Hopf images and inner faithful representations

Teodor Banica, Julien Bichon

Introduction

The aim of this paper is to provide an axiomatization and systematic study of the concept of Hopf image of a Hopf algebra representation, as well as the related concept of inner faithful representation. These notions appeared, under various degrees of generality, in a number of independent investigations: vertex models and related quantum groups , , , locally compact quantum groups and their outer actions , . These were used extensively in the recent paper in order to study the quantum symmetries of Hadamard matrices and of the corresponding subfactors.

The leading idea is that we want to translate the notion of faithful representation of a discrete group at a Hopf algebra level. Let Γ\Gamma be a group, let AA be a kk-algebra (kk is a field) and consider a representation

There are two possible notions of faithfulness for π\pi:

faithfulness of π\pi as an algebra map, in which case we simply say that π\pi is faithful;

faithfulness of the induced group morphism π∣Γ:Γ⟶A×\pi_{|\Gamma}:\Gamma\longrightarrow A^{\times}.

It is clear that the first notion is much more restrictive than the second one, and choice of one of these notions as the good one for faithfulness depends on whether one is interested by the algebra k[Γ]k[\Gamma] or rather by the group Γ\Gamma itself.

It is not difficult so see that π∣Γ\pi_{|\Gamma} is faithful if and only if Ker(π)⊂k[Γ]{\rm Ker}(\pi)\subset k[\Gamma] does not contain any non-zero Hopf ideal. This simple observation leads to a notion of inner faithful representation for arbitrary Hopf algebras: if HH a Hopf algebra, we say that a representation

is inner faithful is Ker(π){\rm Ker}(\pi) does not contain any non-zero Hopf ideal. Of course HH is viewed as the group algebra of a discrete quantum group, and faithfulness refers to this discrete quantum group.

If the representation π\pi is not inner faithful, there is however a minimal Hopf algebra HπH_{\pi} that factorizes π\pi, that we call the Hopf image of π\pi (for H=k[π]H=k[\pi], we have k[Γ]π=k[π(Γ)]k[\Gamma]\pi=k[\pi(\Gamma)]). The exact universal property of the Hopf image is stated in Section 2. The Hopf image measures how much π\pi fails to be faithful in the discrete quantum group sense. In the situation of , the Hopf image of the representation of the quantum permutation algebra associated to a complex Hadamard matrix measures the complexity of the quantum invariants of the Hadamard matrix.

A natural concept arising from these considerations is the notion of inner linear Hopf algebra: we say that a Hopf algebra is inner linear if it admits a finite-dimensional inner faithful representation. Therefore the problem of inner linearity for Hopf algebras is a generalization of the celebrated linearity problem for discrete groups. More generally, we believe that the study of Hopf images leads to interesting new questions and problems in Hopf algebra theory, as well as in group theory through the study of group duals.

The paper is devoted to a general study of the notion of Hopf image, culminating in a Tannakian formulation, together with the study of several key examples.

Notations and conventions. We work in general over a fixed field kk. We assume that the reader has some familiarity with Hopf algebras, for which the textbooks or are convenient. Our terminology and notation are the standard ones: in particular, for a Hopf algebra, Δ\Delta, ε\varepsilon and SS denote the comultiplication, counit and antipode, respectively.

Ackowledgements. We wish to thank Rupert Yu for helpful discussions on algebraic groups.

Construction of the Hopf image and basic properties

In this section we give the precise formulation of the concept of Hopf image, prove its existence and study of some of its basic properties. The case of Hopf ∗*-algebras is also considered at the end of the section.

First, let us give a precise formulation of the notion of Hopf image of a representation. Let HH be a Hopf algebra over a field kk. As usual, a representation of HH on an algebra AA is an algebra morphism π:H⟶A\pi:H\longrightarrow A.

Let us say that a factorization of π\pi is a triple (L,q,φ)(L,q,\varphi) where LL is a Hopf algebra, q:H⟶Lq:H\longrightarrow L is a surjective Hopf algebra map and φ:L⟶A\varphi:L\longrightarrow A is a representation, with the decomposition π=φ∘q\pi=\varphi\circ q. We define in a straightforward manner the category of factorizations of π\pi, and the Hopf image of π\pi is defined to be the final object in this category (hence we can also say that this is a minimal factorization).

The above proof uses the Hopf ideal IπI_{\pi}, the largest Hopf ideal contained in Ker(π){\rm Ker}(\pi). This Hopf ideal is constucted in a very abstract manner, and it is useful for several purposes to have a more concrete description of IπI_{\pi}, that we give now.

To any element g∈Fg\in F, we associate an algebra AgA^{g}, defined inductively on the lenght of gg as follows. We put A1=kA^{1}=k, Aαk=AA^{\alpha_{k}}=A if kk is even and Aαk=AopA^{\alpha_{k}}=A^{\rm op} if kk is odd. Now for g,h∈Fg,h\in F with l(g)>1l(g)>1 and l(h)>1l(h)>1, we put Agh=Ag⊗AhA^{gh}=A^{g}\otimes A^{h}.

Now we associate an algebra morphism πg:H⟶Ag\pi^{g}:H\longrightarrow A^{g} to any g∈Fg\in F, again by induction on the length of gg. We put π1=ε\pi^{1}=\varepsilon, παk=π∘Sk\pi^{\alpha_{k}}=\pi\circ S^{k}, and for g,h∈Fg,h\in F with l(g)>1l(g)>1 and l(h)>1l(h)>1, we put πgh=(πg⊗πh)∘Δ\pi^{gh}=(\pi^{g}\otimes\pi^{h})\circ\Delta.

Let π:H⟶A\pi:H\longrightarrow A be a representation and let IπI_{\pi} be the largest Hopf ideal contained in Ker(π){\rm Ker}(\pi). We have

The proof of Proposition 2.2 uses several lemmas. We put Jπ=⋂g∈FKer(πg)⊂HJ_{\pi}=\bigcap_{g\in F}{\rm Ker}(\pi^{g})\subset H. By construction JπJ_{\pi} is an ideal in HH, and we wish to prove now that JπJ_{\pi} is a Hopf ideal. The following result ensures that it is a coideal.

Let CπC_{\pi} be the linear subspace in H∗H^{*} generated by the elements

Then CπC_{\pi} is a subalgebra of H∗H^{*}, and Jπ=Cπ⊥J_{\pi}=C_{\pi}^{\perp}. In particular JπJ_{\pi} is a coideal in HH.

For ψ,ϕ∈H∗\psi,\phi\in H^{*} and g,h∈Fg,h\in F, we have

and since ε∈Cπ\varepsilon\in C_{\pi}, we conclude that CπC_{\pi} is a subalgebra of H∗H^{*}. It is clear that Cπ⊥=IπC_{\pi}^{\perp}=I_{\pi}, and we conclude that JπJ_{\pi} is a coideal by Proposition 1.4.6 in . ∎

For all g∈Fg\in F, there exists a linear isomorphism Rg:Aτ(g)⟶AgR_{g}:A^{\tau(g)}\longrightarrow A^{g} such that πg∘S=Rg∘πτ(g)\pi^{g}\circ S=R_{g}\circ\pi^{\tau(g)}. In particular S(Jπ)⊂JπS(J_{\pi})\subset J_{\pi}, and JπJ_{\pi} is a Hopf ideal in HH.

We prove the result by induction on l(g)l(g). For l(g)=0l(g)=0 or l(g)=1l(g)=1, this follows immediately from the definitions. So assume that l(g)>1l(g)>1, so that g=hh′g=hh^{\prime}, with l(g)>l(h)≥1l(g)>l(h)\geq 1 and l(g)>l(h′)≥1l(g)>l(h^{\prime})\geq 1. For xx in HH, we have

The following lemma finishes the proof of Proposition 2.2.

