Tensor product of correspondence functors
Serge Bouc, Jacques Th\'evenaz

TL;DR
This paper explores the tensor product structure of correspondence functors, demonstrating that those associated with finite lattices form commutative algebras within the tensor category.
Contribution
It introduces the tensor product of correspondence functors and proves that functors from finite lattices are commutative algebras in this context.
Findings
Correspondence functors can be tensor-multiplied with well-defined properties.
Functor associated with finite lattices forms a commutative algebra.
Main properties of the tensor product are established.
Abstract
As part of the study of correspondence functors, the present paper investigates their tensor product and proves some of its main properties. In particular, the correspondence functor associated to a finite lattice has the structure of a commutative algebra in the tensor category of all correspondence functors.
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Tensor product of correspondence functors
Serge Bouc
and
Jacques Thévenaz
Abstract.
As part of the study of correspondence functors, the present paper investigates their tensor product and proves some of its main properties. In particular, the correspondence functor associated to a finite lattice has the structure of a commutative algebra in the tensor category of all correspondence functors.
Key words and phrases:
finite set, correspondence, relation, functor category, tensor product
2010 Mathematics Subject Classification:
06B05, 06B15, 06D05, 06D50, 16B50, 18B05, 18B10, 18B35, 18E05
1. Introduction
In recent papers [BT2, BT3, BT4], we developed the theory of correspondence functors, namely functors from the category of finite sets and correspondences to the category of all -modules, where is a commutative ring. This theory turns out to be very rich and we describe here another piece of structure. We introduce the tensor product of any two correspondence functors (Section 3) and analyse its main properties, such as projectivity, finite generation, and behaviour under induction (Section 5).
Whenever and are correspondence functors, we not only define their tensor product , but also their internal hom , which satisfies the usual adjointness property (Section 6). The constructions and its properties depend on the symmetric monoidal structure on given by the disjoint union of finite sets. We also show that our construction turns out to be an instance of the general construction known as Day convolution.
A main instance of correspondence functors is the functor associated to a finite lattice , as defined in [BT3]. We prove in Section 4 that . Finally, in Section 7, we show that carries the additional structure of a commutative algebra in the tensor category of all correspondence functors. We prove conversely that, over a field (or more generally if is connected), any commutative algebra in the tensor category is isomorphic to for some finite lattice , provided it satisfies two additional conditions, one of them being of an exponential nature (see Theorem 7). A few small examples are discussed in Section 8.
Throughout this paper, denotes a fixed commutative ring and all modules are left -modules.
2. Correspondence functors
In this section, we recall the definitions and basic properties of correspondence functors. We refer to Sections 2–4 of [BT2] and Section 2 of [BT3] for more details. We denote by the category of finite sets and correspondences. Its objects are the finite sets and the set of morphisms from to (using a reverse notation which is convenient for left actions) is the set of all correspondences from to , namely all subsets of . Given two correspondences and , their composition is defined by
[TABLE]
The correspondence is a unit element for this composition. A correspondence from to is also called a relation on . In particular,
[TABLE]
is a -algebra, the algebra of the monoid of all relations on .
For our fixed commutative ring , we let be the -linearization of . The objects are again the finite sets and is the free -module with basis . A correspondence functor over is a -linear functor from to the category of all -modules. We let be the category of all correspondence functors over (for some fixed commutative ring ).
If is a correspondence functor and is a correspondence, then acts as a linear map and we simply write for this left action. In other words, for any , we define
[TABLE]
In particular, we have for any correspondence .
The following examples have been introduced in [BT2] and [BT3] respectively.
2.1. Example.*
*For any finite set , the representable functor is a projective correspondence functor by Yoneda’s lemma.
More generally, for any left -module , there is a correspondence functor
defined by
[TABLE]
This is left adjoint to the evaluation at , in the sense that it satisfies the adjointness property
[TABLE]
This example is used in [BT2], but it is in fact a general construction for representations of categories which goes back to [Bo]. In particular, it is used for the construction of simple functors. **
2.2. Example.*
*The constant functor is defined by for any finite set
and for any and any correspondence .
