The representation theory of the wreath product of a finite group with the monoid of all partial functions on a finite set as an EI-category algebra
Abstract
Let be a finite group. We provide a description of the ordinary quiver of the complex monoid algebra of the wreath product , where denotes the monoid of all partial functions on an -element set. This description depends on the multiplicities of simple -modules appearing in the decomposition of tensor products of simple -modules. We also prove that the global dimension of this algebra is . Both results are obtained by analyzing the associated Ehresmann EI-category related to the monoid. Finally, we describe the quiver of the algebra of the wreath product of with the submonoid of all order-preserving partial functions.
1 Introduction
A central aim in the study of monoid representations is to connect them with the general representation theory of associative algebras. Investigating the invariants of the monoid algebra of a finite monoid is of particular interest. Throughout this paper, all modules are over the field of complex numbers , so we consider the complex monoid algebra .
Among invariants of an algebra, the (ordinary) quiver plays a foundational role. A standard way to present a finite-dimensional algebra is via a quiver, which is a directed graph, bound by a set of relations on its paths. In this context, the quiver can be viewed as the generators part in a generators-and-relations presentation of the algebra. Even without explicit knowledge of the relations, the quiver alone encodes a significant amount of data about the algebra.
Determining the quiver of a monoid algebra is a fundamental problem in the representation theory of finite monoids [31, Chapter 17]. To date, descriptions of the quiver have been obtained for many monoids and families of monoids [4, 13, 14, 15, 16, 17, 19, 22, 24, 26, 30, 32]. In particular, in [26], the author described the quiver of the monoid algebra , where is the monoid of all partial functions on an -element set. In this paper, we aim to generalize this result to the complex monoid algebra of the partial wreath product of any finite group with .
Partial wreath products of groups with (partial) transformation semigroups play a crucial role in the Krohn-Rhodes decomposition theory of finite automata and Krohn-Rhodes complexity theory [18]. This monoid was also studied recently in [2, Section 9].
To compute the quiver of the monoid algebra of , we follow the general framework established in [26] for . However, the introduction of the finite group into the structure introduces complications in the underlying representation theory.
After reviewing the necessary preliminaries in Section 2, we introduce several branching rules in Section 3 that will be used in our proof.
The computation of the quiver is carried out in Section 4. Since is a finite -Ehresmann and right restriction semigroup, its algebra is isomorphic to that of its associated Ehresmann category.
This category is the wreath product of with the category of all onto functions between subsets of an -element set (see also [23]). This is an EI-category, meaning that every endomorphism monoid is a group. To determine the quiver of an EI-category algebra, a well-known method (see [16, Section 6.3.1] and [11]) reduces the problem to the representation theory of its endomorphism groups. We follow this approach here.
The endomorphism groups in this case are of the form , where is the symmetric group. This computation utilizes known branching rules for to establish our main result. The description of the quiver itself is given in Theorem 4.10 and relies on the decomposition of tensor products of simple -modules.
We remark that the similar problem of finding the quiver of the wreath product of with the category of injective functions between subsets of an -element set was solved in [27, Section 6]. However, in that case, the structure of the group plays a minimal role in the description.
In Section 5, we prove that the global dimension of is by applying the EI-category framework to lift known results on the global dimension of from [29].
Finally, in Section 6, we compute the quiver of the complex monoid algebra , where is the monoid of all order-preserving partial functions on an -element set. The method is identical to that applied in the case of , but the branching rules are simpler in this setting.
Acknowledgement: The author is grateful to Professor Stuart Margolis for several discussions on the monoid .
2 Preliminaries
2.1 Partial wreath product
Let be a small category. We denote by and the sets of objects and morphisms of , respectively. For , we write for the hom-set of morphisms with domain and range . Recall that a monoid can be viewed as a category with a single object. Following [25], we denote by the category whose objects are finite sets and whose morphisms are partial functions, and by the subcategory consisting of total functions as morphisms.
Let be a finite group with identity element , and let denote the set of all partial functions from to . For every , we denote by its domain. The set is a monoid under pointwise multiplication, where for any , the product has domain and is defined by:
The identity element of this monoid is the constant function mapping every to .
Let be a functor. Define a new category in the following way. The set of objects is the same as the set of objects of , that is, . Given two objects , the hom-set is
Now, given two morphisms and the composition is
It is routine to verify that this composition is well defined and that is indeed a category. If is the identity morphism of and is the function defined by for every , then the identity morphism of the object is . The category is called the partial wreath product of and with respect to . We will apply this construction in two special cases. In the first case, is a functor . In this case, the construction reduces to the standard wreath product of a group with a category (see, for example, [23, 34]). In the second case, is a monoid with identity element . Here the construction is well-known, even when and are semigroups. It appears in [5] in the language of transformation semigroups, and in [10] under the name of 0-wreath products. See also [2, Section 9.1] and references therein. In this case, a functor is an incomplete -action. That is, it consists of a set and a monoid homomorphism . For and , we will write instead of . For every , we write
The monoid acts on the right of by . Explicitly, for , the partial function is given by
In this case, the partial wreath product is a monoid whose underlying set is
The operation is given by
where and the identity element is .
Remark 2.1.
Many authors adopt the convention of composing functions from left to right. Under this convention, the monoid acts on the right of and on the left of . Consequently, the multiplication in is often written in a different form in the literature.
