Bourbaki

§ 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

m′=⨂i∈Imi:⨂i∈I(Ei⊗AEi)→⨂i∈IEi=E; m' = \bigotimes_{i \in I} m_i: \bigotimes_{i \in I} (E_i \otimes_A E_i) \to \bigotimes_{i \in I} E_i = E;

the composite mapping

(⨂i∈IEi)⊗A(⨂i∈IEi)→τ⨂i∈I(Ei⊗AEi)→m′⨂i∈IEi \left( \bigotimes_{i \in I} E_i \right) \otimes_A \left( \bigotimes_{i \in I} E_i \right) \xrightarrow{\tau} \bigotimes_{i \in I} (E_i \otimes_A E_i) \xrightarrow{m'} \bigotimes_{i \in I} E_i

where τ\tau is the associativity isomorphism (II, § 3, no. 9) is an A-linear mapping m:E⊗AE→Em : E \otimes_A E \to E; we shall see that mm defines an (associative and unital) algebra structure on EE. For, on explicitly performing the multiplication defined by mm, we obtain the formula

(1)

(⨂i∈Ixi)(⨂i∈Iyi)=⨂i∈I(xiyi)for xi,yi in Ei and i∈I. \left( \bigotimes_{i \in I} x_i \right) \left( \bigotimes_{i \in I} y_i \right) = \bigotimes_{i \in I} (x_i y_i) \quad \text{for } x_i, y_i \text{ in } E_i \text{ and } i \in I.

It is therefore seen already, by linearity, that if eie_i is the unit element of EiE_i, e=⨂i∈Ieie = \bigotimes_{i \in I} e_i is unit element of EE. On the other hand, the associativity of each of the EiE_i implies the relation

((⨂i∈Ixi)(⨂i∈Iyi))(⨂i∈Izi)=⨂i∈I(xiyizi)=(⨂i∈Ixi)((⨂i∈Iyi)(⨂i∈Izi)) \left( \left( \bigotimes_{i \in I} x_i \right) \left( \bigotimes_{i \in I} y_i \right) \right) \left( \bigotimes_{i \in I} z_i \right) = \bigotimes_{i \in I} (x_i y_i z_i) = \left( \bigotimes_{i \in I} x_i \right) \left( \left( \bigotimes_{i \in I} y_i \right) \left( \bigotimes_{i \in I} z_i \right) \right)

whence, by linearity, the relation x(yz)=(xy)zx(yz) = (xy)z for all x,y,zx, y, z in EE.

Definition 1

Given a family* (Ei)i∈I(E_i)_{i \in I} of algebras over AA, the tensor product of this family, denoted by ⨂i∈IEi\bigotimes_{i \in I} E_i (or, when II is the interval {1,n}\{1, n\} of N\mathbf{N}, E1⊗AE2⊗⋯⊗AEnE_1 \otimes_A E_2 \otimes \cdots \otimes_A E_n, or simply E1⊗E2⊗⋯⊗EnE_1 \otimes E_2 \otimes \cdots \otimes E_n) is the algebra obtained by giving the tensor product of the AA*-modules* EiE_i the multiplication defined by (1).

Relation (1) shows that the tensor product ⨂i∈IEi0\bigotimes_{i \in I} E_i^0 of the opposite algebras to the EiE_i is the opposite algebra to ⨂i∈IEi\bigotimes_{i \in I} E_i; in particular, if the EiE_i are commutative, so is ⨂i∈IEi\bigotimes_{i \in I} E_i.

Let (Ei)i∈I(E_i)_{i \in I} and (Fi)i∈I(F_i)_{i \in I} be two families of AA-algebras with the same finite indexing set II. For each i∈Ii \in I, let fi:Ei→Fif_i : E_i \to F_i be an AA-algebra homomorphism. Then the AA-linear mapping

f=⨂i∈Ifi:⨂i∈IEi→⨂i∈IFi f = \bigotimes_{i \in I} f_i : \bigotimes_{i \in I} E_i \to \bigotimes_{i \in I} F_i

is an A-algebra homomorphism, as follows from (1).

For every partition (Ij)j∈J(I_j)_{j \in J} of II, the associativity isomorphisms

⨂j∈J(⨂i∈IjEi)→⨂i∈IEi \bigotimes_{j \in J} \left( \bigotimes_{i \in I_j} E_i \right) \to \bigotimes_{i \in I} E_i

(II, § 3, no. 9) are also algebra isomorphisms, as follows from (1) and their definitions.

When II is the interval [1,n][1, n] of N\mathbf{N} and all the algebras EiE_i are equal to the same algebra EE, the tensor product algebra ⨂i∈IEi\bigotimes_{i \in I} E_i is also denoted by E⊗nE^{\otimes n}.

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 E,FE, F be two AA-algebras; if aa (resp. bb) is a left ideal of EE (resp. FF), the canonical image Im⁡(a⊗b)\operatorname{Im}(a \otimes b) of a⊗Aba \otimes_A b in E⊗AFE \otimes_A F is a left ideal of E⊗AFE \otimes_A F; there are analogous results when "left ideal" is replaced by "right ideal" or "two-sided ideal". Moreover:

Proposition 1

Let E,FE, F be two AA-algebras and aa (resp. bb) a two-sided ideal of EE (resp. FF). Then the canonical AA-module isomorphism

(E/a)⊗(E/b)→(E⊗F)/(Im⁡(a⊗F)+Im⁡(E⊗b)) (E/a) \otimes (E/b) \to (E \otimes F)/(\operatorname{Im}(a \otimes F) + \operatorname{Im}(E \otimes b))

(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 EE be an AA-algebra and aa an ideal of AA. Then the AA-module aEaE is a two-sided ideal of EE and the canonical (A/a)(A/a)-module isomorphism

(A/a)⊗AE→E/aE (A/a) \otimes_A E \to E/aE

is an (A/a)(A/a)*-algebra isomorphism*.

Corollary 2

If a,ba, b are two ideals of AA, (A/a)⊗A(A/b)(A/a) \otimes_A (A/b) is canonically isomorphic to A/(a+b)A/(a + b)*.

Corollary 3

Let E,FE, F be two AA-algebras and aa an ideal of AA contained in the annihilator of FF. Then the (A/a)(A/a)-algebra E⊗AFE \otimes_A F is canonically isomorphic to (E/aE)⊗A/aF(E/aE) \otimes_{A/a} F*.

Proposition 2

Let (Eλ)λ∈L(E_\lambda)_{\lambda \in L} and (Fμ)μ∈M(F_\mu)_{\mu \in M} be two families of AA-algebras. The canonical mapping* (II, § 3, no. 7)

(⨁λ∈LEλ)⊗A(⨁μ∈MFμ)→⨁(λ,μ)∈L×M(Eλ⊗AFμ) \left( \bigoplus_{\lambda \in L} E_\lambda \right) \otimes_A \left( \bigoplus_{\mu \in M} F_\mu \right) \to \bigoplus_{(\lambda, \mu) \in L \times M} (E_\lambda \otimes_A F_\mu)

is an algebra isomorphism.

This follows immediately from II, § 3, no. 7, Proposition 7 and the definition of multiplication on E⊗FE \otimes F.

Proposition 3

Let A,BA, B be two commutative rings, φ:A→B\varphi : A \to B a ring homomorphism and E,FE, F two AA-algebras. Then the canonical BB-module isomorphism

φ∗(E)⊗Bφ∗(F)→φ∗(E⊗AF) \varphi^*(E) \otimes_B \varphi^*(F) \to \varphi^*(E \otimes_A F)

(II, § 5, no. 1, Proposition 3) is a BB-algebra isomorphism.

Proposition 4

Let A,BA, B be two commutative rings, ρ:A→B\rho : A \to B a ring homomorphism, EE an AA-algebra and FF a BB-algebra. Then the canonical AA-module isomorphism

ρ∗(F)⊗AE→ρ∗(F⊗Bρ∗(E)) \rho_*(F) \otimes_A E \to \rho_*(F \otimes_B \rho^*(E))

(II, § 5, no. 2, Proposition 6) is an AA-algebra isomorphism.

The verifications are trivial on account of § 1, no. 5.

In particular, the AA-algebra structure on B⊗AEB \otimes_A E, obtained by restricting the ring BB of scalars to AA, is identical with the structure of the algebra B⊗AEB \otimes_A E, the tensor product of the AA-algebras BB and EE.

Finally, if (Ai,ϕji)(A_i, \phi_{ji}) is a direct system of commutative rings, (Ei,fji)(E_i, f_{ji}) and (Fi,gji)(F_i, g_{ji}) two direct systems of AiA_i-algebras (§1§ 1, no. 6) and A=lim⁡→AiA = \lim \rightarrow A_i, the canonical AA-module isomorphism

lim⁡→(Ei⊗AiFi)→(lim⁡→Ei)⊗A(lim⁡→Fi) \lim \rightarrow (E_i \otimes_{A_i} F_i) \to (\lim \rightarrow E_i) \otimes_A (\lim \rightarrow F_i)

(II, § 6, no. 3, Proposition 7) is also an AA-algebra isomorphism, as follows from the definitions.

Examples of tensor products of algebras. (1) Let AA be a commutative ring and M,NM, N two AA-modules; the canonical mapping

EndA(M)⊗AEndA(N)→EndA(M⊗AN) \text{End}_A(M) \otimes_A \text{End}_A(N) \to \text{End}_A(M \otimes_A N)

(II, § 4, no. 4) is an AA-algebra homomorphism, as follows from II, § 3, no. 2, formula (5). When MM or NN is a finitely generated projective AA-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 S,TS, T be two monoids and A(S)A^{(S)} and A(T)A^{(T)} the algebras of the monoids SS and TT over the ring AA (III, § 2, no. 6); then there is a canonical AA-algebra isomorphism

A(S)⊗AA(T)→A(S×T). A^{(S)} \otimes_A A^{(T)} \to A^{(S \times T)}.

The elements es⊗ete_s \otimes e_t (resp. e(s,t)e_{(s,t)}), where ss runs through SS and tt runs through TT, form a basis of A(S)⊗AA(T)A^{(S)} \otimes_A A^{(T)} by virtue of II, § 3, no. 7, Corollary 2 to Proposition 7 (resp. of A(S×T)A^{(S \times T)}; the desired isomorphism is obtained by mapping es⊗ete_s \otimes e_t to e(s,t)e_{(s,t)} and it follows from the definitions that this is indeed an algebra isomorphism.

2. Universal characterization of tensor products of algebras

Proposition 5

Let (Ei)i∈I(E_i)_{i \in I} be a finite family of AA-algebras and, for each i∈Ii \in I, let eie_i be the unit element of EiE_i. For each i∈Ii \in I, let ui:Ei→E=⨂i∈IEiu_i : E_i \to E = \bigotimes_{i \in I} E_i be the AA-linear mapping defined by

ui(xi)=⨂jxj′with xi′=xi and xj′=ej for j≠i. u_i(x_i) = \bigotimes_j x'_j \quad \text{with } x'_i = x_i \text{ and } x'_j = e_j \text{ for } j \neq i.

