Maximal Subalgebras of Finite-Dimensional Algebras
Miodrag Iovanov, Alexander Sistko

TL;DR
This paper classifies maximal subalgebras of finite-dimensional algebras over fields, providing a comprehensive framework that includes semisimple and non-semisimple cases, with applications to representation theory.
Contribution
It offers a complete classification of maximal subalgebras, especially in the semisimple case, and extends results to non-semisimple algebras, including those presented by quivers with relations.
Findings
Complete classification in the semisimple case
Lifting classification to non-semisimple algebras
Relations between algebra properties and subalgebras
Abstract
We study maximal subalgebras of an arbitrary finite dimensional algebra over a field, and obtain full classification/description results of such algebras. This is done by first obtaining a complete classification in the semisimple case, and then lifting to non-semisimple algebras. The results are sharpest in the case of algebraically closed fields, and take special forms for algebras presented by quivers with relations. We also relate representation theoretic properties of the algebra and its maximal and other subalgebras, and provide a series of embeddings between quivers, incidence algebras and other structures which relate indecomposable representations of algebras and some subalgebras via induction/restriction functors. Some results in literature are also re-derived as a particular case, and other applications are given.
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Maximal Subalgebras of Finite-Dimensional Algebras
Miodrag Cristian Iovanov
University of Iowa, USA and University of Bucharest, Romania
Alexander Sistko
University of Iowa, USA
Abstract
We study maximal associative subalgebras of an arbitrary finite dimensional associative algebra over a field , and obtain full classification/description results of such algebras. This is done by first obtaining a complete classification in the semisimple case, and then lifting to non-semisimple algebras. The results are sharpest in the case of algebraically closed fields, and take special forms for algebras presented by quivers with relations. We also relate representation theoretic properties of the algebra and its maximal and other subalgebras, and provide a series of embeddings between quivers, incidence algebras and other structures which relate indecomposable representations of algebras and some subalgebras via induction/restriction functors. Some results in literature are also re-derived as a particular case, and other applications are given. 1112000 Mathematics Subject Classification. Primary 16S99; Secondary 16G60, 16G10, 16S50, 16W20
Keywords maximal subalgebra, semisimple algebra, separable functor, separable, split, split-by-nilpotent
Introduction
Given a mathematical object, it is often natural to consider its maximal subobjects as a means of further understanding it. Maximal subalgebras of (not-necessarily associative) algebras, and in particular maximal abelian subalgebras, have classically guided such inquiry. A well-known instance of this principle arises, of course, in the structure theory of finite-dimensional semisimple Lie algebras, where a central role is played by their Cartan subalgebras: over , these are simply maximal abelian subalgebras, as seen in the classical papers [17], [34]. Others have subsequently generalized this work, and have applied similar ideas to maximal sub-structures of other possibly non-associative algebraic structures such as Malcev algebras, Jordan algebras, associative superalgebras, or classical groups ([18], [21], [22], [23], [35], [45], [46], [47]). On the associative side, a well known result of Schur [50] states that a commutative subalgebra of can have dimension at most , and this dimension is attained. A nice short proof of this interesting result was given later by Mirzakhani [37]. In another related direction, Motzkin and Taussky proved that the variety of commuting -by- complex matrices is irreducible in [38], [39], and Gerstenhaber [26] noted that this bounds the dimension of any -generated abelian subalgebra of by . There has been a lot of interest in studying dimensions of certain subalgebras of matrix algebras, as well as irreducible components of matrix varieties satisfying various properties. Often, these questions are tightly related to representation theory ([10], [11], [12], [13], [25], [26], [28], [29], [44], [38], [39], [49]).
The results of Schur concerning the maximal dimension of commutative subalgebras were generalized in several directions. One such extension is attributed to Jacobson [31], who generalized Schur’s theorem to any field . Maximal subfields of algebraically closed fields were studied by Guralnick and Miller in [27]. At the other end, Laffey [33] gave lower bounds for maximal abelian subalgebras of . In the general case of not necessarily commutative maximal subalgebras of matrix algebras, the problem was studied by Racine, who obtained a structure theorem for maximal subalgebras of associative central simple algebras [45], [46]. Using a deep theorem of Gerstenhaber from [25], in [1] Agore showed that the maximal dimension of a subalgebra in is . Recently, on the infinite dimensional side, interest for maximal subalgebras arose as well in commutative algebra [36]. However, there does not seem to be a general classification of maximal subalgebras of finite dimensional associative algebras beyond the case of matrix algebras.
The main result and first goal of this paper is to provide such a complete classification. More precisely, given a finite-dimensional associative algebra , we wish to answer two questions:
Can we classify/describe the maximal associative subalgebras ? 2. 2.
Can we determine under what conditions a maximal subalgebra shares interesting representation-theoretic data with , and what can be said about such a minimal extension of algebras?
For instance, as it turns out, a relevant question for (2) above will be finding conditions under which the extension is separable, split, or split-by-nilpotent.
We first provide a general structure theorem for maximal associative subalgebras of any finite dimensional associative algebra . The study proceeds in two steps: one deals first with the semisimple case, where there are essentially four types of maximal subalgebras, and then this is used to “lift” modulo the Jacobson radical, to deal with the general case. In the semisimple case, our proofs are a blend of techniques characteristic to finite dimensional simple algebras and representation theoretic arguments. In the non-semisimple case, there are two types of subalgebras: one coming essentially from maximal subalgebras of via pull-back, where is the Jacobson radical (and these further ramify via the semisimple classification); and another one, characterized by the property that irreducible modules of and “coincide” via restriction. These two types will give rise to examples of separable extensions and of split extensions of algebras, respectively, and both situations can be understood as particular cases of separable functors. The results take particularly nice forms when additional mild hypotheses are imposed, such that the algebra is separable (in particular, when is algebraically closed, or when it is a splitting field for ); in this case, the main result can be formulated as follows.
Theorem 0.1**.**
*Let be a finite dimensional algebra over a field whose simple modules are all Schur, that is, for each simple -module , and let be the Jacobson radical of . If is a subalgebra such that (so via the canonical projection; this exists by Wedderburn-Malcev) and if , then every maximal subalgebra of is conjugate (inside ) to an algebra of the following three types:
(a) , where is the subalgebra of of block upper triangular matrices with blocks of size and on the diagonal, and the parenthesis is considered as a subalgebra of .
(b) , where and is the image of the diagonal embedding (here, this diagonal embedding lands in components of the direct product ).
(c) , where and is a maximal -sub-bimodule of .*
The theorem above follows as a consequence of Sections 2 and 3. Its version for basic algebras, stated in the language of quivers with relations, takes an even more precise form (Theorem 4.1). As a consequence, for any finite dimensional algebra over an algebraically closed field, we find the maximal dimension of a proper subalgebra; it turns out that depends only on the smallest dimension of a simple module. The formula we obtain extends the results of [1] to the most general case.
On the other hand, our other major motivation is representation theoretic. The study of subalgebras of certain particular classes of associative algebras is certainly not new, and is crucial in several fields: in group representation theory, for example, induction and restriction to and from subgroups is an indispensable central tool. Similarly, Hopf subalgebras of finite dimensional Hopf algebras play an important role in understanding the structure, via the Nichols-Zoeller theorem [19]. More generally, subgroups of algebraic groups provide further examples. In fact, given a finite group and a subgroup , the extension often has nice properties: it is easily seen to be separable when is a p-Sylow subgroup and (which is, essentially, Maschke’s theorem), and it is also split in general, in the sense that is a direct summand of as -bimodule.
