Autoequivalences of tensor categories attached to quantum groups at roots of $1$
Alexei Davydov, Pavel Etingof, and Dmitri Nikshych

TL;DR
This paper calculates the group of braided tensor autoequivalences and the Brauer-Picard group for the representation category of small quantum groups at roots of unity, advancing understanding of their symmetries.
Contribution
It provides explicit computations of autoequivalence groups for tensor categories associated with quantum groups at roots of unity, a previously uncharted area.
Findings
Determined the group of braided tensor autoequivalences.
Computed the Brauer-Picard group of the category.
Enhanced understanding of symmetries in quantum group categories.
Abstract
We compute the group of braided tensor autoequivalences and the Brauer-Picard group of the representation category of the small quantum group , where is a root of unity.
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
Taxonomy
TopicsAlgebraic structures and combinatorial models · Homotopy and Cohomology in Algebraic Topology · Advanced Algebra and Geometry
Autoequivalences of tensor categories attached to quantum groups at roots of
Alexei Davydov
A.D.: Department of Mathematics, Ohio University, Athens, OH 45701, USA
,
Pavel Etingof
P.E.: Department of Mathematics, Massachusetts Institute of Technology, Cambridge, MA 02139, USA
and
Dmitri Nikshych
D.N.: Department of Mathematics and Statistics, University of New Hampshire, Durham, NH 03824, USA
Abstract.
We compute the group of braided tensor autoequivalences and the Brauer-Picard group of the representation category of the small quantum group , where is a root of unity.
To the memory of Bertram Kostant
1. Introduction
Let be an algebraically closed field of characteristic zero. Let be a simple algebraic group over , and let be its Lie algebra. Let be a root of unity of odd order coprime to if is of type , and coprime to the determinant of the Cartan matrix of . Let be Lusztig’s small quantum group attached to [Lu1]. Then is a quasitriangular Hopf algebra, so the category of its finite dimensional representations is a finite braided tensor category [EGNO]. One of the main goals of this paper is to compute the Picard group of this category, i.e., the group of equivalence classes of invertible -module categories. Picard groups of braided tensor categories and, in particular, Brauer-Picard groups of tensor categories play a crucial role in classification of graded extensions [ENO] and also appear as symmetry groups of three-dimensional topological field theories [FS]. It is known that is isomorphic to the group of braided autoequivalences of [DN, ENO]. We show under some restrictions on that is isomorphic to the group of automorphisms of , i.e., , where is the adjoint group of and is the automorphism group of the Dynkin diagram of . Namely, we prove this when the order of is sufficiently large and also for classical groups if .
Moreover, we show that has only two braidings (the standard one and its reverse) and deduce that any tensor autoequivalence of is necessarily braided. Thus, the group of tensor autoequivalences (also known as the group of biGalois objects) of is isomorphic to . This generalizes the result of Bichon [Bi2], who proved this fact for .
We also consider the braided tensor category of finite dimensional comodules over the function algebra , which is the -equivariantization of . We show that every braided autoequivalence of comes from a Dynkin diagram automorphism if is sufficiently large, and prove a similar result in the non-braided case. This generalizes a result of Neshveyev and Tuset [NT1, NT2], who proved this when is not a root of unity. We also show this for the classical groups if .
As a tool, we introduce the notion of a finitely dominated tensor category. We show that the category of comodules over a finitely presented Hopf algebra is finitely dominated and prove that tensor autoequivalences of a finitely dominated category that preserve a tensor generator form an algebraic group. While this theory plays an auxiliary role in our paper, it may be of independent interest.
We expect that the main results of this paper extend without significant difficulties to roots of unity of arbitrary order , not necessarily satisfying the above coprimeness assumptions (at least when is sufficiently large). However, this would require some important modifications in the statements. Notably, if , where is the the ratio of squared norms of long and short roots of , and is simply connected, then is a -equivariantization (rather than a -equivariantization) of an appropriate version of , where is the Langlands dual group of , see [AG]. Therefore, we expect that in this case (note that by definition ).
The paper is organized as follows. In Section 2 we give preliminaries and auxiliary results. In Section 3 we develop the theory of finitely dominated tensor categories and study groups of tensor autoequivalences of such categories. In Section 4 we classify tensor autoequivalences of . Finally, in Section 5 we prove that any tensor autoequivalence of is braided and classify such autoequivalences. As a consequence, we compute the Brauer-Picard groups of and .
Acknowledgements. We are very grateful to Julien Bichon, Ken Brown, David Kazhdan, George Lusztig, Sergey Neshveyev, Victor Ostrik, Noah Snyder, and Milen Yakimov for useful discussions. The work of P.E. was partially supported by the NSF grant DMS-1502244. The work of D.N. was partially supported by the NSA grant H98230-16-1-0008.
2. Preliminaries and auxiliary results
Let be an algebraically closed field. In this paper we consider tensor categories over [EGNO, Definition 4.1.1] which we will simply refer to as tensor categories. The most basic example of a tensor category is the trivial tensor category , i.e., the category of finite dimensional vector spaces over . More generally, given a Hopf -algebra , the category of finite dimensional left -modules and the category of finite dimensional left -comodules are examples of tensor categories. For a tensor category , let denote the group of isomorphism classes of tensor autoequivalences of .
2.1. Braided tensor categories and their Picard groups
We refer the reader to [EGNO, Chapter 8] for basic definitions related to braided tensor categories. Let be a braided tensor category with braiding . The reverse braiding of is, by definition, , . We will denote by the tensor category with the reverse braiding. Let denote the group of isomorphism classes of braided tensor autoequivalences of .
Let denote the Drinfeld center of . Then the assignment is a braided embedding (i.e., a fully faithful braided tensor functor) . Similarly, the assignment is a braided embedding . These embeddings combine together into a single braided tensor functor
[TABLE]
Assume in addition that is finite (i.e., has finitely many simple objects and enough projective objects). We say that is factorizable if the functor (1) is an equivalence.
