Filtrations on block subalgebras of reduced universal enveloping algebras
Abstract.
We study the interaction between the block decompositions of reduced universal enveloping algebras in positive characteristic, the PBW filtration, and the nilpotent cone. We provide two natural versions of the PBW filtration on the block subalgebra of the restricted universal enveloping algebra and show these are dual to each other. We also consider a shifted PBW filtration for which we relate the associated graded algebra to the algebra of functions on the Frobenius neighbourhood of in the nilpotent cone and the coinvariants algebra corresponding to . In the case of in characteristic we determine the associated graded algebras of these filtrations on block subalgebras of . We also apply this to determine the structure of the adjoint representation of .
1. Introduction
The key feature of the representation theory of algebraic groups and Lie algebras in characteristic is the linkage principle providing the block decomposition of the category of representations ([7], [13], [1], [12], [3]). In order to formulate it for a Lie algebra of an algebraic group one first decomposes the category of representations with respect to the -character and passes to the corresponding reduced universal enveloping algebra . We note here that via the differential map the case is related to the representation theory of algebraic group by the equivalence of categories , where is the Frobenius kernel of and, therefore, is of particular importance. Finally, for the block decomposition could be understood as the direct sum decomposition of algebras
indexed by certain equivalence-classes of simple -modules. In the current paper we use the PBW filtration on to study the block subalgebras .
We study three filtrations on the block subalgebra . The first two are natural ways to put a PBW filtration on , by either pushing forward the PBW filtration on by the map projecting onto or by intersection with the PBW filtration on . The shifted PBW filtration is obtained from the push forward filtration by additionally assigning the generators of the Harish-Chandra center degree .
We realize associated graded algebra as a quotient of a tensor product , where is the Frobenius neighbourhood of inside the nilpotent cone and is the coinvariants algebra corresponding to the block. For the trivial character this quotient is moreover -equivariant. We also show that the first two PBW filtrations we put on are dual to each other.
In the case of , we compute explicit central idempotents for the block decomposition of . In this case for or regular semisimple we are furthermore explicitly determine associated graded algebras of the filtrations as well as determining the structure of -representations on them for . Finally, we use this to determine the structure of the adjoint representation of . Our result agrees with the main result of [20] for the small quantum group of at the -th root of unity.
The key ingredient of our approach is understanding the structure of -representation on the algebra of functions on the nilpotent cone, which in the case of can be exploited to understand block subalgebras as -modules. In the case of characteristic the answer were provided in [16]. In the case of characteristic though the question is substantially less explored and in general only the existence of the good filtration on is known ([17], [15], §II Proposition 4.20).
This approach to the block subalgebras could possibly be applied to understanding the center of the block subalgebra. The multiplicity of the trivial -representation as a subrepresentation in or provides an upper bound on the dimension of the center of . It would be interesting to understand if this method could be used in the general case to understand .
We note that for a block containing a single simple projective module , we have . It was communicated to us by Pavel Etingof that even in the characteristic case the pushforward of the PBW filtration onto for simple modules is not well-understood, despite it being an important problem.
Notation. Throughout, will denote an algebraically closed field of characteristic . We let be the Frobenius twist of an affine variety over , where is a scheme with -algebra structure on given via . We equip this with a map arising from the universal property of the fibre product and the absolute Frobenius .
By an algebraic group we will mean a linear algebraic group, so that as a variety it is affine. We put for the Lie algebra of . We use to denote the universal enveloping algebra, and to denote the reduced universal enveloping algebra for . There is an adjoint action of on induced by the adjoint action of on . For , the map is -equivariant, as we have . This yields a -action on .
We use for the categories of representations of and respectively. We put for a Cartan subalgebra, which we assume to be fixed, and for the corresponding Weyl group. We put to denote the dot-action on the weight lattice and : , with being the sum of fundamental weights.
For a graded vector space , we write for the degree component. We set .
2. Background
This section will cover the background material on the block decomposition for . We will begin with general background, and at the end of the section discuss how these results present themselves in the case . For further details we refer to [15], a good summary of the results is also presented in [4].
2.1. Structure of the center
Let be a semisimple connected simply connected algebraic group. Assume that the characteristic of the field is ‘very good’ as in [19]. Throughout the paper, we will need to understand the structure of the center of and its image under the quotient map to .
Definition.
To describe the center , we will need two subalgebras of :
-
·
We set to be the -center, where the collection of elements is a basis of the Lie algebra as a vector space.
-
·
We set to be the subalgebra of -invariant elements in under the adjoint action of on , which is called the Harish-Chandra center.
Under our assumptions we may write the center down explicitly using the following theorem:
Theorem.
We have
where elements of are the -invariant elements in the -center.
Proof.
See Theorem 2 of [19]. ∎
Furthermore, we may make further characterizations of and - the Harish-Chandra isomorphism allows us to understand -invariant elements through the Cartan subalgebra .
Theorem.