Special classes of finite-dimensional associative algebras also possess nice subalgebras, which influence the representation theory of the full algebra. For instance, every cluster-tilted algebra can be obtained as a trivial extension of a tilted algebra [3]. Furthermore, it is known that one can obtain the tilted algebra from its cluster-tilted algebra by deleting certain arrows from the cluster-tilted algebra [2]. Such a process of deleting arrows has a natural interpretation as a filtration of subalgebras , where is tilted, is the cluster-tilted algebra corresponding to , and is a maximal subalgebra of for all , obtained by deleting a suitable arrow at each step. The problem of finding all such filtrations is essentially the problem of determining which tilted algebras give rise to a fixed cluster-tilted algebra, and which arrows are suitable for deletion. This problem has been solved in [2], [4]. Since trivial extensions are in particular split extensions, the induction and coinduction functors between a tilted algebra and its corresponding cluster-tilted algebra also share nice properties. These have been studied in [51].
For general finite dimensional associative algebras, however, there does not seem to have been much work done towards understanding the representation theory via induction/restriction to subalgebras; rather, one often looks at quotient by various ideals. Perhaps the absence of a good supply of easily understood subalgebras with good properties is a reason for this. Hence, this paper is also intended to take a step in this direction; naturally, maximal subalgebras can be regarded as a first such step. Certainly, the case of induction/restriction to subalgebras can be regarded as a particular case of relating algebras via bimodules; but in general, given an algebra , it is usually not straightforward to find an algebra and bimodule such that the functor has the “right” properties. Nevertheless, in our study, we obtain constructions that yield classes of subalgebras of associative algebras which have good representation theoretic properties and are easily described at the same time. In the last section, we provide many examples of maximal subalgebras, as well as embeddings of algebras with such relevant properties. We give examples of embeddings of quiver algebras and incidence algebras, and in particular of Dynkin quivers, and show how indecomposable representations of many ADE quivers can be obtained via induction/restriction from suitable subalgebras, which are often also ADE, thus providing relations between indecomposables of various quivers (of finite type or not). Such induction/restriction functors sometimes even produce morphisms between the representation rings, and can thus be used to relate them. While we do not attempt to create a general theory - which could go into different directions as per various types of subalgebras - the multitude of examples and flexibility in the choices seem to suggest plenty of possible applications and a further study may be warranted.
The paper is organized into four sections. In the first, we give background on separable functors, and related notions of split/separable extensions of algebras. In the second section, we prove several fundamental results, and define two essential types of maximal subalgebras, which we call maximal subalgebras of semisimple (or separable) type and of split type. In the third section we provide a complete classification of maximal subalgebras of semisimple algebras, and prove the full classification, and the above Theorem 0.1. Finally, in the fourth section we provide examples, illustrate the theory in several important instances, and discuss possible future investigations.
Acknowledgments. The authors would like to thank Ryan Kinser for a careful reading of a preliminary version of this paper and many useful suggestions which improved the paper; they would also and Victor Camillo encouraging discussions and suggesting a few additional references.
1 Split Extensions, Split-by-Nilpotent Extensions, and Separable Functors
1.1 Separable Functors
In this section we give some general background on separable functors, and extensions of algebras related to such functors. We will see that separable functors provide a good context in which algebras can share representation-theoretic data. Much of our exposition will follow Chapter 3 of [15].
Throughout the rest of this paper, denotes a field, and an extension of rings. We say that is maximal in if for any subalgebra such that , it follows that or . We denote by the Jacobson radical of the algebra , and the center of . We will also write for all to denote the centralizer of in , and for all the bicommutant subalgebra. It is a standard fact (of Galois connections) that for any . Unless otherwise stated, all rings are associative -algebras, and all -algebras and modules are finite-dimensional over .
Definition 1.1**.**
Let be a functor between categories and . Then induces a natural transformation , defined by . is called separable if admits a natural section, i.e. a natural transformation with .
Separable functors were first studied in [40]. The terminology comes from the fact that an extension of rings is separable if and only if the restriction functor is separable (Prop. 1.3.1 of [40].) Such functors have found applications in representation theory as a general setting for Maschke-type theorems [15]. For the purposes of this paper, we need only a few essential facts, which we list and recall below without proof.
Theorem 1.2** (Rafael).**
Let have a right adjoint .
* is separable if and only if the unit of the adjunction splits, in the sense that there is a natural transformation such that , the identity transformation of .* 2. 2.
* is separable if and only if the counit of the adjunction cosplits, in the sense that there is a natural transformation such that , the identity transformation of .*
Proof. See Ch. 3.1, Thm. 24 of [15].
The following are straightforward corollaries to the general theory of separable functors, known to specialists, and they provides us with motivation for considering split and separable extensions. Such results also arise in the context of separable bimodules [16]. Recall that an algebra is representation finite if, up to isomorphism, there are only finitely many left (equivalently, right) indecomposable -modules (in which case, every module is a direct sum of indecomposable modules). For this and other notions in the representation theory of finite dimensional algebras we refer to the well known textbooks [6, 9]. In what follows, we let be an adjoint pair between categories of finite dimensional modules over algebras and , respectively. Denote the sets of isomorphism classes of -, and respectively, -modules. We include a brief argument only as an illustration of the theory; it also follows readily as consequence of more general results on separable bimodules and functors; see e.g. [15, 16].
Lemma 1.3**.**
*(i) If is separable, then for each , there is such that is a direct summand in . In particular, if is representation finite, then so is .
(ii) Moreover, if the unit is an isomorphism, for every , where are indecomposables, and for all . If, in addition, is faithful, then induces an injective map from to .*
Proof. If , then Rafael’s Theorem implies that is a direct summand of (the unit map splits); decomposing as a finite direct sum of indecomposables yields . So for some . Moreover, if is an isomorphism, then it follows that all but one term in the direct sum decomposition are zero, and . If is faithful, the last part follows from this.
Of course, the previous Lemma has a similar version for the right adjoint:
Lemma 1.4**.**
*(i) If is separable, then for each , there is such that is a direct summand in . In particular, if is representation finite, then so is .
(ii) Moreover, if the counit is an isomorphism, for every , where are indecomposable, and for all . If, in addition, is faithful, then induces an injective map from to .*
1.2 Localization
We remark how the localization or “corner rings” also produce examples of such separable functors. If is any ring, and an idempotent in , we have the following adjoint pairs:
[TABLE]
where ; ; . Then can be regarded as a localization functor in the sense of P. Gabriel [24]. The functors and form adjoint pairs. It is well known (and not difficult to see) that and via the unit, and respectively, counit of the adjunction. These identities also imply that and are faithful.
Corollary 1.5**.**
The functors are separable. If is a finite dimensional algebra, then each indecomposable -module is of the form for an indecomposable module ; moreover, one can pick such in two ways: (1) such that , a direct sum of indecomposable -modules with or (2) such that a direct sum of indecomposable -modules with .
We note that results as the previous one can be obtained in more general context of localization of categories, as in many instances such localizations have left and right adjoints which are “one-sided” inverses, hence satisfying such properties [24].