Lemma 2.1**.**
Let be a factorizable braided tensor category with braiding . Suppose that is not pointed and that has no proper non-trivial tensor subcategories. Then has exactly two braidings: and .
Proof.
A braiding on is the same thing as a section of the forgetful functor , i.e., a tensor subcategory such that is an equivalence. By the hypothesis, is either or . The former case corresponds to the original braiding . Let us deal with the latter case. We will argue that is non-trivial, and, hence, , which corresponds to the reverse braiding .
Any simple object of is of the form , where are simple objects of . If is in then since it is a subquotient of . Thus, , so must be invertible. Similarly, . Since is non-pointed, one can choose a non-invertible . Therefore, , as required. ∎
Let be a finite braided tensor category. By definition, the Picard group of [ENO, DN] is the group of equivalence classes of invertible -module categories. When is factorizable, there is a canonical group isomorphism
[TABLE]
see [ENO, Theorem 6.2] and [DN, Corollary 4.6].
Thus, computing the Picard group of a factorizable braided tensor category amounts to computing its group of braided tensor autoequivalences.
Corollary 2.2**.**
Let be a factorizable braided tensor category such that . Suppose that is not pointed and that has no proper non-trivial tensor subcategories. Then any tensor autoequivalence of is automatically braided and
[TABLE]
Proof.
Follows from Lemma 2.1. ∎
2.2. Algebraic group actions on categories, equivariantization and de-equivariantization
Let us recall the construction of [AG]. Let be an abstract group. An action of on a category [EGNO, 2.7] is a collection of functors attached to each such that , equipped with functorial isomorphisms satisfying the 2-cocycle condition . Given such an action, a -equivariant object in is an object together with a collection of isomorphisms such that , and the -equivariantization of is the category of -equivariant objects in . If is monoidal or braided, then we require that the functors be monoidal, respectively braided, and preserve the tensor (respectively, braided) structure, in which case the equivariantization inherits the same structure.
For an affine group scheme over , let denote the algebra of regular functions on (i.e., the coordinate Hopf algebra), and let denote the category of -modules. If is artinian and is finite, then we can represent the collection of functors as a single functor , where the Deligne tensor product may be interpreted as the category of -modules in . Namely, is the fiber of at , and (note that in the case of finite ). Then the isomorphisms are also combined into a single isomorphism , where
[TABLE]
is the functor of sheaf-theoretic pullback under the multiplication map : . Similarly, the morphisms are combined into a single morphism , where is the functor attached to the trivial -action on . If is monoidal or braided, we require that be a tensor (respectively, braided) functor, where the tensor product in is over , and that preserve these structures in an appropriate sense.
In this form, the definitions of an action and equivariantization make sense when is an affine algebraic group (as they formalize the requirements that the functors and morphisms depend algebraically on the group elements). Namely, in this case stands for the algebra of regular functions on , is replaced by the category of quasicoherent sheaves , and , where embeds into via the coproduct (induced by the product in ). Also, should be required to be an -module in the -completion of , rather than in itself, and it is no longer the direct sum of (since may be infinite dimensional and non-semisimple). With these definitions, if is a finite tensor category then is a tensor category (in general, not finite), and if is braided then so is (provided that the -action preserves the tensor structure and the braiding). Moreover, sits as a tensor subcategory in (namely, the category of equivariant objects which are multiples to as objects of ), and in the braided case this subcategory is contained in the Müger center of (i.e., the squared braiding of an object of with any object of is the identity).
Finally, given a tensor category together with a braided tensor functor which gives rise to an inclusion (for an affine algebraic group ), we can define the de-equivariantization of to be the category of finitely generated -modules in the ind-completion of , where is the algebra of regular functions on equipped with the action of by left (or, alternatively, right) translations [EGNO, 8.23]. Moreover, if is braided and lies in the Müger center of then is braided and carries a -action, and we have . Conversely, for a braided tensor category with a -action we have , i.e., equivariantization and de-equivariantization are inverses of each other (this fact is essentially proved in [AG] and can also be obtained by adjusting arguments of [DGNO, Section 4] to the infinite setting).
2.3. Quantum groups at roots of unity
Let . Let be a simple algebraic group over and let be the associated Lie algebra. Let denote the coordinate Hopf algebra of and let denote its quantized form, see [BG, KS].
Let be an odd integer, relatively prime to the determinant of the Cartan matrix of and to if is of type . Let be a primitive -th root of unity in . Let be the small quantum group, i.e., the Frobenius-Lusztig kernel [Lu1]. Recall [T, XI.6.3] that is a factorizable quasitriangular Hopf algebra. Also, it was shown in [DL] that there is a cocleft central exact sequence of Hopf algebras
[TABLE]
Moreover, the pullback of the coquasitriangular structure of (dual to the universal -matrix of ) to defines a coquasitriangular structure on , giving the structure of a braided tensor category such that the forgetful functor is braided.
It follows that there is a natural action of on as a braided category. Furthermore, it follows from [AG, AGP] that with respect to this action is equivalent to the -equivariantization of , which can, in turn, be recovered as the de-equivariantization of :
[TABLE]
More precisely, [AG] considers the case when is a root of unity of order , where is the ratio of the squared norm of long roots of to the squared norm of short roots. In this case the role of is played by , where is the Langlands dual group to , but the arguments of [AG] apply without significant changes to our case.
It is easy to see that a maximal torus acts on by Hopf algebra automorphisms of (i.e., by conjugation). Hence, the center of acts trivially on (as it is contained in , and conjugation by a central element induces the identity automorphism). On the other hand, the action of is non-trivial, as is not equivalent to . Thus, we get
Proposition 2.3**.**
There is an inclusion .
Remark 2.4**.**
In the case of the inclusion was established by Bichon [Bi2], who also proved that this inclusion is an isomorphism for .
We also have the following (well known) lemmas.
