On the Drinfeld double of a finite group scheme and its representation category


Abstract

We classify equivalence classes of Hopf algebra quotient pairs \((D,\theta)\) of the Drinfeld double \(D(G)\) of a finite group scheme \(G\) over an algebraically closed field \(\mathbf{k}\) of characteristic \(p\ge 0\), in terms of group scheme-theoretical data. We prove that such Hopf algebra quotients \(D\) are Hopf algebra extensions \(\mathscr{O}(K)^{\mathrm{cop}}\#_{\sigma}^{\tau} \mathbf{k}[G/H]\), where \(K\) and \(H\) are normal subgroup schemes of \(G\) that centralize each other and \(B:\mathbf{k}[H]\to \mathscr{O}(K)\) is a \(G\)-equivariant Hopf algebra map, and describe the surjective Hopf algebra map \(\theta:D(G)\twoheadrightarrow D\). Using this classification, we determine the tensor subcategories of the center \(\mathscr{Z}(G):=\operatorname{Rep}(D(G))\) of \(G\), describe their centralizers, determine when they are symmetric or non-degenerate, and give a description of their simple and projective objects using [1]. Our categorical results generalize those found in [2] in characteristic \(0\).

1 Introduction↩︎

The representation category \(\mathscr{Z}(G):=\operatorname{Rep}(D(G))\) of the Drinfeld double \(D(G)\) of a finite group scheme \(G\) over an algebraically closed field \(\mathbf{k}\) of characteristic \(p\ge 0\) plays a central role in the theory of finite braided tensor categories [1][13]. In characteristic \(p=0\), the category \(\mathscr{Z}(G)\) is a non-degenerate braided fusion category; in this semisimple setting the tensor subcategories of \(\mathscr{Z}(G)\) were classified by Naidu, Nikshych, and Witherspoon [2]. A key feature of [2] is that modular data can be used as an effective organizing principle. Namely, the \(S\)-matrix of \(\mathscr{Z}(G)\) detects when two simple objects of \(\mathscr{Z}(G)\) centralize each other, and Müger centralizers can be computed from \(S\)-matrix relations, ultimately translating the subcategory problem into explicit group-theoretic conditions involving commuting normal subgroups of \(G\).

In positive characteristic \(p>0\), \(\mathscr{Z}(G)\) is typically not semisimple. While one still has a robust notion of non-degeneracy for finite braided tensor categories (e.g. in the sense of Lyubashenko, equivalent to factorizability in the sense of Etingof–Nikshych–Ostrik by Shimizu [14]), there is in general no computable \(S\)-matrix attached to the simple objects that could play the same role as in the fusion case. Thus, the strategy of [2] does not directly extend to the non-semisimple setting.

Our approach replaces \(S\)-matrix technology with a Hopf-theoretic classification of Hopf quotient pairs of \(D(G)\), and then uses the fact that Hopf quotient pairs of \(D(G)\) encode tensor subcategories of \(\mathscr{Z}(G)\). Indeed, tensor subcategories of \(\operatorname{Rep}(H)\), for a finite dimensional Hopf algebra \(H\), correspond to equivalence classes of Hopf algebra quotient pairs of \(H\) (see, e.g. [15]), so one can study tensor subcategories of \(\mathscr{Z}(G)=\operatorname{Rep}(D(G))\) by classifying Hopf algebra quotient pairs of \(D(G)\). This perspective is particularly well-suited to positive characteristic: although \(S\)-matrices are unavailable, the braiding on \(\operatorname{Rep}(D(G))\) is still controlled by the universal \(R\)-matrix of \(D(G)\), and centralizing conditions can be tested on the Hopf algebra side via the element \(R_{21}R\) (cf. the criterion used in the proof of Theorem 12 below).

The first main result of this paper is a classification of Hopf algebra quotient pairs \((D,\theta)\) of \(D(G)\) in terms of group scheme-theoretical data. We show that every Hopf algebra quotient \(D\) of \(D(G)\) is of the form \[D(K,H,B):=\mathscr{O}(K)^{\mathrm{cop}}\#^{\tau}_{\sigma} \mathbf{k}[G/H],\] where \(K\) and \(H\) are normal subgroup schemes of \(G\) that centralize each other and \(B\colon \mathbf{k}[H]\to \mathscr{O}(K)\) is a \(G\)-equivariant Hopf algebra map, and describe the surjective Hopf algebra map \(\theta:D(G)\twoheadrightarrow D\) (Theorems 6 and 9). Moreover, \(D(K,H,B)\) is always ribbon braided, and we give explicit formulas for its \(R\)-matrix and ribbon element (Corollary 3). We also determine precise criteria for \(D(K,H,B)\) to be triangular or factorizable, yielding large families of quasitriangular Hopf algebras realized as Hopf algebra quotients of \(D(G)\).

The second main result is a complete, group scheme-theoretical description of the tensor subcategory lattice of \(\mathscr{Z}(G)\) and its centralizer theory. Using the above Hopf algebra quotient pairs classification, we show that the assignment \[(K,H,B)\mapsto \mathscr{Z}(K,H,B):=\operatorname{Rep}(D(K,H,B))\] yields a bijection between triples \((K,H,B)\) and tensor subcategories of \(\mathscr{Z}(G)\). We then compute Müger centralizers inside \(\mathscr{Z}(G)\): for each tensor subcategory \(\mathscr{Z}(K,H,B)\), its centralizer is \(\mathscr{Z}(H,K,\overline{B})\) (Theorem 12), generalizing the characteristic-\(0\) picture of [2] from modular-data methods to a purely Hopf-theoretic criterion. As consequences, we obtain explicit criteria for symmetry, non-degeneracy, and Lagrangianity of tensor subcategories of \(\mathscr{Z}(G)\) (Corollary 7).

Finally, using the geometric description of \(\mathscr{Z}(G)\) from [1], we describe the simple and projective objects in \(\mathscr{Z}(K,H,B)\) and compute their Frobenius-Perron dimensions (Theorem 13). In §5, we discuss some special cases and examples illustrating our results. In particular, our factorizability criteria produce families of non-degenerate finite braided tensor categories in positive characteristic (coming from factorizable Hopf algebra quotients of \(D(G)\)), and we exhibit examples in both the constant and connected cases.

Remark 1. The results of this paper can be extended to the twisted Drinfeld double \(D^{\omega}(G)\) of a finite group scheme \(G\) (it is a quasi-Hopf algebra) and its representation category \(\operatorname{Rep}(D^{\omega}(G))\), by using similar ideas and results from [9], [11]. In characteristic \(p=0\), this was done in [2]. 0◻

1.1 Organization↩︎

In §2 we recall background on finite group schemes, Hopf algebras, and Drinfeld doubles. In §3 we construct and classify Hopf algebra quotient pairs of \(D(G)\) and analyze the induced (quasitriangular ribbon) structures on \(D(K,H,B)\). In §4 we apply these results to classify tensor subcategories of \(\mathscr{Z}(G)\), compute their centralizers, and derive criteria for symmetry, nondegeneracy, and Lagrangianity. We then describe the simples and projectives in \(\mathscr{Z}(K,H,B)\) using [1].

1.2 Acknowledgements↩︎

The work of S.G. was supported by Simons Foundation Award 963288.

2 Preliminaries↩︎

We work over an algebraically closed field \(\mathbf{k}\) of characteristic \(p\ge0\). We assume familiarity with the theory of finite tensor categories and finite group schemes over \(\mathbf{k}\), and refer to [16][18] for any unexplained notion.

2.1 Finite group schemes↩︎

A finite group scheme \(G\) over \(\mathbf{k}\) is a finite scheme over \(\mathbf{k}\) whose coordinate algebra \(\mathscr{O}(G)\) is a finite dimensional commutative Hopf algebra (see, e.g., [17], [18]), so that its group algebra \(\mathbf{k}[G]:=\mathscr{O}(G)^*\) is a finite dimensional cocommutative Hopf algebra. We set \(|G|:=\dim_{\mathbf{k}}(\mathscr{O}(G))=\dim_{\mathbf{k}}(\mathbf{k}[G])\).

Let \(G^{\circ}\) be the identity component of \(G\), and let \(G(\mathbf{k})\subseteq G\) be the subgroup of closed points of \(G\). Recall that we have a split exact sequence of finite group schemes \[\label{sesG} 1\to G^{\circ}\xrightarrow{} G \mathrel{\mathop{\rightleftarrows}^{\pi}_{\gamma}} G(\mathbf{k})\to 1.\tag{1}\]

Let \(L\) be a closed subgroup scheme of \(G\), let \[\label{iotaL} \iota=\iota_L=\iota_{L,G}:L\hookrightarrow G\tag{2}\] be the inclusion of group schemes, and let \[\label{qL} q=q_L=q_{G,L}=\iota_{L}^{\sharp}:\mathscr{O}(G)\twoheadrightarrow\mathscr{O}(L)\tag{3}\] be the corresponding surjective Hopf algebra map. Recall [19] that we can choose a section \[\label{muL} \mu=\mu_L:\mathscr{O}(L)\xrightarrow{1:1} \mathscr{O}(G)\tag{4}\] for \(q\), so that \(\mu\) is an \(\mathscr{O}(L)\)-colinear map; that is, \(\varepsilon \mu = \varepsilon\) and \[\label{mucolinear} \mu(a_1)\otimes a_2=\mu(a)_1\otimes q(\mu(a)_2);\quad\forall a\in \mathscr{O}(L),\tag{5}\] such that \(\mu(1)=1\) and \[\label{qLmuLsection} q(\mu(a))=a;\quad \forall a\in \mathscr{O}(L).\tag{6}\] We will denote the dimension of the algebra \(\mathscr{O}(G/L)=\mathscr{O}(G)^L\) by \([G:L]\).

Recall that the right adjoint (or conjugation) action of \(G\) on itself is given by \[\label{right32adjoint32action} {\rm ad_r}:G\times G\to G,\quad (g,f)\mapsto f^{-1}gf;\tag{7}\] that is, \({\rm ad_r}(u)(\tilde{u})=S(u_1)\tilde{u}u_2\) for \(u,\tilde{u}\in\mathbf{k}[G]\), and the algebra comorphism \[\label{coadog} {\rm ad_r}^{\sharp}:\mathscr{O}(G)\to\mathscr{O}(G)\otimes\mathscr{O}(G),\quad b\mapsto b_2\otimes S(b_1)b_3,\tag{8}\] is the right adjoint coaction of \(\mathscr{O}(G)\) on itself. Then \({\rm ad_r}^{\sharp}\) corresponds to the left coadjoint action \(\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\) of \(\mathbf{k}[G]\) on \(\mathscr{O}(G)\), given by \[\label{left32coadjoint32action} \mathbf{k}[G]\otimes\mathscr{O}(G)\to \mathscr{O}(G),\quad u\otimes b\mapsto u \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup b := \left\langle S(b_1)b_3, u \right\rangle b_2.\tag{9}\] Namely, for every \(u,\tilde{u}\in \mathbf{k}[G]\) and \(b\in \mathscr{O}(G)\), we have \[\label{left32coadjoint32action2} \langle u \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup b,\tilde{u}\rangle=\langle b,{\rm ad_r}(u)(\tilde{u})\rangle.\tag{10}\] Clearly, if \(G\) is commutative (that is, \(\mathscr{O}(G)\) is cocommutative), then \(\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\) is trivial.

2.2 Normal subgroup schemes↩︎

Fix a finite group scheme \(G\) over \(\mathbf{k}\) as in §2.1. Let \(H\subseteq G\) be a normal subgroup scheme; that is, \({\rm ad_r}(H\times G)\subseteq H\), so that \(G/H\) is a finite group scheme. Let \(\pi=\pi_H:G\twoheadrightarrow G/H\) be the quotient group scheme morphism. By [19], the exact sequence of Hopf algebras \[\label{gammaH} \mathbf{k}\to \mathbf{k}[H]\xrightarrow{\iota} \mathbf{k}[G]\xrightarrow{\pi} \mathbf{k}[G/H] \to \mathbf{k}\tag{11}\] is cleft. That is, viewing \(\mathbf{k}[G]\) as a right \(\mathbf{k}[G/H]\)-comodule via \[\rho=\rho_H:\mathbf{k}[G]\to \mathbf{k}[G]\otimes\mathbf{k}[G/H],\quad u\mapsto u_1\otimes\pi(u_2),\] we have \(\mathbf{k}[G]^{\text{co} \mathbf{k}[G/H]} = \mathbf{k}[H]\), and we can choose a section \[\label{gamma} \gamma=\gamma_H:\mathbf{k}[G/H]\xrightarrow{1:1} \mathbf{k}[G],\tag{12}\] which is a convolution invertible \(\mathbf{k}[G/H]\)-colinear map; that is, \(\varepsilon \gamma = \varepsilon\) and \[\label{gammacolinear} \gamma(x_1)\otimes x_2=\gamma(x)_1\otimes\pi(\gamma(x)_2);\quad\forall x\in \mathbf{k}[G/H],\tag{13}\] such that \[\pi(\gamma(x))=x;\quad\forall x\in \mathbf{k}[G/H].\]

Consider the map \(\eta=\eta_H:=\operatorname{id}\star(\gamma^{-1}\pi)\); that is, \[\label{etafromgamma} \eta: \mathbf{k}[G] \to \mathbf{k}[H],\quad u\mapsto u_1\gamma^{-1}(\pi(u_2)).\tag{14}\] Note that since \(\gamma\) and \(\gamma^{-1}\) preserve the counit, \[\pi(u_1 \gamma^{-1}(\pi(u_2))) = \pi(u_1) S(\pi(u_2)) = \varepsilon(u) = \varepsilon(\gamma^{-1}\pi(u)) = \varepsilon(u_1 \gamma^{-1}(\pi(u_2))),\] so indeed \(\eta(u) \in \mathbf{k}[G]^{\text{co} \mathbf{k}[G/H]} = \mathbf{k}[H]\).

Lemma 1. The following hold:

  1. \(\eta\) is a \(\mathbf{k}[H]\)-linear retraction for the inclusion map \(\iota:\mathbf{k}[H]\hookrightarrow \mathbf{k}[G]\), such that for every \(x\in \mathbf{k}[G/H]\), we have \(\eta(\gamma(x))=\varepsilon(x)\).

  2. For every \(u\in \mathbf{k}[G]\), we have \(u=\eta(u_1)\gamma(\pi(u_2))\).

  3. For every \(u,\tilde{u}\in \mathbf{k}[G]\), we have \[\eta(u\tilde{u})=\eta(u_1)\gamma(\pi(u_2))_1\eta(\tilde{u}_1)S(\gamma(\pi(u_2))_2)\eta\{\gamma(\pi(u_2))_3\gamma(\pi(\tilde{u}_2))\}.\]

  4. For every \(u\in \mathbf{k}[G]\), we have \(\gamma(\pi(u))=\eta^{-1}(u_1)u_2\).

  5. For every \(u\in \mathbf{k}[G]\), we have \(\eta^{-1}(u)=\gamma(\pi(u_1))S(u_2)\).

Proof. (1) Using (13 ) we verify \(\eta(\gamma(x)) = \gamma(x)_1 \gamma^{-1}(\pi(\gamma(x)_2)) = \gamma(x_1) \gamma^{-1}(x_2) = \varepsilon(x)\).

(2) Since \(\eta= \operatorname{id}\star (\gamma^{-1}\pi)\), we have \(\eta\star (\gamma \pi) = \operatorname{id}\).

(3) By (2), we have \[\begin{align} \\ & = & \eta(u_1)\left\{\gamma(\pi(u_2))_1\eta(\tilde{u}_1)S(\gamma(\pi(u_2))_2)\right\} \gamma(\pi(u_2))_3\gamma(\pi(\tilde{u}_2)), \end{align}\] which implies that \[\eta(u\tilde{u})=\eta(u_1)\left\{\gamma(\pi(u_2))_1\eta(\tilde{u}_1)S(\gamma(\pi(u_2))_2)\right\}\eta\left\{\gamma(\pi(u_2))_3\gamma(\pi(\tilde{u}_2))\right\},\] as claimed.

(4)-(5) Straightforward. ◻

Recall that the Hopf algebra \(\mathbf{k}[G/H]\) measures \(\mathbf{k}[H]\) via \(\cdot\), given by \[\mathbf{k}[G/H]\otimes\mathbf{k}[H]\to \mathbf{k}[H],\quad x\cdot u=\gamma(x_1)u\gamma^{-1}(x_2).\] Recall also that the \(\mathbf{k}\)-linear map \[\label{defnolsigma} \overline{\sigma}: \mathbf{k}[G/H] \otimes \mathbf{k}[G/H] \to \mathbf{k}[H],\quad \overline{\sigma}(x,y)=\gamma(x_1)\gamma(y_1)\gamma^{-1}(x_2y_2),\tag{15}\] is a \(2\)-cocycle, and the \(\mathbf{k}\)-linear map \[\label{defnoltau} \begin{align} & \overline{\tau}: \mathbf{k}[G/H] \to \mathbf{k}[H]\otimes \mathbf{k}[H],\\ & \overline{\tau}(x)= \eta^{-1}(\gamma(x)_1)_1\eta(\gamma(x)_2)\otimes \eta^{-1}(\gamma(x)_1)_2\eta(\gamma(x)_3), \end{align}\tag{16}\] is a co-cocycle. For example, to see that \(\overline{\sigma}\) is well defined, note first that \[\pi(\gamma(x_1)\gamma(y_1)\gamma^{-1}(x_2y_2)) = x_1y_1S(x_2y_2) = \varepsilon(xy).\] On the other hand, using (13 ) we have \[\begin{align} \\ & = & \varepsilon(\gamma^{-1}(\pi(\varepsilon(\gamma(x)_1) \gamma(x)_2 \varepsilon(\gamma(y)_1)\gamma(y)_2))) \\ & = & \varepsilon(\gamma^{-1}(\pi(\gamma(x)\gamma(y)))) = \varepsilon(\gamma^{-1}(xy))= \varepsilon(xy). \end{align}\] This shows that \(\gamma(x_1)\gamma(y_1)\gamma^{-1}(x_2y_2) \in \mathbf{k}[G]^{\text{co} \mathbf{k}[G/H]} = \mathbf{k}[H]\), as required.

Finally, it is well known (see e.g. [20]) that the map \[{\rm f}:\mathbf{k}[G]\to \mathbf{k}[H]\#_{\overline{\sigma}}^{\overline{\tau}} \mathbf{k}[G/H],\quad u\mapsto \eta\left(u_1\right)\# \pi\left(u_2\right),\] is a Hopf algebra isomorphism, whose inverse is given by \[{\rm f}^{-1}:\mathbf{k}[H]\#_{\overline{\sigma}}^{\overline{\tau}}\mathbf{k}[G/H]\to \mathbf{k}[G],\quad v\# x\mapsto v\gamma(x).\] For example, using (13 ) and the fact that \(\eta\) is \(\mathbf{k}[H]\)-linear, we compute \[\begin{align} \\ & = & v_1\eta\left(\gamma(x)_1\right)\otimes\varepsilon(v_2)\pi\left(\gamma(x)_2\right)= v\eta\left(\gamma(x)_1\right)\otimes\pi\left(\gamma(x)_2\right)\\ & = & v\eta\left(\gamma(x_1)\right)\otimes x_2=v\varepsilon(x_1)\otimes x_2=v\otimes x, \end{align}\] and \[\begin{align} \\ & = & u_1\gamma^{-1}(\pi(u_2))\gamma\left(\pi\left(u_3\right) \right)=u_1\varepsilon(\pi(u_2))=u, \end{align}\] so \({\rm f}\) and \({\rm f}^{-1}\) are indeed inverse of each other.

Remark 2. (1) If \(\gamma\) (12 ) is an algebra map then \(\overline{\sigma}\) (15 ) is trivial.