1.3 Split and separable extensions
For any morphism of algebras , we have an adjoint pair of functors between right -modules and right -modules given by induction and restriction along . For the purposes of this paper we may assume that is injective, identify with , and only consider the inclusion ; however, the statements below hold in general.
Definition 1.6**.**
Let be an extension of algebras. is called a split extension of if is separable, and separable if is separable.
The functor characterizations of separable and split extensions are often useful. However, it is usually easier to use the following criterion to directly verify that a given extension of algebras is split or separable:
Lemma 1.7**.**
Let be an extension of algebras. Then the following hold:
* is a split extension of if and only if there is an -sub-bimodule of such that as -bimodules.* 2. 2.
* is a separable extension of if and only if the multiplication map is a split epimorphism of -bimodules, if and only if there is an element such that and for all .*
We note that another notion of split extensions, in the spirit of Hochschild, is often present in literature, which requires the subspace above to be an ideal.
Corollary 1.8**.**
Let be an extension of algebras. Then the following hold:
If is a split extension of , then every indecomposable -module is a direct summand of a restriction of an indecomposable -module; in particular, if is representation-finite, then so is . 2. 2.
If is a separable extension of , then every indecomposable -module is a direct summand of a module induced from an indecomposable -module; in particular, if is representation-finite, then so is .
Hence split extensions hence allow one to transfer representation-theoretic properties of down to , whereas separable extensions allow one to transfer such data from to . To close this section, we recall some common representation-theoretic terminology:
Definition 1.9**.**
Suppose is a split extension, with as before. Then is split-by-nilpotent if is a nilpotent ideal of .
Definition 1.10**.**
Suppose is a split-extension, with as before. If , we say that is the trivial extension of through the -bimodule .
Split-by-nilpotent extensions have a fairly rich theory. In particular, trivial extensions arise prominently as cluster tilted algebras (see [3], [4], [14], [43], [51].) We will see in the next section that, under suitable hypotheses, we are able to gather partial information about the maximal subalgebras of a fixed algebra by considering related trivial extensions. This reduction works for general , but relies heavily on the ideals shared by and its maximal subalgebras. For more on split-by-nilpotent extensions in general, see [2], [5], [7], [8], [16], [43], [51].
2 General Results
We start off by recalling a simple lemma related to primitive orthogonal idempotents. It appears as Theorem 10.3.6 in [30], but does not appear to be well-known. Hence, we reproduce the brief proof here:
Lemma 2.1**.**
Let be a ring, a decomposition of into right ideals with and two collections of pairwise orthogonal idempotents which sum to . Furthermore suppose that as -modules. Then there is an invertible element such that . In particular, if and are two complete systems of primitive orthogonal idempotents, then for a suitable permutation .
Proof. We know that , with homomorphisms in given by left multiplication by elements in ; hence, the isomorphism is realized by left multiplication by some with . Set . Let realize the inverse isomorphism to . Then and . Set . Then and , so is a unit. Since , we have for all .
Corollary 2.2**.**
Let be an extension of finite-dimensional -algebras, and let be a complete collection of primitive orthogonal idempotents for . Then there is a unit such that the subalgebra contains a complete collection of primitive orthogonal idempotents for , whose elements are sums of elements in .
Proof. Let be a complete collection of primitive orthogonal idempotents for . Then in , the ’s are still a complete collection of orthogonal idempotents, and each can be written as a sum of primitive orthogonal idempotents, say . By the previous lemma, there is a unit such that form a permutation of for all and , from which the claim follows.
Note: Automorphisms of preserve maximality of subalgebras. In other words, if is an automorphism of and is a maximal subalgebra, then is another maximal subalgebra. More generally, -algebra endomorphisms of induce order-preserving maps on the poset of subalgebras of (ordered with respect to inclusion.) Often, it will be natural to classify maximal subalgebras of up to conjugation by a unit (i.e. up to orbits of the action of inner automorphisms on .)
Note: In general, it is not true that if and are isomorphic subalgebras of , that for some automorphism . For instance, if , then , but for any automorphism of . Indeed, any such would necessarily map to . Since , , for some element , and where is a multiple of . But in , and , a contradiction. In section 4, we will see more examples of this behavior.
Lemma 2.3**.**
Let be a maximal subalgebra of . Then , and exactly one of the following holds:
(i) and is a maximal subalgebra of the semisimple algebra .
(ii) , in which case and and have the same simple modules, that is, the functor induces a bijection from simple -modules to simple -modules.
Proof. Note that is a subalgebra with , and hence, either or . If the latter equality holds, then as left -modules, , and since and are finite-dimensional, we get by Nakayama’s Lemma. But then , contradicting the properness of the inclusion . Hence, , and the proof of is similar.
Now, since and is a subalgebra, either or . If , then in particular , and by correspondence, in this case is a maximal subalgebra of . Otherwise, . In this case as -modules. In fact, this is an isomorphism of -algebras, and since is semisimple, . But since is a nil (and nilpotent) ideal of (since is so as ), we also have . Therefore, ; it is easy to see now that this implies that induces a bijection from simple -modules to simple -modules.
This Lemma breaks maximal subalgebras into two possible types: those subalgebras of corresponding to maximal subalgebras of the semisimple algebra , and the rest, which satisfy . The first type reduces to the study of the maximal subalgebras of semisimple algebras, and we call them maximal subalgebras of semisimple type or maximal subalgebras of separable type, for reasons that will be apparent later. We call the maximal subalgebras of the second kind maximal subalgebras of split type. We construct a large class of subalgebras of the split type in the following main example; this class essentially produces all examples in many cases, as will be shown next.
Example 2.4** (Maximal subalgebras of split type.).**
*(1) Let be a two-sided ideal of , properly contained in , and maximal with this property (that is, a maximal -sub-bimodule of ), and such that the projection admits an algebra retract; equivalently, there is a subalgebra such that is a trivial extension, and also a Hochschild split extension, with the ideal satisfying . Let be a subalgebra of containing , such that . Then is a maximal subalgebra of , which we will say is of split type. Indeed, this follows if we show that is a maximal subalgebra of . Note that as -bimodules; is a simple -bimodule, and therefore a simple -bimodule. Since , the -part of acts trivially on itself, which implies that is a simple -bimodule. Now, if is an intermediate subalgebra, then is an -sub-bimodule, and since is a simple -bimodule, the conclusion follows.
(2) Assume now that is separable over . By the Wedderburn-Malcev theorem, there exists a subalgebra of such that . If is a maximal two-sided ideal contained in , then as in (1), it follows that is a maximal subalgebra of . In particular, this is true when is perfect (so when it is algebraically closed), or when the algebra is Schur (i.e. for every simple module), and so when the algebra is basic pointed (that is, every simple module is 1-dimensional).*
The next theorem gives the complete general structure of maximal subalgebras. We will need to use the following well known fact: if is a simple -bimodule which is finite dimensional (or, more generally, artinian or semiartinian both as a left and as a right module over ), then is semisimple as left and as right -module (and even isotypical). Indeed, taking to be the socle of and , then is semisimple since it is a quotient of the left module , so and so a sub-bimodule. Since , .
