Bourbaki

§ 11. Cogebras, products of multilinear forms, inner products and duality

In this paragraph, A is a commutative ring with the trivial graduation. For a graded A-module M of type N, M^{gr} will denote the graded A-module of type N, whose homogeneous elements of degrees n are the A-linear forms which are zero on M_k for all k ≠ n.

1. Cogebras

Definition 1

A cogebr a over A (or A-cogebra, or simply cogebr a if no confusion can arise) is a set E with a structure defined by giving the following: (1) an A-module structure on E; (2) an A-linear mapping c: E → E ⊗_A E called the coproduct of E.

Definition 2

Given two cogebras E, E', whose coproducts are denoted respectively by c and c', a morphism of E into E' is an A-linear mapping u: E → E' such that (1) (u⊗u)∘c=c′∘u,(u \otimes u) \circ c = c' \circ u, in other words, it renders commutative the diagram of A-linear mappings

E→uE′↓c↓c′E⊗AE→u⊗uE′⊗AE′ \begin{array}{ccc} E & \xrightarrow{u} & E' \\ \downarrow c & & \downarrow c' \\ E \otimes_A E & \xrightarrow{u \otimes u} & E' \otimes_A E' \end{array}

It is immediately verified that the identity mapping is a morphism, that the composition of two morphisms is a morphism and that every bijective morphism is an isomorphism.

Example

(1) The canonical isomorphism A→A⊗AAA \to A \otimes_A A (II, § 3, no. 5) defines an A-cogebra structure on A.

(2) Let E be a cogebra, cc its coproduct and σ\sigma the canonical automorphism of the A-module E⊗AEE \otimes_A E such that σ(x⊗y)=y⊗x\sigma(x \otimes y) = y \otimes x for x∈E,y∈Ex \in E, y \in E; the A-linear mapping σ∘c\sigma \circ c defines a new cogebra structure on E. With this structure E is called the opposite cogebra to the given cogebra E.

(3) Let B be an A-*algebra* and let m:B⊗AB→Bm : B \otimes_A B \to B be the A-linear mapping defining multiplication on B (§ 1, no. 3). The transpose tm^t m is then an A-linear mapping of the dual B∗B^* of the A-module B into the dual (B⊗AB)∗(B \otimes_A B)^* of the A-module B⊗ABB \otimes_A B. If also B is a finitely generated projective A-module, the canonical mapping μ:B∗⊗AB∗→(B⊗AB)∗\mu : B^* \otimes_A B^* \to (B \otimes_A B)^* is an A-module isomorphism (II, § 4, no. 4); the mapping c=μ−1∘tmc = \mu^{-1} \circ ^t m is then a coproduct defining a cogebra structure on the dual B∗B^* of the A-module B.

(4) Let X be a set, A(X)A^{(X)} the A-module of formal linear combinations of elements of X with coefficients in A (II, § 1, no. 11) and (ex)x∈X(e_x)_{x \in X} the canonical basis of A(X)A^{(X)}. An A-linear mapping c:A(X)→A(X)⊗AA(X)c : A^{(X)} \to A^{(X)} \otimes_A A^{(X)} is defined by the condition c(ex)=ex⊗exc(e_x) = e_x \otimes e_x and a canonical cogebra structure is thus obtained on A(X)A^{(X)}.

(5) Let M be an A-module and T(M)T(M) the tensor algebra of M (§ 5, no. 1); by II, § 3, no. 9 there exists one and only one A-linear mapping cc of the A-module T(M)T(M) into the A-module T(M)⊗AT(M)T(M) \otimes_A T(M) such that, for all n≥0n \geq 0,

c(x1x2…xn)=∑0≤p≤n(x1x2…xp)⊗(xp+1…xn) c(x_1 x_2 \ldots x_n) = \sum_{0 \leq p \leq n} (x_1 x_2 \ldots x_p) \otimes (x_{p+1} \ldots x_n)

for all xi∈Mx_i \in M (x1x2…xnx_1 x_2 \ldots x_n denotes the product in the algebra T(M)T(M)). Thus T(M)T(M) is given a cogebra structure.

(6) Let M be an A-module and S(M)S(M) the symmetric algebra of M (§ 6, no. 1); the diagonal mapping Δ:x↦(x,x)\Delta : x \mapsto (x, x) of M into M×MM \times M is an A-linear mapping to which there therefore corresponds a homomorphism S(Δ)S(\Delta) of the A-algebra S(M)S(M) into the A-algebra S(M×M)S(M \times M) (§ 6, no. 2, Proposition 3). On the other hand, in § 6, no. 6 we defined a canonical graded algebra isomorphism h:S(M×M)→S(M)⊗AS(M)h : S(M \times M) \to S(M) \otimes_A S(M); by composition we therefore obtain an A-algebra homomorphism

c=h∘S(Δ):S(M)→S(M)⊗AS(M), c = h \circ S(\Delta) : S(M) \to S(M) \otimes_A S(M),

thus defining on S(M)S(M) a cogebra structure. For all x∈Mx \in M, by definition S(Δ)(x)=(x,x)S(\Delta)(x) = (x, x) and the definition of hh given in § 6, no. 6 shows that

h((x,x))=x⊗1+1⊗x. h((x, x)) = x \otimes 1 + 1 \otimes x.

It follows that cc is the unique algebra homomorphism such that, for all x∈Mx \in M,

(4)

c(x)=x⊗1+1⊗x. c(x) = x \otimes 1 + 1 \otimes x.

As cc is an algebra homomorphism, it follows that, for every sequence (xi)1≤i≤n(x_i)_{1 \leq i \leq n} of nn elements of MM,

(5)

c(x1x2…xn)=∏i=1n(xi⊗1+1⊗xi) c(x_1 x_2 \ldots x_n) = \prod_{i=1}^n (x_i \otimes 1 + 1 \otimes x_i)
=∑(xi1…xip)⊗(xj1…xjn−p) = \sum (x_{i_1} \ldots x_{i_p}) \otimes (x_{j_1} \ldots x_{j_{n-p}})

the summation on the right hand side of (5) being taken over all ordered pairs of strictly increasing sequences (in some cases empty)

i1<i2<⋯<ip,j1<j2<⋯<jn−p i_1 < i_2 < \cdots < i_p, \quad j_1 < j_2 < \cdots < j_{n-p}

of elements of {1,n}\{1, n\}, whose sets of elements are complementary. The element c(x1x2…xn)c(x_1 x_2 \ldots x_n) is an element of total degree nn in S(M)⊗AS(M)S(M) \otimes_A S(M) and its component of bidegree (p,n−p)(p, n-p) is

(6)

∑σ(xσ(1)…xσ(p))⊗(xσ(p+1)…xσ(n)) \sum_{\sigma} (x_{\sigma(1)} \ldots x_{\sigma(p)}) \otimes (x_{\sigma(p+1)} \ldots x_{\sigma(n)})

where the summation is taken over all permutations σ∈Sn\sigma \in S_n which are increasing in each of the intervals {1,p}\{1, p\} and {p+1,n}\{p+1, n\}.

(7) Let MM be an AA-module and proceed with the exterior algebra Λ(M)\Lambda(M) as with S(M)S(M) in Example 6; the diagonal mapping Δ:M→M×M\Delta : M \to M \times M this time defines a homomorphism Λ(Δ)\Lambda(\Delta) of the AA-algebra Λ(M)\Lambda(M) into the AA-algebra Λ(M×M)\Lambda(M \times M) (§ 7, no. 2, Proposition 2); on the other hand there is a canonical graded algebra isomorphism

h:Λ(M×M)→Λ(M)g⊗AΛ(M) h : \Lambda(M \times M) \to \Lambda(M)^g \otimes_A \Lambda(M)

(§ 7, no. 7, Proposition 10), whence by composition there is an algebra homomorphism c=h∘Λ(Δ):Λ(M)→Λ(M)g⊗AΛ(M)c = h \circ \Lambda(\Delta) : \Lambda(M) \to \Lambda(M)^g \otimes_A \Lambda(M), which can be considered as an AA-module homomorphism Λ(M)→Λ(M)⊗AΛ(M)\Lambda(M) \to \Lambda(M) \otimes_A \Lambda(M) and which therefore defines on Λ(M)\Lambda(M) a cogebra structure. It can be proved as in Example 6 that cc is the unique algebra homomorphism such that, for all x∈Mx \in M,

(7)

c(x)=x⊗1+1⊗x, c(x) = x \otimes 1 + 1 \otimes x,

whence, for every sequence (xi)1≤i≤n(x_i)_{1 \leq i \leq n} of elements of MM,

c(x1∧x2∧⋯∧xn)=(x1⊗1+1⊗x1)∧…∧(xn⊗1+1⊗xn) c(x_1 \wedge x_2 \wedge \cdots \wedge x_n) = (x_1 \otimes 1 + 1 \otimes x_1) \wedge \ldots \wedge (x_n \otimes 1 + 1 \otimes x_n)
where the product on the right hand side is taken in the algebra
⋀(M)g⊗A⋀(M); \bigwedge(M)^{\mathfrak{g}} \otimes_A \bigwedge(M);
to calculate this product, consider, for every ordered pair of strictly increasing sequences i1<i2<⋯<ip, j1<j2<⋯<jn−pi_1 < i_2 < \cdots < i_p,\ j_1 < j_2 < \cdots < j_{n-p} of elements of [1,n][1, n], whose sets of elements are complementary, the product y1y2…yny_1 y_2 \ldots y_n, where yih=xih⊗1y_{i_h} = x_{i_h} \otimes 1 (1≤h≤p1 \leq h \leq p) and yjk=1⊗xjky_{j_k} = 1 \otimes x_{j_k} (1≤k≤n−p1 \leq k \leq n - p) and the sum is taken over all these products. As the graded algebra ⋀(M)g⊗A⋀(M)\bigwedge(M)^{\mathfrak{g}} \otimes_A \bigwedge(M) is anticommutative and the elements xi⊗1x_i \otimes 1 and 1⊗xi1 \otimes x_i are of total degree 1, by § 4, no. 6, Lemma 3 and Lemma 1,
(8)c(x1∧x2∧⋯∧xn)(8)\quad c(x_1 \wedge x_2 \wedge \cdots \wedge x_n)
=∑(−1)v(xi1∧⋯∧xip)⊗(xj1∧⋯∧xjn−p) = \sum (-1)^v (x_{i_1} \wedge \cdots \wedge x_{i_p}) \otimes (x_{j_1} \wedge \cdots \wedge x_{j_{n-p}})
vv being the number of ordered pairs (h,k)(h, k) such that jk<ihj_k < i_h and the summation being taken over the same set as in (5). The element c(x1∧⋯∧xn)c(x_1 \wedge \cdots \wedge x_n) is of total degree nn in ⋀(M)g⊗A⋀(M)\bigwedge(M)^{\mathfrak{g}} \otimes_A \bigwedge(M) and its homogeneous component of bi-degree (p,n−p)(p, n - p) is equal to
(9)∑σεσ(xσ(1)∧⋯∧xσ(p))⊗(xσ(p+1)∧⋯∧xσ(n))(9)\quad \sum_{\sigma} \varepsilon_\sigma (x_{\sigma(1)} \wedge \cdots \wedge x_{\sigma(p)}) \otimes (x_{\sigma(p+1)} \wedge \cdots \wedge x_{\sigma(n)})
the summation being taken over permutations σ∈Sn\sigma \in S_n which are increasing in each of the intervals [1,p][1, p] and [p+1,n][p + 1, n].

When in future we speak of A(x),T(M),S(M)A^{(x)}, T(M), S(M) or ⋀(M)\bigwedge(M) as cogebras, we shall mean, unless otherwise mentioned, with the cogebra structures defined in Examples 4, 5, 6 and 7 respectively.

(8) Let E,FE, F be two AA-cogebras and c,c′c, c' their respective coproducts. Let τ:(E⊗AE)⊗A(F⊗AF)→(E⊗AF)⊗A(E⊗AF)\tau : (E \otimes_A E) \otimes_A (F \otimes_A F) \to (E \otimes_A F) \otimes_A (E \otimes_A F) denote the associativity isomorphism such that τ((x⊗x′)⊗(y⊗y′))=(x⊗y)⊗(x′⊗y′)\tau((x \otimes x') \otimes (y \otimes y')) = (x \otimes y) \otimes (x' \otimes y') for x,x′x, x' in EE and y,y′y, y' in FF. Then the composite linear mapping

E⊗AF→c⊗c′(E⊗AE)⊗A(F⊗AF)→τ(E⊗AF)⊗A(E⊗AF) E \otimes_A F \xrightarrow{c \otimes c'} (E \otimes_A E) \otimes_A (F \otimes_A F) \xrightarrow{\tau} (E \otimes_A F) \otimes_A (E \otimes_A F)
defines a cogebra structure on the AA-module E⊗AFE \otimes_A F, called the tensor product of the cogebras EE and FF.