(i) *The uiu_i are A\mathbf{A}-algebra isomorphisms; further, for i≠ji \neq j, the elements ui(xi)u_i(x_i) and uj(xj)u_j(x_j) are permutable in E\mathbf{E} for all xi∈Eix_i \in \mathbf{E}_i and xj∈Ejx_j \in \mathbf{E}_j and E\mathbf{E} is generated by the union of the subalgebras ui(Ei)u_i(\mathbf{E}_i).

(ii) Let F\mathbf{F} be an A\mathbf{A}-algebra and, for all i∈Ii \in \mathbf{I}, let vi:Ei→Fv_i : \mathbf{E}_i \to \mathbf{F} be an A\mathbf{A}-algebra homomorphism, where the viv_i are such that, for i≠ji \neq j, vi(xi)v_i(x_i) and vj(xj)v_j(x_j) are permutable in F\mathbf{F} for all xi∈Eix_i \in \mathbf{E}_i and xj∈Ejx_j \in \mathbf{E}_j. Then there exists one and only one A\mathbf{A}-algebra homomorphism w:E→Fw : \mathbf{E} \to \mathbf{F} such that

vi=w∘uifor all i∈I. v_i = w \circ u_i \quad \text{for all } i \in \mathbf{I}.

(i) The mapping uiu_i is an algebra homomorphism by definition of the multiplication on E\mathbf{E}. If i≠ji \neq j, xi∈Ei,xj∈Ejx_i \in \mathbf{E}_i, x_j \in \mathbf{E}_j, then

ui(xi)=⨂kxk′with xi′=xi,xk′=ek for k≠i, u_i(x_i) = \bigotimes_k x'_k \quad \text{with } x'_i = x_i, x'_k = e_k \text{ for } k \neq i,
uj(xj)=⨂kxk′′with xj′′=xj,xk′′=ek for k≠j. u_j(x_j) = \bigotimes_k x''_k \quad \text{with } x''_j = x_j, x''_k = e_k \text{ for } k \neq j.

Clearly xk′xk′′=xk′′xk′x'_k x''_k = x''_k x'_k for all k∈Ik \in \mathbf{I} and hence ui(xi)u_i(x_i) and uj(xj)u_j(x_j) commute in E\mathbf{E} by formula (1) (no. 1) defining the multiplication in E\mathbf{E}. The last assertion follows from the relation ⨂ixi=∏i∈Iui(xi)\bigotimes_i x_i = \prod_{i \in \mathbf{I}} u_i(x_i).

(ii) For each i∈Ii \in \mathbf{I}, let xix_i be an element of Ei\mathbf{E}_i. The product ∏i∈Ivi(xi)\prod_{i \in \mathbf{I}} v_i(x_i) is then defined in F\mathbf{F} independently of any ordering on I\mathbf{I} since the algebra F\mathbf{F} is associative and the elements vi(xi)v_i(x_i) are pairwise permutable. The mapping (xi)i∈I→∏i∈Ivi(xi)(x_i)_{i \in \mathbf{I}} \to \prod_{i \in \mathbf{I}} v_i(x_i) of ∏i∈IEi\prod_{i \in \mathbf{I}} \mathbf{E}_i into F\mathbf{F} is obviously A\mathbf{A}-multilinear and there therefore exists one and only one A\mathbf{A}-linear mapping w:E→Fw : \mathbf{E} \to \mathbf{F} such that

w(⨂ixi)=∏ivi(xi). w\left( \bigotimes_i x_i \right) = \prod_i v_i(x_i).

Now, the desired A\mathbf{A}-algebra homomorphism w:E→Fw : \mathbf{E} \to \mathbf{F} must satisfy (5), which follows from (4) and the fact that ⨂ixi=∏i∈Iui(xi)\bigotimes_i x_i = \prod_{i \in \mathbf{I}} u_i(x_i). This proves the uniqueness of ww; it remains to show that the A\mathbf{A}-linear mapping ww defined by (5) is an A\mathbf{A}-algebra homomorphism and satisfies (4). The fact that ww satisfies (4) is obvious: it suffices to apply (5) to the case where xj=ejx_j = e_j for j≠ij \neq i and we obtain w(ui(xi))=vi(xi)w(u_i(x_i)) = v_i(x_i). Finally, ww is an algebra homomorphism, for

w((⨂ixi)(⨂iyi))=w(⨂i(xiyi))=∏ivi(xiyi) w\left( \left( \bigotimes_i x_i \right) \left( \bigotimes_i y_i \right) \right) = w\left( \bigotimes_i (x_i y_i) \right) = \prod_i v_i(x_i y_i)
=∏i(vi(xi)vi(yi))=(∏ivi(xi))⋅(∏ivi(yi)) = \prod_i (v_i(x_i) v_i(y_i)) = \left( \prod_i v_i(x_i) \right) \cdot \left( \prod_i v_i(y_i) \right)

since vi(xi)v_i(x_i) commutes with vj(yj)v_j(y_j) for j≠ij \neq i; hence

ww((⨂ixi)(⨂iyi))=w(⨂ixi).w(⨂iyi) w w \left( \left( \bigotimes_i x_i \right) \left( \bigotimes_i y_i \right) \right) = w \left( \bigotimes_i x_i \right) . w \left( \bigotimes_i y_i \right)

which, by linearity, completes the proof.

The ordered pair consisting of E and the canonical mapping ϕ:(xi)↦⨂ixi\phi : (x_i) \mapsto \bigotimes_i x_i of ∏iEi\prod_i E_i into E is a solution of the universal mapping problem (Set Theory, IV, § 3, no. 1) where Σ\Sigma is the species of A-algebra structure, the morphisms being the A-algebra homomorphisms and the α\alpha-mappings the mappings ∏iui\prod_i u_i of ∏iEi\prod_i E_i into an A-algebra such that the uiu_i are A-algebra homomorphisms and ui(xi)u_i(x_i) and uj(xj)u_j(x_j) commute for i≠ji \neq j, for all xi∈Eix_i \in E_i and xj∈Ejx_j \in E_j.

Corollary

Let* (Ei)i∈I,(Fi)i∈I(E_i)_{i \in I}, (F_i)_{i \in I} be two finite families of A-algebras and, for all i∈Ii \in I, let fi:Ei→Fif_i : E_i \to F_i be an algebra homomorphism. If ui:Ei→⨂j∈IEj,vi:Fi→⨂j∈IFju_i : E_i \to \bigotimes_{j \in I} E_j, v_i : F_i \to \bigotimes_{j \in I} F_j are the canonical homomorphisms, the mapping f=⨂ifif = \bigotimes_i f_i (cf. no. 1) is the unique A-algebra homomorphism such that f∘ui=vi∘fif \circ u_i = v_i \circ f_i for all i∈Ii \in I.

It suffices to note that the homomorphisms gi=vi∘fig_i = v_i \circ f_i are such that gi(xi)=vi(fi(xi))g_i(x_i) = v_i(f_i(x_i)) and gj(xj)=vj(fj(xj))g_j(x_j) = v_j(f_j(x_j)) commute for i≠ji \neq j, xi∈Eix_i \in E_i and xj∈Ejx_j \in E_j; then apply Proposition 5.

When, in Proposition 5, the algebra F is assumed to be commutative, the hypothesis that vi(xi)v_i(x_i) and vj(xj)v_j(x_j) are permutable for i≠ji \neq j is automatically satisfied. Hence, when F is commutative, there is a canonical bijection

HomA-alg.(⨂iEi,F)→∏iHomA-alg.(Ei,F), \text{Hom}_{A\text{-alg.}} \left( \bigotimes_i E_i, F \right) \to \prod_i \text{Hom}_{A\text{-alg.}} (E_i, F),

namely the one which associates with every homomorphism ww of ⨂iEi\bigotimes_i E_i into F the family of w∘uiw \circ u_i.

Note that if E is a commutative A-algebra, the ring structure of E⊗AFE \otimes_A F is the same as that of F(E)F_{(E)} (§ 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 η:A→E\eta : A \to E (§ 1, no. 4) then defines on M an A-module structure, said to be underlying the E-module structure on M; for α∈A,s∈E,x∈M\alpha \in A, s \in E, x \in M,

α(sx)=s(αx)=(αs)x, \alpha(sx) = s(\alpha x) = (\alpha s)x,

so that for all s∈Es \in E, the homothety hs:x↦sxh_s : x \mapsto sx 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 s↦hss \mapsto h_s of E into EndA(M)\mathrm{End}_A(M).

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 e′e' are the unit elements of E and F respectively, then

(αe)x=(αe′)xfor α∈A,x∈M; (\alpha e)x = (\alpha e')x \quad \text{for } \alpha \in A, x \in M;

then αx\alpha x 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 s↦hs′s \mapsto h'_s of E into EndA(M)\mathrm{End}_A(M) and t↦ht′′t \mapsto h''_t of F into EndA(M)\mathrm{End}_A(M) such that hs′ht′′=ht′′hs′h'_s h''_t = h''_t h'_s for all s∈Es \in E and t∈Ft \in F. Consequently (no. 2, Proposition 5) an A-algebra homomorphism u↦huu \mapsto h_u of E⊗AFE \otimes_A F into EndA(M)\mathrm{End}_A(M) is canonically derived such that hs⊗t=hs′ht′′=ht′′hs′h_{s \otimes t} = h'_s h''_t = h''_t h'_s for s∈Es \in E and t∈Ft \in F. In other words, an (E⊗AF)(E \otimes_A F)-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

(s⊗t).x=s(tx)=t(sx)for s∈E,t∈F and x∈M. (s \otimes t).x = s(tx) = t(sx) \quad \text{for } s \in E, t \in F \text{ and } x \in M.

The given E-module and F-module structures on M can be derived from this (E⊗AF)(E \otimes_A F)-module structure by restrictions of the ring of scalars, corresponding to the two canonical homomorphisms E→E⊗AFE \to E \otimes_A F and F→E⊗AFF \to E \otimes_A F.

Conversely, if an (E⊗AF)(E \otimes_A F)-module structure is given on M, by means of the canonical homomorphisms E→E⊗AFE \to E \otimes_A F and F→E⊗AFF \to E \otimes_A F 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 (E⊗AF)(E \otimes_A F)-module structure is associated with this bimodule structure.

Thus a one-to-one correspondence has been established between (E⊗AF)(E \otimes_A F)-module and bimodules over the algebras E and F. Clearly every sub-bimodule of M is a submodule for the associated (E⊗AF)(E \otimes_A F)-module structure and conversely. There are analogous results for quotients, products, direct sums and inverse and direct limits. Finally, if M′M' is another bimodule over the algebras E and F and f:M→M′f : M \to M' is a bimodule homomorphism, ff is also an (E⊗AF)(E \otimes_A F)-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 (E,F)(E, F)-bimodule and being given such a structure amounts to being given a left bimodule structure over E and FoF^o.

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 (αe)x=x(αe)=αx(\alpha e)x = x(\alpha e) = \alpha x for all x∈Bx \in B and all α∈A\alpha \in A; B can therefore be considered as a left bimodule over the algebras B and BoB^o (opposite to B); there is therefore associated with the (B, B)-bimodule structure on B a (B ⊗ABo\otimes_A B^o)-module structure such that, for b,xb, x and b′b' in B,

(b⊗b′).x=bxb′ (b \otimes b').x = bx b'

the right-hand side being the product in the ring B.