Let π:H⟶A\pi:H\longrightarrow A be an algebra map, let q:H⟶Lq:H\longrightarrow L be a Hopf algebra map, and let φ:L⟶A\varphi:L\longrightarrow A be an algebra map with π=φ∘q\pi=\varphi\circ q. Then Ker(q)⊂Jπ{\rm Ker}(q)\subset J_{\pi}, and hence any Hopf ideal contained in Ker(π){\rm Ker}(\pi) is contained in JπJ_{\pi}.

with the same notation for φ\varphi as the one for π\pi. We show this by induction on l(g)l(g). This is true if l(g)=0l(g)=0 since qq is a coalgebra map and if l(g)=1l(g)=1, we have παk=π∘Sk=φ∘q∘Sk=φ∘Sk∘q=φαk∘q\pi^{\alpha_{k}}=\pi\circ S^{k}=\varphi\circ q\circ S^{k}=\varphi\circ S^{k}\circ q=\varphi^{\alpha_{k}}\circ q. Assume now that l(g)>1l(g)>1, so that g=hh′g=hh^{\prime} with l(g)>l(h)≥1l(g)>l(h)\geq 1 and l(g)>l(h′)≥1l(g)>l(h^{\prime})\geq 1, and that the result is proved for elements of lenght <l(g)<l(g). Then

and this proves our assertion by induction. Hence we have Ker(q)⊂Jπ{\rm Ker}(q)\subset J_{\pi}. Any Hopf ideal is the kernel of a Hopf algebra map, and hence the last assertion follows. ∎

The notion of Hopf image considered here is in general different from the one given in , Definition 1.2.0, which refers to the category of Hopf algebras. Our definition of Hopf image uses the largest category of algebras.

2. Inner faithful representations

The following definition was already given in the introduction.

Let π:H⟶A\pi:H\longrightarrow A be a representation of a Hopf algebra HH on an algebra AA. We say that π\pi is inner faithful if Ker(π){\rm Ker}(\pi) does not contain any non-zero Hopf ideal.

We have several equivalent formulations for inner faithfulness.

Let π:H⟶A\pi:H\longrightarrow A be a representation of a Hopf algebra HH on an algebra AA. The following assertions are equivalent.

The Hopf algebra morphism p:H⟶Hπp:H\longrightarrow H_{\pi} in Theorem 2.1 is an isomorphism.

If (L,q,φ)(L,q,\varphi) is any factorization of π\pi, then qq is an isomorphism.

The equivalence between these assertions follows from the previous considerations and Proposition 2.2. Under a special assumption, we also have another equivalent criterion for inner faithfulness.

Let π:H⟶A\pi:H\longrightarrow A be a representation of a Hopf algebra HH on an algebra AA such that Ker(π){\rm Ker}(\pi) is SS-stable: S(Ker(π))⊂Ker(π)S({\rm Ker}(\pi))\subset{\rm Ker}(\pi). Then π\pi is inner faithful if and only if (0)(0) is the only bi-ideal contained in Ker(π){\rm Ker}(\pi).

We also have a characterization of the Hopf image using inner faithfulness, which can be useful in some contexts (for example see the proof of Proposition 3.3).

When considering Hopf algebra maps, Hopf images are usual images and inner faithfulness is equivalent to faithfulness.

Let HH and AA be Hopf algebras and π:H⟶A\pi:H\longrightarrow A be a Hopf algebra map. Then the Hopf image of π\pi is π(H)\pi(H), and π\pi is inner faithful if and only if it is faithful.

The first assertion is immediate, as well as the second one, since Ker(π){\rm Ker}(\pi) is a Hopf ideal. The following result is also immediate using the universal property of the Hopf image.

Let π:H⟶A\pi:H\longrightarrow A be a representation of a Hopf algebra HH on an algebra AA and let θ:A⟶B\theta:A\longrightarrow B be an algebra isomorphism. Then we have a Hopf algebra isomorphism Hθ∘π≃HπH_{\theta\circ\pi}\simeq H_{\pi}. In particular θ∘π\theta\circ\pi is inner faithful if and only if π\pi is inner faithful.

Of course one cannot expect that an inner faithful representation H⟶AH\longrightarrow A will transmit all the algebra properties of the algebra AA to the algebra HH. This is true however for commutativity.

Let π:H⟶A\pi:H\longrightarrow A be a representation of a Hopf algebra HH on a commutative algebra AA. Then the Hopf image HπH_{\pi} is a commutative algebra, and hence if π\pi is inner faithful, then HH is also commutative.

Since AA is commutative, the ideal of HH generated by the commutators of elements of HH is contained in Ker(π){\rm Ker}(\pi). But the commutator ideal is also a Hopf ideal, so is contained in IπI_{\pi}, and hence HπH_{\pi} is commutative. ∎

3. Hopf ∗*-algebras.

Let us begin by recalling the appropriate language. First, a Hopf ∗*-algebra is a Hopf algebra HH which is a ∗*-algebra and such that the comultiplication Δ:H⟶H⊗H\Delta:H\longrightarrow H\otimes H is a ∗*-algebra map. It follows that the counit is a ∗*-morphism and that the antipode is bijective, and its inverse satisfies S−1(x)=S(x∗)∗S^{-1}(x)=S(x^{*})^{*}. A ∗*-representation of HH on a ∗*-algebra is a ∗*-algebra map H⟶AH\longrightarrow A.

The formulation of the problem of the existence of a Hopf ∗*-image is the same as in the introduction, adding “∗*” where needed. In this framework, Theorem 2.1 has the following form.

The details are left to the reader (to show that ⋂g∈F+Ker(πg)\bigcap_{g\in F^{+}}{\rm Ker}(\pi^{g}) is ∗*-stable, one uses the formula S∘∗=∗∘S−1)S\circ*=*\circ S^{-1}). ∎

We have used the same notation HπH_{\pi} for the Hopf ∗*-image of a ∗*-representation π:H⟶A\pi:H\longrightarrow A and its Hopf image. In general it seems possible that two notions might not coincide, although we do not have an explicit example. This should cause no confusion: unless specifically notified, when we have such a ∗*-representation, the notation HπH_{\pi} will always denote the Hopf ∗*-image.

We will say that a ∗*-representation π:H⟶A\pi:H\longrightarrow A of a Hopf ∗*-algebra HH on an ∗*-algebra AA is inner faithful if Ker(π){\rm Ker}(\pi) does not contain any non zero Hopf ∗*-ideal (similarly to Proposition 2.8 there are several equivalent characterizations). Again it seems to be possible that such a ∗*-representation be inner faithful as a ∗*-representation, but not as a representation. However the two notions coincide when S2=idHS^{2}={\rm id}_{H} (or more generally if some power of S2S^{2} is an inner automorphism).

The proof of Theorem 2.14 also shows that Hopf images exist in the category of Hopf algebras having a bijective antipode (more precisely, the Hopf ideal Iπ+I^{+}_{\pi} is the largest Hopf ideal with S(Iπ+)=Iπ+S(I_{\pi}^{+})=I_{\pi}^{+} contained in Ker(π){\rm Ker}(\pi)), and the Hopf image in this category coincides with the Hopf ∗*-image. Note that the construction of Theorem 2.1 does not give the Hopf image in the category of Hopf algebras with bijective antipode, since there exist quotients of Hopf algebras with bijective antipode that do not have a bijective antipode: see e.g. .

