Quantum generalized Kac--Moody algebras via Hall algebras of complexes
Jonathan D. Axtell, Kyu-Hwan Lee

TL;DR
This paper constructs an embedding of quantum generalized Kac--Moody algebras into Hall algebras of complexes, addressing challenges from infinite-dimensional projectives by focusing on finitely-presented representations and complexes with finite homology.
Contribution
It introduces a novel embedding of quantum Kac--Moody algebras into Hall algebras of complexes, overcoming issues related to infinite-dimensional projectives.
Findings
Established an embedding of quantum Kac--Moody algebras into Hall algebras.
Developed methods to handle infinite-dimensional projectives.
Connected representation theory with Hall algebra structures.
Abstract
We establish an embedding of the quantum enveloping algebra of a symmetric generalized Kac--Moody algebra into a localized Hall algebra of -graded complexes of representations of a quiver with (possible) loops. To overcome difficulties resulting from the existence of infinite dimensional projective objects, we consider the category of finitely-presented representations and the category of -graded complexes of projectives with finite homology.
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 · Advanced Combinatorial Mathematics · Advanced Topics in Algebra
Quantum generalized Kac–Moody algebras
via Hall algebras of complexes
Jonathan D. Axtell*†*
Sungkyunkwan University, Suwon 16419, Republic of Korea
and
Kyu-Hwan Lee*∗*
Department of Mathematics, University of Connecticut, Storrs, CT 06269, U.S.A.
Abstract.
We establish an embedding of the quantum enveloping algebra of a symmetric generalized Kac–Moody algebra into a localized Hall algebra of -graded complexes of representations of a quiver with (possible) loops. To overcome difficulties resulting from the existence of infinite dimensional projective objects, we consider the category of finitely-presented representations and the category of -graded complexes of projectives with finite homology.
*†*This paper was supported by the National Research Foundation of Korea (NRF) funded by the Ministry of Science (NRF-2017R1C1B5018384).
*∗*This work was partially supported by a grant from the Simons Foundation (#318706).
1. Introduction
Let be an abelian category such that the sets and are both finite for all . The Hall algebra of is defined to be the -vector space with basis elements indexed by isomorphism classes in and with associative multiplication which encodes information about extensions of objects. Typical examples of such abelian categories arise as the category of finite-dimensional representations of an acyclic quiver over a finite field . This category became a focal point of intensive research when C. Ringel [20] realized one half of a quantum group via a twisted Hall algebra of the category. This twisted Hall algebra is usually called the Ringel–Hall algebra. The construction was further generalized by J. A. Green [9] to one half of the quantum group of an arbitrary Kac–Moody algebra.
Even though there is a construction, called Drinfeld double, which glues together two copies of one-half quantum group to obtain the whole quantum group, it is desirable to have an explicit realization of the whole quantum group in terms of a Hall algebra. Among various attempts, the idea of using a category of -graded complexes was suggested by the works of M. Kapranov [15], L. Peng and J. Xiao [17, 18]. In his seminal work [4], T. Bridgeland successfully utilized this idea to achieve a Hall algebra realization of the whole quantum group. More precisely, given a Kac–Moody algebra , he took the category of finite dimensional representations of an acyclic quiver associated with , and considered the full subcategory of projective objects in . By studying the category of -graded complexes in , he showed that the whole quantum group is embedded into the reduced localization of a twisted Hall algebra of .
The purpose of this paper is to extend Bridgeland’s construction to generalized Kac–Moody algebras. These algebras were introduced by R. Borcherds [2] around 1988. He used a generalized Kac–Moody algebra, called the Monster Lie algebra, to prove the celebrated Moonshine Conjecture [3]. Since then, many of the constructions in the theory of Kac–Moody algebras have been extended to generalized Kac–Moody algebras. In particular, the quantum group of a generalized Kac–Moody algebra was defined by Kang [12], and one half of the quantum group was realized via a Hall algebra by Kang and Schiffmann [13], following Ringel–Green’s construction.
The main difference from the usual Kac–Moody case is that the quiver may have loops in order to account for imaginary simple roots. A natural question arises:
Is it possible to realize the whole quantum group of a generalized Kac–Moody algebra in terms of a Hall algebra of -graded complexes?
A straightforward approach would run into an obstacle. Namely, when there is a loop, a projective object may well be infinite dimensional, and the Hall product would not be defined.
In this paper, we show that this difficulty can be overcome by considering the category of finitely-presented representations of a locally finite quiver , possibly with loops, and the category of -graded complexes in the category of projectives with finite homology. In contrast to Bridgeland’s construction, however, it is not clear that the corresponding product in the Hall algebra is associative. Therefore the proof of associativity for the (localized) Hall algebra is one of the main results of this paper.
Following the approach of [4], we work in the more general setting of a category satisfying certain natural assumptions listed in the next subsection (Section 1.1) which we keep throughout Sections 2-4. The main theorem (Theorem 4.6) for this general setting states that a certain localization of the Hall algebra is isomorphic to the Drinfeld double of the (extended) Hall algebra of , generalizing a result of Yanagida [23]. As a corollary (Corollary 4.7), the localized Hall algebra is shown to be an associative algebra.
In Section 5, we show that the category of finitely-presented representations of a locally finite quiver satisfies all the assumptions in Section 1.1 under some minor restrictions on the quiver. As a consequence of the results of Section 4 in the general setting, we obtain the main result for the quantum group (Theorem 5.12) which establishes an embedding
[TABLE]
of the whole quantum group of a generalized Kac–Moody algebra into a reduced version of the localized Hall algebra .
1.1. Assumptions
Given an abelian category , let denote its Grothendieck group and write to denote the class of an object .