The case where is a group is of great importance. If is a (total) function, we denote by the function defined by for every If is a group, then is a group, and the inverse of is given by
There is a natural incomplete action of the monoid on the set . Formally, the action is given by the identity function . In this case, we simply write for . If , we denote the corresponding wreath product by . In this special case, the wreath product has a natural description using matrices over . For and with , we denote by an matrix over defined by
Let denote the set of all such matrices. Note that each has at most one non-zero entry in each column, so matrix multiplication is well-defined. It is straightforward to verify that the function defined by is a monoid isomorphism.
2.2 Ehresmann semigroups
Let be a semigroup and let be a subset of idempotents. We define two equivalence relations and on .
A subset of idempotents is called a subsemilattice if it is a commutative subsemigroup. It is well known that any commutative semigroup of idempotents has the structure of a semilattice (i.e. a poset where every two elements have a meet) if one defines whenever . A semigroup with a subsemilattice is called right -Ehresmann if every -class contains a unique idempotent from and is a right congruence. We denote the unique idempotent in the -class of by . Note that is the unique minimal element such that . It is well known that is a right congruence if and only if the identity holds for every .
Dually, we can consider semigroups for which every class contains a unique idempotent. We denote the unique idempotent in the class of by . Such a semigroup is called left -Ehresmann if is a left congruence, or equivalently if for every . A semigroup with a subsemilattice is called -Ehresmann if it is both left and right -Ehresmann. The semilattice is also called the set of projections of .
A right (left) Ehresmann semigroup is called right (respectively, left) restriction if the “right ample” (respectively, “left ample”) identity (respectively, ) holds for every and .
For every Ehresmann semigroup , we can associate a category in the following way. The object set of is the set of projections and the morphisms of are in one-to-one correspondence with elements of . For every , we associate a morphism with domain and range and if the range of is the domain of , the composition is defined to be . For more facts and proofs on Ehresmann semigroups and Ehresmann categories, the reader is referred to [6, 7].
2.3 Algebras and modules
Let be an algebra. We will only discuss unital, finite-dimensional -algebras in this paper. Likewise, when we say that is a module over (or an -module or an -representation), we mean that is a finite-dimensional left module over . For and , we write for the action of on the module element . An -module is simple (or irreducible) if is its only proper submodule. The ordinary quiver of a finite dimensional algebra is a directed graph defined in the following way: The vertices of are in a one-to-one correspondence with the simple modules of (up to isomorphism). If and are simple modules of (identified with two vertices of the quiver), then the number of arrows from to is
where is the first right derived functor of , see [20, Chapters 6-7]. More about modules of algebras and quivers can be found in [1].
In this paper, we discuss complex algebras of finite categories. Let be a finite category. The category algebra is a vector space over with the morphisms of as its basis. It consists of all formal linear combinations:
The multiplication in is the linear extension of the following:
The algebra has a unit element given by the sum of the identity morphisms of all objects in :
Since a monoid is a category with a single object, this construction naturally specializes to the definition of a monoid algebra. In this case, the algebra consists of all formal linear combinations of elements of the monoid , with multiplication defined as the linear extension of the monoid operation.
2.4 Complex group representations
Let be a finite group. If is a G-module, we will usually simply say that is a -module (or a -representation). Equivalently, a -module is a pair of a -vector space and a group homomorphism . We denote the set of simple modules of (up to isomorphism) by . It is well known that every -module is a finite direct sum of simple modules and that the number of different simple -modules (up to isomorphism) is the number of conjugacy classes of . We denote the trivial module of any group by . Recall that if is a -module, then is also a -module with operation . Let and be -modules. The inner tensor product is again a -module with action defined by and extending linearly. Now, assume that and are modules of and , respectively. The outer tensor product of and is the ()-module where . Although the two types of tensor product can be distinguished by context, we prefer to use a different notation for the outer tensor product, denoting it by . Similarly, the simple tensors of will be denoted by . It is well known that . The character of the -module is the function defined by . Recall that the multiplicity of as a simple constituent in some -module is given by the inner product of characters
We may omit the subscript when the group is clear from the context. Recall also that , and . In order to simplify notation, we will usually omit and write also for the character of . Hence the above inner product will be written as
Let be a -module and let be a subgroup. The restriction of to is the -module defined by
that is, restricting the homomorphism to the subgroup . Note that and if is a simple -module, then does not have to be a simple -module. Let be an -module, the induction to , denoted is the tensor product
where the action is given by
where and . However, we will also use the following more concrete description. Choose to be representatives of the left cosets of in (where ). Note that any element can be written in a unique way as where and . Every element of is a formal sum of the form
where and . In other words, as a vector space is , that is, copies of . The action is defined on elements of the form by
where and are unique such that . The required action is given by extending linearly. Note that . It is important to mention that the modules and depend not only on the groups and but also on the specific embedding of into . Hence, we will have to give the specific embeddings when discussing these modules. Both induction and restriction are transitive and additive, that is, if then
and
For the restriction this is a trivial statement, and for the induction the proof is [3, Propositions 1.1.10 and 1.1.11]. An important fact that relates induction to restriction is the following one (for a proof, see [3, Corollary 1.1.20 ]).
Theorem 2.2 (Frobenius reciprocity).
Let and let and be and -modules respectively. Then the multiplicity of in equals the multiplicity of in .