We now turn to compact Hopf algebras: these are the Hopf ∗*-algebras having all their finite-dimensional comodules equivalent to unitary ones (see , these are called CQG algebras there), and are the algebras of representative functions on compact quantum groups.

Let π:H⟶A\pi:H\longrightarrow A be a ∗*-representation of a compact Hopf algebra HH on a ∗*-algebra AA. Then the Hopf ∗*-image HπH_{\pi} is a compact Hopf algebra, and hence Hopf ∗*-images exist in the category of compact Hopf algebras.

It is clear from Theorem 27, Section 11.3 in , that a quotient of a compact Hopf algebra is again a compact Hopf algebra. Thus since we have a surjective Hopf ∗*-algebra map H⟶HπH\longrightarrow H_{\pi}, we conclude that HπH_{\pi} is a compact Hopf algebra. ∎

Classical examples: group algebras and Lie algebras

In this section we get back to the motivating examples for the notion of inner faithfulness: group algebras and universal enveloping algebras of Lie algebras.

The following result is announced in the introduction. Its origin goes back to Proposition 2.2 in .

Let Γ\Gamma be group, let AA be an algebra and let π:k[Γ]⟶A\pi:k[\Gamma]\longrightarrow A be an algebra map. Then we have

In particular π\pi is inner faithful if and only if the group morphism π∣Γ:Γ⟶A×\pi_{|\Gamma}:\Gamma\longrightarrow A^{\times} is injective (faithful).

Let (L,q,φ)(L,q,\varphi) be a factorization of π\pi. Then LL is the group algebra k[q(Γ)]k[q(\Gamma)], and we have a group factorization

Hence we have q(Γ)⊂π(Γ)q(\Gamma)\subset\pi(\Gamma), and this induces the appropriate Hopf algebra map k[q(Γ)]=L⟶k[π(Γ)]k[q(\Gamma)]=L\longrightarrow k[\pi(\Gamma)]. ∎

The above result motivates the following definition.

A Hopf algebra HH is said to be inner linear if there exists an inner faithful representation π:H⟶A\pi:H\longrightarrow A into a finite-dimensional algebra AA.

Indeed the group algebra k[Γ]k[\Gamma] is inner linear if and only the group Γ\Gamma is linear (over kk). It is clear that a Hopf algebra is inner linear if and only if it contains an ideal of finite codimension that does not contain non-zero Hopf ideals.

2. Lie algebras

Let g\mathfrak{g} be a Lie algebra, and let U(g)U(\mathfrak{g}) be its universal enveloping algebra. Algebra maps U(g)⟶AU(\mathfrak{g})\longrightarrow A correspond exactly to Lie algebra maps g⟶gl(A)\mathfrak{g}\longrightarrow\mathfrak{gl}(A), where gl(A)\mathfrak{gl}(A) is the Lie algebra associated to AA: as a vector space gl(A)=A\mathfrak{gl}(A)=A and the Lie bracket is defined by [a,b]=ab−ba[a,b]=ab-ba, ∀a,b∈A\forall a,b\in A. The Hopf image is described as follows in characteristic zero.

Let g\mathfrak{g} be a Lie algebra over a characteristic zero field, let AA be an algebra and let π:U(g)⟶A\pi:U(\mathfrak{g})\longrightarrow A be an algebra map. Then we have

In particular π\pi is inner faithful if and only if the Lie algebra map π∣g:g⟶gl(A)\pi_{|\mathfrak{g}}:\mathfrak{g}\longrightarrow\mathfrak{gl}(A) is injective (faithful). Thus the Hopf algebra U(g)U(\mathfrak{g}) is inner linear if and only if g\mathfrak{g} is finite-dimensional.

Let us first show if π∣g:g⟶gl(A)\pi_{|\mathfrak{g}}:\mathfrak{g}\longrightarrow\mathfrak{gl}(A) is injective, then π:U(g)⟶A\pi:U(\mathfrak{g})\longrightarrow A is inner faithful. The space of primitive elements P(U(g))\mathcal{P}(U(\mathfrak{g})) equals g\mathfrak{g} by the characteristic zero assumption and 11 is the only group-like in U(g)U(\mathfrak{g}) (see e.g. Proposition 5.5.3 in ). Thus the canonical map p:U(g)⟶U(g)πp:U(\mathfrak{g})\longrightarrow U(\mathfrak{g})_{\pi} is injective on primitive elements, and since the Hopf algebra U(g)U(\mathfrak{g}) is pointed, we use Corollary 5.4.7 in to conclude that pp is injective, and hence π\pi is inner faithful.

In general we have a Hopf algebra factorization

The algebra map on the right is inner faithful by the previous discussion, and hence by Proposition 2.9 we have the announced isomorphism U(g)π≃U(π(g))≃U(g/Ker(π∣g))U(\mathfrak{g})_{\pi}\simeq U(\pi(\mathfrak{g}))\simeq U(\mathfrak{g}/{\rm Ker}(\pi_{|\mathfrak{g}})). Finally if π\pi is inner faithful, it induces an isomorphism U(g)≃U(π(g))U(\mathfrak{g})\simeq U(\pi(\mathfrak{g})), which induces an isomorphism between the Lie algebras of primitive elements, and hence between g\mathfrak{g} and π(g)\pi(\mathfrak{g}): π∣g\pi_{|\mathfrak{g}} is injective.

If U(g)U(\mathfrak{g}) is inner linear, then g\mathfrak{g} is finite-dimensional by the previous discussion. The converse follows from Ado’s Theorem: a finite dimensional Lie algebra g\mathfrak{g} has a faithful finite-dimensional representation g⟶gln(k)\mathfrak{g}\longrightarrow\mathfrak{gl}_{n}(k) for some nn. ∎

In fact the main argument we have used for the proof this proposition, Corollary 5.4.7 in , a result due independently to Takeuchi and Radford, is valid for arbitrary pointed Hopf algebras. We use it in a similar manner in the next section to get an inner faithfulness criterion for representations of arbitrary pointed Hopf algebras.

Pointed Hopf algebras

After the motivating examples of group algebras and enveloping algebras of Lie algebras, the next natural step is the study of pointed Hopf algebras. These have been much studied in recent years (see e.g. for quantized enveloping algebras of Lie algebras and for the finite-dimensional case). In this section we study the inner faithfulness of a representation of a pointed Hopf algebra. The criterion that we give unifies those given in the previous section.

Recall that a Hopf algebra HH is said to be pointed if all its simple comodules are one-dimensional, hence corresponding to group-like elements. The group of group-like elements of HH is denoted by Gr(H)(H). An element x∈Hx\in H is said to be (g,h)(g,h)-primitive for g,h∈Gr(H)g,h\in{\rm Gr}(H) if

The space of (g,h)(g,h)-primitive elements is denoted Pg,h(H)\mathcal{P}_{g,h}(H).

Let π:H⟶A\pi:H\longrightarrow A be a representation of a pointed Hopf algebra HH on an algebra AA. The following assertions are equivalent.

∀g∈Gr(H)\forall g\in{\rm Gr}(H), the restriction π∣Pg,1(H):Pg,1(H)⟶A\pi_{|\mathcal{P}_{g,1}(H)}:\mathcal{P}_{g,1}(H)\longrightarrow A is injective.

∀g∈Gr(H)\forall g\in{\rm Gr}(H), the restriction π∣P1,g(H):P1,g(H)⟶A\pi_{|\mathcal{P}_{1,g}(H)}:\mathcal{P}_{1,g}(H)\longrightarrow A is injective.