Throughout this paper is an abelian category. Let denote the full subcategory of projectives and the full subcategory of objects such that is a finite set for any . There are several conditions that we will impose on the triple . Precisely, we shall always assume that
- (a)
is essentially small and linear over ,
- (b)
is hereditary, that is of global dimension at most 1, and has enough projectives,
- (c)
for any objects , the relation implies ,
- (d)
every element in is a -linear combination of elements in ,
- (e)
the identity implies for all , .
It is clear that the category is Hom-finite, that is is a finite set for all . Since has enough projectives by (b), it follows that the subcategory is abelian and hence a Krull–Schmidt category by [16]. It is also easy to check that is closed under extensions in . We note, however, that the category is not necessarily Krull-Schmidt in general.
The condition (c) is required in the proof of Proposition 3.18 to show that the localized Hall algebra is a free module over the group algebra . Conditions (d) and (e) are needed in Section 2.3 to ensure that the Euler form on can be lifted to a bilinear form on the whole category , albeit with values in .
The class of categories satisfying the above conditions (a)-(e) generalizes the class of categories satisfying Bridgeland’s conditions, also denoted (a)-(e) in [4], although our conditions do not correspond precisely. In particular, if the category is Hom-finite then so that condition (d) is superfluous, and it is also clear that (c) holds since is Krull-Schmidt in this case. One may check using Proposition 2.4 that the remaining conditions (a), (b), (e) hold in case if and only if the conditions (a)-(e) in [4] hold for .
1.2. Notation
Assume throughout that is a finite field () with elements. Let be such that . We denote by the positive real -th root of for , and write . We also write .
2. Hall algebras
We assume that the triple satisfies axioms (a)-(e) in Section 1.1.
2.1. Hall algebras
Given a small category , denote by the set of isomorphism classes in . Suppose that is abelian. Given objects , define to be the set of (equivalence classes of) extensions with middle term isomorphic to in .
Since has enough projectives, it follows from the definition of that the set is finite for all . The Hall algebra is defined to be the -vector space with basis indexed by elements , and with associative multiplication defined by
[TABLE]
The unit is given by , where [math] is the zero object in .
Recall from [4] that the multiplication (2.1) is a variant of the usual Hall product (see e.g. [20]) defined as follows. Given objects , define the number
[TABLE]
Writing to denote the cardinality of the automorphism group of an object , recall that
[TABLE]
Hence using as alternative generators, the product takes the form
[TABLE]
The associativity of multiplication in then reduces to the equality
[TABLE]
which holds for any .
2.2. Twisted and Extended Hall algebras
The Euler form on is a bilinear mapping
[TABLE]
defined by
[TABLE]
for all . This form factors through the Grothendieck group (see Lemma 2.1). We also introduce the associated symmetric form
We define the twisted Hall algebra to be the same as the Hall algebra of with a new multiplication given by
[TABLE]
We extend by adjoining new generators for all with the relations
[TABLE]
where we use the symmetric form . The resulting algebra will be called the extended Hall algebra and denoted by .
2.3. Generalized Euler form
Since the category has enough projectives, it follows from the definition of that is a finite set for any and . Define an Euler form by setting
[TABLE]
for all . The following lemma shows that the Euler form induces a bilinear map
[TABLE]
Lemma 2.1**.**
The Euler form depends only on the classes of objects and in the Grothendieck groups and , respectively.
Proof.
Suppose is an exact sequence in . Then there is a long exact sequence
[TABLE]
which shows that
[TABLE]
So the Euler form is well-defined on the class of . The proof for the class of is similar. ∎
In the remainder, let us write to denote the class of an object in , and continue to write for classes in . The inclusion induces a canonical map
[TABLE]
Write to denote the image of under this map.
Suppose that is a complete list of isomorphism classes of indecomposable projective objects in , for some indexing set . Then define the dimension vector of an object to be
[TABLE]
From condition (e), we have
[TABLE]
for any objects , whenever the classes are equal in the Grothendieck group .
Lemma 2.2**.**
Suppose that . Then for all if and only if
[TABLE]
for all .
Proof.
The only-if-part follows from the fact that for all and . For the if-part, let , , and suppose is a projective resolution. Then there is a long exact sequence
[TABLE]
which shows that
[TABLE]
The converse statement now follows. ∎
The above lemma now has the following consequence.
Corollary 2.3**.**
The Euler form on factors through a bilinear form
[TABLE]
Now suppose . Then it follows from condition (d) that there exist objects such that
[TABLE]
for some coefficients . Define a bilinear form
[TABLE]
by setting
[TABLE]
and extend it through linearity. We again define a symmetric version by setting for any .
Proposition 2.4**.**
Let be a nonzero object in . Then the classes and are both nonzero.
Proof.
Consider a nonzero object . Since has enough projectives, there exists a surjection for some projective . It follows that is a nonzero set. We obtain
[TABLE]
By Lemma 2.2 and Corollary 2.3, we obtain
[TABLE]
Thus neither nor is zero. ∎
Denote by the positive cone in the Grothendieck group generated by the classes for . Define
[TABLE]
Then it follows from Proposition 2.4 that is a partial order on .
2.4. The extended Hall algebra
The algebra is naturally graded by the Grothendieck group :
[TABLE]
We define a slight modification of the extended Hall algebra from Section 2.2. Starting again from with multiplication (2.5), the extended Hall algebra is defined by adjoining generators for all with the relations
[TABLE]
The algebra is also -graded, with the degree of each equal to zero. Note that the multiplication map
[TABLE]
is an isomorphism of vector spaces.