Let EE be a cogebra and Δ\Delta a commutative monoid. A graduation (Eλ)λ∈Δ(E_\lambda)_{\lambda \in \Delta} on the AA-module EE is said to be compatible with the coproduct cc of EE if cc is a graded homomorphism of degree OO of the graded AA-module EE into the graded AA-module (of type Δ\Delta) E⊗AEE \otimes_A E, in other words (II, § 11, no. 5) if

(10)c(Eλ)⊂∑μ+ν=λEμ⊗AEν.(10)\quad c(E_\lambda) \subset \sum_{\mu + \nu = \lambda} E_\mu \otimes_A E_\nu.

In what follows, we shall most often limit our attention to graduations of type N\mathbf{N} compatible with the coproduct; a cogebrà with such a graduation will also be called a graded cogebrà. If F is another graded cogebrà, a graded cogebrà morphism ϕ:E→F\phi : E \to F is by definition a cogebrà morphism (Definition 2) which is also a graded homomorphism of degree 0 of graded A-modules.

Example

(9) It is immediate that the cogebras T(M)T(M), S(M)S(M) and Λ(M)\Lambda(M) defined above are graded cogebras.

2. Coassociativity, cocommutativity, counit

Let E be a cogebrà, cc its coproduct, N, N′N', N′′N'' three A-modules and mm a bilinear mapping of N×N′N \times N' into N′′N''. Let m~:N⊗AN′→N′′\tilde{m} : N \otimes_A N' \to N'' denote the A-linear mapping corresponding to mm. If u:E→Nu : E \to N, v:E→N′v : E \to N' are two A-linear mappings, we derive an A-linear mapping u⊗v:E⊗AE→N⊗AN′u \otimes v : E \otimes_A E \to N \otimes_A N' and a composite A-linear mapping of E into N′′N'':

m(u,v):E→cE⊗AE→u⊗vN⊗AN′→m~N′′. m(u, v) : E \xrightarrow{c} E \otimes_A E \xrightarrow{u \otimes v} N \otimes_A N' \xrightarrow{\tilde{m}} N''.

Clearly we have thus defined an A-bilinear mapping (u,v)↦m(u,v)(u, v) \mapsto m(u, v) of HomA(E,N)×HomA(E,N′)\mathrm{Hom}_A(E, N) \times \mathrm{Hom}_A(E, N') into HomA(E,N′′)\mathrm{Hom}_A(E, N'').

When E is a graded cogebrà, N, N′N', N′′N'' graded A-modules of the same type and m~\tilde{m} a graded homomorphism of degree k of N⊗AN′N \otimes_A N' into N′′N'', then, if uu (resp. vv) is a graded homomorphism of degree pp (resp. qq), m(u,v)m(u, v) is a graded homomorphism of degree p+q+kp + q + k.

Example

(1) Take E to be the graded cogebrà T(M)T(M) (no. 1) and suppose that N, N′N', N′′N'' have the trivial graduation. A graded homomorphism of degree −p-p of T(M)T(M) into N (resp. N′N', N′′N'') then corresponds to a multilinear mapping of MpM^p into N (resp. N′N', N′′N''). Given a multilinear mapping u:Mp→Nu : M^p \to N and a multilinear mapping v:Mq→N′v : M^q \to N', the above method allows us to deduce a multilinear mapping m(u,v):Mp+q→N′′m(u, v) : M^{p+q} \to N'' called the product (relative to mm) of uu and vv. Formulae (3) (no. 1) and (11) show that, for x1,…,xp+qx_1, \ldots, x_{p+q} in M,

(m(u,v))(x1,…,xp+q)=m(u(x1,…,xp),v(xp+1,…,xp+q)). (m(u, v))(x_1, \ldots, x_{p+q}) = m(u(x_1, \ldots, x_p), v(x_{p+1}, \ldots, x_{p+q})).

(2) Take E to be the graded cogebrà S(M)S(M) (no. 1), preserving the same hypotheses on N, N′N', N′′N''. A graded homomorphism of degree −p-p of S(M)S(M) into N then corresponds to a symmetric multilinear mapping of MpM^p into N (§ 6, no. 3). Then we derive from a symmetric multilinear mapping u:Mp→Nu : M^p \to N and a symmetric multilinear mapping v:Mq→N′v : M^q \to N' a symmetric multilinear mapping m(u,v):Mp+q→N′′m(u, v) : M^{p+q} \to N'', also denoted (to avoid confusion) by u.mvu._m v (or even u.vu.v) and called the symmetric product (relative to mm) of uu and vv. Formulae (6) (no. 1) and (11) show that, for x1,…,xp+qx_1, \ldots, x_{p+q} in M,

(u⋅mv)(x1,…,xp+q)=∑σm(u(xσ(1),…,xσ(p)),v(xσ(p+1),…,xσ(p+q)))(u \cdot_m v)(x_1, \ldots, x_{p+q}) = \sum_\sigma m(u(x_{\sigma(1)}, \ldots, x_{\sigma(p)}), v(x_{\sigma(p+1)}, \ldots, x_{\sigma(p+q)}))

the summation being taken over permutations σ∈Sp+q\sigma \in \mathfrak{S}_{p+q} which are increasing on each of the intervals [1,p][1, p] and [p+1,p+q][p+1, p+q].

(3) Take E to be the graded cogebra ⋀(M)\bigwedge(M) (no. 1). Then we deduce similarly from an alternating multilinear mapping u:Mp→Nu : M^p \to N and an alternating multilinear mapping v:Mq→N′v : M^q \to N' an alternating multilinear mapping m(u,v):Mp+q→N′′m(u, v) : M^{p+q} \to N'', also denoted by u∧mvu \wedge_m v or u∧vu \wedge v and called the alternating product (relative to mm) of uu and vv. Formulae (9) (no. 1) and (11) show in this case that, for x1,…,xp+qx_1, \ldots, x_{p+q} in MM,

(u∧mv)(x1,…,xp+q)=∑σεσm(u(xσ(1),…,xσ(p)),v(xσ(p+1),…,xσ(p+q)))(u \wedge_m v)(x_1, \ldots, x_{p+q}) = \sum_\sigma \varepsilon_\sigma m(u(x_{\sigma(1)}, \ldots, x_{\sigma(p)}), v(x_{\sigma(p+1)}, \ldots, x_{\sigma(p+q)}))

the summation again being taken over permutations σ∈Sp+q\sigma \in \mathfrak{S}_{p+q} which are increasing on each of the intervals [1,p][1, p] and [p+1,p+q][p+1, p+q].

We return to the case where E is an arbitrary graded cogebra (of type N) and assume that the three modules N, N', N'' are all equal to the underlying A-module of a graded A-algebra B of type Z\mathbf{Z}, the mapping mm being multiplication in B, so that m~:B⊗AB→B\tilde{m} : B \otimes_A B \to B is a graded A-linear mapping of degree 0. Thus a graded A-algebra structure is obtained on the graded A-module HomgrA(E,B)=C\mathrm{Homgr}_A(E, B) = C.

In particular, suppose that B=AB = A (with the trivial graduation), so that HomgrA(E,A)\mathrm{Homgr}_A(E, A) is the graded dual E∗grE^{*gr}, which thus has a graded A-algebra structure.

Let F be another graded cogebra c′c' its coproduct and ϕ:E→F\phi : E \to F a graded cogebra morphism (no. 1); then the canonical graded morphism

ϕ~=Hom(ϕ,1B):HomgrA(F,B)→HomgrA(E,B)\tilde{\phi} = \mathrm{Hom}(\phi, 1_B) : \mathrm{Homgr}_A(F, B) \to \mathrm{Homgr}_A(E, B)

is a graded algebra homomorphism. For u,vu, v in HomgrA(F,B)\mathrm{Homgr}_A(F, B) and x∈Ex \in E,

(ϕ~(uv))(x)=(uv)(ϕ(x))=m((u⊗v)(c′(ϕ(x)))).(\tilde{\phi}(uv))(x) = (uv)(\phi(x)) = m((u \otimes v)(c'(\phi(x)))).

But by hypothesis c′(ϕ(x))=(ϕ⊗ϕ)(c(x))c'(\phi(x)) = (\phi \otimes \phi)(c(x)), hence

(u⊗v)(c′((x)))=(ϕ~(u)⊗ϕ~(v))(c(x))(u \otimes v)(c'((x))) = (\tilde{\phi}(u) \otimes \tilde{\phi}(v))(c(x))

and therefore ϕ~(uv)=ϕ~(u)ϕ~(v)\tilde{\phi}(uv) = \tilde{\phi}(u)\tilde{\phi}(v), which proves our assertion.

In particular, the graded transpose tϕ:F∗gr→E∗gr^t\phi : F^{*gr} \to E^{*gr} is a graded algebra homomorphism.

Remark

Suppose that the EpE_p are finitely generated projective AA-modules, so that the graded AA-modules (E⊗AE)∗gr(E \otimes_A E)^{*gr} and E∗gr⊗AE∗grE^{*gr} \otimes_A E^{*gr} can be canonically identified (II, § 4, no. 4, Corollary 1 to Proposition 4). If also the AA-modules A⊗AAA \otimes_A A and AA are then canonically identified (II, § 3, no. 4), the linear mapping E∗gr⊗AE∗gr→E∗grE^{*gr} \otimes_A E^{*gr} \to E^{*gr} which defines multiplication in E∗grE^{*gr} can be called the graded transpose of the coproduct cc.

Proposition 1

Let EE be a cogebra over AA. In order that, for every associative AA-algebra BB, the AA-algebra HomA(E,B)\mathrm{Hom}_A(E, B) be associative, it is necessary and sufficient that the coproduct c:E→E⊗AEc : E \to E \otimes_A E be such that the diagram

E→cE⊗AE↓c↓lE⊗cE⊗AE→c⊗lEE⊗AE⊗AE \begin{array}{ccc} E & \xrightarrow{c} & E \otimes_A E \\ \downarrow c & & \downarrow l_E \otimes c \\ E \otimes_A E & \xrightarrow{c \otimes l_E} & E \otimes_A E \otimes_A E \end{array}

be commutative.

Let BB be an associative AA-algebra and u,v,wu, v, w three elements of C=HomA(E,B)C = \mathrm{Hom}_A(E, B). Let m3m_3 denote the AA-linear mapping B⊗AB⊗AB→BB \otimes_A B \otimes_A B \to B which maps b⊗b′⊗b′′b \otimes b' \otimes b'' to bb′b′′bb'b''. By definition of the product on the algebra CC, (uv)w(uv)w is the composite mapping

E→cE⊗E→c⊗1EE⊗E⊗E→u⊗v⊗wB⊗B⊗B→m3B E \xrightarrow{c} E \otimes E \xrightarrow{c \otimes 1_E} E \otimes E \otimes E \xrightarrow{u \otimes v \otimes w} B \otimes B \otimes B \xrightarrow{m_3} B

whilst u(vw)u(vw) is the composite mapping

E→cE⊗E→lE⊗cE⊗E⊗E→u⊗v⊗wB⊗B⊗B→m3B. E \xrightarrow{c} E \otimes E \xrightarrow{l_E \otimes c} E \otimes E \otimes E \xrightarrow{u \otimes v \otimes w} B \otimes B \otimes B \xrightarrow{m_3} B.

It follows that if diagram (12) is commutative, the algebra HomA(E,B)\mathrm{Hom}_A(E, B) is associative for every associative AA-algebra BB. To establish the converse, it suffices to show that there exists an associative AA-algebra BB and three AA-linear mappings u,v,wu, v, w of EE into BB such that the mapping m3∘(u⊗v⊗w)m_3 \circ (u \otimes v \otimes w) of E⊗E⊗EE \otimes E \otimes E into BB is injective. Take BB to be the AA-algebra T(E)\mathscr{T}(E) and u,v,wu, v, w the canonical mapping of EE into T(E)\mathscr{T}(E). The mapping m3∘(u⊗v⊗w)m_3 \circ (u \otimes v \otimes w) is then the canonical mapping E⊗E⊗E=T3(E)→T(E)E \otimes E \otimes E = \mathscr{T}^3(E) \to \mathscr{T}(E), which is injective.