We begin by showing that π\pi is inner faithful if and only if for all g,h∈Gr(H)g,h\in{\rm Gr}(H), the restriction π∣Pg,h(H):Pg,h(H)⟶A\pi_{|\mathcal{P}_{g,h}(H)}:\mathcal{P}_{g,h}(H)\longrightarrow A is injective. Assume that π\pi is inner faithful. Let x∈Pg,h(H)x\in\mathcal{P}_{g,h}(H) be such that π(x)=0\pi(x)=0 and let II be the ideal of HH generated by xx. It is clear from the identities

that II is a Hopf ideal, and since II is contained in Ker(π){\rm Ker}(\pi), we get I=0I=0 and x=0x=0.

Conversely, assume that π\pi is injective on each space of primitives. Then so is p:H⟶Hπp:H\longrightarrow H_{\pi}, and hence by Corollary 5.4.7 in , we conclude that pp is an isomorphism and that π\pi is inner faithful.

For x∈Pg,h(H)x\in\mathcal{P}_{g,h}(H), we have g−1x∈P1,g−1h(H)g^{-1}x\in\mathcal{P}_{1,g^{-1}h}(H) and h−1x∈Ph−1g,1(H)h^{-1}x\in\mathcal{P}_{h^{-1}g,1}(H). Hence if (2) or (3) holds, then π\pi is injective when restricted to each space of primitives, and the previous discussion shows that π\pi is inner faithful. ∎

It is a direct computation to check that the conditions of Theorem 4.1 are fulfilled, and hence π\pi is inner faithful. If qq is a root of unity, then π\pi is not injective on the group-like elements and hence is not inner faithful. ∎

Function algebras

In this section we study Hopf images for various function algebras: polynomial functions on algebraic groups and representative functions on compact groups. The idea for the computation of the Hopf image goes back to , but we are a little bit more general here. These simple examples are already interesting for testing the possibility of generalizing representation theoretic properties of discrete group algebras to arbitrary Hopf algebras.

Let GG be a linear algebraic group over an algebraically closed field of characteristic zero and let π:O(G)⟶A\pi:\mathcal{O}(G)\longrightarrow A be a representation on an algebra AA. Assume that the algebra π(A)\pi(A) is reduced, so that π(A)≃O(X)\pi(A)\simeq\mathcal{O}(X) for an affine algebraic set XX and that the algebra map O(G)⟶π(A)≃O(X)\mathcal{O}(G)\longrightarrow\pi(A)\simeq\mathcal{O}(X) is induced by a polynomial map ν:X⟶G\nu:X\longrightarrow G. Then O(G)π≃O(⟨ν(X)⟩‾)\mathcal{O}(G)_{\pi}\simeq\mathcal{O}(\overline{\langle\nu(X)\rangle}), where ⟨ν(X)⟩‾\overline{\langle\nu(X)\rangle} is the Zariski closure in GG of the subgroup generated by ν(X)\nu(X).

By the assumption and Proposition 2.12 we may assume that π:O(G)⟶O(X)\pi:\mathcal{O}(G)\longrightarrow\mathcal{O}(X) is induced by an injective polynomial map ν:X⟶G\nu:X\longrightarrow G. The injections X→⟨ν(X)⟩‾⊂GX\rightarrow\overline{\langle\nu(X)\rangle}\subset G yield a factorization of π\pi. Now let (L,q,φ)(L,q,\varphi) be a factorization of π\pi. Then LL is finitely generated and is reduced by Cartier’s theorem (kk has characteristic zero), hence we can assume that L=O(H)L=\mathcal{O}(H) for a linear algebraic group HH, and that qq and ρ\rho are induced by polynomial maps X→H⊂GX\rightarrow H\subset G whose composition is ν\nu. Hence ⟨ν(X)⟩‾⊂H\overline{\langle\nu(X)\rangle}\subset H, and this gives the required Hopf algebra map O(H)⟶O(⟨ν(X)⟩‾)\mathcal{O}(H)\longrightarrow\mathcal{O}(\overline{\langle\nu(X)\rangle}). ∎

Let GG be a linear algebraic group over an algebraically closed field of characteristic zero and let g1,…,gn∈Gg_{1},\ldots,g_{n}\in G. The algebra map

has O(⟨g1,…,gn⟩‾)\mathcal{O}(\overline{\langle g_{1},\ldots,g_{n}\rangle}) as Hopf image and is inner faithful if and only if G=⟨g1,…,gn⟩‾G=\overline{\langle g_{1},\ldots,g_{n}\rangle}.

The compact group case is worked out similarly. Let GG be a compact group. The Hopf ∗*-algebra of representative functions on GG is denoted by R(G)\mathcal{R}(G): this a dense ∗*-subalgebra of C(G)(G) by the Peter-Weyl theorem, and moreover C(G)(G) is the enveloping C∗{\rm C}^{*}-algebra of R(G)\mathcal{R}(G).

Let GG be a compact group and let π:R(G)⟶A\pi:\mathcal{R}(G)\longrightarrow A be a ∗*-representation on a C∗{\rm C^{*}}-algebra AA. Extend π\pi to a ∗*-algebra map π+:C(G)⟶A\pi^{+}:C(G)\longrightarrow A, and let XX be the spectrum of π+(C(G))\pi^{+}(C(G)), so that π+(C(G))≃C(X)\pi^{+}(C(G))\simeq C(X) and that the induced C∗{\rm C^{*}}-algebra map C(G)⟶π+(C(G))≃C(X)C(G)\longrightarrow\pi^{+}(C(G))\simeq C(X) comes from a continuous map ν:X⟶G\nu:X\longrightarrow G. Then R(G)π≃R(⟨ν(X)⟩‾)\mathcal{R}(G)_{\pi}\simeq\mathcal{R}(\overline{\langle\nu(X)\rangle}), where ⟨ν(X)⟩‾\overline{\langle\nu(X)\rangle} is the closure in GG of the subgroup generated by ν(X)\nu(X).

The proof is essentially the same as the one of the previous proposition, because a quotient of a compact Hopf algebra is itself compact, and by the Hopf algebra version of the Tannaka-Krein theorem, a commutative compact Hopf algebra is the algebra of representative functions on a unique compact group. ∎

We end the section by showing that the simple example of function algebras shows that it is not possible to deduce inner faithfulness of a representation of a cosemisimple Hopf algebra by only studying its restriction to characters.

Let us assume that kk is algebraically closed. Recall that a cosemisimple Hopf algebra is a Hopf algebra HH whose category of comodules is semisimple. This is equivalent to say that HH has a Peter-Weyl decomposition

where Λ\Lambda is the set of simple HH-comodules and for λ∈Λ\lambda\in\Lambda, HλH_{\lambda} is the comatrix coalgebra of corresponding coefficients. Let dλd_{\lambda} be the dimension of the simple HH-comodule corresponding to λ\lambda, and let χλ∈Hλ\chi_{\lambda}\in H_{\lambda} be the corresponding character.

The group algebra case corresponds to when dλ=1d_{\lambda}=1 for any λ\lambda, and then the characters correspond to the group-like elements. Since for group algebras inner faithfulness can be detected by only studying the restriction of a representation to group-like elements, it would be natural to hope that in the general case, the restriction to characters would lead to the same information. The following simple example shows that this is not true.

The elements τ1\tau_{1}, τ2\tau_{2} and τ3\tau_{3} are all conjugate in S4S_{4}, so this representation is not injective on characters. Thus an inner faithful representation is not necessarily injective on characters.

is injective on characters (as one easily checks on the character table of S4S_{4}) but is not inner faithful since the elements τ1\tau_{1} and (1,2,3)(1,2,3) do not generate S4S_{4}.

As a conclusion, it seems that there is no link between the inner faithfulness of a representation and its injectivity on characters.