Theorem 2.5**.**
*Let be a finite dimensional -algebra. Then any maximal subalgebra of is either of semisimple type, or of split type. Moreover, if is a separable -algebra, and is a subalgebra of with (which exists by Wedderburn-Malcev Theorem), then:
(i) Every maximal subalgebra of of split type is conjugate to one of the form in 2.4 (2); that is, , where , and is a two-sided ideal of maximal inside .
(ii) Every maximal subalgebra of of semisimple type is of the form , where is a maximal subalgebra of .*
Proof. As in Lemma 2.3, if then is of semisimple type. Otherwise, . Let be the largest (two-sided) ideal of contained in , and let be an ideal of , minimal over (such an ideal exists since is finite dimensional). Then is a simple -bimodule, and thus semisimple as a left and right -module. By Lemma 2.3, it is also semisimple as a left and right -module. Also, , and so is left and right -semisimple (it is a quotient of as -bimodules). Note that , since it is an intermediate subalgebra .
We have the following isomorphisms of -bimodules
[TABLE]
Hence, is semisimple both as a left and right -module. Therefore, so . Similarly, . But then and similarly , which shows that is in fact a two sided ideal of .
Since is a simple -bimodule, , and acts trivially on , it follows that is simple as an -bimodule. Also, is a non-zero -bimodule quotient of , and so it is a simple -bimodule. By the above isomorphism, so is . Since , is a simple -bimodule as well. Therefore, the semisimplicity of as a left and right -module also implies that so .
Finally, denote . By the above, is an maximal -sub-bimodule of . It is clear that is a semisimple subalgebra of , and that where has , and this is a trivial extension.
Furthermore, assuming that is separable, by the Wedderburn-Malcev theorem there is a sub-algebra of with (see e.g. [42, Chapter 11]) and by the same theorem, in the case when is of split type, and are conjugate inside by some invertible . Lifting back, this easily implies that and are conjugate too.
If is of semisimple type, then the maximal subalgebras of are in 1-1 correspondence with those of , since the composition of maps is an isomorphism of algebras . If is maximal of semisimple type, it contains , and it follows from this correspondence that has the form for some maximal subalgebra , so . But, within , by Lemma 3.6, Theorem 3.10 and Remark 3.11, every such maximal subalgebra is conjugate to one of this form by some invertible element ; obviously, then the algebra is conjugate to via .
In the particular case when is algebraically closed or at least each simple module is Schur (, i.e. is a splitting field for ), this theorem will take more precise forms.
Remark 2.6*.*
We note that, if is a maximal sub-bimodule of , then is semisimple both as a left and as a right -module, and so . Hence, in order to find such , one needs to determine a maximal -sub-bimodule (or, equivalently, -sub-bimodule) of and pull back in . In the case of particular interest when is separable, and is a subalgebra of with as before, then to build maximal subalgebras of semisimple type we need to determine an -sub-bimodule of , and then let be such that . It is easy to note that such is in fact a two sided ideal of . In particular, if the endomorphism ring of each simple -module is , then one can write as -bimodules, and one only needs to determine the maximal -sub-bimodules of . Throughout the rest of this paper, we say that is a Schur, or Schurian, -algebra if for all simple -modules .
3 Semisimple Classification
3.1 The Simple Case
Example 2.4 show us how maximal subalgebras of split type arise in general. In turn, Theorem 2.5 and Remark 2.6 show us that under relatively weak conditions, the problem of constructing them is equivalent to the problem of constructing maximal sub-ideals of the Jacobson radical. However, at this stage we have comparatively little information on maximal subalgebras of “semsimple” or “separable” type. To completely understand the classification of maximal subalgebras, we will need to further examine these subalgebras. Essentially, this means understanding maximal subalgebras of semisimple algebras.
Some of our results hold in extra generality, and wherever possible, we have tried to state them under the weakest conditions possible. Before stating these results, however, it will be convenient to fix some notation for certain important matrix subalgebras:
Definition 3.1**.**
Let be an arbitrary (non-commutative) ring, a natural number, and a composition of , i.e. a collection of non-negative integers such that . Throughout, assume that for all . Given such , one can decompose each as , where is a -matrix with entries in . Let denote the collection of all such with whenever . If the ring is understood, we write . We call the ring of block upper-triangular matrices corresponding to the composition .
Note: As is convenient, we will use the frequency notation for a composition , i.e. we will write , where denotes the cardinality of the set .
As one would expect, the classification maximal subalgebras of semisimple algebras depends in good part on the maximal subalgebras of simple algebras. We will now construct the main classes of such algebras; the terminology chosen (type numbering) is done such that it agrees with that of [45]; there will be one additional new type of example.
Example 3.2** (Maximal subalgebras of semisimple type 1 (or type S1)).**
Let be a division ring (-algebra), , and . Then the -subalgebra of block triangular matrices is a maximal subring (-subalgebra) of . Indeed, if is an intermediate subalgebra and , then by subtracting a suitable block triangular matrix we may assume x=\left(\begin{array}[]{cc}0&0\\ T&0\end{array}\right) with an non-zero block. Then for ,
[TABLE]
*But it is well-known that is a simple --bimodule, so \left(\begin{array}[]{cc}0&0\\ &0\end{array}\right)\subseteq A^{\prime} which implies .
We remark that these subalgebras were considered in [45, 46] where it was proved they are maximal -subalgebras; here we need that they are also maximal as -subalgebras (and, in fact, they are maximal subrings).*
Example 3.3** (Maximal subalgebras of semisimple type 2 (or type S2)).**
Let be a division ring (-algebra), and a minimal field extension contained in (i.e. there are no intermediate subfields). Then its centralizer is a maximal subring (-subalgebra) of . Indeed, contains so it is a -subalgebra, and by [45], it is a maximal subalgebra of . But any intermediate subring (or -subalgebra) contains and is a -subalgebra, so maximality as a subring (resp. -subalgebra) follows from maximality as a -subalgebra. We note that in this case, as it is well known for simple subalgebras of central simple algebras, the algebra is a simple -subalgebra of and .
admits a third type of maximal subalgebra, not present in [45], [46]. Building up to it, we need a few remarks.
Proposition 3.4**.**
Suppose is a maximal subring (subalgebra) of the algebra , and . Then is a maximal subring (subalgebra) of the algebra .
Proof. Let ; we prove that the subring generated by together with is . There is some entry . Multiplying by appropriate matrix units (which are in ) we can assume , and using appropriate permutation matrices, that . But , and since the subring of generated by and is , it follows that . Again using permutation matrices, for all , which then implies the claim.
Example 3.5** (Maximal subalgebras of semisimple type 3 (or type S3)).**
Let be a minimal field extension, and a central division -algebra. Then the algebra (ring) is a maximal -subalgebra (subring) of . First, since is contained in , we may work with subalgebras instead of subrings. The commutative diagram
[TABLE]
*shows that it is enough to prove the minimality of the extension , and by the previous proposition, it suffices to show that is maximal in . Consider and let be an element of minimal tensor rank among elements in . Write , where is the tensor rank of , and assume . Then the ’s, and the ’s, are each linearly independent over . By multiplying with , we may assume , and .
For , the commutator is in and has tensor rank . Hence, for some uniquely determined element (which depends on ). But since are linearly independent over , by basic tensor linear algebra, the equality implies that for there are such that and . Again since the are independent, such are uniquely determined and they will not depend on . Hence, we have . Note that - otherwise, for all implies ( is central), so and are not independent, a contradiction. Also, for all and all , which again implies . Write , . Then*
[TABLE]
for suitable and . In particular, this means that to begin with. But , so , which contradicts the original assumption that . It follows that has the form to begin with, and then . We deduce that , and so the set strictly contains ; it is also a subfield of , and so by the minimality of . Finally, and implies , and the proof is finished.