(2) If \(\eta\) (14 ) is a coalgebra map, equivalently if \(\gamma\) (12 ) is a coalgebra map (e.g. if \(H=1\), or \(G=G(\mathbf{k})\) is constant), then \(\overline{\tau}\) (16 ) is trivial. Indeed, since \(\mathbf{k}[G]\) is cocommutative, \(\eta^{-1}=(\gamma\pi)\star S\) is also a coalgebra map (see Lemma 1(4)), so \[\begin{align} \\ & = & \eta^{-1}(\gamma(x_1))_1\eta(\gamma(x_2))\otimes \eta^{-1}(\gamma(x_1))_2\eta(\gamma(x_3))\\ & = & \eta^{-1}(\gamma(x_1))_1\varepsilon(x_2)\otimes \eta^{-1}(\gamma(x_1))_2\varepsilon(x_3)\\ & = & \eta^{-1}(\gamma(x))_1\otimes \eta^{-1}(\gamma(x))_2= \eta^{-1}(\gamma(x_1))\otimes \eta^{-1}(\gamma(x_2))\\ & = & \varepsilon(x_1)\otimes \varepsilon(x_2)=\varepsilon(x)1\otimes 1, \end{align}\] as claimed. 0◻

2.3 The Drinfeld double of a finite group scheme↩︎

Fix a finite group scheme \(G\) over \(\mathbf{k}\) as in §2.1. Recall that the Drinfeld double \[D(G)=\mathscr{O}(G)^{{\rm cop}} \bowtie \mathbf{k}[G]\] of \(\mathbf{k}[G]\) is the tensor coalgebra \(\mathscr{O}(G)^{{\rm cop}} \otimes \mathbf{k}[G]\), equipped with the product rule \[(b \bowtie u)(b' \bowtie u') = b(u_1 \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup b') \bowtie u_2u',\] where \(\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\) is defined in (9 ). Recall that \(D(G)\) is an involutive Hopf algebra, such that the natural maps \[\mathbf{k}[G] \hookrightarrow D(G),\quad {\rm and}\quad \mathscr{O}(G)^{{\rm cop}} \hookrightarrow D(G)\] are Hopf algebra inclusions. Since for every \(u \in \mathbf{k}[G]\) and \(b \in \mathscr{O}(G)\), \[\begin{align} \\ & = & (u_1 \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup b) \bowtie u_2S(u_3)= (u_1 \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup b) \bowtie \varepsilon(u_2) = (u \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup b) \bowtie 1, \end{align}\] it follows that \(\mathscr{O}(G)\) is a normal Hopf subalgebra of \(D(G)\), so we have an exact sequence of Hopf algebras \[\mathbf{k}\rightarrow \mathscr{O}(G) \rightarrow D(G) \rightarrow D(G)/(D(G)\mathscr{O}(G)^+) \rightarrow \mathbf{k}.\] Since the map \[\label{qkg} D(G)/(D(G)\mathscr{O}(G)^+) \to \mathbf{k}[G],\quad [b \bowtie u]\mapsto \varepsilon(b)u,\tag{17}\] is a Hopf algebra isomorphism, we have an exact sequence of Hopf algebras \[\mathbf{k}\rightarrow \mathscr{O}(G) \rightarrow D(G) \rightarrow \mathbf{k}[G] \rightarrow \mathbf{k}.\]

Finally, let \(\mathcal{B}\) be a basis for \(\mathbf{k}[G]\), and let \(\{\delta_u\mid u\in\mathcal{B}\}\) be the dual basis for \(\mathscr{O}(G)\). Recall that the element \[\label{rmatrix} R:=\sum_{u \in \mathcal{B}} (1\bowtie u) \otimes (\delta_u\bowtie 1)\tag{18}\] is an \(R\)-matrix for \(D(G)\), and \((D(G),R)\) is factorizable and ribbon, with ribbon element \[\label{ribbon} V:=\sum_{u \in \mathcal{B}} S(\delta_u)\bowtie u.\tag{19}\]

2.4 The representation category of \(D(G)\)↩︎

Fix a finite group scheme \(G\) over \(\mathbf{k}\) as in §2.1. Let \({\rm ad_{\ell}}\) be the left adjoint action of \(G\) on itself, defined by \[{\rm ad_{\ell}}(u)(\tilde{u})=u_1\tilde{u}S(u_2);\quad \forall u,\tilde{u}\in \mathbf{k}[G].\] Let \({\rm C}:=G/{\rm ad_{\ell}}\) be the finite quotient scheme of conjugacy orbits in \(G\) [1], [11], and let \({\rm p}:G\twoheadrightarrow {\rm C}:=G/{\rm ad_{\ell}}\) be the quotient scheme morphism [17]. Then \({\rm p}^{\sharp}:\mathscr{O}({\rm C})\xrightarrow{1:1} \mathscr{O}(G)\) is an injective algebra map, and \[\text{im}({\rm p}^{\sharp})=\mathscr{O}(G)^{{\rm co}G}:=\{b\in \mathscr{O}(G)\mid {\rm ad_{\ell}}^{\sharp}(b)=1\otimes b\}\] is a subalgebra of \(\mathscr{O}(G)\), so that \(\mathscr{O}({\rm C})=\mathscr{O}(G)^{{\rm co}G}\) via \({\rm p}^{\sharp}\).

Given a closed point \(g\in G(\mathbf{k})\), consider the scheme morphism \[\label{adg} {\rm ad}_g:G\to G,\quad f\mapsto {\rm ad_{\ell}}(g,f)=fgf^{-1},\tag{20}\] and let \[\label{Cg} C_g:=\text{im}({\rm ad}_g)\subset G\tag{21}\] be the conjugacy orbit of \(g\) [1], [11]. Then \[\mathbf{k}[C_g]:=\{{\rm ad_{\ell}}(u)(g)\mid u\in \mathbf{k}[G]\}\] is a subcoalgebra of \(\mathbf{k}[G]\), \(C_g(\mathbf{k})\subset G(\mathbf{k})\) is the conjugacy class of \(g\) in \(G(\mathbf{k})\), and \({\rm C}(\mathbf{k})=\{C_g\mid g\in G(\mathbf{k})\}\). Also, let \[\label{Gg} G_g:=\{f\in G\mid {\rm ad}_g(f)=g\}\tag{22}\] be the centralizer of \(g\) in \(G\); it is a subgroup scheme of \(G\), so that \[\mathbf{k}[G_g]:=\{u\in \mathbf{k}[G]\mid ug=gu\}\] is a Hopf subalgebra of \(\mathbf{k}[G]\). The scheme morphism \({\rm ad}_g\) (20 ) factors through the finite quotient scheme \(G/G_g\), and induces a canonical scheme isomorphism \[\label{iotag} i_g:G/G_g\xrightarrow{\cong} C_g\tag{23}\] (see [17] for more details). In other words, the map \[i_g^{\sharp}:\mathscr{O}(C_g)\to \mathscr{O}(G/G_g)=\mathscr{O}(G)^{G_g}\subseteq \mathscr{O}(G),\quad \langle i_g^{\sharp}(c),u\rangle=\langle c,u_1gS(u_2)\rangle,\] is an algebra isomorphism.

Recall that \(\mathscr{O}(G/G_g)\subseteq \mathscr{O}(G)\) is a left coideal subalgebra; that is, \[\Delta\left(\mathscr{O}(G/G_g)\right)\subset \mathscr{O}(G)\otimes\mathscr{O}(G/G_g).\] Let \(q_g:=q_{G_g}:\mathscr{O}(G)\twoheadrightarrow \mathscr{O}(G_g)\) be as in (3 ), and consider the Hopf-Galois extension \[0\to \mathscr{O}(G/G_g)\hookrightarrow \mathscr{O}(G)\xrightarrow{q_g}\mathscr{O}(G_g)\to 0,\] where we view \(\mathscr{O}(G)\) as a right \(\mathscr{O}(G_g)\)-comodule via \[\rho_g:\mathscr{O}(G)\to \mathscr{O}(G)\otimes\mathscr{O}(G_g),\quad b\mapsto b_1\otimes q_g(b_2),\] so that \(\mathscr{O}(G/G_g)=\mathscr{O}(G)^{\text{co} \mathscr{O}(G_g)}=\{b\in \mathscr{O}(G)\mid b_1\otimes q_g(b_2)=b\otimes 1\}\subseteq \mathscr{O}(G)\). Let \[\mu_g:=\mu_{G_g}:\mathscr{O}(G_g)\xrightarrow{1:1}\mathscr{O}(G)\] be a section for \(q_g\) as in (4 ), and let \[\alpha_g:\mathscr{O}(G)\twoheadrightarrow\mathscr{O}(G/G_g),\quad b\mapsto b_1\mu_g^{-1}(q_g(b_2)),\] be a retraction for the inclusion map \(\mathscr{O}(G/G_g)\subseteq \mathscr{O}(G)\); it is \(\mathscr{O}(G/G_g)\)-linear. Recall that \(\mu_g\) is a convolution invertible \(\mathscr{O}(G/G_g)\)-colinear map; that is, \(\varepsilon \mu_g = \varepsilon\) and \[\label{mu-gcolinear} \mu_g(d_1)\otimes d_2=\mu_g(d)_1\otimes q_g(\mu_g(d)_2);\quad\forall d\in \mathscr{O}(G_g),\tag{24}\] such that for every \(d\in \mathscr{O}(G_g)\), we have \[\label{mu-greta-g} q_g(\mu_g(d))=d\quad and \quad\alpha_g(\mu_g(d))=\varepsilon(d).\tag{25}\]

For each \(C\in {\rm C}(\mathbf{k})\) (21 ), let \(\pi_C:C\twoheadrightarrow C(\mathbf{k})\) and \(\gamma_C:C(\mathbf{k})\xrightarrow{1:1} C\) be the scheme morphisms obtained from \(\pi:G\twoheadrightarrow G(\mathbf{k})\) and \(\gamma:G(\mathbf{k})\xrightarrow{1:1} G\) (1 ) by restriction, and define the \(\mathscr{O}(G)\)-linear algebra maps \[\begin{gather} \chi_{C}:=\operatorname{id}\otimes\gamma_{C}^{\sharp}:\mathscr{O}(G^{\circ})\otimes\mathscr{O}(C)\twoheadrightarrow \mathscr{O}(G^{\circ})\otimes\mathscr{O}(C(\mathbf{k})),\,\,\,{\rm and}\\ \nu_{C}:=\operatorname{id}\otimes\pi_{C}^{\sharp}:\mathscr{O}(G^{\circ})\otimes\mathscr{O}(C(\mathbf{k}))\xrightarrow{1:1}\mathscr{O}(G^{\circ})\otimes\mathscr{O}(C). \end{gather}\] (See [1], [11] for more details.)

Now let \(\mathscr{Z}(G):=\operatorname{Rep}(D(G))\) be the category of finite dimensional \(\mathbf{k}\)-representations of \(D(G)\); it is a finite non-degenerate ribbon braided tensor category. Recall [9] that there is a canonical tensor equivalence \[\label{the32center32is32gequiv} {\rm Coh}(G)^{G}\simeq \mathscr{Z}(G),\tag{26}\] where \({\rm Coh}(G)^{G}\) is the category of \(G\)-equivariant sheaves on \(G\) with respect to the right conjugation action of \(G\) on itself (7 ). That is, an object of \({\rm Coh}(G)^{G}\) is an object \(X\in {\rm Coh}(G)\) equipped with a right \(\mathscr{O}(G)\)-comodule structure \(\rho:X\to X\otimes\mathscr{O}(G)\), such that \(\rho(a\cdot x)={\rm ad_r}^{\sharp}(a)\cdot \rho(x)\). In particular, \(\mathscr{Z}(G)\) is a group scheme-theoretical category [9].

For each \(C\in {\rm C}(\mathbf{k})\), let \(\mathscr{Z}(G)_{C}\subset \mathscr{Z}(G)\) be the full Abelian subcategory consisting of all objects annihilated by the defining ideal \(\mathscr{I}(C)\subset \mathscr{O}(G)\) of \(C\), and let \(\overline{\mathscr{Z}(G)_{C}}\) be the Serre closure of \(\mathscr{Z}(G)_{C}\) inside \(\mathscr{Z}(G)\); that is, \(\overline{\mathscr{Z}(G)_{C}}\) is the full Abelian subcategory of \(\mathscr{Z}(G)\) consisting of all objects whose composition factors belong to \(\mathscr{Z}(G)_{C}\).

Theorem 3. [1]The following hold:

  1. For each \(C_g\in {\rm C}(\mathbf{k})\), with representative \(g\in C_g(\mathbf{k})\), there is an equivalence of Abelian categories \[\label{funfc} \mathbf{F}_{C_g}:{\rm Corep}(\mathscr{O}(G_g))\xrightarrow{\simeq} \mathscr{Z}(G)_{C_g},\,\,\,(M,\rho_M)\mapsto \left(\mathscr{O}(C_g)\otimes M,\rho_M^g\right),\tag{27}\] where \(\rho_M:M\to \mathscr{O}(G_g)\otimes M\), \(m\mapsto \sum m^{(-1)}\otimes m^{(0)}\), and \[\begin{align} & \rho_M^g:\mathscr{O}(C_g)\otimes M\to \mathscr{O}(C_g)\otimes M\otimes \mathscr{O}(G),\\ & \rho_M^g(c\otimes m)= \left(i_g^{-1}\right)^{\sharp}\alpha_{g}\left(i_g^{\sharp}(c)_1\mu_g\left(m^{(-1)}\right)_1 \right)\otimes m^{(0)}\otimes i_g^{\sharp}(c)_2\mu_g\left(m^{(-1)}\right)_2. \end{align}\] Here, \(\mathscr{O}(G)\) acts on the first factor of \(\mathscr{O}(C_g)\otimes M\) via the surjective algebra map \(q_{C_g}:\mathscr{O}(G)\twoheadrightarrow \mathscr{O}(C_g)\).

    In particular, the composition functor \[\operatorname{Rep}(G)\simeq {\rm Corep}(\mathscr{O}(G))\xrightarrow{\mathbf{F}_{1}}\mathscr{Z}(G)_1\hookrightarrow \mathscr{Z}(G)\] coincides with the canonical embedding \(\operatorname{Rep}(G)\hookrightarrow \mathscr{Z}(G)\) of braided categories.

  2. For each \(C_g\in {\rm C}(\mathbf{k})\), with representative \(g\in C_g(\mathbf{k})\), there is a bijection between equivalence classes of simple objects \((M,\rho_M)\in {\rm Corep}(\mathscr{O}(G_g))\) and simple objects of \(\mathscr{Z}(G)_{C_g}\), assigning \((M,\rho_M)\) to \(\mathbf{F}_{C_g}(M,\rho_M)\). Moreover, we have a direct sum decomposition of Abelian categories \[\mathscr{Z}(G)=\bigoplus_{C_g\in {\rm C}(k)}\overline{\mathscr{Z}(G)_{C_g}},\] and \(\overline{\mathscr{Z}(G)_{1}}\subseteq \mathscr{Z}(G)\) is a braided subcategory. In particular, if \(G\) is connected then the simples of \(\mathscr{Z}(G)\) are precisely those of \(\operatorname{Rep}(G)\simeq {\rm Corep}(\mathscr{O}(G))\).

  3. For each simple \((M,\rho_M)\in {\rm Corep}(\mathscr{O}(G_g))\), with projective cover \(P_{G_g}(M,\rho_M)\), we have \[P_{\mathscr{Z}(G)}\left(\mathbf{F}_{C_g}(M,\rho_M)\right)\cong \left(\mathscr{O}(G^{\circ})\otimes\mathscr{O}(C_g(\mathbf{k}))\otimes P_{G_g}(M,\rho_M),R_M^g\right),\] where \(\mathscr{O}(G)\) acts diagonally on the first two factors, and \[R_{M}^g:=\left(\chi_{C_g}\otimes\operatorname{id}^{\otimes 2}\right)\left(\operatorname{id}_{\mathscr{O}(G^{\circ})}\otimes\rho_{P_{G_g}(M,\rho_M)}^g\right)\left(\nu_{C_g}\otimes\operatorname{id}\right).\]

  4. For each \((M,\rho_M)\in {\rm Corep}(\mathscr{O}(G_g))\), we have \[{\rm FPdim}\left(\mathbf{F}_{C_g}(M,\rho_M)\right)=|C_g|{\rm dim}_{\mathbf{k}}\left(M\right),\quad\text{and}\] \[{\rm FPdim}\left(P_{\mathscr{Z}(G)}\left(\mathbf{F}_{C_g}(M,\rho_M)\right)\right)=[G:G_g(\mathbf{k})]{\rm dim}_{\mathbf{k}}\left(P_{G_g}(M,\rho_M)\right).\qquad\qquad\qquad\qquad\qed\]

3 Hopf algebra quotients of \(D(G)\)↩︎

Fix a finite group scheme \(G\) over \(\mathbf{k}\) as in §2.1.

3.1 Construction of Hopf quotients of \(D(G)\)↩︎

Let \(K\) be a normal subgroup scheme of \(G\). Let \(q_K: \mathscr{O}(G) \twoheadrightarrow \mathscr{O}(K)\) be the corresponding surjective Hopf algebra map, and \[\label{mu} \mu_K:\mathscr{O}(K)\xrightarrow{1:1} \mathscr{O}(G)\tag{28}\] be a section for \(q_{K}\) as in (3 )-(4 ). Since \(K\) is normal in \(G\), the Hopf subalgebra \(\mathscr{O}(G/K)\) of \(\mathscr{O}(G)\) is stable under the left coadjoint \(\mathbf{k}[G]\)-action (9 ), so we obtain a well defined action \(*\) of \(\mathbf{k}[G]\) on \(\mathscr{O}(K)\), given by \[\label{themeasureofog} \mathbf{k}[G] \otimes \mathscr{O}(K) \to \mathscr{O}(K),\quad u\otimes a\mapsto u * a:= q_K(u \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\mu_K(a)),\tag{29}\] which is independent of the choice of \(\mu_K\). Indeed, if \(\mu_K':\mathscr{O}(K)\to \mathscr{O}(G)\) is another section of \(q_K\), then \(\mu_K'(a)-\mu_K(a)\in \mathscr{O}(G/K)^+\mathscr{O}(G)\) for every \(a\in \mathscr{O}(K)\). Since the Hopf ideal \(\mathscr{O}(G/K)^+\mathscr{O}(G)\) is stable under the left coadjoint \(\mathbf{k}[G]\)-action (9 ), we have \(u \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup(\mu_K'(a)-\mu_K(a)) \in \mathscr{O}(G/K)^+\mathscr{O}(G)\) for all \(u \in \mathbf{k}[G]\). Hence, \[q_K (u \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\mu_K'(a)) = q_K (u \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\mu_K(a)),\] so \(*\) (29 ) is independent of the choice of \(\mu_K\), as claimed.

In particular, we have \[\label{piyaction} u * q_K(b):= q_K(u \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup b);\quad \forall u\in \mathbf{k}[G],\, b\in \mathscr{O}(G).\tag{30}\]

Suppose now that \(H\) is another normal subgroup scheme of \(G\), so that we have an exact sequence of Hopf algebras \[\mathbf{k}\xrightarrow{\iota_H} \mathbf{k}[H]\to \mathbf{k}[G]\xrightarrow{\pi_H} \mathbf{k}[G/H] \to \mathbf{k},\] and choose a section \(\gamma_H\) as in (12 ). Assume further that \(H\) and \(K\) centralize each other; that is, \(vw=wv\) for every \(v\in \mathbf{k}[H]\) and \(w \in \mathbf{k}[K]\). Equivalently, \[{\rm ad_{r}}(v)(w)=S(v_1)wv_2 = \varepsilon(v)w;\quad\forall v\in \mathbf{k}[H],\,w \in \mathbf{k}[K].\] Then for any \(v \in \mathbf{k}[H]\) and \(b \in \mathscr{O}(G)\), we have for every \(w \in \mathbf{k}[K]\), \[\begin{align} \\ & = & {\left\langle b, {\rm ad_{r}}(v)(\iota_K(w)) \right\rangle} = {\left\langle b, \varepsilon(v)\iota_K(w) \right\rangle}={\left\langle \varepsilon(v)q_K(b),w \right\rangle}, \end{align}\] so \(q_K(v \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup b) = \varepsilon(v)q_K(b)\). Thus, (29 ) induces a well defined \(\mathbf{k}\)-linear map \(\cdot\), given by \[\label{themeasure} \mathbf{k}[G/H] \otimes \mathscr{O}(K) \to \mathscr{O}(K),\quad x \otimes a\mapsto x\cdot a:=\gamma_H(x)*a =q_K(\gamma_H(x)\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\mu_K(a)),\tag{31}\] which is independent of the choice of \(\gamma_H\) (as well as \(\mu_K\)). Indeed, if \(\gamma_H':\mathbf{k}[G/H]\to \mathbf{k}[G]\) is another section of \(\pi_H\), then for each \(x\in \mathbf{k}[G/H]\), we have \(\gamma_H'(x)-\gamma_H(x)\in \mathbf{k}[G]\mathbf{k}[H]^+\). But for any \(uv\), \(u\in \mathbf{k}[G]\) and \(v\in \mathbf{k}[H]^+\), we have that \[(uv)*a=u*(v*a)=u*(q_K(v \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\mu_K(a)))=u*(\varepsilon(v)q_K(\mu_K(a)))=0\] for every \(a\in \mathscr{O}(K)\). Therefore, for every \(a\in \mathscr{O}(K)\), \[\gamma_H'(x)*a = (\gamma_H(x)+\gamma_H'(x)-\gamma_H(x))*a = \gamma_H(x)*a,\] so \(\cdot\) (31 ) is independent of the choice of \(\gamma_H\), as claimed.