Twistings

In this section we study the behaviour of Hopf images under various deformation procedures such as Drinfeld’s twisting, or the dual operation, often called 2-cocycle deformation, that we will call here cotwisting for simplicity.

We begin with the twisting operation, in the sense of Drinfeld . More exactly the definitions we use are taken or adapted from .

Let HH be a Hopf algebra and let Ω\Omega be an invertible element in H⊗HH\otimes H. Consider the linear maps δΩ,ΔΩ:H⟶H⊗H\delta_{\Omega},\Delta_{\Omega}:H\longrightarrow H\otimes H defined respectively by

We say that Ω\Omega is a twist on HH if (H,δΩ,ε)(H,\delta_{\Omega},\varepsilon) is a coalgebra. The element u=m∘(idH⊗S)(Ω)u=m\circ({\rm id_{H}}\otimes S)(\Omega) is then invertible in HH, and HΩ=(H,m,u,ΔΩ,ε,Su)H_{\Omega}=(H,m,u,\Delta_{\Omega},\varepsilon,S_{u}) is a Hopf algebra, where Su:H⟶HS_{u}:H\longrightarrow H is defined by Su(x)=uS(x)u−1S_{u}(x)=uS(x)u^{-1}.

We say that Ω\Omega is a pseudo-twist on HH if (ε⊗id)(Ω)=1=(id⊗ε)(Ω)(\varepsilon\otimes{\rm id})(\Omega)=1=({\rm id}\otimes\varepsilon)(\Omega), if (H,ΔΩ,ε)(H,\Delta_{\Omega},\varepsilon) is a coalgebra, and if there exists an invertible element u∈Hu\in H such that Su:H⟶HS_{u}:H\longrightarrow H, defined by Su(x)=uS(x)u−1S_{u}(x)=uS(x)u^{-1}, is an antipode for the bialgebra (H,m,u,ΔΩ,ε)(H,m,u,\Delta_{\Omega},\varepsilon), so that HΩ=(H,m,u,ΔΩ,ε,Su)H_{\Omega}=(H,m,u,\Delta_{\Omega},\varepsilon,S_{u}) is a Hopf algebra.

A Hopf algebra having the form HΩH_{\Omega} for some twist (resp. pseudo-twist) Ω\Omega on HH is said to be a twist (resp. pseudo-twist) of HH.

The following lemma gives some basic properties of twisting, probably well-known. The direct verification is left to the reader.

Let Ω\Omega be a pseudo-twist on a Hopf algebra HH.

Let f:H⟶Lf:H\longrightarrow L be a surjective Hopf algebra map. Then f∗(Ω)=(f⊗f)(Ω)f^{*}(\Omega)=(f\otimes f)(\Omega) is also a pseudo-twist for LL.

The Hopf ideals in HH are exactly the Hopf ideals in HΩH_{\Omega}.

Let HH be a Hopf algebra, let Ω\Omega be a pseudo-twist on HH and let π:H⟶A\pi:H\longrightarrow A be a representation on an algebra AA, that we also view as a representation π:HΩ⟶A\pi:H_{\Omega}\longrightarrow A. We have (HΩ)π=(Hπ)p∗(Ω)(H_{\Omega})_{\pi}=(H_{\pi})_{p^{*}(\Omega)}, where p:H⟶Hπp:H\longrightarrow H_{\pi} is the canonical projection, and π\pi is inner faithful as a representation of HH if and only if it is inner faithful as a representation of HΩH_{\Omega}.

Since by the previous lemma the Hopf ideals of HH and of HΩH_{\Omega} are the same, this is also true for the Hopf ideals contained in Ker(π){\rm Ker}(\pi), and the largest one is the same. So the defining Hopf ideal of (HΩ)π(H_{\Omega})_{\pi} is the Hopf ideal IπI_{\pi} constructed in Section 2, so that (HΩ)π=HΩ/Iπ(H_{\Omega})_{\pi}=H_{\Omega}/I_{\pi}, and since (H/Iπ)p∗(Ω)=HΩ/Iπ(H/I_{\pi})_{p^{*}}(\Omega)=H_{\Omega}/I_{\pi}, we have the claimed result. The last assertion is also immediate after the previous discussion. ∎

It follows that the twist of an inner linear Hopf algebra is still inner linear. The reader will find several examples of twisted Hopf algebras in , for example, for which the above theorem furnishes inner faithful representations of the new Hopf algebra from the old one. Some of the Hopf algebras considered in Section 9 are also obtained by twisting.

2. Cotwisting

We now deal with the dual operation to twisting, that we call cotwisting. The situation is more complicated here, because we deform the product rather than the coproduct, and so a representation of the given Hopf algebra is not a representation of the deformed one.

Let us recall the basic vocabulary, which is dual to the one of the previous subsection. We only consider the cotwist case.

Let H=HH=H be a Hopf algebra. We use Sweedler’s notation Δ(x)=x1⊗x2\Delta(x)=x_{1}\otimes x_{2}. Recall (see e.g. ) that a cotwist (=2-cocycle) is a convolution invertible linear map σ:H⊗H⟶C\sigma:H\otimes H\longrightarrow{\rm C} satisfying

and σ(x,1)=σ(1,x)=ε(x)\sigma(x,1)=\sigma(1,x)=\varepsilon(x), for x,y,z∈Hx,y,z\in H.

Following and , we associate various algebras to a cotwist. First consider the algebra σ ⁣H{}_{\sigma}\!H. As a vector space we have σ ⁣H=H{}_{\sigma}\!H=H and the product of σH{}_{\sigma}H is defined to be

where an element x∈Hx\in H is denoted {x}\{x\}, when viewed as an element of σ ⁣H{}_{\sigma}\!H.

We also have the algebra Hσ−1H_{\sigma^{-1}}, where σ−1\sigma^{-1} denotes the convolution inverse of σ\sigma. As a vector space we have Hσ−1=HH_{\sigma^{-1}}=H and the product of Hσ−1H_{\sigma^{-1}} is defined to be

where an element x∈Hx\in H is denoted ⟨x⟩\langle x\rangle, when viewed as an element of Hσ−1H_{\sigma^{-1}}. The cocycle condition ensures that σ ⁣H{}_{\sigma}\!H and Hσ−1H_{\sigma^{-1}} are associative algebras with 11 as a unit.

Finally we have the Hopf algebra Hσ=σ ⁣H ⁣σ−1H^{\sigma}={{}_{\sigma}\!H}\!_{\sigma^{-1}}. As a coalgebra Hσ=HH^{\sigma}=H. The product of HσH^{\sigma} is defined to be

where an element x∈Hx\in H is denoted [x][x], when viewed as an element of HσH^{\sigma}, and we have the following formula for the antipode of HσH^{\sigma}:

A Hopf algebra having the form HσH^{\sigma} for some cotwist σ\sigma on HH is said to be a cotwist of HH.

Let HH be a Hopf algebra and let σ:H⊗H→k\sigma:H\otimes H\to k be a cotwist induced by a finite-dimensional quotient Hopf algebra of HH. Assume that S2S^{2} is an inner automorphism of HH. If HH is inner linear, then HσH^{\sigma} is also inner linear.

The proof will be a consequence of the following technical result.

Let θ:H⟶A⊗L\theta:H\longrightarrow A\otimes L be an algebra map, where H,LH,L are Hopf algebras and AA is an algebra, and let φ:L⟶B\varphi:L\longrightarrow B be an inner faithful representation of LL on an algebra BB. Assume that there exists ψ∈A∗\psi\in A^{*} such that (ψ⊗idL)∘θ:H⟶L(\psi\otimes{\rm id}_{L})\circ\theta:H\longrightarrow L is an injective coalgebra map. Assume moreover that one of the following conditions holds.