We have an isomorphism
Moreover, the center is a polynomial algebra for a set of generators (). Furthermore, upon restricting to we get an isomorphism
The map is the Artin-Schreier map.
When considering the image of in , we may use these results to understand this as well.
Lemma.
The image of the in is given by
where is the 1-dimensional algebra over induced by the character .
Proof.
This follows from applying the quotient map to . ∎
2.2. The block decomposition
Suppose is a reductive algebraic group. We may decompose as a direct sum of smaller categories, which creates the block decomposition that we study. Before stating this decomposition, we need to define the notion of a Serre subcategory.
Definition.
Let be an abelian category. A Serre subcategory is a non-empty full subcategory so that for any exact sequence
where if and only if .
Proposition 1.
Let denote the weight lattice of , be the subset of positive weights, the affine Weyl group, and the -dilated dot action of . We have a decomposition
Here, is the Serre subcategory generated by simple modules for in .
We note that when we refer to we fix a fundamental domain for . This applies to all other block decompositions as well. When explicitly needed, we will give a description of this fundamental domain.
The similar results hold for .
Proposition 2.
Let denote the weight lattice of , the finite Weyl group, and the dot action of . We have a decomposition
Here, is the Serre subcategory generated by the simple modules for in .
In the case for , we say that are -linked. Letting be a character of , we may pass to the reduced universal enveloping algebra
Through the universal property of , we have a bijection
This restricts to -modules when we consider -modules with -character .
Restricting the result of Proposition 2 to the subcategory of -modules with a given character -character , we obtain a block decomposition of . The simple modules in are constructed as the quotients of the so-called baby Verma modules given by . It is known that all simple -modules arise in this way, see [12].
We have a block decomposition in this case, which is simply an algebraic fact. One may define a linkage relation among principal indecomposable modules for , as in [7] §55.
Theorem 1.
We have a decomposition
where is the two-sided ideal of equal to the sum of all principal indecomposable modules belonging to an equivalence class under the linkage relation.
Proof.
See [7], Theorem 55.2 in §55. ∎
The blocks can again be viewed as Serre subcategories for corresponding simple modules. In the case of , we know this decomposition explicitly because there is a complete understanding of the baby Verma modules and simple modules for any character .
A more precise result is an explicit description of the blocks in terms of -linkage classes. We may explicitly characterize the blocks by the associated baby Verma modules. We assume is semisimple, and define a modified weight lattice as in [14] §6.2 via
We have . This will index all of the baby Verma modules .
Theorem 2.
For , the blocks of are in natural bijection with the -linkage classes of weights in .
Proof.
See [3] §3.18. ∎
We note that the Harish-Chandra center of and, in particular, the elements , act by a constant on the simple modules within a given block. For this action uniquely determines the block and thus we will sometimes refer to the block by the constant by which the generator of the Harish-Chandra center acts on the simples in the block.
It is worth noting that in characteristic , the differentiation functor
induces an equivalence of categories between and -modules, so in this case Theorem 2 is an immediate consequence of a block decomposition on . Here, is the kernel of the Frobenius twist . This illustrates the connection between the two block decompositions.
Given this block decomposition, we may decompose the algebra into blocks associated to each Serre subcategory. In particular, we may write
where nonzero element if it acts nontrivially on and trivially on all the other subcategories in the decomposition of Theorem 2.
For any decomposition of an algebra into direct summands, there exists a corresponding collection of central idempotents. In particular, the decomposition can be written as
where are central idempotents. Note that due to the result of [11], the central idempotents of lie in the image of the center of . This allows to interpret the projection maps onto each block as multiplication by .
Remark.
By abuse of notation we will refer to the projection maps onto blocks as well as the central idempotents in the above decomposition by .
Recall from the introduction that there is a natural -action on induced by the adjoint action of . Since the central idempotents are -invariant, the corresponding projections are -equivariant and the adjoint action preserves the subalgebras .
2.3. Representation theory of and
In this subsection, we briefly review the representation theory of and in characteristic . A good reference for this is [18]. This is also summarized (on a less detailed level) in [12] and [14]. Throughout this subsection, we will need for these results to hold.
The flag variety of is . This group has weight lattice and . We construct representations of known as Weyl modules - these are defined as . We can identify this with
where are homogeneous coordinates for and the subscript denotes the degree part of the grading on . We note that are indexed by and the Weyl modules are defined for a general reductive algebraic group in a similar fashion.
Lemma 1.
For , the module is simple. For , it is no longer simple, with simple socle . We have
As a submodule of , we may embed as .
Next, we discuss the representations of . We first need to choose a basis, which will be fixed for the rest of the paper.
Definition.
Let , , and . These form a basis for , and have the relations
Because we assume , the trace form is non-degenerate and hence we have . Thus, when classifying characters we may consider the associated elements in . We may divide them into three categories, up to conjugacy by :
Lemma 2.
We may divide the characters of into three cases up to conjugacy:
-
(1)
.
-
(2)
but nilpotent. We pick as a representative.
-
(3)
regular. We pick with as a representative.