Lemma 2.5**.**
* has no nontrivial Hopf quotients. In particular, it has no nontrivial central grouplike elements.*
Proof.
The second statement follows since is coprime to the determinant of the Cartan matrix of .
To prove the first statement, recall that is a pointed Hopf algebra, and let be its associated graded Hopf algebra under the coradical filtration (it is defined by the same generators and the same relations as , except that now for all ). Then is a pointed Hopf algebra generated in degree . Hence, any proper Hopf ideal in must contain a nonzero element of degree under the coradical filtration. Hence must contain a nonzero -skew-primitive element for some grouplike element . If it is trivial, i.e., is a multiple of , then must contain for some (since is not central and thus acts on some with eigenvalue ). Thus, in any case contains a nontrivial -skew-primitive element, say . Since
[TABLE]
we have . Thus (as is odd). Thus and for connected to in the Dynkin diagram of (as acts on these elements with eigenvalues ). Continuing in this way, we will get that for all (as the Dynkin diagram of is connected). Hence is the augmentation ideal. This implies the required statement. ∎
Lemma 2.6**.**
The only tensor automorphism of the identity functor of is the identity.
Proof.
This follows from Lemma 2.5, since any such automorphism is defined by a central grouplike element. ∎
Finally, we will need the following lemma. Let be the weight lattice of , its dominant part, and be the simple -comodule with highest weight . Recall that is the semisimple subcategory whose simple objects are for ([Lu2, DL]).
Lemma 2.7**.**
If is not divisible by then the matrix elements of and generate , where is a central subgroup of .
Proof.
Let be the Hopf subalgebra generated by the matrix elements of and . It is clear that the -comodule (which is a -module) is a subquotient of . Let be the kernel of the action of on . Then the matrix elements of generate , so . Let be the fiber of the -module at , a finite dimensional Hopf algebra. It is clear that , and the fiber of at is , so is a Hopf subalgebra of , hence is a Hopf quotient of . Also since is not divisible by and hence . Since by Lemma 2.5 has no nontrivial Hopf quotients, we get . Thus, the de-equivariantization is actually the entire category . Hence, and , as desired. ∎
2.4. Compatibility of tensor functors on comodule categories with vector space dimensions.
Proposition 2.8**.**
Let be a finitely generated Hopf algebra over of slower than exponential growth (e.g., of finite GK dimension). Then
- (i)
for any fiber functor one has ; 2. (ii)
For any tensor autoequivalence one has .
Proof.
(i) We have , so there is a simple composition factor in which has dimension . The matrix elements of span a space of dimension and are noncommutative polynomials of degree of the matrix elements of . So if , then has exponential growth.
(ii) Let be the usual fiber functor on . Then is another fiber functor, so by (i) . Also, the same is true for . Hence, . ∎
Remark 2.9**.**
If has exponential growth then both parts of Proposition 2.8 may fail. Indeed, Bichon showed in [Bi1] that for any integer there exists a Hopf algebra such that , so that the 2-dimensional irreducible -module corresponds to an -dimensional -comodule (namely, but has exponential growth for ). Now the usual fiber functor of on for gives a counterexample to (i), and the autoequivalence of the category , switching the factors gives a counterexample to (ii).
2.5. Basic properties of tensor autoequivalences of .
Let be a tensor autoequivalence of . In this section we prove some basic properties of .
Recall that a tensor category is said to be tensor-generated by its object if every object of is a subquotient of a direct sum of tensor powers of .
Lemma 2.10**.**
* induces an autoequivalence of .*
Proof.
By Lemma 2.7, if and then tensor-generates a nonsemisimple category. Hence, if is a simple object then (as tensor-generates a semisimple category). The same holds for . This implies the statement. ∎
By the results of [NT2], the restriction of to belongs to the group , where is the group of outer automorphisms of and is the center of (this uses the theorem of McMullen that any automorphism of the Grothendieck semiring of comes from an automorphism of ). On the other hand, the group acts naturally on . So composing with an element of this group if needed, we may assume that .
Remark 2.11**.**
If is braided then another way to prove Lemma 2.10 is to note that is the Müger center of (since is a factorizable Hopf algebra, is a factorizable braided tensor category and so its Müger center is trivial), hence must be preserved by .
Moreover, in this case by the uniqueness of a fiber functor of a Tannakian category [DM], is given by an outer automorphism of . Thus, by composing with such an automorphism if needed, we may assume that (i.e., we do not have to use [NT2]).
Proposition 2.12**.**
For any finite dimensional -comodule we have .
Proof.
This follows from Proposition 2.8(ii), since has GK dimension (as it is module-finite over ). ∎
Proposition 2.13**.**
If is a tensor autoequivalence of such that then for each simple object .
Proof.
Let be a maximal torus, and the Weyl group. The character map gives an isomorphism (where Gr stands for the Grothendieck ring). Thus, defines an automorphism . Moreover, let be the map defined by raising to power on . Then, since acts trivially on , we have . Also by Proposition 2.12. But the map defines an automorphism of the formal neighborhood of in . Hence, acts trivially on the formal neighborhood of in , and hence . Thus, for each the character of equals the character of . But characters of simple objects are linearly independent, which implies that for all simple objects . ∎
Proposition 2.14**.**
There are no tensor autoequivalences of which reverse the braiding.
Proof.
Suppose for the sake of contradiction that is a braiding-reversing autoequivalence. Then preserves the Müger center , and we may assume without loss of generality that . Hence, by Proposition 2.13, for all simple objects .
Let be the weight lattice of and be the set of dominant integral weights. The eigenvalue of the Drinfeld central element (the double twist) on the simple comodule of highest weight is . Since and reverses braiding, this eigenvalue must equal its reciprocal, so we must have in for all . Subtracting these conditions for two weights , we get in . Thus, in for all , which is a contradiction. ∎
3. Tensor autoequivalences of tensor categories
3.1. Tensor autoequivalences of a finite tensor category
One of the goals of this section is to put algebraic structure on the groups and their subgroups. We start with the following proposition.