Using characters, Frobenius reciprocity can be written as the following equality
Let be a -module. Consider the swap transformation defined on simple tensors by . We define the symmetric square and the alternating square as the following submodules of the tensor product :
As -modules, . The characters of these modules are given by:
2.5 Representation theory of and
We will recall some elementary facts regarding the representation theory of the symmetric group. More details can be found in [9, 21]. Recall that an integer composition of is a tuple of non-negative integers such that while an integer partition of (denoted ) is an integer composition such that . From now on, when dealing with a partition we will write its elements in superscript because we want to reserve the subscript for multipartitions. Note that has one partition, namely the empty partition, denoted by . We can associate to any partition a graphical description called a Young diagram, which is a table with boxes in its -th row. For instance, the Young diagram associated to the partition of is:
We will identify the two notions and regard integer partition and Young diagram as synonyms. It is well-known that simple modules of are indexed by integer partitions of . We denote the simple module associated to the partition (also called its Specht module) by . An explicit description of can be found in [21, Section 2.3]. It will be often convenient to draw the diagram instead of writing . For instance we may write
instead of: for partitions and .
Let be an integer composition of . A tuple such that for every is called a multipartition of with components. We also call it a multipartition of the composition and denote this by . We define a multi-Young diagram to be a tuple of Young diagrams. As we identify partitions with Young diagrams, we also identify multipartitions with multi-Young diagrams.
Let be a finite group with conjugacy classes. It is well-known ([3, Theorem 2.6.1]) that multi-Young diagrams with boxes and components index the simple modules of the wreath product . If is a multi-Young diagram, then we denote by its associated -module.
3 Branching rules
Let be a finite group with conjugacy classes. Fix to be its set of simple modules. In this section we will describe several known branching rules for the group that we will need later on.
3.1 Restriction of
Let be the symmetric group of order where will always be the swap permutation. We denote by the trivial module of and by the sign module of . The group can be embedded in by . In this section, we study the restriction . Every simple module of is of the form or where (). The description of simple modules of is more complicated, but well-known (see [3, Chapter 2] for the description of simple modules of in general). If are two non-isomorphic simple modules of then is a simple module. Clearly, embeds in by . One type of simple module is obtained by induction . This gives us simple modules. Note that . The module corresponds to the multipartition with and for . Given , another type of simple module is the tensor product where the action is
We denote this simple module by . This gives another simple modules. The module corresponds to the multipartition with and for . Finally, we denote by the inflation of to a module. This means that acts like . The last simple modules of are obtained by the tensor product and we denote them by . The module corresponds to the multipartition with and for . In total, we have simple modules for .
Remark 3.1.
In the literature, the module is defined by the action
(in fact, with , but in our case.) This variation arises because, in the context of groups, the composition in the wreath product is defined by
where . As shown in [27, Lemma 6.3], the two definitions are isomorphic under the map
but it changes the concrete description of the module . In any case, we are interested in the action of elements of the form . For such elements, the two actions coincide, ensuring there is no ambiguity in our context.
The characters of these modules are well-known and essential for computing the desired restriction. Recall that we use the same notation for a module and its character. If we take and as representatives of the cosets of in , it is easy to see that swaps the cosets and fixes them. The character of the induction is summation of the base character over the fixed cosets (see [21, Section 1.12]). Therefore, the character for an element is given by:
For the modules and , the character values on the elements are given as follows (see [9, 4.3.10 (vi), p. 150]):
and
Lemma 3.2.
The multiplicities of and in are both equal to the multiplicity of in .
Proof.
Let be either the trivial module or the sign module of . The multiplicity of in the restriction is:
As , the sum over only has a contribution from . Since for both the trivial and sign modules, the expression becomes:
which completes the proof. ∎
Lemma 3.3.
The multiplicities of and in the restrictions and are given by the multiplicities of in and as follows:
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1.
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2.
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3.
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4.
Proof.
We prove the first case; the others follow by similar character computations. By the definition of the inner product of characters on , we have:
Substituting the character values and , we obtain:
The term in parentheses is precisely the character of . Thus, the expression reduces to , which is the multiplicity of in . ∎
3.2 Littlewood-Richardson rules for small additions
Let be a group with conjugacy classes. The group is naturally embedded in . If and we define by
Then, the natural embedding is defined by where () can be regarded as an element of that fixes (). The branching rules for describing the induction from to are known (see [8, Theorem 4.7] or [27, Theorem 4.5]), but we will give here only the cases for as this is what we need in this paper.
Let be a composition of and let be a multi-Young diagram and let be the associated -module. Let be a -module. We can think of it as a multi-Young diagram with one box in the -th component and all the other components are empty. Let be the set of multi-Young diagrams that can be obtained from by adding one box at the -th component. Conversely, let be the set of multi-Young diagrams obtained from by removing one box from the -th component.
Proposition 3.4.
The induction and restriction rules are as follows:
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1.
Induction:
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2.
Restriction: By Frobenius reciprocity, the restriction of a -module to the subgroup is given by:
For the case , we define the sets of multi-Young diagrams obtained by adding exactly two boxes to :
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: one box added to component and one box added to component ().
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: a horizontal strip of two boxes added to component . This means that we cannot add the two boxes in the same column.
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: a vertical strip of two boxes added to component . This means that we cannot add the two boxes in the same row.
Proposition 3.5.
The induction from to for the various simple -modules is given by:
4 The quiver of
4.1 Ehresmann structure
For every we define to be the partial identity of the set
and to be the function
Set and note that this is a subsemilattice of . It is routine to verify that the idempotent is a left (right) identity of if and only if (respectively, ). Therefore, we have that two elements and of are -related if and only if , and they are -related if and only if . In other words, if and then
In [2, Proposition 9.11], it was proved that is a right -restriction monoid. It is also easy to prove that the left congruence condition holds.