Following Green [9] and Xiao [22], we define a coalgebra structure on . We refer to [23] for the definition of a topological coalgebra, which involves a completed tensor product.
Definition 2.5**.**
[9, 22] In the extended Hall algebra define , and , by setting
[TABLE]
for all , , where the numbers are defined in (2.2) and is the completed tensor product. This gives the structure of a topological coassociative coalgebra.
As noted in [21, Remark 1.6], the coproduct on takes values in , instead of the completion , if and only if the following condition holds:
[TABLE]
This condition is satisfied if is the category of quiver representations considered in Section 5.
Now we have an algebra structure and a coalgebra structure on . It follows from [9, 22] that these structures are compatible to give a (topological) bialgebra structure. Below, we simply denote by the bialgebra . The bialgebra admits a natural bilinear form compatible with the bialgebra structure called a Hopf pairing.
Definition 2.6** ([9, 22, 23]).**
Define a bilinear form on by setting
[TABLE]
for , where as before.
It is clear that the restriction of this bilinear form to the subalgebra is nondegenerate. The following result was stated for in [22]. It is easy to check that it holds for as well.
Proposition 2.7** ([21, 22]).**
The bilinear form is a Hopf pairing on the bialgebra , that is, for any , one has
[TABLE]
where we use the usual pairing on the tensor product space:
[TABLE]
2.5. The Drinfeld double
We briefly recall the Drinfeld double construction for Hall bialgebras. A complete treatment of Drinfeld doubles is given in [10, §3.2] and [21, §5.2].
In [22], Xiao showed that the extended Hall algebra is a Hopf algebra and gave an explicit formula for both the antipode and its inverse , provided that is a category of quiver representations. It can be shown that Xiao’s formulas hold more generally provided that satisfies (2.11).
Athough the formula for is no longer well-defined in the case where does not satisfy (2.11), there is a more general condition that ensures the formula for is still defined. Recall from [8] that an anti-equivalence between two objects is a pair of strict filtrations
[TABLE]
such that for all . Two objects and in are called anti-equivalent if there exists at least one anti-equivalence between them.
It follows from results in [5] and [8] that Xiao’s formula for the map is still well-defined provided that the following condition holds for every pair of objects :
[TABLE]
Since the map generally takes values in a certain completion of , an extra condition is needed to ensure that corresponding relations in the bialgebra, such as
[TABLE]
are still well-defined. The required condition can be stated as follows:
[TABLE]
Up to minor modifications, the formulas for (and corresponding properties of) and continue to hold, respectively, in , whenever they are defined in .
If the conditions (2.12) and (2.13) are both satisfied by the category , then the Drinfeld double of is the vector space equipped with the multiplication uniquely determined by the following conditions:
- (D1)
The maps
[TABLE]
and
[TABLE]
are injective homomorphisms of -algebras;
- (D2)
For all elements , one has
[TABLE]
- (D3)
For all elements , one has
[TABLE]
where and .
The last identity is equivalent to
[TABLE]
for all , where and .
An argument similar to the proof given in [10, Lemma 3.2.2] shows that the multiplication is associative.
3. Hall algebras of complexes
Assume that is an abelian category for which the triple satisfies axioms (a)-(e) of Section 1.1. We now introduce certain categories of complexes over and define corresponding Hall algebras and their localizations. The associativity of multiplication in the localized Hall algebras will be established later in Section 4.
3.1. Categories of complexes
Define a -graded chain complex in to be a diagram
[TABLE]
such that for all .
A morphism consists of a diagram
[TABLE]
with .
Let denote the category of all -graded chain complexes in with morphisms defined above. Two morphisms are homotopic if there are morphisms such that
[TABLE]
We write for the category obtained from by identifying homotopic morphisms.
The shift functor defines an involution
[TABLE]
which shifts the grading and changes the sign of the differential
[TABLE]
The image of under the shift functor will be denoted by . Every complex defines a class in the Grothendieck group of .
We are mostly concerned with the full subcategories
[TABLE]
consisting of complexes of objects in and , respectively.
3.2. Root category
Let denote the (-graded) bounded derived category of , with its shift functor . Let be the orbit category, also known as the root category of . This has the same objects as , but the morphisms are given by
[TABLE]
Since is an abelian category of finite global dimension () with enough projectives, the category is equivalent to the (-graded) bounded homotopy category . Thus we can equally well define as the orbit category of .
Lemma 3.1** ([4]).**
There is a fully faithful functor
[TABLE]
sending a -graded complex of projectives to the -graded complex
[TABLE]
3.3. Decompositions
From now on, we omit in the notations for categories and write
[TABLE]
The homology of a complex will be denoted
[TABLE]
To each morphism in the category , we associate the following complexes
[TABLE]
in .
Lemma 3.2**.**
Every complex of projectives can be decomposed uniquely, up to isomorphism, as a direct sum of complexes of the form
[TABLE]
for some injective morphisms in such that and .
Proof.
Consider the short exact sequences
[TABLE]
[TABLE]
Since the the category is hereditary by assumption, all the objects appearing in these sequences are projective. Thus the sequences split, and we can find morphisms
[TABLE]
such that , , , and . This yields the following split exact sequence of morphisms of complexes
[TABLE]
where denote the obvious inclusions. (Note that and .) The desired decomposition of is thus given by setting: , .
Now suppose there is an isomorphism for some other pair of injective morphisms in . Then one can easily define corresponding isomorphisms of complexes and , showing uniqueness. ∎
Given , it will be convenient to write the decomposition in Lemma 3.2 as
[TABLE]
where and . Let the sign map
[TABLE]
be defined by , .
Lemma 3.3**.**
Let . Then there is an isomorphism
[TABLE]
of -vector spaces.