When the cogebra EE satisfies the condition of Proposition 1, it is said to be coassociative.

Example

(4) It is immediately verified that the cogebra AA (no. 1, Example (1)) the cogebra A(X)A^{(X)} (no. 1, Example 4) and the cogebra T(M)\mathscr{T}(M) (no. 1, Example 5) are coassociative. If BB is an associative AA-algebra which is a finitely generated projective AA-module, the cogebra B∗B^* (no. 1, Example 3) is coassociative: for the commutativity of diagram (12) then follows by transposition from that of the diagram which expresses the associativity of BB (§ 1, no. 3). Conversely, the same argument and the canonical identification of the A-module B with its bidual (II, § 2, no. 7, Corollary 4 to Proposition 13) show that if the cogebras B* is coassociative, the algebra B is associative. Finally, the cogebras S(M) and Λ(M)\Lambda(M) (no. 1, Examples 6 and 7) are coassociative; this follows from the commutativity of the diagram

M→ΔM×M↓↓1M×ΔM×M→Δ×1MM×M×M \begin{array}{ccc} M & \xrightarrow{\Delta} & M \times M \\ \downarrow & & \downarrow 1_M \times \Delta \\ M \times M & \xrightarrow{\Delta \times 1_M} & M \times M \times M \end{array}

the functorial properties of S(M) (§ 6, no. 2) and Λ(M)\Lambda(M) (§ 7, no. 2), which give the corresponding commutative diagrams

{S(M)→S(Δ)S(M×M)↓S(Δ)↓S(ΔM×1)S(M×M)→S(Δ×1M)S(M×M×M) \left\{ \begin{array}{ccc} S(M) & \xrightarrow{S(\Delta)} & S(M \times M) \\ \downarrow S(\Delta) & & \downarrow S(\Delta_M \times 1) \\ S(M \times M) & \xrightarrow{S(\Delta \times 1_M)} & S(M \times M \times M) \end{array} \right.
{Λ(M)→Λ(Δ)Λ(M×M)↓Λ(Δ)↓Λ(1M×Δ)Λ(M×M)→Λ(Δ×1M)Λ(M×M×M) \left\{ \begin{array}{ccc} \Lambda(M) & \xrightarrow{\Lambda(\Delta)} & \Lambda(M \times M) \\ \downarrow \Lambda(\Delta) & & \downarrow \Lambda(1_M \times \Delta) \\ \Lambda(M \times M) & \xrightarrow{\Lambda(\Delta \times 1_M)} & \Lambda(M \times M \times M) \end{array} \right.

and the existence and functoriality of canonical isomorphisms for symmetric and exterior algebras of a direct sum (§ 6, no. 6 and § 7, no. 7).

Proposition 2

Let E be a cogebras over A. In order that, for every commutative A-algebra B, the A-algebra HomA(E,B)\mathrm{Hom}_A(E, B) be commutative, it is necessary and sufficient that the coproduct c:E→E⊗AEc : E \to E \otimes_A E be such that the diagram

E↙c↘cE⊗AE→σE⊗AE \begin{array}{ccc} E & & \\ & \swarrow_c & \searrow_c \\ E \otimes_A E & \xrightarrow{\sigma} & E \otimes_A E \end{array}

(where σ\sigma is the symmetry homomorphism such that σ(x⊗y)=y⊗x\sigma(x \otimes y) = y \otimes x) is commutative (in other words, it suffices that the cogebras E be identical with its opposite (no. 1, Example 2).

Let B be a commutative A-algebra and u,vu, v two elements of C=HomA(E,B)C = \mathrm{Hom}_A(E, B).

By definition of the product in C, uvuv and vuvu are respectively equal to the composite mappings

E→cE⊗E→u⊗vB⊗B→mB E \xrightarrow{c} E \otimes E \xrightarrow{u \otimes v} B \otimes B \xrightarrow{m} B

and

E→cE⊗E→v⊗uB⊗B→mB. E \xrightarrow{c} E \otimes E \xrightarrow{v \otimes u} B \otimes B \xrightarrow{m} B.

It follows that if diagram (15) is commutative the algebra HomA(E,B)\mathrm{Hom}_A(E, B) is commutative for every commutative A-algebra B. To establish the converse, it suffices to show that there exist a commutative A-algebra B and two A-linear mappings u,vu, v of E into B such that m∘(u⊗v):E⊗E→Bm \circ (u \otimes v): E \otimes E \to B is injective. Take B to be the algebra S(E⊕E)S(E \oplus E) and uu (resp. vv) the composition of the canonical mapping E⊕E→S(E⊕E)E \oplus E \to S(E \oplus E) and the mapping x↦(x,0)x \mapsto (x, 0) (resp. x↦(0,x)x \mapsto (0, x)) of E into E⊕EE \oplus E. If h:S(E)⊗S(E)→S(E⊗E)h: S(E) \otimes S(E) \to S(E \otimes E) is the canonical isomorphism (§ 6, no. 6, Proposition 9) and λ:E→S(E)\lambda: E \to S(E) is the canonical mapping, then h−1∘m∘(u⊗v)=λ⊗λh^{-1} \circ m \circ (u \otimes v) = \lambda \otimes \lambda. Now λ⊗λ\lambda \otimes \lambda is injective, for λ(E)\lambda(E) is a direct factor of S(E)S(E) (II, § 3, no. 7, Corollary 5 to Proposition 7).

When the cogebra E satisfies the condition of Proposition 2, it is said to be cocommutative.

Example

(5) It is immediate that the cogebra A (no. 1, Example 1) and the cogebra A(X)A^{(X)} (II, § 11, no. 1, Example 4) are cocommutative. It follows from formula (5) of no. 1 that the cogebra S(M)S(M) is cocommutative. Finally, for an A-algebra B such that the A-module B is projective and finitely generated to have the property that the cogebra B∗B^* (no. 1, Example 3) is cocommutative, it is necessary and sufficient that B be commutative; for (using the canonical identification of the A-module B with its bidual (II, § 2, no. 7)), this follows from the fact that the commutativity of diagram (14) is equivalent by transposition to that of the diagram which expressed the commutativity of B (§ 1, no. 3).

Proposition 3

Let E be a cogebra over A. In order that, for every unital A-algebra B, the A-algebra HomA(E,B)\mathrm{Hom}_A(E, B) be unital, it is necessary and sufficient that there exist a linear form γ\gamma on E rendering commutative the diagrams

E→cE⊗AE↓γ⊗1EA⊗AE \begin{array}{ccc} E & \xrightarrow{c} & E \otimes_A E \\ & & \downarrow \gamma \otimes 1_E \\ & & A \otimes_A E \end{array}
h′h'
E→cE⊗AE↓1E⊗γE⊗AA \begin{array}{ccc} E & \xrightarrow{c} & E \otimes_A E \\ & & \downarrow 1_E \otimes \gamma \\ & & E \otimes_A A \end{array}
h′′h''

where c:E→E⊗AEc: E \to E \otimes_A E is the coproduct and h′h' and h′′h'' the canonical isomorphisms

(II, § 3, no. 4, Proposition 4). The unit of HomA_A(E, B) is then the linear mapping x ↦\mapsto γ(x)1\gamma(x)1 (where 1 denotes the unit element of B).

Let γ\gamma be a linear form on E rendering diagram (16) commutative. Let B be a unital A-algebra with unit element 1, η:A→B\eta:A \to B the canonical mapping and v=η∘γv = \eta \circ \gamma the element of the A-algebra C = HomA_A(E, B). For every element u∈Cu \in C, uvuv is the composite mapping

(17)E→cE⊗E→1E⊗γE⊗A→u⊗ηB⊗B→mB. \text{(17)} \quad E \xrightarrow{c} E \otimes E \xrightarrow{1_E \otimes \gamma} E \otimes A \xrightarrow{u \otimes \eta} B \otimes B \xrightarrow{m} B.

Then uv=m∘(u⊗η)∘h′′=uuv = m \circ (u \otimes \eta) \circ h'' = u. It is similarly proved that vu=uvu = u and hence vv is unit element of C. Conversely, let the A-module A ⊕\oplus E be given a unital algebra structure such that (a,x)(a′,x′)=(aa′,ax′+a′x)(a, x)(a', x') = (aa', ax' + a'x) for a,a′a, a' in A and x,x′x, x' in E. Let B denote the A-algebra thus defined and let C be the A-algebra HomA_A(E, B). Suppose that C is unital and let e:x↦(γ(x),λ(x))e:x \mapsto (\gamma(x), \lambda(x)) be its unit element (where γ(x)∈A\gamma(x) \in A and λ(x)∈E\lambda(x) \in E). On the other hand let ff be the element x↦(0,x)x \mapsto (0, x) of C. An immediate calculation shows that fefe is the element

x↦(0,(h′′)−1((1E⊗γ)(c(x)))) x \mapsto (0, (h'')^{-1}((1_E \otimes \gamma)(c(x))))

of C. The condition fe=ffe = f implies the commutativity of the second diagram of (16) and it is similarly seen that the condition ef=fef = f implies the commutativity of the first diagram of (16).

A linear form γ\gamma on E rendering diagrams (16) commutative is called a counit of the cogebra E. A cogebra admits at most one counit: for it is the unit element of the algebra HomA_A(E, A). A cogebra with a counit is called counital.

Example

(6) The identity mapping is the counit of the cogebra A; on the cogebra A(X)^{(X)} (no. 1, Example 4) the linear form γ\gamma such that γ(ex)=1\gamma(e_x) = 1 for all x∈Xx \in X is the counit. On the cogebra T(M) (resp. S(M), Λ(M)\Lambda(M)) the linear form γ\gamma such that γ(1)=1\gamma(1) = 1 and γ(z)=0\gamma(z) = 0 for zz in the Tn(M)T^n(M) (resp. Sn(M)S^n(M), Λn(M)\Lambda^n(M)) for n≥1n \geq 1 is the counit. Finally, let B be an A-algebra which is a finitely generated projective A-module and has a unit element ee; then on the cogebra B* (no. 1, Example 3) the linear form γ:x∗↦⟨e,x∗⟩\gamma: x^* \mapsto \langle e, x^* \rangle is the counit, for this form is just the transpose of the A-linear mapping ηe:ξ↦ξe\eta_e: \xi \mapsto \xi e of A into B and by transposition the commutativity of diagrams (16) follows from that of the diagrams which express (using ηe\eta_e) the fact that ee is unit element of B (§ 1, no. 3); the same argument moreover shows that conversely, if the cogebra B* admits a counit γ\gamma, the transpose of γ\gamma defines a unit element e=tγ(1)e = t_\gamma(1) of B.

Proposition 4

Let E be a cogebra admitting a counit γ\gamma and suppose that there exists in E an element e such that γ(e)=1\gamma(e) = 1; then E is the direct sum of the sub-A-modules Ae and Eγ=Ker(γ)E_{\gamma} = \mathrm{Ker}(\gamma) and

(18){c(e)≡e⊗e(modEγ⊗Eγ)c(x)≡x⊗e+e⊗x(modEγ⊗Eγ)for all x∈Eγ. \text{(18)} \quad \begin{cases} c(e) \equiv e \otimes e \pmod{E_{\gamma} \otimes E_{\gamma}} \\ c(x) \equiv x \otimes e + e \otimes x \pmod{E_{\gamma} \otimes E_{\gamma}} & \text{for all } x \in E_{\gamma}. \end{cases}

The first assertion is immediate, for γ(x−γ(x)e)=0\gamma(x - \gamma(x)e) = 0 and the relation γ(αe)=0\gamma(\alpha e) = 0 implies α=0\alpha = 0. Let c(e)=∑isi⊗tic(e) = \sum_i s_i \otimes t_i, so that

e=∑iγ(si)ti=∑iγ(ti)si e = \sum_i \gamma(s_i)t_i = \sum_i \gamma(t_i)s_i
by (16) and 1=γ(e)=∑iγ(si)γ(ti)1 = \gamma(e) = \sum_i \gamma(s_i)\gamma(t_i). Therefore
∑i(si−γ(si)e)⊗(ti−γ(ti)e)=∑isi⊗ti−∑ie⊗γ(si)ti−∑iγ(ti)si⊗e+∑iγ(si)e⊗γ(ti)e \sum_i (s_i - \gamma(s_i)e) \otimes (t_i - \gamma(t_i)e) = \sum_i s_i \otimes t_i - \sum_i e \otimes \gamma(s_i)t_i \\ - \sum_i \gamma(t_i)s_i \otimes e \\ + \sum_i \gamma(s_i)e \otimes \gamma(t_i)e
which, by the above relation, is just c(e)−e⊗ec(e) - e \otimes e; this therefore proves the first relation of (18). On the other hand the decomposition of E⊗EE \otimes E as a direct sum
A(e⊗e)⊕((Ae)⊗Eγ)⊕(Eγ⊗(Ae))⊕(Eγ⊗Eγ) A(e \otimes e) \oplus ((Ae) \otimes E_\gamma) \oplus (E_\gamma \otimes (Ae)) \oplus (E_\gamma \otimes E_\gamma)
allows us to write, for x∈Eγx \in E_\gamma, c(x)=λ(e⊗e)+(e⊗y)+z⊗e)+uc(x) = \lambda(e \otimes e) + (e \otimes y) + z \otimes e) + u where u=∑jvj⊗wj,y,zu = \sum_j v_j \otimes w_j, y, z and the vjv_j and wjw_j belong to EγE_\gamma. The definition of the counit γ\gamma then gives x=λe+y=λe+zx = \lambda e + y = \lambda e + z and, as γ(x)=0\gamma(x) = 0, necessarily λ=0,x=y=z\lambda = 0, x = y = z, whence the second relation of (18).