For each of these cases, we have a corresponding classification of simple modules, or simple -modules with -character . To distinguish from the notation for -modules, we add the subscript to denote which character we are using. We state with these the grouping into different blocks following Theorem 2.
Lemma 3.
We have three cases for the simple modules corresponding to Lemma 2.
-
(1)
When , there are nonisomorphic simple modules for which are quotients of the baby Verma modules via the exact sequences
We group together in the block decomposition for , meaning we have a single block at with a single simple module at called the Steinberg module and blocks with two simple modules.
-
(2)
When , all of the baby Verma modules are simple. We have non-isomorphic baby Verma modules. We have over . Each block has a single simple module.
-
(3)
When is regular, we have all simple over roots of and they are non-isomorphic. In the block decomposition, each block has a single simple module.
In our computations, we will also need some understanding of the projective covers of .
Lemma 4.
We have three cases.
-
(1)
: Each simple for (as in Lemma 3) has a projective cover. The simple module is the unique simple projective, and every other has a dimension indecomposable projective cover with composition factors .
-
(2)
: Each has an indecomposable projective cover of dimension which is a self-extension.
-
(3)
: Each simple module is projective.
Proof.
See §13 of [12]. ∎
The representations of and are related by differentiation functor in the following way.
Lemma 5.
We have for , and is a trivial representation so that in general
Proof.
See [18] §2.4. ∎
Using the following lemma, we can determine bases for and write down the kernel of .
Lemma 6.
For any character , we have for as a basis for . Depending on the character, we have three possibilities for the ideal .
-
(1)
For , it is .
-
(2)
For , it is .
-
(3)
For , it is .
Finally, we discuss the center of . As discussed above, this is generated by and . The lemma above essentially tells us the form of . As for , we observe that for the Cartan subalgebra is simply the span of . Then we have , and thus
The finite Weyl group for is isomorphic to , and the dot action sends . Thus, is isomorphic to , and has a single generator. For our convenience we will denote by .
Lemma 7.
Under the Harish-Chandra isomorphism for , the element maps to in .
This result tells us that for is . This is not the usual quadratic Casimir element for , but rather . For the convenience of notations and computations we shift it so that it vanishes at the fixed point of the -action.
3. Filtrations on block subalgebras
3.1. Filtrations of interest
We will be discussing three filtrations of interest in this section. First, recall the definition of the PBW filtration.
Definition.
The Poincaré-Birkhoff-Witt (PBW) filtration on is the filtration with given by the degree elements with the degree induced from the tensor algebra.
If we choose a basis of then we have monomial basis of as a vector space over by the PBW theorem. Then is the subspace of spanned by elements with . The filtration is compatible with multiplication in a sense that and is uniquely characterized by this property together with . It is also preserved by the adjoint action of on . Finally, for the associated graded algebra of this filtration we have an isomorphism .
We obtain a filtration on by applying the quotient map to each vector space in the filtration. From this point onward, we will denote this PBW filtration on by . The associated graded algebra of this filtration is isomorphic to , where is the Frobenius neighbourhood of inside , which is defined to be the preimage of under the Frobenius map . Inside it is given by the ideal generated by the elements , where runs through a basis of .
Definition 1.
There are two natural ways we put a filtration on a block :
-
(1)
The pushforward PBW filtration is given by .
-
(2)
The intersection PBW filtration is given by .
We note that both filtrations are compatible with multiplication and the pushforward filtration is uniquely characterized by this together with and .
The last filtration we consider is a shifted PBW filtration.
Definition 2.
This last filtration is also compatible with multiplication and is uniquely characterized by this together with .
The associated graded algebras for these on are denoted by respectively. Finally, note that for all three filtrations as well as are preserved by the -actions.
3.2. The shifted PBW filtration and the nilpotent cone
In this subsection we study the relation between the nilpotent cone and the associated graded algebra of with respect to the shifted PBW filtration .
Throughout this subsection, we let be a semisimple connected simply connected linear algebraic group with Lie algebra . We additionally impose the following assumptions on :
-
(1)
The derived group of is simply connected.
-
(2)
is odd and a good prime for (as in §2.1)
-
(3)
The Killing form on is non-degenerate.
Recall that is the intersection of all normal algebraic subgroups so that is commutative. It can be viewed as the algebraic group analogue to the commutator subgroup . With these conditions on , we may use the relevant results for - we note that for , all these conditions apply, so any theorems of this section may be used for in characteristic .
Definition.
By abuse of notation we identify generators of the Harish-Chandra center with their image in the associated graded algebra . We define the nilpotent cone to be a closed subscheme of considered as an affine space.
Under our assumptions on the set of closed points of is the set of nilpotent elements of (see for example Theorem 2.6, [9]). Note also, that the adjoint -action preserves .
As we work in characteristic , we have a morphism
We define the Frobenius neighborhood of in , denoted by , to be the preimage of a point under this map. This can be written as .
For this subsection, we fix a block throughout. Let be the constant by which the generator of the center acts on the simple modules associated to the block .