Proof.
First suppose that , is a pair of injective morphisms in . We note that there is a short exact sequence
[TABLE]
for , . One may also check directly that
[TABLE]
The decomposition of now follows easily by applying Lemma 3.2 to both and , respectively, and by using the involutive shift functor together with (3.2) and (3.3). ∎
3.4. Acyclic complexes
Given a projective object , there are associated acyclic complexes
[TABLE]
Notice that is acyclic precisely if in .
Lemma 3.4**.**
If is an acyclic complexes of projectives, then there exist objects , unique up to isomorphism, such that .
Proof.
If is acyclic, then by Lemma 3.2 we have for some isomorphisms and of projectives. It follows that . Since the complexes and are unique up to isomorphism, the objects are unique up to isomorphism as well. ∎
Lemma 3.5**.**
Suppose that and are injective morphisms in . Then in , if and only if there is an isomorphism
[TABLE]
of complexes in , for some objects .
Proof.
This is a reformulation of Schanuel’s lemma. We refer to [7, Theorem 0.5.3] for the proof. ∎
Proposition 3.6**.**
Suppose . Then there exists an isomorphism
[TABLE]
*for some acyclic complexes , if and only if in . *
Proof.
This follows directly from Lemmas 3.2 and 3.5, and by applying to the latter. ∎
3.5. Extensions of complexes
Given any morphism of complexes in , we can form a corresponding exact sequence
[TABLE]
of complexes in , where the middle term is defined by
[TABLE]
with
[TABLE]
This leads to the following result.
Lemma 3.7** ([4]).**
Let . The mapping defines an isomorphism
[TABLE]
We also have the following.
Lemma 3.8**.**
Suppose , are injective morphisms in the category . Let denote the cokernels: , . Then the following hold.
- (i)
; 2. (ii)
.
Proof.
The category can be identified as a full subcategory of by considering any object in as a complex concentrated in degree 0. It follows that
[TABLE]
The objects have the projective resolutions
[TABLE]
So the complexes are quasi-isomorphic to respectively, and isomorphisms (i), (ii) thus follow by Lemmas 3.1. ∎
Note that the isomorphism in Lemma 3.8 (i) may be given explicitly by , where is the unique morphism making the diagram
[TABLE]
commutative.
3.6. Hall algebras of complexes
We denote by the full subcategory of consisting of all complexes with finite homology, i.e. complexes such that
[TABLE]
The following result will be crucial for our definition of the Hall algebra of .
Lemma 3.9**.**
The set is finite for all .
Proof.
This follows by using the involution together with Lemma 3.8 and combining with Lemmas 3.2 and 3.7. ∎
Since the category is not necessarily Hom-finite, we must consider a generalization of the coefficients appearing in the definition (2.1) of the Hall product. First define a bilinear map, , given by
[TABLE]
where denotes the generalized Euler form (Section 2.3).
Then for any , we define
[TABLE]
where is the cardinality of , and we also write
[TABLE]
which is well-defined by Lemma 3.9.
In the remainder, let us write for the set of isomorphism classes in .
Definition 3.10**.**
The Hall algebra is defined to be the -vector space with basis elements indexed by isoclasses , and with multiplication defined by
[TABLE]
for all .
Remark 3.11**.**
Suppose there are complexes such that is a finite set. Then it can be checked using Lemma 3.3 and the definition of Euler form that
[TABLE]
The above definition thus generalizes the (twisted) Hall algebras of complexes of projectives defined by Bridgeland in [4].
3.7. Localization
As before, let us write , for each . The following result shows that the acyclic complexes introduced in Section 3.4 define elements of with particularly simple properties.
Lemma 3.12**.**
For any projective object and any complex the following identities hold in
[TABLE]
Proof.
It is easy to check directly from (3.6) that
[TABLE]
so that
[TABLE]
The complexes are homotopy equivalent to the zero complex, so Lemma 3.7 shows that the extension group in the definition of the Hall product vanishes. Taking into account Definition 3.10 gives the result. ∎
Lemma 3.13**.**
For any projective object and any complex the following identities are true in
[TABLE]
Proof.
Equation (3.10) is immediate from Lemma 3.12. Equation (3.11) follows by applying the involution . ∎
In particular, since , we have for ,
[TABLE]
[TABLE]
where . Note that any element of the form is central.
Let us write to denote the full subcategory of all acyclic complexes of projectives. It then follows from (3.12) and (3.13) that the subspace spanned by the isoclasses of objects in is closed under the multiplication and has the structure of a commutative associative algebra.
The following result is also clear.
Lemma 3.14**.**
The left and right actions of on given by restricting multiplication make the Hall algebra into an -bimodule.
Notice that the basis is a multiplicative subset in . Let us write to denote the localization of at . More explicitly, we have
[TABLE]
The assignment extends to a group homomorphism
[TABLE]
This map is given explicitly by writing an element in the form for objects and then setting . Composing with the involution gives another map
[TABLE]
Taking these maps together an extending linearly defines a -linear map from the group algebra
[TABLE]
which is an isomorphism by Lemma 3.4. It follows that the set gives a -basis of
Definition 3.15**.**
The localized Hall algebra, , is the right -module obtained from by extending scalars,
[TABLE]
That is, is the localization . We also consider as a -bimodule by setting
[TABLE]
for all and . We thus have a well-defined binary operation
[TABLE]
which agrees with the map induced from the multiplication in Definition 3.10 by restricting along the canonical map .
Given a complex , define a corresponding element in given by
[TABLE]
Then we claim that
[TABLE]
for any acyclic complex of projectives . Indeed, suppose that for some . Then clearly , and it follows by Lemma 3.12 that
[TABLE]
so we get the same element .