Proposition 3.1**.**
Let be a finite tensor category over . Then has a natural structure of an affine algebraic group over . Moreover, if is braided then so does .
Proof.
The idea of the proof is to express categorical data (tensor functors) entirely in terms of linear-algebraic data (linear maps, i.e., eventually, matrices).
Let be the direct sum of the indecomposable projectives of , and . Then we have a natural identification as abelian categories, given by . Under this identification, the tensor product functor is given by tensoring over with an -bimodule , and the associativity isomorphism is represented by an isomorphism of -bimodules satisfying the pentagon relation. Any tensor autoequivalence can then be defined by an algebra automorphism together with a bimodule isomorphism which preserves . It is clear that pairs form an affine algebraic group under the obvious composition. Denote this group by . Also, let , also an affine algebraic group. Then we have a homomorphism of algebraic groups given by , where , . It is clear that a tensor functor determined by is isomorphic to the identity if and only if for some . Thus, is normal in , and is an affine algebraic group, as claimed. ∎
Remark 3.2**.**
A different (but similar) proof of Proposition 3.1 may be obtained by using [EO, Proposition 2.7] which states that any finite tensor category is the representation category of a finite dimensional weak quasi-Hopf algebra , and representing tensor autoequivalences of linear-algebraically as twisted automorphisms of (as in [Da2]).
3.2. Tensor autoequivalences of a tensor category generated by one object
Now let be a tensor category which is not necessarily finite. Then in general is not an algebraic or even a proalgebraic group. For instance, if then . Thus, to obtain a proalgebraic group, we need to put some restrictions on the tensor autoequivalences.
Given , let be the subgroup of elements such that . The following proposition is a generalization of Proposition 3.1 to the infinite case.
Proposition 3.3**.**
Suppose that is tensor-generated by . Then has a natural structure of an affine proalgebraic group. Moreover, if is braided then so does .
Proof.
The proof is analogous to the proof of Proposition 3.1, with additional technical details to deal with the fact that may not be finite.
Namely, has an exhausting increasing filtration , where is the full subcategory whose objects are subquotients of . Note that are finite, and we have compatible tensor product functors . Also, if is a tensor autoequivalence such that then preserves this filtration and these tensor products, and conversely, any autoequivalence with these properties is a tensor autoequivalence such that (indeed, implies ). Here by “ preserves the tensor products” we mean that is equipped with an appropriate tensor structure.
Let be the group of isomorphism classes of autoequivalences preserving the filtration and the tensor products for . Then the groups form an inverse system (i.e., we have natural homomorphisms ), and . Thus, it suffices to show that are affine algebraic groups and are homomorphisms of algebraic groups.
Let be the direct sum of the indecomposable projectives of . Then we have surjections , such that is the intersection of kernels of all morphisms from to objects of . Let . Then any preserves and thus descends to , which defines morphisms . For , the map is an isomorphism, which implies that are surjective. Moreover, we have natural identifications as abelian categories, given by , and the inclusions correspond to the surjections . Under this identification, the tensor product functors are given by tensoring over with an -bimodule , and the associativity isomorphism is represented by an isomorphism of -bimodules
[TABLE]
satisfying the pentagon relation. Moreover, the bimodules are equipped with natural identifications , , coming from restricting the tensor product to and .
Any autoequivalence preserving and the tensor product functors can then be defined by a collection of algebra automorphisms , compatible with and a collection bimodule isomorphisms , preserving and compatible with . It is clear that pairs form an affine algebraic group under the obvious composition. Denote this group by . Also, let , also an affine algebraic group. Then we have a homomorphism of algebraic groups given by , where , . It is clear that a tensor functor determined by is isomorphic to the identity if and only if for some . Thus, is normal in , is an affine algebraic group, and is a morphism of algebraic groups, as claimed. ∎
3.3. Tensor autoequivalences of the category of comodules over a Hopf algebra
Let us describe the affine proalgebraic group more explicitly in the case when , where is a Hopf algebra over . The condition that is tensor-generated by means that is generated as an algebra by the finite dimensional subcoalgebra spanned by the matrix elements of .
Definition 3.4**.**
A co-twisted automorphism of is a pair , where is a coalgebra automorphism, and is a Hopf 2-cocycle such that , where is the product twisted by .
Remark 3.5**.**
This notion is dual to the notion of a twisted automorphism in [Da2], which explains the terminology.
Clearly, co-twisted automorphisms form a group under the obvious composition operation. Let us denote this group by . We have a natural homomorphism given by , where is defined by .
Assume from now on that has slower than exponential growth.
Proposition 3.6**.**
* is surjective.*
Proof.
Let . Recall that , where runs over simple -comodules and is the injective hull of (here the subscript “space” indicates that we are considering just as a vector space, without any actions). By Proposition 2.8, preserves vector space dimensions of -comodules. Hence, , i.e., is induced by a coalgebra automorphism of . Further, since is a tensor equivalence, gives rise to a Hopf 2-cocycle on (which we denote by the same letter) such that preserves the product up to twisting by . Then is a co-twisted automorphism of and . ∎
Let us now describe the kernel of . By definition, it consists of pairs where is the inner automorphism corresponding to an invertible element and is the coboundary of . Moreover, the pair corresponding to equals if and only if is a central grouplike element of . Thus, , where is the group of invertible elements of and is the group of central grouplike elements of . Therefore, we get
Corollary 3.7**.**
There is an isomorphism of groups
[TABLE]
Let be the subgroup of co-twisted automorphisms of for which
[TABLE]
Also note that is a proalgebraic group, and is a closed normal subgroup in it. Thus, is a proalgebraic group, which sits as a closed normal subgroup in . Therefore, we have
Corollary 3.8**.**
The restriction is a surjective homomorphism of affine proalgebraic groups. Thus, we have an isomorphism of affine proalgebraic groups
[TABLE]
Proof.