Actually, it is elementary to check that , so in particular is projective.
**
2.3. Example.*
*For any finite lattice , let for any finite set ,
where is the set of all maps and denotes the free -module with basis .
The action of a correspondence on a function is a function defined by the join
[TABLE]
with the usual comment that the join over an empty set yields the least element of the lattice. It is easy to check that this defines a correspondence functor (see [BT3]).
Recall that a join-morphism of finite lattices is a map such that for any subset of . In particular, must be order-preserving. Moreover, the case when is empty shows that , where denotes the least element of any lattice. Any join morphism induces a morphism of correspondence functors by composition with . **
3. Tensor product
In this section, we define the tensor product of two correspondence functors and discuss its basic properties.
3.1. Definition.* Let and be correspondence functors over . The tensor product of and is the correspondence functor defined as follows. For any finite set ,*
[TABLE]
If is a finite set and , then acts as a -linear map
[TABLE]
defined by
[TABLE]
The properties of this tensor product use the symmetric monoidal structure on given by the disjoint union of finite sets, which we write throughout this paper. More precisely, if are finite sets, and if and , then the disjoint union can be viewed as a subset of . We will represent this correspondence in the matrix form
[TABLE]
This yields a bifunctor , still denoted by a disjoint union symbol.
We also use the following matrix notation. If and , then
[TABLE]
denotes the obvious subset of . Similarly, if and , then
[TABLE]
denotes the obvious subset of .
3.2. Proposition.*
Let , and be correspondence functors over .*
- (a)
The assignment is a -linear bifunctor and is right exact in and . 2. (b)
There are natural isomorphisms of correspondence functors
[TABLE]
where is the constant functor introduced in Example 2.
**Proof : **(a) This is a straightforward consequence of the usual properties of tensor products.
(b) For any finite set , the standard -linear isomorphisms
[TABLE]
are clearly compatible with the action of correspondences.
There is also a connection between tensor product and bilinear pairings. If , , and are correspondence functors over , the -module of bilinear pairings is the -module of natural transformations from the bifunctor
[TABLE]
to the bifunctor
[TABLE]
3.3. Theorem.*
Let , and be correspondence functors over .
The -module of all bilinear pairings is isomorphic to the -module .*
**Proof : **Given a morphism of correspondence functors , we need to construct a bilinear pairing . For any finite set , there is a -linear map with the property that, for any finite set and any correspondence , the diagram
[TABLE]
is commutative. If and are finite sets, we define a map
[TABLE]
as the following composition
[TABLE]
If and are finite sets, if and , then we claim that the diagram
[TABLE]
is commutative. The left hand side square is commutative because
[TABLE]
and similarly
[TABLE]
The right hand side square is commutative by the defining property of the morphism . It follows that
[TABLE]
so that the family of maps define a natural transformation from the bifunctor to the bifunctor , in other words a bilinear pairing .
Conversely, given a bilinear pairing , we have to construct a morphism of correspondence functors . For any finite sets , there is a -linear map
[TABLE]
such that, for any finite set and any correspondences and , the diagram
[TABLE]
is commutative.
In particular, for , we have a map which we can compose with the map given by the action of the correspondence , to get a map
[TABLE]
If is a finite set and , we claim that the diagram
[TABLE]
is commutative. The commutativity of the left hand side square is a special case of the commutativity of the diagram (3.3). The right hand side square is commutative because
[TABLE]
It follows that
[TABLE]
and therefore the family of maps define a morphism of correspondence functors from to .
The constructions and are -linear and we need to prove that they are inverse to each other.
Let be a morphism of correspondence functors. For any finite set , we have
[TABLE]
because and . Since acts as the identity on , we get , as required.