We note that a minimal projective resolution of need not be unique because the category is not Krull–Schmidt in general. However, it will be convenient to fix a (not necessarily minimal) resolution for each object .
Definition 3.16**.**
(i) For each object , fix a projective resolution
[TABLE]
and the complex is defined to be .
(ii) Given objects , write to denote the element in .
The next lemma shows that the definition of is independent of the choice of resolutions defining and .
Lemma 3.17**.**
Suppose , and let be any complex such that and . Then .
Proof.
Let be such a complex. By Proposition 3.6 there exist acyclic complexes in such that , and the result follows from (3.15). ∎
The following result provides an explicit basis for the localized Hall algebra.
Proposition 3.18**.**
The algebra is free as a right -module, with basis consisting of elements indexed by all pairs of objects .
Proof.
Suppose , and set , . Then by Lemma 3.17, and one may check using (3.14) that
[TABLE]
for and . This shows that the elements span as a -module.
It remains to check that the elements are –linearly independent. Notice that the Hall algebra is naturally graded as a -vector space by the set :
[TABLE]
Since the action of on is -homogeneous, it follows that also has an -grading. It is thus clear that the elements span distinct graded components of . To see that each component is a free -module of rank one, it remains to check that for each , we have implies .
Let us write . Then it will suffice to show that for any , the element
[TABLE]
is a -torsion element only if . Suppose that
[TABLE]
for some constants and distinct elements . One may check using Lemma 3.4 and condition (c) in Section 1.1, that for any the elements are also distinct. Next suppose that in . This gives an equation
[TABLE]
One may again use condition (c) together with Lemmas 3.2 and 3.4 to check that the terms appearing in this dependence relation are unit multiples of distinct basis elements in . So the relation must be trivial: , which gives . This completes the proof. ∎
4. Associativity via the Drinfeld double
In this section we prove that is the Drinfeld double of the bialgebra under suitable finiteness conditions. As a corollary, we show that is an associative algebra with respect to the multiplication described in the previous section.
4.1. Multiplication formulas
Suppose and recall the element in defined in Definition 3.16. Notice that the image under the involution is given by . Let us write
[TABLE]
so that .
Lemma 4.1**.**
Suppose . The following equality holds in .
[TABLE]
Proof.
Let be the complexes associated to in Definition 3.16. Then using the formula
[TABLE]
together with the relations and in the Grothendieck group , we have
[TABLE]
It follows by (3.14) that
[TABLE]
Consider an extension
[TABLE]
By Lemma 3.7, we may assume for some morphism , so that
[TABLE]
where
[TABLE]
Since are monomorphisms, so is . Thus implies that . Setting , it follows that (4.2) induces an extension
[TABLE]
One may check that this extension agrees with the corresponding image of (4.2) under the isomorphism
[TABLE]
given by Lemma 3.7 and Lemma 3.8 (ii). It follows that
[TABLE]
Finally, notice that for any extension of by . Putting everything together shows that equation (4.1) becomes
[TABLE]
which completes the proof. ∎
Lemma 4.2**.**
Let . The following equations hold in ,
- (i)
** 2. (ii)
**
where each sum runs over classes of objects in .
Proof.
(i) Again let be complexes associated to as in Definition 3.16. By definition, the product is equal to
[TABLE]
Then using , it is easy to check that
[TABLE]
This gives
[TABLE]
where we have used the equalities and in . It thus follows by (3.14) that
[TABLE]
Now suppose that is an extension of by . By Lemma 3.7, we may assume that for some . The extension thus takes the form
[TABLE]
where , , and are defined in (3.16). This extension induces an exact commutative diagram
[TABLE]
where “” denotes the map induced by , etc.
Since the map induced by in (4.4) is an isomorphism, it follows that the direct summands in the decomposition of Lemma 3.2 have the form
[TABLE]
where the maps are obtained from by restriction.
The objects and thus have projective resolutions
[TABLE]
respectively. This gives relations
[TABLE]
in . Substituting in (4.1), we have
[TABLE]
One may check directly using (4.4) that the map induced by (3.5) coincides with the connecting homomorphism in the long exact sequence of cohomology. In particular, note that , and .
Hence, we may conclude that
[TABLE]
By the equality on [23, p.984], the preceding equation may be rewritten as
[TABLE]
The equality in part (i) is now obtained by combining (4.1), (4.7) and (2.3).
(ii) This follows by interchanging and in (i) and taking on both sides. ∎
4.2. Embedding in
In this subsection we make some more precise statements about the relationships between the various Hall algebras we have been considering.
Consider the injective linear map defined by
[TABLE]
and let denote the image of this map.
Proposition 4.3**.**
The restriction of multiplication in makes the subspace into an associative algebra, and the embedding restricts to an isomorphism of (unital) associative algebras.
Proof.
The result follows from Lemma 4.1, together with a comparison of the relations (2.6) defining the extended Hall algebra with the relation (3.14) in the localized Hall algebra. ∎
Composing with the involution gives another embedding
[TABLE]
defined by , whose image is again an associative algebra such that restricts to an algebra isomorphism .
4.3. Drinfeld double of
Lemma 4.4**.**
The multiplication map defines an isomorphism of vector spaces
[TABLE]
Proof.
It follows from Proposition 3.18 that the algebra has a -basis consisting of elements
[TABLE]
Recall the partial order on defined in (2.9) and define for to be the subspace of spanned by elements from this basis for which . We claim that
[TABLE]
so that this defines a filtration on .
Suppose that and let
[TABLE]
Then consider an extension of complexes
[TABLE]
The long exact sequence in homology can be split to give two long exact sequences
[TABLE]
for some objects . It follows that there is a relation in ,
[TABLE]
which proves (4.8).