This follows from Proposition 3.3, Proposition 3.6, and Corollary 3.7. ∎
3.4. Finitely dominated tensor categories and their tensor autoequivalences
Let be a tensor category, be a collection of objects of , and be a collection of morphisms between tensor products of .
Definition 3.9**.**
We say that is dominated by and if any tensor functor from to any tensor category is determined by and up to an isomorphism. We say that is finitely dominated if it is dominated by a finite collection of objects and morphisms.
Here by we mean the morphism between tensor products of corresponding to .
Remark 3.10**.**
If are rings then one says that is dominated by if for a ring homomorphism , is determined by , [Is]. Further, one says that is dominated by if this is true for each (this is equivalent to saying that the inclusion is an epimorphism in the category of rings). Note that this definition makes perfect sense if is just a subset of , rather than a subring (in fact, the notions of domination by a subset and the subring generated by are obviously equivalent). Thus, it is natural to talk of a ring dominated by a subset . Note that this is a weaker condition than being generated by (e.g., is dominated by ). Our notion of domination is a categorification of this notion, which justifies the terminology.
Proposition 3.11**.**
Suppose that is finitely dominated and tensor-generated by an object . Then is of finite type, i.e., is an affine algebraic group.
Proof.
Let be a finite set of objects and morphisms dominating . Let be the finite abelian subcategories of defined in the proof of Proposition 3.3. Let be so large that and belong to . Let be the affine algebraic group defined in the proof of Proposition 3.3, and let be the kernel of the natural homomorphism . Then for , we have for all and for all . Thus, , i.e. . Hence, , so that is an affine algebraic group, as claimed. ∎
3.5. Finitely presented Hopf algebras
Let be a Hopf algebra which is finitely generated as an algebra. This means that the category is tensor-generated by a single object . Hence, we have a natural surjective homomorphism of -bicomodule algebras .
Now assume that is finitely presented (e.g., , where is an algebraic group). This means that for some (and, hence, any) finite set of generators for there is a finite set of defining relations. In other words, the ideal is generated by a finite dimensional bicomodule , so that is the cokernel of the natural -bicomodule morphism
[TABLE]
We have . Let be the corresponding projections, .
Proposition 3.12**.**
Let be a finitely presented Hopf algebra and let be a tensor category over . Then a tensor functor is determined up to an isomorphism by , , and . That is, the tensor category is finitely dominated (by and ).
Proof.
Let be the diagrammatic additive monoidal category whose objects are direct sums of tensor products of symbols and , and morphisms are freely generated by , . Then we have a natural monoidal functor
[TABLE]
and our job is to show that is determined up to an isomorphism by the composition .
In the completion of under infinite direct sums, there is an obvious morphism such that . Hence, is determined by . Thus, so is . Moreover, let be a morphism of left -comodules. Then is given by the right action of an element of , which we will also call . Let be the endomorphism of in obtained by the right action of on the second component. By taking a direct sum over , we get a morphism
[TABLE]
in such that in . This implies that is determined by .
Now, any admits an injective resolution by multiples of :
[TABLE]
where , and is a vector space. Indeed, for any -comodule (not necessarily finite dimensional) we have a canonical inclusion ; so we may define as , where (where and ). The above argument implies that the action of on this resolution is determined by . Thus, is determined by . Further, if is a morphism in then it lifts to a morphism of resolutions , which implies that is determined by , i.e., is determined by as a functor.
Now, the tensor structure is determined by its values at . In turn, is determined by , where . Finally, is determined by . This proves the proposition. ∎
Corollary 3.13**.**
Let be a finitely presented Hopf algebra such that is tensor-generated by . Then
- (i)
* is an affine algebraic group;* 2. (ii)
* is an affine algebraic group.*
Proof.
Part (i) follows from Proposition 3.11 and Proposition 3.12. Part (ii) follows from (i) and Corollary 3.8. ∎
3.6. The second invariant cohomology of a tensor category
Given a tensor category , let be the group of isomorphism classes of tensor autoequivalences of that are isomorphic to the identity as abelian equivalences, [Da1, BC, GKa]. We will call this group the second invariant cohomology group of .
Proposition 3.14**.**
* has a natural structure of an affine proalgebraic group.*
Proof.
Let be the set of isomorphism classes of objects of . Let be the closed subgroup of the affine proalgebraic group cut out by the functoriality condition in and and the tensor structure axiom
[TABLE]
i.e., the closed subgroup in cut out by the tensor structure axiom. Also let be the closed subgroup cut out by the functoriality condition in (i.e., , a commutative affine proalgebraic group). Let be the homomorphism defined by . Then is a homomorphism of affine proalgebraic groups, is a central subgroup of , and . This implies the statement. ∎
Remark 3.15**.**
In the case , where is a Hopf algebra, Proposition 3.14 follows from Theorem 6.7 of [BKa].
Corollary 3.16**.**
(i) If is finitely dominated then the second invariant cohomology is an affine algebraic group (i.e., is of finite type).
(ii) If is a finitely presented Hopf algebra then the second invariant cohomology is an affine algebraic group.
Proof.
(i) It is clear that is a closed subgroup of , where is a tensor-generating object. Thus, the statement follows from Proposition 3.11.
Part (ii) follows from (i) and Corollary 3.13. ∎
Example 3.17**.**
Let be an abstract group, and be its group algebra. Then is finitely generated, respectively finitely presented, iff so is . Also, , the tensor category of finite dimensional -graded vector spaces. Thus, . Hence, Corollary 3.16 reduces in this case to the well known result that for a finitely presented group the group is an algebraic group, which holds due to the Serre-Hochschild exact sequence where is a finite presentation of (i.e., is a finitely generated free group). Indeed, since this presentation is finite, is the normal closure of a finitely generated group, hence is an affine algebraic group (i.e., is of finite type).