We put for the image of the center of in , which is known as the algebra of coinvariants.
For a root of let be a corresponding root space. For a positive root of we let to be the unique element of so that (recall ). We now have the following lemma, which is a combination of results from [19] and [3].
Lemma 8.
The algebra is a local ring. Moreover,
-
(1)
For nilpotent, assigning degree to the elements provides a grading on .
-
(2)
We have if and only if we have , such that for all simple roots . In particular, we will endow it with the trivial grading.
Proof.
Let denote the weight lattice of . Let be the stabilizer of under the action of the finite Weyl group , and the stabilizer of , consisting of so . Given , is a character of the Frobenius twist . As discussed in [19], this th power has a Jordan decomposition . In particular, by the result of [19] and the discussion of §3.8 in [3] we have an isomorphism
As fixes this will be a local ring. Now further suppose is nilpotent. This identification shows that the algebra of coinvariants is graded because in this case. Explicitly identifying generators, we see that the grading is the degree grading in .
The second case follows from the theorem of §3.10 of [3], since the condition of part (2) of the theorem is equivalent to the algebra of coinvariants being . ∎
Remark.
For a regular semisimple character each block satisfies the condition of case (2) of the Lemma. The singular block (stabilized by the -action) satisfies the condition of case (2) of the Lemma as well.
In either case, the above Lemma implies that the inclusion after passing to associated graded algebra becomes an injective map of graded algebras. In the situation of case (2) we have , since the coinvariant algebra is trivial and so is a scalar element of .
Since we have , there is a well defined map . Note that, since is semisimple, the images of the central elements have smaller degree with respect to the shifted filtration then with respect to pushforward filtration and, thus, the image of the ideal in lies in the kernel of the map. It follows that the above map quotients through since . We then obtain a map
Furthermore, recall from the end of §2.2 that if there are -actions on and and the map is -equivariant and then so is the map .
Putting these maps together, we obtain a map from to . We may then show the following theorem.
Theorem 3.
Assume we are in either case (1) or (2) of Lemma 8. We have a well defined surjective map
of graded algebras. In particular, in case (2) of the above Lemma, we get a surjective map
Furthermore, for the map is -equivariant, with the -action on defined to be trivial.
Proof.
It remains to prove the surjectivity. The algebra is generated by the images of and in it. The first ones lie in the image of and the second ones lie in the image of as degrees of are bigger then and so . ∎
Given that is by definition a quotient of a polynomial -algebra , we may interpret its spectrum as a subscheme of the affine space . Given that and hence are affine schemes, we can interpret the tensor product as a fibre product of these schemes. The surjection onto the associated graded algebra tells us that
can be realized as a closed subscheme of . Note that for case (2) of Lemma 8 is a point and for a nilpotent character it is the spectrum of a local ring, so it has a unique closed point.
Let be the set of minimal coset representatives for the subgroup (the stabilizer of ). By [3] §3.19, we, in addition, know the Hilbert series for , namely
In particular, we have .
In the case of the scheme is equal to or , with being either or a first order thickening of it. Geometrically, we aim to explicitly describe the ideal sheaves of as subschemes in the case of . This is the same as determining the kernel of the map in Theorem 3, which in the case is -invariant. Once we decompose the ring of functions on the nilpotent cone into -modules we may compute as a -module.
3.3. Duality between pushforward and intersection PBW filtrations
In this section we show that the filtrations and have a simple relationship, allowing us to only focus on the pushforward filtration.
The precise relation between these filtrations requires us to provide a non-degenerate associative bilinear form
In [2], the case is treated. In [10] it is generalized to arbitrary . We will sketch the construction of this bilinear form in the following lemma.
Let be a basis for , so for form a basis for . We define as the span of where the are not all . The bilinear form constructed in [2] is defined as , where the linear map is given by and . The same definition works in the general case.
Lemma 9 ([10]).
There exists a non-degenerate associative bilinear form
Proof.
We claim that there is a -bilinear pairing
defined via the pairing on . The algebra is known to be a free module over as a consequence of the PBW theorem (see [14]). The elements for form a basis for as a -algebra. Define a lifted map in the same way as , as the -linear map given by
We define the pairing as . The same argument as in [2] is applicable and shows non-degeneracy and associativity.
Let be the one dimensional -algebra determined by the character (as a map ). Noting that , upon a base change we see induces the desired pairing on any . ∎
If we let and be as in §3.1 we have a filtration of length on
Here, denotes the trivial vector space. From the competibility of the filtration with multiplication and the definition of the bilinear form we see that
where denotes the orthogonal complement with respect to .
Additionally, suppose we have a block decomposition . The are mutually orthogonal with respect to the algebra structure of , and hence we deduce that the bilinear form restricts to which is still a non-degenerate associative pairing. We denote the orthogonal complement in with respect to by .
Theorem 4.
Let for some . Then is also a term of the PBW-filtration, and
In particular, we have .
Proof.