Suppose now that and for some objects . Then , and by Lemmas 3.1, 3.7, and 3.8
[TABLE]
and the extension class is completely determined by the connecting morphism . By Proposition 2.4, we therefore know that exactly when the extension is trivial. It follows that in the graded algebra associated to the filtered algebra , one has a relation
[TABLE]
It follows that takes a basis to a basis and is hence an isomorphism. ∎
As a corollary, we have
Corollary 4.5**.**
The algebra has a linear basis consisting of elements
[TABLE]
Now we state the main result of this section.
Theorem 4.6**.**
Suppose that satisfies conditions (2.12) and (2.13). Then the algebra is isomorphic to the Drinfeld double of the bialgebra .
Proof.
Because of the description of the basis of (Corollary 4.5) and the definition of Drinfeld double, the proof of the theorem is reduced to check equation (2.14) for the elements consisting of the basis of .
Let us write equation (2.14) in the present situation:
[TABLE]
Now let and . Let us write
[TABLE]
By the Hopf pairing (Definition 2.6 and Proposition 2.7) and (3.14), the left hand side of (4.9) becomes
[TABLE]
Similarly, the right hand side becomes
[TABLE]
After removing the term from both sides, equation (4.9) reduces to
[TABLE]
By Definition 2.6 and (3.14), the left hand side of (4.10) becomes
[TABLE]
Thus by Lemma 4.2 (i) we have
[TABLE]
Similar computations using Lemma 4.2 (ii) show that the right hand side of (4.10) becomes
[TABLE]
It follows by associativity (2.3) that this can be rewritten as
[TABLE]
One may check that this expression agrees with the LHS of (4.10), which completes the proof. ∎
It is now possible to verify that the multiplication in is associative.
Corollary 4.7**.**
If the category is Hom-finite (so that ) or if the subcategory satisfies conditions (2.12) and (2.13), then the algebra is associative.
Proof.
If , then it follows by Remark 3.11 that the algebra is isomorphic to the localized Hall algebra defined in [4]. It follows by results in [4] that the category is Hom-finite, so that and are both associative in this case.
The remaining statement is a consequence of Theorem 4.6 since the multiplication in the Drinfeld double is associative. ∎
Remark 4.8**.**
From the above result we can only conclude that the algebra is “locally associative” in general, in the sense that given we have
[TABLE]
for some element .
4.4. Reduction
Define the reduced localized Hall algebra by setting in whenever is an acyclic complex, invariant under the shift functor. More formally, we set
[TABLE]
By Lemma 3.4 this is the same as setting
[TABLE]
for all . One can check that the shift functor defines involutions of .
We have the following triangular decomposition.
Proposition 4.9**.**
The multiplication map defines an isomorphism of vector spaces
[TABLE]
Proof.
The same argument given for Lemma 4.4 also applies here. ∎
4.5. Commutation relations
In this subsection, we prove commutation relations among generators that are important to understand .
Lemma 4.10**.**
Suppose satisfy
[TABLE]
Then .
Proof.
It follows from (4.1) and (4.6) that . Exchanging and in this equation and taking on both sides gives as well, and the result follows. ∎
Lemma 4.11**.**
Suppose satisfies . Then
[TABLE]
Proof.
Using formulas (4.1) and (4.6) again, we have . Taking on both sides gives the equation , since is -invariant. The result follows by subtracting these equations. ∎
5. Realization of quantum groups
5.1. Quivers
Let be a locally finite quiver with vertex set and (oriented) edge set . For we denote by and the head and tail, respectively, and sometimes use the notation . We will denote by the number of loops at (i.e., the number of edges with ). A (finite) path in is a sequence of edges which satisfies for . For each , we let denote the trivial path. We again let and denote the head and tail vertices of a path .
Consider the sub-quiver with vertex set and edge set . We make the following assumptions throughout:
- (A)
There are no infinite paths of the form in . In particular, is acyclic and has no oriented cycles other than loops.
- (B)
Each vertex of the quiver has either zero loops or more than one loop, i.e. for all .
It follows from (A) that is partially ordered, with if there exists a path such that and , and the set satisfies the descending chain condition.
From now on, we assume that the quiver satisfies the conditions (A) and (B).
Example 5.1**.**
Write to denote the quiver consisting of a single vertex and loops. If , then the quiver trivially satisfies the assumptions (A) and (B). Below is a diagram for .
[TABLE]
Let denote the path algebra, with basis given by the set of paths and multiplication defined via concatenation. The elements are pairwise orthogonal idempotents. It follows from (A) that the subring is isomorphic to a free associative -algebra on generators. (If then .) Hence each left ideal is an indecomposable projective -module. It can then be checked that splits as a direct sum
[TABLE]
of pairwise non-isomorphic projective left -submodules.
A representation of over is a collection , where is a (possibly infinite dimensional) -vector space and . We let denote the abelian category consisting of the representations of over which are of finite support, i.e. such that for almost all . A representation is called finite-dimensional if each is finite-dimensional. For such a representation, set . We denote by the full subcategory of consisting of the finite dimensional representations of .
Any representation of is naturally an -module for the path algebra . Whenever it is convenient, particularly in the next subsection, we will consider representations of as -modules. It follows from the decomposition (5.1) that any left -module has a decomposition into -subspaces, , with . Then we have for a finite dimensional -module , which is equal to the dimension vector as a representation. We say that an -module is of finite support if the associated representation is.