Lemma 3.6**.**
Let be a division ring containing with , and let be a maximal -subalgebra. Then is conjugate to a maximal subalgebra of one of the three types S1, S2, or S3. More precisely, exactly one of the following holds:
- (i)
* is not semisimple and is conjugate to , for some (so is of type “S1”).* 2. (ii)
* is a simple subalgebra of , say , for a division ring with , and either:*
- (a)
The bicommutant of is , and is a maximal -subalgebra of the central simple -algebra ; in this case, , where is a minimal field extension of contained in (the algebra is of type “S2”); or
- (b)
The bicommutant of is , is a minimal field extension and , and the extension is (canonically) isomorphic to the extension of algebras . Hence, the algebra is of type “S3” in this case.
Proof. If is not semisimple, then . Since the simple left -module is -faithful, . But note that is invariant under right multiplication by , where we consider the usual right -module structure of . Hence, is a filtration of right -vector spaces and left -modules. Choose a -basis for compatible with this filtration, and let be the corresponding change-of-basis matrix. Then conjugation by is an algebra automorphism of which carries into a subalgebra of the subalgebra of block upper-triangular matrices, where . By maximality of and , and the claim follows.
Assume now is semisimple. Let be as before. Then we can write as , where we let be the direct sum of all submodules of isomorphic to the simple corresponding to the block in the Wedderburn decomposition of . Note that for all , right multiplication by is an -module endomorphism of ; in other words, it is an element of , where the last equality follows by Schur’s Lemma. In other words, right multiplication by restricts to an -module endomorphism of , for each , and so each is a right -vector space. Choosing a -basis for which respects the direct sum decomposition , we see that is conjugate to a block diagonal matrix subalgebra of ; obviously, this is maximal only if . Since is -faithful, this implies that has only one type of simple module up to isomorphism, and is therefore a simple algebra.
To prove the final two claims, we first note that is a -subalgebra and . If , then a -subalgebra of . Since it is maximal as a -subalgebra, it is also clearly maximal as a -subalgebra, and the claim follows from [45].
If , then , and hence (here, we abuse notation slightly by omitting the natural embedding maps and ; hence, we obtain an embedding ). This inclusion is strict, since otherwise would be contained in and we could reduce to the previous case. We show that this is a minimal field extension. Indeed, if is a field such that , then we have a surjective map defined by . But is central simple over its center, and is simple, so that is simple, and hence . By -dimension or -dimension, this algebra would then be strictly contained between and . By the same argument, it also follows that , and the last part is now automatic.
Maximal subalgebras of central separable algebras over arbitrary commutative rings were studied in [46].
3.2 The Semisimple Case
To get the complete picture, we now extend the results and describe maximal subalgebras of semisimple algebras.
Definition 3.7**.**
For a ring and natural numbers , we set to be the image of the diagonal map taking . We call this the diagonal ring corresponding to . If and/or are understood, we will write .
Lemma 3.8**.**
Let and be (not necessarily finite-dimensional) -algebras, with a maximal subalgebra of . If the restriction of to is not surjective, then is surjective, is a maximal subalgebra of , and .
Proof. Consider the inclusions . Since , is a proper subalgebra of containing . By maximality, , which implies that is surjective. If is a -algebra with , then the containment implies or , and the claim follows.
Proposition 3.9**.**
Let be a division ring, with a field contained in the center of . Suppose that is a maximal -subalgebra, such that each projection is surjective when restricted to . Then there is a -algebra automorphism such that . If and , then is conjugate to under an inner automorphism.
Proof. We first show that is a maximal subalgebra of . If there is algebra , then contains an element , with . Since , then contains the element with . It follows that and for all , so . Similarly ; but then , a contradiction. So is maximal in .
By hypothesis, for each , there is such that . Note that such is unique: with , then with , and we may repeat the argument above: using surjectivity of the projections, for every , there are elements so implies , and similarly , leading to a contradiction. The uniqueness of now easily implies that is linear, and in fact an algebra endomorphism (since ). Moreover, is injective since otherwise some element of the form would belong to ; surjectivity follows (or can be deduced applying the surjectivity of the first projection). Hence is an automorphism and the final claim follows by Skolem-Noether.
Theorem 3.10**.**
Let be a maximal subring (resp. -subalgebra) of , where for some division ring (resp. -algebra). Furthermore, suppose that the restriction to of the projection map is surjective, for each . Then there exists a pair such that , and there is a ring (resp. -algebra) automorphism of , such that is the direct product of the maximal diagonal subring (resp. -subalgebra) with the ring (resp. -algebra) . Furthermore, if all are central -algebras, then can be chosen inner.
Proof. Let be the (unique up to isomorphism) simple -module. Then is a -module in a natural way, and so an -module by restriction via . Let be any non-zero -submodule of . Since , for any we can find an such that . Therefore, , and so is a non-zero -submodule of , and hence . This shows that is a simple -module. But the inclusion is an embedding of -modules. Since as a -modules and -modules, and are simple -modules, it is a semisimple -module, and hence is semisimple too as a left -module.
Note that since , the -modules exhaust all simple -module (up to isomorphism). We claim that amongst the , …, , there are exactly isomorphism types of simple -modules. Let be the number of distinct isomorphism classes of -modules amongst the , . To begin, we claim . Indeed, if the ’s were all non-isomorphic -modules, then the Wedderburn decomposition of would be , where and is the number of times appears in the decomposition of as a module over itself. We claim that and . It is clear that . To prove the reverse inclusion, let . Pick and such that . Then if , , so that in fact , which implies and hence . That follows immediately from the surjectivity of the projections. Hence , contradicting the properness of . From this, it follows that .
To see , find a partition of with such that, after possibly permuting the matrix factors , the modules represent the first isomorphism class of -modules, represent a distinct isomorphism class, etc. By the above argument, . We claim that . Indeed, since for , we also have for . Using the surjectivity of the projections, for as well.
Consider a decomposition isomorphism , where is the block corresponding to the simple isomorphic -modules with . The isomorphim of left -modules for implies and the surjectivity of these projections then shows that the maps are bijective. Moreover, considering as a block of with its algebra (ring) strucutre, the maps become isomorphisms of algebras; they are also unital, since if (), then so . Thus, applying the automorphism of the algebra , we see that the algebra is sent to the algebra . The latter algebra is maximal if and only if , which implies the claim. By definition, we then have for all . But by a similar argument, if then we can find an automorphism of which carries into the subalgebra , which is not maximal in . Hence , which implies for all .
The last statement is again a consequence of Skolem-Noether.
Remark 3.11*.*
Suppose that is a semisimple -algebra whose simples are Schur, with Wedderburn decomposition . If is a maximal subalgebra of and each projection map is surjective, then there exist indices such that and is conjugate to . Otherwise is, up to conjugation (up to an inner automorphism), the product of a maximal subalgebra of with the other matrix factors of . Setting , we see from the simple classification that since is necessarily a -subalgebra of , is either of type S1 or S2. If is also an algebraically closed field, then only subalgebras of type S1 are possible.
