4-cocycle whenever ω is. Normalization of β makes δβ equal to 1 if any input is e.

1.2F1givenconstruct

Define the underlying pseudofunctor to be the identity on objects, functors, and natural transformations; take its tensorator and unitator to be identity equivalences. For each triple of homogeneous input degrees (g,h,k), define its associativity coherence 2-cell to be multiplication by β(g,h,k). Extend to arbitrary objects by direct sums. Since scalar multiplication commutes with every linear map, these components are natural and define an invertible modification.

2.1F1givenstep 1.2algebra

On four homogeneous inputs, the monoidal 2-functor coherence equation compares the source pentagonator ω(g,h,k,l), the target pentagonator ω′(g,h,k,l), and the five triple-coherence components. Their ratio is β(h,k,l)β(gh,k,l)−1β(g,hk,l)β(g,h,kl)−1β(g,h,k)=δβ(g,h,k,l). Thus the coherence equation is precisely ω′=ω δβ. Normalization gives the unit equations, and the same scalar identity on homogeneous summands gives the equation on all direct sums. The underlying functor is the identity, hence an equivalence; its inverse uses β−1.

3.1F1step 2.1algebra∎

Conversely, in this gauge family the underlying functor, tensorator, and unitator are fixed as identities. Any normalized scalar triple-coherence modification is a normalized 3-cochain β, and its four-input coherence forces ω′/ω=δβ by step 2.1. Therefore ω can be untwisted by these data exactly when it is a coboundary, equivalently when [ω]=0. This makes no claim about equivalences that change the grading group or the underlying 2-category.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Categorical separability contracts the module deformation complex

Statement

Let C be a fusion category over an algebraically closed field of characteristic zero. For finite semisimple C-module categories, the normalized deformation complexes of a fixed module action and of a fixed module functor, defined below, admit an explicit homotopy satisfying dh+hd=id in every positive degree. In particular their degree-two cohomology vanishes.

Use left actions initially, writing MX and NX for the action functors on M and N. For a module functor T:M→N, use its comparisons γX:NXT→TMX. Set CTn=Nat⁡((X1,…,Xn)↦NX1⋯NXnT, (X1,…,Xn)↦TMX1⋯MXn). Here CT0=Nat⁡(T,T). The zeroth coface is (γX1MX2⋯MXn+1)(NX1fX2,…,Xn+1); the last coface is (fX1,…,XnMXn+1)(NX1⋯NXnγXn+1). The jth interior coface merges Xj,Xj+1 and transports f by the specified module associators. Their alternating sum, with signs (−1)j for 0≤j≤n+1, is d. Normalization means zero whenever any Xj=1, using the given unit comparisons. For T=idM these are the module-action deformation cochains. For a fixed general T they are the module-functor deformation cochains.

For the right-action convention of Finite semisimple module category over a fusion category, apply this definition to Crev and reverse the variable list: MX(m)=m⊙X, and the action comparison is MYMX→MX⊗Y. In particular degree two is the space of natural endomorphisms of (X,Y)↦MYMX, after transporting through the fixed action comparisons.

Facts & Assumptions

[F1]

The canonical algebra K=⨁ii⊠i∗ in C⊠Crev has a separability element e:1→K⊗K, by The canonical algebra of a characteristic-zero fusion category is separable. Here ev⁡i:i⊗i∗→1 fixes the duality convention. For split matrix units qar:r→i⊗j and par:i⊗j→r, its multiplication has components ∑apar⊠(qar)∗.

[F2]

The formula hnf=λB(id⊗f)(e⊗id) contracts the positive-degree normalized Hochschild complex of a separable algebra with arbitrary bimodule coefficients, by A separability element contracts the normalized categorical Hochschild complex in positive degrees.

Proof

Given: The categories, actions, functor, comparisons, and cochain complex in the statement. All natural transformations are natural in both the objects of C and the module-category variable.

1.1givenF1constructalgebra

Put E=Fun⁡k(M,N) and Q=End⁡k(N)⊠End⁡k(M)rev. The action (U⊠V)⋅S=USV makes E a Q-module category. These underlying categories are finite semisimple: after choosing their finitely many simple objects, linear functors and transformations are finite matrices of vector spaces and linear maps. The two action functors give a tensor functor C⊠Crev→Q. Let A be the image of K and eA the image of e; tensor functors preserve the two separability identities. The comparisons γ give an action ρT:A⋅T→T: on a simple summand it is the adjoint of γi:NiT→TMi, namely NiTMi∗→T. The product and unit equations for this action are exactly the module-functor equations, as one sees by inserting ∑qarpar=idi⊗j in the displayed multiplication of K.

2.1step 1.1constructalgebra

The object BT=End⁡‾Q(T) represents W↦Hom⁡E(W⋅T,T): explicitly, sum each simple object of Q with the multiplicity of the corresponding finite-dimensional Hom space. Composition of evaluations makes BT an algebra, and ρT corresponds to an algebra map A→BT. In particular BT is an A-bimodule. Internal-Hom adjunction and duality give isomorphisms Hom⁡Q(A⊗n,BT)≅Hom⁡E(A⊗n⋅T,T)≅CTn. For the last map, the summand indexed by (i1,…,in) is the adjunction Hom⁡E(Ni1⊗⋯⊗inTM(i1⊗⋯⊗in)∗,T)≅Hom⁡E(Ni1⊗⋯⊗inT,TMi1⊗⋯⊗in). The module associators identify tensor-word actions with the iterated actions in the statement. Values on simple tuples extend uniquely to natural transformations because every object is a finite direct sum of simples. Thus these maps are isomorphisms, not just injections into the cochain spaces.