In particular, we have \[\label{piyactiononq} \pi_H(u)\cdot a=u*a;\quad \forall u\in \mathbf{k}[G],\, a\in \mathscr{O}(K),\tag{32}\] and by (30 ), we have \[\label{piyactiononq0} \pi_H(u)\cdot q_K(b)=u*q_K(b)= q_K(u \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup b);\quad \forall u\in \mathbf{k}[G],\, b\in \mathscr{O}(G).\tag{33}\]

Lemma 2. The Hopf algebra \(\mathbf{k}[G/H]\) acts and measures \(\mathscr{O}(K)\) via (31 ); that is, for every \(x,y\in \mathbf{k}[G/H]\) and \(a,\tilde{a}\in \mathscr{O}(K)\), we have \[x\cdot(y\cdot a)=(xy)\cdot a,\quad x \cdot 1=\varepsilon(x),\quad \text{and}\quad x \cdot (a\tilde{a})=(x_1 \cdot a)(x_2 \cdot \tilde{a}).\]

Proof. First we have \((xy)\cdot a=\gamma_H(xy)*a\), and \[x\cdot(y\cdot a)=x\cdot (\gamma_H(y)*a)=\gamma_H(x)*(\gamma_H(y)*a)=(\gamma_H(x)\gamma_H(y))*a,\] so the first equation follows from \(\gamma_H(xy)-\gamma_H(x)\gamma_H(y)\in \mathbf{k}[G]\mathbf{k}[H]^+\).

Second, since \(\mu_K(1)=1\) and \(\varepsilon(\gamma_H(x))=\varepsilon(x)\), we have for every \(x\in \mathbf{k}[G/H]\), \[x \cdot 1= q_K(\gamma_H(x) \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup 1) = q_K(\varepsilon(\gamma_H(x))) = \varepsilon(x),\] as claimed.

Finally, since we have \[\label{useful} \begin{align} & q_K(\mu_K(a\tilde{a}))=a\tilde{a}=q_K(\mu_K(a)\mu_K(\tilde{a})),\, \text{and}\\ & (\pi_H\otimes \pi_H)(\gamma_H(x)_1\otimes \gamma_H(x)_2)=\Delta(x)=(\pi_H\otimes \pi_H)(\gamma_H(x_1)\otimes \gamma_H(x_2)), \end{align}\tag{34}\] it follows that \[\begin{align} \\ & = & q_K(\gamma_H(x)_1 \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\mu_K(a))(\gamma_H(x)_2 \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\mu_K(\tilde{a}))\\ & = & q_K(\gamma_H(x)_1 \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\mu_K(a))q_K(\gamma_H(x)_2 \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\mu_K(\tilde{a}))\\ & = & q_K(\gamma_H(x_1) \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\mu_K(a))q_K(\gamma_H(x_2) \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\mu_K(\tilde{a}))= (x_1 \cdot a)(x_2 \cdot \tilde{a}), \end{align}\] as claimed, where we used (34 ) in the second and fifth equations. ◻

Now suppose in addition that we have a Hopf algebra map \[\label{B} B : \mathbf{k}[H] \to \mathscr{O}(K),\tag{35}\] which is \(G\)-equivariant, in the sense that \[\label{Binv} \pi_H(u)\cdot B(v)=u*B(v)=B({\rm ad_{\ell}}(u)(v));\quad \forall u \in \mathbf{k}[G],\,v \in \mathbf{k}[H].\tag{36}\]

Remark 4. (1) The \(G\)-equivariant Hopf algebra map \(B\) (35 ) can be viewed as a \(G\)-invariant bicharacter \(B:H\times K\to \mathbb{G}_m\), in the sense that the Hopf algebra pairing \[\label{Bpairing} \mathbf{k}[H]\otimes\mathbf{k}[K]\to \mathbf{k},\quad v\otimes w\mapsto \left\langle B(v),w\right\rangle,\tag{37}\] is \(G\)-invariant; that is, \[\label{G-invariant} \left\langle B({\rm ad_{\ell}}(u_1)(v)),{\rm ad_{\ell}}(u_2)(w)\right\rangle=\varepsilon(u)\left\langle B(v),w\right\rangle\tag{38}\] or equivalently, \[\langle B(\operatorname{ad}_{\ell}(u)(v)), w\rangle = \langle B(v), \operatorname{ad}_{\ell}(S(u))(w) \rangle\] for every \(u \in \mathbf{k}[G]\), \(v \in \mathbf{k}[H]\) and \(w \in \mathbf{k}[K]\).

(2) Since the image of \(B\) (35 ) is a cocommutative Hopf subalgebra of \(\mathscr{O}(K)\), there exists a normal subgroup scheme \(L\subseteq K\), such that \(K/L\) is commutative, so that we have \(\text{im}(B)=\mathscr{O}(K/L)=\mathbf{k}[\left(K/L\right)^{\vee}]\), where \(\left(K/L\right)^{\vee}\) is the Cartier dual of \(K/L\) (see, e.g. [1]). Thus, if \({\rm Ker}(B)=\mathbf{k}[N]^+\mathbf{k}[H]\), \(N\subseteq H\) a normal subgroup scheme, then \(H/N\) is a commutative group scheme, and \(B\) induces a \(G\)-equivariant group scheme isomorphism \(B:H/N\xrightarrow{\cong}\left(K/L\right)^{\vee}\). 0◻

Now let \(\eta_H\), \(\overline{\sigma}\) and \(\overline{\tau}\) be as in (14 ), (15 ) and (16 ), respectively, and define the \(\mathbf{k}\)-linear maps \[\sigma:=B\overline{\sigma}\quad\text{and}\quad\tau:=B^{\otimes 2}\overline{\tau};\] that is, \[\label{defnsigma} \sigma : \mathbf{k}[G/H] \otimes \mathbf{k}[G/H] \to \mathscr{O}(K),\quad \sigma(x,y)=B\left(\gamma_H(x_1)\gamma_H(y_1)\gamma_H^{-1}(x_2y_2)\right),\tag{39}\] and \[\label{defntau} \begin{align} & \tau : \mathbf{k}[G/H] \to \mathscr{O}(K)\otimes \mathscr{O}(K),\\ & \tau(x)=(B\otimes B) \left\{ \eta^{-1}_H(\gamma_H(x)_1)_1\eta_H(\gamma_H(x)_2)\otimes \eta^{-1}_H(\gamma_H(x)_1)_2\eta_H(\gamma_H(x)_3) \right\}, \end{align}\tag{40}\] and write \(\tau(x)=\tau(x)^1\otimes \tau(x)^2\). Note that \(\tau(x)^1\otimes \tau(x)^2=\tau(x)^2\otimes \tau(x)^1\), by cocommutativity of \(\mathbf{k}[G]\).

Remark 5. (1) By the discussion preceding Remark 2, \(\sigma\) and \(\tau\) are well-defined.

(2) By Remark 2, if \(\gamma_H\) is an algebra map then \(\sigma\) (39 ) is trivial, and if \(\eta_H\) (14 ) is a coalgebra map, equivalently if \(\gamma_H\) (12 ) is a coalgebra map (e.g. if \(H=1\), or \(G=G(\mathbf{k})\) is constant), then \(\tau\) (40 ) is trivial.

(3) If \(B=1\) then both \(\sigma\) (39 ) and \(\tau\) (40 ) are trivial. 0◻

Lemma 3. Set \(\pi:=\pi_H\), and \(\eta:=\eta_H\). For every \(u,\tilde{u}\in\mathbf{k}[G]\), the following hold:

  1. \(\sigma(\pi(u),\pi(\tilde{u}))=B\left\{\eta(\gamma(\pi(u))\gamma(\pi(\tilde{u})))\right\}\).

  2. \(\tau(\pi(u))=(B\otimes B)\left\{\eta^{-1}(u_1)_1\eta(u_2)\otimes\eta^{-1}(u_1)_2\eta(u_3)\right\}\).

Proof. (1) For every \(x,y\in \mathbf{k}[G/H]\), we have by (13 ), \[\begin{align} \\ & = & \gamma(x)_1\gamma(y)_1\gamma^{-1}(\pi(\gamma(x)_2)\pi(\gamma(y)_2))= \gamma(x_1)\gamma(y_1)\gamma^{-1}(x_2y_2), \end{align}\] so the claim follows.

(2) Since \(\gamma(\pi(u))=\eta^{-1}(u_1)u_2\) by Lemma 1(4), we have \[\gamma(\pi(u))_1\otimes\gamma(\pi(u))_2\otimes\gamma(\pi(u))_3=\eta^{-1}(u_1)_1u_2\otimes\eta^{-1}(u_1)_2u_3\otimes\eta^{-1}(u_1)_3u_4.\] Thus, we have \[\begin{align} \\ & = & B^{\otimes 2} \{ \eta^{-1}(\eta^{-1}(u_1)_1u_2)_1\eta(\eta^{-1}(u_1)_2u_3)\otimes \eta^{-1}(\eta^{-1}(u_1)_1u_2)_2\eta(\eta^{-1}(u_1)_3u_4) \}\\ & = & B^{\otimes 2} \{\eta^{-1}(u_2)_1S(\eta^{-1}(u_1)_1) \eta^{-1}(u_1)_2\eta(u_3)\otimes \eta^{-1}(u_2)_2S(\eta^{-1}(u_1)_3) \eta^{-1}(u_1)_4\eta(u_4)\}\\ & = & B^{\otimes 2}\{\eta^{-1}(u_2)_1\varepsilon(\eta^{-1}(u_1)_1) \eta(u_3)\otimes\eta^{-1}(u_2)_2S(\eta^{-1}(u_1)_2) \eta^{-1}(u_1)_3\eta(u_4)\}\\ & = & B^{\otimes 2}\{\eta^{-1}(u_2)_1\eta(u_3)\otimes \eta^{-1}(u_2)_2S(\eta^{-1}(u_1)_1) \eta^{-1}(u_1)_2\eta(u_4)\}\\ & = & B^{\otimes 2}\{\eta^{-1}(u_2)_1\eta(u_3)\otimes \eta^{-1}(u_2)_2\varepsilon(\eta^{-1}(u_1))\eta(u_4)\}\\ & = & B^{\otimes 2}\{\eta^{-1}(u_2)_1\eta(u_3)\otimes \eta^{-1}(u_2)_2\varepsilon(u_1)\eta(u_4)\}= B^{\otimes 2} \{\eta^{-1}(u_1)_1\eta(u_2)\otimes\eta^{-1}(u_1)_2\eta(u_3)\}, \end{align}\] as claimed. ◻

Theorem 6. Let \(K,H\subseteq G\) be commuting normal subgroup schemes of \(G\), and let \(\cdot\), \(B\), \(\sigma\), and \(\tau\) be as in (31 ), (35 ), (39 ) and (40 ), respectively. Then there exists a pair \(\left(D(K,H,B),\theta\right)\), such that the following hold:

  1. \[D(K,H,B)=\mathscr{O}(K)^{{\rm cop}} \#^{\tau}_{\sigma} \mathbf{k}[G/H]\] is a Hopf algebra with multiplication given by \[(a \# x)(\tilde{a} \# \tilde{x}) = a(x_1 \cdot \tilde{a}) \sigma(x_2, \tilde{x}_1) \# x_3 \tilde{x}_2,\] comultiplication map \(\delta\) given by \[\delta(a\# x)=\left(a_2\tau(x_1)^1\# x_2\right)\otimes \left(a_1\tau(x_1)^2\# x_3\right),\] and antipode map \(S\) given by \[S(a\# x)=(1\# S(x))(S(a)\# 1).\]

  2. \[\theta:D(G)\to D(K,H,B),\quad b\bowtie u\mapsto q_K(b)B(\eta_H(u_1))\# \pi_H(u_2),\] is a surjective Hopf algebra map whose kernel is the ideal generated by \(\mathscr{O}\left(G/K\right)^+\) and the vector subspace \(\left\{\mu_K(B(v))\bowtie 1 - 1\bowtie v\mid v\in \mathbf{k}[H]\right\}\).

Proof. It suffices to show that \(\theta\) is a surjective map, such that \[\label{p1} \theta\left((b\bowtie u)(\tilde{b}\bowtie \tilde{u})\right)=\theta(b\bowtie u)\theta(\tilde{b}\bowtie \tilde{u}),\quad\text{and}\tag{41}\] \[\label{p2} \theta(b_2\bowtie u_1) \otimes \theta(b_1\bowtie u_2)=\delta(\theta(b\bowtie u))\tag{42}\] for every \(b,\tilde{b} \in \mathscr{O}(G)\) and \(u,\tilde{u} \in \mathbf{k}[G]\).

Set \(\pi:=\pi_H\), \(\gamma:=\gamma_H\), \(\eta:=\eta_H\), \(\mu:=\mu_K\), and \(q:=q_K\).

First we verify (41 ). On one hand, we have \[\begin{align} \\ & = & q(b(u_1 \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\tilde{b}))B\left\{\eta(u_2)\gamma(\pi(u_3))_1\eta(\tilde{u}_1)S(\gamma(\pi(u_3))_2)\eta\left\{\gamma(\pi(u_3))_3\gamma(\pi(\tilde{u}_2))\right\}\right\} \# \pi(u_4 \tilde{u}_3)\\ & = & q(b(u_1 \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\tilde{b}))B\left\{\eta(u_2)\left\{{\rm ad_{\ell}}(\gamma(\pi(u_3))_1)(\eta(\tilde{u}_1))\right\}\eta\left\{\gamma(\pi(u_3))_2\gamma(\pi(\tilde{u}_2))\right\}\right\} \# \pi(u_4 \tilde{u}_3)\\ & = & q(b(u_1 \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\tilde{b}))B(\eta(u_2))\{\gamma(\pi(u_3))_1 * B(\eta(\tilde{u}_1))\}B\left\{\eta\left\{\gamma(\pi(u_3))_2\gamma(\pi(\tilde{u}_2))\right\}\right\} \# \pi(u_4 \tilde{u}_3)\\ & = & q(b(u_1 \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\tilde{b}))B(\eta(u_2))\{\pi(\gamma(\pi(u_3))_1)\cdot B(\eta(\tilde{u}_1))\}B\left\{\eta\left\{\gamma(\pi(u_3))_2\gamma(\pi(\tilde{u}_2))\right\}\right\} \# \pi(u_4 \tilde{u}_3)\\ & = & q(b(u_1 \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\tilde{b}))B(\eta(u_2))\{\pi(u_3)_1\cdot B(\eta(\tilde{u}_1))\}B\left\{\eta\left\{\gamma(\pi(u_3)_2)\gamma(\pi(\tilde{u}_2))\right\}\right\} \# \pi(u_4 \tilde{u}_3)\\ & = & q(b(u_1 \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\tilde{b}))B(\eta(u_2))\{\pi(u_3)\cdot B(\eta(\tilde{u}_1))\}B\left\{\eta\left\{\gamma(\pi(u_4))\gamma(\pi(\tilde{u}_2))\right\}\right\} \# \pi(u_5 \tilde{u}_3), \end{align}\] where we used Lemma 1(3) in the third equality, (36 ) in the fifth one, and (13 ) in the seventh one.

On the other hand, we have \[\begin{align} \\ & = & \{q(b)B(\eta(u_1))\#\pi(u_2)\}\{q(\tilde{b})B(\eta(\tilde{u}_1))\#\pi(\tilde{u}_2) \}\\ & = & q(b)B(\eta(u_1))\{\pi(u_2)\cdot (q(\tilde{b})B(\eta(\tilde{u}_1)))\}\sigma(\pi(u_3),\pi(\tilde{u}_2))\#\pi(u_4\tilde{u}_3)\\ & = & q(b)B(\eta(u_1))\{(\pi(u_2)\cdot q(\tilde{b}))(\pi(u_3)\cdot B(\eta(\tilde{u}_1)))\}\sigma(\pi(u_4),\pi(\tilde{u}_2))\#\pi(u_5\tilde{u}_3)\\ & = & q(b(u_1 \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\tilde{b}))B(\eta(u_2))\{\pi(u_3)\cdot B(\eta(\tilde{u}_1))\}\sigma(\pi(u_4),\pi(\tilde{u}_2))\#\pi(u_5\tilde{u}_3)\\ & = & q(b(u_1 \rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\tilde{b}))B(\eta(u_2))\{\pi(u_3)\cdot B(\eta(\tilde{u}_1))\}B\left\{\eta\left\{\gamma(\pi(u_4))\gamma(\pi(\tilde{u}_2))\right\}\right\} \# \pi(u_5 \tilde{u}_3), \end{align}\] as desired, where we used Lemma 2 in the third equality, (32 ) and cocommutativity of \(\mathbf{k}[G]\) in the fourth one, and Lemma 3(1) in the last one.

Next we verify (42 ). On one hand, we have \[\begin{align} \\ & = & (q(b_2)B(\eta(u_1))\#\pi(u_2))\otimes (q(b_1)B(\eta(u_3))\#\pi(u_4))). \end{align}\] On the other hand, we have \[\begin{align} \\ & = & \left(q(b_2)B(\eta(u_1)_2)\tau(\pi(u_2))^1\# \pi(u_3)\right) \otimes \left(q(b_1)B(\eta(u_1)_1)\tau(\pi(u_2))^2\# \pi(u_4)\right)\\ & = & \left(q(b_2)B(\eta(u_1)_2\eta^{-1}(u_2)_1\eta(u_3))\# \pi(u_4)\right) \otimes \left(q(b_1)B(\eta(u_1)_1\eta^{-1}(u_2)_2\eta(u_5))\# \pi(u_6)\right)\\ & = & \left(q(b_2)B(\eta(u_1)_1\eta^{-1}(u_2)_1\eta(u_3))\# \pi(u_4)\right) \otimes \left(q(b_1)B(\eta(u_1)_2\eta^{-1}(u_2)_2\eta(u_5))\# \pi(u_6)\right)\\ & = & \left(q(b_2)B((\eta(u_1)\eta^{-1}(u_2))_1\eta(u_3))\# \pi(u_4)\right) \otimes \left(q(b_1)B((\eta(u_1)\eta^{-1}(u_2))_2\eta(u_5))\# \pi(u_6)\right)\\ & = & \left(q(b_2)B(\eta(u_1))\# \pi(u_2)\right) \otimes \left(q(b_1)B(\eta(u_3))\# \pi(u_4)\right), \end{align}\] as desired, where we used Lemma 3(2) in the second equation and the cocommutativity of \(\mathbf{k}[G]\) in the last equation.

Finally we verify that \(\theta\) is surjective. Clearly, \(\theta(b\bowtie 1) = q(b) \# 1\) for any \(b \in \mathscr{O}(G)\). Also for any \(u \in \mathbf{k}[G]\), using the cocommutativity of \(\mathbf{k}[G]\), we have \[\begin{align} \\ & = & B(\eta^{-1}(u_1))B(\eta(u_2))\# \pi(u_3)=B(\eta^{-1}(u_1)\eta(u_2))\# \pi(u_3)\\ & = & B(\varepsilon(u_1)) \# \pi(u_2) = 1 \# \pi(u). \end{align}\] Thus, \(\theta\) is surjective, as claimed.