Remark

Let C be a counital coassociative A-coalgebra, B a unital associative A-algebra and M a left B-module. The A-bilinear mapping (b,m)↦bm(b, m) \mapsto bm of B×MB \times M into M defines an A-bilinear mapping

Hom⁡A(C,B)×Hom⁡A(C,M)→Hom⁡A(C,M) \operatorname{Hom}_A(C, B) \times \operatorname{Hom}_A(C, M) \to \operatorname{Hom}_A(C, M)
by the general procedure described at the beginning of this no. It is immediately verified that this mapping defines on Hom⁡A(C,M)\operatorname{Hom}_A(C, M) a left module structure over the ring Hom⁡A(C,B)\operatorname{Hom}_A(C, B).

3. Properties of graded cogebras of type n

Proposition 5

(i) *Let E be a graded cogebra admitting a counit γ\gamma; then γ\gamma is a homogeneous linear form of degree 0.

(ii) Suppose further that there exists an element e∈Ee \in E such that E0=AeE_0 = Ae and γ(e)=1\gamma(e) = 1. Then the kernel EγE_\gamma of γ\gamma is equal to E+=∑n≥1EnE_+ = \sum_{n \geq 1} E_n, c(e)=e⊗ec(e) = e \otimes e and

c(x)≡x⊗e+e⊗x (mod. E+⊗E+) c(x) \equiv x \otimes e + e \otimes x \ (\text{mod. } E_+ \otimes E_+)
for all x∈E+x \in E_+.

(i) It suffices to verify that γ(x)=0\gamma(x) = 0 for x∈Enx \in E_n, for all n≥1n \geq 1. Since cc is a graded homomorphism of degree 0,

c(x)=∑0≤j≤n(∑iyij⊗zi,n−j) c(x) = \sum_{0 \leq j \leq n} \left( \sum_i y_{ij} \otimes z_{i, n-j} \right)

with, for all jj such that 0≤j≤n0 \leq j \leq n, yijy_{ij} and zijz_{ij} in EjE_j; applying (16) (no. 2) we obtain

x=∑0≤j≤n(∑iγ(yij)zi,n−j)=∑0≤j≤n(∑iγ(zi,n−j)yij), x = \sum_{0 \leq j \leq n} \left( \sum_i \gamma(y_{ij}) z_{i, n-j} \right) = \sum_{0 \leq j \leq n} \left( \sum_i \gamma(z_{i, n-j}) y_{ij} \right),

whence, equating the components of degree 0 and degree nn on the two sides

x=∑iγ(yi0)zin=∑iγ(zi0)yin x = \sum_i \gamma(y_{i0}) z_{in} = \sum_i \gamma(z_{i0}) y_{in}
0=∑iγ(yin)zi0=∑iγ(zin)yi0 0 = \sum_i \gamma(y_{in}) z_{i0} = \sum_i \gamma(z_{in}) y_{i0}

and therefore γ(x)=∑iγ(yin)γ(zi0)=γ(0)=0\gamma(x) = \sum_i \gamma(y_{in}) \gamma(z_{i0}) = \gamma(0) = 0.

(ii) Since Ker(γ)\mathrm{Ker}(\gamma) and E+E_+ are both supplementary sub-A-modules of Ae=E0Ae = E_0 and E+⊂Ker(γ)E_+ \subset \mathrm{Ker}(\gamma) by (i), E+=Ker(γ)E_+ = \mathrm{Ker}(\gamma) (II, § 1, no. 8, Remark 1); the other assertions follow from Proposition 4 of no. 2.

Proposition 6

Let E be a graded cogebra over A. In order that, for every commutative A-algebra B, with the trivial graduation, the graded A-algebra of type ZHomgrA(E,B)\mathbf{Z} \mathrm{Homgr}_A(E, B) (no. 2) be anticommutative (§ 4, no. 9, Definition 7), it is necessary and sufficient that, if σg\sigma_g denotes the automorphism of the A-module E⊗AEE \otimes_A E such that

σg(xp⊗xq)=(−1)pqxq⊗xp \sigma_g(x_p \otimes x_q) = (-1)^{pq} x_q \otimes x_p

for xp∈Ep,xq∈Eqx_p \in E_p, x_q \in E_q, where p and q are arbitrary elements of N\mathbf{N}, the diagram

E↘c↙cE⊗AE→σgE⊗AE \begin{array}{ccc} E & & \\ & \searrow^c & \swarrow^c \\ E \otimes_A E & \xrightarrow{\sigma_g} & E \otimes_A E \end{array}

be commutative.

The proof is analogous to that of Proposition 2 of no. 2.

When the graded cogebra E satisfies the condition of Proposition 6, it is said to be anticocommutative.

Example

It follows immediately from formula (8) of no. 1 that for every A-module M, the graded cogebra ⋀(M)\bigwedge(M) is anticocommutative.

4. Bigebras and skew-bigebras

Definition 3

A graded bigebra (resp. skew graded bigebra) over a ring A is a set E with a graded A-algebra structure of type N\mathbf{N} and a graded A-cogebra structure of type N\mathbf{N}, with the same underlying graded A-module structure and such that:

(1) The A-algebra E is associative and unital.

(2) The A-cogebra E is coassociative and counital. (3) The coproduct c : E \to E \otimesA E is a homomorphism of the graded algebra E into the graded algebra E \otimes_A E* (resp. graded algebra E^g \otimesA E* (cf. § 4, no. 7)). (4) The counit γ\gamma of E is a homomorphism of the graded algebra E into the algebra A (with the trivial graduation) such that, if e denotes the unit element of the A-algebra E, γ(e)=1\gamma(e) = 1.

If E is a graded bigebra whose graduation is trivial, E is called simply a bigebra. A graded bigebra is called commutative (resp. cocommutative) if the underlying algebra is commutative (resp. if the underlying cogebra is cocommutative); a skew graded bigebra is called anticommutative (resp. anticocommutative) if the underlying graded algebra is anticommutative (resp. if the underlying graded cogebra is anticocommutative).

It follows from Definition 3 and no. 2, Proposition 5 that, for a graded bigebra or a skew graded bigebra E,

c(e)=e⊗ec(x)≡x⊗e+e⊗x(mod. E+⊗E+)for x∈E+=⨁n≥1En. c(e) = e \otimes e \\ c(x) \equiv x \otimes e + e \otimes x (\text{mod. } E_+ \otimes E_+) \quad \text{for } x \in E_+ = \bigoplus_{n \geq 1} E_n.

If E and F are two graded bigebras (resp. two skew graded bigebras), a mapping ϕ:E→F\phi : E \to F is called a graded bigebra morphism (resp. skew graded bigebra morphism) if: (1) ϕ\phi is a graded algebra morphism (and hence maps the unit element of E to the unit element of F); (2) ϕ\phi is a graded cogebra morphism such that, if γ\gamma and γ′\gamma' are the respective counits of E and F, then γ=γ′∘ϕ\gamma = \gamma' \circ \phi.

Example

(1) Let S be a monoid with identity element u, so that the algebra E=A(S)E = A^{(S)} of the monoid S over A admits the unit element eue_u (§ 2, no. 6); it has been seen on the other hand that E has canonically a coassociative cocommutative A-cogebra structure with a counit γ\gamma such that γ(es)=1\gamma(e_s) = 1 for all s∈Ss \in S (no. 1, Example 4 and no. 2, Examples 4, 5 and 6). The formula c(es)=es⊗esc(e_s) = e_s \otimes e_s giving the coproduct shows also immediately that c is an algebra homomorphism. Thus a cocommutative bigebra structure has been defined on E and E, with this structure, is called the bigebra of the monoid S over A.

If T is another monoid with unit element v, f:S→Tf : S \to T a homomorphism such that f(u)=vf(u) = v and f(A):A(S)→A(T)f_{(A)} : A^{(S)} \to A^{(T)} the A-algebra homomorphism derived from ff (§ 2, no. 6), it is immediately verified that f(A)f_{(A)} is a bigebra homomorphism.

(2) Let M be an A-module. The graded A-algebra (§ 6, no. 1) and graded A-cogebra (no. 1, Example 6) structures defined on S(M) define on this set a commutative cocommutative graded bigebra structure; for we have seen (no. 1, Example 6) that the coproduct on S(M) is an algebra homomorphism and it follows from the definition of the counit γ\gamma (no. 2, Example 6) that γ(1)=1\gamma(1) = 1 and that γ\gamma is an algebra homomorphism of E into A.

(3) Let M be an A-module. We see as in Example 2 that the graded A-algebra (§ 7, no. 1) and graded A-cogebra (no. 1, Example 7) structures on ⋀(M)\bigwedge(M) define on this set an anticommutative anticocommutative skew graded bigebra structure.

Remark

If M is an A-module such that M⊗AM≠{0}M \otimes_A M \neq \{0\}, the graded A-algebra (§ 5, no. 1) and graded A-cogebra (no. 1, Example 5) structures on T(M)T(M) do not define a bigebra structure, for in general

c(x1x2y1y2)≠c(x1x2)c(y1y2) c(x_1 x_2 y_1 y_2) \neq c(x_1 x_2) c(y_1 y_2)

for four elements x1,x2,y1,y2x_1, x_2, y_1, y_2 of M, as formula (3) of no. 1, shows.

5. The graded duals T(M)∗grT(M)^{*gr}, S(M)∗grS(M)^{*gr} and ⋀(M)∗gr\bigwedge(M)^{*gr}

From now on we return to the general conventions of the chapter on algebras, which will therefore be assumed (unless otherwise mentioned) to be associative and unital.

Let M be an A-module; the graded A-cogebra structures defined on T(M)T(M) (no. 1, Example 5), S(M)S(M) (no. 1, Example 6) and ⋀(M)\bigwedge(M) (no. 1, Example 7) allow us to define canonically on the graded duals T(M)∗grT(M)^{*gr}, S(M)∗grS(M)^{*gr} and ⋀(M)∗gr\bigwedge(M)^{*gr} graded algebra structures of type N, by virtue of no. 2, Propositions 1 and 3 and the convention made on the graduation of the graded dual of a graded module (no. 1). Moreover, the graded algebra S(M)∗grS(M)^{*gr} is commutative (no. 2, Proposition 2 and Example 5) and the graded algebra ⋀(M)∗gr\bigwedge(M)^{*gr} is anticommutative (no. 3, Proposition 6 and Example). In ⋀(M)∗gr\bigwedge(M)^{*gr} every element of degree 1 is of zero square; such an element is identified with a linear form ff on M and its square is the alternating bilinear form f∧ff \wedge f on M2M^2 such that

(f∧f)(x,y)=f(x)f(y)−f(y)f(x) (f \wedge f)(x, y) = f(x) f(y) - f(y) f(x)

(no. 2, Example 3).

