Braided $T$-categories introduced by Turaev [1] are of interest due to their applications in homotopy quantum field theories, which are generalizations of ordinary topological quantum field theories. Braided crossed categories based on a group $G$, is braided monoidal categories in Freyd-Yetter categories of crossed $G$-sets (see [2]) play a key role in the construction of these homotopy invariants. In [3], Zhou and Yang studied cotriangular weak Hopf group-coalgebras and promoted Kegel theorem on the weak Hopf group-coalgebras. Motivated by this fact, the author Yang [4] introduced the notion of a monoidal Hom-group-coalgebra as a development of the notion of monoidal Hom-coalgebras in sense of Caenepeel and Goyvaerts (see [5]), and as a natural generalization of the notions of both the Hom-type Hopf algebras and the Hopf group-coalgebra in [1, 6], and constructed a new kind of braided T-categories.
Starting from a finite-dimensional Hopf algebra $H$, Drinfeld [7] showed how to obtain a quasitriangular Hopf algebra $D(H)$, the quantum double of $H$. It is now very natural to ask how to construct Drinfeld quantum double for finite-type monoidal Hom-Hopf group-coalgebras. In this article, we essentially construct Drinfeld quantum double over monoidal Hom-Hopf group-coalgebras.
This article is organized as follows. In Section 1, we recall some notions and results about monoidal Hom-Hopf group-coalgebras. In Section 2, we construct the Drinfeld quantum double over monoidal Hom-Hopf group-coalgebras and study quasitriangular monoidal Hom-Hopf group-coalgebras.
In this section, we recall the definitions and properties of monoidal Hom-Hopf algebras and monoidal Hom-Hopf group-coalgebras. Throughout this paper, we always let $G$ be a discrete group with a neutral element $1$ and $k$ a field. If $U$ and $V$ are $k$-spaces, $T_{U, V}: U\otimes V\rightarrow V\otimes U$ will denote the flip map defined by $T_{U, V}(u\otimes v)=v\otimes u$ for all $u\in U$ and $v\in V$.
Definition 2.1 (see [4]) A monoidal Hom-$G$-coalgebra is a family of $k$-spaces $C=\{(C_{\alpha }, \xi_{C_{\alpha }})\}_{\alpha \in G}$ together with a family of $k$-linear maps $\Delta=\{ \Delta_{\alpha , \beta}: C_{\alpha \beta}\rightarrow C_{\alpha } \otimes C_{\beta}\}_{\alpha , \beta\in G}$ and a $k$-linear map $\varepsilon: C_1\rightarrow k$, such that $\Delta$ is coassociative in the sense that
Remark 2.2 $(C_1, \xi_{C_{1}}, \Delta_{1, 1}, \varepsilon)$ is a monoidal Hom-coaglegbra in the sense of Caenepeel and Goyvaerts [5].
Following the Sweedler's notation for $G$-coalgebras, for any $\alpha , \beta \in G$ and $c\in (C_{\alpha \beta }, \xi_{C_{\alpha \beta }})$ one writes
The coassociativity axiom (2.1) gives that, for any $\alpha , \beta , \gamma \in G$ and $c\in (C_{\alpha \beta \gamma }, \xi_{C_{\alpha \beta \gamma }}), $
Definition 2.3 (see [4]) A monoidal Hom-Hopf $G$-coaglebra is a monoidal Hom-$G$-coalgebra $H=(\{H_{\alpha }, \xi_{H_{\alpha }}\}, \Delta, \varepsilon)$ together with a family of $k$-linear maps $S=\{S_\alpha :H_\alpha \rightarrow H_{\alpha ^{-1}}\}_{\alpha \in G}$ such that the following data holds:
Note that $(H_1, m_1, 1_1, \Delta_{1, 1}, \varepsilon, S_1)$ is a monoidal Hom-Hopf algebra. A monoidal Hom-Hopf $G$-coalgebra $H$ is termed to be of finite type if, for all $\alpha \in G$, $H_{\alpha }$ is finite-dimensional as $k$-vector space.