Finally, let \(I\) be the ideal of \(D(G)\) generated by \(\mathscr{O}(G/K)^+\) and the subspace \[\left\{\mu(B(v))\bowtie 1 - 1\bowtie v\mid v\in \mathbf{k}[H]\right\}.\] Since \(\theta|_{\mathscr{O}(K)} = q\), we clearly have \(\mathscr{O}(G/K)^+ \subseteq \ker \theta\). Moreover, for every \(v \in \mathbf{k}[H]\), we have \(\theta(\mu(B(v)) \bowtie 1) = B(v) \# 1 = \theta(1 \bowtie v)\). Thus, \(I \subseteq \ker \theta\).

On the other hand, quotienting \(D(G)\) by the ideal generated by \(\mathscr{O}(G/K)^+\) identifies the \(\mathscr O(G)\)–factor with \(\mathscr{O}(K)\), hence every class in \(D(G)/I\) has a representative of the form \(a\bowtie u\) with \(a\in\mathscr O(K)\) and \(u\in \mathbf{k}[G]\). Moreover, since \(\mu(B(v))\bowtie 1 = 1\bowtie v\) for every \(v\in \mathbf{k}[H]\), the class of \(a\bowtie u\) in \(D(G)/I\) depends only on the image of \(u\) in the quotient Hopf algebra \(\mathbf{k}[G/H]\). It follows that \(D(G)/I\) is spanned by the elements represented by \(a\bowtie \gamma(x)\) with \(a\in\mathscr{O}(K)\) and \(x \in \mathbf{k}[G/H]\). Consequently, \(\dim \left(D(G)/I\right) \le \dim \left(\mathscr{O}(K)\right)\dim \left(\mathbf{k}[G/H]\right)\). Hence, \(\dim (I) \ge \dim (\ker \theta)\).

Thus, \(I=\ker \theta\), as claimed. ◻

Remark 7. It follows from Theorem 6 that \(\sigma\) (39 ) is a cocycle, \(\tau\) (40 ) is a co-cocycle, and \(\mathbf{k}[G]\) co-measures \(\mathscr{O}(K)\) trivially (see e.g., [20], [21] for the necessary definitions). 0◻

Proposition 8. For each Hopf algebra \(D(K,H,B)\), the following hold:

  1. \(D(K,H,B)\) is involutive, with \(\dim_{\mathbf{k}}(D(K,H,B))=|K|[G:H]\).

  2. The map \[\mathscr{O}(K)^{{\rm cop}}\xrightarrow{1:1} D(K,H,B),\quad a\mapsto a\# 1,\] is an injective Hopf algebra map.

  3. The map \[D(K,H,B)\twoheadrightarrow \mathbf{k}[G/H],\quad a\# x\mapsto \varepsilon(a)x,\] is a surjective Hopf algebra map whose kernel is the ideal generated by \(\mathscr{O}(K)^+\).

  4. If \(\eta_H\) (14 ) is a coalgebra map, then \(D(K,H,B)=\mathscr{O}(K)^{{\rm cop}}\otimes \mathbf{k}[G/H]\) is a tensor product coalgebra.

  5. If \(B=1\), then \(D(K,H):=D(K,H,1)=\mathscr{O}(K)^{{\rm cop}}\# \mathbf{k}[G/H]\) is a smash product algebra, and \(D(K,H)=\mathscr{O}(K)^{{\rm cop}}\otimes \mathbf{k}[G/H]\) is a tensor product coalgebra.

  6. The map \[\overline{B}:=B^*\circ S:\mathbf{k}[K]\to \mathscr{O}(H)\] is a \(G\)-equivariant Hopf algebra map, so we have the corresponding Hopf algebra quotient \(D(H,K,\overline{B})\) of \(D(G)\).

  7. If \(K\) is commutative then \(D(K,H,B)=\mathbf{k}[\widetilde{G}]\), where \(\widetilde{G}\) is the group scheme extension of \(G/H\) by \(K^{\vee}\) corresponding to \[\sigma\in Z^2(G/H,K^{\vee})\quad\text{and}\quad\tau\in Z^1(G/H,(K^2)^{\vee}),\] where \(G/H\) acts trivially on \(K^{\vee}\) and \((K^2)^{\vee}\).

Proof. (1)-(2) These are straightforward.

(3) This is straightforward noting that \(\varepsilon(x\cdot a)=\varepsilon(x)\varepsilon(a)\), \(\varepsilon(\sigma(x,\tilde{x}))=\varepsilon(x)\varepsilon(\tilde{x})\), and \((\varepsilon\otimes \varepsilon)(\tau(x))=\varepsilon(x)(1\otimes 1)\).

(4)-(5) These follow in a straightforward manner using Remark 5.

(6) This follows since \(\mathbf{k}[H]\) is cocommutative.

(7) This follows since \(D(K,H,B)\) is cocommutative when \(K\) is commutative. ◻

3.2 Classification of Hopf quotient pairs of \(D(G)\)↩︎

A Hopf quotient pair of \(D(G)\) is a pair \((D,\varphi)\) where \(\varphi:D(G)\twoheadrightarrow D\) is a surjective Hopf algebra map. We will say that two Hopf quotient pairs \((D_1,\varphi_1)\) and \((D_2,\varphi_2)\) are equivalent if there is a Hopf algebra isomorphism \(f:D_1\xrightarrow{\cong} D_2\), such that \(\varphi_2=f\varphi_1\).

Lemma 4. Two Hopf quotient pairs \(\left(D(K,H,B),\theta\right)\) and \(\left(D\left(K',H',B'\right),\theta'\right)\) as constructed in Theorem 6 are equivalent if and only if \((K,H,B)=(K',H',B')\).

Proof. Suppose that \(f:D(K,H,B)\xrightarrow{\cong} D\left(K',H',B'\right)\) is a Hopf algebra isomorphism, such that \(\theta'=f\theta\). In particular, \(\theta'_{\mid \mathscr{O}(G)}=(f\theta)_{\mid \mathscr{O}(G)}\); that is, \(q_{K'}=(f_{\mid \mathscr{O}(K)})\circ q_K\), or equivalently, \(\iota_{K'}=\iota_K\circ\widetilde{(f_{\mid \mathscr{O}(K)})}\), where \(\widetilde{(f_{\mid \mathscr{O}(K)})}:K'\twoheadrightarrow K\) is the corresponding surjective group scheme morphism. Thus, \(K=K'\) and \(f_{\mid \mathscr{O}(K)}:\mathscr{O}(K)\to \mathscr{O}(K)\) is the identity map.

Also, for every \(v\in \mathbf{k}[H]\), we have \(\eta_H(v)=v\) and \(\pi_H(v)=\varepsilon(v)\), so we have that \(\theta(1\bowtie v)=B(v)\#1\). Applying \(\varepsilon\otimes\mathrm{id}\) to \[f(B(v)\#1)=f\theta(1\bowtie v)=\theta'(1\bowtie v)=B'(\eta_{H'}(v_1))\#'\pi_{H'}(v_2)\] then yields \(\pi_{H'}(v)=\varepsilon(v)\). Hence, \(\mathbf{k}[H]^+\subseteq\ker(\pi_{H'})=\mathbf{k}[G]\mathbf{k}[H']^+\). By symmetry, we obtain \(\ker(\pi_H)=\ker(\pi_{H'})\), and therefore \(H=H'\).

Finally, it follows from the above and Theorem 6(2) that \[B'=\theta'_{\mid \mathbf{k}[H]}=(f\circ\theta)_{\mid \mathbf{k}[H]}=f_{\mid \mathscr{O}(K)}\circ \theta_{\mid \mathbf{k}[H]}=\theta_{\mid \mathbf{k}[H]}=B\] since \(f_{\mid \mathscr{O}(K)}:\mathscr{O}(K)\to \mathscr{O}(K)\) is the identity map. ◻

Theorem 9. The assignment \((K,H,B)\mapsto (D(K,H,B),\theta)\) constructed in Theorem 6 determines a bijection between the set of triples \((K,H,B)\) and the set of equivalence classes of Hopf quotient pairs of \(D(G)\).

Proof. By Theorem 6 and Lemma 4, it remains to prove that for any Hopf quotient pair \((D,\varphi)\) of \(D(G)\), there exist a Hopf quotient pair \((D(K,H,B),\theta)\) of \(D(G)\), and a Hopf algebra isomorphism \(\overline{\varphi}:D(K,H,B)\xrightarrow{\cong}D\), such that \(\overline{\varphi} \theta = \varphi\).

So, let \(\varphi : D(G) \twoheadrightarrow D\) be a surjective Hopf algebra map. Since the image of \(\varphi_{\mid \mathscr{O}(G)}\) is a Hopf algebra quotient of \(\mathscr{O}(G)\), we may assume that \(\varphi(\mathscr{O}(G))=\mathscr{O}(K)\subseteq D\), and \(\varphi_{\mid \mathscr{O}(G)}=q_K:\mathscr{O}(G)\twoheadrightarrow \mathscr{O}(K)\) for some subgroup scheme \(K\subseteq G\). Moreover, since \(\mathscr{O}(G)\subseteq D(G)\) is a normal Hopf subalgebra, \(\mathscr{O}(K)\subseteq D\) is a normal Hopf subalgebra.

\(\mathbf{Claim\, 1.}\) \(K\subseteq G\) is a normal subgroup scheme.

Fix \(a\in \mathscr{O}(G/K)^+\mathscr{O}(G)\). Then \(\varphi(a\bowtie 1)=q_K(a)=0\), hence \[0=\varphi\left((1\bowtie u_1)(a\bowtie 1)(1\bowtie S(u_2)\right) = \varphi\left((u\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup a)\bowtie 1\right)=q_K(u\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup a);\] that is, \(u\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup a\in \mathscr{O}(G/K)^+\mathscr{O}(G)\) for every \(u\in \mathbf{k}[G]\). It follows that \({\rm coad}\) (8 ) maps \(\mathscr{O}(G/K)^+\mathscr{O}(G)\) to \(\mathscr{O}(G/K)^+\mathscr{O}(G)\otimes\mathscr{O}(G)\); that is, \(K\) is normal in \(G\). 0◻

Next consider the exact sequence of Hopf algebras \[\mathbf{k}\to \mathscr{O}(K) \to D \to D/(\mathscr{O}(K)^+D)\to \mathbf{k}.\] Since \(D(G)/(\mathscr{O}(G)^+D(G))\cong \mathbf{k}[G]\) (17 ), it follows that the Hopf algebra \(D/(\mathscr{O}(K)^+D)\) is a Hopf quotient of \(\mathbf{k}[G]\), so we may assume that \[D/(\mathscr{O}(K)^+D)=\mathbf{k}[G/H]\] for some normal subgroup scheme \(H\) of \(G\), so that we have a commutative diagram with exact rows \[\label{commdiagram} \begin{tikzcd} \mathbf{k}\arrow[r] & \mathscr{O}(G) \arrow[r] \arrow[d, "q_K"] & D(G) \arrow[r, "\varepsilon\otimes\operatorname{id}"] \arrow[d, "\varphi"] & {\mathbf{k}[G]} \arrow[r] \arrow[d, "\pi_H"] & \mathbf{k}\\ \mathbf{k}\arrow[r] & \mathscr{O}(K) \arrow[r] & D \arrow[r, "p"] & \mathbf{k}[G/H] \arrow[r] & \mathbf{k}. \end{tikzcd}\tag{43}\] In particular, by [19], [20], we may assume that \(D=\mathscr{O}(K) \#^{\tilde{\tau}}_{\tilde{\sigma}} \mathbf{k}[G/H]\) as Hopf algebras, so that \(D=\mathscr{O}(K)\otimes\mathbf{k}[G/H]\) as vector spaces, and we can view \(\mathscr{O}(K)\) as a Hopf subalgebra of \(D\) in the obvious way. To avoid confusion, we will write \(a\widetilde{\#}x\) to denote an element of \(D\).

\(\mathbf{Claim\, 2.}\) For every \(v\in \mathbf{k}[H]\), \(\varphi(1\bowtie v)\in \mathscr{O}(K)\). Moreover, the Hopf algebra map \[B:=\varphi_{\mid \mathbf{k}[H]} : \mathbf{k}[H] \to \mathscr{O}(K),\quad v\mapsto \varphi(1\bowtie v),\] is \(G\)-equivariant as in (38 ).

By (43 ), for every \(v\in \mathbf{k}[H]\), we have \[\begin{align} \\ & = & \varphi(1\bowtie v_1)\otimes p(\varphi(1\bowtie v_2))=\varphi(1\bowtie v_1)\otimes \pi_H(v_2)\\ & = &\varphi(1\bowtie v_1)\otimes \varepsilon(v_2)= \varphi(1\bowtie v)\otimes 1, \end{align}\] which implies that \(\varphi(1\bowtie v)\in D^{{\rm co}\mathbf{k}[G/H]}=\mathscr{O}(K)\).

Furthermore, for every \(v \in \mathbf{k}[H]\) and \(u \in \mathbf{k}[G]\), we have \[\begin{align} \\ & = & \varphi((1\bowtie u_1)(1\bowtie v)(1\bowtie S(u_2))) =\varphi(1\bowtie u_1)\varphi(1\bowtie v)\varphi(1\bowtie S(u_2))\\ & = & \varphi(1\bowtie u_1)\varphi(\mu_K(B(v))\bowtie 1)\varphi(1\bowtie S(u_2))=\varphi((1\bowtie u_1)(\mu_K(B(v))\bowtie 1)(1\bowtie S(u_2)))\\ & = & \varphi((u_1\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\mu_K(B(v))\bowtie u_2)(1\bowtie S(u_3)))=\varphi((u_1\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\mu_K(B(v)))\bowtie u_2S(u_3))\\ & = & \varphi((u\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\mu_K(B(v)))\bowtie 1)=q_K(u\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\mu_K(B(v)))=u*B(v). \end{align}\] Here \(\mu_K\) is a section of \(q_K\) as in (4 ). Thus, for every \(w\in \mathbf{k}[K]\), we have \[\begin{align} \\ & = & \left\langle q_K\left(S(u_2)\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\mu_K(q_K\left(u_1\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\mu_K(B(v))\right))\right),w\right\rangle\\ & = & \left\langle S(u_2)*q_K\left(u_1\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\mu_K(B(v))\right),w\right\rangle= \left\langle S(u_2)*(u_1*B(v)),w\right\rangle\\ & = & \varepsilon(u)\left\langle B(v),w\right\rangle, \end{align}\] as claimed. 0◻

\(\mathbf{Claim\, 3.}\) The normal subgroup schemes \(K,H\subseteq G\) centralize each other.

We claim that \(\mathbf{k}[H]\) acts trivially on \(\mathscr{O}(K)\) via \(\varphi\). Indeed, for every \(v \in \mathbf{k}[H]\) and \(b \in \mathscr{O}(G)\), we have \[\begin{align} \\ & = & \varphi(1\bowtie v_1)\varphi(1\bowtie S(v_2))\varphi(b\bowtie 1)= \varphi(1\bowtie v_1S(v_2))\varphi(b\bowtie 1)= \varepsilon(v) \varphi(b\bowtie 1), \end{align}\] as claimed, where we applied Claim 2 to use the commutativity of \(\mathscr{O}(K)\) in the second equality.

Now since \((\operatorname{ad}_{\ell}(1\bowtie v))(b\bowtie 1) = (v\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup b)\bowtie 1\), it follows that \[q_K(v\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup b) = \varepsilon(v) q_K(b); \quad\forall\,v\in\mathbf{k}[H],\;b\in\mathscr{O}(G).\] Pairing with \(w \in \mathbf{k}[K]\) and using (10 ), we obtain \[\langle b,{\rm ad_r}(v)(w)\rangle=\langle v\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup b,w\rangle = \langle q_K(v\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup b), w \rangle = \varepsilon(v)\langle q_K(b), w \rangle = \varepsilon(v) \langle b, w \rangle.\] Since this holds for all \(b \in \mathscr{O}(G)\), it follows that \({\rm ad_r}(v)(w) = \varepsilon(v) w\) for all \(w \in \mathbf{k}[K]\); that is, \(\mathbf{k}[H]\) and \(\mathbf{k}[K]\) commute. 0◻

Set \(\pi:=\pi_H\), \(\gamma:=\gamma_H\), \(\eta:=\eta_H\), and \(q:=q_K\).

\(\mathbf{Claim\, 4.}\) For every \(u\in \mathbf{k}[G]\), we have \(\varphi(1\bowtie u)=B(\eta(u_1))\widetilde{\#} \pi(u_2)\).

First note that the commutativity of (43 ) implies that for every \(x\in \mathbf{k}[G/H]\), \[\varphi(1\bowtie \gamma(x))=1\widetilde{\#} x.\] Now since by Lemma 1(2), \(u=\eta(u_1)(\gamma(\pi(u_2)))\) for every \(u\in \mathbf{k}[G]\), it follows that \[\begin{align} \\ & = & (B(\eta(u_1))\widetilde{\#} 1)(1\widetilde{\#} \pi(u_2))= B(\eta(u_1))\widetilde{\#} \pi(u_2), \end{align}\] as claimed. 0◻

It now follows from Claims 2 and 4 that we have \[\label{varphiis} \varphi(b\bowtie u)=\varphi(b\bowtie 1)\varphi(1\bowtie u)=q(b)B(\eta(u_1))\widetilde{\#} \pi(u_2);\quad \forall\, b\bowtie u\in D(G).\tag{44}\]

Finally, let \((D(K,H,B),\theta)\) be the Hopf quotient pair of \(D(G)\) corresponding, by Theorem 6 and Claims 2-3, to the triple \((K,H,B)\), and consider the identity map \[\overline{\varphi}:=\operatorname{id}_{\mathscr{O}(K)\otimes\mathbf{k}[G/H]} : D(K,H,B) \to D,\quad a \# x\mapsto a\widetilde{\#}x.\] Then \(\overline{\varphi} \theta = \varphi\) by (44 ), so \(\theta = \varphi\), and \(\overline{\varphi}\) is a Hopf algebra isomorphism, so \((D,\varphi)\) is equivalent to \((D(K,H,B),\theta)\). ◻

Corollary 1. For each Hopf quotient pair \((D(K,H,B),\theta)\) of \(D(G)\) and surjective Hopf algebra homomorphism \(\varphi:D(K,H,B)\twoheadrightarrow D\), the Hopf quotient pair \((D,\varphi\theta)\) is equivalent to a Hopf quotient pair \((D(K',H',B'),\theta')\) for some normal subgroup schemes \(K'\subseteq K\) and \(H\subseteq H'\) of \(G\), such that \[\iota^{\sharp}_{K',K}\circ B =B'\circ \iota_{H,H'}:\mathbf{k}[H]\to \mathscr{O}(K').\]

Proof. Since \((D,\varphi\theta)\) is a Hopf quotient pair of \(D(G)\), it follows from Theorem 9 that there exists a Hopf quotient pair \((D(K',H',B'),\theta')\) together with a Hopf algebra isomorphism \(f:D(K',H',B')\xrightarrow{\cong} D\), such that \(\varphi\theta=f\theta'\). In particular, we have \[(\varphi\theta)|_{\mathscr{O}(G)}=\left(\varphi|_{\mathscr{O}(K)}\right)\circ q_K.\] On the other hand, since \(\varphi\theta=f\theta'\) and \(\theta'|_{\mathscr{O}(G)}=q_{K'}\), we have \((\varphi\theta)|_{\mathscr{O}(G)}=\left(f|_{\mathscr{O}(K')}\right)\circ q_{K'}\). Thus, \(\varphi q_K=f q_{K'}\), so \(f^{-1}\circ\left(\varphi|_{\mathscr{O}(K)}\right):\mathscr{O}(K)\twoheadrightarrow \mathscr{O}(K')\) is a surjective Hopf algebra map, so \(K'\subseteq K\) is a subgroup scheme.

Next, for every \(v\in \mathbf{k}[H]^+\), we have \[\varphi(B(v)\# 1)=\varphi\theta(1\bowtie v)=f\theta'(1\bowtie v)=f\left(B'(\eta_{H'}(v_1))\#\pi_{H'}(v_2)\right),\] thus, we have \[B'(\eta_{H'}(v_1))\#\pi_{H'}(v_2)=f^{-1}\left(\varphi(B(v)\# 1)\right)\in \mathscr{O}(K')^+\# 1.\] Applying \(\varepsilon\otimes\operatorname{id}\) to both sides of the last equation yields \(\pi_{H'}(v)=0\), which implies that \(v\in \mathbf{k}[H']^+\mathbf{k}[G]\). Thus, \(\mathbf{k}[H]^+\mathbf{k}[G]\subseteq \mathbf{k}[H']^+\mathbf{k}[G]\); that is, \(H\subseteq H'\), as desired.