(2) Let E and F be two A-algebras, e,e′e, e' 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 M⊗ANM \otimes_A N, defined by

x.(m⊗n)=(x.m)⊗n,y.(m⊗n)=m⊗(y.n) x.(m \otimes n) = (x.m) \otimes n, \quad y.(m \otimes n) = m \otimes (y.n)

for x∈E,y∈F,m∈M,n∈Nx \in E, y \in F, m \in M, n \in N (II, § 3, no. 4); it is also seen that conditions (8) hold and hence the above bimodule structure is associated with an (E⊗AF)(E \otimes_A F)-module structure on M⊗ANM \otimes_A N, such that

(x⊗y).(m⊗n)=(x.m)⊗(y.n) (x \otimes y).(m \otimes n) = (x.m) \otimes (y.n)

for x∈E,y∈F,m∈M,n∈Nx \in E, y \in F, m \in M, n \in N.

In particular, taking M=Es,Es⊗ANM = E_s, E_s \otimes_A N has canonically an (E⊗AF)(E \otimes_A F)-module structure; on the other hand, E⊗ANE \otimes_A N is canonically identified with E⊗A(Fd⊗FN)=(E⊗AF)⊗FNE \otimes_A (F_d \otimes_F N) = (E \otimes_A F) \otimes_F N, where E⊗AFE \otimes_A F is considered as having its right F-module structure defined by the canonical homomorphism v:F→E⊗AFv : F \to E \otimes_A F; for x,x′x, x' in E, y∈F,n∈Ny \in F, n \in N, x′⊗nx' \otimes n is thus identified with (x′⊗e′)⊗n(x' \otimes e') \otimes n and (x⊗y).(x′⊗n′)=(xx′)⊗(y.n)(x \otimes y).(x' \otimes n') = (xx') \otimes (y.n) with ((xx′)⊗y)⊗n((xx') \otimes y) \otimes n. The (E⊗AF)(E \otimes_A F)-module Es⊗ANE_s \otimes_A N is thus identified with the (E⊗AF)(E \otimes_A F)-module derived from N by extending the scalars to E⊗AFE \otimes_A F by means of the homomorphism vv (II, § 5, no. 1). The canonical mapping n↦e⊗nn \mapsto e \otimes n of N into Es⊗ANE_s \otimes_A N is identified with the canonical mapping n↦(e⊗e′)⊗nn \mapsto (e \otimes e') \otimes n of N into (E⊗AF)⊗FN(E \otimes_A F) \otimes_F N; 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)

P⊗E⊗AF(Es⊗AN)→P⊗FN P \otimes_{E \otimes_A F} (E_s \otimes_A N) \to P \otimes_F N

where on the right-hand side P is considered as a right F-module by means of the canonical homomorphism vv. For P is canonically identified with P⊗E⊗AF(E⊗AF)P \otimes_{E \otimes_A F} (E \otimes_A F) and (E⊗AF)⊗FN(E \otimes_A F) \otimes_F N with E⊗A(F⊗FN)E \otimes_A (F \otimes_F N) and hence with E⊗ANE \otimes_A N, 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 e,e′e, e' are non-zero. Then the homomorphisms ηE:K→E\eta_E : K \to E and ηF:K→F\eta_F : K \to F (§ 1, no. 3) are injections which allow us to identify K with a subfield of E (resp. F). The canonical homomorphisms u:E→E⊗KFu : E \to E \otimes_K F and v:F→E⊗KFv : F \to E \otimes_K F, defined by u(x)=x⊗e′u(x) = x \otimes e' and v(y)=e⊗yv(y) = e \otimes y are injective (II, § 7, no. 9, Proposition 19) and allow us to identify E and F with subalgebras of E⊗KFE \otimes_K F, both having as unit element the unit element e⊗e′e \otimes e' of E⊗KFE \otimes_K F. In E⊗KF,E∩F=KE \otimes_K F, E \cap F = K (II, § 7, no. 9, Proposition 19).

If E' and F' are subalgebras of E and F respectively, the canonical homomorphism E′⊗KF′→E⊗KFE' \otimes_K F' \to E \otimes_K F is injective and allows us to identify E′⊗KF′E' \otimes_K F' with the subalgebra of E⊗KFE \otimes_K F generated by E′∪F′E' \cup F' (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 z=∑ixi⊗yiz = \sum_i x_i \otimes y_i of the centralizer of C⊗KDC \otimes_K D (xi∈F,yi∈Fx_i \in F, y_i \in F) belongs to C′⊗KD′C' \otimes_K D'; we know that

C′⊗KD′=(C′⊗KF)∩(E⊗KD′) C' \otimes_K D' = (C' \otimes_K F) \cap (E \otimes_K D')

(II, § 7, no. 7, Corollary to Proposition 14). The yiy_i may be assumed to be linearly independent over K; for all x∈Cx \in C, of necessity (x⊗e′)z=z(x⊗e′)(x \otimes e')z = z(x \otimes e'), that is ∑i(xxi−xix)⊗yi=0\sum_i (xx_i - x_ix) \otimes y_i = 0, whence xxi=xixxx_i = x_ix for all ii (II, § 3, no. 7, Corollary 1 to Proposition 7); hence of necessity xi∈C′x_i \in C' for all ii and therefore z∈C′⊗KFz \in C' \otimes_K F; it can similarly be shown that z∈E⊗KD′z \in E \otimes_K D', 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 i:E→G,j:F→Gi : E \to G, j : F \to G define a canonical homomorphism h=i⊗j:E⊗KF→Gh = i \otimes j : E \otimes_K F \to G (no. 2, Proposition 5) such that

(i⊗j)(x⊗y)=xyfor x∈E,y∈F. (i \otimes j)(x \otimes y) = xy \quad \text{for } x \in E, y \in F.

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 E⊗KFE \otimes_K F 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 h:E⊗KF→Gh : E \otimes_K F \to G is an isomorphism of E⊗KFE \otimes_K F onto the subalgebra of G generated by E∪FE \cup F; (ii) E∩F=K;E \cap F = K; (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 E⊗KFE \otimes_K F 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 E⊗KFE \otimes_K F under h is the set of sums ∑ixiyi=∑iyixi\sum_i x_i y_i = \sum_i y_i x_i in G, with xi∈Ex_i \in E and yi∈Fy_i \in F; if (aλ)(a_\lambda) is a basis of E over K, H is therefore also the submodule of the (right or left) F-module G, generated by (aλ)(a_\lambda). The condition of the statement therefore means that there exists a basis (aλ)(a_\lambda) 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 E⊗KFE \otimes_K F 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 E∪FE \cup F be such that*

[H:K]=[E:K]⋅[F:K]. [H : K] = [E : K] \cdot [F : K].
This says that the rank over K of the surjective canonical homomorphism h : E \otimes_K F \to H is equal to the rank of E \otimes_K F over K, which is equivalent to saying that this homomorphism is bijective (II, § 7, No. 4, Proposition 9).

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 ⨂i∈JEi\bigotimes_{i \in J} E_i of the algebras E_i of index i∈Ji \in J; let eie_i denote the unit element of E_i and eJ=⨂i∈Jeie_J = \bigotimes_{i \in J} e_i the unit element of E_J; let fJ,if_{J,i} denote the canonical homomorphism Ei→EJE_i \to E_J for i∈Ji \in J (no. 2, Proposition 5). If J, J' are two finite subsets of I such that J⊂J′J \subset J', a homomorphism fJ′J:EJ→EJ′f_{J'J} : E_J \to E_{J'} is canonically derived (no. 2, Proposition 5), by the condition fJ′J∘fJ,i=fJ′,if_{J'J} \circ f_{J,i} = f_{J',i} for all i∈Ji \in J. Moreover the uniqueness of fJ′Jf_{J'J} implies that if J, J', J'' are three finite subsets of I such that J⊂J′⊂J′′J \subset J' \subset J'', then fJ′′J=fJ′′J′∘fJ′Jf_{J''J} = f_{J''J'} \circ f_{J'J}. In other words, (EJ,fJ′J)(E_J, f_{J'J}) is a direct system of A-algebras whose indexing set is the right directed set F(I)\mathscr{F}(I) of finite subsets of I.

Definition 5

The direct limit E of the direct system* (EJ,fJ′J)(E_J, f_{J'J}) is called the tensor product of the family of A-algebras (Ei)i∈I(E_i)_{i \in I}.

If I is finite, E is identified with ⨂i∈IEi\bigotimes_{i \in I} E_i. By an abuse of notation, E is also denoted by ⨂i∈IEi\bigotimes_{i \in I} E_i even if I is infinite.

For every finite subset J of I, let fJf_J denote the canonical homomorphism ⨂i∈JEi→⨂i∈IEi\bigotimes_{i \in J} E_i \to \bigotimes_{i \in I} E_i (writing fif_i instead of f{i}f_{\{i\}}); if e is the unit element of ⨂i∈IEi\bigotimes_{i \in I} E_i, then fJ(eJ)=ef_J(e_J) = e for all J∈F(I)J \in \mathscr{F}(I). It is immediate that if all the algebras E_i are commutative, so is ⨂i∈IEi\bigotimes_{i \in I} E_i.

Proposition 8

(i) The homomorphisms fi:Ei→E=⨂k∈IEkf_i : E_i \to E = \bigotimes_{k \in I} E_k are such that for two indices i, j such that i≠ji \neq j, fi(xi)f_i(x_i) and fj(xj)f_j(x_j) commute in E for all xi∈Eix_i \in E_i and xj∈Ejx_j \in E_j; further, E is generated by the union of the subalgebras fi(Ei)f_i(E_i).

(ii) Let F be an A-algebra and, for all i∈Ii \in I, let ui:Ei→Fu_i : E_i \to F be an A-algebra homomorphism such that, for i≠ji \neq j, ui(xi)u_i(x_i) and uj(xj)u_j(x_j) commute in F for all xi∈Eix_i \in E_i and xj∈Ejx_j \in E_j. Then there exists one and only one A-algebra homomorphism u:E→Fu : E \to F such that ui=u∘fiu_i = u \circ f_i for all i∈Ii \in I.

(i) As, for every finite subset J of I, fi=fJ∘fJ,if_i = f_J \circ f_{J,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 fJ(EJ)f_J(E_J) when J runs through F(I)\mathscr{F}(I).

(ii) For every finite subset J of I, it follows from no. 2, Proposition 5 that there exists a unique homomorphism uJ:EJ→Fu_J : E_J \to F such that uJ∘fJ,i=uiu_J \circ f_{J,i} = u_i for all i∈Ji \in J; it immediately follows from this uniqueness property that, for J⊂J′J \subset J', uJ=uJ′∘fJ′Ju_J = u_{J'} \circ f_{J'J}; in other words, the uJu_J form a direct system of homomorphisms. Let u=lim⁡→uJ:E→Fu = \lim \to u_J : E \to F; then by definition uJ=u∘fJu_J = u \circ f_J for every finite subset JJ of II and in particular ui=u∘fiu_i = u \circ f_i for all i∈Ii \in I; the uniqueness of uu follows from these relations and the fact that the fi(Ei)f_i(E_i) generate the algebra EE.