The assertion is equivalent to . We have
Now we recall that the map is a projection map as it is a central idempotent, and also that the kernel is precisely . This is due to the definition of , since if we have . Thus, we have .
Since we have
Knowing the kernel of , the left side is . Thus . ∎
Due to this result, it suffices to study just one of the filtrations of Definition 1. In what follows we understand the pushforward filtration using its relation to the shifted filtration.
4. The case of
Notation. Throughout this section we will refer to the block by the action of the central element (defined by Lemma 7) on the simple modules in the block, which is a constant we denote by (similar to the of §3.2). We also assume throughout.
4.1. Central idempotents
We start by providing explicit formulas for the central idempotents corresponding to the block and defining the projections . In order to do this, we compute the image of in . We will denote this image by .
Proposition 3.
We have
-
(1)
When or the image of the center is
-
(2)
When the image of the center is
Proof.
By results of 2.1 we have
We identify with via Lemma 7. As this is a PID we need only find the relation induced by the tensor product. We may identify
Knowing this, we see that once we expand we get the relation in case (1) of the proposition. Using our preimage of the generator , once we reverse the Harish-Chandra isomorphism we get for the center.
In the same way in case (2) we get the relation for since acts by on , and hence
∎
Now we are ready to compute the central idempotents for the block decompositions of .
Theorem 5.
As in Proposition 3, we have two cases for the central idempotents of the block decomposition:
-
(1)
Set . When or , the block decomposition becomes
where and for a quadratic residue modulo .
-
(2)
Set for . We have for the block decomposition
where , where is a normalizing constant so that .
Here, we abuse notation by writing the idempotents as elements of , and then passing to or to obtain the actual idempotents.
We will break the proof of this theorem into several parts.
Lemma 10.
Dividing by cases in Theorem 5, we have:
-
(1)
When or , if is a square and we view as an element of then unless , in which case we get .
-
(2)
When for and is a root of , we have unless , in which case we get .
Proof.
We begin with case (1). A helpful observation in this case is that already factors completely over as . Then we have
and so for any nonzero square we get . At we get a product of squares of quadratic residues. This is , because by Wilson’s theorem. For , we can use the factorization to obtain
Obviously, this implies the value is at any square not equal to . Note that as a polynomial in we have
This is equal to . This can be computed explicitly over and the value at is , and so reducing to we see that the value is equal to .
In case (2), by definition and all roots have multiplicity . The statement now immediately follows from the definition of and . ∎
Lemma 11.
The elements in all cases are central idempotents, and .
Proof.
By construction are central. Consider first the case or .
Let us check . For , we observe that
Reducing modulo and repeatedly applying this relation we get . Thus, . Using a similar reduction method, we can show is idempotent.
Now we show . We claim that this relation holds already in . By the previous lemma, as a polynomial in the element on each quadratic residue modulo has value . For nonresidues and any we have
To see this, note that in for a nonresidue we have . This gives the claim for . The rest comes from the relation , since upon pulling this factor into the product in the factorization of we get . We conclude that
Hence, we may deduce that is a polynomial of degree which is constant on the set of quadratic residues and on the set of nonresidues modulo . The bound on the degree holds because we know that the leading coefficients of the sum to in .
Due to its degree, the residue modulo is uniquely determined. By the Chinese remainder theorem, its residues modulo uniquely determine the result. That is, we have
Now evaluating on a quadratic residue gives , so . We can evaluate at to get the constant term as , so we force . This implies as desired.
Since in case (2) the polynomial has simple roots the claim follows from the previous lemma and the Chinese remainder theorem. ∎
We may now prove the theorem.
Proof of Theorem 5.
The previous lemma shows that in any case the are central idempotents. It is easy to check that they are mutually orthogonal (via Proposition 3), and since they sum to they define a direct sum decomposition
What remains to check is that this is indeed the block decomposition. For a block corresponding to , by definition the action of on the simples in the block is equal to . It follows that for a constant the action of is invertible on the block, by the definition of the Serre subcategory. We claim that acts by on this block, where is the degree of the factor in . Indeed, the action of on the object in the block is equal up to the invertible element to the multiplication by but on the other hand it is by Proposition 3. Alternatively, this may be seen from the construction of Theorem 1, because the action of is on the indecomposable projective covers for the block (see Lemma 4).
It follows that vanishes on the blocks other then the one corresponding to . We conclude that . The statement follows by a dimension argument. ∎
An immediate corollary of Theorem 5 is an understanding of the algebra of coinvariants for every block, as we now know the maps and the image of the Harish-Chandra center explicitly.
Corollary 1.
We have two results corresponding to the cases of the previous theorem.
-
(1)
For or , the algebra of coinvariants for the block (indexed by squares in ) is for and for .
-
(2)
For regular, the algebra of coinvariants for (indexed by roots of ) is .
Proof.
The statement follows immediately from the fact that . ∎
This is consistent with Lemma 8, since these are all local rings and graded (all characters of are either regular or nilpotent). We also conclude that for regular , and for or it is and for .
