§ 4. Tensor products of algebras
From § 4 to § 8 inclusive, A denotes a commutative ring and, unless otherwise mentioned, the algebras considered are assumed to be associative and unital and the algebra homomorphisms are assumed to be unital.
1. Tensor product of a finite family of algebras
A always denotes a commutative ring with unit element. Let (E_i)_{i \in I} be a finite family of A-algebras and let E = \bigotimes_{i \in I} E_i be the tensor product A-module of the A-modules E_i (II, § 3, no. 9). We shall define an A-algebra structure on E. Let m_i: E_i \otimes_A E_i \to E_i be the A-linear mapping defining the multiplication on E_i (§ 1, no. 3). Consider the A-linear mapping
the composite mapping
where is the associativity isomorphism (II, § 3, no. 9) is an A-linear mapping ; we shall see that defines an (associative and unital) algebra structure on . For, on explicitly performing the multiplication defined by , we obtain the formula
(1)
It is therefore seen already, by linearity, that if is the unit element of , is unit element of . On the other hand, the associativity of each of the implies the relation
whence, by linearity, the relation for all in .
Definition 1
Given a family* of algebras over , the tensor product of this family, denoted by (or, when is the interval of , , or simply ) is the algebra obtained by giving the tensor product of the *-modules* the multiplication defined by (1).
Relation (1) shows that the tensor product of the opposite algebras to the is the opposite algebra to ; in particular, if the are commutative, so is .
Let and be two families of -algebras with the same finite indexing set . For each , let be an -algebra homomorphism. Then the -linear mapping
is an A-algebra homomorphism, as follows from (1).
For every partition of , the associativity isomorphisms
(II, § 3, no. 9) are also algebra isomorphisms, as follows from (1) and their definitions.
When is the interval of and all the algebras are equal to the same algebra , the tensor product algebra is also denoted by .
We shall restrict our attention in the remainder of this no. to the properties of tensor products of two algebras, leaving to the reader the task of extending them to tensor products of arbitrary finite families.
Let be two -algebras; if (resp. ) is a left ideal of (resp. ), the canonical image of in is a left ideal of ; there are analogous results when "left ideal" is replaced by "right ideal" or "two-sided ideal". Moreover:
Proposition 1
Let be two -algebras and (resp. ) a two-sided ideal of (resp. ). Then the canonical -module isomorphism
(II, § 3, no. 6, Corollary 1 to Proposition 6) is an algebra isomorphism.
This follows from (1) and the definition given loc. cit.
Corollary 1
Let be an -algebra and an ideal of . Then the -module is a two-sided ideal of and the canonical -module isomorphism
is an *-algebra isomorphism*.
Corollary 2
If are two ideals of , is canonically isomorphic to *.
Corollary 3
Let be two -algebras and an ideal of contained in the annihilator of . Then the -algebra is canonically isomorphic to *.
Proposition 2
Let and be two families of -algebras. The canonical mapping* (II, § 3, no. 7)
is an algebra isomorphism.
This follows immediately from II, § 3, no. 7, Proposition 7 and the definition of multiplication on .
Proposition 3
Let be two commutative rings, a ring homomorphism and two -algebras. Then the canonical -module isomorphism
(II, § 5, no. 1, Proposition 3) is a -algebra isomorphism.
Proposition 4
Let be two commutative rings, a ring homomorphism, an -algebra and a -algebra. Then the canonical -module isomorphism
(II, § 5, no. 2, Proposition 6) is an -algebra isomorphism.
The verifications are trivial on account of § 1, no. 5.
In particular, the -algebra structure on , obtained by restricting the ring of scalars to , is identical with the structure of the algebra , the tensor product of the -algebras and .
Finally, if is a direct system of commutative rings, and two direct systems of -algebras (, no. 6) and , the canonical -module isomorphism
(II, § 6, no. 3, Proposition 7) is also an -algebra isomorphism, as follows from the definitions.
Examples of tensor products of algebras. (1) Let be a commutative ring and two -modules; the canonical mapping
(II, § 4, no. 4) is an -algebra homomorphism, as follows from II, § 3, no. 2, formula (5). When or is a finitely generated projective -module, we know that this homomorphism is bijective (II, § 4, no. 4, Proposition 4). In particular we recover the definition of the tensor product of two square matrices.