Recall that any has the standard presentation of the form
[TABLE]
Let denote the full subcategory of whose objects are finitely-generated, projective -modules. Let be the full subcategory of whose objects are finitely presented representations of , i.e. the full subcategory consisting of all objects for which there exists a presentation
[TABLE]
for some .
As in Section 1.1, define to be the full subcategory of projectives in and the full subcategory of objects such that is a finite set for any . It is easy to see that . For the category , we have the following characterization.
Lemma 5.2**.**
The category is equal to the full subcategory of consisting of all finite-dimensional representations, i.e. .
Proof.
Assume that . From the standard resolution (5.2), we see that . Clearly, is finite as a set. Since any is finitely generated, the set is also finite. Thus is an object of . For the converse, assume that is infinite dimensional. Then there is a vertex such that is infinite dimensional. For each , we have a homomorphism given by . Thus is an infinite set and does not belong to . ∎
5.2. Krull–Schmidt property for
Since the endomorphism ring is not local in general, the usual Krull–Schmidt theorem does not hold in the category . In this subsection, we describe a suitable analogue.
First note the following.
Lemma 5.3**.**
Suppose are distinct vertices such that . Then either or .
Proof.
It follows from the stated condition that there are paths such that and are both nonzero and
[TABLE]
We then have , for some . Let be such that , , , and . Suppose without loss of generality that . Then is a path such that and . Thus . ∎
Let -Mod denote the abelian category of all left -modules of finite support. We identify -Mod with , and consider as a full subcategory of -Mod. We write for -Mod. Recall that for any idempotent there is an exact functor from the category -Mod to -Mod given by . Now suppose . Then is a finitely-generated, projective -module. Since is a free associative -algebra, is a free -module of finite rank, say . (See, for example, [7].) Write to denote the vector formed by these ranks. Notice that and unless . It follows that the vectors, , form a basis for .
Given a subset , consider the set . If is finite then so is by (A), and there are corresponding idempotents
[TABLE]
Lemma 5.4**.**
Suppose is a finite subset and write . Then there is an equivalence between and the full subcategory of consisting of modules such that .
Proof.
Consider the functor . Then , and an inverse functor is given by extending the action of on -Mod to all of by letting act by zero. ∎
Lemma 5.5**.**
Suppose is a finitely generated left ideal of . For , the following hold.
- (i)
*The ideal is a projective left -module. *
** 2. (ii)
*Any nonzero -module homomorphism, , is injective. *
** 3. (iii)
*Suppose and are homomorphisms such that . Then either or . *
** 4. (iv)
As a left -module, is isomorphic to a finite direct sum of copies of the modules .
Proof.
(i) Suppose is a left ideal with a finite set of generators. Then for some finite set and it follows that . If we set , then , which shows that is a left ideal of a hereditary ring and thus projective as an -module. It follows that is a projective -module by Lemma 5.4.
(ii) The image is a projective left -module by (i). So the exact sequence
[TABLE]
splits. Since is indecomposable, it follows that is injective.
(iii) Letting and , we have and . We thus have . It follows by Lemma 5.3 that or . Assume without loss of generality that . It then follows from the proof of Lemma 5.3, that there exists a path such that . It follows that .
(iv) First set , and choose a maximal vertex . Then is an -module with a finite set, say , of free generators of size . It follows from (ii) that for each generator the mapping, , defines an injective -module homomorphism. By (iii), we thus have a corresponding isomorphism
[TABLE]
Next choose a maximal vertex belonging to the subset
[TABLE]
It follows that is a free -module of rank , for some . Let be a set of free -generators such that generates . Then has size , and it follows as in the previous paragraph that we have an embedding
[TABLE]
By the maximality of we have . It is also clear that . It follows by (iii) that . We thus obtain an embedding
[TABLE]
Continuing in this way the process eventually terminates, since is finite, yielding the desired decomposition. ∎
The following is an analogue of the Krull–Schmidt theorem for the category of finitely-generated projective -modules.
Proposition 5.6**.**
Given any finitely-generated, projective left -module , there is an -module isomorphism
[TABLE]
for some nonnegative integers , only finitely many of which are nonzero. Moreover, given another such decomposition, , we must have for all .
Proof.
Since is finitely generated, is finite. Letting , we see that is a projective module of the hereditary ring . It follows from [6, Theorem 5.3] or [14] that is isomorphic to a finitely generated left ideal of . Hence Lemma 5.5 yields a decomposition
[TABLE]
It follows that
[TABLE]
Since the vectors form a basis for , the decomposition must be unique. ∎
5.3. Assumptions (a)-(e)
Let be a simple module supported only at . Then we obtain from (5.2) the standard resolution
[TABLE]
where for some integers . Then clearly unless . In particular, if is a minimal vertex then and hence
[TABLE]
which is non-zero by assumption (B). Now if is not minimal, then by assumption (A) the set is finite. We may thus use (5.2) and (5.3) inductively to write as a linear combination
[TABLE]
The following proposition makes it possible to apply the results in the general setting of the previous sections to the category of finitely-presented quiver representations.
Proposition 5.7**.**
The triple satisfies the assumptions (a)-(e) in Section 1.1.
Proof.
(a) It is clear. (b) Since the path algebra is hereditary, the category is hereditary as well. Furthermore, has enough projectives by definition. (c) It is clear that , so this condition follows easily from Proposition 5.6. (d) It follows from the expression (5.4). (e) If for , the standard resolution (5.2) tells us that and have the same number of elements for each . Then for each , and thus for by Proposition 5.6. ∎
It is also clear that the subcategory satisfies the finite subobjects condition (2.11), since each object is a finite dimensional vector space by Lemma 5.2. Thus also satisfies conditions (2.12) and (2.13).