Corollary

Let* (Ei)i∈I, (Ei′)i∈I(E_i)_{i \in I},\ (E'_i)_{i \in I} be two families of AA*-algebras with the same indexing set and, for all* i∈Ii \in I, let ui:Ei→Ei′u_i : E_i \to E'_i be an algebra homomorphism. Then there exists one and only one AA*-algebra homomorphism* u:⨂i∈IEi→⨂i∈IEi′u : \bigotimes_{i \in I} E_i \to \bigotimes_{i \in I} E'_i such that, for all i∈Ii \in I, *the diagram

Ei→uiEi′∣∣⨂i∈IEi→u⨂i∈IEi′ \begin{array}{ccc} E_i & \xrightarrow{u_i} & E'_i \\ | & & | \\ \bigotimes_{i \in I} E_i & \xrightarrow{u} & \bigotimes_{i \in I} E'_i \end{array}

is commutative, fif_i and fi′f'_i denoting the canonical homomorphisms.

It suffices to apply Proposition 8 to the homomorphism fi′∘uif'_i \circ u_i.

The homomorphism uu defined in the Corollary to Proposition 8 is denoted by ⨂i∈Iui\bigotimes_{i \in I} u_i. If JJ is any subset of II, Proposition 8 can be applied to the family (fi)i∈J(f_i)_{i \in J} of canonical homomorphisms fi:Ei→⨂i∈IEi=Ef_i : E_i \to \bigotimes_{i \in I} E_i = E; a canonical homomorphism EJ→EE_J \to E is derived which is also denoted by fJf_J and which, when JJ is finite, coincides with the homomorphism denoted thus above.

Now let (xi)i∈I(x_i)_{i \in I} be an element of ∏i∈IEi\prod_{i \in I} E_i such that the family (xi−ei)i∈I(x_i - e_i)_{i \in I} has finite support HH. It is immediate that, if JJ and J′J' are two finite subsets of II containing HH, then

fJ((xi)i∈J)=fJ′((xi)i∈J′). f_J((x_i)_{i \in J}) = f_{J'}((x_i)_{i \in J'}).

The common value of the fJ((xi)i∈J)f_J((x_i)_{i \in J}) for the finite subsets J⊃HJ \supset H of II is denoted by ⨂i∈Ixi\bigotimes_{i \in I} x_i.

Proposition 9

Let* (Ei)i∈I(E_i)_{i \in I} be a family of AA*-algebras and for each* i∈Ii \in I let BiB_i be a basis of EiE_i such that the unit element eie_i belongs to BiB_i. Let BB be the set of elements of the form ⨂i∈Ixi\bigotimes_{i \in I} x_i, where (xi)(x_i) runs through the set of elements of ∏i∈IBi\prod_{i \in I} B_i such that the family (xi−ei)(x_i - e_i) has finite support. Then BB is a basis of the algebra ⨂i∈IEi\bigotimes_{i \in I} E_i and this basis contains the unit element ee.

For every finite subset JJ of II, let BJB_J be the basis of EJ=⨂i∈JEiE_J = \bigotimes_{i \in J} E_i the tensor product of the bases BiB_i for i∈Ji \in J (II, § 3, no. 9). It follows immediately from the definitions that BB is the union of the fJ(BJ)f_J(B_J) when JJ runs through F(I)\mathscr{F}(I) and that fJ′,J(BJ)⊂BJ′f_{J',J}(B_J) \subset B_{J'} when J⊂J′J \subset J'; hence (BJ)(B_J) is a direct system of subsets of the EJE_J and B=lim⁡→BJB = \lim \rightarrow B_J; the conclusion then follows from II, § 6, no. 2, Corollary to Proposition 5.

The basis BB is also called the tensor product of the bases BiB_i for i∈Ii \in I; when the conditions of Proposition 9 are fulfilled, the canonical homomorphisms fJ:EJ→E=⨂i∈IEif_J : E_J \to E = \bigotimes_{i \in I} E_i are injective for every subset JJ of II, for if BJB_J is the basis of EJE_J the tensor product of the BiB_i for i∈Ji \in J, it is immediately verified that the restriction of fJf_J to BJB_J is injective and maps BJB_J onto a subset of BB.

6. Commutation lemmas

Lemma 1

Let AA be a commutative ring, EE an AA-algebra, (xi)1≤i≤n(x_i)_{1 \leq i \leq n} a finite sequence of elements of EE, (λi)1≤i≤n(\lambda_i)_{1 \leq i \leq n} a finite sequence of elements of AA and yy an element of EE; suppose that*

xiy=λiyxifor 1≤i≤n. x_i y = \lambda_i y x_i \quad \text{for } 1 \leq i \leq n.
Then
(x1x2…xn)y=(λ1λ2…λn)y(x1x2…xn). (x_1 x_2 \ldots x_n) y = (\lambda_1 \lambda_2 \ldots \lambda_n) y (x_1 x_2 \ldots x_n).

The lemma being trivial for n=1n = 1, we argue by induction on n≥2n \geq 2. Now

(x1x2…xn)y=(x1…xn−1)(xny)=(x1…xn−1)(λnyxn)=λn((x1…xn−1)y)xn, (x_1 x_2 \ldots x_n) y = (x_1 \ldots x_{n-1})(x_n y) = (x_1 \ldots x_{n-1})(\lambda_n y x_n) = \lambda_n ((x_1 \ldots x_{n-1}) y) x_n,
which, by the induction hypothesis, is equal to
λn(λ1…λn−1)y(x1…xn−1)xn=(λ1…λn−1λn)y(x1…xn−1xn), \lambda_n (\lambda_1 \ldots \lambda_{n-1}) y (x_1 \ldots x_{n-1}) x_n = (\lambda_1 \ldots \lambda_{n-1} \lambda_n) y (x_1 \ldots x_{n-1} x_n),
whence the lemma.

Lemma 2

Let AA be a commutative ring, EE an AA-algebra and (xi)1≤i≤n(x_i)_{1 \leq i \leq n} and (yi)1≤i≤n(y_i)_{1 \leq i \leq n} two finite sequences of nn elements of EE; suppose that for 1≤j≤i≤n1 \leq j \leq i \leq n,*

xiyj=λijyjxiwith λij∈A. x_i y_j = \lambda_{ij} y_j x_i \quad \text{with } \lambda_{ij} \in A.
Then
(x1x2…xn)(y1y2…yn)=(∏i>jλij)(x1y1)(x2y2)…(xnyn). (x_1 x_2 \ldots x_n)(y_1 y_2 \ldots y_n) = \left( \prod_{i > j} \lambda_{ij} \right) (x_1 y_1)(x_2 y_2) \ldots (x_n y_n).

The lemma being trivial for n=1n = 1, we again argue by induction on nn for n≥2n \geq 2. By virtue of Lemma 1,

(x1…xn)(y1…yn)=x1(x2…xn)y1(y2…yn)=(∏i>1λi1)(x1y1)(x2…xn)(y2…yn) (x_1 \ldots x_n)(y_1 \ldots y_n) = x_1 (x_2 \ldots x_n) y_1 (y_2 \ldots y_n) = \left( \prod_{i > 1} \lambda_{i1} \right) (x_1 y_1)(x_2 \ldots x_n)(y_2 \ldots y_n)
and it then suffices to apply the induction hypothesis to obtain (16).

For every family λ=(λij)\lambda = (\lambda_{ij}) of elements of A\mathbf{A}, with 1≤j<i≤n1 \leq j < i \leq n, and for every permutation σ∈Sn\sigma \in \mathfrak{S}_n, we write

εσ(λ)=∏i>j, σ−1(i)<σ−1(j)λij=∏i<j, σ(i)>σ(j)λσ(i), σ(j). \varepsilon_\sigma(\lambda) = \prod_{i > j,\ \sigma^{-1}(i) < \sigma^{-1}(j)} \lambda_{ij} = \prod_{i < j,\ \sigma(i) > \sigma(j)} \lambda_{\sigma(i),\ \sigma(j)}.

Observe that, when A=Z\mathbf{A} = \mathbf{Z} and λij=−1\lambda_{ij} = -1 for every ordered pair (i,j)(i, j) such that 1≤j<i≤n1 \leq j < i \leq n, εσ(λ)\varepsilon_\sigma(\lambda) is just the signature εσ\varepsilon_\sigma of the permutation σ\sigma (I, § 5, no. 7).

Lemma 3

Let A\mathbf{A} be a commutative ring, E\mathbf{E} an A\mathbf{A}-algebra, (xi)1≤i≤n(x_i)_{1 \leq i \leq n} a finite sequence of elements of E\mathbf{E} and suppose that, for every ordered pair (i,j)(i, j) of integers such that 1≤j<i≤n1 \leq j < i \leq n,

xixj=λijxjxiwith λij∈A. x_i x_j = \lambda_{ij} x_j x_i \quad \text{with } \lambda_{ij} \in \mathbf{A}.

Then, for every permutation σ∈Sn\sigma \in \mathfrak{S}_n,

xσ(1)xσ(2)⋯xσ(n)=εσ(λ)x1x2⋯xn. x_{\sigma(1)} x_{\sigma(2)} \cdots x_{\sigma(n)} = \varepsilon_\sigma(\lambda) x_1 x_2 \cdots x_n.

The lemma is trivial for n=1n = 1 and n=2n = 2; we proceed by induction on nn for n≥3n \geq 3. If σ(n)=n\sigma(n) = n, relation (19) follows from the induction hypothesis. Suppose therefore that σ(n)=k,k≠n\sigma(n) = k, k \neq n, and let τ\tau be the permutation of {1,n}\{1, n\} defined by

{τ(i)=ifor i<kτ(i)=i+1for k≤i<nτ(n)=k. \begin{cases} \tau(i) = i & \text{for } i < k \\ \tau(i) = i + 1 & \text{for } k \leq i < n \\ \tau(n) = k. \end{cases}

Let π=τ−1∘σ\pi = \tau^{-1} \circ \sigma; the permutation π\pi leaves nn fixed; now σ=τ∘π\sigma = \tau \circ \pi and therefore, writing yi=xτ(i), yπ(i)=xσ(i)y_i = x_{\tau(i)},\ y_{\pi(i)} = x_{\sigma(i)}. If i≠ni \neq n and j≠nj \neq n, the relations π(i)>π(j)\pi(i) > \pi(j) and σ(i)>σ(j)\sigma(i) > \sigma(j) are equivalent (since τ\tau is a strictly increasing mapping of {1,n−1}\{1, n-1\} into {1,n}\{1, n\}). For i≠n,j≠ni \neq n, j \neq n and σ(i)>σ(j)\sigma(i) > \sigma(j),

yπ(i)yπ(j)=xσ(i)xσ(j)=λσ(i), σ(j)xσ(j)xσ(i)=λσ(i), σ(j)yπ(j)yπ(i) y_{\pi(i)} y_{\pi(j)} = x_{\sigma(i)} x_{\sigma(j)} = \lambda_{\sigma(i),\ \sigma(j)} x_{\sigma(j)} x_{\sigma(i)} = \lambda_{\sigma(i),\ \sigma(j)} y_{\pi(j)} y_{\pi(i)}

whence, by the induction hypothesis (using the fact that π(n)=n\pi(n) = n):

yπ(1)yπ(2)⋯yπ(n)=(∏i<j<n, σ(i)>σ(j)λσ(i), σ(j))y1y2⋯yn y_{\pi(1)} y_{\pi(2)} \cdots y_{\pi(n)} = \left( \prod_{i < j < n,\ \sigma(i) > \sigma(j)} \lambda_{\sigma(i),\ \sigma(j)} \right) y_1 y_2 \cdots y_n

that is

xσ(1)xσ(2)⋯xσ(n)=(∏i<j<n, σ(i)>σ(j)λσ(i), σ(j))xτ(1)⋯xτ(n). x_{\sigma(1)} x_{\sigma(2)} \cdots x_{\sigma(n)} = \left( \prod_{i < j < n,\ \sigma(i) > \sigma(j)} \lambda_{\sigma(i),\ \sigma(j)} \right) x_{\tau(1)} \cdots x_{\tau(n)}.