3.1F1step 1.1step 2.1algebra

Under these isomorphisms the two outer Hochschild faces compose with ρT on the two sides; taking their adjoints gives precisely the zeroth and last cofaces displayed in the statement. For an interior face, the component ∑apar⊠(qar)∗ of multiplication inserts ∑r,aqarpar=id in the adjacent tensor factors; its adjoint is the merge coface, transported by the module associators. The unit of A is the image of the unit summand of K, so the normalized conditions also agree. Consequently the maps in the preceding step identify the stated normalized complex with the normalized Hochschild complex of A with coefficients BT. This also proves d2=0 for the stated differential.

4.1F2step 3.1constructalgebra∎

Denote this complex isomorphism by Φn:CTn→Hom⁡Q(A⊗n,BT). For n≥1 define the required homotopy by hn(f)=Φn−1−1(λBT(idA⊗Φn(f))(eA⊗idA⊗(n−1))). All maps in this formula have been specified in the preceding steps. Fact [F2] and the complex isomorphism give dhn+hn+1d=idCTn and preservation of normalization. The same proof with T=idM gives the action complex; replacing C by its tensor reversal gives the prescribed right-action convention. Thus every positive-degree cocycle is a coboundary, in particular every degree-two cocycle.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Module-functor categories are finite semisimple

Statement

For finite semisimple right C-module categories M,N over a fusion category over an algebraically closed field k of characteristic zero, the category Fun⁡C(M,N) of module functors and module-natural transformations is finite semisimple. In addition, evaluation at the tensor unit identifies Fun⁡C(C,C) with C and sends the identity module functor to 1C; hence the unit object of the monoidal 2-category is simple. Here “finite semisimple” means a k-linear abelian category with finitely many simple isomorphism classes, finite dimensional Hom spaces, and every object a finite direct sum of simples.

Facts & Assumptions

[F1]

By The canonical algebra of a characteristic-zero fusion category is separable, the canonical algebra K=⨁ii⊠i∨ in D=C⊠Crev is separable. Here i∨ has evaluation i⊗i∨→1. Its multiplication on (i⊗j)⊠(j∨⊗i∨) is the sum of f⊠g∨ over simple k and dual splitting maps f:i⊗j→k, g:k→i⊗j, with fg=1k for matching basis indices. Its separability element e:1→K⊗K satisfies μe=η and the centrality equation.

[F2]

Right actions, module comparisons and transformations are as in Finite semisimple module category over a fusion category. Reconstruction and the correctly oriented Eilenberg–Watts equivalence, without any separability hypothesis, are proved in Right module internal ends and Eilenberg–Watts equivalence.

Proof

Given: C,M,N as stated. Write RXM(m)=m⊙X and similarly for N; all products below retain the given associators.

1.1F1F2construct

The ordinary linear functor category E=Fun⁡k(M,N) is finite semisimple: evaluation on representatives ma of the simples of M, followed by decomposition in simples nb of N, identifies it with the category of finite matrices of vector spaces Vba=Hom⁡(nb,F(ma)). A natural transformation is exactly a matrix of linear maps; conversely the matrix defines the functor by additive extension. The category D acts on E by (X⊠Y)⋅F=RYNFRXM. Indeed RYRW=RW⊗Y and RZRX=RX⊗Z, giving the product (X⊗Z)⊠(W⊗Y) in D. The action coherence follows by applying the two module pentagons; its two unit equations are the two module triangles. Thus K⋅− is an exact linear monad on E with multiplication induced by that of K.

2.1step 1.1F1F2construct

A left K-action on F consists of components θi,m:F(m⊙i)⊙i∨→F(m). By duality these correspond bijectively to cm,i:F(m⊙i)→F(m)⊙i; the inverse correspondence is θi,m=(1⊙ev⁡i)(cm,i⊙1). Finite semisimplicity extends these maps uniquely and naturally from simple i to every X: decompose X into simples, use additivity on the source, and the dual decomposition on the dual factor. Independence of bases follows from the identity ∑agafa=1X for dual inclusion/projection maps. Expanding θ(μ⋅1)=θ(1⋅θ) on the (i,j) summand and using the formula for μ in F1 gives, after taking mates, cm,i⊗j=(cm,i⊙1j)cm⊙i,j with the module associators inserted: the sum over f,g inserts exactly ∑gf=1i⊗j. The unit action equation gives cm,1=1 under the unitors. Conversely those two equations give the action equation on every summand of K⊗K, hence on the full direct sum.

3.1step 2.1F2construct

These initially lax comparisons are invertible by rigidity. Choose a dual X♭ with b:1→X⊗X♭ and d:X♭⊗X→1. An inverse to cm,X is the composite F(m)⊙X→F(1m⊙b)⊙1XF(m⊙X⊙X♭)⊙X→cm⊙X,X♭⊙1XF(m⊙X)⊙X♭⊙X→1⊙dF(m⊙X). For its composite after cm,X, naturality with b, followed by the product equation of step 2.1, leaves the zigzag (1X⊗d)(b⊗1X)=1X. For the composite before cm,X use naturality with d and the same product equation; the other zigzag and the unit equation leave 1F(m⊙X). A map of K-actions is exactly a natural transformation commuting with all θi, equivalently all cX. Thus the category of K-modules in E is precisely Fun⁡C(M,N), including its morphisms.