Remark 2.4 Let $H=(\{H_{\alpha }, \xi_{H_{\alpha }}\}, \Delta, \varepsilon, S)$ be a monoidal Hom-Hopf $G$-coalgebra. Suppose that the antipode $S=\{S_\alpha \}_{\alpha \in G}$ of $H$ is bijective. For any $\alpha \in G$, let $H_{\alpha }^{op}$ be the opposite algebra to $H_\alpha .$ Then $H^{op}=\{H_\alpha ^{op}\}_{\alpha \in G}$, endowed with the comultiplication and the counit of $H$ and with the antipode $S^{op}=\{S_\alpha ^{op}=S_{\alpha ^{-1}}^{-1}\}_{\alpha \in G}, $ is an opposite monoidal Hom-Hopf $G$-coalgebra of $H.$ The coopposite monoidal Hom-$G$-coalgebra equipped with $H_\alpha ^{cop}=H_{\alpha ^{-1}}$ as an algebra and with the comultiplication $\Delta_{\alpha , \beta }=T_{C_{\beta{-1}}, C_{\alpha ^{-1}}}\Delta_{\beta^{-1}, \alpha ^{-1}}$ and with the antipode $S^{cop}=\{S_{\alpha }^{cop}=S_{\alpha }^{-1}\}_{\alpha \in G}.$
Definition 2.5 (see [4]) A monoidal Hom-$G$-coalgebra $H=(\{H_{\alpha }, \xi_{H_{\alpha }}\}, \Delta, \varepsilon, S)$ is said to be a monoidal Hom-$T$-coalgebra provided it is endowed with a family of algebra isomorphisms $\varphi=\{\varphi_{\beta }:H_{\alpha }\rightarrow H_{\beta\alpha \beta ^{-1}}\}_{\alpha , \beta \in G}$ such that each $\varphi_\beta $ preserves the comultiplication and the counit, i.e., for all $\alpha , \beta , \gamma \in G, $
and $\varphi$ is multiplicative in the sense that $\varphi_{\alpha \beta }=\varphi_\alpha \circ\varphi_\beta , $ for all $\alpha , \beta \in G.$
Let $H$ be a monoidal Hom-$T$-coalgebra. Then one has that $\varphi_1|H_{\alpha }=id_{H_\alpha }, $ $\varphi_{\alpha }^{-1}=\varphi_{\alpha ^{-1}}, $ for all $\alpha \in G$ and $\varphi$ preserves the antipode, i.e., $\varphi_{\beta}\circ S_{\alpha } =S_{\beta\alpha \beta^{-1}}\circ\varphi_{\beta}$ for all $\alpha , \beta\in G.$
In order to construct the Drinfeld quantum double for monoidal Hom-Hopf $T$-coalgebras and study the definition of quasitriangular monoidal Hom-Hopf group-algebra. The following definitions are necessary.
Definition 3.1 The Duality $C^*$. Let $C=(\{C_{\alpha }, \xi_{C_\alpha }, \Delta, \varepsilon\})$ be a $G$-coalgebra and $A$ an algebra with multiplication $m$ and unit element $1_A.$ For any $f\in {\rm Hom}_{k}(C_\alpha , A)$ and $g\in {\rm Hom}_{k}(C_\beta , A), $ we have their convolution product by
for all $c\in C_{\alpha , \beta }.$ Equations (2.1) and (2.2) will imply that $k$-space
endowed with the convolution product $*$ and the unit element $1_{A}\varepsilon$, is a $G$-algebra, called a convolution algebra.
In particular, for $A=k$, the $G$-algebra $Conv(C, k)=\oplus_{\alpha \in G}C_{\alpha }^*$ is called dual to $C$ and is denoted by $C^*$.
