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Equivariant fusion subcategories

We provide a parameterization of all fusion subcategories of the equivariantization by a group action on a fusion category. As applications, we classify the Hopf subalgebras of a family of semisimple Hopf algebras of Kac-Paljutkin type and recover Naidu-Nikshych-Witherspoon classification of the fusion subcategories of the representation category of a twisted quantum double of a finite group.


Introduction
Fusion categories generalize the representation categories of finite-dimensional semi-simple (quasi) Hopf algebras [ENO05]. A fundamental construction in the theory of fusion categories is equivariantization by a group action, [EGNO15]. Given a categorical action of a finite group G on a fusion category C, the equivariantization C G is a new fusion category, consisting of categorical "fixed points" under the G action. Equivariantization, and its reciprocal construction called de-equivariantization, have been extensively studied and used in recent years to classify and characterize families of fusion categories, see [ENO11], [DGNO10]. The goal of this note is to identify the lattice of fusion subcategories of C G in terms of the lattice of fusion subcategory of C and cohomological data arising from the G-action (Theorem 4.8).
If a fusion category C is equivalent to the category of (right) comodules of a finite-dimensional semisimple Hopf algebra H, then the lattice of fusion subcategories of C is isomorphic to the lattice of Hopf subalgebras of H, see [NR96,Theorem 6]. Many interesting Hopf algebras (in particular Hopf algebras of Kac-Paljutkin type and quantum groups at roots of unity) contain a central Hopf subalgebra C G , and this implies the existence of a central exact sequence of Hopf algebras of the form In this case, the category of H-comodules is a G-equivariantization of the category of Q-comodules, [AGP14]. Thus we can apply our results to obtain a parameterization of the Hopf subalgebras of central extensions of semisimple Hopf algebras, particularly to Hopf algebras of Kac-Paljutkin type associated to semidirect products of groups.
César Galindo was partially supported by Faculty of Science of Universidad de los Andes, Convocatoria 2020-2022 para la Financiación de Programas de Investigación. Corey Jones was supported by NSF grant DMS 1901082/2100531. It is well known how to parameterize the simple objects of the equivariantization and compute their fusion rules in terms of the data of the G action (for example, [BN13]). Fusion subcategories of a fusion category D correspond with fusion sub-rules of the Grothendieck ring K 0 (D). Hence, in principle, having the fusion rules of C G , the computation of fusion subcategories of C G reduces to the computation of fusion sub-rules of K 0 (C G ). However, even the computation of K 0 (C G ) and its multiplication could be computationally demanding. Therefore, it is desirable to obtain a parameterization of the fusion subcategories of an equivariantization directly in terms of the data of the group action.
After posting an initial version of this paper to the arXiv, Dmitri Nikshych brought to our attention that our Theorem 4.8 was previously obtained by Alex Levin and presented at conferences in 2017. Levin's work has not yet been made publicly available. We thank Dmitri for bringing this to our attention.
The paper is organized as follows. In Sections 2 and 3 we recall the basic definitions and results concerning equivariantization by a categorical group action and de-equivariantization of a fusion containing a central inclusion of Rep(G). In Section 4, we prove our main result, which provides a parameterization of equivariant fusion subcategories of a fusion category. In Section 5, we take a closer look at the parameterization in the case of group actions on pointed fusion categories, providing an obstruction theory for Ginvariant trivializations. Finally, in Section 6, we apply this to parameterize Hopf subalgebras of a class of Kac-Paljutkin type studied in [Sek96] and [Mas97].

Preliminaries
A fusion category is a finitely semi-simple rigid tensor category. In this paper, we assume our field is algebraically closed and characteristic 0. We refer the reader to the comprehensive reference [EGNO15] for categorical background. In this section, we will recall some basic notions and set up notation for categorical actions of groups on fusion categories and equivariantization.