Note that if is finitely generated but not finitely presented, then this may be false. E.g., if is the Grigorchuk group [Gri], then is infinitely generated 2-elementary abelian, hence is an infinite product of copies of (a proalgebraic group of infinite type). Thus, the finite presentation assumption in Proposition 3.12 and the finite domination assumption in Proposition 3.11 cannot be dropped.
4. Tensor autoequivalences of
4.1. Finite presentation for over
Let be a simple algebraic group. Let be an indeterminate and let denote the quantized function algebra of over .
Proposition 4.1**.**
* is finitely presented as an algebra.*
Proof.
Let be a finite generating subset of the cone of dominant weights of . Let be the direct sum of all standard -comodules whose highest weights are in . Then we have an element determining the coaction of on . By [Lu3, Proposition 3.3] the matrix elements of generate . Also, satisfies the Faddeev-Reshetikhin-Takhtajan (FRT) relation
[TABLE]
where is the specialization of the universal R-matrix to (note that to define , one may need to adjoin for some , but the FRT relations contain only integer powers of ). Let be the algebra generated over by the matrix elements of with these relations taken as defining. Then we have a surjective homomorphism . By [BG, Lemma I.8.17], the algebra is Noetherian (more precisely, this lemma is proved when is specialized to , but it generalizes verbatim to our setting). Hence the ideal is finitely generated. This implies that is finitely presented, as desired. ∎
Corollary 4.2**.**
For any , the algebra is finitely presented. Also, the -algebra is finitely presented.
Remark 4.3**.**
- (1)
Proposition 4.1 also holds over (i.e., in the setting of [Lu3]), with the same proof. 2. (2)
A nice finite presentation of (and thus of for transcendental ) is given in [I].
4.2. Tensor autoequivalences of outside finitely many roots of unity
In this subsection we classify tensor and braided autoequivalences of . Here we don’t make any coprimeness assumptions on the order of , and just assume that is a root of unity of sufficiently large order .
Note that any tensor autoequivalence of naturally acts on the center of , as is the universal grading group of . Thus, for a subgroup , defines an equivalence .
Let (e.g., if is simply connected then ) and .
Theorem 4.4**.**
For all except finitely many roots of unity:
- (i)
. 2. (ii)
.
Proof.
If is not a root of unity, this is shown in [NT2] (for (i)) and [NT1] (for (ii)); more precisely, the results of [NT1, NT2] are proved for simply connected groups, but the arguments extend without significant changes to the general case. So we only have to prove the statements for roots of unity.
Let us prove (i). For a positive integer , let be the set of all nonzero dominant integral weights for such that the irreducible representation of with highest weight has dimension . If the order of is large enough, these have -analogs, -comodules of the same dimension as , which are also irreducible.
Let . We claim that for sufficiently large order of , the functor permutes , . Indeed, by Steinberg’s tensor product theorem for quantum groups ([Lu2, Proposition 9.2]), for large enough the only irreducible comodules over which have dimension , don’t belong to the Müger center of , and cannot be nontrivially decomposed as a tensor product are , . But cannot belong to the Müger center of , as it generates a subcategory of the form , while is not contained in the Müger center of . So, since by Proposition 2.12 preserves vector space dimensions, it must permute , .
Now pick so large that is a tensor generator of . Then , so . Note that we have a natural inclusion (see [NT2]). Thus, our job is to show that for sufficiently large , this inclusion is an equality.
Let , where is a nonzero polynomial vanishing at roots of unity of low order. Since by Proposition 4.1 is finitely presented, by Corollary 3.13 the commutative algebra is the specialization at of a finitely generated commutative algebra over (for all but finitely many roots of unity ). Indeed, we can take a finite presentation of the -algebra and define by the same generators and relations over (for a suitable choice of ). Moreover, since acts faithfully by automorphisms of , we have a surjective algebra homomorphism , where is the algebra of -valued functions on . Let . By Grothendieck’s generic freeness lemma [Eis, Theorem 14.4], since is finitely generated, we may assume without loss of generality that is a free -module (by choosing appropriately). Then as an -module, hence is a projective -module.
Moreover, by the result of [NT2], becomes an isomorphism upon tensoring with , hence . As is projective, this implies that , i.e., is an isomorphism. Thus, is an isomorphism after specializing to all roots of unity that are not roots of . Hence, for all such roots of unity we have an isomorphism , as desired.
Part (ii) is proved in the same way, using the group instead of , and [NT1] instead of [NT2]. ∎
Remark 4.5**.**
It would be interesting to obtain a more direct proof of Theorem 4.4 (and desirably of its stronger version, giving an explicit list of excluded roots of unity) by generalizing the arguments of [NT1, NT2] to the case when is a root of unity.
4.3. Sharper results for classical groups
For classical groups , we can use the Faddeev-Reshetikhin-Takhtajan presentations of to obtain a sharper result, i.e., one for all of order . Note that in these cases is cyclic, so .
Theorem 4.6**.**
If and then
[TABLE]
Proof.
Let us first prove that . Take the tensor generator , the defining comodule. In all three cases we have the Faddeev-Reshetikhin-Takhtajan presentation of , in which is generated by the entries of with defining relations
[TABLE]
plus some additional relations depending on which case we are considering, see [FRT, RTF, Ta, Ha].
Consider first the case . Then the additional relation is the quantum determinant relation . Thus, any braided autoequivalence of is determined by and the action of on the morphism whose image is , the quantum top exterior power of . The only -dimensional simple -comodules are and their Frobenius twists (since the set of weights of a comodule is Weyl group invariant). Then maps to or to (as tensor-generates the category, while does not). So by composing with an element of , we may assume without loss of generality that . By rescaling this isomorphism it is also easy to make sure that , so , as desired.
Now consider ( even). Then the additional relation says that preserves the morphism which deforms the symplectic form on . Thus any braided autoequivalence of is determined by and . As before, the only -dimensional simple comodules are and the Frobenius twist , and (since tensor-generates the category but does not). Thus . By rescaling this isomorphism we can also make sure that . Thus , as desired.