Now

xτ(1)⋯xτ(n)=x1⋯xk−1xk+1⋯xnxk x_{\tau(1)} \cdots x_{\tau(n)} = x_1 \cdots x_{k-1} x_{k+1} \cdots x_n x_k

and this, by Lemma 1, is equal to

(∏j>kλjk)x1⋯xn=(∏σ(i)>σ(n)λσ(i), σ(n))x1⋯xn. \left( \prod_{j > k} \lambda_{jk} \right) x_1 \cdots x_n = \left( \prod_{\sigma(i) > \sigma(n)} \lambda_{\sigma(i),\ \sigma(n)} \right) x_1 \cdots x_n.

Finally, (20) and (21) give

xσ(1)⋯xσ(n)=α⋅x1⋯xn x_{\sigma(1)} \cdots x_{\sigma(n)} = \alpha \cdot x_1 \cdots x_n

with

α=(∏i<j<n,σ(i)>σ(j)λσ(i),σ(j))⋅(∏i<n,σ(i)>σ(n)λσ(i),σ(n)) \alpha = \left( \prod_{i < j < n, \sigma(i) > \sigma(j)} \lambda_{\sigma(i), \sigma(j)} \right) \cdot \left( \prod_{i < n, \sigma(i) > \sigma(n)} \lambda_{\sigma(i), \sigma(n)} \right)
=∏i<j,σ(i)>σ(j)λσ(i),σ(j)=εσ(λ) = \prod_{i < j, \sigma(i) > \sigma(j)} \lambda_{\sigma(i), \sigma(j)} = \varepsilon_\sigma(\lambda)

which completes the proof of Lemma 3.

7. Tensor product of graded algebras relative to commutation factors

Definition 6

Let* (Δi)i∈I(\Delta_i)_{i \in I} be a finite family of commutative monoids written additively. A system of commutation factors over the Δi\Delta_i with values in a commutative ring A\mathbf{A} is a system of mappings εij:Δi×Δj→A\varepsilon_{ij}: \Delta_i \times \Delta_j \to \mathbf{A}, where i∈Ii \in I, j∈Ij \in I, i≠ji \neq j satisfying the following conditions:

(22)

εij(αi+αi′,βj)=εij(αi,βj)εij(αi′,βj) \varepsilon_{ij}(\alpha_i + \alpha'_i, \beta_j) = \varepsilon_{ij}(\alpha_i, \beta_j) \varepsilon_{ij}(\alpha'_i, \beta_j)
(23)
εij(αi,βj+βj′)=εij(αi,βj)εij(αi,βj′) \varepsilon_{ij}(\alpha_i, \beta_j + \beta'_j) = \varepsilon_{ij}(\alpha_i, \beta_j) \varepsilon_{ij}(\alpha_i, \beta'_j)
(24)
εij(αi,βj)εji(βj,αi)=1, \varepsilon_{ij}(\alpha_i, \beta_j) \varepsilon_{ji}(\beta_j, \alpha_i) = 1,

for all αi,αi′\alpha_i, \alpha'_i in Δi\Delta_i, βj,βj′\beta_j, \beta'_j in Δj\Delta_j.

If I is given a total ordering and the Δi\Delta_i are groups, a system of commutation factors is defined over the Δi\Delta_i by taking for every ordered pair (i,j)(i, j) such that i<ji < j an arbitrary Z\mathbf{Z}-*bilinear* mapping of Δi×Δj\Delta_i \times \Delta_j into the (multiplicative) Z\mathbf{Z}-module A∗\mathbf{A}^* of invertible elements of the ring A\mathbf{A} and then writing

εji(βj,αi)=(εij(αi,βj))−1 \varepsilon_{ji}(\beta_j, \alpha_i) = (\varepsilon_{ij}(\alpha_i, \beta_j))^{-1}

for i<ji < j.

Note that, since the εij(αi,βj)\varepsilon_{ij}(\alpha_i, \beta_j) are invertible,

εij(0,βj)=εij(αi,0)=1, \varepsilon_{ij}(0, \beta_j) = \varepsilon_{ij}(\alpha_i, 0) = 1,

by virtue of (22) and (23).

Example

(1) The trivial system of commutation factors consists of the εij\varepsilon_{ij} such that εij(αi,βj)=1\varepsilon_{ij}(\alpha_i, \beta_j) = 1 for all i,ji, j, αi∈Δi\alpha_i \in \Delta_i, βj∈Δj\beta_j \in \Delta_j.

(2) If we take A=Z\mathbf{A} = \mathbf{Z} and Δi=Z\Delta_i = \mathbf{Z} for all i∈Ii \in I, a system of commutation factors is obtained by taking εij(αi,βj)=(−1)αiβj\varepsilon_{ij}(\alpha_i, \beta_j) = (-1)^{\alpha_i \beta_j}. Note that this number depends only on the parities of αi\alpha_i and βj\beta_j and the εij\varepsilon_{ij} can therefore be considered as commutation factors when certain of the Δi\Delta_i are equal to Z/2Z\mathbf{Z}/2\mathbf{Z} and the others to Z\mathbf{Z}.

These two examples are the most frequent cases encountered in applications.

Proposition 10

Let A\mathbf{A} be a commutative ring and (Δi)i∈I(\Delta_i)_{i \in I} a finite family of commutative monoids written additively; for each i∈Ii \in I let EiE_i be a graded A\mathbf{A}-algebra of type Δi\Delta_i. Finally, let (εij)(\varepsilon_{ij}) be a system of commutation factors over the Δi\Delta_i with values in A\mathbf{A}. Then there exist a graded A\mathbf{A}-algebra EE of type Δ=∏i∈IΔi\Delta = \prod_{i \in I} \Delta_i and for each i∈Ii \in I an algebra homomorphism hi:Ei→Eh_i : E_i \to E, with the following properties:

(i) If ϕi:Δi→Δ\phi_i : \Delta_i \to \Delta is the canonical homomorphism, then hih_i is a graded homomorphism (II, § 11, no. 2), in other words, hi(Eiαi)⊂Eϕi(αi)h_i(E_i^{\alpha_i}) \subset E^{\phi_i(\alpha_i)}, where (Eiαi)(E_i^{\alpha_i}) and (Eα)(E^{\alpha}) denote the respective graduations on EiE_i and EE.

(ii) If i≠ji \neq j and xix_i (resp. xjx_j) is a homogeneous element of EiE_i (resp. EjE_j) of degree αi∈Δi\alpha_i \in \Delta_i (resp. βj∈Δj\beta_j \in \Delta_j), then

hi(xi)hj(xj)=εij(αi,βj)hj(xj)hi(xi). h_i(x_i) h_j(x_j) = \varepsilon_{ij}(\alpha_i, \beta_j) h_j(x_j) h_i(x_i).

(iii) For every A\mathbf{A}-algebra FF and every system of homomorphisms fi:Ei→Ff_i : E_i \to F satisfying the conditions

fi(xi)fj(xj)=εij(αi,βj)fj(xj)fi(xi), f_i(x_i) f_j(x_j) = \varepsilon_{ij}(\alpha_i, \beta_j) f_j(x_j) f_i(x_i),

where i,j,xi,xj,αi,βji, j, x_i, x_j, \alpha_i, \beta_j are as in (ii), then there exists one and only one algebra homomorphism f:E→Ff : E \to F such that fi=f∘hif_i = f \circ h_i for all i∈Ii \in I. Moreover the underlying A\mathbf{A}-module of EE is the tensor product ⨂i∈IEi\bigotimes_{i \in I} E_i.

Consider the A-module\mathbf{A}\text{-module} E=⨂i∈IEiE = \bigotimes_{i \in I} E_i; it is identified with the direct sum of the submodules EαE^{\alpha}, where, for each α=(αi)∈Δ\alpha = (\alpha_i) \in \Delta, we write Eα=⨂i∈IEiαiE^{\alpha} = \bigotimes_{i \in I} E_i^{\alpha_i}; the EαE^{\alpha} therefore form a graduation of type Δ\Delta on the A\mathbf{A}-module EE. We shall define on EE a graded A\mathbf{A}-algebra structure of type Δ\Delta. For this let II be given a total ordering; for every ordered pair of elements α=(αi),β=(βi)\alpha = (\alpha_i), \beta = (\beta_i) of Δ\Delta, we must first define an A\mathbf{A}-bilinear mapping of Eα×EβE^{\alpha} \times E^{\beta} into Eα+βE^{\alpha + \beta}, or alternatively an A\mathbf{A}-linear mapping mαβm_{\alpha \beta} of Eα⊗AEβE^{\alpha} \otimes_{\mathbf{A}} E^{\beta} into Eα+βE^{\alpha + \beta}. We shall define mαβm_{\alpha \beta} by the condition

mαβ((⨂i∈Ixi)⊗(⨂i∈Iyi))=ε(α,β)⨂i∈I(xiyi) m_{\alpha \beta} \left( \left( \bigotimes_{i \in I} x_i \right) \otimes \left( \bigotimes_{i \in I} y_i \right) \right) = \varepsilon(\alpha, \beta) \bigotimes_{i \in I} (x_i y_i)

for xi∈Eiαi,yi∈Eiαix_i \in E_i^{\alpha_i}, y_i \in E_i^{\alpha_i}, where

ε(α,β)=∏i>jεij(αi,βj). \varepsilon(\alpha, \beta) = \prod_{i > j} \varepsilon_{ij}(\alpha_i, \beta_j).