4.1step 1.1step 3.1F1constructalgebra

Kernels and cokernels of K-module maps exist and are their underlying kernels and cokernels in E, since K⋅− is exact. They carry the induced actions by the universal properties. For modules (P,ρP),(Q,ρQ) and an arbitrary underlying arrow t:P→Q, put Av⁡(t)=ρQ(1K⋅t)(1K⋅ρP)(e⋅1P). In symbolic notation for this composite it is Av⁡(t)(p)=∑axat(yap), where e=∑axa⊗ya denotes the morphism e, not actual elements. Centrality says ∑bxa⊗ya=∑xa⊗yab, so associativity of the actions gives Av⁡(t)(bp)=bAv⁡(t)(p) as an equality of the corresponding composites. Thus it is a module map. If t already is a module map, the identity μe=η gives Av⁡(t)=t. If q:Q→P is a module epimorphism and qt=1P, the same formula gives qAv⁡(t)=Av⁡(qt)=1P. Every underlying epi splits in E, so all module epis split.

5.1step 3.1step 4.1F2construct

Hom spaces of modules are finite dimensional subspaces of those in E. Every module has finite length, since its subobject chains give strict subobject chains in its underlying object of E. Therefore the splitting in step 4.1 implies that every module is a finite direct sum of simples. To prove finiteness of the simple set, let g be the sum of the finitely many simples of E. The free module K⋅g has finite length. Every module is a quotient of a finite sum of copies of K⋅g: its underlying object is a summand of a finite sum of copies of g, apply the free functor and then the action epimorphism. Each simple is therefore a summand of a finite sum of K⋅g and hence is isomorphic to a simple constituent of K⋅g. There are only finitely many. Steps 3.1–5.1 prove the finite semisimplicity assertion. Under F2 this also proves it for the correctly oriented bimodule categories, without assuming separability of their representing algebras in advance.

6.1F2construct∎

A right module endofunctor F of the regular category satisfies F(X)=F(1⊗X)≅F(1)⊗X, naturally and compatibly with its comparison. Conversely a↦(a⊗−) is a right module functor, with the associator as comparison. The same comparison shows that any module-natural transformation is h⊗1 for its component h at 1, and every h defines one. Thus evaluation at 1 and a↦(a⊗−) are inverse equivalences. The identity functor corresponds to 1, whose endomorphism algebra is k. Hence the identity 1-morphism of the regular module is simple, which is the asserted simple-unit condition.

Remarks

Characteristic zero is essential to the unrestricted statement. If k has characteristic p and G=Z/p, the pointed category Vec⁡G is fusion and Vec⁡ is its one-simple module category via forgetting the grading. Module endofunctors of Vec⁡ are vector spaces V with coherent automorphisms indexed by G, hence form Rep⁡k(G). The algebra kG=k[t]/((t−1)p) is not semisimple, so this functor category is not semisimple. The corrected field scope is the characteristic-zero scope approved for PA-48.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Bounded-rank module-structure varieties have finitely many open orbits

Statement

Assume the Axiom of Choice. Fix a fusion category C over an algebraically closed field k of characteristic zero. For each fixed possible rank of a finite semisimple right C-module category, its module structures are represented, after choosing action multiplicities, by a finite union of affine varieties of finite type. The change-of-basis group on each such variety has finitely many orbits, each open, if the degree-two normalized action-deformation cohomology vanishes at every point. This vanishing is supplied by Categorical separability contracts the module deformation complex. Orbits on a fixed labelled action skeleton are equivalence classes of its normalized module structures with that labelling; forgetting labels can only identify further classes. There are consequently finitely many module categories of any fixed rank and finitely many indecomposable finite semisimple module categories up to module equivalence.

The finite union over action multiplicity arrays is essential: rank alone does not specify an action functor. No algebra classification or categorical trace positivity is assumed.

Facts & Assumptions

Given: The field, fusion category and specified rank, and AC for the algebraic geometry suppliers.

[F1]

Module categories, their action comparisons, and module equivalence are as in Finite semisimple module category over a fusion category.

[F2]

For fixed fusion data, action multiplicities satisfy the uniform bound naib≤D/di, and an indecomposable module category has rank at most ⌊D⌋ (A uniform rank and action-multiplicity bound for module categories).

[F3]

For F:Crev→End⁡k(M) associated to a right action, the normalized tensor-functor complex has Cn=Nat⁡(F(Xn)⋯F(X1),F(Xn)⋯F(X1)) in right-action order. Its differential consists of the two outside whiskerings and the alternating adjacent tensor mergers, transported by the action comparison, and H2=0 (Categorical separability contracts the module deformation complex). Reversing the displayed variable order gives the standard tensor-functor order used below.

[F4]

A finite product of general linear groups acting on a reduced affine finite-type variety with surjective orbit differentials at every point has finitely many open orbits (Surjective orbit tangents give finitely many open orbits).

[F5]

The Axiom of Choice is used through [F4] and its algebraic geometry suppliers (The Axiom of Choice).