Let N be another A-module and uu an A-linear mapping of M into N. We know that uu defines canonically graded algebra homomorphisms

{T(u):T(M)→T(N)S(u):S(M)→S(N)⋀(u):⋀(M)→⋀(N) \begin{cases} T(u): T(M) \to T(N) \\ S(u): S(M) \to S(N) \\ \bigwedge(u): \bigwedge(M) \to \bigwedge(N) \end{cases}

(§ 5, no. 2, § 6, no. 2 and § 7, no. 2). It is immediately verified in formula (3) of no. 1 that T(u)T(u) is also a cogebra morphism. On the other hand, if ΔM\Delta_M (resp. ΔN\Delta_N) denotes the diagonal mapping M→M×MM \to M \times M (resp. N→N×NN \to N \times N), there is the relation (u×u)∘ΔM=ΔN∘u(u \times u) \circ \Delta_M = \Delta_N \circ u; it follows that S(u×u)∘S(ΔM)=S(ΔN)∘S(u)S(u \times u) \circ S(\Delta_M) = S(\Delta_N) \circ S(u)

(resp. Λ(u×u)∘Λ(ΔM)=Λ(ΔN)∘Λ(u)\Lambda(u \times u) \circ \Lambda(\Delta_M) = \Lambda(\Delta_N) \circ \Lambda(u)).

Using the definition of coproduct in S(M)S(M) and Λ(M)\Lambda(M) (no. 1, Examples 6 and 7) and the functorial character of the canonical isomorphisms

S(M×M)→S(M)⊗AS(M) S(M \times M) \to S(M) \otimes_A S(M)

and Λ(M×M)→Λ(M)g⊗AΛ(M)\Lambda(M \times M) \to \Lambda(M)^{\text{g}} \otimes_A \Lambda(M), it is seen that S(u)S(u) and Λ(u)\Lambda(u) are also cogebra morphisms† (and hence in this case bigebra morphisms). It follows immediately that the graded transposes (II, § 11, no. 6) of the homomorphisms (23)

tT(u):T(N)∗gr→T(M)∗grtS(u):S(N)∗gr→S(M)∗grtΛ(u):Λ(N)∗gr→Λ(M)∗gr \begin{align*} tT(u): T(N)^{*gr} &\to T(M)^{*gr} \\ tS(u): S(N)^{*gr} &\to S(M)^{*gr} \\ t\Lambda(u): \Lambda(N)^{*gr} &\to \Lambda(M)^{*gr} \end{align*}

are graded algebra homomorphisms.

We now note that the dual M∗M^* of MM is identified with the submodule of elements of degree 1 in T(M)∗grT(M)^{*gr} (resp. S(M)∗grS(M)^{*gr}, Λ(M)∗gr\Lambda(M)^{*gr}). It therefore follows from the universal property of the tensor algebra (§ 5, no. 1) and the universal property of the symmetric algebra (§ 6, no. 1) that there exists one and only one graded algebra homomorphism

θT:T(M∗)→T(M)∗gr \theta_T: T(M^*) \to T(M)^{*gr}

which extends the canonical injection M∗→T(M)∗grM^* \to T(M)^{*gr}, and one and only one graded algebra homomorphism

θS:S(M∗)→S(M)∗gr \theta_S: S(M^*) \to S(M)^{*gr}

which extends the canonical injection M∗→S(M)∗grM^* \to S(M)^{*gr}. On the other hand, the canonical injection of M∗M^* in the opposite algebra to Λ(M)∗gr\Lambda(M)^{*gr} is such that the square of every element of M∗M^* is zero; hence (§ 7, no. 1, Proposition 1) there exists one and only one graded algebra homomorphism

θΛ:Λ(M∗)→(Λ(M)∗gr)0 \theta_\Lambda: \Lambda(M^*) \to (\Lambda(M)^{*gr})^0

which extends the canonical injection M∗→Λ(M)∗grM^* \to \Lambda(M)^{*gr}.‡ These homomorphisms

† This also follows from formulae (5) and (9) of no. 1. ‡ This injection is extended to a homomorphism into the opposite algebra to Λ(M)∗gr\Lambda(M)^{*gr} instead of a homomorphism into Λ(M)∗gr\Lambda(M)^{*gr} for reasons of convenience in the calculations.

are functorial: for example, for every AA-module homomorphism u:M→Nu : M \to N, the diagram

T(N∗)→T(tu)T(M∗)θT↓θT↓T(N)∗gr→tT(n)T(M)∗gr \begin{array}{ccc} T(N^*) & \xrightarrow{T(tu)} & T(M^*) \\ \theta_T \downarrow & & \theta_T \downarrow \\ T(N)^{*gr} & \xrightarrow{t_{T(n)}} & T(M)^{*gr} \end{array}

is commutative, as follows immediately from the universal property of the tensor algebra (§ 5, no. 1); there are analogous commutative diagrams for θS\theta_S and θ∧\theta_\wedge.

We shall find the homomorphisms θT,θS\theta_T, \theta_S and θ∧\theta_\wedge explicitly. For this we consider more generally a coassociative AA-cogebra EE with coproduct cc and define by induction on nn, for n≥2n \geq 2, the linear mapping cnc_n of EE into E⊗nE^{\otimes n} by c2=cc_2 = c and

cn=(cn−1⊗1E)∘c. c_n = (c_{n-1} \otimes 1_E) \circ c.
On the other hand we denote by mn:A⊗n→Am_n : A^{\otimes n} \to A the canonical linear mapping such that mn(ξ1⊗ξ2⊗⋯⊗ξn)=ξ1ξ2⋯ξnm_n(\xi_1 \otimes \xi_2 \otimes \cdots \otimes \xi_n) = \xi_1 \xi_2 \cdots \xi_n and note that, for n≥2n \geq 2,
mn=m∘(mn−1⊗1A) m_n = m \circ (m_{n-1} \otimes 1_A)
writing m=m2m = m_2. With this notation:

Lemma 1

(i) In the associative algebra E∗=HomA(E,A)E^* = \mathrm{Hom}_A(E, A), the product of nn elements u1,u2,…,unu_1, u_2, \ldots, u_n of degree 1 is given by

u1u2…un=mn∘(u1⊗u2⊗⋯⊗un)∘cn. u_1 u_2 \ldots u_n = m_n \circ (u_1 \otimes u_2 \otimes \cdots \otimes u_n) \circ c_n.
(ii) Suppose also that the cogebra EE is graded. Then, in the graded associative algebra E∗gr=HomgrA(E,A)E^{*gr} = \mathrm{Homgr}_A(E, A), the product of nn elements u1,u2,…,unu_1, u_2, \ldots, u_n of degree 1 is given by
u1u2…un=mn∘(u1⊗u2⊗⋯⊗un)∘δn u_1 u_2 \ldots u_n = m_n \circ (u_1 \otimes u_2 \otimes \cdots \otimes u_n) \circ \delta_n
*where δn:E→E⊗n\delta_n : E \to E^{\otimes n} is the linear mapping which maps each x∈Ex \in E to the component of cn(x)c_n(x) of multidegree (1,1,…,1)(1, 1, \ldots, 1).

Formula (26) is just the definition of the product in E∗E^* for n=2n = 2; to prove it by induction on nn, observe that

u1u2…un u_1 u_2 \ldots u_n
=m∘((u1u2…un−1)⊗un)∘c = m \circ ((u_1 u_2 \ldots u_{n-1}) \otimes u_n) \circ c
=m∘((mn−1∘(u1⊗u2⊗⋯⊗un−1)∘cn−1)⊗un)∘c = m \circ ((m_{n-1} \circ (u_1 \otimes u_2 \otimes \cdots \otimes u_{n-1}) \circ c_{n-1}) \otimes u_n) \circ c
=m∘(mn−1⊗1A)∘(u1⊗u2⊗⋯⊗un−1⊗un)∘(cn−1⊗1E)∘c = m \circ (m_{n-1} \otimes 1_A) \circ (u_1 \otimes u_2 \otimes \cdots \otimes u_{n-1} \otimes u_n) \circ (c_{n-1} \otimes 1_E) \circ c
=mn∘(u1⊗u2⊗⋯⊗un)∘cn = m_n \circ (u_1 \otimes u_2 \otimes \cdots \otimes u_n) \circ c_n
by virtue of (24), (25), II, § 3, no. 3, formula (5) and the relation
un=1A∘un∘1E∗. u_n = 1_A \circ u_n \circ 1_{E^*}.

When E is graded and the elements ui∈E∗gru_i \in E^{*gr} homogeneous of degree 1, then by definition for homogeneous elements xi∈Ex_i \in E,

(u1⊗u2⊗⋯⊗un)(x1⊗x2⊗⋯⊗xn)=0 (u_1 \otimes u_2 \otimes \cdots \otimes u_n)(x_1 \otimes x_2 \otimes \cdots \otimes x_n) = 0

unless all the xix_i are of degree 1, whence formula (27).

It follows from formulae (3), (5) and (7) of no. 1 and formula (24) that when E is taken to be one of the three graded cogebras T(M)\mathbf{T}(M), S(M)\mathbf{S}(M) and Λ(M)\mathbf{\Lambda}(M), we obtain respectively by induction on nn (using the fact that the coproduct is a graded homomorphism of degree 0), for x1,x2,…,xnx_1, x_2, \ldots, x_n in M:

when E=T(M)E = \mathbf{T}(M),

δn(x1x2⋯xn)=x1⊗x2⊗⋯⊗xn \delta_n(x_1 x_2 \cdots x_n) = x_1 \otimes x_2 \otimes \cdots \otimes x_n

when E=S(M)E = \mathbf{S}(M),

δn(x1x2⋯xn)=∑σ∈Snxσ(1)⊗xσ(2)⊗⋯⊗xσ(n) \delta_n(x_1 x_2 \cdots x_n) = \sum_{\sigma \in \mathfrak{S}_n} x_{\sigma(1)} \otimes x_{\sigma(2)} \otimes \cdots \otimes x_{\sigma(n)}

when E=Λ(M)E = \mathbf{\Lambda}(M),

δn(x1x2⋯xn)=∑σ∈Snεσ⋅xσ(1)⊗xσ(2)⊗⋯⊗xσ(n). \delta_n(x_1 x_2 \cdots x_n) = \sum_{\sigma \in \mathfrak{S}_n} \varepsilon_\sigma \cdot x_{\sigma(1)} \otimes x_{\sigma(2)} \otimes \cdots \otimes x_{\sigma(n)}.

It suffices to note, for example when E=Λ(M)E = \mathbf{\Lambda}(M), that in the expression

cn(x1x2⋯xn)=(cn−1⊗1E)(∑(−1)v(xi1…xip)⊗(xj1…xjn−p)) c_n(x_1 x_2 \cdots x_n) = (c_{n-1} \otimes 1_E) \left( \sum (-1)^v (x_{i_1} \ldots x_{i_p}) \otimes (x_{j_1} \ldots x_{j_{n-p}}) \right)
arising from formula (8) of no. 1, the only terms which can give a term of multidegree (1,1,…,1)(1, 1, \ldots, 1) are those for which n−p=1n - p = 1 and hence
δn(x1x2⋯xn) \delta_n(x_1 x_2 \cdots x_n)
is the term of multidegree (1,1,…,1)(1, 1, \ldots, 1) in the sum
∑i=1n(−1)n−icn−1(x1…xi−1xi+1…xn)⊗xi \sum_{i=1}^n (-1)^{n-i} c_{n-1}(x_1 \ldots x_{i-1} x_{i+1} \ldots x_n) \otimes x_i
and this term is necessarily equal to
∑i=1n(−1)n−iδn−1(x1…xi−1xi+1…xn)⊗xi, \sum_{i=1}^n (-1)^{n-i} \delta_{n-1}(x_1 \ldots x_{i-1} x_{i+1} \ldots x_n) \otimes x_i,
whence the result by the induction hypothesis.