Lemma 4.1.
The relation is a left congruence on .
Proof.
Let such that . This is equivalent to . Let be any element in . Note that so
Thus, is a left congruence. ∎
It follows that is a -Ehresmann and right restriction monoid. This will be crucial in view of the following fact.
Theorem 4.2 ([28, Theorem 1.5]).
Let be a finite -Ehresmann and right restriction monoid and let be its associated Ehresmann category. Then, for every unital commutative ring there is an isomorphism of algebras
Therefore, we can switch to studying the representation theory of the associated category . We start by describing it. The objects of are in one-to-one correspondence with the elements of . Thus, the objects are of the form for . For two subsets , the hom-set is identified with the elements such that
Note that in this case, and . We denote by the morphism associated with .
Let be the category defined as follows. The objects of are subsets . For , the hom-set contains all the onto (total) functions . Let be a group. We denote by the wreath product , where is the inclusion functor.
Proposition 4.3.
There is an isomorphism of categories .
Proof.
It follows immediately from the above discussion. Formally, an isomorphism
is defined by and . Note that if is a morphism in , then and , so is indeed a total onto function . Moreover, , so as required in the definition of . It is easy to see now that is an isomorphism. ∎
4.2 The skeleton
If and are equivalent categories, then their algebras are Morita equivalent (see [33, Proposition 2.2]). Since the quiver of an algebra is an invariant of Morita equivalence, we can switch our attention to a simpler category which is equivalent to .
We can take a full subcategory with one object from every isomorphism class in . This category is called the skeleton of . To describe it, we first have to characterize which objects in are isomorphic.
Lemma 4.4.
Two objects in are isomorphic if and only if .
Proof.
First, note that if , then the hom-set is empty because there are no onto functions from to . If and are isomorphic, then both and are non-empty, which implies .
Conversely, if , we can take any invertible function , and we claim that is an isomorphism with inverse . Indeed,
Note that since , we have . Therefore,
which is the identity morphism of the object . Likewise, since , it follows that . ∎
Denote by the full subcategory of whose objects are the sets and for . As the notation suggests, this category can be identified with the wreath product of with the category , where the set of objects is and the morphisms are total onto functions. Following the discussion above, to determine the quiver of the original algebra, it suffices to focus our attention on the quiver of the algebra .
It is also convenient to describe using matrices. Let be the category defined as follows. The set of objects of is . For , the hom-set consists of all matrices over with exactly one non-zero element in every column and at least one non-zero element in every row. Composition of morphisms is given by standard matrix multiplication, which is well-defined because each column contains only one group element.
It is straightforward to see that there is an isomorphism of categories . To each morphism , we associate an matrix defined by:
By construction, the -th column of contains a unique non-zero element in the -th row. The condition that is surjective implies that every row contains at least one non-zero element. It is routine to verify that this assignment respects composition and thus defines an isomorphism of categories.
4.3 The quiver of a skeletal EI-category algebra
A category is called an EI-category if its endomorphism monoids are groups. In other words, in an EI-category, every endomorphism is an isomorphism.
The category is an EI-category because for any morphism , the map is a surjective map from a finite set to itself, which is necessarily a bijection. Therefore, the endomorphism monoid of an object is the group .
The problem of finding the ordinary quiver of the complex algebra of a skeletal EI-category can be reduced to a problem in group representation theory. We define a few concepts below and then state the relevant theorem.
For any finite set , we denote by (or ) the complex vector space consisting of all formal linear combinations of elements of . If a group acts on , then naturally becomes a -module called a permutation module.
Let be a finite EI-category. A morphism is called irreducible if it is not an isomorphism, and whenever , either or is an isomorphism. We denote the set of irreducible morphisms from object to object by . Recall that we denote the set of simple modules of a group by .
Theorem 4.5 ([16, Theorem 6.13], [11, Theorem 4.7]).
Let be a finite skeletal EI-category and let be the quiver of . Then:
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1.
The set of vertices of is given by
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2.
The vector space can be viewed as an -module with the action given by . For and , the number of arrows from to is the multiplicity of as a simple constituent in .
In view of the theorem above, the vertices of the quiver of are indexed by the simple modules of the automorphism groups for each object in . Since has conjugacy classes, these modules are indexed by multipartitions (or equivalently, multi-Young diagrams) with boxes and components, where varies from to .
4.4 Irreducible morphisms
The next step for using Theorem 4.5 is identifying the irreducible morphisms of .
Lemma 4.6.
The irreducible morphisms of are precisely the morphisms from to for . In other words,
Proof.
It is clear that every morphism from to is irreducible. Indeed, if one decomposes , the size of the sets implies that one of the factors must be an endomorphism and hence an isomorphism.
Now, if where , then it is known that we can write for some onto functions and (see [26, Lemma 3.3]). In this case, and are both well-defined morphisms which are not endomorphisms and therefore are not invertible. Finally,
so is not irreducible. ∎
Let and . If , there are no arrows in the quiver of from to because is empty. Consequently, we focus on the case and examine the module under the action of as described in Theorem 4.5.
For convenience, we denote the set of irreducible morphisms by
The group acts on via
where , , , and . The module of interest is the linearization , which is a permutation module for this action.