The right hand side of (27) obviously belongs to Eα+βE^{\alpha + \beta} and the mapping (x1,…,xn,y1,…,yn)↦ε(α,β)⨂i∈I(xiyi)(x_1, \ldots, x_n, y_1, \ldots, y_n) \mapsto \varepsilon(\alpha, \beta) \bigotimes_{i \in I} (x_i y_i) is A\mathbf{A}-multilinear in the product of the EiαiE_i^{\alpha_i} and the EiβiE_i^{\beta_i} (1≤i≤n1 \leq i \leq n). Then it must be proved that the multiplication thus defined on E is associative; now, if γ=(γi)\gamma = (\gamma_i) is a third element of Δ\Delta and zi∈Eiγi′z_i \in E_i^{\gamma_i'} for 1≤i≤n1 \leq i \leq n, then

((⨂ixi)(⨂iyi))(⨂izi)=ε(α+β,γ)ε(α,β)⨂i(xiyizi) \left( \left( \bigotimes_i x_i \right) \left( \bigotimes_i y_i \right) \right) \left( \bigotimes_i z_i \right) = \varepsilon(\alpha + \beta, \gamma) \varepsilon(\alpha, \beta) \bigotimes_i (x_i y_i z_i)
(⨂ixi)((⨂iyi)(⨂izi))=ε(α,β+γ)ε(β,γ)⨂i(xiyizi) \left( \bigotimes_i x_i \right) \left( \left( \bigotimes_i y_i \right) \left( \bigotimes_i z_i \right) \right) = \varepsilon(\alpha, \beta + \gamma) \varepsilon(\beta, \gamma) \bigotimes_i (x_i y_i z_i)

and it reduces to verifying the identity

ε(α+β,γ)ε(α,β)=ε(α,β+γ)ε(β,γ). \varepsilon(\alpha + \beta, \gamma) \varepsilon(\alpha, \beta) = \varepsilon(\alpha, \beta + \gamma) \varepsilon(\beta, \gamma).

But the latter follows immediately from the relations

ε(α+β,γ)=ε(α,β)ε(β,γ) \varepsilon(\alpha + \beta, \gamma) = \varepsilon(\alpha, \beta) \varepsilon(\beta, \gamma)
ε(α,β+γ)=ε(α,β)ε(α,γ) \varepsilon(\alpha, \beta + \gamma) = \varepsilon(\alpha, \beta) \varepsilon(\alpha, \gamma)

themselves immediate consequences of the definition (28) and (22) and (23).

If, for all i∈Ii \in I, eie_i denotes the unit element of EiE_i, we know that eie_i is homogeneous of degree 0 (§ 3, no. 1), hence e=⨂i∈Ieie = \bigotimes_{i \in I} e_i is homogeneous of degree 0 and it follows from (27), (28) and the relations

εij(αi,0)=εij(0,βj)=1 \varepsilon_{ij}(\alpha_i, 0) = \varepsilon_{ij}(0, \beta_j) = 1

that ee is unit element of EE, which completes the definition on EE of the desired graded A-algebra structure. Then take hi(xi)=xi⊗⨂j≠iejh_i(x_i) = x_i \otimes \bigotimes_{j \neq i} e_j; to verify that hi(xixi′)=hi(xi)hi(xi′)h_i(x_i x_i') = h_i(x_i) h_i(x_i') for xi,xi′x_i, x_i' in EiE_i, attention may be confined to the case where xix_i and xi′x_i' are homogeneous and then this relation follows immediately from (27) and the relations εij(αi,0)=εij(0,βj)=1\varepsilon_{ij}(\alpha_i, 0) = \varepsilon_{ij}(0, \beta_j) = 1; the same relations and (24) prove also that the hih_i satisfy conditions (i) and (ii) of the statement and that

⨂i∈Ixi=∏i∈Ihi(xi) \bigotimes_{i \in I} x_i = \prod_{i \in I} h_i(x_i)

where the right hand side is the product of the ordered sequence (hi(xi))i∈I(h_i(x_i))_{i \in I} in E with the given total ordering on I (I, § 1, no. 2) (it suffices to argue by induction on the number of xix_i (assumed homogeneous) distinct from the eie_i).

It remains to prove condition (iii); note that the mapping

(xi)i∈I↦∏i∈Ifi(xi), (x_i)_{i \in I} \mapsto \prod_{i \in I} f_i(x_i),

where the right hand side is the product of the ordered sequence (fi(xi))i∈I(f_i(x_i))_{i \in I} with the given total ordering on II, is A-multilinear. Then there exists one and only one A-linear mapping f:E→Ff : E \to F such that

f(⨂i∈Ixi)=∏i∈Ifi(xi). f\left( \bigotimes_{i \in I} x_i \right) = \prod_{i \in I} f_i(x_i).

Clearly f(e)f(e) is the unit element of FF and f∘hi=fif \circ h_i = f_i; to verify that ff is an algebra homomorphism, in other words that f(x)f(y)=f(xy)f(x)f(y) = f(xy) for x,yx, y in EE, attention may be confined, by linearity, to the case where x=⨂i∈Ixix = \bigotimes_{i \in I} x_i and y=⨂i∈Iyiy = \bigotimes_{i \in I} y_i, xix_i (resp. yiy_i) being homogeneous of degree αi\alpha_i (resp. βi\beta_i) for all i∈Ii \in I. The relation to be verified then reduces, by (27), to

(∏i∈Ifi(xi))(∏i∈Ifi(yi))=ε(α,β)∏i∈I(fi(xi)fi(yi)). \left( \prod_{i \in I} f_i(x_i) \right) \left( \prod_{i \in I} f_i(y_i) \right) = \varepsilon(\alpha, \beta) \prod_{i \in I} (f_i(x_i) f_i(y_i)).

But, taking account of relations (26), this is a consequence of Lemma 2 of no. 6.

Clearly the algebra EE and the canonical mapping ψ:⨂i∈IEi→E\psi : \bigotimes_{i \in I} E_i \to E constitute a solution of the universal mapping problem (Set Theory, IV, § 3, no. 1), where Σ\Sigma is the species of A-algebra structure and the α\alpha-mappings ∏ifi\prod_i f_i from ∏iEi\prod_i E_i to an A-algebra, satisfying conditions (26).

For a fixed total ordering on II, the graded algebra EE defined in the proof of Proposition 10 will be called a graded tensor ε\varepsilon-product of type Δ\Delta of the family (Ei)i∈I(E_i)_{i \in I} of graded algebras of type Δi\Delta_i and will be denoted by ε⨂i∈IEi^{\varepsilon} \bigotimes_{i \in I} E_i (if no confusion can arise over the ordering on II); similarly, the homomorphism f:E→Ff : E \to F defined in the proof of Proposition 10 will be denoted by ε⨂i∈Ifi^{\varepsilon} \bigotimes_{i \in I} f_i. The homomorphisms hih_i are called canonical. We also write εG⊗n^{\varepsilon} G^{\otimes n} when I={1,n}I = \{1, n\} and all the EiE_i are equal to the same algebra GG.

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 εij(αi,βj)=1\varepsilon_{ij}(\alpha_i, \beta_j) = 1 for all i,j,αii, j, \alpha_i and βj\beta_j.

(2) Suppose that all the Δi\Delta_i are equal to Z\mathbf{Z} and write εij(αi,βj)=(−1)αiβj\varepsilon_{ij}(\alpha_i, \beta_j) = (-1)^{\alpha_i \beta_j}; the tensor ε\varepsilon-product ε⨂i∈IEi^{\varepsilon} \bigotimes_{i \in I} E_i corresponding to this system of commutation factors is then called the skew tensor product of the graded algebras EiE_i of type Z\mathbf{Z} and denoted by ε⨂i∈IEi^{\varepsilon} \bigotimes_{i \in I} E_i (or E ε⊗AFE \ ^{\varepsilon} \otimes_A F for two algebras, or εG⊗n^{\varepsilon} G^{\otimes n} instead of εG⊗n^{\varepsilon} G^{\otimes n}).

Corollary 1

In the notation of Proposition 10, suppose further that F is a graded A-algebra of type Δ\Delta and that each fif_i is a graded algebra homomorphism relative to ϕi:Δi→Δ\phi_i : \Delta_i \to \Delta; then f=ε⨂ifif = \varepsilon \bigotimes_i f_i is a graded algebra homomorphism.

This follows immediately from the definition of ff and the fact that

∑i∈Iϕi(αi)=(αi) \sum_{i \in I} \phi_i(\alpha_i) = (\alpha_i)
by definition of the ϕi\phi_i.

It is therefore seen that (E,ψ)(E, \psi) is also a solution of another universal mapping problem, where this time Σ\Sigma is the species of graded A-algebra structure of type Δ\Delta, the morphisms being graded algebra homomorphisms of type Δ\Delta and the α\alpha-mappings the mappings ∏ifi\prod_i f_i, where, in addition to conditions (26), it is assumed that fif_i is a graded algebra homomorphism relative to ϕi\phi_i.

Corollary 2

Let* (Ei)i∈I,(Fi)i∈I(E_i)_{i \in I}, (F_i)_{i \in I} be two finite families of A*-algebras, with* EiE_i and FiF_i graded of type Δi\Delta_i for all i∈Ii \in I. For each i∈Ii \in I, let gi:Ei→Fig_i : E_i \to F_i be a graded algebra homomorphism of type Δi\Delta_i. Then, if hi:Ei→ε⨂i∈IEih_i : E_i \to \varepsilon \bigotimes_{i \in I} E_i and hi′:Fi→ε⨂i∈IFih'_i : F_i \to \varepsilon \bigotimes_{i \in I} F_i are the canonical homomorphisms, there exists one and only one homomorphism of graded A*-algebras of type* Δ\Delta, g:ε⨂i∈IEi→ε⨂i∈IFig : \varepsilon \bigotimes_{i \in I} E_i \to \varepsilon \bigotimes_{i \in I} F_i such that g∘hi=hi′∘gig \circ h_i = h'_i \circ g_i for all i∈Ii \in I. Also, if each gig_i is bijective, so is gg.

It suffices to apply Corollary 1 to fi=hi′∘gif_i = h'_i \circ g_i, noting that conditions (26) then follow from relations (25) applied to the hi′h'_i.

The homomorphism defined in Corollary 2 is also denoted by ε⨂igi\varepsilon \bigotimes_i g_i (if no confusion can arise); if, for each i∈Ii \in I, GiG_i is a third graded A-algebra of type Δi\Delta_i and gi′:Fi→Gig'_i : F_i \to G_i a graded algebra homomorphism, then

(ε⨂igi′)∘(ε⨂igi)=ε⨂i(gi′∘gi), \left( \varepsilon \bigotimes_i g'_i \right) \circ \left( \varepsilon \bigotimes_i g_i \right) = \varepsilon \bigotimes_i (g'_i \circ g_i),
as follows immediately from (30).

In the case of a skew tensor product of graded algebras of type Z\mathbf{Z}, we write ε⨂ifi\varepsilon \bigotimes_i f_i instead of ε⨂ifi\varepsilon \bigotimes_i f_i for homomorphisms fi:Ei→Fif_i : E_i \to F_i of graded algebras of type Z\mathbf{Z}; when I={1,2}I = \{1, 2\}, this homomorphism is also denoted by f1ε⊗f2f_1 \varepsilon \otimes f_2; when I={1,n}I = \{1, n\} and all the EiE_i (resp. FiF_i) are equal and all the fif_i equal to the same homomorphism ff, we write εf⊗n\varepsilon f^{\otimes n}.

Remark

In the proof of Proposition 10, a total ordering on II was used to define an algebra structure on the tensor product ⨂i∈IEi\bigotimes_{i \in I} E_i of the A-modules

E_i. If the ordering on I is changed, another multiplicative structure arises on ⨂i∈IEi\bigotimes_{i \in I} E_i, 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 I={1,2}I = \{1, 2\}, the canonical isomorphism of the algebra E1⊗εAE2E_1 \overset{\varepsilon}{\otimes}_A E_2 onto the algebra E2⊗εAE1E_2 \overset{\varepsilon}{\otimes}_A E_1 maps x1⊗x2x_1 \otimes x_2 to ε2,1(α,β)x2⊗x1\varepsilon_{2,1}(\alpha, \beta)x_2 \otimes x_1, where x1x_1 is homogeneous of degree α\alpha and x2x_2 homogeneous of degree β\beta.