Using Lemma 1, the product in T(M)∗gr\mathbf{T}(M)^{*gr} of nn linear forms x1∗,x2∗,…,xn∗x_1^*, x_2^*, \ldots, x_n^* of M∗M^* is given by

⟨x1∗x2∗…xn∗,x1x2…xn⟩=∏i=1n⟨xi∗,xi⟩ \langle x_1^* x_2^* \ldots x_n^*, x_1 x_2 \ldots x_n \rangle = \prod_{i=1}^n \langle x_i^*, x_i \rangle
for xi∈Mx_i \in M (1≤i≤n1 \leq i \leq n); the product of these nn forms in S(M)∗gr\mathbf{S}(M)^{*gr} is given by

⟨x1∗x2∗…xn∗,x1x2…xn⟩=∑σ∈Sn(∏i=1n⟨xσ(i)∗,xi⟩); \langle x_1^* x_2^* \ldots x_n^*, x_1 x_2 \ldots x_n \rangle = \sum_{\sigma \in \mathfrak{S}_n} \left( \prod_{i=1}^n \langle x_{\sigma(i)}^*, x_i \rangle \right);

finally, the product of these forms in ⋀(M)∗gr\bigwedge(M)^{*gr} is given by

⟨x1∗x1∗…xn∗,x1x2…xn⟩=det⁡(⟨xi∗,xj⟩). \langle x_1^* x_1^* \ldots x_n^*, x_1 x_2 \ldots x_n \rangle = \det(\langle x_i^*, x_j \rangle).
In each of the three cases, we have respectively
θT(x1∗⊗x2∗⊗…⊗xn∗)=x1∗x2∗…xn∗ \theta_T(x_1^* \otimes x_2^* \otimes \ldots \otimes x_n^*) = x_1^* x_2^* \ldots x_n^*
θS(x1∗x2∗…xn∗)=x1∗x2∗…xn∗ \theta_S(x_1^* x_2^* \ldots x_n^*) = x_1^* x_2^* \ldots x_n^*
θΛ(x1∗∧x2∗∧⋯∧xn∗)=xn∗xn−1∗…x1∗=(−1)n(n−1)/2x1∗x2∗…xn∗ \theta_\Lambda(x_1^* \wedge x_2^* \wedge \cdots \wedge x_n^*) = x_n^* x_{n-1}^* \ldots x_1^* = (-1)^{n(n-1)/2} x_1^* x_2^* \ldots x_n^*
and hence we deduce from (28), (29) and (30) the relations
(28 bis)⟨θT(x1∗⊗x2∗⊗⋯⊗xn∗),x1⊗x2⊗⋯⊗xn⟩=∏i=1n⟨xi∗,xi⟩(28\ \mathrm{bis})\quad \langle \theta_T(x_1^* \otimes x_2^* \otimes \cdots \otimes x_n^*), x_1 \otimes x_2 \otimes \cdots \otimes x_n \rangle = \prod_{i=1}^n \langle x_i^*, x_i \rangle
(in other words θT\theta_T restricted to T2(M∗)T^2(M^*) is just the canonical homomorphism of II, § 4, no. 4)
(29 bis)⟨θS(x1∗x2∗…xn∗),x1x2…xn⟩=∑σ∈Sn(∏i=1n⟨xσ(i)∗,xi⟩)(29\ \mathrm{bis})\quad \langle \theta_S(x_1^* x_2^* \ldots x_n^*), x_1 x_2 \ldots x_n \rangle = \sum_{\sigma \in S_n} \left( \prod_{i=1}^n \langle x_{\sigma(i)}^*, x_i \rangle \right)
(30 bis)⟨θΛ(x1∗∧x2∗∧⋯∧xn∗),x1∧x2∧⋯∧xn⟩(30\ \mathrm{bis})\quad \langle \theta_\Lambda(x_1^* \wedge x_2^* \wedge \cdots \wedge x_n^*), x_1 \wedge x_2 \wedge \cdots \wedge x_n \rangle
=(−1)n(n−1)/2det⁡(⟨xi∗,xj⟩). = (-1)^{n(n-1)/2} \det(\langle x_i^*, x_j \rangle).

Proposition 7

Let M be a finitely generated projective A-module. Then the canonical homomorphisms θT:T(M∗)→T(M)∗gr\theta_T : T(M^*) \to T(M)^{*gr} and θΛ:⋀(M∗)→(⋀(M)∗gr)0\theta_\Lambda : \bigwedge(M^*) \to (\bigwedge(M)^{*gr})^0 are bijective. Also the graded dual ⋀(M)∗gr\bigwedge(M)^{*gr} is then equal to the dual ⋀(M)∗\bigwedge(M)^* of the A-module ⋀(M)\bigwedge(M).

Suppose first that M has a finite basis (ei)1≤i≤m(e_i)_{1 \leq i \leq m} and let (ei∗)1≤i≤m(e_i^*)_{1 \leq i \leq m} be the dual basis of M∗M^* (II, § 10, no. 4). Formula (28 bis) shows that, for every finite sequence s=(jk)1≤k≤ns = (j_k)_{1 \leq k \leq n} of n elements of the interval [1,m][1, m] of N\mathbf{N},

θT(ej1∗⊗⋯⊗ejn∗) \theta_T(e_{j_1}^* \otimes \cdots \otimes e_{j_n}^*)
is the element of index s in the basis of (Tn(M))∗(T^n(M))^*, dual to the basis of Tn(M)T^n(M) consisting of the es=ej1⊗⋯⊗ejne_s = e_{j_1} \otimes \cdots \otimes e_{j_n} (§ 5, no. 5, Theorem 1). Hence θT\theta_T is bijective.

Similarly, formula (30 bis) shows that, for every finite subset H of [1,m][1, m] with n elements, (−1)n(n−1)/2θΛ(eH∗)(-1)^{n(n-1)/2} \theta_\Lambda(e_H^*) (notation of § 7, no. 8, Theorem 1) is the element of index H in the basis of (⋀n(M))∗(\bigwedge^n(M))^*, dual to the basis of ⋀n(M)\bigwedge^n(M) consisting of the eHe_H. Hence θΛ\theta_\Lambda is bijective.

Suppose now only that M is finitely generated and projective; then M is a direct factor of a finitely generated free A-module L, so that there exist two

A-linear mappings M→jL→pMM \xrightarrow{j} L \xrightarrow{p} M whose composition is the identity lMl_M. We deduce a commutative diagram

T(M∗)→T(tj)T(L∗)θT↓θT↓T(M)∗gr→tT(j)T(L)∗gr \begin{array}{ccc} T(M^*) & \xrightarrow{T(tj)} & T(L^*) \\ \theta_T \downarrow & & \theta_T \downarrow \\ T(M)^{*gr} & \xrightarrow{tT(j)} & T(L)^{*gr} \end{array}
T(L∗)→T(tp)T(M∗)θT↓θT↓T(L)∗gr→tT(p)T(M)∗gr \begin{array}{ccc} T(L^*) & \xrightarrow{T(tp)} & T(M^*) \\ \theta_T \downarrow & & \theta_T \downarrow \\ T(L)^{*gr} & \xrightarrow{tT(p)} & T(M)^{*gr} \end{array}

and an analogous commutative diagram where TT is replaced by Λ\Lambda. The proposition then follows from the following lemma:

Lemma 2

Let

X→uY→vXf↓g↓f↓X′→u′Y′→v′X′ \begin{array}{ccccc} X & \xrightarrow{u} & Y & \xrightarrow{v} & X \\ f \downarrow & & g \downarrow & & f \downarrow \\ X' & \xrightarrow{u'} & Y' & \xrightarrow{v'} & X' \end{array}

be a commutative diagram of sets and mappings such that v∘uv \circ u and v′∘u′v' \circ u' are the identity mappings of XX and X′X' respectively. Then, if gg is injective (resp. surjective, resp. bijective), so is ff.

uu is injective since v∘uv \circ u is, hence, if gg is injective, u′∘f=g∘uu' \circ f = g \circ u is injective and therefore ff is injective. Similarly v′v' is surjective since v′∘u′v' \circ u' is; hence, if gg is surjective, f∘v=v′∘gf \circ v = v' \circ g is surjective and therefore ff is surjective.

The last assertion of Proposition 7 follows from the fact that Λ(M)\Lambda(M) is then a finitely generated A-module (§ 7, no. 3, Proposition 6 and II, § 11, no. 6, Remark).

We now examine what can be said concerning the homomorphism θS\theta_S when MM is projective and finitely generated. Suppose first that MM admits a finite basis (ei)1≤i≤m(e_i)_{1 \leq i \leq m}. In the notation at the beginning of the chapter the A-module Sn(M)S^n(M) admits as basis the family of elements eαe^\alpha such that ∣α∣=n|\alpha| = n. Let uαu_\alpha (for ∣α∣=n|\alpha| = n) denote the element of index α\alpha in the basis of (Sn(M))∗(S^n(M))^* dual to (eα)(e^\alpha). The elements uαu_\alpha, for α∈Nm\alpha \in \mathbf{N}^m, therefore form a basis of the algebra S(M)∗grS(M)^{*gr} and we shall obtain the multiplication table of this basis explicitly. We write

uαuβ=∑γ∈Nmaαβγuγwith aαβγ∈A. u_\alpha u_\beta = \sum_{\gamma \in \mathbf{N}^m} a_{\alpha \beta \gamma} u_\gamma \quad \text{with } a_{\alpha \beta \gamma} \in A.

Then by definition

aαβγ=⟨uαuβ,eγ⟩=m((uα⊗uβ)(c(eγ))), a_{\alpha \beta \gamma} = \langle u_\alpha u_\beta, e^\gamma \rangle = m((u_\alpha \otimes u_\beta)(c(e^\gamma))),

where m:A⊗A→Am : A \otimes A \to A defines the multiplication on AA and cc is the coproduct of S(M)S(M). In other words, aαβγa_{\alpha \beta \gamma} is just the coefficient of eα⊗eβe^\alpha \otimes e^\beta when c(eγ)c(e^\gamma) is written in terms of the basis of S(M)⊗S(M)S(M) \otimes S(M) consisting of the eξ⊗eηe^\xi \otimes e^\eta, where ξ\xi and η\eta run through Nm\mathbf{N}^m. But since cc is an algebra homomorphism,

c(eγ)=∏i=1m(c(ei))ri=∏i=1m(ei⊗1+1⊗ei)ri c(e^\gamma) = \prod_{i=1}^m (c(e_i))^{r_i} = \prod_{i=1}^m (e_i \otimes 1 + 1 \otimes e_i)^{r_i}

by formula (4) of no. 1; this gives

(31)

c(eγ)=∑ξ+η=γ(ξ,η)eξ⊗eη c(e^\gamma) = \sum_{\xi + \eta = \gamma} (\xi, \eta) e^\xi \otimes e^\eta
where we write

(32)

((ξ,η))=∏i=1n(ξi+ηi)!ξi!ηi!(cf. § 10, no. 4, formula (18)). ((\xi, \eta)) = \prod_{i=1}^n \frac{(\xi_i + \eta_i)!}{\xi_i! \eta_i!} \quad \text{(cf. § 10, no. 4, formula (18))}.
Hence we obtain the multiplication table

(33)

uαuβ=((α,β))uα+β. u_\alpha u_\beta = ((\alpha, \beta)) u_{\alpha + \beta}.
On the other hand, if (ei∗)1≤i≤m(e_i^*)_{1 \leq i \leq m} is the basis of M∗M^*, dual to (ei)(e_i), it follows from formula (29 bis) that, for all α∈Nm\alpha \in \mathbf{N}^m,

(34)

θS(e∗α)=α!uα \theta_S(e^{*\alpha}) = \alpha! u_\alpha
in the notation of § 6, no. 6. Hence the homomorphism θS\theta_S is bijective if and only if the α!uα\alpha! u_\alpha form a basis of S(M)∗grS(M)^{*gr}, or also if the elements α!1\alpha! 1 are invertible.

Proposition 8

Suppose that the ring AA is an algebra over the field Q\mathbf{Q} of rational numbers; then, for every finitely generated projective AA-module MM, the homomorphism

θS:S(M∗)→S(M)∗gr \theta_S : S(M^*) \to S(M)^{*gr}
is bijective.

It amounts to proving this when MM is finitely generated and free; we pass from this to the general case using Lemma 2 as in the proof of Proposition 7.

Remark

Let MM be an AA-module and ρ:A→B\rho : A \to B a commutative ring homomorphism. Then there is a commutative diagram of graded BB-algebra homomorphisms

T((M∗)(B))⟶(T(M)∗gr)(B)↓T(uM)↓uT(M)T((M(B))∗)→θTT(M(B))∗gr \begin{array}{ccc} T((M^*)_{(B)}) & \longrightarrow & (T(M)^{*gr})_{(B)} \\ \downarrow_{T(u_M)} & & \downarrow^{u_{T(M)}} \\ T((M_{(B)})^*) & \xrightarrow{\theta_T} & T(M_{(B)})^{*gr} \end{array}

where the first row is a homomorphism composed of the homomorphism θT⊗1B:T(M∗)⊗AB→T(M)∗gr\theta_T \otimes 1_B : T(M^*) \otimes_A B \to T(M)^{*gr} and the canonical isomorphism

T((M∗)(B))→T(M∗)⊗AB T((M^*)_{(B)}) \to T(M^*) \otimes_A B

§ 5, no. 3, Proposition 5). It is immediately verified, using formula (28) and the definition of the homomorphism vEv_E (II, § 5, no. 4), that this diagram is commutative. When M is a finitely generated projective A-module, M(B)M_{(B)} is a finitely generated projective B-module (II, § 5, no. 1, Corollary to Proposition 4) and all the homomorphisms of the above diagram are bijective (Proposition 7 and II, § 5, no. 4, Proposition 8). There are analogous commutative diagrams with T replaced by S or Λ\Lambda; the diagram for Λ\Lambda also consists of bijective homomorphisms when M is projective and finitely generated (Proposition 7); if further A is an algebra over Q\mathbf{Q}, the diagram for S also consists of bijective homomorphisms (Proposition 8).