Finally, since \(\varphi\theta=f\theta'\), and Theorem 6(2) gives \(\theta|_{\mathbf{k}[H]}=B\) and \(\theta'|_{\mathbf{k}[H']}=B'\), functoriality implies that we have \(\iota^{\sharp}_{K',K}\circ B =B'\circ \iota_{H,H'}:\mathbf{k}[H]\to \mathscr{O}(K')\), as desired. ◻

Corollary 2. Let \((D(K,H,B),\theta)\) and \((D\left(K',H',B'\right),\theta')\) be two Hopf quotient pairs of \(D(G)\), such that \(K\subseteq K'\) and \(H'\subseteq H\) are normal subgroup schemes of \(G\), and \(\mathbf{q}\circ B' =B\circ \iota_{H',H}:\mathbf{k}[H']\to \mathscr{O}(K)\), where \(\mathbf{q}:=\iota^{\sharp}_{K,K'}:\mathscr{O}(K')\twoheadrightarrow \mathscr{O}(K)\) is the canonical surjective Hopf algebra map. Then there is a unique surjective Hopf algebra map \(\varphi:D\left(K',H',B'\right)\twoheadrightarrow D(K,H,B)\), such that \(\theta =\varphi\theta'\).

Proof. Since \(K\subseteq K'\), we have \(\mathscr{O}(G/K')\subseteq \mathscr{O}(G/K)\) as Hopf subalgebras of \(\mathscr{O}(G)\), so \(\mathscr{O}(G/K')^+\subseteq \mathscr{O}(G/K)^+\). Next fix \(v\in \mathbf{k}[H']\) and consider \[r_v:=\mu_{K'}(B'(v))\bowtie 1-1\bowtie v\;\in D(G).\] We claim that \(r_v\in \ker(\theta)\). First note that \[\theta(1\bowtie v)=B(\eta_H(v_1))\#\pi_H(v_2)=B(v_1)\#\varepsilon(v_2)=B(v)\# 1.\] On the other hand, \[\theta(\mu_{K'}(B'(v))\bowtie 1)=q_K(\mu_{K'}(B'(v)))\# 1.\] Using \(\mathbf{q}\,q_{K'}=q_K\) and \(q_{K'}\mu_{K'}={\rm id}_{\mathscr{O}(K')}\), we get \[q_K(\mu_{K'}(B'(v)))=\mathbf{q}(q_{K'}(\mu_{K'}(B'(v))))=\mathbf{q}(B'(v)).\] By assumption, \(\mathbf{q}\circ B'=B\circ \iota_{H',H}\), and viewing \(v\in \mathbf{k}[H']\) inside \(\mathbf{k}[H]\) via \(\iota_{H',H}\), this gives \(\mathbf{q}(B'(v))=B(v)\). Hence, \[\theta(\mu_{K'}(B'(v))\bowtie 1)=B(v)\# 1=\theta(1\bowtie v),\] so \(\theta(r_v)=0\), as claimed.

Thus, by Theorem 6(3), we obtain \(\ker(\theta') \subseteq \ker({\theta})\), so there is a unique surjective Hopf algebra map \(\varphi:D(K',H',B')\twoheadrightarrow D(K,H,B)\), such that \(\theta=\varphi\theta'\), as claimed. ◻

Fix two Hopf quotient pairs \((D(K,H,B),\theta)\) and \((D\left(K',H',B'\right),\theta')\) of \(D(G)\), and define the Hopf algebra map \[\label{phibbprime} \begin{align} & \beta _{B,B'}:\mathbf{k}[K\cap K']\to \mathscr{O}(H\cap H')\\ & w\mapsto \left(\iota^{\sharp}_{H\cap H',H}B^*\iota_{K\cap K',K}(w_1)\right)\left(\iota^{\sharp}_{H\cap H',H'}\overline{B'}\iota_{K\cap K',K'}(w_2)\right); \end{align}\tag{45}\] that is, \(\beta_{B,B'} =\left(\iota^{\sharp}_{H\cap H',H}B^*\iota_{K\cap K',K}\right)\star\left(\iota^{\sharp}_{H\cap H',H'}\overline{B'}\iota_{K\cap K',K'}\right)\).

Let \(L\subseteq K\cap K'\) be the subgroup scheme, such that \[{\rm Ker}(\beta_{B,B'})=\mathbf{k}[L]^+\mathbf{k}[K\cap K'],\] and define the \(G\)-equivariant Hopf algebra map \[\label{psibbprime} \begin{align} & \mathbf{B}_{B,B'}:\mathbf{k}[L]\to \mathscr{O}(HH'),\\ & w\mapsto \left(\mu_{H,HH'}B^*\iota_{L,K}(w_1)\right)\left(\mu_{H',HH'}\overline{B'}\iota_{L,K'}(w_2)\right); \end{align}\tag{46}\] that is, \(\mathbf{B}_{B,B'}=\left(\mu_{H,HH'}B^*\iota_{L,K}\right)\star\left(\mu_{H',HH'}\overline{B'}\iota_{L,K'}\right)\). Set \[\label{Bint} \mathbf{B}:=\mathbf{B}_{B,B'}^*:\mathbf{k}[HH']\to \mathscr{O}(L),\tag{47}\] and let \(\left(D\left(L,HH',\mathbf{B}\right),\Theta\right)\) be the corresponding Hopf quotient pair of \(D(G)\).

Proposition 10. The following hold:

  1. There exist surjective Hopf algebra maps \(\varphi:D(K,H,B)\twoheadrightarrow D\left(L,HH',\mathbf{B}\right)\) and \(\varphi':D\left(K',H',B'\right)\twoheadrightarrow D\left(L,HH',\mathbf{B}\right)\), such that \(\varphi\theta=\Theta =\varphi'\theta'\).

  2. The Hopf quotient pair \(\left(D\left(L,HH',\mathbf{B}\right),\Theta\right)\) is the maximal one having the properties in (1).

Proof. (1) This follows from Corollary 2.

(2) Suppose that \[\phi:D(K,H,B)\twoheadrightarrow D\left(K'',H'',B''\right),\quad\phi':D\left(K',H',B'\right)\twoheadrightarrow D\left(K'',H'',B''\right)\] are surjective Hopf algebra maps, such that \(\phi\theta=\theta'' =\phi'\theta'\). Then by Corollary 1, \(K''\subseteq K\cap K'\) and \(HH'\subseteq H''\) are normal subgroup schemes of \(G\), \[\iota^{\sharp}_{K'',K}\circ B=B''\circ \iota_{H,H''}:\mathbf{k}[H]\to \mathscr{O}(K''),\quad\text{and}\] \[\iota^{\sharp}_{K'',K'}\circ B' =B''\circ \iota_{H',H''}:\mathbf{k}[H']\to \mathscr{O}(K'').\]

We claim that \(K''\subseteq L\). Indeed, for every \(w\in \mathbf{k}[K'']\) and \(v\in \mathbf{k}[H\cap H']\), we have \[\begin{align} \\ & = & \langle \iota^{\sharp}_{H\cap H',H}B^*\iota_{K\cap K',K}(\iota_{K'',K\cap K'}(w_1)),v_1\rangle \langle \iota^{\sharp}_{H\cap H',H'}\overline{B'}\iota_{K\cap K',K'}(\iota_{K'',K\cap K'}(w_2)),v_2\rangle\\ & = & \langle \iota^{\sharp}_{H\cap H',H}B^*\iota_{K'',K}(w_1),v_1\rangle \langle \iota^{\sharp}_{H\cap H',H'}\overline{B'}\iota_{K'',K'}(w_2),v_2\rangle\\ & = & \langle w_1,\iota^{\sharp}_{K'',K}B\iota_{H\cap H',H}(v_1)\rangle \langle S(w_2),\iota^{\sharp}_{K'',K'}B'\iota_{H\cap H',H'}(v_2)\rangle\\ & = & \langle w_1,B''\iota_{H,H''}\iota_{H\cap H',H}(v_1)\rangle \langle S(w_2),B''\iota_{H',H''}\iota_{H\cap H',H'}(v_2)\rangle\\ & = & \langle w_1,B''\iota_{H\cap H',H''}(v_1)\rangle \langle S(w_2),B''\iota_{H\cap H',H''}(v_2)\rangle\\ & = & \langle w_1S(w_2),B''\iota_{H\cap H',H''}(v)\rangle =\langle \varepsilon(w),B''\iota_{H\cap H',H''}(v)\rangle =\langle \varepsilon(w),v\rangle. \end{align}\] Thus, \(\mathbf{k}[K'']^+\subseteq {\rm Ker}(\beta_{B,B'})=\mathbf{k}[L]^+\mathbf{k}[K\cap K']\), so \(K''\subseteq L\), as claimed.

Next we claim that the surjective Hopf algebra map \[\Phi:D\left(L,HH',\mathbf{B}\right)\twoheadrightarrow D\left(K'',H'',B''\right)\] given by Corollary 2, satisfies \(\Phi\varphi=\phi\) and \(\Phi\varphi'=\phi'\). Indeed, by Corollary 2, \(\theta'' =\Phi\Theta\), and by assumption, \(\varphi\theta=\Theta =\varphi'\theta'\) and \(\phi\theta=\theta'' =\phi'\theta'\). Thus, we have \[\phi\theta=\theta'' =\Phi\Theta=\Phi\varphi\theta,\] so \(\Phi\varphi=\phi\) since \(\theta\) is surjective. Similarly, \(\Phi\varphi'=\phi'\). ◻

3.3 The quasitriangular ribbon structure on \(D(K,H,B)\)↩︎

Fix bases \(\mathcal{B}_K\subseteq \mathcal{B}\) for \(\mathbf{k}[K]\) and \(\mathbf{k}[G]\), respectively, and let \(\{\delta_u\mid u\in \mathcal{B}\}\) be the dual basis for \(\mathscr{O}(G)\). It is clear that \(\{q_K(\delta_u)\mid u\in \mathcal{B}_K\}\) is the dual basis of \(\mathcal{B}_K\) for \(\mathscr{O}(K)\), and that for \(u\in \mathcal{B}_K\), \(\langle q_K(\delta_u),v\rangle\ne 0\) if and only if \(v\in \mathcal{B}_K\).

Corollary 3. Each Hopf quotient \(D(K,H,B)\) of \(D(G)\) is quasitriangular ribbon, with \(R\)-matrix \[R(K,H,B):=\sum_{u \in \mathcal{B}_K} (B(\eta_H(u_1))\#\pi_H(u_2))\otimes (q_K(\delta_u)\# 1),\] and ribbon element \[V(K,H,B):=\sum_{u \in \mathcal{B}_K} q_K(S(\delta_u))B(\eta_H(u_1))\#\pi_H(u_2).\]

Proof. By Theorem 6(2), the element \[\begin{align} \\ & = & \sum_{u \in \mathcal{B}} \theta(1\bowtie u) \otimes \theta(\delta_u\bowtie 1)=\sum_{u \in \mathcal{B}_K}(B(\eta_H(u_1))\#\pi_H(u_2))\otimes (q_K(\delta_u)\# 1) \end{align}\] is an \(R\)-matrix for \(D(K,H,B)\), and \[V(K,H,B)=\theta(V)=\sum_{u \in \mathcal{B}} \theta(S(\delta_u)\bowtie u)=\sum_{u \in \mathcal{B}_K}q_K(S(\delta_u))B(\eta_H(u_1))\#\pi_H(u_2)\] is a ribbon element, as claimed. ◻

4 Tensor subcategories of \(\operatorname{Rep}(D(G))\)↩︎

Fix a finite group scheme \(G\) over \(\mathbf{k}\) as in §2.1.

4.1 Construction and classification↩︎

Let \(\mathscr{Z}(G):=\operatorname{Rep}(D(G))\) as in §2.4. For each triple \((K,H,B)\) as in Theorem 6, set \[\mathscr{Z}(K,H,B):=\operatorname{Rep}(D(K,H,B)).\] Then using the surjective Hopf algebra map \(\theta:D(G)\twoheadrightarrow D(K,H,B)\), we can (and will) view \(\mathscr{Z}(K,H,B)\) as a tensor subcategory of \(\mathscr{Z}(G)\).

Corollary 4. The tensor category \(\mathscr{Z}(K,H,B)\) is ribbon braided, with Frobenius-Perron dimension \(|K| [G : H]\).

Proof. This follows from Proposition 8. ◻

Theorem 11. The assignment \((K,H,B)\mapsto \mathscr{Z}(K,H,B)\) determines a bijection between the set of triples \((K,H,B)\) and the set of tensor subcategories of \(\mathscr{Z}(G)\).

Proof. It is well known that the set of tensor subcategories of the representation category of a finite dimensional Hopf algebra is in bijection with the set of equivalence classes of its quotient pairs (see, e.g., [15]). Thus, the claim follows from Theorem 9. ◻

Theorem 11 yields a classification of certain finite braided group scheme-theoretical categories [9].

Corollary 5. Let \(\mathscr{B}\) be any finite braided group scheme-theoretical category which admits a fiber functor to \({\rm Vect}\). Then there exists a finite group scheme \(G\), and a triple \((K,H,B)\) as in Theorem 6, such that \(\mathscr{B}\) is braided tensor equivalent to \(\mathscr{Z}(K,H,B)\).

Proof. Since any finite braided group scheme-theoretical category \(\mathscr{B}\) is a braided tensor subcategory of its center \(\mathscr{Z}\left(\mathscr{B}\right)\), and by [9] the latter is braided tensor equivalent to \(\mathscr{Z}(G)\) for some finite group scheme \(G\) (since \(\mathscr{B}\) is tensor equivalent to a representation category of a Hopf algebra), the claim follows from Theorem 11. ◻

Corollary 6. The following hold:

  1. \(\mathscr{Z}(K',H',B')\subseteq \mathscr{Z}(K,H,B)\) if and only if \(K'\subseteq K\) and \(H\subseteq H'\) are normal subgroup schemes of \(G\), and \(\iota^{\sharp}_{K',K}\circ B=B'\circ \iota_{H,H'}:\mathbf{k}[H]\to \mathscr{O}(K')\).

  2. \(\mathscr{Z}(K,H,B)\cap \mathscr{Z}\left(K',H',B'\right)=\mathscr{Z}\left(L,HH',\mathbf{B}\right)\), where \(\mathbf{B}\) is defined in (47 ).

Proof. (1) This follows from Corollary 1 and Theorem 11.

(2) This follows from Proposition 10. ◻

4.2 The Müger centralizer of \(\mathscr{Z}(K,H,B)\)↩︎

For each Hopf algebra \(D(K,H,B)\), recall the Hopf algebra \(D(H,K,\overline{B})\) from Proposition 8(6).

Theorem 12. For each tensor subcategory \(\mathscr{Z}(K,H,B)\subseteq \mathscr{Z}(G)\), the tensor subcategory \(\mathscr{Z}(H,K,\overline{B})\subseteq \mathscr{Z}(G)\) is its Müger centralizer in \(\mathscr{Z}(G)\).

Proof. Fix \(D:=D(K,H,B)\), and set \(\overline{D}:=D(H,K,\overline{B})\). Also, let \(\mathscr{Z}:=\mathscr{Z}(K,H,B)\), and \(\overline{\mathscr{Z}}:=\mathscr{Z}(H,K,\overline{B})\). Let \(\theta: D(G) \twoheadrightarrow D\) and \(\overline{\theta}:D(G) \twoheadrightarrow \overline{D}\) be the Hopf algebra quotients constructed in Theorem 6.

\(\mathbf{Claim\,1.}\) \(\mathscr{Z}\) and \(\overline{\mathscr{Z}}\) centralize each other if and only if \((\theta \otimes \overline{\theta})(R_{21}R) = 1 \otimes 1\).

Recall that the square braiding in \(\mathscr{Z}(G)\) is defined by multiplication by \(R_{21}R\). If \(\mathscr{Z}\) and \(\overline{\mathscr{Z}}\) centralize each other, then \((\theta \otimes \overline{\theta})(R_{21}R)\) acts as the identity on \(X \otimes Y\) for all \(X\in \mathscr{Z}\) and \(Y \in \overline{\mathscr{Z}}\). In particular, we can take the faithful representation \(D\otimes \overline{D}\) of \(D\otimes \overline{D}\), and get that \((\theta \otimes \overline{\theta}) (R_{21}R) = 1 \otimes 1\).

Conversely, if \((\theta \otimes \overline{\theta}) (R_{21}R) = 1 \otimes 1\), then \(R_{21}R\) acts by the identity on \(X \otimes Y\) for all \(X \in \mathscr{Z}\) and \(Y \in \overline{\mathscr{Z}}\), so \(\mathscr{Z}\) and \(\overline{\mathscr{Z}}\) centralize each other, as claimed. 0◻

Now fix a basis \(\mathcal{B}\) for \(\mathbf{k}[G]\), such that \(\mathcal{B}\) contains bases \(\mathcal{B}_H\) and \(\mathcal{B}_K\) for \(\mathbf{k}[H]\) and \(\mathbf{k}[K]\), respectively, and let \(\{\delta_u\mid u\in \mathcal{B}\}\) be the dual basis for \(\mathscr{O}(G)\). By (18 ), we have \[R_{21}R= \sum_{u,\tilde{u} \in \mathcal{B}} (\delta_u\bowtie \tilde{u}) \otimes ((u_1\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\delta_{\tilde{u}})\bowtie u_2).\] We claim that \((\theta \otimes \overline{\theta}) (R_{21}R)=1 \otimes 1\). Indeed, we have \[\begin{align} \\ & = & \sum_{u,\tilde{u} \in \mathcal{B}} \left(q_K(\delta_u) B(\eta_H(\tilde{u}_1)) \# \pi_H(\tilde{u}_2)\right) \otimes \left(q_H(u_1\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\delta_{\tilde{u}}) \overline{B}(\eta_K(u_2))\# \pi_K(u_3)\right)\\ & = & \sum_{u\in \mathcal{B}_K,\,\tilde{u}\in \mathcal{B}_H} \left(q_K(\delta_u) B(\eta_H(\tilde{u}_1)) \# \pi_H(\tilde{u}_2)\right) \otimes \left(q_H(u_1\rightharpoonup\mathrel{\mspace{-15mu}}\rightharpoonup\delta_{\tilde{u}}) \overline{B}(\eta_K(u_2))\# \pi_K(u_3)\right)\\ & = & \sum_{u\in \mathcal{B}_K,\,\tilde{u}\in \mathcal{B}_H} \left(q_K(\delta_u) B(\eta_H(\tilde{u})) \# 1\right) \otimes \left(q_H(\delta_{\tilde{u}}) \overline{B}(\eta_K(u))\# 1\right)\\ & = & \sum_{u\in \mathcal{B}_K,\,\tilde{u}\in \mathcal{B}_H} \left(q_K(\delta_u) B(\tilde{u}) \# 1\right) \otimes \left(q_H(\delta_{\tilde{u}}) \overline{B}(u)\# 1\right). \end{align}\] To show that \(\sum_{u\in \mathcal{B}_K,\,\tilde{u}\in \mathcal{B}_H} \left(q_K(\delta_u) B(\tilde{u})\# 1\right)\otimes \left(q_H(\delta_{\tilde{u}}) \overline{B}(u)\# 1\right)=(1\# 1)\otimes (1\# 1)\), we compute for any \(v\in \mathbf{k}[K]\) and \(w\in \mathbf{k}[H]\), \[\begin{align} \\ & = & \sum_{u\in \mathcal{B}_K,\,\tilde{u}\in \mathcal{B}_H} \left\langle q_K(\delta_u),v_1\right\rangle \left\langle B(\tilde{u}),v_2\right\rangle \left\langle q_H(\delta_{\tilde{u}}),w_1\right\rangle \left\langle \overline{B}(u),w_2\right\rangle\\ & = & \sum_{u\in \mathcal{B}_K,\,\tilde{u}\in \mathcal{B}_H} \left\langle q_K(\delta_u)\left\langle u,\overline{B}^*(w_2)\right\rangle,v_1\right\rangle \left\langle q_H(\delta_{\tilde{u}})\left\langle \tilde{u},B^*(v_2)\right\rangle,w_1\right\rangle\\ & = & \left\langle \overline{B}^*(w_2),v_1\right\rangle \left\langle B^*(v_2),w_1\right\rangle =\left\langle \overline{B}^*(w_2),v_1\right\rangle \left\langle B(w_1),v_2\right\rangle=\left\langle \overline{B}^*(w_2)B(w_1),v\right\rangle\\ & = & \left\langle B(S(w_2))B(w_1),v\right\rangle =\left\langle B(S(w_2)w_1),v\right\rangle=\varepsilon(v)\varepsilon(w). \end{align}\] Thus, \((\theta \otimes \overline{\theta}) (R_{21}R) = 1 \otimes 1\), as claimed.