Proof

1.1F1F2givenconstruct

Write Vr=Vec⁡kr with labelled simples m1,…,mr. Every finite semisimple k-linear category of rank r is equivalent to it: the functor m↦(Hom⁡(ma,m))a has inverse (Wa)↦⨁aWa⊗ma. The evaluation map is an isomorphism by semisimplicity and End⁡(ma)=k; the latter follows since any element of a finite-dimensional division algebra over algebraically closed k has an eigenvalue, so subtracting it gives a noninvertible element and hence zero. A bilinear action functor is, up to natural isomorphism, determined by the finite-dimensional multiplicity spaces Vaib=Hom⁡(mb,ma⊙Xi): on general objects and morphisms it is the direct sum of their tensor products with these spaces. Thus, after finite basis choices, it has the standard skeleton Vaib=knaib. By [F2] only finitely many arrays can occur at rank r. Discard arrays violating na0b=δab or the integer module fusion equations; arrays satisfying those equations but having no coherent constraints simply give empty parameter varieties.

2.1F1step 1.1construct

Fix one such array and fixed bases of Hijk=Hom⁡(Xk,Xi⊗Xj) in C. Use its given associator and unitors as fixed matrices. The action is equivalently a strong tensor functor F:D→End⁡k(Vr), where D=Crev has X⋆Y=Y⊗X and the target has tensor product composition. Its underlying linear functor sends X to FX:m↦m⊙X. Its constraints are JX,Y:FXFY→FX⋆Y, the original right action comparisons with inputs reversed. At simple inputs Xi,Xj and ma, its block at mb is an invertible matrix between the fixed spaces ⨁cVajc⊗Vcib and ⨁kHjik⊗Vakb. Their dimensions agree by the module fusion equations. Naturality determines J on all objects from these blocks: on direct sums it is blockwise this map, with the identity on external multiplicity spaces. This also proves that there are no additional unconstrained naturality variables.

3.1F1step 2.1construct

Normalize F1=id⁡ and its unit comparison to the identity; then J1,X and JX,1 are the fixed maps induced by the source unitors. This loses no structures: identify F1 with the identity by the given action unitor, transport all J through that identification, and the module triangle forces the two stated values. This changes no associator of C and invokes no strictification theorem. Introduce the entries of every remaining simple-pair block J and an additional scalar tJ with equation tJdet⁡J=1. Impose the functor-associativity equations F(aX,Y,ZD)JX⋆Y,Z(JX,Y∗1)=JX,Y⋆Z(1∗JY,Z) for simple triples, and the fixed unit equations; here ∗ means whiskering/horizontal composition of natural transformations. Each side is a matrix with entries polynomial in the finitely many variables, because direct-sum extensions and the matrices of aD are fixed. A zero-dimensional block is omitted with its unique invertible map. These equations define an affine finite-type scheme Sn; its reduced variety Xn has exactly the coherent normalized module structures as k-points. Checking triples of simples suffices by the direct-sum naturality of step 2.1. This constructs the asserted parameter variety, including the inverse determinants rather than treating invertibility as a closed equation without localization.

4.1F1step 1.1step 3.1constructalgebra

The normalized natural automorphism group of the underlying F is Gn=∏i≠0,a,bGL⁡(Vaib); omit zero spaces. Its elements gX extend to arbitrary objects by naturality, with g1=1, and act by JX,Yg=gX⋆YJX,Y(gX−1∗gY−1). This is algebraic, since inverse matrices are regular on general linear groups. It preserves the equations: inserting the formula in either side of the associativity equation cancels intermediate g−1g, leaving the old equation precomposed by gX−1∗gY−1∗gZ−1 and postcomposed by gX⋆(Y⋆Z); naturality moves g through F(aD). It preserves the normalized unit maps because g1=1. Two points in the same orbit are isomorphic tensor structures, equivalently module structures through the identity functor of Vr. Conversely a module equivalence preserving the labels is naturally isomorphic as an underlying linear functor to the identity: its map on each simple is isomorphic to that simple, and the direct-sum presentation of step 1.1 extends those isomorphisms naturally. Transport its module constraint through this isomorphism; the resulting natural isomorphisms gX:FX→FX give exactly the displayed gauge equation. Thus these are precisely the labelled equivalences. Arbitrary equivalences additionally permute the finite set of labels, so cannot increase the number of classes.

4.2F3step 3.1algebra

We compute the full scheme tangent at a point J of Sn, to avoid assuming that the displayed ideal is radical. Over k[ϵ]/(ϵ2) every variation is uniquely J′=J(1+ϵzX,Y), where zX,Y is an endomorphism of FXFY natural in both inputs, and zero when one input is the unit. Variations of tJ are uniquely determined by the inverse-determinant equation, so introduce no extra tangents. Differentiating the associativity equation and identifying both unchanged composites gives zX,Y∗1+z~X⋆Y,Z=1∗zY,Z+z~X,Y⋆Z, where z~X⋆Y,Z=(JX,Y∗1)−1zX⋆Y,Z(JX,Y∗1) and z~X,Y⋆Z=(1∗JY,Z)−1zX,Y⋆Z(1∗JY,Z). The fixed factor F(aD) has no variation and cancels with the base equation. Thus TJSn=ker⁡δ2=ZF2, with δ2z=1∗zY,Z−z~X⋆Y,Z+z~X,Y⋆Z−zX,Y∗1. This is precisely the four-term adjacent/outer differential of [F3] in tensor-functor order; reversing the input list returns its right-action order.