4.5 Description of the action and stabilizer
Lemma 4.7.
The action of on is transitive.
Proof.
We show that every element of lies in the orbit of , where is defined by
Let . It is easy to verify (also mentioned in [26, Section 3]) that the action of on the set of surjective maps from to is transitive. Thus, there exist and such that .
Taking and , we observe that:
Thus, the action is indeed transitive. ∎
Let be the stabilizer of under the action of described above, and let denote the trivial module of . Since is a permutation module arising from a transitive group action, it follows that
To proceed, we must characterize the stabilizer more explicitly.
For the action of on the set of surjective maps from to , it is known that the stabilizer of is the subgroup
(see [26, Lemma 3.5]). For any function , let be the function defined by
Note, in particular, that .
Recall that we can view any element as an element of that fixes .
Lemma 4.8.
The stabilizer of under the action of is given explicitly by
Proof.
An element is in if and only if
or equivalently,
Applying the product rule for the wreath product on both sides, we obtain
Since is the identity for the pointwise product, this simplifies to the condition
The map equality implies that is in the stabilizer of under the action of . It follows that and for some .
Finally, the function equality is equivalent to . Indeed, for , we have , and for , we have . This completes the proof. ∎
For any and , we define a function by
Note that every can be uniquely written as for some and .
In what follows, it will be useful to understand how elements of correspond to matrices over . Given an element with , its associated matrix consists of an block associated with and a block containing . Thus, corresponds to a block-diagonal matrix:
For the element , the associated matrix similarly decomposes into two blocks of sizes and . The first block is , and the second is the block , where is the permutation matrix associated with :
Lemma 4.9.
There is an isomorphism of groups
Proof.
Identify with . We define a map by
By Lemma 4.8, it is clear that is a bijection. It remains to show that is a group homomorphism. Indeed,
On the other hand
First note that
because and have disjoint supports and thus commute as elements of . Next, for , we have
because as well. For , we have
since fixes . This establishes that
Proving the last equality is similar. For , we have again
and
because for all . Finally, for , we have
and
where the last equality follows because fixes and takes the value on both and . This completes the proof. ∎
4.6 The quiver computation
Let and . To simplify the notation, we shall use the same notation for a module and its character. For example, we write and in place of and .
The number of arrows in the quiver of from to is the multiplicity of as a simple module in the -module
This multiplicity can be expressed as the inner product of characters:
Using Frobenius reciprocity, this equals
According to Lemma 4.8, a general element of is of the form
where . Therefore,
Now, if we think of as a and block matrix, it is just a general element of so we can write
Likewise, if we view as a and block matrix, it is a general element of so
In order to view this also as a module we will write this as
where is the trivial module of . Therefore, we obtain
By Frobenius reciprocity, this equals
By transitivity of induction we obtain
Now we analyze this expression using the branching rules described in Section 3. Let be a simple module of corresponding to a multipartition .
By Proposition 3.4, we have
where means that is obtained by removing one box from the -th component of . Let be one component in this summation. The next step is to compute the induction
For this we need to compute the induction
Let be the multiplicity of in , let be the multiplicity of in , and let be the multiplicity of in . According to Lemma 3.2 and Lemma 3.3 we have that
so
Finally, by Proposition 3.5 we have that
From this we can conclude:
Theorem 4.10.
Let be a group with conjugacy classes and let . Define as above. The quiver of the monoid is described as follows. The vertices correspond to multi-Young diagrams with components and boxes, where varies from to . Let be a multi-Young diagram with boxes, and be a multi-Young diagram with boxes. If , then there are no arrows from to . If , then the number of arrows depends on the ways that can be constructed from by removing one box and adding two. For each way that can be constructed from by removing one box from the -th component and adding one box in components and () we add arrows. In each way that can be constructed from by removing one box from the -th component and adding two boxes on the -th component but not on the same column we add arrows. In each way that can be constructed from by removing one box from the -th component and adding two boxes on the -th component but not on the same row we add arrows.
4.7 Examples
4.7.1 The quiver of
If is the trivial group then . In this case, contains only the trivial module . Clearly and . Therefore, and . Therefore, we retrieve [26, Theorem 3.8]:
Theorem 4.11.
The vertices of the quiver of the monoid algebra correspond to Young diagrams with boxes where varies from to . Let be a Young diagram with boxes and be a Young diagram with boxes. If , then there are no arrows from to . If , then the number of arrows from to is the number of ways that can be constructed from by removing one box and adding two, but not in the same column.
4.7.2 Generalized monoid of partial functions
Let be the cyclic group with elements, say where . All simple modules are one-dimensional. There are such modules, for , defined by:
where is a primitive -th root of unity. These modules satisfy , where the sum is taken modulo . Since each is one-dimensional, its symmetric square and alternating square satisfy:
Therefore, the decomposition coefficients for the tensor product are given by if and zero otherwise. For the symmetric and alternating squares, the coefficients are if and zero otherwise, while for all . We end with the following result:
Theorem 4.12.
The vertices of the quiver of the monoid algebra correspond to mutli-Young diagrams with components, indexed , and boxes, where varies from to . Let be a multi-Young diagram with boxes and be a multi-Young diagram with boxes. If , then there are no arrows from to . If , then the number of arrows depends on the ways that can be constructed from by removing one box and adding two. For each way that can be constructed from by removing one box from the -th component and adding one box in components and we add an arrow if . In each way that can be constructed from by removing one box from the -th component and adding two boxes on the -th component but not on the same column we add an arrow if .