(2) Let be two monoids and and the algebras of the monoids and over the ring (III, § 2, no. 6); then there is a canonical -algebra isomorphism
The elements (resp. ), where runs through and runs through , form a basis of by virtue of II, § 3, no. 7, Corollary 2 to Proposition 7 (resp. of ; the desired isomorphism is obtained by mapping to and it follows from the definitions that this is indeed an algebra isomorphism.
2. Universal characterization of tensor products of algebras
Proposition 5
Let be a finite family of -algebras and, for each , let be the unit element of . For each , let be the -linear mapping defined by
(i) *The are -algebra isomorphisms; further, for , the elements and are permutable in for all and and is generated by the union of the subalgebras .
(ii) Let be an -algebra and, for all , let be an -algebra homomorphism, where the are such that, for , and are permutable in for all and . Then there exists one and only one -algebra homomorphism such that
(i) The mapping is an algebra homomorphism by definition of the multiplication on . If , , then
Clearly for all and hence and commute in by formula (1) (no. 1) defining the multiplication in . The last assertion follows from the relation .
(ii) For each , let be an element of . The product is then defined in independently of any ordering on since the algebra is associative and the elements are pairwise permutable. The mapping of into is obviously -multilinear and there therefore exists one and only one -linear mapping such that
Now, the desired -algebra homomorphism must satisfy (5), which follows from (4) and the fact that . This proves the uniqueness of ; it remains to show that the -linear mapping defined by (5) is an -algebra homomorphism and satisfies (4). The fact that satisfies (4) is obvious: it suffices to apply (5) to the case where for and we obtain . Finally, is an algebra homomorphism, for
since commutes with for ; hence
which, by linearity, completes the proof.
The ordered pair consisting of E and the canonical mapping of into E is a solution of the universal mapping problem (Set Theory, IV, § 3, no. 1) where is the species of A-algebra structure, the morphisms being the A-algebra homomorphisms and the -mappings the mappings of into an A-algebra such that the are A-algebra homomorphisms and and commute for , for all and .
Corollary
Let* be two finite families of A-algebras and, for all , let be an algebra homomorphism. If are the canonical homomorphisms, the mapping (cf. no. 1) is the unique A-algebra homomorphism such that for all .
It suffices to note that the homomorphisms are such that and commute for , and ; then apply Proposition 5.
When, in Proposition 5, the algebra F is assumed to be commutative, the hypothesis that and are permutable for is automatically satisfied. Hence, when F is commutative, there is a canonical bijection
namely the one which associates with every homomorphism of into F the family of .
Note that if E is a commutative A-algebra, the ring structure of is the same as that of (§ 1, no. 5).
3. Modules and multimodules over tensor products of algebras
Definition 2
Let E be a (unital) A-algebra. A left (resp. right) E-module is a left (resp. right) module over the underlying ring of E.
Unless otherwise mentioned, all the modules and multimodules considered in this no. are left modules and multimodules.
If M is an E-module, the homomorphism (§ 1, no. 4) then defines on M an A-module structure, said to be underlying the E-module structure on M; for ,
so that for all , the homothety of M is an endomorphism of the underlying A-module structure. Conversely, being given an E-module structure on M is equivalent to being given an A-module structure on M and an A-algebra homomorphism of E into .
Definition 3
Let E and F be two (unital) A-algebras and M a set with an E-module structure and an F-module structure. M is called a (left) bimodule over the algebras E and F if:
(1) M is a bimodule over the underlying rings of E and F (II, § 1, no. 14); (2) the two A-module structures underlying the E-module and F-module structures on M are identical.
The latter condition says that if e and are the unit elements of E and F respectively, then
then is used to denote the common value of the two sides.
It can also be said that being given on M a bimodule structure over E and F is equivalent to being given an A-module structure on M and also two A-algebra homomorphisms of E into and of F into such that for all and . Consequently (no. 2, Proposition 5) an A-algebra homomorphism of into is canonically derived such that for and . In other words, an -module structure is thus defined on M, which is said to be associated with the given bimodule structure over E and F and under which
The given E-module and F-module structures on M can be derived from this -module structure by restrictions of the ring of scalars, corresponding to the two canonical homomorphisms and .