Definition 3.2 The Mirror $\overline{H}$. Let $H$ be a monoidal Hom-$T$-coalgebra. Then the notion of the mirror $\overline{H}$ of $H$ is given by the following data.
$ \bullet $ For any $\alpha \in G, $ set $\overline{H}_\alpha =H_{\alpha ^{-1}}.$
$ \bullet $ For any $\alpha , \beta \in G, $ the $G$-coalgebra structure is defined by
for any $h\in \overline{H_{\alpha \beta }}=H_{\beta^{-1}\alpha ^{-1}}.$ The counit of $\overline{H}$ is given by $\varepsilon\in H_{1}^*=\overline{H}_{1}^*.$
$ \bullet $ For any $\alpha \in G, $ the $\alpha $th component of the antipode $\overline{S}$ of $\overline{H}$ is given by $\overline{S}_{\alpha }=\varphi_\alpha \circ S_{\alpha ^{-1}}.$
$ \bullet $ For any $\alpha \in G, $ the $\alpha $th component of the crossed map $\overline{\varphi}$ of $\overline{H}$ is given by $\overline{\varphi}_{\alpha }=\varphi_\alpha .$
Dually, a monoidal Hom-$G$-algebra is a family of $k$-spaces $A=\{(A_{\alpha }, \xi_{A_{\alpha }})\}_{\alpha \in G}$ together with a family of $k$-linear maps $m=\{m_{\alpha , \beta }: A_{\alpha }\otimes A_{\beta }\rightarrow A_{\alpha \beta }\}_{\alpha , \beta \in G}$ and a $k$-linear map $\eta: k\rightarrow A_1$, such that $m$ is associative in the sense that, for any $\alpha , \beta , \gamma \in G, $
and for all $\alpha , \beta \in G, $
A monoidal Hom-Hopf $G$-algebra is a $G$-algebra $H=(\{H_\alpha , \xi_{H_\alpha }\}, m, \eta)$ endowed with a family of $k$-linear maps $S=\{S_\alpha : H_\alpha \rightarrow H_{\alpha ^{-1}}\}_{\alpha \in G}$ such that each $(H_\alpha , \xi_{H_\alpha })$ is a monoidal Hom-coalgebra with a comultiplication $\Delta_\alpha $ and a counit $\varepsilon_\alpha $; the map $\eta: k\rightarrow A_1$ and the maps $m_{\alpha , \beta }:H_\alpha \otimes H_\beta \rightarrow H_{\alpha \beta }$ (for all $\alpha , \beta \in G$) are coalgebra homomorphisms; and for any $\alpha \in G, $ one has that
A monoidal Hom-Hopf $G$-algebra $H$ is said to be of finite type if, for all $\alpha \in G, H_\alpha $ is finite dimensional as $k$-space.
Furthermore, a monoidal Hom-Hopf $T$-algebra is a monoidal Hom-Hopf $G$-algebra $H$ with a set of coalgebra isomorphisms $\psi= \{\psi_{\beta}: H_{\alpha }\rightarrow H_{\beta\alpha \beta^{-1}}\}_{\alpha , \beta\in G}$ called a conjugation, satisfying the following conditions:
$ \bullet $ $\psi$ is multiplicative, i.e., $\psi_{\beta}\circ\psi_{\gamma }=\psi_{\beta\gamma }\, $ for any $\beta, \gamma \in G.$ It follows that, for any $\alpha \in G, $ $\psi_{1}|H_{\alpha }=id_{H_\alpha }.$
$ \bullet $ $\psi$ is compatible with $m$, i.e., for any $\alpha , \beta, \gamma \in G, $ we have $m_{\gamma \alpha \gamma ^{-1}, \gamma \beta \gamma ^{-1}}\circ(\psi_\gamma \otimes \psi_\gamma )=\psi_\gamma \circ m_{\alpha , \beta }.$
$ \bullet $ $\psi$ is compatible with $\eta$, i.e., $\eta\circ\psi_{\gamma }=\eta$ for any $\gamma \in G.$
Let $H$ be a monoidal Hom-Hopf $T$-algebra. Similar to that of [9] we have the construction $H_{pk}$ (called a packed form of $H$) which can form a Hom-Hopf algebra.