4.2. Determining the associated graded algebras
Throughout this and next sections we will assume unless the opposite is specified explicitly.
Recall that under this assumption Theorem 3 provide an -equivariant map
We determined in the previous section. Let us now describe as a representation of and a graded algebra.
Consider a matrix in . It lies in the nilpotent cone if and only if , which happens if and only if . Thus, we have
Recall that the Frobenius neighborhood of the nilpotent cone, , is defined as the preimage of under the map . Thus, for we can write
There is an -action on via the adjoint action on . This induces an action on , and the structure sheaf becomes an equivariant sheaf for this action so that itself is an -module. The action is compatible with the degree, so we may decompose the degree component of as an -module.
Proposition 4.
We have
for , and for through (inclusive) it is or after this point. That is, the dimensions of graded components in the associated graded algebra are
so that .
Proof.
The ideal is concentrated in degree . Hence, for the graded components of are the same as in . We claim these are .
Consider the isomorphism
where act by scalars, given by . It is compatible with the -action and preserves grading up to rescaling by . The -invariants on are exactly even graded components, which are as -representations.
In degree the elements generating the kernel ideal of the map form a -submodule . For , we have an exact sequence
The isomorphism follows via Lemma 1 and this simple submodule is precisely the image of multiplication of the elements in by the generators of the ideal. Hence we conclude
for in this range. At , we have an isomorphism
since the dimension of the left side is and the map is an inclusion. Hence, the graded components are from this point onward. ∎
Remark.
In characteristic the description of the -representation structure on for general is provided in [16]. In particular, for the description is identical to ours.
Consider a block subalgebra of . We put simply for the ideal To understand the map
we will use a map and the multiplication by map
which is well defined since and shifts degree by . We note here that the grading on the ideal is given by intersecting the ideal with the filtration on .
Lemma 12.
We have a surjective map -equivariant map
When , this is still well-defined and surjective but need not be -equivariant.
Proof.
This is a direct consequence of Theorem 3 and its proof. ∎
In terms of the generators the above map is given explicitly by
where we put the overline to denote the image of the element in and then passing to the associated graded algebra. Note that the images of generate , so this map is surjective.
In the case of for the trivial character, we know by Corollary 1. Thus, . The following theorem shows in the rest of the cases that this and the multiplication by maps together suffice to understand the map of Theorem 3.
Theorem 6.
Fix a block for or as in Lemma 2. with algebra of coinvariants . Consider the surjective map
of Theorem 3. A pure tensor for homogeneous is in the kernel when is in the kernel of . A pure tensor for homogeneous is in the kernel if is in the kernel of the composite map
This describes the kernel restricted to and . The kernel is a direct sum of these kernels as vector spaces.
Proof.
From the construction of the map and the proof of Theorem 3 it follows that the image of does not intersect the image of the ideal in the associated graded. This implies the assertion about the elements .
By construction of the map, the element in the coinvariants algebra maps to the image of in the associated graded. Then maps to the image of under
and assertion about such elements follows.
The restrictions of the kernel to and do not intersect and generate the kernel. This yields the splitting. ∎
We apply Theorem 6 in the case of and , because here we can exploit the -invariance of the kernel to compute it. With this theorem, we have reduced the problem to understanding the multiplication by maps and the map . We will understand first.
Lemma 13.
Let . In , we have
where we pick such that and .
Proof.
We may decompose the block subalgebra into indecomposable projectives over itself as , since it is Artinian (it has finite dimension over ). Each of these will be a projective cover of a simple module. On each , the image of multiplication by will be an irreducible module so that or , where is a simple module for . This follows from Lemma 4 and that annihilates the baby Verma modules in the corresponding block.
There are two isomorphism classes of projective covers for simple modules of , which are related to each other by the action of the Weyl group ([6], appendix). This action preserves , so if on one isomorphism class it is on the other. As it does not act by on the block and has a nontrivial kernel, we conclude . We know there are two such simple modules up to isomorphism via the block decomposition, namely and . Then in either case , from which the identity follows. ∎
Lemma 14.
Resume the notation and assumptions of the previous lemma. We have and an isomorphism
Proof.
We start by constructing a map
We may again make a direct sum decomposition into indecomposable projectives . This shows where are simple -modules which are either or . The multiplicity of each equals their dimension by the results stated in [10], and hence .
These are both simple modules for due to being simple -modules - we may explicitly define the action of an element of through the corresponding action under the multiplication by map on . These are all the simple modules for because they are the only simple modules for .
Now we show the map is an isomorphism. The simple -modules are projective because they are direct summands of . Then all of the simple modules are projective, which implies that is a semisimple algebra. The claim follows from the Artin-Wedderburn theorem. ∎
Remark.
These observations will allow us to obtain the following result.
Proposition 5.
Proof.
In degrees we identify all graded components with simple -modules in in Proposition 4. Because the kernel can be checked to be -invariant by Lemma 12, if there is a nontrivial kernel in some degree then the kernel includes all degrees .