Now let be a bilinear pairing. For any finite sets and , the definition of applied to and the definition of yield
[TABLE]
the latter equality coming from the commutative diagram (3.3) for the sets and the correspondences and . Now it is easy to check that
[TABLE]
and this acts as the identity on . Therefore , as was to be shown.
Theorem 3 shows that our construction of tensor product is a special case of the general construction due to Day, known as Day convolution [Da].
4. Lattices
We want to apply the tensor product construction to functors of the form , where is a finite lattice, as defined in Example 2. As in [BT3], we define the category of finite lattices as follows. Its objects are the finite lattices and is the free -module with basis the set of all join-morphisms from to .
The direct product of two lattices is defined using componentwise operations. Our next lemma shows that there is also a direct product for morphisms in .
4.1. Lemma.* Let , , S’ be finite lattices.*
- (a)
If and are join-morphisms, then is a join-morphism. 2. (b)
Extending this direct product by -bilinearity defines a -linear bifunctor .
**Proof : **Given a subset , let (respectively ) denote the first projection of (respectively the second projection). Then
[TABLE]
as required. The second assertion follows by bilinearity.
4.2. Theorem.*
The bifunctors*
[TABLE]
and
[TABLE]
are isomorphic.
**Proof : **Let and be finite lattices. For any finite set , there is a unique isomorphism of -modules
[TABLE]
mapping to . Here of course, the map is obtained by direct product form the maps and . If is a finite set and , then for any ,
[TABLE]
Thus , that is, . Therefore
[TABLE]
is an isomorphism of correspondence functors.
If and are join-morphisms, then is a join-morphism, by Lemma 4. Moreover, we claim that the diagram
[TABLE]
is commutative, where denotes the corresponding isomorphism for the lattices and . This is because, for any finite set , any map , and any map , we have
[TABLE]
It follows that the family of isomorphisms yields an isomorphism between the two bifunctors of the statement.
4.3. Corollary.*
If and are finite sets, then*
[TABLE]
**Proof : **This follows from Theorem 4 applied to the lattice of subsets of and the lattice of subsets of . Then and , because a map from to corresponds to a subset of . Moreover is isomorphic to the lattice of subsets of .
5. More properties of tensor product
We first discuss projectivity. Recall that any correspondence functor is isomorphic to a quotient of where each is a finite set and is some index set. This is because if , Yoneda’s lemma gives a morphism mapping to . Choosing a set of generators of , the sum of the morphisms yields a surjective morphism , as required. In particular, any projective correspondence functor is isomorphic to a direct summand of a direct sum of representable functors.
5.1. Proposition.* Let and be correspondence functors over . If and are projective, then so is .*
**Proof : **By the observation above, it suffices to assume that and , where and are finite sets and where and are some index sets. By Corollary 4, we obtain
[TABLE]
so is projective.
It should be observed that, since for any correspondence functor (Proposition 3) and since is projective (Example 2), tensoring with a projective functor does not yield a projective functor in general, contrary to the case of finite group representations.
Next we consider the functors introduced in Example 2, where is a finite set and is an -module. Recall that . There is an induction procedure
[TABLE]
where is any finite set. Clearly is a left -module. Notice that we have by the definition of .
5.2. Theorem.* Let and be finite sets and let . Let be a -module and be a -module. Then there is an isomorphism of correspondence functors*
[TABLE]
where the -module structure on is induced by the comultiplication defined by for any relation .
**Proof : **Since , the identity map corresponds, by the adjointness property of , to a morphism
[TABLE]
which we need to described explicitly. For a finite set ,
[TABLE]
and
[TABLE]
It is easy to check that the morphism maps the element
[TABLE]
to the element
[TABLE]
where , , , , and .
Conversely, there is a morphism
[TABLE]
defined as follows. For any , , , and , it maps the element
[TABLE]
to the element
[TABLE]
where , and where and .
The map is well defined, for if and , then
[TABLE]
Moreover, if is a finite set and , then
[TABLE]
It follows that the maps define a morphism of correspondence functors
[TABLE]
Moreover, setting , we have
[TABLE]
so is equal to the identity morphism.