5.1F3step 4.1step 4.2algebra

A tangent vector to Gn is gX=1+ϵbX, with b1=0. Substituting in step 4.1 yields Jg=J(1−ϵδ1b), where (δ1b)X,Y=1∗bY−JX,Y−1bX⋆YJX,Y+bX∗1. Consequently the image of the orbit differential is im⁡δ1=BF2, the minus sign leaving the image unchanged. By [F3], HF2=ZF2/BF2=0. Therefore the orbit differential is surjective onto TJSn. The closed inclusion Xn=(Sn)red↪Sn injects TJXn into TJSn; the orbit map factors through Xn because its source Gn is reduced. Hence its image is contained in TJXn and surjectivity onto the larger space forces TJXn=TJSn and surjectivity onto TJXn. This reasoning applies at every point, since [F3] holds for every coherent module structure in the variety.

6.1F2F4F5step 1.1step 3.1step 4.1step 5.1∎

Apply [F4] to Gn acting on Xn: step 3.1 supplies affine finite type, step 4.1 supplies an algebraic product-of-general-linear-groups action, and step 5.1 supplies the tangent hypothesis everywhere. Each Xn has finitely many open orbits. Step 1.1 gives finitely many n at each rank, and step 4.1 identifies their points with all module structures up to the stated equivalences. Thus there are finitely many equivalence classes of rank r module categories. Finally [F2] bounds the ranks of all nonzero indecomposable module categories by ⌊D⌋, so the finite union over these ranks proves the unrestricted indecomposable finiteness. Rank zero contributes just the empty category if it is admitted. AC is inherited by [F4]; all category skeleton, matrix, and cochain choices made here are finite.

TheoremStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Finite semisimple module categories are separable algebra modules

Statement

Let C be a fusion category over an algebraically closed field of characteristic zero, and let M be a finite semisimple right C-module category. There is a separable algebra object A in C and a right C-module equivalence M≃Mod⁡Cl(A), the category of left A-modules fixed in Separable algebra objects and bimodules in a fusion category. The construction below fixes the right-action/internal-Hom convention, gives the internal-end multiplication and a separability section, and proves full faithfulness and essential surjectivity. With these conventions, right module functors from left A-modules to left B-modules correspond to B-A bimodules Q, acting by Q⊗A−; module-natural transformations correspond to bimodule maps.

Facts & Assumptions

[F1]

Right module internal ends and Eilenberg–Watts equivalence proves, without separability, the comparison for A=[m,m], where Hom⁡C(X,[m,n])=Hom⁡M(m⊙X,n) and m is a sum of simple representatives. The multiplication represents successive evaluations, its unit represents 1m, the comparison is n↦[m,n] with its left A-action, and this functor is fully faithful and essentially surjective. The same supplier proves the right exact Eilenberg–Watts equivalence including maps.

[F2]

Module-functor categories are finite semisimple proves finite semisimplicity by canonical-algebra averaging independently of separability of A. In its notation an ordinary natural transformation t:P→Q between module functors is averaged by Av⁡(t)=ρQ(1K⋅t)(1K⋅ρP)(e⋅1P), where e is the canonical separability element. This is module-natural, fixes module-natural maps, and preserves a section of a module-natural epimorphism.

[F3]

Separability and bimodule conventions are as in Separable algebra objects and bimodules in a fusion category.

Proof

Given: C,M as stated. The zero module category uses the zero algebra and zero section, so suppose M is nonzero.

1.1F1construct

Choose m as in F1, construct A=[m,m], and use the stated comparison M≃Mod⁡l(A). Concretely its multiplication is the unique map μ:A⊗A→A representing m⊙(A⊗A)→(m⊙A)⊙A→m⊙A→m, the last two maps being evaluation; hence on ordinary endomorphisms a⋅b=b∘a. Its unit represents 1m. F1 proves associativity, unitality, the left action on [m,n], and right module compatibility by the two rigidity adjunctions, and proves full faithfulness and surjectivity using exact internal Homs and free presentations. In particular the category of left A-modules is finite semisimple before any separability assertion is made.

2.1step 1.1F3construct

On this left module category let S(P)=A⊗U(P), with the free action on the first factor, where U forgets the action. There is a module-natural epimorphism r:S→Id⁡ with rP=lP, the action on P. Epimorphy follows because lP(η⊗1)=1 on underlying objects, and kernels and cokernels of A-module maps are inherited from C. This assertion does not require the displayed underlying section to be A-linear. Choose representatives p of the finitely many simple left A-modules. Since that module category is semisimple, choose an A-linear section jp:p→S(p) of rp. Extend these sections by additive decomposition to an ordinary natural transformation t:Id⁡→S: on P=⨁pHom⁡A(p,P)⊗p, take the direct sum of the corresponding maps jp and transport using the canonical evaluation decomposition. Its naturality follows because any map is a matrix on the multiplicity spaces. By construction rt=1.

3.1step 2.1F2F3constructalgebra

Apply the explicit averaging in F2 to t and set s=Av⁡(t). Then s is module-natural and rs=1. Define the requested separability section by σA=sA:A→S(A)=A⊗A. Every component of s is a left A-module map, so σA is left A-linear. It is also right A-linear: naturality of s at the left A-map μ:A⊗A→A gives S(μ)sA⊗A=sAμ. Module-naturality identifies sA⊗A=sA⊗1A, and S(μ)=1A⊗μ, so (1A⊗μ)(σA⊗1A)=σAμ. Finally rAσA=1A is μσA=1A. This constructs an actual bimodule section; it uses finitely many chosen sections and the fixed normalized canonical separability element, without requiring a pivotal or spherical structure on C. Thus A is separable.