Let Aut(C) denote the 2-group of tensor autoequivalences of a fusion category and tensor natural isomorphisms with tensor product given by composition of tensor functors. A categorical action of G on C is a strong monoidal functor G → Aut(C). We denote the assignment g → g * , and the monoidal natural isomorphisms µ g,h : g * • h * → gh * . We denote the component of a natural isomorphism with a superscript, i.e., the x component of µ g,h is denoted µ x g,h for x ∈ C. Given a categorical action of G on C, recall that the equivariantization C G is a new fusion category whose objects are equivariant objects, given by pairs (x, ρ), where x ∈ C and ρ = {ρ g : g * (x) ∼ = x} g∈G is a family of isomorphisms satisfying µ x g,h ρ g g * (ρ h ) = ρ gh for all g, h ∈ G. Morphisms between equivariant objects (x, ρ) and (y, δ) are morphisms f ∈ C(x, y) such that for all g ∈ G, f ρ g = δ g g * (f ). This forms a new monoidal category called the equivariantization, denoted C G . The product (x, ρ) ⊗ (y, δ) is defined by where β x,y g : g * (x ⊗ y) ∼ = g * (x) ⊗ g * (y) is the tensorator of the monoidal equivalence g * .
An important point of note is that since the unit object of C is simple, there is a canonical copy of Rep(G) ≤ C G embedded as a full subcategory, consisting of equivariant objects which are direct sums of the unit object ½.
Furthermore, this subcategory naturally lifts to the center Z(C G ). Fusion categories C equipped with a fully-faithful monoidal functor F : Rep(G) → C that factors through a braided monoidal functor Rep(G) → Z(C) fusion categories over Rep(G).
Both G-fusion categories and fusion categories over Rep(G) naturally form 2-categories (see [DGNO10,Section 4]). Equivariantization extends to a 2functor from G-fusion categories to fusion categories over Rep(G). This 2-functor has an explicit inverse called the de-equivariantization functor.
Given a fusion category over Rep(G), then identifying Rep(G) with its image under F , the etale algebra Fun(G) ∈ Rep(G) can be viewed as a central algebra in C. Thus the quotient category of right Fun(G) modules C Fun(G) is a fusion category called the de-equivariantization of C, which we also denote by C G . The free module functor C → C Fun(G) = C G is monoidal. Furthermore, one can equip the dequivariantization with a natural categorical action of G, and in fact this extends to a 2-functor from the 2-category of fusion categories over Rep(G) to the 2-category of G-fusion categories. The fundamental theorem of G-actions on fusion categories states that equivariantization and de-equivariantization are mutually inverse 2-functors [DGNO10, Theorem 4.4].

Sequential Equivariantization
Let G be a group acting on a monoidal category C and let H ≤ G be a normal subgroup. First pick a section ι : G/H → G of the canonical projection π : G → G/H and define α : Using the bijection the multiplication on G transports to (h, a)(k, b) = (hι(a)kι(a) −1 α(a, b), ab).
Given (x, ρ) ∈ C H , and a ∈ G/H, we define a * (x, ρ) := (x ′ , ρ ′ ) where It is straightforward to check for each a ∈ G/H this is a monoidal functor, using the tensorator for ι(a) * .
To obtain a categorical action, we need monoidal natural isomorphisms to be the morphism making the following diagram commute which is an equivariant morphism. ν a,b : a * • b * → ab * assembles into a monoidal natural isomorphism. This gives us a categorical action [DGNO10,Equation 75]). One way to see this is using the strictification result of [Gal17], which implies it suffices to consider the case where the G action on C is strict. Here it is very easy to build this equivalence by simply rearranging the data of equivariant objects.

The Parametrization
In this section we parameterize fusion subcategories of an equivariantization of a fusion category by a group action. If C is a fusion category, by a fusion subcategory we mean a full, replete monoidal subcategory (which itself is necessarily a fusion category). These correspond bijectively to unital based subrings of the fusion ring of C.
Recall that the trivial categorical action Tr of a group G on a monoidal category C sends each group element to the identity monoidal functor Id C , and all structure maps are identities as well. If we have a categorical action α : G → Aut(C), a trivialization is a monoidal natural isomorphism α ∼ = Tr. Unpacking this, a trivialization consists of • For each g ∈ G, a monoidal natural isomorphism η g : g * ∼ = Id C .