Remark 3.3 Let $H$ be a finite type monoidal Hom-Hopf $T$-algebra. The dual of $H$ is the monoidal Hom-Hopf $T$-algebra defined as follows. For any $\alpha \in G, $ the $\alpha $th component of $H^{*}$ is the dual coalgebra $(H_{\alpha }^{*}, \xi_{\alpha }^{*-1})$ of the algebra $(H_{\alpha }, \xi_{\alpha }).$ The multiplication of $H^{*}$ is given by
for any $f\in (H_{\alpha }^{*}, \xi_{\alpha }^{*-1}), g\in (H_{\beta}^{*}, \xi_{\beta}^{*-1})$ and $h\in (H_{\alpha \beta}, \xi_{\alpha \beta}), $ with $\alpha , \beta\in G.$ The unit of $H^{*}$ is given by $\varepsilon\in H_{1}^{*}\subset H^{*}.$ The antipode $ \mathscr{A}^{*}$ of $H^{*}$ is given by $ \mathscr{A}_{\alpha }^{*}=S_{\alpha ^{-1}}^{*}, $ for any $\alpha \in G.$ For any $\beta\in G, $ the conjugation isomorphism $\psi_{\beta}^{*}=\varphi_{\beta^{-1}}^{*}.$
Remark 3.4 Given any crossed monoidal Hom-Hopf $T$-coalgebra, then $((H^{*})_{pk})^{cop}$ is the monoidal Hom-Hopf algebra obtained from $(H^{*})_{pk}$ by replacing its comultiplication with the new one $\Delta^{*}=\Delta^{*t, cop}$ given by
for any $f\in H_{\alpha }^{*}\subset \oplus _{\beta\in G} H_{\beta}^{*}$ and $h, k\in H_{\alpha }, $ with $\alpha \in G.$ We also replace the antipode with the new one obtained by $\mathscr{A}_{*}=\mathscr{A}^{*t}=(S^*)^{-1}.$ In particular, we have $ < \mathscr{A}_{*}(f), h>= < f, S_{\alpha }^{-1}(h)>, $ for any $f \in H_{\alpha }^*$ and $h\in H_{\alpha ^{-1}}, $ with $\alpha \in G.$ We can obtain the crossed monoidal Hom-Hopf $T$-coalgebra denoted by $H^{*t, cop}$ based on $((H^{*})_{pk})^{cop}.$ Note that $\varphi_{H^{*t, cop}, \alpha }=\varphi_{H^{*t}, \alpha } =\sum\limits_{\beta\in G}\varphi_{\beta^{-1}}^{*}, $ for any $\alpha \in G.$
Let $H$ be a finite type monoidal Hom-Hopf $T$-coalgebra. We define the Drinfeld quantum double $D(T)$ of $H$ as follows. Consider the following vector spaces
for any $\alpha \in G.$ A multiplication is obtained by setting, for any $h, k\in H_{\alpha ^{-1}}, f\in H_{\gamma }^{*}, $ and $g\in H_{\delta}^*, $ with $\gamma , \delta\in G, $
For any $h, k\in H_{\alpha ^{-1}}$ and $f\in H_{\gamma }^{*}$
We now have the following main result of this section.