Now we show the map of Lemma 12 is an isomorphism in degrees below . If there was a kernel in degree below , this would yield a nontrivial kernel in degree so that we get the simple quotient of in the image.
Note that is generated by its first graded component and, thus the multiplication map from is surjective on the -th graded component. On the other hand the -th graded component is a quotient of , which is an irreducible -representation and consequently vanishes.
We deduce that a nontrivial kernel in degree yields vanishing in degrees . By dimension count we see that . This contradicts our earlier dimension findings in Lemma 14, so in degrees below the map of Lemma 12 is an isomorphism. Thus, we deduce that is for some . Determining this amounts to computing the dimensions of both objects as vector spaces over .
We first consider the case of . The block has dimension . Using identification and Lemma 14, we conclude that the dimension of is
This expands as . At this is maximized, and matches the dimension of . Picking to correspond to each block, we see that having for our block means .
In the case of , the block corresponds to generated by a single simple projective module and has dimension . The result follows from Proposition 4 by summing the dimensions up to degree to get . This yields the claimed decomposition for . ∎
Remark.
For and , a block in this case is isomorphic to so it has dimension . Additionally, by Corollary 1 we see that in , so this tells us the algebra structure of a block as a quotient of if we understand the kernel of Lemma 12. In this case, one may explicitly argue there is no kernel in degrees below . It is sufficient to check this for the map induced by . From the block decomposition we know precisely which elements are annihilated by , so we can conclude the injectivity in degrees below . We then know that injects into , and as it also has dimension this is an isomorphism of algebras.
Next, we use Lemma 13 to deduce the structure of for . When , we note this is trivial by Corollary 1.
Proposition 6.
Let . We have
Proof.
We have a surjective map
This is because the map of algebras is surjective and respects the filtrations. Thus, we indeed have a surjective map on the associated graded algebras. It is also a map of graded -representations, since is invariant under the adjoint action of .
In terms of degrees, since we are in the context of the shifted PBW filtration this sends
We have a map for as for in this range. As a result, the image in the degree components for in this range may be written as quotients of . Using -invariance, they are then either , or .
We showed in Lemma 13 that we have in . We deduce that starting at the degree the kernel of
is nontrivial. By the same argument as in the first part of the proof of Proposition 5 as the nontrivial kernel in degrees below yields vanishing in degrees starting from .
As a result we have a surjection
of -modules. By summing up the dimensions of the summands the dimension of the left handside equals to . From the Weyl modules, we get and from the simple modules, we get : starting at , we get the odd numbers starting at for the dimensions. The above lemma shows this is exactly the dimension of , so we conclude this is an isomorphism of -modules and the statement follows.
∎
These results additionally allow us to write down the -module structure of when . Combined with Theorem 6 we may also describe the algebra structure.
Corollary 2.
As an -module, is a direct sum of -modules for each graded component where
This also determines the dimensions of each graded component. For the algebra structure, we have two cases:
-
(1)
Let . Then .
- (2)
Proof.
We know that we have an exact sequence of graded vector spaces
We claim that it splits as the sequence of graded -representations. From Proposition 1 we know that representations from different blocks do not have nontrivial extensions between them. We observe that on each graded component modules in and lie in the different blocks with the exception of the degree component because of the shift in indexes induced by surjective map between them. In degree , we have (by [5]) so we must have a direct sum in this case.
Now let us consider the claims about the algebra structure. In case (1) we have by Corollary 1 and the claim follows from Proposition 5. Now we consider the claims about generators in case (2). The map is the composite map
The first map has kernel generated in degree by Proposition 5 and the second map has kernel generated in degree by Proposition 6. The rest follows from Proposition 5. ∎
Remark.
We observe that as a subrepresentation of for the trivial module occurs with the multiplicity . This provide an upper bound on the dimension of the center , which is known to be exact in this case.
Two of these dimension comes from . The third copy of appears as the image of in degree .
Through the methods similar to the above one may also describe the pushforward filtration.
Proposition 7.
We have an exact sequence
where and . As with the shifted PBW filtration, as an exact sequence of -modules this splits in each degree.
Proof.
The existence of such an exact sequence is clear, since we induce this by passing to the associated graded algebras as the maps in the corresponding exact sequence of algebras respect the filtration .
The first claim holds because these two filtrations agree on the quotient. The second claim about follows the exact same argument, except the multiplication by map shifts the degree by instead of and as a result just shifts components in the associated graded algebra.
By the same method as with , the block decomposition tells us that there are no nontrivial extensions of -modules appearing in the exact sequence of Proposition 7 so we understand the structure as an -module. ∎
Remark.
By virtue of Theorem 4, we also understand the dimensions of graded components of .
Example.
Let , and suppose . The following table summarizes the dimensions as computed by Proposition 7 for on the blocks of dimensions and .
First, we consider . We let denote the trivial vector space.