• These {η g } g∈G must satisfy the equation Recall if E is a full, replete subcategory of C we say E is invariant under the G-action if α g restricts to an autoequivalence of E.
Definition 4.1. Let E ≤ C be a G-invariant fusion subcategory, and let H ≤ G be a normal subgroup. We say a trivialization η of α| H on the category E is G-equivariant if the following diagram commutes: where can is the canonical morphism arising from coherence.
Writing can out explicitly gives the equation: Definition 4.2. Given a group G acting on a monoidal category C, a lifting of a fusion subcategory E ≤ C is a choice, for every Lemma 4.3. The data of a lifting is precisely the data of a trivialization of the G-action on E.
Proof. Given a lifting of E we can define a trivialization of the G action on E as follows. Set η x g : g(x) ∼ = x by η x g := ρ x g . Equation (4.1) is (1) in the definition of lifting and (2) is equivalent to the naturality of η g for every g.
Conversely, given a trivialization of G on E, then (x, η x g ) defines an equivariant structure. Since the η g are natural, we see Lemma 4.4. Given a G action on C, E ≤ C be a fusion subcategory, and a lifting ρ of E to C H for some normal subgroup H ≤ G, then the corresponding Proof. Let ρ be a lifting of E to C H , and let {η h } h∈H be the trivialization defined by η , and that is exactly the commutativity of diagram (4.2).
We record the following, defined in [Nik19]: Definition 4.5. If C is a fusion category, A ∈ C is a connected separable algebra, and E ≤ C is fusion subcategory, we say E is transversal to A if It's easy to see that transversality is equivalent to requiring for all x ∈ E. We denote by C A the semi-simple category of right A modules in C. We have the following lemma: Lemma 4.6. Let C be fusion, E ≤ C a fusion subcategory, and A ∈ C a connected seperable algebra. Then E is transversal to A if and only if the free module functor Recall that the left adjoint of F A is simply the forgetful functor, i.e. the functor that forgets the right A-module structure on an object. Then is an isomorphism, hence F A is fully faithful.
Conversely, if F A is fully faithful on E, then Lemma 4.7. Let C be a fusion category with G action. There is a bijection between the following: (1) Fusion subcategories D ≤ C with trivializations of the G action on D.
(2) Fusion subcategories E ≤ C G such that F G | E is fully faithful.
(3) Fusion subcategories of C G which are transversal to the algebra Fun(G) ∈ Rep(G) ≤ C G .
Proof. First we establish a bijection between items (1) and (2). Given D ≤ C and a trivialization η, this uniquely defines a lifting ρ by Lemma 4.3. Then we consider the full subcategory E := D ρ ≤ C, spanned by objects {(x, ρ x )} x∈D . By the definition of lifting, this is a full monodial catgeory of C G , such that the forgetful functor is fully faithful.
In the other direction, suppose we have a E ≤ C G such that the forgetful functor is fully faithful. Define D to be the image of E under the forgetful functor. Since the forgetful functor is fully faithful we have Hom E ((x, η x ), (y, η y )) = Hom C (x, y), in particular, that implies that if (x, η x ), (x, λ x ) ∈ E, then η x = λ x . Since E is monoidal, the uniqueness of η x for all x ∈ D implies (4.1). Now for each object x ∈ D, by definition (and repleteness) there exists a unique pre-image (x, η x ) ∈ E. The isomorphisms {η x } x∈D define a lifting of D.
Theorem 4.8. Let C be a fusion category with G action. Fusion subcategories of C G are parameterized by triples (E, H, η) where (1) E ≤ C is a G-invariant fusion subcategory.
(2) H ≤ G is a normal subgroup.
(3) η is a G-equivariant trivialization of H on E.
Proof. Given the above data, let ρ be the lift of E to C H defined by the trivialization (Lemma 4.3). The fusion subcategory E ρ ≤ C H is G/H invariant by Lemma 4.4. Define D to be the replete image of (E ρ ) G/H under the canonical equivalence (C H ) G/H ∼ = C G . This gives a subcategory of C G from our data.