Similarly, setting s=C\otimes_{{\mathcal{R}}_{G}}\big{(}(A\otimes_{{\mathcal{R}}_{E}}v)\otimes_{k}(B\otimes_{{\mathcal{R}}_{F}}w)\big{)},
[TABLE]
so is also equal to the identity morphism.
Finally we consider finite generation. Recall from [BT2] that a correspondence functor has bounded type if there is a finite set such that is generated by , that is, for every finite set . Moreover, is finitely generated if there is a finite set and a finite subset of such that is generated by , that is, for every finite set (see Proposition 6.4 in [BT2]).
5.3. Theorem.* Let and be correspondence functors over .*
- (a)
If and have bounded type, so has . 2. (b)
If and are finitely generated, so is .
**Proof : **(a) Let and be finite sets such that is generated by and is generated by . Then the counit morphisms and are surjective. Therefore is isomorphic to a quotient of . By Theorem 5,
[TABLE]
where . Since is generated by its evaluation at , so is .
(b) Assume now that is generated by a finite subset of and is generated by a finite subset of . In particular, is generated by as an -module and is generated by as an -module. Therefore, as -modules, is generated by the finite set and is generated by the finite set , where as before. It follows that is generated as an -module by the finite set
[TABLE]
Since is generated by its evaluation at , namely the -module , it is also generated by the finite set . Now is isomorphic to a quotient of , so it is generated by the image of . Thus is finitely generated.
6. Internal hom
In this section, we use the symmetric monoidal structure of the category to define an internal hom in the category of correspondence functors. We first introduce a useful construction.
6.1. Definition.* Let be a finite set and let be a correspondence functor over .*
- (a)
We let be the endofunctor defined on objects by and on correspondences by
[TABLE] 2. (b)
We denote by the correspondence functor obtained from by precomposition with the endofunctor . 3. (c)
Let be a finite set and . We define to be the morphism obtained by precomposition with the natural transformation .
Explicitly, we see that and is given by the action of the correspondence
[TABLE]
6.2. Definition.* Let and be correspondence functors over . We denote by the correspondence functor defined on a finite set by*
[TABLE]
and for , by composition with .
6.3. Lemma.*
The assignment is a -linear bifunctor , left exact in and .*
**Proof : **This is straightforward.
Now we prove the basic adjointness property which shows that is an internal hom in the category .
6.4. Theorem.*
There are isomorphisms of -modules*
[TABLE]
natural in . In particular, for any correspondence functor over , the endofunctor
[TABLE]
is left adjoint to the endofunctor
[TABLE]
**Proof : **Let be a morphism of correspondence functors. By Theorem 3, we get a bilinear pairing , hence, for any finite sets and , a -linear map
[TABLE]
or equivalently, a -linear map
[TABLE]
defined by , for and .
Now . Moreover, for any finite set and any , the commutative diagram (3.3), for and , becomes
[TABLE]
or in other words for any and . Therefore, for a fixed set and a fixed , the maps define a morphism of correspondence functors
[TABLE]
hence an element of . Allowing to vary, we obtain a -linear map
[TABLE]
Now if is a finite set and , the commutative diagram (3.3), for and , becomes
[TABLE]
and it follows that the maps define a morphism of correspondence functors .
Conversely, a morphism of correspondence functors is determined by maps
[TABLE]
for all finite sets . Furthermore, for , the morphism is in turn determined by maps
[TABLE]
for all finite sets . We claim that the family of maps
[TABLE]
defines a bilinear pairing . We must show that, for any finite sets and any correspondences and , the diagram
[TABLE]
is commutative. First observe that we have
[TABLE]
because is a morphism of correspondence functors . Now the action of the correspondence \left(\begin{array}[]{cc}\Delta_{X^{\prime}}&\emptyset\\ \emptyset&V\end{array}\right) is the composition with , which is in turn the action of within the correspondence functor . Therefore we obtain
[TABLE]
using the fact that is a morphism of correspondence functors. This proves the claim.