We summarize the results to describe maximal subalgebras of semisimple type in arbitrary finite dimensional algebras.
Corollary 3.12**.**
Maximal subalgebras of semisimple type of a finite dimensional -algebra are in 1-1 correspondence with subalgebras of , which in turn are described by Remark 3.11. If, moreover, is separable, and is a subalgebra of with and , then any maximal subalgebra of of semisimple type is conjugate to one of the form where either for some with , or , where is a maximal subalgebra of of type S1, S2 or S3.
Proof. This follows from Lemma 3.6, Theorem 3.10 and Remark 3.11, and when is separable, Theorem 2.5 is used.
We end this section with a result showing that the maximal algebras of semisimple type produce separable extensions in many interesting cases, thus justifying the alternate name of maximal algebras of “separable type”.
Proposition 3.13**.**
Let be a finite dimensional algebras such that is separable. Then if is any subalgebra of semisimple type, then the extension is separable.
Proof. Let be a subalgebra of with . Since is of semisimple type, . Also, by hypothesis is separable, and let be a separability idempotent of . Let be the image of through the canonical map . We show that is a separability idempotent for . First, obviously . We need to show that for . Since , it is enough to show this for and for . First, if , then
[TABLE]
Also, if , then and , and using also that , we obtain
[TABLE]
which ends the proof.
4 Applications and Examples
We now present a series of examples and applications to illustrate the results from the previous sections. We also determine the maximal subalgebras of several important classes of algebras, such as path algebras of quivers and incidence algebras of posets.
4.1 Pointed Algebras
We begin by stating a particular case of the above results, for algebras which are basic Schurian, that is, each simple module is 1-dimensional (such algebras are also called pointed).
Theorem 4.1**.**
*Let be a basic Schurian (i.e. pointed) algebra. Let be a complete system of primitive orthogonal idempotents of . Then any maximal subalgebra of is conjugate to one of the following two types (as before, denotes the Jacobson radical of ):
(a) .
(b) , where is such that is a maximal -sub-bimodule of , where .*
We now apply this theorem to cases of particular interest, such as path algebras of quivers and incidence algebras. These will follow directly from the previous theorem.
First we consider quiver algebras; in fact, we reformulate the previous theorem in the language of quivers with relations, when one needs to work with an algebra which is given by a presentation.
Let be a finite quiver. For each pair of vertices , we write to denote the set of arrows from to and to denote the span of all arrows in (“generalized arrows” from to ). It is well known that every finite dimensional basic Schurian (i.e. pointed) algebra can be presented as for a finite quiver and an admissible ideal of , that is for some [6] (in particular, every basic algebra over an algebraically closed field ). In this case, since the map is injective, the spaces can be regarded as subspaces of . For each pair of vertices and each subspace of codimension (in particular ), we associate the subalgebra of which is defined by . This is the subalgebra of spanned by the images of all paths of length , all vertices, all arrows for and . Note that is a maximal -sub-bimodule of containing . Furthermore, for , let denote the subalgebra . Then Theorem 4.1 can be reformulated as follows.
Proposition 4.2**.**
The maximal subalgebras of , for a finite quiver and admissible ideal , are precisely the algebras conjugate to either or .
We note that the extension is always a separable extension, with as a separability idempotent.
In the case of the incidence algebra of a poset , this Theorem also directly produces the structure of all maximal subalgebras. Let be a finite poset. Recall that the incidence algebra of has a basis consisting of pairs for (the intervals) and multiplication given by “convolution” . The following proposition is now a direct consequence of the previous one, or of the Theorem 4.1.
Proposition 4.3**.**
Let be a maximal subalgebra of , where is a finite poset. Then is conjugate either to an algebra of the form with , (maximal subalgebras of semisimple type) or to one of the form where , and is a covering relation, that is is minimal (if then either or ).
We note that incidence algebras of quasi-ordered sets are also considered in literature (and are sometimes called Structural Matrix Algebras; a quasi-ordered set is a set with a partial order which is reflexive and transitive, but not necessarily symmetric). Up to Morita equivalence, any incidence algebra of a quasi-ordered set is equivalent the incidence algebra of the poset , where is the equivalence relation generated by symmetrization ( if and . Such incidence algebras will appear implicitly in what follows.
Dynkin quivers and other examples
We will consider a slight relaxation of the notion of a maximal subalgebra of , which will significantly expand the class of examples and applications. Of course, generically when and are not fixed, one can can equivalently talk about minimal extensions of algebras . Such extensions can be regarded via the associated restriction functor between the corresponding module categories; hence, it will be useful from a representation theoretic point of view to consider such extensions “up to Morita equivalence”. We thus introduce the following definition.
Definition 4.4**.**
Let be finite dimensional -algebras, and a functor. We say that is a (minimal) restriction if there is a (minimal) extension of algebras with Morita equivalent to respectively, and the diagram
[TABLE]
is commutative, with vertical arrows being equivalences. If, given the algebras , such a (minimal) restriction exists, we say is a (minimally) embeddable pair. We write when is an embeddable pair.
4.2 Embeddings of quivers of “separable type”
First note that if is a Dynkin quiver, (or more generally an acyclic quiver) then one can introduce a partial order on the vertex set given by paths: if there is a path from to . Without loss of generality, we may assume . In the Dynkin case, or more generally, if the underlying graph of is a tree, the path algebra is isomorphic to the incidence algebra associated to . This isomorphism takes a path between vertices and to the matrix element . Here, we regard also as a morphism , and is the structural matrix algebra (incidence algebra); of course, as a representation, yields an indecomposable representation of ; when is of type , this is the indecomposable of largest dimension.
Let be Dynkin, or more generally, a tree. We use the above to create a minimal embedding. Let and consider two adjacent vertices , so that there is an arrow in , and let be the order as above. We consider a new (quasi-)ordering on generated (via transitivity) by “introducing” the new relation . Hence, the new relation is defined by if either or and . The incidence algebra associated to , as a subalgebra of is the algebra with basis , which is exactly the subalgebra generated by and . Let be the ideal of generated by ; it has a basis the elements for which and . Obviously, . In certain cases, this embedding becomes a minimal embedding.
Proposition 4.5**.**
Let be a quiver whose underlying graph is a tree, and an arrow in such that the following condition () is satisfied:*
() emits no other arrows except , and receives no other arrows but .*
Then the algebra extension is a minimal extension, with a maximal subalgebra of of semisimple type.
Proof. The condition in the hypothesis shows that , so is maximal. The subspace of spanned by has as a complement the space spanned by the ’s with and ; this is an ideal. Hence, is necessarily a block of , but it is not a block of . Thus, by the results of Section 2 the maximal subalgebra of is of semisimple type.
We note now that in general, even in the absence of condition (*), the algebra above is Morita equivalent to the path algebra of , where is the quiver obtained from by collapsing the edge ; that is, is obtained from by removing and then identifying vertex with vertex . Note that in this case, new paths arise in by concatenating paths ending at and paths starting at ; the paths in which contain the arrow are in one-to-one correspondence with a subset of the paths in which contain the vertex . One way to observe this Morita equivalence is by noting that , where the block corresponds to the idempotents . Hence, if , then is Morita equivalent to (it is the basic algebra associated to ); moreover, in , a basis is given by , for and . These correspond exactly to paths in from some to some . This last fact shows that there is an isomorphism . This last assertion shows that we have the following.