Example 4.13.
Consider the case . The quiver of the algebra is given by the following figure:
The first component of each multi-Young diagram corresponds to the trivial module , while the second component corresponds to the alternating module .
Notably, there are two arrows from to . This multiplicity arises because the branching construction can be satisfied in two distinct ways:
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First, by removing one box from the first component () and adding two boxes in the same row, which is valid since .
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•
Second, by removing one box from the second component () and adding one box to each component, which is valid since .
4.7.3 The quiver of
We now consider the case of the smallest non-abelian group . The set contains three simple modules: The trivial module , the sign module , and the standard module . It is well-known and easily verified by character considerations that the symmetric and alternating squares satisfy:
Furthermore, the tensor products are given by:
Therefore, the coefficients are given by:
The coefficients , where , satisfy:
Finally, for the coefficients , where , we have:
Therefore, we obtain:
Theorem 4.14.
The vertices of the quiver of the monoid algebra correspond to multi-Young diagrams with total boxes, where . Let be a multi-Young diagram with boxes and be a multi-Young diagram with boxes.
If , there are no arrows from to . If , the number of arrows from to is the number of ways can be constructed from by removing one box and adding two boxes according to the following rules:
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•
Remove one box from and add two boxes to any one component, provided they are not in the same column.
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•
Remove one box from and add one box to and one box to .
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•
Remove one box from and add two boxes to , provided they are not in the same row.
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•
Remove one box from and add one box to or and another box to .
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•
Remove one box from and add two boxes to , provided they are not in the same column.
Example 4.15.
The quiver of the algebra is given by the following figure:
5 Global dimension of
In this section, we prove that the global dimension of the algebra is based on the results established for the algebra in [29]. We show that every projective module of can be lifted to a corresponding projective module of , allowing us to transfer the known homological properties to the wreath product case.
5.1 The global dimension of an algebra
Let be a finite-dimensional -algebra. An -module is projective if the functor is exact, or equivalently, if is a direct summand of a free module. A module is indecomposable if it cannot be written as a direct sum of two non-zero submodules. Every projective -module decomposes into a direct sum of indecomposable projective modules.
These modules are classified by the idempotents of the algebra. Two idempotents are orthogonal if . An idempotent is primitive if it cannot be written as a sum of two non-zero orthogonal idempotents. A set is a complete set of orthogonal primitive idempotents if the elements are pairwise orthogonal, each is primitive, and . Every indecomposable projective -module is isomorphic to for some primitive idempotent , and a complete set of primitive orthogonal idempotents yields all indecomposable projectives up to isomorphism.
Let be a finite-dimensional -algebra. The Jacobson radical of , denoted , is defined as the intersection of all maximal left ideals of . Equivalently, is the unique maximal nilpotent two-sided ideal of . For any finite-dimensional -module , we define its radical, , as the intersection of all maximal submodules of . A fundamental property of the radical is that it can be computed via the action of the algebra’s radical. Specifically, we have the identity .
Let be a finite-dimensional -algebra and an -module. A projective cover of is a pair , where is a projective -module and is a surjection such that .
For the algebras considered here, every finite-dimensional module admits a projective cover, which is unique up to isomorphism.
Let be a finite-dimensional -algebra and an -module. A projective resolution of is an exact sequence of the form
where each is a projective -module. Such a resolution is called minimal if is the projective cover of , and for each , is the projective cover of .
Every finite-dimensional module possesses a minimal projective resolution, which is unique up to isomorphism of complexes. The projective dimension of , denoted , is the length of its minimal projective resolution, that is, the largest integer such that (or infinity if the resolution does not terminate). For a finite-dimensional algebra , the global dimension of , denoted , is the supremum of the projective dimensions of all simple -modules:
The global dimension is an invariant of the Morita equivalence class of the algebra . If two algebras are Morita equivalent, their global dimensions are equal. Moreover, it is a known fact for finite-dimensional algebras that the global dimension is bounded above by the length of the longest path in the quiver of the algebra.
5.2 Lifting projective resolutions of EI-categories
Let be a category and be a finite group. For simplicity, assume that is a subcategory of so that there is a natural wreath product . Clearly, every -module can be inflated to a -module via the action . We denote the inflation of to by . In fact, we consider as a functor between the category of -modules and -modules. In this subsection, we show that if is an EI-category the inflation functor lifts the minimal projective resolution of to the minimal projective resolution of .
Let be an EI-category. For every object , we denote by the associated endomorphism group, and let be a complete set of orthogonal primitive idempotents of . It is known (see [12, Lemma 9.31] or [33, Corollary 4.5]) that we can obtain a complete set of orthogonal primitive idempotents of by taking the union of all complete sets of orthogonal primitive idempotents of the endomorphism groups:
Therefore, if is a simple -module isomorphic to for some , then
is an indecomposable projective module of . Moreover, every indecomposable projective module is isomorphic to for some and .
It is straightforward to verify that is also an EI-category with the same set of objects . For any object , the associated endomorphism group in the wreath product category is . Given a simple module , its inflation is a module over , which remains simple under the action defined previously. The relationship between the inflation functor and the indecomposable projectives is captured by the following lemma.
Lemma 5.1.
Let and . Then there is an isomorphism of -modules:
Proof.