6. Inner products: case of algebras

Let E=⨁p≥0EpE = \bigoplus_{p \geq 0} E_p be a graded A-algebra of type N\mathbf{N} and P a graded A-module of type Z\mathbf{Z}; for every homogeneous element x∈Epx \in E_p, left multiplication by x is an A-linear mapping e(x)e(x) of E into itself which is graded of degree p. For every element u∈HomgrA(E,P)u \in \mathrm{Homgr}_A(E, P), the right inner product of u by x, denoted by u⊥xu \perp x, is the element u∘e(x)u \circ e(x) of HomgrA(E,P)\mathrm{Homgr}_A(E, P). We also write (i(x))(u)=u⊥x(i(x))(u) = u \perp x and we see that i(x)i(x) is a graded endomorphism of degree p of the graded A-module HomgrA(E,P)\mathrm{Homgr}_A(E, P). If now x=∑p≥0xpx = \sum_{p \geq 0} x_p is an arbitrary element of E (with xp∈Epx_p \in E_p for all p≥0p \geq 0, xp=0x_p = 0 except for a finite number of values of pp), we write i(x)=∑p=0∞i(xp)i(x) = \sum_{p=0}^\infty i(x_p), which is therefore an endomorphism of the A-module HomgrA(E,P)\mathrm{Homgr}_A(E, P).

To remember which element, in the expression u⊥xu \perp x, "operates" on the other, observe that the element x which "operates" on u is placed at the free end of the horizontal line in ⊥\perp.

The associativity of the algebra E goes over to the relation e(xy)=e(x)∘e(y)e(xy) = e(x) \circ e(y) for x,yx, y homogeneous; whence, by definition of i(x)i(x),

i(xy)=i(y)∘i(x) i(xy) = i(y) \circ i(x)

first for x,yx, y homogeneous and then, by linearity, for arbitrary x,yx, y in E; this may also be written

(u⊥x)⊥y=u⊥(xy) (u \perp x) \perp y = u \perp (xy)

for x,yx, y in E and u∈HomgrA(E,P)u \in \mathrm{Homgr}_A(E, P); as on the other hand clearly i(1)i(1) is the identity mapping (since this follows from e(1)=1Ee(1) = 1_E) and x↦i(x)x \mapsto i(x) is A-linear, it is seen that the external law of composition (x,u)↦u⊥x(x, u) \mapsto u \perp x (x∈E,u∈HomgrA(E,P)x \in E, u \in \mathrm{Homgr}_A(E, P)) defines, with addition, a right E-module structure on HomgrA(E,P)\mathrm{Homgr}_A(E, P).

In particular we consider the case P=AP = A, HomgrA(E,P)\mathrm{Homgr}_A(E, P) being in this case the graded dual E∗grE^{*gr} of EE; i(x)i(x) is then the graded transpose of the AA-linear mapping e(x)e(x) (II, § 11, no. 6), in other words, for all x,yx, y in EE, u∈E∗gru \in E^{*gr},

⟨u⊔x,y⟩=⟨u,xy⟩. \langle u \sqcup x, y \rangle = \langle u, xy \rangle.

With the convention at the beginning of the paragraph, note that, if x∈Epx \in E_p, i(x)i(x) is an endomorphism of E∗grE^{*gr} of degree −p-p.

For every homogeneous element x∈Epx \in E_p, right multiplication by xx is similarly denoted by e′(x)e'(x) and the element u∘e′(x)u \circ e'(x) of HomgrA(E,P)\mathrm{Homgr}_A(E, P), called the left inner product of u by x, by x⊔ux \sqcup u; we write i′(x)=x⊔ui'(x) = x \sqcup u and i′(x)i'(x) is therefore a graded endomorphism of HomgrA(E,P)\mathrm{Homgr}_A(E, P) of degree pp; as above this definition can be extended to the case where xx is an arbitrary element of EE. As in this case e′(xy)=e′(y)e′(x)e'(xy) = e'(y)e'(x),

i′(xy)=i′(x)∘i′(y) i'(xy) = i'(x) \circ i'(y)

which may also be written

x⊔(y⊔u)=(xy)⊔u x \sqcup (y \sqcup u) = (xy) \sqcup u

and shows that the external law of composition (x,u)↦x⊔u(x, u) \mapsto x \sqcup u defines, with addition, a left E-module structure on HomgrA(E,P)\mathrm{Homgr}_A(E, P). The associativity of EE implies on the other hand that e(x)∘e′(y)=e′(y)∘e(x)e(x) \circ e'(y) = e'(y) \circ e(x) for x,yx, y homogeneous in EE, whence the relation

(y⊔u)⊔x=y⊔(u⊔x) (y \sqcup u) \sqcup x = y \sqcup (u \sqcup x)

so that the two external laws of composition on HomgrA(E,P)\mathrm{Homgr}_A(E, P) define on this set an (E, E)-*bimodule* structure (II, § 1, no. 14).

When we take P=AP = A, i′(x)i'(x) is the graded transpose of e′(x)e'(x); in other words, for all x,yx, y in EE, u∈E∗gru \in E^{*gr},

⟨y,x⊔u⟩=⟨yx,u⟩. \langle y, x \sqcup u \rangle = \langle yx, u \rangle.

When the graded algebra EE is commutative, obviously u⊔x=x⊔uu \sqcup x = x \sqcup u. When EE is anticommutative and P=AP = A, then for x∈Epx \in E_p, y∈Ery \in E_r and u∈Eq∗u \in E_q^*, yx=(−1)prxyyx = (-1)^{pr} xy, whence, by (37) and (41), ⟨u⊔x,y⟩=(−1)pr⟨y,x⊔u⟩\langle u \sqcup x, y \rangle = (-1)^{pr} \langle y, x \sqcup u \rangle. But as the two sides of this relation are zero except for r=q−pr = q - p,

x⊔u=(−1)p(q−p)u⊔x. x \sqcup u = (-1)^{p(q-p)} u \sqcup x.

Let FF be another graded AA-algebra and ϕ:E→F\phi : E \to F an AA-homomorphism of graded algebras; then ϕ~=Hom(ϕ,1P):HomgrA(F,P)→HomgrA(E,P)\tilde{\phi} = \mathrm{Hom}(\phi, 1_P) : \mathrm{Homgr}_A(F, P) \to \mathrm{Homgr}_A(E, P) is a graded AA-homomorphism of degree 0; by definition, for x,yx, y in EE and u∈HomgrA(F,P)u \in \mathrm{Homgr}_A(F, P)

(ϕ~(u⊔ϕ(x)))(y)=(u⊔ϕ(x))(ϕ(y))=u(ϕ(x)ϕ(y))=u(ϕ(xy))=(ϕ~(u))(xy)=(ϕ~(u)⊔x)(y) \begin{align*} (\tilde{\phi}(u \sqcup \phi(x)))(y) &= (u \sqcup \phi(x))(\phi(y)) \\ &= u(\phi(x)\phi(y)) = u(\phi(xy)) = (\tilde{\phi}(u))(xy) = (\tilde{\phi}(u) \sqcup x)(y) \end{align*}

or also

ϕ~(u⊔ϕ(x))=ϕ~(u)⊔x \tilde{\phi}(u \sqcup \phi(x)) = \tilde{\phi}(u) \sqcup x

and similarly

ϕ~(ϕ(x)⊔u)=x⊔ϕ~(u). \tilde{\phi}(\phi(x) \sqcup u) = x \sqcup \tilde{\phi}(u).

In other words, when Homgr_A(F, P) is considered as an (E, E)-bimodule by means of the ring homomorphism ϕ:E→F\phi : E \to F, it is seen that ϕ~\tilde{\phi} is an (E, E)-bimodule homomorphism (or also an E-homomorphism of the (F, F)-bimodule Homgr_A(F, P) into the (E, E)-bimodule Homgr_A(E, P)).

Example

In particular the above may be applied when E is one of the graded algebras T(M), S(M) or ⋀(M)\bigwedge(M) for an A-module M and P an A-module (with the trivial graduation). To find explicitly the bimodule structures thus obtained, note that the elements of degree −n-n of Homgr_A(T(M), P) (resp. Homgr_A(S(M), P), resp. Homgr_A(⋀(M)\bigwedge(M), P)) are identified with the n-linear mappings (resp. symmetric n-linear mappings, resp. alternating n-linear mappings) of MnM^n into P. It suffices to express the products

f⊔(x1⊗x2⊗⋯⊗xp) f \sqcup (x_1 \otimes x_2 \otimes \cdots \otimes x_p)

(resp. f⊔(x1x2…xp)f \sqcup (x_1 x_2 \ldots x_p)), resp. f⊔(x1∧x2∧⋯∧xp)f \sqcup (x_1 \wedge x_2 \wedge \cdots \wedge x_p)) for every finite sequence (xi)1≤i≤p(x_i)_{1 \leq i \leq p} of elements of M and the analogues for the left inner product. It follows immediately from the definitions that

f⊔(x1⊗x2⊗⋯⊗xp)=(x1⊗x2⊗⋯⊗xp)⊔f=0 f \sqcup (x_1 \otimes x_2 \otimes \cdots \otimes x_p) = (x_1 \otimes x_2 \otimes \cdots \otimes x_p) \sqcup f = 0

if* p>np > n and that, for p≤np \leq n, f⊔(x1⊗x2⊗⋯⊗xp)f \sqcup (x_1 \otimes x_2 \otimes \cdots \otimes x_p) (resp.

(x1⊗x2⊗⋯⊗xp)⊔f) (x_1 \otimes x_2 \otimes \cdots \otimes x_p) \sqcup f)

is the (n - p)-linear mapping defined by

{(f⊔(x1⊗x2⊗⋯⊗xp))(y1,…,yn−p)=f(x1,…,xp,y1,…,yn−p)((x1⊗x2⊗⋯⊗xp)⊔f)(y1,…,yn−p)=f(y1,…,yn−p,x1,…,xp). \begin{cases} (f \sqcup (x_1 \otimes x_2 \otimes \cdots \otimes x_p))(y_1, \ldots, y_{n-p}) \\ \hspace{10cm} = f(x_1, \ldots, x_p, y_1, \ldots, y_{n-p}) \\ ((x_1 \otimes x_2 \otimes \cdots \otimes x_p) \sqcup f)(y_1, \ldots, y_{n-p}) \\ \hspace{10cm} = f(y_1, \ldots, y_{n-p}, x_1, \ldots, x_p). \end{cases}

For p>np > n, there are also in Homgr_A(S(M), P) (resp. Homgr_A(⋀(M)\bigwedge(M), P)) formulae (44) with x1⊗x2⊗⋯⊗xpx_1 \otimes x_2 \otimes \cdots \otimes x_p replaced by x1x2…xpx_1 x_2 \ldots x_p (resp. x1∧x2∧⋯∧xpx_1 \wedge x_2 \wedge \cdots \wedge x_p). For p≤np \leq n, the same substitutions in (45) define the symmetric (n - p)-linear mappings f⊔(x1x2…xp)f \sqcup (x_1 x_2 \ldots x_p) and (x1x2…xp)⊔f(x_1 x_2 \ldots x_p) \sqcup f (resp. the alternating (n - p)-linear mappings

f⊔(x1∧x2∧⋯∧xp)and(x1∧x2∧⋯∧xp)⊔f). f \sqcup (x_1 \wedge x_2 \wedge \cdots \wedge x_p) \quad \text{and} \quad (x_1 \wedge x_2 \wedge \cdots \wedge x_p) \sqcup f).

When n=pn = p, the above products are equal to the constant function on MM equal to f(x1,…,xp)f(x_1, \ldots, x_p).