Conversely, if an -module structure is given on M, by means of the canonical homomorphisms and an E-module structure and an F-module structure on M and it is immediate that M is a bimodule over the algebras E and F with these two structures and that the given -module structure is associated with this bimodule structure.
Thus a one-to-one correspondence has been established between -module and bimodules over the algebras E and F. Clearly every sub-bimodule of M is a submodule for the associated -module structure and conversely. There are analogous results for quotients, products, direct sums and inverse and direct limits. Finally, if is another bimodule over the algebras E and F and is a bimodule homomorphism, is also an -module homomorphism and conversely.
There are obviously corresponding statements for right bimodule structures, or when for example there is a left E-module structure and a right F-module structure; in this case we speak of an -bimodule and being given such a structure amounts to being given a left bimodule structure over E and .
Example
(1) Let B be an A-algebra; the ring B has canonically a (B, B)-bimodule structure (II, § 1, no. 14, Example 1) and, if e is the unit element of B, then for all and all ; B can therefore be considered as a left bimodule over the algebras B and (opposite to B); there is therefore associated with the (B, B)-bimodule structure on B a (B )-module structure such that, for and in B,
the right-hand side being the product in the ring B.
(2) Let E and F be two A-algebras, their respective unit elements, M an E-module and N an F-module; these module structures define on M a bimodule structure over the rings A and E and on N a bimodule structure over the rings A and F; from these is therefore derived a bimodule structure over the rings E and F on the tensor product , defined by
for (II, § 3, no. 4); it is also seen that conditions (8) hold and hence the above bimodule structure is associated with an -module structure on , such that
for .
In particular, taking has canonically an -module structure; on the other hand, is canonically identified with , where is considered as having its right F-module structure defined by the canonical homomorphism ; for in E, , is thus identified with and with . The -module is thus identified with the -module derived from N by extending the scalars to by means of the homomorphism (II, § 5, no. 1). The canonical mapping of N into is identified with the canonical mapping of N into ; this is known to be an F-homomorphism.
With the same notation, let P be a right (E \otimes_A F)-module; then there is a canonical Z-module isomorphism
(11)
where on the right-hand side P is considered as a right F-module by means of the canonical homomorphism . For P is canonically identified with and with and hence with , which establishes the stated isomorphism (II, § 3, no. 8, Proposition 8 and II, § 3, no. 4, proposition 4).
All the above extends to multimodules (II, § 1, no. 14).
4. Tensor product of algebras over a field
Let K be a commutative field and E, F two algebras over K whose respective unit elements are non-zero. Then the homomorphisms and (§ 1, no. 3) are injections which allow us to identify K with a subfield of E (resp. F). The canonical homomorphisms and , defined by and are injective (II, § 7, no. 9, Proposition 19) and allow us to identify E and F with subalgebras of , both having as unit element the unit element of . In (II, § 7, no. 9, Proposition 19).
If E' and F' are subalgebras of E and F respectively, the canonical homomorphism is injective and allows us to identify with the subalgebra of generated by (II, § 7, no. 7, Proposition 14).
Proposition 6
Let E, F be two non-zero algebras over a commutative field, K, C (resp. D) a subalgebra of E (resp. F) and C' (resp. D') the centralizer of C in E (resp. D in F). Then the centralizer of C \otimes_K D in E \otimes_K F is C' \otimes_K D'.
It all reduces to verifying that an element of the centralizer of () belongs to ; we know that
(II, § 7, no. 7, Corollary to Proposition 14). The may be assumed to be linearly independent over K; for all , of necessity , that is , whence for all (II, § 3, no. 7, Corollary 1 to Proposition 7); hence of necessity for all and therefore ; it can similarly be shown that , whence the proposition.
Corollary
If Z and Z' are the respective centres of E and F, the centre of E \otimes_K F is Z \otimes_K Z'*.