Finally, consider the case , . In this case, the additional relations are that preserves the morphism which deforms the inner product on , and that it preserves the morphism (i.e., has quantum determinant 1). Thus, any braided autoequivalence of is determined by , , and . Moreover, the only -dimensional simple -comodules are and , and , since tensor-generates the category but does not. So, for any braided autoequivalence of we have . Finally, we can rescale this isomorphism so that . Then since may be expressed via and hence .
Now we need to consider separately odd and even . If is odd, rescaling the isomorphism by (which preserves the relation ), we can make sure that , so . On the other hand, if is even, then we cannot do this, so we have two cases, and . But in this case we have a nontrivial involutive outer automorphism of implemented by an element of with determinant . So by composing with such automorphism, we can make sure that , i.e., , as desired. ∎
Remark 4.7**.**
-
Note that for , we have the group acting by Dynkin diagram automorphisms (hence automorphisms of ), but only a 2-element subgroup of this descends to .
-
The proof of Theorem 4.6 is similar to the arguments of [KW] for and [TW] for and .
5. Tensor autoequivalences of
Now let us classify tensor autoequivalences of . We again assume that is a root of unity of odd order coprime to if is of type , and coprime to the determinant of the Cartan matrix of .
5.1. The connected component of the identity of .
Recall that for tensor categories and a tensor functor one can define the deformation cohomology , see [Da1, Y] and [EGNO, Section 7.22]. Namely, with the usual differential, and is the -th cohomology of the complex . Then consists of equivalence classes of first order deformations of as a tensor functor. Note that if , where is a Hopf algebra over and is the forgetful functor, then , so if is finite dimensional then . In particular, for we get
Proposition 5.1**.**
One has
[TABLE]
where are the positive and negative nilpotent subalgebras of .
Proof.
As explained above, we have
[TABLE]
On the other hand, by [GK, Proposition 2.3.1] and remark thereafter, we have
[TABLE]
This implies the statement. ∎
Now we can compute the identity component of .
Proposition 5.2**.**
One has .
Proof.
We have a natural map
[TABLE]
Namely, recall that elements of are twisted automorphisms of (in the sense of [Da2]), so the map (6) attaches to a twisted derivation the class of infinitesimal twist . (Here by a twisted derivation we mean a first order deformation of the identity twisted automorphism, see, e.g., [Da3]). Thus, by Proposition 5.1 we have a map
[TABLE]
The kernel of consists of ordinary Hopf algebra derivations of , and it is easy to see that they can be identified with the Cartan subalgebra of . Thus, . Since by Proposition 2.3 we have an embedding
[TABLE]
this implies the required statement. ∎
5.2. Tensor autoequivalences of are braided
Proposition 5.3**.**
As braided tensor categories, .
Proof.
Assume that is a braided equivalence. Then induces an automorphism of and in particular of its connected component of the identity , which by Proposition 5.2 is . Since and every element of is implemented by a tensor autoequivalence in , by composing with such an autoequivalence, we may assume without loss of generality that . Then commutes with . Moreover, by Lemma 2.6, this commutativity is an isomorphism of actions. Hence, by Subsection 2.3, gives rise to a braided equivalence of -equivariantizations . But this contradicts Proposition 2.14. ∎
Now we finally obtain
Theorem 5.4**.**
Every tensor autoequivalence of is automatically braided. In other words, we have .
Proof.
By Lemma 2.5, has no nontrivial tensor subcategories. By Proposition 5.3, the category satisfies the assumptions of Corollary 2.2. Thus, Corollary 2.2 implies the result. ∎
5.3. Classification of tensor autoequivalences of
Introduce the notation We have seen that contains , and by Proposition 5.2 we have . Hence, is normal in . Given , let be the element of induced by . We can view as an element of . Then , where belongs to the centralizer of in (a finite group). Since normalizes , it acts on by conjugation. Thus, we have
Lemma 5.5**.**
.
We can now formulate one of the main results of this paper.
Theorem 5.6**.**
One has in the following cases:
- (i)
If is of a classical type (, or ) and the order of is bigger than ; 2. (ii)
If is exceptional and the order of is sufficiently large.
Proof.
By Lemma 5.5, our job is to show . There is a group homomorphism from to . By Lemma 2.6, this homomorphism admits a unique lift to an action on . Since the action of on commutes with that of , we conclude that acts on the equivariantization , which is the braided category .
Thus, it suffices to prove that the group of braided autoequivalences of coincides with . Indeed, then given , this would yield that , hence (as it acts trivially on ).
Now part (i) follows from Theorem 4.6 and part (ii) follows from Theorem 4.4(ii). ∎
Remark 5.7**.**
We expect that Theorem 5.6 holds without the assumptions on the order of .
5.4. Brauer-Picard groups
Let be a finite tensor category. Recall [ENO] that the Brauer-Picard group of is the group of equivalence classes of invertible -bimodule categories. Recall also that there is a canonical isomorphism
[TABLE]
see [DN] (and [ENO] in the semisimple case).
When is braided, its Picard group is naturally identified with a subgroup of .
Proposition 5.8**.**
Let be a finite tensor category.
- (i)
The group has a natural structure of an affine algebraic group over . 2. (ii)
If is braided then has a natural structure of an affine algebraic group over .
Proof.
Part (i) follows immediately from (7) and Proposition 3.1. To prove part (ii), recall that under isomorphism (7) is identified with the subgroup of classes of autoequivalences trivializable on the subcategory (i.e., those for which as tensor functors), see [DN]. This means that is a Zariski closed subgroup of . ∎
In this subsection we will compute the Brauer-Picard groups of and , where is a Borel subalgebra.
Let . Note that has a natural quadratic form . Let be the orthogonal group of this quadratic form. Note that acts naturally on preserving and therefore .