Proposition 4.6**.**
With the notations above, the pair is an embeddable pair. If condition () is satisfied, then this is a minimally embeddable pair.*
More generally, if is a finite poset and its incidence algebra, we say that an interval is clamped if implies that is comparable to , and implies that is comparable to . We say that covers if . If is a clamped interval with covering , then adding the relation yields a quasi-ordered set , and a minimal extension of algebras . is Morita equivalent to the incidence algebra of the poset obtained by collapsing the arrow in the Hasse diagram of to a point. If is a quiver whose underlying graph is a tree, then it is naturally an incidence algebra, and the condition (*) above is equivalent to the interval being clamped and covering . In fact, using the remarks above and in Section 1, one can see that the resulting functors can be re-interpreted as being exactly localization functors.
The previous considerations allow us to provide many natural examples of embeddable pairs, which produce separable extensions. For example, “embeds” in by “collapsing” one edge; below, the dotted arrow in gets collapsed.
[TABLE]
For instance, if , this is just the embedding , where we use the notation of Definition 3.1 and the note below (here R = .) Given the appropriate orientations so that the collapsed arrow satisfies condition () above, this becomes a minimal embedding. We give a few more examples and note that there are embeddable pairs , and . This is perhaps also interesting as “pictorially” one perhaps normally expects to embed lower order and ’s into higher ones. We draw only the diagrams, with the arrow to be collapsed drawn as a dotted arrow (thus collapsing an arrow produces an embedding up to Morita equivalence). Again, with appropriate orientations satisfying condition () we obtain minimal embeddings (hence, examples of maximal subalgebras).
[TABLE]
[TABLE]
Obviously, in a similar way one can produce many other embeddings, which become minimal embeddings given appropriate orientations on the quiver; these will always be separable. We list a few such possible embeddings which are obtained just as above and leave it to the reader to imagine/draw the appropriate diagrams:
, , , , , .
4.3 Embeddings of quivers of “split type”
We give another series of examples of embeddings of quivers, which will often produce examples of split extensions. These are embeddings of path algebras that are obtained whenever a subquiver of a quiver is considered. Let be an acyclic quiver, and let be the span of all non-trivial paths in which pass through . This is an ideal of . Now consider the subalgebra of generated by all paths which do not pass through ; this is spanned by all these paths (including the ones of length 0 which are vertices ), together with the identity element , and hence contains . Then, we have the following straightforward observation.
Lemma 4.7**.**
With the above notations, is a split extension of , with .
Proof. The direct sum is obvious as any path either contains or doesn’t. If both contain , then , since otherwise the path passes through twice and would contain cycles.
This gives again a multitude of examples of embeddings of quivers. The algebra is itself a path algebra: if is the quiver obtained from by removing all the arrows adjacent to (but keeping the vertex itself), then one easily sees that there is a natural identification as . Thus, this produces a split extension . Again, as before, there are circumstances under which this becomes a maximal embedding. Of course, a more general example of such embeddings is by simply taking to be the subquiver of obtained by removing all the edges whose source or target is a member of . Then is again a split extension, and an embeddable pair. We note that inside the algebra , the idempotents corresponding to vertices of are disconnected; one can remedy that by considering the subalgebra generated by together with all “other” paths in (which are “contained” in ), or the subalgebra of of semisimple type obtained by “joining” the idempotent with some . Then both and are path algebras of corresponding suitable quivers or obtained from by erasing the arrows in the part contained in and collapsing everything to a point (respectively, erasing that part all together), and these give rise to embeddable pairs and .
Suppose that is a leaf, i.e. its valence in the underlying graph of is . Let be the other vertex showing up in the unique edge adjacent to . Using the notation of section 4.1, consider the minimal extensions . Then is a trivial extension, and hence split. Furthermore, is an ideal in and as -bimodules. Hence, is a split extension of . It is easy to note that the quiver of is obtained from by contracting the edge between and to a point. Below we list a few such embeddings between Dynkin quivers. In each picture, the vertex to be “isolated” by the procedure of the above Proposition is depicted by the symbol , while the other vertices of the quiver are depicted as full dots . These are usual embeddings that one often considers.
[TABLE]
[TABLE]
Hence, this case is one where, as “pictorially” expected, lower order and ’s embed into the ones of higher order.
4.4 Remarks on the representation theory
We note that whenever is a map between quivers which is a morphism of partial semigroups between the partial semigroups of paths in and respectively, then the induced morphism of algebras produces a restriction functor which respects tensor products. This can be observed directly with quiver representations, or using the following fact: the structure as a monoidal category of (tensor product) for a quiver is naturally associated to the partial semigroup algebra comultiplication , for all paths . The above morphism is compatible with this comultiplication (), and this implies that the functor commutes with the tensor product of objects (in other words, this is a tensor functor, see [20]). Thus, the previous procedure of deleting arrows between vertices in some subset , and the resulting embeddings of quivers all give rise to morphisms between the representation rings of the underlying quivers.
We also note that Lemmas 1.3, 1.4 and Corollaries 1.5, 1.8 can be used to relate some indecomposables over quivers and their sub-quivers, and algebras and their subalgebras. For quiver of types and , these can be observed directly using the structure of the indecomposables. Indeed, for example, via the embeddings of the previous subsection, every indecomposable over is obtained as the restriction of an indecomposable over , and every indecomposable -representation is obtained as a restriction of an indecomposable -module. One sees that these Lemmas and Corollaries can be interpreted in terms of positive roots: for example, positive roots of are all obtained from some positive root of by deleting one entry; similar statements work for and and and .
We end this subsection with two more examples showing how restriction to subalgebras can give interesting representations, showing the potential of considering subalgebras. The previous examples showed an interpretation on how the thin representations (i.e. representations in which multiplicity of simples in the composition series is at most 1) of lower and are obtained from higher analogues. We now show examples on how the non-thin indecomposable modules in type can be obtained from indecomposable -representations by restriction to subalgebras.
Example 4.8**.**
Consider the following embedding of -algebras, written as subalgebras of .
[TABLE]
The second algebra is an with zig-zag orientation.
The first algebra is isomorphic to a quiver algebra of type , with representing the idempotent corresponding to a sink; correspond to the other three vertices, and represent the three edges going out of . We can represent this embedding symbolically by the following and graphs; one can think of this of this embedding as obtained from a “gluing operation” on the quiver, through which the and arrows are being identified (glued), to create a . In the diagram below, the equal signs are intended to refer to this interpretation.
[TABLE]
As noted, this results in an algebra embedding. Now, let be the 5 dimensional representation given by the embedding of into as above (this is also the defining representation of as an incidence algebra). It is the thin indecomposable dimension of of maximal dimension (5, corresponding to the positive root of ). Restricting this to , it is not difficult to note that we obtain an indecomposable representation of , which is necessarily the 5-dimensional representation of corresponding to the root . While this example has fixed an orientation for simplicity, this procedure can be done with any orientation.
By extending the “tail” of , one can easily generalize this example to an embedding of into , which has the result of obtaining the indecomposable representation corresponding to the root from the indecomposable representation of corresponding to the root (the one of maximal dimension). We note that at the root level, this amounts to “joining” two of the entries - second and third one - of the positive root of to create the root of . This construction shows that this formal procedure actually has a representation theoretic meaning (it is a categorification of this procedure on roots).