Hence, it follows from Claim 1 that \(\mathscr{Z}\subseteq \overline{\mathscr{Z}}'\), and since both categories have the same Frobenius-Perron dimension by Corollary 4 and [14], an equality holds, as claimed. ◻

Recall (see, e.g., [16]) that a finite braided tensor category is called non-degenerate if its Müger center is trivial.

Corollary 7. For each tensor subcategory \(\mathscr{Z}(K,H,B)\subseteq \mathscr{Z}(G)\), the following hold:

  1. \(\left(D(K,H,B),R(K,H,B)\right)\) is triangular if and only if \(\mathscr{Z}(K,H,B)\) is symmetric, if and only if, \(K\subseteq H\) and \(B\circ \iota_{K,H}=\iota_{K,H}^{\sharp}\circ \overline{B}:\mathbf{k}[K]\to \mathscr{O}(K)\).

    Furthermore, in this case \(K\) is commutative, so \(D(K,H,B)=\mathbf{k}[\widetilde{G}]\) as in Proposition 8(7), and we have \[R(K,H,B)=\sum_{u \in \mathcal{B}_K} (B(u)\#1)\otimes (q_K(\delta_u)\# 1)\in\mathbf{k}[K^{\vee}]^{\otimes 2}\quad\text{and}\] \[V(K,H,B)=\sum_{u \in \mathcal{B}_K} q_K(S(\delta_u))B(u)\#1\in\mathbf{k}[K^{\vee}].\]

  2. \(\left(D(K,H,B),R(K,H,B)\right)\) is factorizable if and only if \(\mathscr{Z}(K,H,B)\) is non-degenerate, if and only if, \(HK=G\) and \[\beta _{B,\overline{B}}=\left(\iota^{\sharp}_{K\cap H,K} B^* \iota_{K\cap H,H}\right)\star\left(\iota^{\sharp}_{K\cap H,H} B \iota_{K\cap H,K}\right):\mathbf{k}[K\cap H]\to \mathscr{O}(K\cap H)\] is a Hopf algebra isomorphism. In particular, if \(\mathscr{Z}(K,H,B)\) is non-degenerate then \(K\cap H\) is a self dual central subgroup scheme of \(G\).

  3. \(\mathscr{Z}(K,H,B)\) is Lagrangian if and only if \(K=H\) and \(B=\overline{B}\). In particular, if \(\mathscr{Z}(K,H,B)\) is Lagrangian then \(K=H\) is commutative, so \[D(H,H,B)=\mathbf{k}[H^{\vee}]\#^{\tau}_{\sigma}\mathbf{k}[G/H]=\mathbf{k}[\widetilde{G}],\] as in Proposition 8(7).

Proof. Fix \(\mathscr{Z}:=\mathscr{Z}(K,H,B)\subseteq \mathscr{Z}(G)\).

(1) Since \(\mathscr{Z}\) is symmetric if and only if \(\mathscr{Z}\subseteq \mathscr{Z}'\), if and only if by Theorem 12, \(\mathscr{Z}(K,H,B)\subseteq \mathscr{Z}(H,K,\overline{B})\), the claim follows from Corollary 6(1).

(2) Since \(\mathscr{Z}\) is non-degenerate if and only if \(\mathscr{Z}'\cap \mathscr{Z}=\operatorname{Vec}\), if and only if by Theorem 12, \(\mathscr{Z}(K,H,B)\cap \mathscr{Z}(H,K,\overline{B})=\mathscr{Z}(1,G,1)\), and since by Corollary 6(2), \(\mathscr{Z}(K,H,B)\cap \mathscr{Z}(H,K,\overline{B})=\mathscr{Z}(L,KH,\mathbf{B})\), we get that \(\mathscr{Z}(K,H,B)\) is non-degenerate if and only if \(G=KH\) and \(L=1\), so \(\beta _{B,\overline{B}}:\mathbf{k}[K\cap H]\to \mathscr{O}(K\cap H)\) is injective, hence a Hopf algebra isomorphism, as claimed.

(3) Since \(\mathscr{Z}\) is Lagrangian if and only if \(\mathscr{Z}'=\mathscr{Z}\), if and only if by Theorem 12, \(\mathscr{Z}(H,K,\overline{B})=\mathscr{Z}(K,H,B)\), the claim follows from Theorem 11. ◻

4.3 The simples and projectives of \(\mathscr{Z}(K,H,B)\)↩︎

Retain the notation from §2.4.

Fix a triple \(\left(K,H,B\right)\) as in Theorem 6. Recall that \(K\subseteq G\) is a normal subgroup scheme, so \(C_g\subset K\) for every \(g\in K(\mathbf{k})\), and let \({\rm C}_K(\mathbf{k}):=\{C_g\mid g\in K(\mathbf{k})\}\subseteq {\rm C}(\mathbf{k})\).

Fix \(C_g\in {\rm C}_K(\mathbf{k})\), with representative \(g\in C_g(\mathbf{k})\), and let \((M,\rho_M)\in {\rm Corep}(\mathscr{O}(G_g))\). Recall that for \(m\in M\), we write \(\rho_M(m)=m^{(-1)}\otimes m^{(0)}\in \mathscr{O}(G_g)\otimes M\). Let \[\begin{align} & \rho_M^g:\mathscr{O}(C_g)\otimes M\to \mathscr{O}(C_g)\otimes M\otimes \mathscr{O}(G),\\ & \rho_M^g(c\otimes m)= \left(i_g^{-1}\right)^{\sharp}\alpha_{g}\left(i_g^{\sharp}(c)_1\mu_g\left(m^{(-1)}\right)_1 \right)\otimes m^{(0)}\otimes i_g^{\sharp}(c)_2\mu_g\left(m^{(-1)}\right)_2, \end{align}\] and define \(\mathbf{F}_{C_g}(M,\rho_M)=\left(\mathscr{O}(C_g)\otimes M,\rho_M^g\right)\in \mathscr{Z}(G)_{C_g}\). In particular, the action of \(u\in\mathbf{k}[G]\) on \(c\otimes m\in \mathscr{O}(C_g)\otimes M\) is given by \[\label{actGonCg} \begin{align} & u\cdot (c\otimes m)=\left\langle u,i_g^{\sharp}(c)_2\mu_g\left(m^{(-1)}\right)_2\right\rangle \left(i_g^{-1}\right)^{\sharp}\alpha_{g}\left(i_g^{\sharp}(c)_1\mu_g\left(m^{(-1)}\right)_1 \right)\otimes m^{(0)}. \end{align}\tag{48}\] Note that since \(g\in K\), \(H\subseteq G\) is normal, and \(H\) centralizes \(K\), it follows that \(H\subseteq G_g\) is a normal subgroup scheme, and \(q_{G,H}=q_{G_g,H}\circ q_{G,G_g}\).

Lemma 5. For every \(v\in\mathbf{k}[H]\) and \(c\otimes m\in \mathscr{O}(C_g)\otimes M\), we have \[\iota_{H,G}(v)\cdot (c\otimes m)=\left\langle \iota_{H,G_g}(v),m^{(-1)}\right\rangle c\otimes m^{(0)}=c\otimes m\cdot \iota_{H,G_g}(v).\]

Proof. Since for every \(c\in \mathscr{O}(C_g)\), \(\Delta(i_g^{\sharp}(c))\in \mathscr{O}(G)\otimes\mathscr{O}(G/G_g)\), it follows from (48 ) that for every \(v\in\mathbf{k}[H]\subseteq \mathbf{k}[G_g]\) and \(c\otimes m\in \mathscr{O}(C_g)\otimes M\), we have \[\begin{align} \\ & = & \left\langle \iota_{H,G}(v_1),i_g^{\sharp}(c)_2\right\rangle \left\langle \iota_{H,G}(v_2),\mu_g\left(m^{(-1)}\right)_2\right\rangle \left(i_g^{-1}\right)^{\sharp}\alpha_{g}\left(i_g^{\sharp}(c)_1\mu_g\left(m^{(-1)}\right)_1 \right)\otimes m^{(0)}\\ & = & \varepsilon(i_g^{\sharp}(c)_2)\varepsilon(\iota_{H,G}(v_1)) \left\langle \iota_{H,G}(v_2),\mu_g\left(m^{(-1)}\right)_2\right\rangle \left(i_g^{-1}\right)^{\sharp}\alpha_{g}\left(i_g^{\sharp}(c)_1\mu_g\left(m^{(-1)}\right)_1 \right)\otimes m^{(0)}\\ & = & \left\langle \iota_{H,G}(v),\mu_g\left(m^{(-1)}\right)_2\right\rangle \left(i_g^{-1}\right)^{\sharp}\alpha_{g}\left(i_g^{\sharp}(c)\mu_g\left(m^{(-1)}\right)_1 \right)\otimes m^{(0)}\\ & = & \left\langle \iota_{H,G}(v),\mu_g\left(m^{(-1)}\right)_2\right\rangle \left(i_g^{-1}\right)^{\sharp}\left(i_g^{\sharp}(c)\alpha_{g}\left(\mu_g\left(m^{(-1)}\right)_1 \right)\right)\otimes m^{(0)}\\ & = & \left\langle \iota_{H,G}(v),\mu_g\left(m^{(-1)}\right)_2\right\rangle \left(i_g^{-1}\right)^{\sharp}\left(\alpha_{g}\left(\mu_g\left(m^{(-1)}\right)_1 \right)\right)c\otimes m^{(0)}\\ & = & \left\langle v,q_{G,H}(\mu_g\left(m^{(-1)}\right)_2)\right\rangle \left(i_g^{-1}\right)^{\sharp}\left(\alpha_{g}\left(\mu_g\left(m^{(-1)}\right)_1 \right)\right)c\otimes m^{(0)}\\ & = & \left\langle v,q_{G_g,H}(q_{G,G_g}(\mu_g\left(m^{(-1)}\right)_2))\right\rangle \left(i_g^{-1}\right)^{\sharp}\left(\alpha_{g}\left(\mu_g\left(m^{(-1)}\right)_1 \right)\right)c\otimes m^{(0)}\\ & = & \left\langle v,q_{G_g,H}(m^{(-1)}_2)\right\rangle \left(i_g^{-1}\right)^{\sharp}\left(\alpha_{g}(\mu_g(m^{(-1)}_1))\right)c\otimes m^{(0)}= \left\langle v,q_{G_g,H}(m^{(-1)})\right\rangle c\otimes m^{(0)}\\ & = & \left\langle \iota_{H,G_g}(v),m^{(-1)}\right\rangle c\otimes m^{(0)}=c\otimes m\cdot \iota_{H,G_g}(v), \end{align}\] as claimed, where we used (24 ) in the fourth to last equation and (25 ) in the third to last equation. ◻

From the \(G\)-equivariant Hopf algebra map \(B:\mathbf{k}[H]\to \mathscr{O}(K)\), we obtain the map \[\label{charBg} B_g:\mathbf{k}[H]\to \mathbf{k},\quad v\mapsto \langle B(v),g\rangle,\tag{49}\] which is a \(G_g\)-invariant character since for every \(u\in \mathbf{k}[G_g]\) and \(v\in \mathbf{k}[H]\), \[B_g({\rm ad_{\ell}}(S(u))(v))=\langle B({\rm ad_{\ell}}(S(u))(v)),g\rangle=\langle B(v),{\rm ad_{\ell}}(u)(g)\rangle=\langle B(v),g\rangle=B_g(v).\] We also obtain the Drinfeld twist \(\psi_g\) for \(\mathscr{O}(G_g/H)\) (i.e., a Hopf \(2\)-cocycle for \(\mathbf{k}[G_g/H]\)), given by \[\label{twistJg} \psi_g(x,y)=\langle \sigma(x,y),g\rangle ;\quad\forall x,y\in \mathbf{k}[G_g/H].\tag{50}\] Let \(\mathbf{k}^{\psi_g}[G_g/H]=(\mathscr{O}(G_g/H)_{\psi_g})^*\) be the associated twisted group algebra, and let \(\cdot\) denote its multiplication.

Lemma 6. For each \(g\in K(\mathbf{k})\), the map \[p_g:\mathbf{k}[G_g]\to \mathbf{k}^{\psi_g}[G_g/H],\quad u\mapsto B_g(\eta_H(u_1))\pi_H(u_2),\] is a surjective algebra homomorphism, which maps every \(v\in \mathbf{k}[H]\) to \(B_g(v)1\).

Proof. By Lemma 1(3) and Lemma 3(1), for every \(u,\tilde{u}\in \mathbf{k}[G_g]\), we have \[\begin{align} \\ & = & B_g\left(\eta(u_1)\gamma(\pi(u_2))_1\eta(\tilde{u}_1)S(\gamma(\pi(u_2))_2)\eta\{\gamma(\pi(u_2))_3\gamma(\pi(\tilde{u}_2))\}\right) \pi(u_3\tilde{u}_3)\\ & = & B_g\left(\eta(u_1)\eta(\tilde{u}_1)\eta\{\gamma(\pi(u_2))\gamma(\pi(\tilde{u}_2))\}\right) \pi(u_3\tilde{u}_3)\\ & = & B_g(\eta(u_1)\eta(\tilde{u}_1))\langle \sigma(\pi(u_2),\pi(\tilde{u}_2)),g\rangle \pi(u_3\tilde{u}_3)\\ & = & B_g(\eta(u_1)\eta(\tilde{u}_1))\psi_g(\pi(u_2),\pi(\tilde{u}_2))\pi(u_3\tilde{u}_3)\\ & = & B_g(\eta(u_1)\eta(\tilde{u}_1))\pi(u_2)\cdot \pi(\tilde{u}_2)= p_g(u)\cdot p_g(\tilde{u}), \end{align}\] as claimed. ◻

The injective coalgebra homomorphism \(p_g^*:\mathscr{O}(G_g/H)_{\psi_g}\xrightarrow{1:1}\mathscr{O}(G_g)\) induces an Abelian embedding \({\rm Corep}(\mathscr{O}(G_g/H)_{\psi_g})\subseteq {\rm Corep}(\mathscr{O}(G_g))\), so that \({\rm Corep}(\mathscr{O}(G_g/H)_{\psi_g})\) consists of all \(G_g\)-modules \(M\) for which \[\label{hinv} m\cdot \iota_{H,G_g}(v)=B_g(v)m;\quad \forall v\in \mathbf{k}[H],\,m\in M.\tag{51}\]

Now for each \(C_g\in {\rm C}_K(\mathbf{k})\), consider the full Abelian subcategory \[\widetilde{\mathscr{Z}}(K,H,B)_{C_g}:=\mathbf{F}_{C_g}({\rm Corep}(\mathscr{O}(G_g/H)_{\psi_g}))\subseteq \mathscr{Z}(G)_{C_g},\] and let \[\label{Dg} \widetilde{\mathscr{Z}}(K,H,B):=\bigoplus_{C_g\in {\rm C}_K(\mathbf{k})}\overline{\widetilde{\mathscr{Z}}(K,H,B)_{C_g}}\subseteq \mathscr{Z}(G).\tag{52}\]

Lemma 7. Fix \(\widetilde{\mathscr{Z}}:=\widetilde{\mathscr{Z}}(K,H,B)\) as in (52 ). Then the following hold:

  1. For each simple \(M\in {\rm Corep}(\mathscr{O}(G_g/H)_{\psi_g})\), we have \[P_{\widetilde{\mathscr{Z}}}(\mathbf{F}_{C_g}(M))=\mathscr{O}(K^{\circ})\otimes\mathscr{O}(C_g(\mathbf{k}))\otimes P_{(G_g/H,\psi_g)}(M).\]

  2. The Frobenius-Perron dimension of the Abelian subcategory \(\widetilde{\mathscr{Z}}\subseteq \mathscr{Z}(G)\) is equal to \(|K|[G:H]\).

  3. For each \(C_g\in {\rm C}_K(\mathbf{k})\), we have \(\overline{\widetilde{\mathscr{Z}}_{C_g}}=\mathscr{Z}(K,H,B)\cap \overline{\mathscr{Z}(G)_{C_g}}\). Thus, \[\mathscr{Z}(K,H,B)=\bigoplus_{C_g\in {\rm C}_K(\mathbf{k})}\mathscr{Z}(K,H,B)\cap \overline{\mathscr{Z}(G)_{C_g}}.\]

Proof. (1) The proof is similar to the proof of [1].

(2) By definition, using (1), we have \[\begin{align} \\ & = & \sum_{C_g\in {\rm C}_K(\mathbf{k}),\,M\in \mathcal{O}(G_g/H,\psi_g)} {\rm FPdim}(\mathbf{F}_{C_g}(M)){\rm FPdim}(P_{\widetilde{\mathscr{Z}}}(\mathbf{F}_{C_g}(M)))\\ & = & \sum_{C_g\in {\rm C}_K(\mathbf{k}),\,M\in \mathcal{O}(G_g/H,\psi_g)} |C_g|{\rm dim}_{\mathbf{k}}(M)|K^{\circ}||C_g(\mathbf{k})|{\rm dim}_{\mathbf{k}}\left(P_{(G_g/H,\psi_g)}(M)\right)\\ & = & \sum_{C_g\in {\rm C}_K(\mathbf{k})} |C_g||K^{\circ}||C_g(\mathbf{k})|[G_g:H]=\sum_{C_g\in {\rm C}_K(\mathbf{k})} [G:H]|K^{\circ}||C_g(\mathbf{k})|\\ & = & [G:H]|K|\sum_{C_g\in {\rm C}_K(\mathbf{k})} \frac{|C_g(\mathbf{k})|}{|K(\mathbf{k})|}=[G:H]|K|, \end{align}\] as claimed.

(3) If \(\mathbf{F}_{C_g}(M,\rho_M)\in \mathscr{Z}(K,H,B)\cap \mathscr{Z}(G)_{C_g}\), then by Lemma 5, \[\left\langle \iota_{H,G_g}(v),m^{(-1)}\right\rangle c\otimes m^{(0)}=q_{K,C_g}(B(v))c\otimes m\] for every \(v\in\mathbf{k}[H]\) and \(c\otimes m\in \mathscr{O}(C_g)\otimes M\). Applying \(g\otimes\operatorname{id}_M\) to both sides yields \[\left\langle \iota_{H,G_g}(v),m^{(-1)}\right\rangle c(g)m^{(0)}=B_g(v)c(g)m,\] which implies that \((M,\rho_M)\in {\rm Corep}(\mathscr{O}(G_g/H)_{\psi_g})\), so \[\mathscr{Z}(K,H,B)\cap \mathscr{Z}(G)_{C_g}\subseteq \widetilde{\mathscr{Z}}(K,H,B)_{C_g}.\] Thus, \(\mathscr{Z}(K,H,B)\cap \overline{\mathscr{Z}(G)_{C_g}}\subseteq \overline{\widetilde{\mathscr{Z}}(K,H,B)_{C_g}}\), so \(\mathscr{Z}(K,H,B)\subseteq \widetilde{\mathscr{Z}}(K,H,B)\). Since by (2), \(\widetilde{\mathscr{Z}}(K,H,B)\) and \(\mathscr{Z}(K,H,B)\) have the same Frobenius-Perron dimension, the claim follows. ◻

Theorem 13. Fix a braided subcategory \(\mathscr{Z}:=\mathscr{Z}(K,H,B)\subseteq \mathscr{Z}(G)\), and for each \(C_g\in {\rm C}_K(\mathbf{k})\), set \(\mathscr{Z}_{C_g}:=\mathscr{Z} \cap \mathscr{Z}(G)_{C_g}\). Then the following hold:

  1. The Abelian equivalence \(\mathbf{F}_{C_g}\) (27 ) restricts to an equivalence \[\mathbf{F}_{C_g}:{\rm Corep}(\mathscr{O}(G_g/H)_{\psi_g})\xrightarrow{\simeq}\mathscr{Z}_{C_g},\quad (M,\rho_M)\mapsto \left(\mathscr{O}(C_g)\otimes M,\rho_M^g\right).\] In particular, the composition functor \[\operatorname{Rep}(G/H)\simeq {\rm Corep}(\mathscr{O}(G/H))\xrightarrow{\mathbf{F}_{1}}\mathscr{Z}_1\hookrightarrow \mathscr{Z}\] coincides with the canonical embedding \(\operatorname{Rep}(G/H)\hookrightarrow \mathscr{Z}\) of braided categories.