By Theorem 3, the pairing defines a morphism of correspondence functors
[TABLE]
Now it is straightforward to check that the maps and are inverse isomorphisms between and \operatorname{Hom}\nolimits_{{\mathcal{F}}_{k}}\!\big{(}M,{\mathcal{H}}(M^{\prime},M^{\prime\prime})\big{)}.
In the case of a representable functor , there is the following useful isomorphism.
6.5. Proposition.* Let be a finite set and a correspondence functor over . There is an isomorphism of correspondence functors {\mathcal{H}}\big{(}k{\mathcal{C}}(-,E),N\big{)}\cong N_{E}.*
**Proof : **Let be a finite set. By Yoneda’s lemma, we get
[TABLE]
Moreover, . It is straightforward to check that the resulting isomorphism
[TABLE]
is compatible with correspondences, so that it yields an isomorphism of correspondence functors {\mathcal{H}}\big{(}k{\mathcal{C}}(-,E),N\big{)}\cong N_{E}.
6.6. Corollary.* Let be a correspondence functor over . There is an isomorphism of correspondence functors .*
**Proof : **Take in Proposition 6. Then because is the set of subsets of , which is a singleton. On the other hand we clearly have .
Taking the constant functor in the second variable, we obtain a quite different result.
6.7. Proposition.* Let be a correspondence functor over . There is an isomorphism of correspondence functors*
[TABLE]
where M(\emptyset)^{\scriptscriptstyle\natural}=\operatorname{Hom}\nolimits_{k}\big{(}M(\emptyset),k\big{)}. In particular, if is a field and if is finite-dimensional, is isomorphic to a direct sum of \dim\!\big{(}M(\emptyset)\big{)} copies of .
**Proof : **Let be a finite set. It is straightforward to see that . Therefore
[TABLE]
It is then easy to check that the action of a correspondence yields the identity endomorphism of , so that we get the constant functor tensored with . If is a field and if is finite-dimensional, it follows that is isomorphic to a direct sum of copies of , their number being \dim\!\big{(}M(\emptyset)^{\scriptscriptstyle\natural}\big{)}=\dim\!\big{(}M(\emptyset)\big{)}.
In the same vein as in Theorem 5, we now consider bounded type and finite generation.
6.8. Theorem.* Let and be correspondence functors over .*
- (a)
Let and be finite sets. If is generated by , then is generated by . Therefore, if has bounded type, so has . If is finitely generated, so is . 2. (b)
Assume that the ring is noetherian. If is finitely generated and if has bounded type (respectively is finitely generated), then has bounded type (respectively is finitely generated).
**Proof : **(a) By assumption, for each finite set . Replacing by gives
[TABLE]
Therefore is -linearly generated by the elements , where , , and , because any correspondence in can be written . But we have
[TABLE]
and this is the image of by the correspondence within the functor . It follows that
[TABLE]
Therefore is -linearly generated by , that is,
[TABLE]
as was to be shown. The other two assertions follow immediately.
(b) Since is finitely generated, there is a finite subset such that , so is isomorphic a quotient of the finite direct sum of representable functors. Since is exact by Lemma 6, we deduce an embedding
[TABLE]
using also Proposition 6. If has bounded type, then has bounded type, by (a), so the finite direct sum also has bounded type. Therefore is isomorphic to a subfunctor of a functor of bounded type. Since is noetherian, this implies that has bounded type, by Corollary 11.5 in [BT2]. The same argument with “bounded type” replaced by “finitely generated” goes through, completing the proof.
7. Algebra functors
For any finite lattice , the functor has more structure, namely it is a commutative algebra in the tensor category of all correspondence functors. This section is devoted to a closer analysis of this additional structure. By a -algebra, we always mean an associative -algebra with an identity element.
7.1. Definition.* An algebra correspondence functor over is a correspondence functor with values in the category of -algebras satisfying the following two conditions. For any finite sets and , and for any correspondence , the diagrams*
[TABLE]
are commutative, where denotes the multiplication map of the -algebra and denotes the map .