Example 4.9**.**
Consider the following embedding of algebras
[TABLE]
Here, in the second diagram, the algebra is just the path algebra of the quiver (which can have any orientation). In the first part of the diagram, the dotted line means that if the two arrows \textstyle{4\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$$\textstyle{6} and \textstyle{6\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$$\textstyle{5} are oriented such that a path can be formed with them, then there is a [math] relation in the algebra. The embedding of the two algebras is simply such that , where denotes the idempotent corresponding to the vertex in both algebras. This is a maximal subalgebra embedding (i.e. a minimal embedding), and it is of semisimple type, and is so a separable extension. The second one is a quiver algebra (or even incidence algebra) which is not of finite type (it is an Euclidean ), and hence, the first is not of finite type.
We note that this is very close in spirit to covering theory; in fact, we note that if is an algebra, finding an overalgebra of with good properties means that the restriction functor acts as a “cover” for -modules. If such an extension is separable, one can exclude finite type of if such a “cover” is not of finite type. One can obtain variations of this example by changing the pictures appropriately so that the is a quiver algebra which is not of finite type.
4.5 Maximal subalgebras over non-algebraically closed fields
We also give some examples to illustrate maximal subalgebras of semisimple types S2 and S3.
Example 4.10**.**
Let be a prime, an irreducible polynomial of degree and be the companion matrix of . Then the characteristic polynomial of is and it coincides with its minimal polynomial. Thus, is a subalgebra which is a field extension of . Hence, its centralizer in is a maximal subalgebra. We note that, in fact, , which follows by the irreducibility of the minimal polynomial (and is well known in this case). This is a maximal subalgebra of type S2.
Example 4.11**.**
Let be the division algebra of quaternions, with subfields . Then is a minimal field extension of , and so the centralizer in is a minimal extension of -algebras. One can check that ; indeed, ; now both and are bimodules over . The quotient has dimension , so as an -bimodule it can only be simple. This shows that there are no intermediate -bimodules between and , and proves the equality . The algebra is a maximal subalgebra of , which is thus also of type S2.
Using , we give an example of maximal subalgebra of type S3.
Example 4.12**.**
Note that is a minimal field extension; thus the extension is a maximal -subalgebra. One can also construct this, as shown in the discusion on the simple case in Section 3: regard as an -subalgebra of (it is a maximal subalgebra), and consider the embedding , which gives a maximal -subalgebra of . This is an example of type S3.
4.6 Maximal dimension of subalgebras
We note now how our results can be applied to determine the maximal dimension of a subalgebra of . This problem was considered in [1], over an algebraically closed field. The author did not use the results of [46, 45] (effectively re-descovering some of these) but instead used a deep result of Gerstenhaber regarding the maximal dimension of a subspace of nilpotent matrices [25]. Here we provide a direct argument, based on the above classification; as noted before, in the case of an algebraically closed field the structure of maximal subalgebras is significantly simplified (and does not need the considerations on subalgebras of simple subalgebras of types S2 and S3). In fact, using our approach, we can give a general result for arbitrary finite dimensional algebras; it generalizes the result of [1] where it was shown that for , the maximal dimension of a subalgebra is .
Theorem 4.13**.**
Let be a finite dimensional algebra over an algebraically closed field . Let , and be the dimensions of the blocks of . Then the maximal dimension of a proper subalgebra of is
[TABLE]
That is, it is if (i.e. if has no 1-dimensional blocks) and it is otherwise.
Proof. Write , where . If , then has a codimension- subalgebra , and is a codimension- subalgebra of . Otherwise . If is a subalgebra of maximal dimension, it is also maximal; if it is of split type, then is a (maximal) -sub-bimodule of and ( is the minimum dimension of a -bimodule). Hence, the maximum dimension of such an algebra is . If is of separable type, then is a maximal subalgebra of . Corollary 3.12 shows that the dimension of is either (coming from diagonal embeddings) or for some (coming from maximal subalgebras of blocks). The largest dimension of such a subalgebra is thus , and hence , and there is always a subalgebra of which attains this dimension. Since whenever , the result follows.
4.7 Maximal Subalgebras and automorphisms
In Section 2 we saw an example with two isomorphic subalgebras of a fixed algebra , which were not isomorphic under any automorphism of . We now examine this behavior in greater detail. If is a finite-dimensional algebra over a field , then acts of the poset of subalgebras of . In particular, it permutes the collection of maximal subalgebras of . It is natural to ask whether this action determines the isomorphism classes of subalgebras of . In other words, if are isomorphic maximal subalgebras, does it follow that there exists an such that ? Unfortunately this does not happen in general, and can fail even in nice enough cases of path algebras of not too complicated quivers, as the following example of an acyclic Schurian quiver illustrates.
Example 4.14**.**
Let denote the following quiver:
[TABLE]
Set , for algebraically closed and the Jacobson radical of (the arrow ideal). Then any satisfies , for all . Up to inner automorphisms we may assume that , and with this assumption induces a quiver automorphism of . In particular, no automorphism of can send vertex to vertex (by inspection, has no non-trivial automorphisms). Consider the maximal subalgebras . Then and are isomorphic, but there is no automorphism of carrying one to the other. Indeed, any proposed automorphism would induce an automorphism of sending to , a contradiction. This also happens with algebras of split type. For an edge , let us denote the maximal subalgebra of split type simply by . Then (where are the labeled edges above), but no automorphism of carries to .
Nevertheless, the isomorphism classes of some subalgebras of a finite dimensional algebra are determined by its automorphism group. For instance, this always holds trivially for . More generally, we could fix a subgroup , and ask which isoclasses of subalgebras of are determined by the action of on its subalgebra poset?
Example 4.15**.**
Let be the Kronecker quiver with two arrows:
[TABLE]
Let . Then up to inner automorphisms there is a unique maximal subalgebra of separable type. By contrast, any one-dimensional subspace of yields a maximal subalgebra of split type. A simple computation shows that if and are any two such subspaces, then and lie in the same -orbit of the subalgebra poset if and only if . However, , and there is an automorphism of taking to . Hence the isomorphism classes of maximal subalgebras of are not determined by the -orbits, but they are determined by the -orbits. In fact, it is not much harder to check that any isoclass of subalgebras of is determined by the -orbits.
The collection of subalgebras determined by -orbits is related to the existence of a certain functor between small categories. Let denote the poset of -subalgebras of . Then the action of on can be considered as a functor , where denotes the category of all small categories. We define to be the colimit of this functor. Its objects are the -orbits of .
Let denote the subcategory of whose objects are the subalgebras of , and whose morphisms are the isomorphisms between such algebras. There is a map on objects which sends a subalgebra of to its -orbit. This map does not necessarily extend to a functor. But if its restriction to a full subcategory is functorial, then isomorphic objects of necessarily lie in the same -orbit of . Furthermore, a union of such full subcategories is another full subcategory with the same property. Hence, there is a unique largest full subcategory of , such that the natural map on objects is a functor. It appears that in general, is difficult to compute.
Example 4.16**.**
Let be the Kronecker quiver from the previous example, and . Then . One can check directly that contains four isomorphism classes, represented by , , , and , respectively.
The reference list from the paper itself. Each links out to its DOI / PubMed record.
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