  2. For each \(C_g\in {\rm C}_K(\mathbf{k})\), with representative \(g\in C_g(\mathbf{k})\), there is a bijection between the set of equivalence classes of simple objects \(M\in {\rm Corep}(\mathscr{O}(G_g/H)_{\psi_g})\) and isomorphism classes of simple objects of \(\mathscr{Z}_{C_g}\), assigning \(M\) to \(\mathbf{F}_{C_g}(M)\). Moreover, we have a direct sum decomposition of Abelian categories \[\mathscr{Z}(K,H,B)=\bigoplus_{C_g\in {\rm C}_K(\mathbf{k})}\overline{\mathscr{Z}_{C_g}},\] and \(\overline{\operatorname{Rep}(G/H)}\simeq \overline{\mathscr{Z}_{1}}=\mathscr{Z}\left(K^{\circ},H,\iota^{\sharp}_{K^{\circ},K}\circ B\right)\). In particular, if \(G\) is connected then the simples of \(\mathscr{Z}\) are precisely those of \(\operatorname{Rep}(G/H)\simeq {\rm Corep}(\mathscr{O}(G/H))\).

  3. For each \((M,\rho_M)\in {\rm Corep}(\mathscr{O}(G_g/H)_{\psi_g})\), we have \(\mathbf{F}_{C_g}(M,\rho_M)^*\cong \mathbf{F}_{C_{g^{-1}}}(M^*,\rho_{M^*})\).

  4. For each \((M,\rho_M)\in {\rm Corep}(\mathscr{O}(G_g/H)_{\psi_g})\), we have \[{\rm FPdim}\left(\mathbf{F}_{C_g}(M,\rho_M)\right)=|C_g|{\rm dim}_{\mathbf{k}}(M).\]

  5. For each simple \((M,\rho_M)\in {\rm Corep}(\mathscr{O}(G_g/H)_{\psi_g})\), we have \[P_{\mathscr{Z}}\left(\mathbf{F}_{C_g}(M,\rho_M)\right)\cong \left(\mathscr{O}(K^{\circ})\otimes\mathscr{O}(C_g(\mathbf{k}))\otimes P_{(G_g/H,\psi_g)}(M,\rho_M),R_M^g\right),\] where \(\mathscr{O}(K)\) acts on the first two factors diagonally, and \[R_{M}^g:=\left(\chi_{C_g}\otimes\operatorname{id}^{\otimes 2}\right)\left(\operatorname{id}_{\mathscr{O}(K^{\circ})}\otimes\rho_{P_{(G_g/H,\psi_g)}(M,\rho_M)}^g\right)\left(\nu_{C_g}\otimes\operatorname{id}\right).\] In particular, we have \[{\rm FPdim}\left(P_{\mathscr{Z}}\left(\mathbf{F}_{C_g}(M,\rho_M)\right)\right)=|K^{\circ}||C_g(\mathbf{k})|{\rm dim}_{\mathbf{k}}\left(P_{(G_g/H,\psi_g)}(M,\rho_M)\right).\]

  6. For each \(C_g\in {\rm C}_K(\mathbf{k})\), we have \({\rm FPdim}\left(\overline{\mathscr{Z}_{C_g}}\right)=|K^{\circ}||C_g(\mathbf{k})|[G:H]\).

Proof. (1)-(2) These follow from Lemma 7.

(3) This follows from [1] (see Theorem 3).

(4) This follows from (1).

(5)-(6) These follow from [1] and the previous parts. ◻

5 Some special cases and examples↩︎

5.1 Canonical examples↩︎

The following are some canonical Hopf quotients of \(D(G)\) and their corresponding braided subcategories of \(\mathscr{Z}(G)\):

(1) We have \[D(1,G,1)=\mathbf{k},\quad D(G,1,1)=D(G),\quad D(1,1,1)=\mathbf{k}[G].\] Thus, we have \[\mathscr{Z}(1,G,1)={\rm Vect},\quad \mathscr{Z}(1,G,1)'=\mathscr{Z}(G,1,1)=\mathscr{Z}(G),\quad \mathscr{Z}(1,1,1)=\operatorname{Rep}(G).\]

(2) For every normal subgroup scheme \(K\subseteq G\), we have \(D(1,K,1)=\mathbf{k}[G/K]\), and \(D(K,1,1)=\mathscr{O}(K)^{{\rm cop}}\# \mathbf{k}[G]\) is a tensor product coalgebra and smash product algebra. In particular, \(D(1,G^{\circ},1)=\mathbf{k}[G(\mathbf{k})]\), and \(D(G^{\circ},1,1)=\mathscr{O}(G^{\circ})^{{\rm cop}}\# \mathbf{k}[G]\).

(3) For every normal subgroup scheme \(K\subseteq G\), a central subgroup scheme \(H\subseteq G\), and a \(G\)-equivariant group scheme morphism \(B:K\to H^{\vee}\), the Hopf algebra \[D(K,H,B)=\mathscr{O}(K)\#_{\sigma}^{\tau} \mathbf{k}[G/H]\] is a tensor product coalgebra and smash product algebra, and by Proposition 8(7), \[D(H,K,\overline{B})=\mathbf{k}[H^{\vee}]\#_{\sigma}^{\tau} \mathbf{k}[G/K]=\mathbf{k}[\widetilde{G}],\] where \(\widetilde{G}\) is the group scheme extension of \(H^{\vee}\) by \(G/K\) corresponding to \[\sigma\in Z^2(H^{\vee},G/K),\quad \tau\in Z^1(H^{\vee},G/K),\] with trivial action. Thus, we have \[\mathscr{Z}(K,H,B)=\operatorname{Rep}\left(\mathscr{O}(K)\#_{\sigma}^{\tau} \mathbf{k}[G/H]\right),\] and \(\mathscr{Z}(K,H,B)'=\mathscr{Z}(H,K,\overline{B})=\operatorname{Rep}(\widetilde{G})\).

5.2 Direct products↩︎

Let \(G:=K\times H\), and let \(B:\mathbf{k}[H]\xrightarrow{}\mathscr{O}(K)\) be any \(G\)-equivariant Hopf algebra map. Then \[\mathscr{Z}(K\times 1,1\times H,B)\subseteq \mathscr{Z}(G)\] is a non-degenerate braided subcategory. Note that since \(\sigma\) and \(\tau\) are trivial by Remark 5, it follows that \[\mathscr{Z}(K\times 1,1\times H,B)\cong \mathscr{Z}(K)\] as braided categories (regardless of the choice of \(B\)).

5.3 Constant groups↩︎

Assume that \(G\) is constant; that is, \(G=G(\mathbf{k})\). For \(g\in G\), let \(\delta_g\in \mathscr{O}(G)\) be the delta function at \(g\). The elements \(\{\delta_g\}_{g\in G}\) are pairwise orthogonal idempotents, hence any \(\mathscr{O}(G)\)-module \(V\) decomposes as \[V = \bigoplus_{g\in G} V_g, \qquad V_g:=\delta_gV.\] Recall that in this case a \(D(G)\)-module is a \(G\)-graded vector space \(V=\bigoplus_{g\in G}V_g\), together with an action of \(G\), such that \(x\cdot V_g \subseteq V_{xgx^{-1}}\) for every \(x,g\in G\).

Now fix a triple \((K,H,B)\) and let \(\theta:D(G)\twoheadrightarrow D(K,H,B)\) be the quotient map as in Theorem 6. Since in this case \(\gamma_H\) is a coalgebra map, we have that \[D(K,H,B)=\mathscr{O}(K)^{{\rm cop}}\#_{\sigma}\mathbf{k}[G/H]\] is a tensor product coalgebra by Proposition 8(4).

If \(V\in\operatorname{Rep}(D(K,H,B))=\mathscr{Z}(K,H,B)\), and we inflate \(V\) along \(\theta\) to a \(D(G)\)-module, then the \(\mathscr{O}(G)\)-action factors through \(q_K:\mathscr{O}(G)\twoheadrightarrow\mathscr{O}(K)\). In particular, \(q_K(\delta_g)=0\) for \(g\notin K\), so \(V_g=\delta_gV=0\) unless \(g\in K\). Thus, \(V\) is supported on \(K\). Moreover, for \(h\in H\), we have \(\pi_H(h)=1\) and \(\eta_H(h)=h\), hence \[\theta(1\bowtie h)=B(h)\# 1\in \mathscr{O}(K)\#_{\sigma}\mathbf{k}[G/H],\] so on each homogeneous component \(V_k\), \(k\in K\), the element \(h\) acts by the scalar \(B(h)(k)\). Equivalently, setting \[\beta:H\times K\to \mathbf{k}^\times,\qquad \beta(h,k):=B(h)(k),\] we see that \(\mathscr{Z}(K,H,B)\) consists precisely of \(G\)-equivariant sheaves on \(G\) supported on \(K\) for which the action of \(H\) on the fibre over \(k\in K\) is given by \(\beta(h,k)\), so in the fusion case, \(\mathscr{Z}(K,H,B)\) is the category \(\mathcal{S}(K,H,B)\) from [2].

It follows from Theorem 13, similarly to [11], that we have a direct sum decomposition of Abelian categories \[\mathscr{Z}(K,H,B)=\bigoplus_{C_g\in {\rm C}_K}\mathscr{Z}(K,H,B)_{C_g}\simeq \bigoplus_{C_g\in {\rm C}_K}{\rm Corep}(\mathscr{O}(G_g/H)_{\psi_g}),\] given by \(\mathbf{F}_{C_g}\), \(C_g\in {\rm C}_K\), and for every simple \(M\in {\rm Corep}(\mathscr{O}(G_g/H)_{\psi_g})\), we have \[P_{\mathscr{Z}(K,H,B)}\left(\mathbf{F}_{C_g}(M)\right)= \mathbf{F}_{C_g}(P_{(G_g/H,\psi_g)}(M))= \left(\mathscr{O}(C_g)\otimes P_{(G_g/H,\psi_g)}(M),\rho_{P_{(G_g/H,\psi_g)}(M)}^g\right),\] where \(\mathscr{O}(K)\) acts on the first factor.

5.4 Connected groups↩︎

Assume that \(G\) is connected; that is, \(G(\mathbf{k})=1\) (e.g., \(G\) is the finite group scheme associated to a finite dimensional restricted \(p\)-Lie algebra \(\mathfrak{g}\)). Then it follows from Theorem 13, similarly to [11], that for each triple \(\left(K,H,B\right)\) as in Theorem 6, we have \(\mathscr{Z}(K,H,B)=\overline{{\rm Rep}\left(G/H\right)}\), and for every simple \(M\in \operatorname{Rep}\left(G/H\right)\), we have \[P_{\mathscr{Z}(K,H,B)}\left(\mathbf{F}(M)\right)\cong \left(\mathscr{O}(K)\otimes P_{G/H}(M),\operatorname{id}\otimes\rho_{P_{G/H}(M)}\right),\] where \(\mathscr{O}(K)\) acts on the first factor.

Example 1. Let \(\mathfrak{g}\) be the unique \(2\)-dimensional non-Abelian restricted \(p\)-Lie algebra with basis \(\{x,y\}\), such that \([x,y]=y\), \(x^{[p]}=x\), and \(y^{[p]}=0\). Then \(\mathfrak{g}={\rm Lie}(G_1)\), where \(G_1\) is the Frobenius kernel of the group scheme \(G:=\mathbb{G}_a\rtimes \mathbb{G}_m\) of automorphisms of the affine line \(\mathbb{A}^1\). It is clear that \(\mathfrak{a}:={\rm sp}_{\mathbf{k}}\{y\}={\rm Lie}(\mathbb{G}_{a,1})\subseteq \mathfrak{g}\) is an ideal, \(\mathfrak{g}/\mathfrak{a}={\rm Lie}(\mathbb{G}_{m,1})\), and \(G_1=\mathbb{G}_{a,1}\rtimes \mathbb{G}_{m,1}\).

We have the (degenerate non-symmetric) braided subcategory \[\mathscr{Z}\left(\mathbb{G}_{a,1},1,1\right)=\operatorname{Rep}(\mathbb{G}_{a,1}^{\vee}\times G_1)\subseteq \mathscr{Z}(G_1)\] of Frobenius-Perron dimension \(p^3\), and the infinite family of non-equivalent braided subcategories \[\mathscr{Z}_{\lambda}:=\mathscr{Z}\left(\mathbb{G}_{a,1},\mathbb{G}_{a,1},B_{\lambda}\right)=\operatorname{Rep}(\mathbb{G}_{a,1}^{\vee}\times \mathbb{G}_{m,1},R_{\lambda})\subseteq \mathscr{Z}(G_1)\] of Frobenius-Perron dimension \(p^2\) parameterized by \(\lambda \in \mathbf{k}\), where \(B_{\lambda}\) and \(R_{\lambda}\) are given in §6.2. Note that \(\mathscr{Z}_{\lambda}\) is Lagrangian if and only if \(\lambda=0\), and that \(\mathscr{Z}_0\) and \(\mathscr{Z}\left(1,1,1\right)=\operatorname{Rep}(G_1,1\otimes 1)\) are not equivalent as braided subcategories of \(\mathscr{Z}(G_1)\), as predicted by Theorem 11. 0◻

Example 2. Let \(\mathfrak{g}\) be the \(3\)-dimensional Heisenberg \(p\)-Lie algebra with basis \(\{x,y,z\}\), such that \([x,y]=z\). Let \(\mathfrak{h}:={\rm sp}_{\mathbf{k}}\{z\}\subset \mathfrak{g}\), and let \(\mathfrak{k}:={\rm sp}_{\mathbf{k}}\{x,z\}\subset \mathfrak{g}\); the former is a central ideal, and the latter is an ideal. Recall that for \(p>2\), \(\mathfrak{g}\) admits exactly three non-isomorphic \([p]\)-structures, given by \[x^{[p]}=y^{[p]}=z^{[p]}=0;\quad x^{[p]}=z,\,y^{[p]}=z^{[p]}=0;\quad x^{[p]}=y^{[p]}=0,\,z^{[p]}=z.\]

In each case, let \(G\) be the finite group scheme such that \(\mathscr{O}(G)=(u^{[p]}(\mathfrak{g}))^*\); it is a local commutative Hopf algebra of dimension \(p^3\) (so, \(u^{[p]}(\mathfrak{g})\) is connected). Also, let \(H\subset G\) be the central subgroup scheme such that \(\mathfrak{h}={\rm Lie}(H)\), and \(K\subset G\) the normal subgroup scheme such that \(\mathfrak{k}={\rm Lie}(K)\).

The case \(x^{[p]}=y^{[p]}=z^{[p]}=0\): In this case, \(\mathfrak{g}\) is \([p]\)-unipotent, so that \(u^{[p]}(\mathfrak{g})\) is local (and connected). Thus, \(D(G)=(u^{[p]}(\mathfrak{g}))^{*{\rm cop}}\bowtie u^{[p]}(\mathfrak{g})\) is local and connected. Also, \(H\cong \mathbb{G}_{a,1}\), \(G/H\cong \mathbb{G}_{a,1}^2\), \(K\cong \mathbb{G}_{a,1}^2\), and \(G/K\cong \mathbb{G}_{a,1}\).

(1) We have an infinite family of non-equivalent unipotent braided subcategories \[\mathscr{Z}\left(H,H,B_{\lambda}\right)=\operatorname{Rep}(\mathbf{k}[\mathbb{G}_{a,1}^{\vee}]\#_{\sigma}^{\tau}\mathbf{k}[\mathbb{G}_{a,1}^2],R_{\lambda})=\operatorname{Rep}(\widetilde{G},R_{\lambda})\subseteq \mathscr{Z}(G)\] of Frobenius-Perron dimension \(p^3\), parameterized by \(\lambda \in \mathbf{k}\), where \(\widetilde{G}\) is the finite group scheme extension of \(\mathbb{G}_{a,1}^2\) by \(\mathbb{G}_{a,1}^{\vee}\) corresponding to \(\tau\in Z^1(\mathbb{G}_{a,1}^2,(\mathbb{G}_{a,1}^{\vee})^2)\) and \(\sigma\in Z^2(\mathbb{G}_{a,1}^2,\mathbb{G}_{a,1}^{\vee})\), and \(B_{\lambda}\) and \(R_{\lambda}\) are given in §6.2.

(2) We have an infinite family of non-equivalent unipotent braided subcategories \[\mathscr{Z}(K,H,B)=\operatorname{Rep}(\mathbf{k}[(\mathbb{G}_{a,1}^{\vee})^2]\#_{\sigma}^{\tau}\mathbf{k}[\mathbb{G}_{a,1}^2],R_B)=\operatorname{Rep}(\widetilde{G},R_B)\subseteq \mathscr{Z}(G)\] of Frobenius-Perron dimension \(p^4\), parameterized by \(B\in \operatorname{Hom}(\mathbb{G}_{a,1},(\mathbb{G}_{a,1}^{\vee})^2)\), where \(\widetilde{G}\) is the group scheme extension of \(\mathbb{G}_{a,1}^2\) by \((\mathbb{G}_{a,1}^{\vee})^2\) corresponding to \(\sigma\in Z^2(\mathbb{G}_{a,1}^2,(\mathbb{G}_{a,1}^{\vee})^2)\) and \(\tau\in Z^1(\mathbb{G}_{a,1}^2,(\mathbb{G}_{a,1}^{\vee})^4)\).

The case \(x^{[p]}=z,\,y^{[p]}=z^{[p]}=0\): In this case \(H\cong \mathbb{G}_{a,1}\) and \(G/H\cong \mathbb{G}_{m,1}\times \mathbb{G}_{a,1}\), so we have the infinite family of non-equivalent braided subcategories \[\mathscr{Z}\left(H,H,B_{\lambda}\right)=\operatorname{Rep}(\mathbf{k}[\mathbb{G}_{a,1}^{\vee}]\#_{\sigma}^{\tau}\mathbf{k}[\mathbb{G}_{m,1}\times \mathbb{G}_{a,1}],R_{\lambda})=\operatorname{Rep}(\widetilde{G},R_{\lambda})\subseteq \mathscr{Z}(G)\] of Frobenius-Perron dimension \(p^3\), parameterized by \(\lambda \in \mathbf{k}\), where \(\widetilde{G}\) is the group scheme extension of \(\mathbb{G}_{m,1}\times \mathbb{G}_{a,1}\) by \(\mathbb{G}_{a,1}^{\vee}\) corresponding to \(\sigma\in Z^2(\mathbb{G}_{m,1}\times \mathbb{G}_{a,1},\mathbb{G}_{a,1}^{\vee})\) and \(\tau\in Z^1(\mathbb{G}_{m,1}\times \mathbb{G}_{a,1},(\mathbb{G}_{a,1}^{\vee})^2)\), and \(B_{\lambda}\) and \(R_{\lambda}\) are given in §6.2.