4.1step 1.1step 3.1F1construct∎

For another finite semisimple right module category represented by B, F1 identifies every right exact module functor with Q⊗A− for Q=F(A) a B-A bimodule, whose right action is F(μ) under F(A⊗A)≅F(A)⊗A. Every linear functor between the semisimple categories here is exact, so there is no additional exactness restriction. F1 proves that the canonical free coequalizer of each module gives the natural isomorphism to this tensor functor, and that evaluation of transformations at A and tensoring a bimodule map are inverse operations. This proves the full claimed equivalence and its precise orientation together with the separable-algebra construction.

Remarks

The unrestricted positive-characteristic version is false. For C=Vec⁡Z/p over an algebraically closed field of characteristic p, its one-simple module category Vec⁡ has endofunctor category Rep⁡k(Z/p), which is not semisimple. If it were represented by a separable algebra, averaging by its separability element on the left and right would split every epimorphism of bimodules, making its module endofunctor category semisimple by Eilenberg–Watts, a contradiction. Characteristic zero restores exactly the approved PA-48 field scope.

TheoremStatement: Literature-sourcedProof: AI-adaptedOpen item page →

The relative Deligne product is represented by the braided tensor algebra

Statement

Let C be a braided fusion category and let M≃Mod⁡Cl(A) and N≃Mod⁡Cl(B) be finite semisimple right module categories represented by separable algebras; the left-module notation is fixed in Separable algebra objects and bimodules in a fusion category. Their relative Deligne product as fixed in Relative Deligne product in the braided module 2-category exists, is finite semisimple, and is equivalent as a right C-module category to Mod⁡Cl(A⊗B), where the algebra product uses the braiding cB,A. This equivalence is independent, up to canonical equivalence, of the chosen algebra presentations and supplies the object tensor product in the separable-algebra model of Mod⁡(C). The relative products assemble into a weak monoidal 2-category: associators and unitors are the unique equivalences preserving the relevant universal balanced functors, the pentagon and triangle modifications obey their coherence equations, and the product is compatible with module functors and module-natural transformations.

Facts & Assumptions

Given: A braided fusion category and two right module categories represented by separable algebras A,B as in the statement.

[F1]

Relative Deligne product in the braided module 2-category fixes the balanced universal property and the inverse-braiding left conversion.

[F2]

The braided tensor product of separable algebras is separable and Finite semisimplicity for separable algebra modules and bimodules give separability of K=A⊗B, its finite semisimple module category, and split separability idempotents. Separable algebra objects and bimodules in a fusion category fixes module and bimodule conventions.

Proof

1.1F1F2givenalgebra

The left-module presentation reverses the algebra-bimodule 1-morphism orientation: a module functor Mod⁡l(A)→Mod⁡l(B) is represented by a B-A bimodule, while the algebra convention A→B uses A-B bimodules. Thus the algebra presentation of this module 2-category uses the 1-morphism opposite of that algebra bicategory. Tensor multiplication on objects is unchanged. Under this passage the evaluation and coevaluation arrows exchange, and left and right dual roles exchange; both dual orientations have been constructed separately. Preserve the positive braided tensor algebra K=A⊗B. Let P=Mod^l_C(K). Define b(M,N)=M⊗N, with K-action (l_M⊗l_N)(1_A⊗c_{B,M}⊗1_N).

1.2F1F2givenalgebra

Naturality and the hexagons prove its action equation exactly as for the positive tensor-algebra multiplication. Define balance by 1_M⊗c_{N,X}^{-1}: MXN→MNX; this is K-linear: expand c_{B,MX}, cancel the c_{B,X} against c_{N,X}^{-1} by naturality with l_N, and the remaining composite is the target K-action. The balance/unit equation is the braiding unit equation. For balance associativity on MXYN, both composites are the inverse braid taking XYN to NYX: move Y behind N and then X behind NY, or move XY behind N and then interchange X,Y by cY,X−1. The inverse hexagon expands both to the same three inverse crossings. Compatibility with the outer right action is the other inverse hexagon. Hence b is a balanced right-module functor. It is exact and bilinear because all tensor functors in a fusion category are exact.

1.3F1F2givenalgebra

Here is a proof of universality which also specifies its action on transformations. A right K-object d in a finite semisimple right C-module category D is an object equipped with r:d⊙K→d satisfying the algebra action equations. It determines a module functor H_d:P→D by H_d(L)=d⊙_K L.

1.4F1F2givenalgebra

Construct Hd(L) as the image of the separability idempotent (r⊙l_L)(1_d⊙e_K⊙1_L) on d⊙L. Its image exists because D is finite semisimple. The usual centrality and unit equations for e_K show this image corepresents K-balanced maps, just as for the ordinary bimodule supplier: the idempotent is fixed by every balanced map; conversely its projection is balanced. No new coequalizer existence theorem is being assumed. This construction is functorial in L and K-linear maps d→d'.