In the other direction, let D ≤ C G be a fusion subcategory.
Let E ≤ C be the full fusion subcategory generated by the image of D under the forgetful functor F G : Let H be defined by Rep(G) ∩ D ∼ = Rep(G/H). To get the trivialization of the H action on E, η, Note that we have the following diagram of monoidal functors commutes up to canonical natural isomorphism: By Lemma 4.7, this implies F H induces an equivalence from E ′ to E, and such an equivalence uniquely defines a lifting E → C H which is G/H invariant (since E ′ is G/H invariant by construction). This gives a G-equivariant trivialization η by Lemma 4.3. Now, it is easy to see these two constructions are mutually inverse.
From the construction, we have the following corollary

Pointed fusion categories
Let K be a finite group and ω ∈ Z 3 (K, × ). The data of a categorical action of the group G on Vec(K, ω) can be described by the following: (1) A homomorphism G → Aut(K), g → g * (2) A collection of scalars β k,l g ∈ × for k, l ∈ K, g ∈ G and a collection of scalars µ k g,h ∈ × for k ∈ K and g, h ∈ G, satisying the following equations: To realize this data, pick a skeletal model of Vec(K, ω) with the associator given by ω explicitly. Then extend the action of g * on K linearly to a functor. By semi-simplicity it suffices to define natural transformations of functors on simple objects. The tensorator g * (k ⊗ l) ∼ = g * (k) ⊗ g * (l) is given by β k,l g , and equation (5.1) above is exactly the required compatibility with the associator. We define the natural isomorphisms gh * (k) ∼ = g * • h * (k) by µ k g,h . Equation (5.3) ensures these are monoidal natural isomorphisms, and equation (5.2) guarantees these assemble into a categorical action. Now, our goal is to apply our general results to parameterize subcategories of the equivariantization in terms of the above data. The only remaining task is to interpret the G-equivariant trivializations in terms of this data.
Let L ≤ K be a G-invariant subgroup, and H ≤ G a normal subgroup such that h * | L is trivial. First we can unpack the definition of a trivialization of the H action on L.
It consists of a family η k h ∈ × for k ∈ L, h ∈ H satisfying for all g, h ∈ H (5.4) η lk g = η l g η k g β l,k g (5.5) η l g η l h = η l gh µ l g,h Viewing η : L × H → , we see that it is almost a bicharacter. In particular, it is a character in each variable up to β and µ respectively. Thus we will call η : L × H → satisfying the above equations a (β, µ)bicharacter. Now, we can unpack the definition of a G-equivariant tivialization to obtain where we have used in the superscript on the denominator that H is normal in G, and since H acts trivially on L, g(ghg −1 ) * (k) = g(k) for all k ∈ L. Note that we can assume µ k h,g is normalized so that µ k h,g = 1 for all k if h or g is 1. Then the defining condition for µ implies µ k g −1 ,g = µ g * (k) g,g −1 . Furthermore, the defining equation, together with normalization and the fact that h acts trivially on L implies equation Solving for µ k g −1 ,gh , replacing µ k g −1 ,g with µ g * (k) g,g −1 , and substituting into equation (5.7) gives Definition 5.1. A (β, µ) bicharacter satisfying equations (5.7) or (5.8) is called a G-equivariant (β, µ) bicharacter.
Thus according to Corollary 5.2, since the action of G on G is by conjugation, the subcategories of Z(Vec(G, ω)) are parameterized by triples (L, H, η), where L, H are commuting normal subgroups of G and η is a G-invariant (β, µ)-bicharacter.