An algebra correspondence functor is called commutative if is a commutative -algebra for any finite set .
The commutativity of all the diagrams in the definition can be interpreted in two different ways :
- (a)
The action of any correspondence is a map of -algebras , mapping to . 2. (b)
The family of multiplication maps defines a morphism of correspondence functor and the family of maps defines a morphism of correspondence functors , where denotes the constant functor of Example 2. In other words, the triple is an algebra in the tensor category .
7.2. Lemma.*
Let be an algebra correspondence functor, let be the multiplication map,
let be the associated pairing (see Theorem 3),
and let and be finite sets.*
- (a)
The map
[TABLE]
is obtained as the composite of the action of and the multiplication . 2. (b)
If is commutative, then is an algebra homomorphism. 3. (c)
The composite is equal to .
**Proof : **(a) This follows from the proof of Theorem 3.
(b) The action of is an algebra homomorphism and, whenever is commutative, so is the multiplication .
(c) Using (a), we obtain
[TABLE]
We consider now the functor of Example 2, associated to a finite lattice .
7.3. Proposition.*
Let be a finite lattice and let be its least element.*
- (a)
Commutative algebra.* is a commutative algebra correspondence functor, with respect to the multiplication maps*
[TABLE]
where is a finite set and are maps. Here denotes the map defined by for every . The identity element of is the constant map onto . 2. (b)
Exponential property.* and, for any finite sets and , the bilinear pairing*
[TABLE]
associated with is an isomorphism of -modules.
More precisely, for any maps and , the element is the function equal to on and to on , providing a bijection between the canonical bases of and . 3. (c)
Splitting property.* If denotes a set of cardinality one, then is isomorphic to a finite direct product as -algebras.*
**Proof : **(a) We claim that the map
[TABLE]
is a join-morphism. Given a subset , let be its first projection and its second projection. Then
[TABLE]
proving the claim. By Example 2, the map induces a morphism . Since by Theorem 4, we obtain a morphism . For any finite set , the map
[TABLE]
is easily seen to be the map of the statement. Clearly is associative and commutative and the constant map onto is an identity element. We obtain in this way an algebra correspondence functor because is a morphism of functors, and so is .
(b) One checks easily that is the function from to equal to on , and to on . Similarly is the map equal to on and to on . Thus \Big{(}\binom{\Delta_{X}}{\emptyset}\varphi\Big{)}\vee\Big{(}\binom{\emptyset}{\Delta_{Y}}\psi\Big{)} is the map equal to on and to on .
(c) Since has cardinality one, is a free -module with basis
[TABLE]
where is defined by (with being also the unique element of the set ). Moreover, on restriction to this basis, the multiplication map corresponds to the map of the beginning of the proof, namely . In that case, there is a standard procedure for finding another -basis consisting of orthogonal primitive idempotents whose sum is the identity element (namely ). These primitive idempotents are defined by
[TABLE]
where denotes the Möbius function of the poset (see the appendix in [BT1]). Then we obtain isomorphisms of -algebras
[TABLE]
as required.
Our next main result asserts that, with a small assumption on , the converse of Proposition 7 holds.
7.4. Theorem.* Assume that does not contain a nontrivial idempotent (i.e. is connected). Let be a correspondence functor over and suppose that has the following three properties :*
- (a)
Commutative algebra.* is a commutative algebra correspondence functor (with multiplication written ).* 2. (b)
Exponential property.* For any finite sets and , the associated bilinear pairing*
[TABLE]
is an isomorphism of -modules (hence an isomorphism of -algebras, by commutativity of ). Moreover, . 3. (c)
Splitting property.* If denotes a set of cardinality one, then is isomorphic to a finite direct product as -algebras.*
Then there exists a finite lattice such that (isomorphism of algebra correspondence functors).
We need a preliminary lemma.