SL∘((ψ⊗idL)∘θ)=((ψ⊗idL)∘θ)∘SHS_{L}\circ((\psi\otimes{\rm id}_{L})\circ\theta)=((\psi\otimes{\rm id}_{L})\circ\theta)\circ S_{H}.

SL(Ker(φ))⊂Ker(φ)S_{L}({\rm Ker}(\varphi))\subset{\rm Ker}(\varphi).

Then the representation (idA⊗φ)∘θ:H⟶A⊗B({\rm id}_{A}\otimes\varphi)\circ\theta:H\longrightarrow A\otimes B is inner faithful.

Let I⊂Ker((idA⊗φ)∘θ)I\subset{\rm Ker}(({\rm id}_{A}\otimes\varphi)\circ\theta) be a Hopf ideal. Let J=(ψ⊗idL)(θ(I))⊂LJ=(\psi\otimes{\rm id}_{L})(\theta(I))\subset L: this is a coideal since (ψ⊗idL)∘θ(\psi\otimes{\rm id}_{L})\circ\theta is a coalgebra map. We have

and hence J⊂Ker(φ)J\subset{\rm Ker}(\varphi). Let J+J^{+} be the ideal of LL generated by JJ: we have J+⊂Ker(φ)J^{+}\subset{\rm Ker}(\varphi) and J+J^{+} is a bi-ideal in LL.

Assume that condition (1) holds. Then JJ is SLS_{L}-stable and hence so is J+J^{+}, which is a Hopf ideal. Since φ\varphi is inner faithful, we have J+=J=(0)J^{+}=J=(0), and we conclude that I=(0)I=(0) by the injectivity of (ψ⊗idL)∘θ(\psi\otimes{\rm id}_{L})\circ\theta.

Assume now that condition (2) holds. Then J+=(0)=JJ^{+}=(0)=J by Proposition 2.8, and I=(0)I=(0), again by the injectivity of (ψ⊗idL)∘θ(\psi\otimes{\rm id}_{L})\circ\theta. ∎

By the assumption, there is a Hopf algebra surjection π:H→K\pi:H\to K onto a finite dimensional Hopf algebra KK and a cotwist τ:K⊗K→k\tau:K\otimes K\to k such that σ=τπ\sigma=\tau_{\pi}. As noted in , we have an injective algebra map

Consider the linear map ψ=ε⊗ε:τ ⁣K⊗Kτ−1⟶k\psi=\varepsilon\otimes\varepsilon:{{}_{\tau}\!K}\otimes K_{\tau^{-1}}\longrightarrow k. We have (ψ⊗id)∘θ=id(\psi\otimes{\rm id})\circ\theta={\rm id}, and hence is a coalgebra map. Let φ0:H⟶B\varphi_{0}:H\longrightarrow B be an inner faithful finite-dimensional representation, and let φ:H⟶B×Bop\varphi:H\longrightarrow B\times B^{\rm op}, x⟼(φ0(x),φ0(S(x)))x\longmapsto(\varphi_{0}(x),\varphi_{0}(S(x))). It is clear that φ\varphi is still inner faithful, and the second condition in the previous theorem is satisfied since S2S^{2} is inner. Hence the previous theorem ensures that the representation (id⊗φ)∘θ:H⟶τ ⁣K⊗Kτ−1⊗(B×Bop)({\rm id}\otimes\varphi)\circ\theta:H\longrightarrow{{}_{\tau}\!K}\otimes K_{\tau^{-1}}\otimes(B\times B^{\rm op}) is inner faithful, and we are done since τ ⁣K⊗Kτ−1{{}_{\tau}\!K}\otimes K_{\tau^{-1}} is finite-dimensional. ∎

Tensor and free product of representations

The Hopf image does not behave well with respect to the tensor or free product: the Hopf image of a tensor or free product is not necessarily the tensor or free product of the Hopf images. Here is what can be said in general.

Let HH and LL be Hopf algebras and let π:H⟶A\pi:H\longrightarrow A and φ:L⟶B\varphi:L\longrightarrow B be algebra maps. Then there are surjective Hopf algebra maps

We consider the Hopf algebra factorizations

and the universal property of the Hopf image yields the announced Hopf algebra maps, which are clearly surjective. ∎

The morphisms in the proposition are not injective in general, as the following example shows.

For the tensor product, a faithfulness assumption on one of the algebra morphisms enables one to describe the Hopf image easily. We begin with a lemma. We use the notation of Section 2.

Let HH and LL be Hopf algebras and let π:H⟶A\pi:H\longrightarrow A and φ:L⟶B\varphi:L\longrightarrow B be algebra maps. Then

We first show that for any g∈Fg\in F, there exists a linear isomorphism Tg:Ag⊗Bg⟶(A⊗B)gT_{g}:A^{g}\otimes B^{g}\longrightarrow(A\otimes B)^{g} such that (π⊗φ)g=Tg∘(πg⊗φg)(\pi\otimes\varphi)^{g}=T_{g}\circ(\pi^{g}\otimes\varphi^{g}). We prove this by induction on l(g)l(g). This is clear if l(g)≤1l(g)\leq 1, so we assume that g=hh′g=hh^{\prime} with l(g)>l(h)≥1l(g)>l(h)\geq 1 and l(g)>l(h′)≥1l(g)>l(h^{\prime})\geq 1. Let x∈Hx\in H and y∈Ly\in L. We have, using the induction assumption,

and hence we have the desired result. Thus for g∈Fg\in F, we have Ker((π⊗φ)g)=Ker(πg⊗φg){\rm Ker}((\pi\otimes\varphi)^{g})={\rm Ker}(\pi^{g}\otimes\varphi^{g}), and we have our result. ∎

Let HH and LL be Hopf algebras and let π:H⟶A\pi:H\longrightarrow A and φ:L⟶B\varphi:L\longrightarrow B be algebra maps. Assume that π\pi is faithful and that the antipode of HH is injective. Then (H⊗L)π⊗φ≅H⊗Lφ(H\otimes L)_{\pi\otimes\varphi}\cong H\otimes L_{\varphi}. In particular if π\pi is faithful and φ\varphi is inner faithful, then π⊗φ\pi\otimes\varphi is inner faithful.

It is sufficent to show that Iπ⊗φ=H⊗IφI_{\pi\otimes\varphi}=H\otimes I_{\varphi}, since (H⊗L)/(H⊗Iφ)≃H⊗(L/Iφ)(H\otimes L)/(H\otimes I_{\varphi})\simeq H\otimes(L/I_{\varphi}). For any g∈Fg\in F, the representation πg\pi^{g} is faithful since Δ\Delta and SS are injective, so Ker(πg⊗φg)=H⊗Ker(φg){\rm Ker}(\pi^{g}\otimes\varphi^{g})=H\otimes{\rm Ker}(\varphi^{g}). By the previous lemma we have

and we have our result. The last assertion is immediate. ∎

Of course the assumption of the injectivity of the antipode is satisfied in the most interesting cases. See for an example of a Hopf algebra having a non-injective antipode.

The result in the previous proposition naturally leads to the following question.

Let π:H⟶A\pi:H\longrightarrow A be a representation of a Hopf algebra HH on an algebra AA. Does there exist a condition on π\pi, weaker than faithfulness, that ensures that for any inner faithful representation φ:L⟶B\varphi:L\longrightarrow B of a Hopf algebra LL on an algebra BB, then the representation π⊗φ\pi\otimes\varphi is inner faithful?

If a representation π\pi satisfies to the hypothetic condition of Question 7.6, then in particular π⊗π\pi\otimes\pi will be inner faithful. It seems to be simpler to study first representations with this weaker property, and this leads to the following definition.