Let E and F be two subalgebras of an algebra G over a commutative field K; suppose that every element of E commutes with every element of F. Then the canonical injections define a canonical homomorphism (no. 2, Proposition 5) such that
Definition 4
Given an algebra G over a commutative field K, two subalgebras E, F of G are said to be linearly disjoint over K if they satisfy the following conditions:* (1) every element of E commutes with every element of F; (2) *the canonical homomorphism of into G is injective.
Proposition 7
Let G be an algebra over a commutative field K and E, F two subalgebras of G such that every element of E commutes with every element of F. For E and F to be linearly disjoint over K, it is necessary and sufficient that there exist a basis of E over K which is a free subset of G for the right F-module structure on G. When this is so:* (i) the canonical homomorphism is an isomorphism of onto the subalgebra of G generated by ; (ii) (iii) *every free subset of E (resp. F) over K is a free subset of G with its right or left F-module (resp. E-module) structure.
The condition of the statement is obviously necessary, since every basis of E over K is a basis of with its right F-module structure (II, § 3, no. 7, Corollary 1 to Proposition 7). To see that the condition is sufficient, note that the image H of under h is the set of sums in G, with and ; if is a basis of E over K, H is therefore also the submodule of the (right or left) F-module G, generated by . The condition of the statement therefore means that there exists a basis of E which is also a basis of the F-module H; it follows that h is injective. Assertion (iii) follows from the fact that every free subset of E is contained in a basis of E (II, § 7, no. 1, Theorem 2).
Corollary 1
For the canonical homomorphism of into G to be bijective, it is necessary and sufficient that there exist a basis of E over K which is a basis of the (right or left) F-module G.
Corollary 2
Let E, F be two subalgebras of G, of finite rank over K and such that every element of E commutes with every element of F. For E and F to be linearly disjoint over K, it is necessary and sufficient that the subalgebra H of G generated by be such that*
5. Tensor product of an infinite family of algebras
Let A be a commutative ring and (E_i)_{i \in I} an arbitrary family of (unital) A-algebras. For every finite subset J of I, let E_J denote the tensor product of the algebras E_i of index ; let denote the unit element of E_i and the unit element of E_J; let denote the canonical homomorphism for (no. 2, Proposition 5). If J, J' are two finite subsets of I such that , a homomorphism is canonically derived (no. 2, Proposition 5), by the condition for all . Moreover the uniqueness of implies that if J, J', J'' are three finite subsets of I such that , then . In other words, is a direct system of A-algebras whose indexing set is the right directed set of finite subsets of I.
Definition 5
The direct limit E of the direct system* is called the tensor product of the family of A-algebras .
If I is finite, E is identified with . By an abuse of notation, E is also denoted by even if I is infinite.
For every finite subset J of I, let denote the canonical homomorphism (writing instead of ); if e is the unit element of , then for all . It is immediate that if all the algebras E_i are commutative, so is .
Proposition 8
(i) The homomorphisms are such that for two indices i, j such that , and commute in E for all and ; further, E is generated by the union of the subalgebras .
(ii) Let F be an A-algebra and, for all , let be an A-algebra homomorphism such that, for , and commute in F for all and . Then there exists one and only one A-algebra homomorphism such that for all .
(i) As, for every finite subset J of I, , the first assertion in (i) follows from no. 2, Proposition 5, taking J containing i and j; the second also follows from no. 2, Proposition 5, taking account of the fact that E is the union of the when J runs through .
(ii) For every finite subset J of I, it follows from no. 2, Proposition 5 that there exists a unique homomorphism such that for all ; it immediately follows from this uniqueness property that, for , ; in other words, the form a direct system of homomorphisms. Let ; then by definition for every finite subset of and in particular for all ; the uniqueness of follows from these relations and the fact that the generate the algebra .
Corollary
Let* be two families of *-algebras with the same indexing set and, for all* , let be an algebra homomorphism. Then there exists one and only one *-algebra homomorphism* such that, for all , *the diagram
is commutative, and denoting the canonical homomorphisms.
It suffices to apply Proposition 8 to the homomorphism .