Let J be a subset of I and, for each i∈Ji \in J, consider the canonical homomorphism hi:Ei→ε⨂i∈IEi=Eh_i : E_i \to \varepsilon \bigotimes_{i \in I} E_i = E. By virtue of relations (25) a canonical homomorphism h:E′=ε⨂i∈JEi→Eh : E' = \varepsilon \bigotimes_{i \in J} E_i \to E is derived canonically (by Proposition 10) from these homomorphisms, such that, for all i∈Ji \in J, hi′=h∘hih'_i = h \circ h_i, hi′h'_i being the canonical homomorphism Ei→E′E_i \to E'. Taking the total ordering on J induced by that chosen on I, we obtain

h(⨂i∈Jxi)=∏i∈Ihi(xi)=⨂i∈Ixi′ h\left( \bigotimes_{i \in J} x_i \right) = \prod_{i \in I} h_i(x_i) = \bigotimes_{i \in I} x'_i

where the middle term is the product of the ordered sequence (hi(xi))i∈J(h_i(x_i))_{i \in J} and where, in the right hand term, xi′=xix'_i = x_i for i∈Ji \in J, xi′=eix'_i = e_i for i∉Ji \notin J.

Proposition 11

("associativity" of the tensor ε\varepsilon-product). In the notation of Proposition 10, let (Jλ)λ∈L(J_\lambda)_{\lambda \in L} be a partition of I and write Δλ′=∏i∈JλΔi\Delta'_\lambda = \prod_{i \in J_\lambda} \Delta_i for all λ∈L\lambda \in L. Let Eλ′E'_\lambda be a graded tensor ε\varepsilon-product of type Δλ′\Delta'_\lambda of the family (Ei)i∈Jλ(E_i)_{i \in J_\lambda} for some total ordering chosen on JλJ_\lambda. On the other hand, for λ,μ\lambda, \mu in LL and λ≠μ\lambda \neq \mu, we write, for αλ′=(αi)i∈Jλ\alpha'_\lambda = (\alpha_i)_{i \in J_\lambda}, βμ′=(βj)j∈Jμ\beta'_\mu = (\beta_j)_{j \in J_\mu},

ελμ′(αλ′,βμ′)=∏i∈Jλ,j∈Jμεij(αi,βj). \varepsilon'_{\lambda \mu}(\alpha'_\lambda, \beta'_\mu) = \prod_{i \in J_\lambda, j \in J_\mu} \varepsilon_{ij}(\alpha_i, \beta_j).

Then (ελμ′)(\varepsilon'_{\lambda \mu}) is a system of commutation factors over the Δλ′\Delta'_\lambda with values in AA and there exists one and only one homomorphism of graded algebras of type Δ\Delta, v:ε′⨂λ∈LEλ′→ε⨂i∈IEiv : \varepsilon' \bigotimes_{\lambda \in L} E'_\lambda \to \varepsilon \bigotimes_{i \in I} E_i, such that

v(⨂λ∈L(⨂i∈Jλxi))=⨂i∈Ixi v\left( \bigotimes_{\lambda \in L} \left( \bigotimes_{i \in J_\lambda} x_i \right) \right) = \bigotimes_{i \in I} x_i

for all (xi)∈∏i∈IEi(x_i) \in \prod_{i \in I} E_i, provided that the total ordering is taken on I which induces on each JλJ_\lambda the chosen total ordering, and which is such that, for λ<μ\lambda < \mu in LL, i∈Jλi \in J_\lambda and j∈Jμj \in J_\mu, i<ji < j.

The fact that the ελμ′\varepsilon'_{\lambda \mu} form a system of commutation factors is trivial. Let hi,λ:Ei→Eλ′h_{i,\lambda} : E_i \to E'_\lambda, hλ′:Eλ′→ε′⨂λ∈LEλ′h'_\lambda : E'_\lambda \to \varepsilon' \bigotimes_{\lambda \in L} E'_\lambda be the canonical homomorphisms (for λ∈L\lambda \in L, i∈Jλi \in J_\lambda) and write hi′′=hλ′∘hi,λh''_i = h'_\lambda \circ h_{i,\lambda}; it will suffice by virtue of the uniqueness of the solution of a universal mapping problem, to show that ε′⨂λ∈LEλ′\varepsilon' \bigotimes_{\lambda \in L} E'_\lambda and the hi′′h''_i satisfy the conditions of Proposition 10. Now, for all λ∈L\lambda \in L, let fλ′:Eλ′→Ff'_\lambda : E'_\lambda \to F be the unique algebra homomorphism such that fλ′∘hi,λ=fif'_\lambda \circ h_{i,\lambda} = f_i for all i∈Jλi \in J_\lambda. We show that, for λ≠μ\lambda \neq \mu, αλ′=(αi)i∈Jλ,βμ′=(βj)j∈Jμ\alpha'_\lambda = (\alpha_i)_{i \in J_\lambda}, \beta'_\mu = (\beta_j)_{j \in J_\mu},

fλ′(xλ′)fμ′(xμ′)=ελμ′(αλ′,βμ′)fμ′(xμ′)fλ′(xλ′) f'_\lambda(x'_\lambda)f'_\mu(x'_\mu) = \varepsilon'_{\lambda\mu}(\alpha'_\lambda, \beta'_\mu)f'_\mu(x'_\mu)f'_\lambda(x'_\lambda)

for xλ′∈Eλ′x'_\lambda \in E'_\lambda (resp. xμ′∈Eμ′x'_\mu \in E'_\mu) homogeneous of degree αλ′\alpha'_\lambda (resp. βμ′\beta'_\mu); it suffices, by linearity, to verify it when xμ′=⨂i∈Jλxi,xμ′=⨂j∈Jμxj,xix'_\mu = \bigotimes_{i \in J_\lambda} x_i, x'_\mu = \bigotimes_{j \in J_\mu} x_j, x_i (resp. xjx_j) being homogeneous of degree αi\alpha_i (resp. βj\beta_j) in EiE_i (resp. EjE_j) for i∈Jλ,j∈Jμi \in J_\lambda, j \in J_\mu. But this follows from formula (30) which defines the fλ′f'_\lambda and Lemma 3 of no. 6, taking account of hypothesis (26) and definition (32). There is therefore one and only one algebra homomorphism f:ε′⨂λ∈LEλ′→Ff : \varepsilon' \bigotimes_{\lambda \in L} E'_\lambda \to F such that f∘hλ′=fλ′f \circ h'_\lambda = f'_\lambda for all λ∈L\lambda \in L; whence f∘hi′′=fif \circ h''_i = f_i for all i∈Ii \in I and the uniqueness of ff 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 Δi\Delta_i are equal to the same commutative monoid Δ0\Delta_0; we can then consider on the tensor ε\varepsilon-product ε⨂i∈IEi\varepsilon \bigotimes_{i \in I} E_i the total graduation of type Δ0\Delta_0, associated with the graduation of type Δ=Δ0I\Delta = \Delta_0^I on this algebra (II, § 11, no. 1); we shall call ε⨂i∈IEi\varepsilon \bigotimes_{i \in I} E_i, with this graduation, a graded tensor ε\varepsilon-product of type Δ0\Delta_0 of the family (Ei)i∈I(E_i)_{i \in I} of graded algebras of type Δ0\Delta_0.

Always preserving the notation of Proposition 10 of no. 7, suppose that FF is also a graded A-algebra of type Δ0\Delta_0 and that the fif_i are homomorphisms of graded algebras of type Δ0\Delta_0. Then f:ε⨂i∈IEi→Ff : \varepsilon \bigotimes_{i \in I} E_i \to F is also a homomorphism of graded algebras of type Δ0\Delta_0: for it follows from formula (30) (no. 7) that if xix_i is homogeneous and of degree αi∈Δ0,⨂i∈Ixi\alpha_i \in \Delta_0, \bigotimes_{i \in I} x_i and ∏i∈Ifi(xi)\prod_{i \in I} f_i(x_i) are both homogeneous of degree ∑i∈Iαi∈Δ0\sum_{i \in I} \alpha_i \in \Delta_0.

It can therefore be said that ε⨂i∈IEi\varepsilon \bigotimes_{i \in I} E_i, with the total graduation of type Δ0\Delta_0, constitutes, together with the canonical mapping ψ\psi, a solution of a third universal mapping problem, where Σ\Sigma is the species of graded A-algebra of type Δ0\Delta_0, the morphisms are homomorphisms of graded algebras of type Δ0\Delta_0 and the α\alpha-mappings are the mappings ∏ifi\prod_i f_i, where, in addition to conditions (26) (of no. 7), it is assumed that each fif_i is a homomorphism of graded algebras of type Δ0\Delta_0.

For every subset J of I, the canonical homomorphism ε⨂i∈JEi→ε⨂i∈IEi\varepsilon \bigotimes_{i \in J} E_i \to \varepsilon \bigotimes_{i \in I} E_i (no. 7) is, in fact, a homomorphism of graded algebras of type Δ0\Delta_0, as follows immediately from the above.

Proposition 12

("associativity" of the tensor ε\varepsilon-product of graded algebras of the same types). *With the notation of Proposition 10 of no. 7, suppose that all the Δi\Delta_i are equal to the same monoid Δ0\Delta_0; let (Jλ)λ∈L(J_\lambda)_{\lambda \in L} 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 αλ′′=∑i∈Jλαi,βμ′′=∑j∈Jμβj\alpha''_\lambda = \sum_{i \in J_\lambda} \alpha_i, \beta''_\mu = \sum_{j \in J_\mu} \beta_j, for every ordered pair (λ,μ)(\lambda, \mu) of distinct indices, all αλ′∈Δλ′\alpha'_\lambda \in \Delta'_\lambda and all βμ′∈Δμ′\beta'_\mu \in \Delta'_\mu; let ελμ′′(αλ′′,βμ′′)\varepsilon''_{\lambda \mu}(\alpha''_\lambda, \beta''_\mu) denote the right hand side of (32). *Then (ελμ′′)(\varepsilon''_{\lambda \mu}) is a system of commutation factors over the family (Δλ′′)λ∈L(\Delta''_\lambda)_{\lambda \in L}, where Δλ′′=Δ0\Delta''_\lambda = \Delta_0 for all λ∈L\lambda \in L. *If Eλ′′E''_\lambda is the graded tensor ε\varepsilon-product of type Δ0\Delta_0 of the family (Ei)i∈Jλ(E_i)_{i \in J_\lambda}, there exists one and only one isomorphism of graded algebras of type Δ0\Delta_0, w:ε′′⨂λ∈LEλ′′→ε⨂i∈IEiw : \varepsilon'' \bigotimes_{\lambda \in L} E''_\lambda \to \varepsilon \bigotimes_{i \in I} E_i, such that

w(⨂λ∈L(⨂i∈Jλxi))=⨂i∈Ixi w \left( \bigotimes_{\lambda \in L} \left( \bigotimes_{i \in J_\lambda} x_i \right) \right) = \bigotimes_{i \in I} x_i

provided that total orderings are chosen on the JλJ_\lambda and on I as described in no. 7, Proposition 11.