Remark 5.8**.**
The quiver is called the Jordan quiver, and its path algebra is isomorphic to the polynomial algebra . For each , there is the one-dimensional simple modules over where acts as . Considering the standard resolution (5.2), we see , and the assumptions (d) and (e) are not satisfied. Nonetheless, the Jordan quiver is related to classical examples of Hall algebras. One can find details, for example, in [21].
5.4. Quantum generalized Kac-Moody algebras
In this subsection we recall the basic definitions concerning quantum generalized Kac–Moody algebras. We keep the assumptions on the choice of as in Section 1.2.
Let be a countable index set, and fix a symmetric Borcherds–Cartan matrix whose entries , by definition, satisfy (i) and (ii) for all . Put and , and assume that we are given a collection of positive integers , called the charge of , with whenever . We put
[TABLE]
The quantum generalized Kac–Moody algebra associated with is defined to be the (unital) -algebra generated by the elements for , , subject to the following set of relations: for , and ,
[TABLE]
[TABLE]
[TABLE]
[TABLE]
[TABLE]
The algebra is equipped with a Hopf algebra structure as follows (see [1, 12]):
[TABLE]
[TABLE]
[TABLE]
[TABLE]
We have an involution defined by , and for and . We denote by the subalgebra generated by , and by (resp. ) the subalgebra generated by (resp. ). Similarly, we define (resp. ) to be the subalgebra generated by and (resp. and ) for and . Then
[TABLE]
and the involution identifies with .
The following result provides a triangular decomposition for .
Proposition 5.9** ([1]).**
The multiplication maps
[TABLE]
and
[TABLE]
are isomorphisms of vector spaces.
5.5. Embedding of into a Hall algebra
Let be a symmetric Borcherds–Cartan matrix such that each row has only finitely many nonzero entries and for any . Fix a locally finite quiver associated to satisfying conditions (A) and (B): each vertex has loops, and two distinct vertices and are connected with arrows for . Then, since for any , the condition (B) is satisfied, and we can always choose an orientation for so that (A) is satisfied.
If , then there exists a unique simple object supported at . On the other hand, if then the set of simple objects supported at is in bijection with : if denote the simple loops at then to corresponds the simple module with and for .
Let us now assume that the charge satisfies
[TABLE]
We choose for in such a way that for . Then we set for and , and simply set for . Since have the same projectives in the standard resolution (5.2) for all , they define a unique class in . We will denote this unique class by for any .
The following lemma will be used in the proof of Theorem 5.11.
Lemma 5.10**.**
Let denote the image of the map defined in (2.7). Then the map is well-defined and is an isomorphism. That is,
[TABLE]
Proof.
The map is well-defined by condition (e) which is verified in Proposition 5.7. Clearly, the map is surjective. As noted already, there is a unique class which represents all simple modules in for each . Thus the map is injective. ∎
The following theorem, due to Kang and Schiffmann, is an extension of well-known results of Ringel [20] and Green [9] from the case of a finite quiver without loops to a locally finite quiver with loops:
Theorem 5.11** ([13]).**
Suppose is such that for all . Then there are injective homomorphisms of algebras
[TABLE]
defined on generators by for ,
[TABLE]
where and are defined right before Lemma 5.10.
Proof.
Let be the extended, twisted Hall algebra defined in [13]. It is shown in [13] that
[TABLE]
Thus we have only to check that there exists an injective algebra homomorphism . The only difference between the two algebras is that, while is extended by , the algebra is extended by . Thus the embedding of into follows from Lemma 5.10. ∎
5.6. Embedding of into
We keep the notations in the previous subsection. In particular, the matrix is a Borcherds–Cartan Matrix and is a fixed quiver corresponding to . Suppose that is the quantum group of the generalized Kac-Moody algebra associated with .
Now we state and prove the main result of this paper.
Theorem 5.12**.**
There is an injective homomorphism of algebra
[TABLE]
defined on generators by
[TABLE]
where and is the unique class representing in for each .
Proof.
We have a commutative diagram of linear maps
[TABLE]
where the vertical arrows are the isomorphisms described in Propositions 4.9 and 5.9, respectively, and the homomorphism is constructed out of the homomorphisms of Theorem 5.11. The map is a well-defined algebra homomorphism by Theorem 5.11 and by Lemmas 4.10, 4.11 and Corollary 4.7, which show that the generators satisfy the defining relations of the quantum group. It is clear from this diagram that is injective. ∎
The reference list from the paper itself. Each links out to its DOI / PubMed record.
- 1[1] G. Benkart, S.-J. Kang, and D. Melville, Quantized enveloping algebras for Borcherds superalgebras , Trans. Amer. Math. Soc. 350 (1998), no. 8, 3297–3319.
- 2[2] R. E. Borcherds, Generalized Kac–Moody algebras , J. Algebra 115 (1988), 501–512.
- 3[3] by same author, Monstrous moonshine and monstrous Lie superalgebras , Invent. Math. 109 (1992), 405–444.
- 4[4] T. Bridgeland, Quantum groups via Hall algebras of complexes , Ann. of Math. (2) 177 (2013), no. 2, 739–759.
- 5[5] I. Burban and O. Schiffmann, On the Hall algebra of an elliptic curve, I , Duke Math. J. 161 (2012), 1171–1231.
- 6[6] H. Cartan and S. Eilenberg, Homological algebra , Princeton University Press, Princeton, 1956.
- 7[7] P. M. Cohn, Free ideal rings and localization in general rings , New Mathematical Monographs 3 , Cambridge University Press, Cambridge, 2006.
- 8[8] T. Cramer, Double Hall algebras and derived equivalences , Adv. Math. 224 (2010), 1097–1120.