The homomorphism defined in the Corollary to Proposition 8 is denoted by . If is any subset of , Proposition 8 can be applied to the family of canonical homomorphisms ; a canonical homomorphism is derived which is also denoted by and which, when is finite, coincides with the homomorphism denoted thus above.
Now let be an element of such that the family has finite support . It is immediate that, if and are two finite subsets of containing , then
The common value of the for the finite subsets of is denoted by .
Proposition 9
Let* be a family of *-algebras and for each* let be a basis of such that the unit element belongs to . Let be the set of elements of the form , where runs through the set of elements of such that the family has finite support. Then is a basis of the algebra and this basis contains the unit element .
For every finite subset of , let be the basis of the tensor product of the bases for (II, § 3, no. 9). It follows immediately from the definitions that is the union of the when runs through and that when ; hence is a direct system of subsets of the and ; the conclusion then follows from II, § 6, no. 2, Corollary to Proposition 5.
The basis is also called the tensor product of the bases for ; when the conditions of Proposition 9 are fulfilled, the canonical homomorphisms are injective for every subset of , for if is the basis of the tensor product of the for , it is immediately verified that the restriction of to is injective and maps onto a subset of .
6. Commutation lemmas
Lemma 1
Let be a commutative ring, an -algebra, a finite sequence of elements of , a finite sequence of elements of and an element of ; suppose that*
The lemma being trivial for , we argue by induction on . Now
Lemma 2
Let be a commutative ring, an -algebra and and two finite sequences of elements of ; suppose that for ,*
The lemma being trivial for , we again argue by induction on for . By virtue of Lemma 1,
For every family of elements of , with , and for every permutation , we write
Observe that, when and for every ordered pair such that , is just the signature of the permutation (I, § 5, no. 7).
Lemma 3
Let be a commutative ring, an -algebra, a finite sequence of elements of and suppose that, for every ordered pair of integers such that ,
Then, for every permutation ,
The lemma is trivial for and ; we proceed by induction on for . If , relation (19) follows from the induction hypothesis. Suppose therefore that , and let be the permutation of defined by
Let ; the permutation leaves fixed; now and therefore, writing . If and , the relations and are equivalent (since is a strictly increasing mapping of into ). For and ,
whence, by the induction hypothesis (using the fact that ):
that is
Now
and this, by Lemma 1, is equal to
Finally, (20) and (21) give
with
which completes the proof of Lemma 3.
7. Tensor product of graded algebras relative to commutation factors
Definition 6
Let* be a finite family of commutative monoids written additively. A system of commutation factors over the with values in a commutative ring is a system of mappings , where , , satisfying the following conditions:
(22)
for all in , in .
If I is given a total ordering and the are groups, a system of commutation factors is defined over the by taking for every ordered pair such that an arbitrary -*bilinear* mapping of into the (multiplicative) -module of invertible elements of the ring and then writing
for .
Note that, since the are invertible,
by virtue of (22) and (23).
Example
(1) The trivial system of commutation factors consists of the such that for all , , .
(2) If we take and for all , a system of commutation factors is obtained by taking . Note that this number depends only on the parities of and and the can therefore be considered as commutation factors when certain of the are equal to and the others to .
These two examples are the most frequent cases encountered in applications.
Proposition 10
Let be a commutative ring and a finite family of commutative monoids written additively; for each let be a graded -algebra of type . Finally, let be a system of commutation factors over the with values in . Then there exist a graded -algebra of type and for each an algebra homomorphism , with the following properties:
(i) If is the canonical homomorphism, then is a graded homomorphism (II, § 11, no. 2), in other words, , where and denote the respective graduations on and .
(ii) If and (resp. ) is a homogeneous element of (resp. ) of degree (resp. ), then
(iii) For every -algebra and every system of homomorphisms satisfying the conditions
where are as in (ii), then there exists one and only one algebra homomorphism such that for all . Moreover the underlying -module of is the tensor product .
Consider the ; it is identified with the direct sum of the submodules , where, for each , we write ; the therefore form a graduation of type on the -module . We shall define on a graded -algebra structure of type . For this let be given a total ordering; for every ordered pair of elements of , we must first define an -bilinear mapping of into , or alternatively an -linear mapping of into . We shall define by the condition
for , where
The right hand side of (27) obviously belongs to and the mapping is -multilinear in the product of the and the (). Then it must be proved that the multiplication thus defined on E is associative; now, if is a third element of and for , then
and it reduces to verifying the identity
But the latter follows immediately from the relations
themselves immediate consequences of the definition (28) and (22) and (23).