The parameterization in [NNW09] is given by triples (L, H, B), where L, H are commuting normal subgroups of G, and B : L × H → × is a G-invariant ω-bicharacter ([NNW09, Definition 5.4]). Using [NNW09,Equation 19], we see that B is an ω-bicharacter if and only if B −1 is a (β, µ)-bicharacter in our sense. 5.2. Obstruction theory. In Corollary 5.2, we parameterized the subcategories of the equivariantization of a pointed fusion category in terms of algebraic data, which can be described as solutions to families of equations with a cohomological flavor. It is desirable to have an obstruction theory theory that allows one to determine whether such data exists or not, and to be able to count the solutions if they do exist. In this section, we present some results in this direction.
Let G be a finite group acting on Vec(K, ω) with associated data β k,l g and µ k g,h . Let L ≤ K be a G-invariant subgroup and H ≤ G a normal subgroup such that H acts trivially on L. We will analyze the cohomological conditions for the existence of a G-equivariant (β, µ)-bicharacter η : L × H → × . 5.2.1. Existence of (β, µ) bicharacters. Since H acts trivially on L, it follows from equation (5.1) that for all h ∈ H. If follows from (5.4) that a first necessary condition for the existence of a (β, µ) bicharacter is that the cohomology class of (β h )| L×L is trivial for all h ∈ H. If the cohomology class (β h )| L×L is trivial for all h ∈ H, there exist τ : L × H → × such that τ h l 1 l 2 = τ h l 1 τ h l 2 β l 1 ,l 2 h holds for all h ∈ H, l 1 , l 2 ∈ L.

5.2.2.
Existence of G-invariant (β, µ)-bicharacters. It is easy to see that the set of all (β, µ)-characters is a torsor over the abelian group of all bicharacters H × L → × . Let η : H × L → × be a (β, µ)-bicharacter. Define the function Proposition 5.3. The following conditions are necessary and sufficient for the existence of a G-invariant (β, µ)-bicharacter.
(1) Ω(η, µ) defines an element in Z 1 (G, Hom(L, Hom(H, × ))) whose cohomology class does not depend on the choice of η. In the above group, the action of G on a bicharacter is given by g (χ l h ) = χ g * (l) ghg −1 for all g ∈ G, h ∈ H, l ∈ L.
It follows by the definition of Ω(η, µ) that it vanishes if η is G-invariant. Conversely, if Ω(η, µ) ∈ Z 1 (G, Hom(K, Hom(H, × ))) and there exists a bicharacter χ such that Ω(η, µ) g,h,l = χ l h χ g * (l) h then τ = η χ is a G-invariant 6. The lattice of Hopf subalgebras of a Hopf algebra of Kac-Paljutkin type 6.1. Hopf algebra of Kac-Paljutkin type. Let G be a finite group acting on a finite group K and (β, µ) a data defining an action of G on Vec(K). Let us denote G := Maps(G, ), let δ g ∈ G be the function that assigns 1 to g and 0 otherwise, and let δ g,h be the Dirac's delta associated to the pair g, h ∈ G, namely δ g,h is 1 whenever g = h and 0 otherwise.
Corollary 6.1. Let G # β µ K be a semisimple Hopf algebra of Kac-Paljutkin type, then the lattice of Hopf subalgebras is in correspondence with the lattice of triples (L, H, η) where (1) L ≤ K is a G-invariant subgroup.
(2) H ≤ G is a normal subgroup. ( Proof. It follows from Corollary 5.2 that the triples are in correspondence with fusion subcategories of Vec(K) G . Now, the fusion category of right G # β µ K-comodules is tensor isomorphic to the fusion category Vec(K) G , (see [GGU15,Theorem 7.1]) hence by [NR96, Theorem 6] they correspond to Hopf subalgebras of G # β µ K.
Then the obstruction vanishes if and only if there is ζ ∈ G m such that q x 2 = ζ 2 .
6.2.2. When H is trivial. In general, if H is trival the fusion subcategories associated are given just by pairs (L, η) where L ≤ K is a G-invariant subgroup and η ∈ G is G-invariant linear character. Using Goursat's lemma it is straightforward to see that As a conclusion of the subsections 6.2.1 and 6.2.2 we obtain the following result.
Theorem 6.2. The Hopf subalgebras of C 2 # βq µq (Z/n × Z/n) come in two types, and correspond to