Theorem 3.5 Let $H$ be a finite-type monoidal Hom-Hopf $T$-coalgebra. Then $D(H)$ is a crossed monoidal Hom-Hopf $T$-coalgebra with the following structures:
$ \bullet $ For any $\alpha \in G, \, \alpha $th component $D_{\alpha }(H)$ is an associative algebra with the multiplication given in eq. (3.7) and with unit $ 1_{\alpha ^{-1}}\circledast \varepsilon;$
$ \bullet $ The comultiplication is given by
for any $\alpha , \beta \in G, h\in \bar{H}_{\alpha \beta }$ and $F\in H^{*t, cop}, $ where we have that $\Delta^{*}(F)=F_1\otimes F_2$ defined by eq. (3.6);
$ \bullet $ The counit is obtained by setting
for any $h\in H_{1}$ and $f\in H_{\gamma }^{*}, $ with $\gamma \in G;$
$ \bullet $ For any $\alpha \in G, $ the $\alpha $th component of the antipode of $D(H)$ is given by
for any $h\in\bar{ H}_{\alpha }$ and $F\in H^{*t, cop}, $ where $\mathscr{A}_{*}$ is the antipode of $H^{*t, cop}$ and $\bar{S}_{\alpha }=\varphi_{\alpha }\circ S_{\alpha ^{-1}}$ is the antipode of $\bar{H};$
$ \bullet $ For any $\alpha \in G, $ the conjugation isomorphism is given by
for any $h\in \bar{H}_{\alpha }$ and $f\in H_{\gamma }^{*t, cop}, $ with $\gamma \in G.$
Proof First, for any $\alpha \in G, $ we will show that $D_{\alpha }(H)$ is an Hom-associative algebra with unit. Then we will show that $\Delta$, defined as above, is multipilcative, i.e., that any $\Delta_{\alpha , \beta }$ is an algebra map. After that, we show that $\varepsilon$ is an algebra map. Finally, we will check axioms for the antipode and the conjugation isomorphisms are compatible with the multiplication.
Hom-associativity Let $\alpha $ be in $G$. The multiplication definition eq.(3.7) is associative if and only if, for any $h, k, l\in (H_{\alpha ^{-1}}, \xi_{\alpha ^{-1}}), f\in (H_{\beta }^{*}, \xi_{\beta }^{*-1}), q\in (H_{\delta}^{*}, \xi_{\delta}^{*-1}), $ and $ p\in (H_{\gamma }^{*}, \xi_{\gamma }^{*-1})$ with $\beta, \delta, \gamma \in G, $
By computing the left-hand side of (3.12), we obtain
by the antimultiplicativity of $S$ and the multiplicativity of $\varphi$
while, by computing the right-hand side, we obtain
by the antimultiplicativity of $S$ and the comultiplicativity of $\varphi$
Unit Let $\alpha $ be in $G$. For any $h\in H_{\alpha ^{-1}}$ and $f\in H_{\gamma }^{*}$, with $\gamma \in G$, we have
Remark 3.6 Where we use the fact that both $S_{1}$ and $\varphi_{\alpha }$ commute with $\varepsilon$.
Multiplicativity of $\Delta$ Let us prove that $\Delta_{\alpha , \beta }$ is an algebra map for any $\alpha , \beta \in G$. For any $h, k\in H_{\beta^{-1}\alpha ^{-1}}, f\in H_{\gamma }^{*}$ and $g\in H_{\delta }^*$, with $\gamma , \delta\in G, $ we have
This is proved by evaluating both terms in the above equation (3.13) against the general term $p\otimes x \otimes q\otimes y$ ($p\in H_{\alpha ^{-1}}^{*}, q\in H_{\beta^{-1}}^{*}, $ and $x, y\in H_{\gamma \delta }$).
Multiplicativity of $\varepsilon$ Let us prove that $\varepsilon$ is an algebra map for any $h, k\in H_{1}, f\in H_{\gamma }^{*}, $ and $g\in H_{\delta}^{*}, $ with $\gamma , \delta\in G$,
and
This proves that $\varepsilon$ is multiplicative. Moreover, since $\varepsilon$ is obviously unitary, it is an algebra homomorphism.