If, for all , denotes the unit element of , we know that is homogeneous of degree 0 (§ 3, no. 1), hence is homogeneous of degree 0 and it follows from (27), (28) and the relations
that is unit element of , which completes the definition on of the desired graded A-algebra structure. Then take ; to verify that for in , attention may be confined to the case where and are homogeneous and then this relation follows immediately from (27) and the relations ; the same relations and (24) prove also that the satisfy conditions (i) and (ii) of the statement and that
where the right hand side is the product of the ordered sequence in E with the given total ordering on I (I, § 1, no. 2) (it suffices to argue by induction on the number of (assumed homogeneous) distinct from the ).
It remains to prove condition (iii); note that the mapping
where the right hand side is the product of the ordered sequence with the given total ordering on , is A-multilinear. Then there exists one and only one A-linear mapping such that
Clearly is the unit element of and ; to verify that is an algebra homomorphism, in other words that for in , attention may be confined, by linearity, to the case where and , (resp. ) being homogeneous of degree (resp. ) for all . The relation to be verified then reduces, by (27), to
But, taking account of relations (26), this is a consequence of Lemma 2 of no. 6.
Clearly the algebra and the canonical mapping constitute a solution of the universal mapping problem (Set Theory, IV, § 3, no. 1), where is the species of A-algebra structure and the -mappings from to an A-algebra, satisfying conditions (26).
For a fixed total ordering on , the graded algebra defined in the proof of Proposition 10 will be called a graded tensor -product of type of the family of graded algebras of type and will be denoted by (if no confusion can arise over the ordering on ); similarly, the homomorphism defined in the proof of Proposition 10 will be denoted by . The homomorphisms are called canonical. We also write when and all the are equal to the same algebra .
Remark
(1) We recover the tensor product of algebras defined in no. 1 (with moreover the graduation the tensor product of those of its factors) taking for all and .
(2) Suppose that all the are equal to and write ; the tensor -product corresponding to this system of commutation factors is then called the skew tensor product of the graded algebras of type and denoted by (or for two algebras, or instead of ).
Corollary 1
In the notation of Proposition 10, suppose further that F is a graded A-algebra of type and that each is a graded algebra homomorphism relative to ; then is a graded algebra homomorphism.
This follows immediately from the definition of and the fact that
It is therefore seen that is also a solution of another universal mapping problem, where this time is the species of graded A-algebra structure of type , the morphisms being graded algebra homomorphisms of type and the -mappings the mappings , where, in addition to conditions (26), it is assumed that is a graded algebra homomorphism relative to .
Corollary 2
Let* be two finite families of A*-algebras, with* and graded of type for all . For each , let be a graded algebra homomorphism of type . Then, if and are the canonical homomorphisms, there exists one and only one homomorphism of graded A*-algebras of type* , such that for all . Also, if each is bijective, so is .
It suffices to apply Corollary 1 to , noting that conditions (26) then follow from relations (25) applied to the .
The homomorphism defined in Corollary 2 is also denoted by (if no confusion can arise); if, for each , is a third graded A-algebra of type and a graded algebra homomorphism, then
In the case of a skew tensor product of graded algebras of type , we write instead of for homomorphisms of graded algebras of type ; when , this homomorphism is also denoted by ; when and all the (resp. ) are equal and all the equal to the same homomorphism , we write .
Remark
In the proof of Proposition 10, a total ordering on was used to define an algebra structure on the tensor product of the A-modules
E_i. If the ordering on I is changed, another multiplicative structure arises on , but the new algebra thus obtained is canonically isomorphic to the above, since both are solutions of the same universal mapping problem. For example, when , the canonical isomorphism of the algebra onto the algebra maps to , where is homogeneous of degree and homogeneous of degree .