Proposition 5.9**.**
Under the assumptions of Theorem 5.6 one has:
- (i)
; 2. (ii)
.
Proof.
(i) It is well known that the quantum double is given by
[TABLE]
where the R-matrix is the external product of the R-matrix of with the R-matrix on defined by . Hence, is equivalent as a braided category to the category , where the braiding on the second factor is defined by . Thus, by (7), we have
[TABLE]
Now, any braided autoequivalence of must preserve the second factor, since it is the subcategory spanned by all the invertible objects. Hence also preserves the first factor (as it is the centralizer of the second one). Thus, we get
[TABLE]
Since , the result follows from Theorem 5.6.
(ii) Since the category is factorizable, one has . Thus, by (7), we have
[TABLE]
It follows from Lemma 2.5 that the only nontrivial tensor subcategories of are and , which are not braided equivalent by Proposition 5.3. Hence, any braided autoequivalence of must preserve both factors. So we get
[TABLE]
and the result follows from Theorem 5.6. ∎
Let be the Borel subgroup corresponding to , and be the image of in .
Corollary 5.10**.**
One has .
Proof.
Let be a finite tensor category. Let denote the group of isomorphism classes of invertible objects of . There is an exact sequence
[TABLE]
see [GP, MN], where the first map is induced by the forgetful functor , the second one sends an invertible object to the conjugation functor , and the third one is given by with the usual left action of and the right action of twisted by .
Now take . Then the above exact sequence takes the form
[TABLE]
where the first map is the identity. Thus, the map is injective. Hence, by Proposition 5.9(i), .
It is clear that contains the subgroup , where is the diagonal copy of . Also, one shows similarly to the proof of Proposition 5.2 (using the results of [GK]) that , hence
[TABLE]
Thus, must normalize , hence , where
[TABLE]
It remains to show that . Let , and consider the action of on the invertible objects . First of all, must permute the objects corresponding to the roots , since they are the only invertible objects which have a nontrivial with the unit object. Also, if and only if is connected to in the Dynkin diagram of (as this is exactly the case when there is no quadratic relation between and ). Thus, the permutation of induced by is implemented by an element of . Hence, composing with an element of if needed, we may assume that acts trivially on . Then . This implies the required statement. ∎
Remark 5.11**.**
Corollary 5.10 allows one to describe tensor autoequivalences of in terms of induction. Namely, given a tensor category , its indecomposable exact module categories are in bijection with Lagrangian algebras in . This bijection is given by
[TABLE]
where is the right adjoint to the forgetful functor . As usual, denotes the dual tensor category of with respect to . Furthermore, correspondence (8) is equivariant with respect to the isomorphism . Here the group (respectively, ) acts on the set of module categories (respectively, Lagrangian algebras) in an obvious way. The stabilizer of in is the subgroup of autoequivalences induced from and the orbit of consists of module categories such that [MN].
In our situation , the induction is injective, and is identified with the flag variety . Point stabilizers are identified with images of inductions:
[TABLE]
taken over module categories such that . Since coincides with the union of its Borel subgroups and all Borel subgroups are conjugate, we conclude that every (braided) tensor autoequivalence of is induced from a tensor autoequivalence of a copy of (i.e., from a central tensor functor ).
Remark 5.12**.**
The induction homomorphism and construction of Weyl reflections in are discussed in [LP].
5.5. Twists for
It is an interesting problem to classify twists for up to gauge transformations, i.e., categorically speaking, to classify fiber functors up to isomorphism. By the results of [EK1, EK2], the answer to a similar question for the quantized universal enveloping algebra is given in terms of Belavin-Drinfeld triples (see e.g., [KKSP]). On the other hand, twists for associated to Belavin-Drinfeld triples were worked out in [Ne] following the method of [EN] and [ESS]. Let us call them Belavin-Drinfeld twists, and call the corresponding fiber functors Belavin-Drinfeld functors.
Question 5.13**.**
(see also [Ne], Question 9.5) Is any fiber functor on a composition of a Belavin-Drinfeld functor with a tensor autoequivalence of ? In other words, is any twist for gauge equivalent to a composition of a Belavin-Drinfeld twist with one coming from a twisted automorphism of ?
The answer is positive for by [Mo, Proposition 8.11]. In this case there are no nontrivial Belavin-Drinfeld functors, so every fiber functor is the composition of the standard one with a tensor autoequivalence, and tensor autioequivalences form the group .
The reference list from the paper itself. Each links out to its DOI / PubMed record.
- 1[AGP] I. Angiono, C. Galindo, M. Pereira, De-equivariantization of Hopf algebras , Algebras and Representation Theory 17 (2014), no. 1, 161-180.
- 2[AG] S. Arkhipov, D. Gaitsgory, Another realization of the category of modules over the small quantum group , Adv. Math. 173 (2003), no. 1, 114-143.
- 3[Bi 1] J. Bichon, The representation category of the quantum group of a non-degenerate bilinear form , Comm. Algebra 31 (2003), no. 10, 4831-4851.
- 4[Bi 2] J. Bichon, The group of bi-Galois objects over the coordinate algebra of the Frobenius-Lusztig kernel of S L ( 2 ) 𝑆 𝐿 2 SL(2) , Glasg. Math. J. 58 (2016), no. 3, 727–738.
- 5[BC] J. Bichon, G. Carnovale, Lazy cohomology: An analogue of the Schur multiplier for arbitrary Hopf algebras , J. Pure and Applied Algebra 204 (2006), no. 3, 627-665.
- 6[B Ka] J. Bichon and C. Kassel, The lazy homology of a Hopf algebra , J. Algebra 323 (2010), no. 9, 2556–2590.
- 7[BG] K. Brown, K. Goodearl, Lectures on algebraic quantum groups , Birkhäuser (2012).
- 8[DL] C. De Concini, V. Lyubashenko, Quantum function algebra at roots of 1 , Adv. Math. 108 (1994), no. 2, 205–262.