The case \(x^{[p]}=y^{[p]}=0,\,z^{[p]}=z\): In this case \(H\cong \mathbb{G}_{m,1}\) and \(G/H\cong \mathbb{G}_{a,1}^2\). Since the only group scheme morphism \(\mathbb{G}_{a,1}\to \mathbb{Z}/p\mathbb{Z}\) is the trivial one, we only have the symmetric subcategory \[\mathscr{Z}\left(H,H,1\right)=\operatorname{Rep}(\mathbb{Z}/p\mathbb{Z}\times \mathbb{G}_{a,1}^2,1\otimes 1)\subseteq \mathscr{Z}(G)\] of Frobenius-Perron dimension \(p^3\). 0◻

5.5 Trivial \(B\)↩︎

Set \(\mathscr{Z}(K,H):=\mathscr{Z}(K,H,1)\). Since by definition, an object \(X\) in \({\rm Coh}(K)^{G/H}\) is an \(\mathscr{O}(K)\)-module in the category \(\operatorname{Rep}(G/H)\), it follows from Proposition 8(5) that we have a natural embedding of tensor categories \[{\rm Coh}(K)^{G/H}\xrightarrow{1:1} \mathscr{Z}(K,H).\] Since both categories have the same Frobenius-Perron dimension, it follows that we have an equivalence of tensor categories \[\mathscr{Z}(K,H)\simeq {\rm Coh}(K)^{G/H}.\]

Now consider \(K\) as a subgroup scheme of \(K\times G/H\) via the group scheme embedding \[\Delta_{K,H}:K\to K\times G/H,\quad k\mapsto (k,\pi_H(k)).\] Then, similarly to the proof that \(\mathscr{Z}(G)\simeq {\rm Coh}(G)^{G}\simeq \mathscr{C}(G\times G,\Delta_{G,1}(G))\) [1], we have an equivalence of tensor categories \[{\rm Coh}(K)^{G/H}\simeq \mathscr{C}(K\times G/H,\Delta_{K,H}(K)),\] so \(\mathscr{Z}(K,H)\) is group scheme-theoretical in the sense of [9]. In particular, by [13], it follows that \(\mathscr{Z}(K,H)\) has the finite generation property, and [9] implies the classification of exact indecomposable module categories over \(\mathscr{Z}(K,H)\).

5.6 Commutative groups↩︎

Assume that \(A\subseteq G\) is a normal commutative subgroup scheme (e.g. \(A\) is contained in the center of \(G\)). Then \(D(A,A,1)=\mathbf{k}[A^{\vee}\times G/A]\) is a triangular Hopf algebra, where \(A^{\vee}\) is the Cartier dual of \(A\), and \[\mathscr{Z}(A,A,1)=\operatorname{Rep}\left(A^{\vee}\times G/A\right)\subseteq \mathscr{Z}(G)\] is a Lagrangian subcategory.

More generally, if \(B:A\to A^{\vee}\) is any \(G\)-equivariant group scheme morphism, then \((D(A,A,B),R_B)=(\mathbf{k}[A^{\vee}]\#_{\sigma}^{\tau} \mathbf{k}[G/A],R_B)=(\mathbf{k}[\widetilde{G}],R_B)\) is a quasitriangular Hopf algebra (see Proposition 8(7)), and by Corollary 7(3), the braided subcategory \[\mathscr{Z}(A,A,B)=\operatorname{Rep}\left(\mathbf{k}[A^{\vee}]\#_{\sigma}^{\tau} \mathbf{k}[G/A],R_B\right)=\operatorname{Rep}(\widetilde{G},R_B)\subseteq \mathscr{Z}(G)\] is Lagrangian if and only if \(B=\overline{B}:=B^{\vee}S\).

Assume further that \(G\) is commutative. Then for any group scheme morphism \(B:A\xrightarrow{}A^{\vee}\), we have the braided subcategory \[\mathscr{Z}(A,A,B)=\operatorname{Rep}\left(\mathbf{k}[A^{\vee}]\#_{\sigma}^{\tau} \mathbf{k}[G/A],R_B\right)=\operatorname{Rep}(\widetilde{G},R_B)\subseteq \mathscr{Z}(G);\] by Corollary 7(3), it is Lagrangian if and only if \(B=\overline{B}\).

Assume even further that \(G\) is self dual. Then for each group scheme morphism \(B:G\xrightarrow{}G^{\vee}\), by Corollary 7(2), the braided subcategory \[\mathscr{Z}(G,G,B)=\operatorname{Rep}\left(\mathbf{k}[G^{\vee}],R_B\right)\subseteq \mathscr{Z}(G)\] is non-degenerate if and only if \(B\star B^{\vee}:G\xrightarrow{\cong }G^{\vee}\) is a group scheme isomorphism.

For example, let \(G:=\mathbb{G}_{a,1}\). In §6.2 we show that \[\mathscr{Z}(\mathbb{G}_{a,1},\mathbb{G}_{a,1},B_{\lambda})=\operatorname{Rep}\left(\mathbf{k}[\mathbb{G}_{a,1}^{\vee}],R_{\lambda}\right)\subseteq \mathscr{Z}(\mathbb{G}_{a,1})\] is an infinite family of non-equivalent non-degenerate braided subcategories of Frobenius-Perron dimension \(p\), parametrized by \(\lambda\in \mathbf{k}^{\times}\), where \(R_{\lambda}\) is given in (54 ).

Example 3. As mentioned in Remark 7, if \(\eta\) or \(\gamma\) is a coalgebra map, then \(\tau\) is trivial. In §6.3 we give an example of a nontrivial \(\tau\) for \(G= \mathbb{G}_{a,2}\) and \(H = K = \mathbb{G}_{a,1}\) (9), and deduce that for each \(\lambda\in \mathbf{k}^{\times}\), the quasitriangular Hopf algebra \[\left(D(\mathbb{G}_{a,1},\mathbb{G}_{a,1},B_{\lambda}),R_{\lambda}\right)= \left(\mathbf{k}[\mathbb{G}_{a,1}^{\vee}]\#^{\tau} \mathbf{k}[\mathbb{G}_{a,2}/\mathbb{G}_{a,1}],R_{\lambda}\right)=\left(\mathbf{k}[\widetilde{\mathbb{G}_{a,1}}],R_{\lambda}\right)\] is neither a tensor product coalgebra nor a tensor product algebra, where \(R_{\lambda}\) is given in (55 ). Thus, \[\mathscr{Z}(\mathbb{G}_{a,1},\mathbb{G}_{a,1},B_{\lambda})=\operatorname{Rep}\left(\mathbf{k}[\mathbb{G}_{a,1}^{\vee}]\#^{\tau} \mathbf{k}[\mathbb{G}_{a,2}/\mathbb{G}_{a,1}],R_{\lambda}\right)=\operatorname{Rep}\left(\widetilde{\mathbb{G}_{a,1}},R_{\lambda}\right)\subseteq \mathscr{Z}(\mathbb{G}_{a,2})\] is an infinite family of non-equivalent braided subcategories of Frobenius-Perron dimension \(p^2\), parametrized by \(\lambda\in \mathbf{k}\).

Note that since \(\sigma\) is trivial, we have \(\widetilde{\mathbb{G}_{a,1}}=\mathbb{G}_{a,1}^2\). 0◻

6 Appendix↩︎

6.1 The group scheme \(\mathbb{G}_{a,r}\)↩︎

Let \(\mathbb{G}_{a,r}\) denote the \(r\)-th Frobenius kernel of \(\mathbb{G}_a\). Recall that \(\mathscr{O}(\mathbb{G}_{a,r}) = \mathbf{k}[t]/(t^{p^r})\) with \(t\) primitive. Fix the basis \(\{t^i\}_{0\le i\le p^r-1}\) for \(\mathscr{O}(\mathbb{G}_{a,r})\) and denote by \(\{\delta_i\}_{0\le i\le p^r-1}\) the dual basis. The multiplication in \(\mathbf{k}[\mathbb{G}_{a,r}]\) is determined by \[\delta_m\delta_n=\begin{cases} \binom{m+n}{m}\delta_{m+n},& m+n<p^r\\ 0,& \text{otherwise}. \end{cases}\] The unit is \(\delta_0\), and one has \[\Delta(\delta_n)=\sum_{a+b=n}\delta_a\otimes\delta_b,\quad \varepsilon(\delta_n)=\delta_{n,0},\quad S(\delta_n)=(-1)^n\delta_n.\] It is well-known that the map \[F_r: \mathbf{k}[X_0,\ldots,X_{r-1}]/(X_0^p,\ldots,X_{r-1}^p) \to \mathbf{k}[\mathbb{G}_{a,r}],\quad X_i\mapsto \delta_{p^i},\] is an algebra isomorphism with inverse given by \[F_r^{-1}:\mathbf{k}[\mathbb{G}_{a,r}]\to \mathbf{k}[X_0,\ldots,X_{r-1}]/(X_0^p,\ldots,X_{r-1}^p),\quad \delta_n\mapsto \frac{1}{a_{0}! \cdots a_{r-1}!} X_0^{a_0} \cdots X_{r-1}^{a_{r-1}},\] where \(n = a_0 + \cdots + a_{r-1}p^{r-1}\) is the \(p\)-adic expansion of \(n\).

6.2 The center \(\mathscr{Z}(\mathbb{G}_{a,1})\)↩︎

Since \(F_1^{-1}:\mathbf{k}[\mathbb{G}_{a,1}] \xrightarrow{\cong }\mathscr{O}(\mathbb{G}_{a,1})\) is a Hopf algebra isomorphism, it follows that Hopf algebra maps \(\mathbf{k}[\mathbb{G}_{a,1}] \to \mathscr{O}(\mathbb{G}_{a,1})\) are parameterized by elements \(\lambda \in \mathbf{k}\), where \[\label{bz} B_{\lambda}: \mathbf{k}[\mathbb{G}_{a,1}] \to \mathscr{O}(\mathbb{G}_{a,1}),\quad \delta_n\mapsto \frac{\lambda^n}{n!}t^n.\tag{53}\] This is an isomorphism if and only if \(\lambda \neq 0\). Note that \(B_{\lambda}=\overline{B_{\lambda}}\) if and only if \(\lambda=0\) or \(p=2\) (since \(B_{\lambda}=B_{\lambda}^*\)).

It now follows from Corollary 3 in a straightforward manner that for each \(\lambda\in\mathbf{k}\), \[\label{rz1} R_{\lambda}:=\sum_{i=0}^{p-1}\frac{\lambda^i}{i!}(t^i\otimes t^i)\tag{54}\] is an \(R\)-matrix for \(D(\mathbb{G}_{a,1},\mathbb{G}_{a,1},B_{\lambda})=\mathbf{k}[\mathbb{G}_{a,1}^{\vee}]\). By Corollary 7(2), \((\mathbf{k}[\mathbb{G}_{a,1}^{\vee}],R_{\lambda})\) is factorizable if and only if \(\lambda \neq 0\); that is, \(R_{\lambda}\ne 1\otimes 1\).

6.3 The center \(\mathscr{Z}(\mathbb{G}_{a,2})\)↩︎

By Theorem 6, since \(\mathbb{G}_{a,2}\) is commutative, Hopf quotient pairs of \(D(\mathbb{G}_{a,2})\) are indexed by \((K,H,B)\), where \(K\) and \(H\) are subgroup schemes of \(\mathbb{G}_{a,2}\), and \(B : \mathbf{k}[H] \to \mathscr{O}(K)\) is a Hopf algebra map. We will now compute the Hopf quotient pairs for \(K = H = \mathbb{G}_{a,1}\), up to equivalence, following the construction laid out in §3.

We have \[q:=q_{\mathbb{G}_{a,1}} : \mathscr{O}(\mathbb{G}_{a,2}) \twoheadrightarrow \mathscr{O}(\mathbb{G}_{a,1}),\quad t\mapsto t,\] with section \[\mu:=\mu_{\mathbb{G}_{a,1}} : \mathscr{O}(\mathbb{G}_{a,1}) \xrightarrow{1:1} \mathscr{O}(\mathbb{G}_{a,2}),\quad t\mapsto t.\]

Next consider the exact sequence of Hopf algebras \[\mathbf{k} \to \mathbf{k}[\mathbb{G}_{a,1}] \to \mathbf{k}[\mathbb{G}_{a,2}] \xrightarrow{\pi:=\pi_{\mathbb{G}_{a,1}}} \mathbf{k}[\mathbb{G}_{a,2}/\mathbb{G}_{a,1}] \to \mathbf{k}.\]

Lemma 8. The following hold:

  1. The surjective Hopf algebra map \(\pi\) is determined by \[\delta_n \mapsto \begin{cases} \delta_{n/p},& p\mid n\\ 0,& p\nmid n \end{cases}\]

  2. The map \(\gamma:=\gamma_{\mathbb{G}_{a,1}}\) determined by \[\gamma: \mathbf{k}[\mathbb{G}_{a,2}/\mathbb{G}_{a,1}] \to \mathbf{k}[\mathbb{G}_{a,2}],\quad \delta_n \mapsto \delta_{pn},\] is a cleaving map.

  3. \(\gamma\) is not a coalgebra map.

  4. The convolution inverse of \(\gamma\) is given by \(\gamma^{-1}(\delta_n)=(-1)^n\delta_{pn}\).

  5. The action \(\cdot\) of \(\mathbf{k}[\mathbb{G}_{a,2}/\mathbb{G}_{a,1}]\) on \(\mathscr{O}(\mathbb{G}_{a,1})\) is trivial.

  6. \(\eta:=\eta_{\mathbb{G}_{a,1}} = \operatorname{id}\star \gamma^{-1}\pi\) is the projection of \(\mathbf{k}[\mathbb{G}_{a,2}]\) onto the subspace \(\mathbf{k}[\mathbb{G}_{a,1}]\).

  7. The convolution inverse of \(\eta\) is given by \[\eta^{-1}(\delta_n)= \begin{cases} (-1)^n\delta_n,& 0\le n<p,\\ 0,& p\le n<p^2. \end{cases}\]

Proof. (1) It is easy to see that \(\mathbf{k}[\mathbb{G}_{a,1}]^+ = \text{sp}_{\mathbf{k}}\{\delta_1,\ldots,\delta_{p-1}\}\), and moreover that \[\mathbf{k}[\mathbb{G}_{a,1}]^+ \mathbf{k}[\mathbb{G}_{a,2}] = \text{sp}_{\mathbf{k}}\{\delta_n \mid p \nmid n\}.\] The \(\mathbf{k}\)-linear map \(\mathbf{k}[\mathbb{G}_{a,2}] \to \mathbf{k}[\mathbb{G}_{a,1}]\) determined by \[\delta_n \mapsto \begin{cases} \delta_{n/p},& p\mid n\\ 0,& p\nmid n \end{cases}\] is a surjective algebra map with kernel \(\mathbf{k}[\mathbb{G}_{a,1}]^+ \mathbf{k}[\mathbb{G}_{a,2}]\), so \(\mathbf{k}[\mathbb{G}_{a,2}/\mathbb{G}_{a,1}]\cong \mathbf{k}[\mathbb{G}_{a,1}]\) and this map is precisely the Hopf algebra map \(\pi\), as claimed.

(2) - (4) These are straightforward verification, and (5) is clear.

(6) For every \(0\le n<p^2\), we have \[\eta(\delta_n) = \sum_{a+b = n} \delta_a \gamma^{-1}\pi(\delta_b) = \sum_{a+pb' = n} (-1)^{b'} \delta_a \delta_{pb'} = \sum_{a + pb' = n} (-1)^{b'} \binom{n}{a} \delta_{n}.\] Write \(n = ps + r\) with \(0 \le s,r < p\). Then pairs \((a,b')\) satisfying \(a+pb' = n\) are of the form \((r+ip, s-i)\) for \(0 \le i \le s\). Hence \[\eta(\delta_n) = \sum_{i=0}^s (-1)^{s-i} \binom{r+ps}{r+pi} \delta_n = \sum_{i=0}^s (-1)^{s-i} \binom{s}{i} \delta_n,\] the last equality being another application of Lucas’ theorem. This sum equals \(0\) if \(s > 0\), and equals \(\delta_n\) if \(s = 0\). In other words, we have \[\eta(\delta_n) = \begin{cases} \delta_n,& 0\le n<p,\\ 0,& p\le n<p^2, \end{cases}\] so the claim follows.

(7) Similar to (6). ◻

Recall the definitions of \(\overline{\sigma}, \overline{\tau}\) and \(\sigma, \tau\) given in (15 ), (16 ) and (39 ), (40 ).

Lemma 9. The cocycle \(\sigma\) is trivial and the cococycle \(\tau\) satisfies \(\tau(\delta_0) = 1 \otimes 1\), \[\tau(\delta_1) = \sum_{j=1}^{p-1} \frac{\lambda^p}{j! (p-j)!} t^j \otimes t^{p-j},\] and \(\tau(\delta_n) = 0\) for \(2 \le n < p\).

Proof. By the definition of \(\overline{\sigma}\), \(\overline{\sigma}(\delta_m,\delta_n)\) is an integer multiple of \(\delta_{p(m+n)}\). Since the image of \(\overline{\sigma}\) is in \(\mathbf{k}[\mathbb{G}_{a,1}]\), it is nonzero only when \(m = n = 0\), so \(\overline{\sigma} = \varepsilon \otimes \varepsilon\).

Next we compute \(\overline{\tau}\). Since \(\eta\) and \(\eta^{-1}\) annihilate \(\delta_j\) for \(j\ge p\), any nonzero contribution to \(\overline{\tau}(\delta_n)\) must come from summands in \(\Delta^{(2)}(\gamma(\delta_n))=\Delta^{(2)}(\delta_{pn}) =\sum_{a+b+c=pn}\delta_a\otimes\delta_b\otimes\delta_c\) with \(a,b,c<p\). Expanding the definition of \(\overline{\tau}\) we get \[\overline{\tau}(\delta_n)=\sum_{\substack{a+b+c=pn\\ a,b,c<p}} (-1)^a\sum_{r+s=a}\binom{r+b}{b}\binom{s+c}{c} \delta_{r+b}\otimes\delta_{s+c}\in \mathscr{O}(\mathbb{G}_{a,1})^{\otimes 2}.\] Since \((r+b) + (s+c) = pn\), every term has total degree \(pn\). Since the total degree of a simple tensor \(\delta_u \otimes \delta_v\) in \(\mathscr{O}(\mathbb{G}_{a,1})^{\otimes 2}\) is at most \(2(p-1)\), \(\overline{\tau}(\delta_n) = 0\) for \(n \ge 2\).

Since \(\delta_0\) is the unit in \(\mathbf{k}[\mathbb{G}_{a,1}]\), we have \(\gamma(\delta_0)=\delta_0\) and \(\eta(\delta_0)=\eta^{-1}(\delta_0)=\delta_0\), so \(\overline{\tau}(\delta_0)=\delta_0\otimes\delta_0\). All that is left to compute is the case when \(n=1\). We have \[\overline{\tau}(\delta_1)=\sum_{\substack{a+b+c=p\\ a,b,c<p}} (-1)^a\sum_{r+s=a}\binom{r+b}{b}\binom{s+c}{c} \delta_{r+b}\otimes\delta_{s+c}.\] Let us extract the coefficient \(\kappa_j\) of \(\delta_j\otimes\delta_{p-j}\). Since \(a=p-b-c\) and \(a < p\), we have \(b+c > 0\). Setting \(r+b=j\) and \(s+c=p-j\) gives \[\kappa_j =\sum_{\substack{0\le b,c<p\\ 0 < b+c\le p}} (-1)^{p-b-c}\binom{j}{b}\binom{p-j}{c}.\] If \(1 \le j \le p-1\), then grouping by \(m=b+c\) yields \[\kappa_j = \sum_{m=1}^{p}(-1)^{p-m}\sum_{b=0}^m\binom{j}{b}\binom{p-j}{m-b} = \sum_{m=1}^{p}(-1)^{p-m}\binom{p}{m} = 1,\] where we have used Vandermonde’s identity in the second equality. If \(j = 0\) or \(j = p\), then we cannot have \(m = p\) when grouping by \(m = b+c\). Thus, in this case \[\kappa_j = \sum_{m=1}^{p-1} (-1)^{p-m}\binom{p}{m} = 0.\] Hence, \(\overline{\tau}(\delta_1)=\sum_{j=1}^{p-1}\delta_j\otimes\delta_{p-j}\), so by (53 ), we get the result. ◻

Finally, it follows from Corollary 3 in a straightforward manner that \[\label{rz2} R_{\lambda}:=\sum_{i=0}^{p-1}\frac{\lambda^i}{i!}(t^i\#1)\otimes(t^i\#1)\tag{55}\] is an \(R\)-matrix for \(D(\mathbb{G}_{a,1},\mathbb{G}_{a,1},B_{\lambda})= \mathbf{k}[\mathbb{G}_{a,1}^{\vee}]\#^{\tau} \mathbf{k}[\mathbb{G}_{a,2}/\mathbb{G}_{a,1}]=\mathbf{k}[\widetilde{\mathbb{G}_{a,1}}]\) for each \(\lambda\in\mathbf{k}\).

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