We denote by the function in that maps every element of the set to the identity and by we denote the identity function of . To establish the isomorphism
we first observe that for every and we have
Next, define a linear map
on simple tensors by
where and . To see that is well-defined, note that for any , the inflation action on satisfies . Thus,
which confirms respects the tensor relation over .
To verify that is a -module homomorphism, let where and let where . By the definition of the inflation action, we have:
On the other hand, acting on the image gives:
To prove that is an isomorphism, we construct its inverse
Define on spanning elements by . To show that is well-defined, let ; then:
On the other hand:
Thus is well-defined.
To show that is a -module homomorphism, let and be a spanning element of the domain. We have:
On the other hand, acting after applying gives:
so is a -module homomorphism.
From the definitions it follows immediately that is the identity on , as:
Conversely, for any in the target, we previously established the identity . Therefore:
which shows is the identity. Thus, is an isomorphism of -modules. ∎
As a consequence of the fact that inflation preserves the structure of indecomposable projective modules, we obtain the following result regarding general projective modules.
Corollary 5.2.
If is a projective -module, then its inflation is a projective -module.
Proof.
Each projective -module can be decomposed into a direct sum of indecomposable projectives, each isomorphic to for some and . According to Lemma 5.1, the inflation of each such indecomposable projective is an indecomposable projective -module. Since the inflation functor preserves direct sums, it follows that is a direct sum of projective modules and is, therefore, projective. ∎
The next step is to characterize the radical of an EI-category algebra.
Proposition 5.3 ([11, Proposition 4.6]).
Let be a finite EI-category. The radical is the subspace spanned by all non-invertible morphisms in .
In an EI-category, a morphism is non-invertible if and only if its domain and codomain are not isomorphic ().
Lemma 5.4.
Let be a projective -module. Then .
Proof.
First, assume is an indecomposable projective module. Then for some and . The radical of is given by . Using the characterization of the radical for EI-category algebras, and are spanned by the set
On the other hand, by Lemma 5.1, . The radical of the latter is , which is spanned by simple tensors of the form where and . As shown in the proof of Lemma 5.1, .
Under the isomorphism , the image of the spanning set
is exactly the set defined above. Therefore, also spans . Since both and are spanned by the same set of elements within , we have .
The result for a general projective module follows immediately from the fact that is a direct sum of indecomposable projectives and both the radical and the inflation functor preserve direct sums. ∎
Lemma 5.5.
Let be a -module and let be its projective cover. Then is the projective cover of the -module .
Proof.
Recall that a surjective homomorphism is a projective cover if and only if is a projective module and .
Applying yields
and it is clear that is surjective and .
Next, we know from Lemma 5.1 that is a projective -module. Finally, applying the result of our previous lemma, we have:
Since is projective and the kernel of the surjection is contained in its radical, is the projective cover of . ∎
Corollary 5.6.
Let be a minimal projective resolution of a -module . Then the inflated sequence is a minimal projective resolution of the -module .
Proof.
Let be the resolution . It is easy to verify that is an exact functor. Therefore, the sequence
is exact. By Lemma 5.1, each is a projective -module.
By definition, the resolution is minimal if is a projective cover and each induces a projective cover . By Lemma 5.5, inflation preserves the projective cover property. Thus, is the projective cover of and each induces the projective cover of . It follows that is a minimal projective resolution. ∎
Corollary 5.7.
The inflation functor preserves the projective dimension of modules. That is, for any -module , we have
5.3 The Global Dimension
Finally, we apply the preceding results to compute the global dimension of . Recall that is the EI-category whose objects are the subsets of and whose morphisms are onto functions. Since is Morita equivalent to the category algebra , we may instead determine the global dimension of the latter.
Theorem 5.8.
The global dimension of the category algebra is .
Proof.
We first establish as an upper bound. The global dimension is bounded above by the length of the longest path in the quiver of the algebra. In Theorem 4.10, we characterized the vertices of the quiver as multi-Young diagrams. Specifically, we showed that if is a multi-Young diagram with boxes and is one with boxes, an arrow can only exist if . Furthermore, there are no arrows directed toward the vertex corresponding to a multipartition with 0 boxes (the ”bottom” element). Consequently, the longest directed path in the quiver has length , which provides the required upper bound: .
For the lower bound, we consider the -simple module corresponding to the partition . It was shown in [29, Corollary 6.9] that . By Corollary 5.7, the inflation functor preserves projective dimension, implying:
Since the global dimension of an algebra is the supremum of the projective dimensions of its simple modules, it follows that . Combining these bounds, we conclude that the global dimension is exactly . ∎
Corollary 5.9.
For every finite group , the global dimension of the monoid algebra is .
6 The quiver of the wreath product of a group with the monoid of all order-preserving partial functions
A partial function is called order-preserving if for every in the domain of . Let be the submonoid of consisting of all order-preserving partial functions. In this section, we describe the quiver of the complex algebra .
In this case, the wreath product is
Recall the set of idempotents , which forms a subsemilattice of . It is a straightforward consequence that is an -Ehresmann and a right restriction monoid.
Let be the subcategory of the category , defined in Section 4.1, which has the same set of objects but whose morphisms consist of surjective, total order-preserving functions. It follows that is the Ehresmann category associated with . Thus, by Theorem 4.2, we obtain an isomorphism of algebras
Following the approach in Section 4.2, we now consider the skeleton of . If is an order-preserving bijection, then its inverse is also order-preserving. Consequently, Lemma 4.4 implies that two objects and of are isomorphic if and only if . Let denote the category whose objects are for , and whose morphisms are surjective, total order-preserving functions. The skeleton of is then the wreath product . Our goal now is to describe the quiver of the algebra .