Antipode Let $h\in H_{1}$ and let $f\in H_{\gamma }^{*}, $ with $\gamma \in G$,
Conjugation Let us check that $\varphi_{\beta }$ is an algebra isomorphism for any $\alpha , \beta \in G.$ For all $h, k\in H_{\alpha }^{-1}, f\in H_{\gamma }^{*}, $ and $g\in H_{\delta}^{*}, $ with $\gamma , \delta\in G, $
for all $x\in H_{\beta\gamma \delta\beta ^{-1}}, p\in H_{\beta\alpha ^{-1}\beta^{-1}}^{*}$.
For any $\alpha \in G, $ we set $n_{\alpha }=\dim H_{\alpha }.$ Let $(\kappa_{(\alpha , i)})_{i=1, \cdots, n_{\alpha }}$ and $(\kappa^{(\alpha , i)})_{i=1, \cdots, n_{\alpha }}$ be dual bases in $H_{\alpha }$ and $H_{\alpha }^*.$ Then we have the following proposition.
Definition 3.7 A quasitriangular Hom-Hopf $T$-coalgebra is a Hom-Hopf $T$-coalgebra endowed with a family $R=\{R_{\alpha , \beta}=\kappa_{\alpha , i}\otimes \kappa_{\beta, i} \in H_{\alpha }\otimes H_{\beta}\}_{\alpha , \beta\in G}, $ called a universal $R$-matrix, such that $R_{\alpha , \beta}$ is invertible for any $\alpha , \beta\in G$ and the following conditions are satisfied:
for all $h\in H_{\alpha \beta}$ and $\alpha , \beta\in G, $
for all $\alpha , \beta, \gamma \in G.$
Remark 3.8 (1) We introduce the notation $\tilde{\kappa}_{\alpha , i}\otimes \tilde{\kappa}_{\beta, i} =\tilde{R}_{\alpha , \beta}=(R^{-1})_{\alpha , \beta}.$ (2) $R_{1, 1}$ is an $R$-matrix for the Hom-Hopf algebra $H_{1}$ (see [8]).
Proposition 3.9 The Drinfeld double $D(H)=\{D_{\alpha }(H)\}_{\alpha \in G}$ has a quasitriangular structure given by
Proof Relation (3.14):
Let $\alpha , \beta , \gamma \in G.$ Given $h\in H_{\beta^{-1}\alpha ^{-1}}$ and $f\in H_{\gamma }^{*}, $ we have
Relation (3.14) is proved by observing that evaluating the two expressions above against the tensor $i{{d}_{{{\alpha }^{-1}}}}\otimes id_{\gamma }^{*}\otimes i{{d}_{{{\beta }^{-1}}}}\otimes \left\langle \cdot ,x \right\rangle $ (for $x\in H_{\alpha ^{-1}\gamma }$) we get the same result
where we used
for all $f\in H_{\alpha ^{-1}}^{*}, h\in H_{\alpha ^{-1}}$ and $\alpha \in G.$
Then we check Relation (3.16) and (3.17). The identities
can be written as (identifying $\bar{H_{\alpha }}\otimes \varepsilon$ with $\bar{H_{\alpha }}$ and $1_{\beta^{-1}}\otimes H^*$ with $H^*$)
The above equalities can be verified by evaluating both sides on element $f\in H_{\alpha ^{-1}}^{*}$ in the first factor (respectively, on $h\in \overline{H}_{\alpha \beta }$ in the third factor) (see Zunino [9], Theorem 11).
Finally, let us check that
Now, $\xi_{\alpha ^{-1}}$ is a linear isomorphism, so $(\xi_{\alpha ^{-1}}(\kappa_{(\alpha ^{-1}, i)}))_{i=1, \cdots, n_{\alpha }}$ is a basis of $H_{\alpha ^{-1}}, $ and
is its dual basis. So $(\xi_{D_{\alpha }(H)}\otimes \xi_{D_{\beta }(H)})R_{\alpha , \beta } =R_{\alpha , \beta }.$
for $x\in H_{\alpha ^{-1}}.$
This completes the proof.