Let π:H⟶A\pi:H\longrightarrow A be a representation of a Hopf algebra HH on an algebra AA. We say that π\pi is projectively inner faithful if π⊗π\pi\otimes\pi is inner faithful.

Once again the terminology is motivated by the discrete group case: a representation π:k[Γ]⟶A\pi:k[\Gamma]\longrightarrow A is projectively inner faithful if and only if the associated group morphism Γ⟶A×/k∗\Gamma\longrightarrow A^{\times}/k^{*} is faithful. When A=End(V)A={\rm End}(V), this means that Γ\Gamma embeds into the projective linear group PGL(V){\rm PGL}(V).

The example of function algebras shows that it is in general difficult to decide when an inner faithful representation is projectively inner faithful. This specific example leads to the following definition. This is a purely discrete group theoretic definition, but of course we have in mind discrete groups embedded as dense subgroups of algebraic groups.

Let Γ\Gamma be a discrete group and let {s1,…,sn}\{s_{1},\ldots,s_{n}\} be a family of generators of Γ\Gamma. We say that {s1,…,sn}\{s_{1},\ldots,s_{n}\} is a family of projective generators of Γ\Gamma if the group Γ×Γ\Gamma\times\Gamma is generated by the elements (si,sj)(s_{i},s_{j}), 1≤i,j≤n1\leq i,j\leq n.

Of course {s1,…,sn}\{s_{1},\ldots,s_{n}\} is a family of projective generators if 1∈{s1,…sn}1\in\{s_{1},\ldots s_{n}\}. It would be interesting to have more examples and to characterize the family of projective generators of a group.

We end the section by noting that there is no analogous result to Proposition 7.4. in the free product case, as shown by the following example.

Tannaka duality

Tannaka duality studies the interplays between a Hopf algebra and its category of comodules. In this section we formulate some Tannaka type results for Hopf images. These results are used in , in the study of quantum permutation groups associated to complex Hadamard matrices.

Let HH be a Hopf algebra and let U,VU,V be HH-comodules. The coaction on UU is denoted αU:U⟶U⊗H\alpha_{U}:U\longrightarrow U\otimes H. The set of HH-comodule morphisms from UU to VV is denoted HomH(U,V){\rm Hom}_{H}(U,V). If f:H⟶Lf:H\longrightarrow L is a Hopf algebra map, then ff induces natural LL-comodule structures on UU and VV (the resulting comodules still being denoted UU and VV if no confusion arises), with

We now introduce a key space for the computation of Hom spaces of a Hopf image.

Let π:H⟶A\pi:H\longrightarrow A be a representation of a Hopf algebra HH on an algebra AA, and let U,VU,V be some HH-comodules. The space of π\pi-morphisms from UU to VV is defined by

The idea is that the space of π\pi-morphisms is a more concrete one than the space of HπH_{\pi}-comodules (at least if the algebra AA is a more concrete one than HH), and hence should be easier to describe. In fact it contains all the necessary information.

Let π:H⟶A\pi:H\longrightarrow A be a representation of a Hopf algebra HH on an algebra AA. Let UU and VV be finite dimensional HH-comodules and let (L,q,φ)(L,q,\varphi) be a factorization of π\pi. Then we have

The first three inclusions on the left arise from the Hopf algebra maps H→L→HπH\rightarrow L\rightarrow H_{\pi}. Let f∈HomHπ(U,V)f\in{\rm Hom}_{H_{\pi}}(U,V). Then we have, with the notations of Theorem 2.1:

Hence f∈Hom(Uπ,Vπ)f\in{\rm Hom}(U_{\pi},V_{\pi}) and HomHπ(U,V)⊂Hom(Uπ,Vπ){\rm Hom}_{H_{\pi}}(U,V)\subset{\rm Hom}(U_{\pi},V_{\pi}). Assume conversely that f∈Hom(Uπ,Vπ)f\in{\rm Hom}(U_{\pi},V_{\pi}), and let e1,…,eme_{1},\ldots,e_{m} and e1′,…,em′e^{\prime}_{1},\ldots,e^{\prime}_{m} be respective bases of UU and VV with

Let (λij)∈Mm,n(k)(\lambda_{ij})\in M_{m,n}(k) be such that f(ei)=∑jλjiej′f(e_{i})=\sum_{j}\lambda_{ji}e^{\prime}_{j}. Then since f∈Hom(Uπ,Vπ)f\in{\rm Hom}(U_{\pi},V_{\pi}), we have for 1≤i≤n1\leq i\leq n, 1≤l≤m1\leq l\leq m:

Let II be the ideal generated by the elements PliP_{li}. We have

and hence that II is a bi-ideal. Multiplying PilP_{il} on the left by S(vrl)S(v_{rl}) and on the right by S(uis)S(u_{is}) and summing over ii and ll gives

Thus II is a Hopf ideal and hence I⊂Iπ=Ker(p)I\subset I_{\pi}={\rm Ker}(p). Thus we have, for 1≤i≤n1\leq i\leq n, 1≤l≤m1\leq l\leq m:

This exactly means that f∈HomHπ(U,V)f\in{\rm Hom}_{H_{\pi}}(U,V), and we are done. ∎

Let π:H⟶A\pi:H\longrightarrow A be a representation of a Hopf algebra HH on an algebra AA. If π\pi is inner faithful, then we have,

The converse of the corollary is not true in general. To see this, assume that kk has characteristic zero and consider H=O(SL2(k))H=\mathcal{O}({\rm SL}_{2}(k)) and L=O(B)L=\mathcal{O}(B), with BB being the Borel subgroup of SL2(k){\rm SL}_{2}(k) consisting of triangular matices. The restriction map O(SL2(k))⟶O(B)\mathcal{O}({\rm SL}_{2}(k))\longrightarrow\mathcal{O}(B) is not inner faithful because it is not faithful, and has O(B)\mathcal{O}(B) as Hopf image. One easily sees that for the irreducible representations of SL2(k){\rm SL}_{2}(k) (the symmetric powers of the fundamental representation), one has HomSL2(k)(U,V)=HomB(U,V){\rm Hom}_{{\rm SL}_{2}(k)}(U,V)={\rm Hom}_{B}(U,V), and hence by the cosemisimplicity of O(SL2(k))\mathcal{O}({\rm SL}_{2}(k)), this is true for any representation of SL2(k){\rm SL}_{2}(k).

However we have a converse to the corollary if both HH and the Hopf image are cosemisimple.

Let π:H⟶A\pi:H\longrightarrow A be a representation of a cosemisimple Hopf algebra HH on an algebra AA. Assume that the Hopf image HπH_{\pi} is cosemisimple. Then π\pi is inner faithful if and only if

for any simple HH-comodules UU and VV.

The ⇒\Rightarrow part is the previous corollary. Conversely, let us assume that

for any simple HH-comodules UU and VV. Then the canonical projection p:H⟶Hπp:H\longrightarrow H_{\pi} induces an injection from the set of simple HH-comodules to the set of simple HπH_{\pi}-comodules, and using the respective Peter-Weyl decompositions of HH and HπH_{\pi}, we see that pp is injective, and hence is an isomorphism. ∎

It seems to be difficult in general to ensure that the Hopf image is cosemisimple. However this is automatically true when one works in the category of compact Hopf algebras (in the sense of Section 2), and hence we get the following interesting characterization of inner faithfulness for ∗*-representations.

Let π:H⟶A\pi:H\longrightarrow A be a ∗*-representation of a compact Hopf algebra HH on a ∗*-algebra AA. Then π\pi is inner faithful if and only if

for any simple HH-comodules UU and VV.