Let J be a subset of I and, for each , consider the canonical homomorphism . By virtue of relations (25) a canonical homomorphism is derived canonically (by Proposition 10) from these homomorphisms, such that, for all , , being the canonical homomorphism . Taking the total ordering on J induced by that chosen on I, we obtain
where the middle term is the product of the ordered sequence and where, in the right hand term, for , for .
Proposition 11
("associativity" of the tensor -product). In the notation of Proposition 10, let be a partition of I and write for all . Let be a graded tensor -product of type of the family for some total ordering chosen on . On the other hand, for in and , we write, for , ,
Then is a system of commutation factors over the with values in and there exists one and only one homomorphism of graded algebras of type , , such that
for all , provided that the total ordering is taken on I which induces on each the chosen total ordering, and which is such that, for in , and , .
The fact that the form a system of commutation factors is trivial. Let , be the canonical homomorphisms (for , ) and write ; it will suffice by virtue of the uniqueness of the solution of a universal mapping problem, to show that and the satisfy the conditions of Proposition 10. Now, for all , let be the unique algebra homomorphism such that for all . We show that, for , ,
for (resp. ) homogeneous of degree (resp. ); it suffices, by linearity, to verify it when (resp. ) being homogeneous of degree (resp. ) in (resp. ) for . But this follows from formula (30) which defines the and Lemma 3 of no. 6, taking account of hypothesis (26) and definition (32). There is therefore one and only one algebra homomorphism such that for all ; whence for all and the uniqueness of is trivial.
8. Tensor product of graded algebras of the same types
Assuming the hypotheses of no. 7, Proposition 10 hold, suppose further that all the are equal to the same commutative monoid ; we can then consider on the tensor -product the total graduation of type , associated with the graduation of type on this algebra (II, § 11, no. 1); we shall call , with this graduation, a graded tensor -product of type of the family of graded algebras of type .
Always preserving the notation of Proposition 10 of no. 7, suppose that is also a graded A-algebra of type and that the are homomorphisms of graded algebras of type . Then is also a homomorphism of graded algebras of type : for it follows from formula (30) (no. 7) that if is homogeneous and of degree and are both homogeneous of degree .
It can therefore be said that , with the total graduation of type , constitutes, together with the canonical mapping , a solution of a third universal mapping problem, where is the species of graded A-algebra of type , the morphisms are homomorphisms of graded algebras of type and the -mappings are the mappings , where, in addition to conditions (26) (of no. 7), it is assumed that each is a homomorphism of graded algebras of type .
For every subset J of I, the canonical homomorphism (no. 7) is, in fact, a homomorphism of graded algebras of type , as follows immediately from the above.
Proposition 12
("associativity" of the tensor -product of graded algebras of the same types). *With the notation of Proposition 10 of no. 7, suppose that all the are equal to the same monoid ; let be a partition of I. With the notation of Proposition 11 of no. 7, suppose that the right hand side of formula (32) (no. 7) depends only on the sums , for every ordered pair of distinct indices, all and all ; let denote the right hand side of (32). *Then is a system of commutation factors over the family , where for all . *If is the graded tensor -product of type of the family , there exists one and only one isomorphism of graded algebras of type , , such that
provided that total orderings are chosen on the and on I as described in no. 7, Proposition 11.
By the hypothesis, for in , for some and some , as is seen by considering the elements and such that for , for ; it follows immediately that the form a system of commutation factors. The rest of the proof is then analogous to that of Proposition 11 (no. 7) and is left to the reader.