0 | 1 | 2 | 3 | 4 | 5 | 6 | … | |
---|---|---|---|---|---|---|---|---|
1 | 4 | 9 | 16 | 25 | 25 | 25 | … | |
1 | 4 | 10 | 20 | 34 | 49 | 50 | … | |
1 | 4 | 10 | 20 | 34 | 45 | 50 | … |
For , we get the dimensions of the filtration on which are the squares. The other blocks have contributions from both graded algebras in the exact sequence. Next, we put down the dimensions for .
5 | 6 | 7 | 8 | 9 | 10 | 11 | 12 | ||
---|---|---|---|---|---|---|---|---|---|
0 | 0 | 0 | 0 | 9 | 16 | 21 | 24 | 25 | |
0 | 0 | 1 | 16 | 30 | 40 | 46 | 49 | 50 | |
0 | 0 | 5 | 16 | 30 | 40 | 46 | 49 | 50 |
As can be seen, the dimensions in the two tables sum in pairs to the total dimension of the block due to Theorem 4.
Let us discuss the algebraic structure of . Due to the projection , we have a map
We wish to determine the kernel of this map using our previous results. By Proposition 5, when we already understand the kernel is generated by the degree component along with because we may write this as the composition
For and the kernel is generated by which has degree and elements in degree and . The additional comes from now having degree two and shifting degrees in Proposition 6, as discussed in Proposition 7. We can see this using the diagram
where the bottom map has kernel generated by and elements in degree . Through our understanding of the all maps besides , we deduce the stated kernel.
4.3. The adjoint representation
Having computed the structure of and as -modules for , we can use these results to determine the structure of the adjoint representation for . We define it as the result of applying the differentiation functor to the adjoint action of on . More explicitly, we extend the adjoint representation of to via the Leibnitz rule, and consider the corresponding -representation.
Proposition 8.
As an -module we have
where is an indecomposable -module, such that for projective modules of Lemma 4.
Proof.
Recall that we have
in this case. Note that among the presented Weyl modules only pairs of and lie in the same block as -representations and can form a nontrivial extension. We aim to show that when possible, we do have a nontrivial extension in this decomposition.
Note that as an -representation. In particular, it is a projective -module. Since, indecomposable projective -modules have dimension or , extensions between and are all necessarily nontrivial and, hence, the same is true for and . We identify the corresponding projective -module as being exactly by noticing that its socle is equal to the socle of , which in turn equals to for .
∎
The following lemma allows us to extend the calculation for this block to other blocks for the trivial character.
Lemma 15.
In , the -submodule is independent of , where the bar denotes reduction modulo .
Proof.
We have a map
which after passing to the associated graded algebras for the PBW filtration and pushforward PBW filtration on provide a map
The quotient is identified with as an algebra and -module and, thus, we know that the second map is isomorphism in degrees below . It follows that the first map is also an isomorphism in degrees below .
Note now that the algebra is free as a module over its Harish-Chandra center . By the definition acts trivially on . It follows that the -module structure on does not depend on . This implies the claim. ∎
Corollary.
There is an isomorphism of -representations .
From this, we may deduce the -module structure of both and .
Proposition 9.
For all , we have a decomposition of -modules
For when , we have a decomposition
Proof.
The result on can be deduced by using Proposition 5. In degrees we have a projective -submodule, which, hence splits off as a direct summand. Remaining simple -modules belong to different blocks and, hence, do not have nontrivial extensions between them. It remains to observe that .
The decomposition of comes from applying the multiplication by map to . By Proposition 6 we know that in degrees it is an isomorphism. Hence for the modules map isomorphically from onto its image in . The resulting sum is a projective module and consequently splits off as a direct summand. In degrees the multiplication by map is not an isomorphism, and so we are left with a collection of simple modules for with two copies each as possible subquotients. Different such modules belong to different blocks and, therefore, have no nontrivial extensions. The two copies of appear as a direct sum because prior to applying the modules appear as a direct sum as they have no nontrivial extensions by [5]. They lie in different blocks than the other -modules which appear, and so each remaining simple enters the module as a direct summand. ∎
Lemma 16.
For as an -module, we have
Proof.
As seen above there are surjective morphisms of -representations
Let be the kernel of the composition.
Consider a short exact sequence of -representations
As is a projective -module the sequence splits.
Note further that we know that the projection quotients through with mapping onto . Hence we also have the splitting of the sequence
and the statement follows. ∎
With these results, we have now determined the structure of as a direct summand in the adjoint representation of .
Theorem 7.
The structure of a block as an -module. For the adjoint representation is the direct sum of the two components in Proposition 9.
Proof.
Follows from the previous results. ∎
Remark.
The decomposition matches with the decomposition of the adjoint representation for the small quantum group at the th root of unity established in [20].
5. Acknowledgments
The authors thank Roman Bezrukavnikov for introducing the problem and many helpful suggestions. The authors are grateful to the MIT SPUR program and its organizers and, especially, its advisors Ankur Moitra and David Jerison for helpful conversations. The first author was funded by RFBR, project number 19-31-90078.
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