The endomorphism groups in have a straightforward structure. Since the only order-preserving bijection from to itself is the identity map, the endomorphism group of any object in is simply the direct product .
By applying Theorem 4.5 to the skeletal category , the set of vertices of is the disjoint union of the simple modules of the endomorphism groups of the objects in the skeleton. Since the endomorphism group of the object is isomorphic to , the vertex set is:
Any simple module of is an outer tensor product of simple modules of . Thus, the vertices of the quiver are naturally indexed by sequences of length , where each . So the vertex set is:
For , the unique vertex is the trivial module of the trivial group .
Our next step is to identify the irreducible morphisms in the category .
Lemma 6.1.
The irreducible morphisms of are precisely the morphisms from to for . That is,
Proof.
As in the proof of Lemma 4.6, any morphism from to is clearly irreducible because any factorization would force one of the factors to be an isomorphism. Conversely, suppose with . Since is a surjective order-preserving function, it is known that factors as , where and are both surjective order-preserving functions (see [26, Lemma 5.1]). We may then define the morphisms and . Since neither nor is a bijection, these factors are not invertible in . Their product is
which shows that is not irreducible. ∎
Let and be vertices of the quiver. If , there are no arrows in the quiver of from to because is empty. Consequently, we focus on the case and examine the structure of as a -module, with the action defined in Theorem 4.5.
A morphism in is a pair , where is a surjective order-preserving function and . It is easy to see that there are exactly surjective order-preserving maps from to , denoted . The map is defined by:
so for some . Set and define
We naturally identify with .
Lemma 6.2.
The -module decomposes as a direct sum of submodules:
Proof.
Since the set of all such pairs forms a basis for , and since the are disjoint except for the zero vector and their union spans , we can write as a direct sum of vector spaces
To show this is a decomposition of -modules, we examine the action defined in Theorem 4.5. For and , the action on a basis element is:
Since and by calculating the product in the wreath product category:
Crucially, the underlying order-preserving map remains unchanged by the action of the endomorphism groups so each subspace is a submodule of . ∎
For each , let denote the natural basis for the subspace . By Lemma 6.2, the action of preserves and maps basis elements to basis elements. Consequently, we can view as the permutation module arising from the action of on the set . To analyze the structure of this permutation module, we first establish that this action is transitive.
Lemma 6.3.
For each , the action of on the set is transitive.
Proof.
Let be the element of where is the constant function mapping every element of to . For any arbitrary , we choose . Applying the action, we have:
This shows that any element of can be reached from , and thus the action is transitive. ∎
The transitivity of the action allows us to identify each as a permutation module induced by the stabilizer of our chosen base point. Let denote the stabilizer of in .
Lemma 6.4.
For each , the stabilizer of the element is given by
Proof.
An element belongs to if and only if . This condition is satisfied if and only if:
Equating the first components, we obtain the equation , which implies . ∎
In particular, the elements of are in one-to-one correspondence with . Note that if we write as , then
.
Since is a transitive permutation module, we have the following isomorphism of -modules:
For each , we define a group monomorphism by . Explicitly, for , we have
It is easy to verify that this is indeed a group monomorphism.
Proposition 6.5.
Let and . For each , the multiplicity of the simple -module in is equal to the multiplicity of in the induced module , where the induction is taken along the group homomorphism . In terms of characters, this is expressed as:
Proof.
Using the character of the permutation module as identified in Lemma 6.4:
Applying Frobenius reciprocity:
As a summation, we have:
Note that where the restriction is taken along the homomorphism .
Therefore, the final expression becomes:
Finally, applying Frobenius reciprocity again, we obtain:
This completes the proof. ∎
Clearly, since acts as the identity on all coordinates , investigating the induction from to along reduces to understanding the induction from to along the diagonal homomorphism .
Lemma 6.6.
Let . The multiplicity of in the induced module is equal to the multiplicity of in the tensor product as a -module.
Proof.
By Frobenius reciprocity for the group pair , we have:
The restriction of the external tensor product to the diagonal subgroup is the internal tensor product . Substituting this into the inner product, we obtain:
∎
Lemma 6.7.
Let and . The multiplicity of in is non-zero only if:
-
•
for all ,
-
•
for all .
In this case, the multiplicity is given by the multiplicity of in the tensor product .
Proof.
From Proposition 6.5, we have:
Since the induction along is the identity on all components except the -th one, where it is the diagonal induction, we have:
Comparing this with , the result follows from Lemma 6.6. ∎
If we use the Kronecker delta notation:
then the multiplicity formula can be expressed compactly as:
In order to obtain the number of arrows from to all is left is to sum this number over from to . We can conclude:
Theorem 6.8.
The quiver of the algebra or, equivalently, is constructed as follows:
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•
Vertices: The set of vertices is the disjoint union , where each vertex is a simple module of the form with .
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•
Arrows: For any and , the number of arrows from to is given by the sum:
where is the multiplicity of in the tensor product as a -module.
Example 6.9.
We illustrate Theorem 6.8 by constructing the quiver of the algebra . The group has two simple modules: the trivial module and the sign module .
The tensor product rules for these modules are straightforward:
The quiver is a bit crowded, and given by:
Note that a multiplicity of two between vertices is denoted by a double-lined arrow.
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