7.5. Lemma.*
With the assumptions above, define a comultiplication*
[TABLE]
as the composition of the action of and the isomorphism
[TABLE]
- (a)
* is an algebra homomorphism.* 2. (b)
* is coassociative and cocommutative.* 3. (c)
. 4. (d)
The map induced by the action of the empty correspondence is a counit for the comultiplication and is an algebra homomorphism.
**Proof : **(a) The action of is an algebra homomorphism. So is the map by Lemma 7, hence so is the composite .
(b) This is left as an exercise for the reader. For the cocommutativity, use both the twist of and the action of the correspondence \left(\begin{array}[]{cc}\emptyset&\Delta_{\bullet}\\ \Delta_{\bullet}&\emptyset\end{array}\right).
(c) We compute
[TABLE]
(d) A special case of diagram (3.3) yields the commutative diagram
[TABLE]
and it easy to check that the bottom composite is the identity . We deduce the commutative diagram
[TABLE]
and since the composite of the first row is equal to , we obtain that is the identity , as required for a counit.
**Proof of Theorem 7 : ** By the splitting property, the -algebra contains a -basis
[TABLE]
consisting of orthogonal idempotents such that , where is a finite index set. Our first aim is to show that has a lattice structure.
Now is a -basis of orthogonal idempotents of , so we can write
[TABLE]
Since is an algebra homomorphism by Lemma 7, is an idempotent of . Therefore is an idempotent of , hence by our assumption on , and
[TABLE]
where is a subset of . Since the idempotents are orthogonal and sum to , the idempotents are orthogonal and sum to . This shows that for any pair of distinct elements of , and that . Hence we can define a operation on by
[TABLE]
In other words, for any ,
[TABLE]
Since is coassociative by Lemma 7, this operation is associative. Similarly, since is cocommutative, is commutative. Finally, by Lemma 7 again, for any , we have
[TABLE]
because if . It follows that for any . Hence is a commutative idempotent semigroup. Equivalently, if we define a relation on by
[TABLE]
we get an order relation on , and any pair of elements of has a greatest lower bound . Thus is a meet semilattice.
Since the counit is an algebra homomorphism by Lemma 7 and since the only idempotents of are 0 and 1, we have for any . Moreover
[TABLE]
so there exists such that . This element is unique because if are such that , then , so , hence . Moreover, since is a counit, we have, for any ,
[TABLE]
and it follows that , hence . Therefore is a meet semilattice with a greatest element , so it is a lattice. We write for its join operation and for its least element.
Now, for any , we define
[TABLE]
The elements form another basis of , because the transition matrix is unitriangular. Now for any , we have
[TABLE]
and also
[TABLE]
This means that the map , from to , induces an algebra homomorphism
[TABLE]
and this is an isomorphism because it maps a basis to a basis.
Whenever we have a disjoint union , there is a bilinear pairing
[TABLE]
which is an isomorphism by the exponential property. Decomposing as a union of singletons, we obtain by induction an isomorphism of -algebras
[TABLE]
By part (a) of Lemma 7, the isomorphism maps to the product , where . We then obtain a sequence of isomorphisms of -algebras
[TABLE]
It is easy to check that the first isomorphism maps a function to the element , where is defined by . The second isomorphism maps to , which in turn maps to via the third isomorphism . Therefore we get the composite isomorphism of -algebras
[TABLE]
We are going to show that the isomorphisms are compatible with the action of correspondences, but we first need a lemma.
7.6. Lemma.*
Let be a finite set and let and be subsets of .
Let and let as defined above. Then, in the -algebra , we have an equality*
[TABLE]
**Proof : **By (3.3), there is a commutative diagram
[TABLE]
and we compute the image of using both paths. For the top path, the definition of gives
[TABLE]
and since (\Delta_{Y},\Delta_{Y})\leavevmode\hbox{\footnotesize\left(!!\begin{array}[]{cc}W&!!!!\emptyset\ \emptyset&!!!!Z\end{array}!!\right)}\binom{\Delta_{\bullet}}{\Delta_{\bullet}}=W\cup Z, we obtain the element
[TABLE]
For the bottom path, we first have
[TABLE]
and this is mapped to by the vertical map . Since the composition of the two bottom maps is , we obtain
[TABLE]
This completes the proof of the lemma.