1.5F1F2givenalgebra

Conversely any module functor H:P→D is canonically H_d with d=H(K). Its right action is H(m_K):H(K⊗K)≅H(K)⊙K→H(K). On free modules K⊗X, its module constraint gives H(K⊗X)≅d⊙X. Every K-module L is a retract of K⊗L: the action is the retraction and the section is (1_K⊗l_L)(e_K⊗1_L). This section is K-linear by centrality, and its action composite is 1_L. Hence the free-module comparison extends uniquely to all retracts. To check naturality it suffices to check free maps. Such a map K⊗X→K⊗Y is uniquely (m_K⊗1_Y)(1_K⊗f) for f:X→K⊗Y obtained by inserting η_K; H and H_d agree on this expression by the definition of r. Transformations agree precisely when their value at K is K-linear. This proves an equivalence of categories, including transformations, between module functors P→D and right K-objects in D. For a balanced module functor F:Mod^l(A)×Mod^l(B)→D, put d=F(A,B). Denote its outer constraint by δ:F(M,NX)→F(M,N)⊙X and its balance by β. Put θ=δβ:F(MX,N)→F(M,N)⊙X. Define r_A=F(m_A,1_B) θ_{A,A,B}^{-1}:d⊙A→d, r_B=F(1_A,m_B) δ_{A,B,B}^{-1}:d⊙B→d.

1.6F1F2givenalgebra

Naturality with the algebra multiplications proves their associative/unital action equations. Expanding the balance/outer compatibility square gives the precise exchange equation r_A(r_B⊙1_A)=r_B(r_A⊙1_B)(1_d⊙c_{B,A}):d⊙B⊙A→d.

1.7F1F2givenalgebra

For an explicit verification, replace θ by δβ, move each multiplication through δ by its naturality, and through β by naturality in its module arguments. The residual two routes move the free B slot past the free A slot. The balance-associativity equation for the chosen inverse left conversion replaces that move by c_{B,A}; its inverse crossing is cancelled by the inverse in θ^-1. The remaining maps are F(m_A,m_B) on both routes. Thus r=r_B(r_A⊙1_B) is a right K-action: its iterated action on dABAB first moves the middle B past A by c_{B,A}, then uses the two individual action equations, exactly giving r(1_d⊙m_K). This proves the action equation without assuming ordinary commuting actions.

1.8F1F2givenalgebra

The functor H_d b is canonically equivalent to F. On free pairs first use δ to identify F(AX,BY) with F(AX,B)⊙Y, and then θ on the first factor, to obtain F(A⊗X,B⊗Y)≅d⊙X⊙Y. Meanwhile the positive crossing 1_A⊗c_{B,X}⊗1_Y is a K-linear isomorphism K⊗X⊗Y→b(A⊗X,B⊗Y).

1.9F1F2givenalgebra

This free-pair isomorphism identifies H_d b on this pair with d⊙X⊙Y. The two identifications commute with arbitrary free A-module and B-module morphisms: express such morphisms by their adjoint maps X→A⊗X' and Y→B⊗Y', then use r_A,r_B respectively. For a simultaneous morphism the exchange equation is exactly the required compatibility of the two orders. Every M,N is a retract of its free module by the displayed separability section, so this natural equivalence extends to all pairs by taking images of the two commuting retract idempotents. The construction respects the balance and outer action because it does so on free pairs, where these equations are the already verified β,δ equations. Thus composition with b is essentially surjective on balanced functors.

1.10F1F2givenalgebra

A transformation between two balanced functors is determined on free pairs by its component at (A,B), using θ,δ, and then on all pairs by retracts. Naturality with m_A and m_B says exactly that this component preserves r_A,r_B, equivalently the K-action r. Conversely any K-linear component gives such a transformation via H_d. Consequently composition with b is fully faithful and is the required equivalence of categories. This proves the exact stated universal property, not merely existence of a bilinear functor.

1.11F1F2givenalgebra

Finite semisimplicity of P follows from separability of K: module Hom spaces are images of the averaging idempotent on Hom_C(M,N), so are finite dimensional; every module is a retract of a free module, and the finitely many free modules K⊗S_i for simple S_i of C form a finite additive generator. Its endomorphism algebra is semisimple because any module subobject splits by averaging an underlying splitting. Therefore the module category is finite semisimple. It is a right C-module category by the inherited tensor action. The preceding argument applies to arbitrary D, so uniqueness of representing objects makes the answer independent of the chosen algebra presentations, with a canonical equivalence preserving b.

1.12F1F2givenalgebra

For module functors G:M→M',H:N→N', apply the universal property to b'(G×H); its balanced structure is inherited from the module constraints of G,H. This defines G⊠H. For module-natural transformations use full faithfulness to define their product. Identity and composite comparison maps are the unique maps whose pullbacks to b equal the identity or the corresponding composite constraint. Their associativity, unit and interchange equations hold by full faithfulness, since after pullback they are the same equation for ordinary functor composition.

2.1F1F2givenalgebra∎

Both parenthesizations of three module categories represent the category of three-variable exact functors balanced in the two adjacent slots, with outer right-module compatibility. This follows by applying the just-proved equivalence twice; the same free/retract argument shows that no balanced transformations are lost. Their comparison is therefore the unique equivalence preserving the universal three-variable functor, with its specified natural isomorphism. For the regular module category C, the action functor M×C→M (and the converted left action C×M→M) has the universal property by inserting the unit object and applying balance. These give the unitors. On four variables the two pentagon composites have the same pullback comparison to the universal four-variable functor. Full faithfulness gives the unique pentagonator modification; on five variables the two composites of these modifications have identical pullback, hence are equal. The unitor triangle modification and all its compatibility equations follow in exactly the same way from the three-variable functor with a unit slot. This is the weak monoidal 2-category coherence assertion: one should say 'canonical modifications' rather than incorrectly demanding literal equality of unchosen equivalences. Naturality with G,H and their transformations follows by pulling back to the same multivariable functor. Thus the product supplies all morphism levels and weak coherence required in the carrier statement.