The proof is done by the straightforward adaptation of the arguments of Theorem 8.2 and Theorem 8.4 to the ∗*-case. ∎

Let π:H⟶A\pi:H\longrightarrow A be a ∗*-representation of a compact Hopf algebra HH on a ∗*-algebra AA, and let UU be a faithful HH-comodule. Then π\pi is inner faithful if and only if

When the faithful HH-comodule is self-dual (for example in the case of quantum permutation algebras as in ), the previous theorem has the following simpler form.

Let π:H⟶A\pi:H\longrightarrow A be a ∗*-representation of a compact Hopf algebra HH on a ∗*-algebra AA, and let UU be a faithful self-dual HH-comodule. Then π\pi is inner faithful if and only if

All the comodules UxU^{x} of the previous theorem are isomorphic with U⊗nU^{\otimes n} for some nn, and hence the result follows. ∎

Hopf algebras with small corepresentation level

This section gives a concrete application of the inner faithfulness criterion of the previous section to compact Hopf algebras having all their simple comodules of dimension smaller than 22. The Hopf algebras we consider arise in the study of 4×44\times 4 Hadmard matrices (). Let us begin with some vocabulary.

Pointed Hopf algebras are exactly the Hopf algebras with cl(H)=1cl(H)=1. The finite groups Γ\Gamma having all their irreducible representations of dimension ≤2\leq 2 (in characteristic zero) are described in , corresponding to the function Hopf algebras kΓk^{\Gamma} such that cl(kΓ)≤2cl(k^{\Gamma})\leq 2.

We begin with a general result (Theorem 9.2) that ensures that a representation of a compact Hopf algebra with corepresentation level 22 is inner faithful. Then this result will be used to construct inner faithful representations of some concrete Hopf algebras in Theorems 9.3 and 9.4.

Let HH be a compact Hopf algebra with cl(H)=2cl(H)=2. Let Γ\Gamma be the group of group-like elements of HH and let Λ\Lambda be the set of isomorphism classes of simple two-dimensional HH-comodules. For each λ∈Λ\lambda\in\Lambda, fix a matrix uλ=(uijλ)∈M2(H)u^{\lambda}=(u_{ij}^{\lambda})\in M_{2}(H) of corresponding coefficients. Let π:H⟶A\pi:H\longrightarrow A be a ∗*-representation. Assume that the following conditions are fulfilled.

∀λ∈Λ\forall\lambda\in\Lambda, π(u11λ)=0=π(u22λ)\pi(u_{11}^{\lambda})=0=\pi(u_{22}^{\lambda}).

∀λ∈Λ\forall\lambda\in\Lambda, ∀g∈Γ\forall g\in\Gamma, π(u12λ)\pi(u_{12}^{\lambda}) and π(g)\pi(g) are linearly independent.

∀λ,μ∈Λ\forall\lambda,\mu\in\Lambda, π(u12λ)\pi(u_{12}^{\lambda}) and π(u21μ)\pi(u_{21}^{\mu}) are linearly independent.

∀λ,μ∈Λ\forall\lambda,\mu\in\Lambda with λ≠μ\lambda\not=\mu, π(u12λ)\pi(u_{12}^{\lambda}) and π(u12μ)\pi(u_{12}^{\mu}) are linearly independent.

We now use Theorem 9.2 to provide inner faithful representations of a class of Hopf algebras considered in , Section 7. We refer the reader to for the precise origins of these Hopf algebras, which we present now. First we have the Hopf algebra Ah(2)A_{h}(2): this is the universal ∗*-algebra presented by generators (vij)1≤i,j≤2(v_{ij})_{1\leq i,j\leq 2} and relations:

The matrix v=(vij)v=(v_{ij}) is orthogonal (with vij∗=vijv_{ij}^{*}=v_{ij}).

vijvik=vikvkj=0=vjivki=vkivjiv_{ij}v_{ik}=v_{ik}v_{kj}=0=v_{ji}v_{ki}=v_{ki}v_{ji} if j≠kj\not=k.

endow Ah(2)A_{h}(2) with a compact Hopf algebra structure. We have cl(Ah(2))=2cl(A_{h}(2))=2, and the fusion rules of the corepresentations of Ah(2)A_{h}(2) are those of the orthogonal group O(2)(2).

The Hopf algebra Ah(2)A_{h}(2) has a series of finite-dimensional quotients defined as follows.

If qq is not a root of unity, then the ∗*-representation πq\pi_{q} is inner faithful.

If qq has order 2m+12m+1, then Ah(2)πq≃A(2m+1,1)A_{h}(2)_{\pi_{q}}\simeq A(2m+1,1).

If qq has order 4m4m, then Ah(2)πq≃A(2m,−1)A_{h}(2)_{\pi_{q}}\simeq A(2m,-1).

If qq has order 4m+24m+2, then Ah(2)πq≃A(2m+1,−1)A_{h}(2)_{\pi_{q}}\simeq A(2m+1,-1).

It is straightforward to check the existence of the ∗*-representation πq\pi_{q}. For m≥1m\geq 1, we have

(1) We have cl(Ah(2))=2cl(A_{h}(2))=2 and the simple Ah(2)A_{h}(2)-comodules are as follows: there is only one non-trivial one dimensional comodule, corresponding to the group-like d=v112−v122d=v_{11}^{2}-v_{12}^{2}, and a family of simple 2-dimensional comodules VnV_{n}, n≥1n\geq 1, corresponding to the simple subcoalgebras

It is straightforward to check that if qq is not a root of unity, the representation πq\pi_{q} satisfies to the conditions of Theorem 9.2, and hence we have our result.

The Hopf algebra Ah(2)A_{h}(2) is in fact a particular case of a construction given in , Example 2.5, that we describe now, and the inner faithful representation of the previous theorem has a natural generalization.

Then An(Γ)A_{n}(\Gamma) is a compact Hopf algebra, with:

We need some notation to state a generalization of the first part of Theorem 9.3. We consider the group free product Γ∗Γ\Gamma*\Gamma, with the canonical morphisms still denoted ν1,ν2:Γ⟶Γ∗Γ\nu_{1},\nu_{2}:\Gamma\longrightarrow\Gamma*\Gamma. The canonical involutive group automorphism of Γ∗Γ\Gamma*\Gamma is denoted by τ\tau, with τ∘ν1=ν2\tau\circ\nu_{1}=\nu_{2} and τ∘ν2=ν1\tau\circ\nu_{2}=\nu_{1}.

In particular, if there exists a group embedding Γ∗Γ⊂PU(n)\Gamma*\Gamma\subset{\rm PU}(n) for some n≥1n\geq 1, then the Hopf algebra A2(Γ)A_{2}(\Gamma) is inner linear.

It is a direct verification to check that the above formulae define a ∗*-representation π:A2(Γ)⟶A\pi:A_{2}(\Gamma)\longrightarrow A. Recall from that we have an algebra isomorphism

The comodules UxU_{x} and UyU_{y} are isomorphic if and only if x=yx=y or x=τ(y)x=\tau(y). Any 22-dimensional A2(Γ)A_{2}(\Gamma)-comodule is isomorphic to some UxU_{x}, and cl(A2(Γ))=2cl(A_{2}(\Gamma))=2. For x∈Γ∗Γ∖{1}x\in\Gamma*\Gamma\setminus\{1\}, we have

Then it is a straightforward verification to check that the conditions of Theorem 9.2 are fulfilled, using the properties of the group morphism π0\pi_{0} (using also that x=1x=1 if and only if x=τ(x)x=\tau(x)), and we conclude that π\pi is inner faithful. ∎

References