Now we return to the proof of the theorem and we let and . Since and since , we obtain
[TABLE]
using Lemma 7. Therefore
[TABLE]
This proves that is an isomorphism of algebra correspondence functors.
7.7. Remark.*
*In Theorem 7, the algebra structure on is uniquely determined from that of .
More precisely, if and are correspondence functors satisfying the three properties of Theorem 7 and if ,
then . This follows from the proof, because the lattice is uniquely determined by the algebra structure of .
**
7.8. Remark.*
*The assumption on is necessary in Theorem 7.
Let be the direct product of two nontrivial rings
and, for , let be the functor over associated to a lattice ,
but viewed as a functor over (with the other factor acting by zero).
It can be shown that, if and have the same cardinality but are not isomorphic,
then satisfies the three assumptions of Theorem 7 but is not isomorphic to for any lattice .
**
8. Examples
Finding the decomposition of tensor products is not straightforward, due in particular to fast increasing dimensions. We only give here a few small examples, based on [BT3] and [BT4]. We refer to those two papers for details. For simplicity, we assume that is a field.
For any , we let and . Then is a totally ordered lattice and is its subset of irreducible elements. There is a simple correspondence functor introduced in Section 11 of [BT3]. It appears as a direct summand of the functor associated to the lattice .
8.1. Example.*
*When , then is the constant functor of Example 2.
For any correspondence functor , we have , by Proposition 3.
**
8.2. Example.*
*When , we have , by Theorem 11.6 of [BT3].
Moreover, by Theorem 4, we know that
[TABLE]
where denotes the lattice of subsets of a set of cardinality 2. Applying Example 8, we obtain
[TABLE]
On the other hand, by Example 8.7 of [BT4], there is a direct sum decomposition
[TABLE]
where is the fundamental functor associated to the poset of cardinality 2 ordered by the equality relation.
We now have two expressions for and we apply the Krull-Remak-Schmidt theorem, which holds by Proposition 6.6 in [BT2]. It follows that
[TABLE]
8.3. Example.*
*When , we have , by Theorem 11.6 of [BT3].
Moreover, by Theorem 4, we know that
[TABLE]
where . Applying the previous two examples, we obtain
[TABLE]
On the other hand, by Example 8.11 of [BT4], there is a direct sum decomposition
[TABLE]
where (respectively \mathbb{S}_{{}^{\mathop{\mathop{\scriptscriptstyle\circ\;\circ}^{\scriptscriptstyle/\backslash}\limits}^{\raisebox{-2.15277pt}{\scriptscriptstyle\circ}}\limits}}) denotes the fundamental functor associated to the poset indicated as a subscript, and where is an indecomposable projective functor of Loewy length 3 described in Example 8.11 of [BT4].
We now have two expressions for and it follows from the Krull-Remak-Schmidt theorem that
[TABLE]
We note that both and are projective functors, hence so is by Proposition 5. **
Acknowledgments. The first author is grateful to Antoine Touzé for an inspiring talk about exponential functors, given at the Amiens group theory seminar, and to Robert Boltje, for fruitful discussions around Remark 7.
The reference list from the paper itself. Each links out to its DOI / PubMed record.
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- 3[BT 2] S. Bouc, J. Thévenaz. Correspondence functors and finiteness conditions, J. Algebra 495 (2018), 150–198.
- 4[BT 3] S. Bouc, J. Thévenaz. Correspondence functors and lattices, J. Algebra 518 (2019), 453–518. .
- 5[BT 4] S. Bouc, J. Thévenaz. The algebra of Boolean matrices, correspondence functors, and simplicity, preprint, 2018, ar Xiv:1902.05422.
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