TheoremStatement: Literature-sourcedProof: AI-adaptedOpen item page →

The algebraic 2-category Mod(C) is a fusion 2-category

Statement

Assume the Axiom of Choice. Let C be a braided fusion category over an algebraically closed field of characteristic zero. The 2-category Mod⁡(C) of finite semisimple right C-module categories, module functors, and module-natural transformations, with monoidal product given by relative Deligne tensor product over C (using its braiding to convert one action), is a fusion 2-category. In particular it is finite semisimple, has a simple unit, has left and right object duals, every 1-morphism has adjoints, every separable monad splits, and it has finitely many equivalence classes of simple objects.

Facts & Assumptions

Given: The Axiom of Choice and a braided fusion category C over an algebraically closed field of characteristic zero.

[F1]

Module-functor categories are finite semisimple gives finite semisimple hom categories and identifies regular-module endofunctors with C, sending the identity to its unit.

[F2]

Module functor adjoints and separable-monad splittings in Mod(C) gives both module adjoints and separable-monad splittings.

[F3]

A uniform rank and action-multiplicity bound for module categories bounds indecomposable ranks and all action multiplicities by fixed fusion data.

[F4]

Bounded-rank module-structure varieties have finitely many open orbits gives finitely many equivalence classes at every bounded rank.

[F5]

The relative Deligne product is represented by the braided tensor algebra constructs the relative products, their unit, and their complete weak monoidal coherence on objects, functors and transformations.

[F6]

Object duals in the separable-algebra model of Mod(C) constructs the object duals with both invertible cusp composites.

[F7]

Finite semisimple module categories are separable algebra modules gives separable algebra presentations of every object and the bimodule equivalence on hom categories.

[F8]

Fusion 2-category requires finite semisimplicity, weak monoidality, simple unit and left and right object duals.

[A1]

The Axiom of Choice is used through the classical algebraic geometry suppliers of [F4]; finite category decompositions introduce no additional choice.

Proof

1.1F1F2givenconstruct

Composition of module functors is ordinary functor composition with the composite action comparison; its module equation follows by substituting the two module equations. Identities have identity comparison. Horizontal and vertical composition of module-natural transformations are their ordinary compositions and obey interchange because horizontal composition is a functor on the functor categories. Each hom category is finite semisimple by [F1]. The zero module category and finite direct sums of module categories are obtained componentwise; inclusions and projections are module functors. Their biproduct equations hold componentwise, and composition preserves these sums since every functor is linear. Both adjoints and all separable-monad splittings exist by [F2].

2.1A1F1F3F4step 1.1algebra

To identify simple objects, write the simple objects of a module category as ma. Join a to b when mb is a summand of ma⊙X for a simple X∈C. Rigidity makes this an undirected graph. Its components are precisely action-stable full semisimple summands, so indecomposability is connectedness. A natural endomorphism of the identity acts on ma as ta1ma, because the field is algebraically closed and simple endomorphism rings are finite dimensional. Module-naturality and naturality along each summand inclusion force ta=tb along every edge. Conversely scalars constant on components define module-natural endomorphisms. Thus the endomorphism algebra of the identity is one copy of the field for every component. In the semisimple hom category from [F1], an object is simple exactly when its endomorphism algebra is the field: decompose it into simples, whose endomorphism algebras are the field, and use the resulting product of matrix algebras. Hence nonzero simple objects of Mod⁡(C) are exactly indecomposable module categories. By [F3] their ranks are bounded and only finitely many action multiplicity arrays occur; [F4] gives finitely many module equivalence classes for each array. There are consequently finitely many simple-object equivalence classes.

2.2F1F5F6F7step 1.1construct

The universal relative products from [F5] supply the tensor pseudofunctor, its composition and identity comparisons, unit C, associator and unit equivalences, and their coherence modifications. Its proofs establish naturality, the pentagon and triangle and interchange on transformations, so this is a weak monoidal structure on the same 2-category of step 1.1. Under [F1], the identity of the regular module is the simple unit of C; therefore the tensor unit is simple. Every object admits a separable algebra presentation by [F7]. The orientation is essential: an A-B bimodule X, regarded as A→B in the algebra bicategory, acts on left modules by X⊗B−:Mod⁡l(B)→Mod⁡l(A). Thus Eilenberg–Watts identifies Mod⁡(C) with the 1-morphism-opposite of that algebra bicategory. Composing these functors identifies composition with balanced tensor, by the common balanced trilinear universal property. The product construction in [F5], evaluated on free modules and extended to their separability retracts, identifies tensoring these functors with tensoring their bimodules using the positive middle braid. Consequently this identification is monoidal with the stated reversal of 1-morphisms. Fact [F6] supplies both left and right object duals there, with separate negative and positive opposite algebras. Reversing 1-morphisms interchanges evaluation and coevaluation, so a left dual becomes a right dual and conversely; its invertible cusp maps become the corresponding inverse comparisons. Therefore both duals transport to Mod⁡(C) with all their required source, target and inverse equations.

3.1F8step 1.1step 2.1step 2.2algebra∎

Steps 1.1 and 2.1 establish every clause of finite semisimplicity; step 2.2 establishes weak monoidality, a simple unit, and both object duals. These are exactly the requirements in [F8]. Thus Mod⁡(C) is a fusion 2-category under the full stated hypotheses.

5 · Examples, counterexamples and false statements

None yet.

Sources