By the hypothesis, for γ,δ\gamma, \delta in Δ0\Delta_0, ελμ′′(γ,δ)=εi0j0(γ,δ)\varepsilon''_{\lambda \mu}(\gamma, \delta) = \varepsilon_{i_0 j_0}(\gamma, \delta) for some i0∈Jλi_0 \in J_\lambda and some j0∈Jμj_0 \in J_\mu, as is seen by considering the elements αλ′=(αi)i∈Jλ\alpha'_\lambda = (\alpha_i)_{i \in J_\lambda} and βμ′=(βj)j∈Jμ\beta'_\mu = (\beta_j)_{j \in J_\mu} such that αi0=γ,αi=0\alpha_{i_0} = \gamma, \alpha_i = 0 for i≠i0i \neq i_0, βj0=δ,βj=0\beta_{j_0} = \delta, \beta_j = 0 for j≠j0j \neq j_0; it follows immediately that the ελμ′′\varepsilon''_{\lambda \mu} 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 Δ0=Z\Delta_0 = \mathbf{Z} and that (εij)(\varepsilon_{ij}) is, either the trivial system of factors (εij(αi,βj))=1(\varepsilon_{ij}(\alpha_i, \beta_j)) = 1 for all i,ji, j, or the system of factors defined by εij(αi,βj)=(−1)αiβj\varepsilon_{ij}(\alpha_i, \beta_j) = (-1)^{\alpha_i \beta_j}; in the latter case, the right hand side of formula (32) is equal to (−1)γ(-1)^\gamma, where

γ=∑i∈Jλ,j∈Jμαiβj=(∑i∈Jλαi)(∑j∈Jμβj). \gamma = \sum_{i \in J_\lambda, j \in J_\mu} \alpha_i \beta_j = \left( \sum_{i \in J_\lambda} \alpha_i \right) \left( \sum_{j \in J_\mu} \beta_j \right).

Remark

(1) Let I be an infinite indexing set and Δ0\Delta_0 a commutative monoid; let (Δi)i∈I(\Delta_i)_{i \in I} denote the family such that Δi=Δ0\Delta_i = \Delta_0 for all ii and suppose given for every ordered pair of distinct indices (i,j)(i, j) of I a mapping εij:Δi×Δj→A\varepsilon_{ij} : \Delta_i \times \Delta_j \to A satisfying conditions (22), (23) and (24) (no. 7); this will also be called a system of commutation factors over the family (Δi)(\Delta_i). Consider a family (Ei)i∈I(E_i)_{i \in I} of graded A-algebras of type Δ0\Delta_0; for each finite subset J of I, let EJE_J denote a graded tensor ε\varepsilon-product of type Δ0\Delta_0 of the subfamily (Ei)i∈J(E_i)_{i \in J} (with an arbitrary choice of a total ordering on J). If J, J' are two finite subsets of I such that J⊂J′J \subset J', a canonical homomorphism of graded algebras of type Δ0\Delta_0, 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 Δ0\Delta_0 (§ 3, no. 3), whose indexing set is the right directed set F(I)\mathfrak{F}(I) of finite subsets of I. The graded algebra of type Δ0\Delta_0, the direct limit of this direct system (§ 3, no. 3), is called a graded tensor ε\varepsilon-product of type Δ0\Delta_0 of the family (Ei)i∈I(E_i)_{i \in I}; it is also denoted by ε⨂i∈IEi\varepsilon \bigotimes_{i \in I} E_i. When all the Δi\Delta_i are equal to Z\mathbf{Z} and εij(ai,βj)=(−1)αiβj\varepsilon_{ij}(a_i, \beta_j) = (-1)^{\alpha_i \beta_j}, the tensor product ε⨂i∈IEi\varepsilon \bigotimes_{i \in I} E_i is also called the skew tensor product of the family (Ei)i∈I(E_i)_{i \in I} and is denoted by g⨂i∈IEig \bigotimes_{i \in I} E_i. 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 ε⨂i∈IEi\varepsilon \bigotimes_{i \in I} E_i is the same as that underlying the (non-graded) tensor product of the family (Ei)i∈I(E_i)_{i \in I} of non-graded algebras defined in no. 5.

(2) Let E be a graded A-algebra of type Δ0\Delta_0 (where Δ0\Delta_0 is a commutative monoid) and ρ:A→B\rho : A \to B a ring homomorphism; the graduation on ρ∗(E)\rho^*(E) (II, § 11, no. 5) is identical with the graduation on the graded tensor product B⊗AEB \otimes_A E, where B has the trivial graduation.

9. Anticommutative algebras and alternating algebras

Definition 7

A graded A-algebra E of type Z\mathbf{Z} is called anticommutative if for all non-zero homogeneous elements x, y of E

xy=(−1)deg⁡(x)deg⁡(y)yx. xy = (-1)^{\deg(x)\deg(y)} yx.

The algebra E is called alternating if it is anticommutative and also x2=0x^2 = 0 for every homogeneous element x∈Ex \in E of odd degree.

Remark

(1) Let E+E^+ be the graded subalgebra of E the direct sum of the E2nE_{2n} (n∈Zn \in \mathbf{Z}); it follows from Definition 7 that if E is anticommutative, E+E^+ 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 x∈Ex \in E homogeneous and of odd degree, x2=−x2x^2 = -x^2 by (36), whence 2x2=02x^2 = 0 and x2=0x^2 = 0 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 Z\mathbf{Z} and S a set of homogeneous elements ≠0\neq 0; the set F of elements of E all of whose homogeneous components x≠0x \neq 0 satisfy relation (36) for all y∈Sy \in S is a graded subalgebra of E.

It suffices to note that: (1) if x′,x′′x', x'' are two homogeneous elements of the same degree pp, yy a homogeneous element of degree qq and x′y=(−1)pqyx′x'y = (-1)^{pq}yx', x′′y=(−1)pqyx′′x''y = (-1)^{pq}yx'', then also (x′+x′′)y=(−1)pqy(x′+x′′)(x' + x'')y = (-1)^{pq}y(x' + x''); (2) if x′,x′′x', x'' are two homogeneous elements of respective degrees p′,p′′p', p'', yy a homogeneous element of degree qq and x′y=(−1)p′qyx′x'y = (-1)^{p'q}yx', x′′y=(−1)p′′qyx′′x''y = (-1)^{p''q}yx'', then

(x′x′′)y=(−1)(p′+p′′)qy(x′x′′). (x'x'')y = (-1)^{(p'+p'')q}y(x'x'').

Proposition 13

Let E be a graded A-algebra of type Z\mathbf{Z} and S a generating system of the algebra E consisting of homogeneous elements ≠0\neq 0; for E to be anticommutative (resp. alternating), it is necessary and sufficient that (36) hold for all x∈Sx \in S and y∈Sy \in S (resp. that this condition hold and further that x2=0x^2 = 0 for all xx 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 x≠0x \neq 0 satisfy (36) for all y∈Sy \in S, contains all the elements of S and hence F=EF = E. If now F′F' is similarly the subalgebra of E consisting of the elements all of whose homogeneous components x≠0x \neq 0 satisfy (36) for every homogeneous element y≠0y \neq 0, it follows from the above that F′F' contains all the elements of S and hence F′=EF' = E, 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 ∑izixi\sum_i z_ix_i, where zi∈E+z_i \in E^+ and xi∈Sx_i \in S is of odd degree (using the fact that E+E^+ is contained in the centre of E); it follows that (∑izixi)2=∑izi2xi2+∑i<jzizj(xixj+xjxi)=0\left( \sum_i z_ix_i \right)^2 = \sum_i z_i^2x_i^2 + \sum_{i<j} z_i z_j (x_ix_j + x_jx_i) = 0 since xi2=0x_i^2 = 0 by hypothesis and xixj+xjxi=0x_ix_j + x_jx_i = 0 by (36).

Proposition 14

Let E and F be two graded A-algebras of type Z\mathbf{Z}, both anticommutative (resp. alternating). Then the skew tensor product Eg⊗AFE^g \otimes_A F (no. 7) is an anticommutative (resp. alternating) algebra.

A generating system of Eg⊗AFE^g \otimes_A F consists of the x⊗yx \otimes y, where xx (resp. yy) is a homogeneous element ≠0\neq 0 of E (resp. F). Consider two such elements x⊗y,x′⊗y′x \otimes y, x' \otimes y', with deg⁡(x)=p,deg⁡(y)=q,deg⁡(x′)=p′,deg⁡(y′)=q′\deg(x) = p, \deg(y) = q, \deg(x') = p', \deg(y') = q', so that x⊗yx \otimes y is of degree p+qp + q and x′⊗y′x' \otimes y' of degree p′+q′p' + q'. Then by definition (no. 7, formula (27)) and by virtue of (36),

(x⊗y)(x′⊗y′)=(−1)qp′(xx′)⊗(yy′)(x′⊗y′)(x⊗y)=(−1)pq′(x′x)⊗(y′y)=(−1)pq′+pp′+qq′(xx′)⊗(yy′) \begin{align*} (x \otimes y)(x' \otimes y') &= (-1)^{qp'}(xx') \otimes (yy') \\ (x' \otimes y')(x \otimes y) &= (-1)^{pq'}(x'x) \otimes (y'y) \\ &= (-1)^{pq'+pp'+qq'}(xx') \otimes (yy') \end{align*}
and the criterion of Proposition 13 shows that Eg⊗AFE^g \otimes_A F is anticommutative since pq′+pp′+qq′−qp′≡(p+q)(p′+q′)pq' + pp' + qq' - qp' \equiv (p + q)(p' + q') (mod. 2). If further E and F are alternating and p+qp + q is odd, one of the numbers p,qp, q is necessarily odd, hence (x⊗y)2=±(x2)⊗(y2)=0(x \otimes y)^2 = \pm (x^2) \otimes (y^2) = 0 and Proposition 13 shows that Eg⊗AFE^g \otimes_A F is alternating.

Corollary

Let E be an anticommutative* (resp. alternating) *graded A-algebra of type Z\mathbf{Z}. Then for every ring homomorphism ρ:A→B\rho : A \to B, the graded B-algebra ρ∗(E)\rho^*(E) (no. 8, Remark 2) is anticommutative (resp. alternating).

The ring B with the trivial graduation can be considered as an alternating A-algebra and ρ∗(E)=Eg⊗AB\rho^*(E) = E^g \otimes_A B, hence Proposition 14 can be applied.

Remark

Let E be an anticommutative graded A-algebra of type Z\mathbf{Z}. Then the A-linear mapping of E⊗AEE \otimes_A E into E defined by multiplication of E (§1§ 1, no. 3) is a homomorphism of the graded A-algebra Eg⊗AEE^g \otimes_A E into E, for in the notation of Proposition 14, in the algebra E,

(xy)(x′y′)=(−1)qp′(xx′)(yy′). (xy)(x'y') = (-1)^{qp'}(xx')(yy').

Exercises

See the exercises for § 4.

Transcribed from the printed edition, 1998, Springer. Not translated.