Note that the additional hypotheses of Proposition 12 are fulfilled when and that is, either the trivial system of factors for all , or the system of factors defined by ; in the latter case, the right hand side of formula (32) is equal to , where
Remark
(1) Let I be an infinite indexing set and a commutative monoid; let denote the family such that for all and suppose given for every ordered pair of distinct indices of I a mapping satisfying conditions (22), (23) and (24) (no. 7); this will also be called a system of commutation factors over the family . Consider a family of graded A-algebras of type ; for each finite subset J of I, let denote a graded tensor -product of type of the subfamily (with an arbitrary choice of a total ordering on J). If J, J' are two finite subsets of I such that , a canonical homomorphism of graded algebras of type , h_{J'J}: E_J \to E_{J'}, has been defined above and the uniqueness properties of these homomorphisms show immediately that if J \subset J' \subset J'' are three finite subsets of I, then h_{J''J} = h_{J'J'} \circ h_{J'J}. Thus there is a direct system (E_J, h_{J'J}) of graded algebras of type (§ 3, no. 3), whose indexing set is the right directed set of finite subsets of I. The graded algebra of type , the direct limit of this direct system (§ 3, no. 3), is called a graded tensor -product of type of the family ; it is also denoted by . When all the are equal to and , the tensor product is also called the skew tensor product of the family and is denoted by . We leave to the reader the task of formulating and proving the proposition which generalizes Proposition 10 of no. 7 to the case where I is infinite, as Proposition 8 of no. 5 generalizes Proposition 5 of no. 2 to the case where I is infinite. Note that the underlying A-module of is the same as that underlying the (non-graded) tensor product of the family of non-graded algebras defined in no. 5.
(2) Let E be a graded A-algebra of type (where is a commutative monoid) and a ring homomorphism; the graduation on (II, § 11, no. 5) is identical with the graduation on the graded tensor product , where B has the trivial graduation.
9. Anticommutative algebras and alternating algebras
Definition 7
A graded A-algebra E of type is called anticommutative if for all non-zero homogeneous elements x, y of E
The algebra E is called alternating if it is anticommutative and also for every homogeneous element of odd degree.
Remark
(1) Let be the graded subalgebra of E the direct sum of the (); it follows from Definition 7 that if E is anticommutative, is a subalgebra contained in the centre of E (and hence commutative).
(2) Suppose that 2 is not a divisor of 0 in E; then if E is anticommutative E is alternating, since for homogeneous and of odd degree, by (36), whence and by virtue of the hypothesis.
(3) We shall study in detail in § 7 important examples of alternating algebras.
Lemma 4
Let E be a graded algebra of type and S a set of homogeneous elements ; the set F of elements of E all of whose homogeneous components satisfy relation (36) for all is a graded subalgebra of E.
It suffices to note that: (1) if are two homogeneous elements of the same degree , a homogeneous element of degree and , , then also ; (2) if are two homogeneous elements of respective degrees , a homogeneous element of degree and , , then
Proposition 13
Let E be a graded A-algebra of type and S a generating system of the algebra E consisting of homogeneous elements ; for E to be anticommutative (resp. alternating), it is necessary and sufficient that (36) hold for all and (resp. that this condition hold and further that for all homogeneous of odd degree belonging to S).
We consider first the case of anticommutative algebras. By Lemma 4, the subalgebra F consisting of the elements all of whose homogeneous components satisfy (36) for all , contains all the elements of S and hence . If now is similarly the subalgebra of E consisting of the elements all of whose homogeneous components satisfy (36) for every homogeneous element , it follows from the above that contains all the elements of S and hence , which completes the proof of the proposition in this case.
To prove the proposition in the case of alternating algebras, it can be assumed that E is already anticommutative; it is then immediate that every homogeneous element of odd degree in E is of the form , where and is of odd degree (using the fact that is contained in the centre of E); it follows that since by hypothesis and by (36).
Proposition 14
Let E and F be two graded A-algebras of type , both anticommutative (resp. alternating). Then the skew tensor product (no. 7) is an anticommutative (resp. alternating) algebra.
A generating system of consists of the , where (resp. ) is a homogeneous element of E (resp. F). Consider two such elements , with , so that is of degree and of degree . Then by definition (no. 7, formula (27)) and by virtue of (36),
Corollary
Let E be an anticommutative* (resp. alternating) *graded A-algebra of type . Then for every ring homomorphism , the graded B-algebra (no. 8, Remark 2) is anticommutative (resp. alternating).
The ring B with the trivial graduation can be considered as an alternating A-algebra and , hence Proposition 14 can be applied.
Remark
Let E be an anticommutative graded A-algebra of type . Then the A-linear mapping of into E defined by multiplication of E (, no. 3) is a homomorphism of the graded A-algebra into E, for in the notation of Proposition 14, in the algebra E,
Exercises
See the exercises for § 4.