If u:M→Nu : M \to N is an AA-module homomorphism, T(u):T(M)→T(N)T(u) : T(M) \to T(N) is a graded AA-algebra homomorphism, then it follows from what we have seen above that (T(u))∼(T(u))^\sim is a T(M)T(M)-homomorphism of the (T(N),T(N))(T(N), T(N))-bimodule HomgrA(T(N),P)\mathrm{Homgr}_A(T(N), P) into the (T(M),T(M))(T(M), T(M))-bimodule HomgrA(T(M),P)\mathrm{Homgr}_A(T(M), P), relative to the ring homomorphism T(u)T(u). There are analogous results for (S(u))∼(S(u))^\sim and (∧(u))∼(\wedge(u))^\sim.

7. Inner products: case of cogebras

Let E=⨁p≥0EpE = \bigoplus_{p \geq 0} E_p be a coassociative counital graded cogebra. Then we know (no. 2, Propositions 1 and 3) that the graded dual E∗grE^{*\mathrm{gr}} has (with the convention on graduations made at the beginning of the paragraph) a graded algebra structure of type N\mathbf{N} over AA, the product of two elements u,vu, v of this algebra being defined by uv=m∘(u⊗v)∘cuv = m \circ (u \otimes v) \circ c, where c:E→E⊗AEc : E \to E \otimes_A E is the coproduct and m:A⊗AA→Am : A \otimes_A A \to A defines the multiplication. In other words, if, for x∈Ex \in E, c(x)=∑iyi⊗zic(x) = \sum_i y_i \otimes z_i, we can write (canonically identifying A⊗AEA \otimes_A E and EE)

⟨x,uv⟩=(uv)(x)=∑iu(yi)v(zi)=v(∑iu(yi)zi)=v(((u⊗1E)∘c)(x))=⟨((u⊗1E)∘c)(x),v⟩. \langle x, uv \rangle = (uv)(x) = \sum_i u(y_i)v(z_i) = v\left( \sum_i u(y_i)z_i \right) = v(((u \otimes 1_E) \circ c)(x)) = \langle ((u \otimes 1_E) \circ c)(x), v \rangle.

This can be interpreted by saying that, for all uu homogeneous of degree pp in E∗grE^{*\mathrm{gr}}, the left multiplication e(u):v↦uve(u) : v \mapsto uv in E∗grE^{*\mathrm{gr}} is the graded transpose of the graded endomorphism of degree −p-p

(46)(46)
i(u)=(u⊗1E)∘c i(u) = (u \otimes 1_E) \circ c
of EE; hence, in the above notation,

(i(u))(x)=∑iu(yi)zi. (i(u))(x) = \sum_i u(y_i)z_i.

Formula (46) also defines an element i(u)∈EndgrA(E)i(u) \in \mathrm{Endgr}_A(E) for every element u∈E∗gru \in E^{*\mathrm{gr}}; for all x∈Ex \in E and all u∈E∗gru \in E^{*\mathrm{gr}}, we write

(47)(47)
x⊥u=(i(u))(x) x \perp u = (i(u))(x)
so that, for uu and vv in E∗grE^{*\mathrm{gr}},

⟨x,uv⟩=⟨x⊥u,v⟩. \langle x, uv \rangle = \langle x \perp u, v \rangle.

The element x⊥ux \perp u of EE is called the right inner product of xx by uu.

Here again the element uu which "operates" on xx is placed at the free end of the horizontal line in x‾\underline{\phantom{x}}.

For any two elements u,vu, v of E∗grE^{*\mathrm{gr}},

x(uv)‾=(xu‾)v‾, x \underline{\phantom{(uv)}} = (x \underline{\phantom{u}}) \underline{\phantom{v}},

in other words

i(uv)=i(v)∘i(u). i(uv) = i(v) \circ i(u).

As above let c(x)=∑iyi⊗zic(x) = \sum_i y_i \otimes z_i, so that x(uv)‾=∑i(uv)(yi)zix \underline{\phantom{(uv)}} = \sum_i (uv)(y_i)z_i. If

c(yi)=∑jyij′⊗yij′′, c(y_i) = \sum_j y_{ij}' \otimes y_{ij}'',

then

x(uv)‾=∑i,ju(yij′)v(yij′′)zi. x \underline{\phantom{(uv)}} = \sum_{i,j} u(y_{ij}')v(y_{ij}'')z_i.

On the other hand, if c(zi)=∑kzik′⊗zik′′c(z_i) = \sum_k z_{ik}' \otimes z_{ik}'', then

(xu‾)v‾=∑i,ku(yi)v(zik′)zik′′. (x \underline{\phantom{u}}) \underline{\phantom{v}} = \sum_{i,k} u(y_i)v(z_{ik}')z_{ik}''.

Now, the coassociativity of EE shows that (no. 2, Proposition 1)

∑i,jyij′⊗yij′′⊗zi=∑i,kyi⊗zik′⊗zik′′ \sum_{i,j} y_{ij}' \otimes y_{ij}'' \otimes z_i = \sum_{i,k} y_i \otimes z_{ik}' \otimes z_{ik}''

and the equality of expressions (49) and (50) follows from the fact that they are respectively the image of the left and right hand sides of (51) under the linear mapping ff from E⊗E⊗EE \otimes E \otimes E to EE such that f(x⊗y⊗z)=u(x)v(y)zf(x \otimes y \otimes z) = u(x)v(y)z.

We recall on the other hand (no. 2, Proposition 3) that the unit element of the algebra E∗grE^{*\mathrm{gr}} is the linear form e:x↦γ(x).1e : x \mapsto \gamma(x).1; hence

xe‾=∑iγ(yi)zi=x x \underline{\phantom{e}} = \sum_i \gamma(y_i)z_i = x

by virtue of the definition of counit. As the mapping u↦i(u)u \mapsto i(u) is linear, it is seen that the external law of composition (u,x)↦xu‾(u, x) \mapsto x \underline{\phantom{u}} defines a right E∗grE^{*\mathrm{gr}}-module structure on EE.

Similarly we define, for all u∈E∗gru \in E^{*\mathrm{gr}}, the endomorphism of EE

i′(u)=(1E⊗u)∘c i'(u) = (1_E \otimes u) \circ c

and, for all x∈Ex \in E, we write

(i′(u))(x)=ux‾ (i'(u))(x) = u \underline{\phantom{x}}

and this element of EE is called the left inner product of x by u. As above it is seen that the external law (u,v)↦u⊔x(u, v) \mapsto u \sqcup x defines a left E∗grE^{*\mathrm{gr}}-module structure on EE. Moreover, these two structures are compatible, in other words,

(54)(54)
(u⊔x)⊓v=u⊔(x⊓v)(u \sqcup x) \sqcap v = u \sqcup (x \sqcap v)

for u,vu, v in E∗grE^{*\mathrm{gr}} (II, § 1, no. 14). With the same notation as above, the left hand side of (54) is ∑i,ju(zi)v(yij′)yij′′\sum_{i,j} u(z_i)v(y_{ij}')y_{ij}'' and the right hand side is ∑i,kv(yi)u(zik′′)zik′\sum_{i,k} v(y_i)u(z_{ik}'')z_{ik}'; their equality follows from the fact that they are the respective images of the left and right hand sides of (51) under the linear mapping gg of E⊗E⊗EE \otimes E \otimes E into EE such that g(x⊗y⊗z)=v(x)u(z)yg(x \otimes y \otimes z) = v(x)u(z)y.

It is therefore seen that the two external laws of composition on EE defines on this set an (E∗gr,E∗gr)(E^{*\mathrm{gr}}, E^{*\mathrm{gr}})*-bimodule* structure.

When the cogebra EE is cocommutative, then u⊔x=x⊓uu \sqcup x = x \sqcap u for all x∈Ex \in E and u∈E∗gru \in E^{*\mathrm{gr}}; when it is anticocommutative (§ 4, no. 9) and u∈Ep∗u \in E_p^* and x∈Eqx \in E_q, we can write c(x)=∑0≤j≤q(∑iyij⊗zi,q−j)c(x) = \sum_{0 \leq j \leq q} \left( \sum_i y_{ij} \otimes z_{i, q-j} \right) with yijy_{ij} and zijz_{ij} in EjE_j for all jj and then by hypothesis

∑izij⊗yi,q−j=(−1)j(q−j)∑iyij⊗zi,q−j.\sum_i z_{ij} \otimes y_{i, q-j} = (-1)^{j(q-j)} \sum_i y_{ij} \otimes z_{i, q-j}.

By definition, x⊓u=∑0≤j≤q(∑iu(yij)zi,q−j)x \sqcap u = \sum_{0 \leq j \leq q} \left( \sum_i u(y_{ij})z_{i, q-j} \right) and

u⊔x=∑0≤j≤q(∑iu(zi,q−j)yij).u \sqcup x = \sum_{0 \leq j \leq q} \left( \sum_i u(z_{i, q-j})y_{ij} \right).

As u(yij)=0u(y_{ij}) = 0 (resp. u(zi,q−j)=0u(z_{i, q-j}) = 0 unless j=pj = p (resp. q−j=pq - j = p), it is seen by the above that u⊔x=(−1)p(q−p)x⊓uu \sqcup x = (-1)^{p(q-p)} x \sqcap u.

Finally, let ϕ:E→F\phi : E \to F be a graded cogebra morphism; then it has been seen (no. 2) that the graded transpose tϕ:F∗gr→E∗grt\phi : F^{*\mathrm{gr}} \to E^{*\mathrm{gr}} is a graded algebra homomorphism; therefore, for x∈Ex \in E, u,vu, v in F∗grF^{*\mathrm{gr}},

⟨ϕ(x⊓tϕ(u)),v⟩=⟨x⊓tϕ(u),tϕ(v)⟩=⟨x,tϕ(u)tϕ(v)⟩=⟨x,tϕ(uv)⟩ \langle \phi(x \sqcap t\phi(u)), v \rangle = \langle x \sqcap t\phi(u), t\phi(v) \rangle = \langle x, t\phi(u)t\phi(v) \rangle = \langle x, t\phi(uv) \rangle
=⟨ϕ(x),uv⟩=⟨ϕ(x)⊓u,v⟩ = \langle \phi(x), uv \rangle = \langle \phi(x) \sqcap u, v \rangle

whence

(55)(55)
ϕ(x)⊓u=ϕ(x⊓tϕ(u));\phi(x) \sqcap u = \phi(x \sqcap t\phi(u));

and similarly

(56)(56)
u⊔ϕ(x)=ϕ(tϕ(u)⊔x).u \sqcup \phi(x) = \phi(t\phi(u) \sqcup x).

In other words, ϕ\phi is an F∗grF^{*\mathrm{gr}}*-homomorphism* of the (E∗gr,E∗gr)(E^{*\mathrm{gr}}, E^{*\mathrm{gr}})*-bimodule* EE into the (F∗gr,F∗gr)(F^{*\mathrm{gr}}, F^{*\mathrm{gr}})*-bimodule* FF, relative to the ring homomorphism

tϕ:F∗gr→E∗gr. t\phi : F^{*\mathrm{gr}} \to E^{*\mathrm{gr}}.

Example

In particular the above can be applied when E is one of the graded cogebras T(M), S(M) or Λ(M)\Lambda(M) for an A-module M (no. 1, Examples 5, 6 and 7). To find explicitly the bimodule structures thus obtained, we again identify a homogeneous element f of degree n in T(M)∗grT(M)^{*gr} (resp. S(M)∗grS(M)^{*gr}, resp. Λ(M)∗gr\Lambda(M)^{*gr}) with an n-linear form (resp. symmetric n-linear form, resp. alternating n-linear form, also called an n-form) on MnM^n. It suffices to express the products

(x1⊗x2⊗⋯⊗xp)◃f (resp. (x1x2…xp)◃f, (x_1 \otimes x_2 \otimes \cdots \otimes x_p) \triangleleft f \text{ (resp. } (x_1 x_2 \ldots x_p) \triangleleft f,

resp. (x1∧x2∧⋯∧xp)◃f(x_1 \wedge x_2 \wedge \cdots \wedge x_p) \triangleleft f for every finite sequence (xi)1≤i≤p(x_i)_{1 \leq i \leq p} of elements of M and the analogues for the left inner product. Now, definitions (46) and (52) and formulae (3), (6) and (9) of no. 1 give respectively:

{(x1⊗x2⊗⋯⊗xp)◃f=f▹(x1⊗x2⊗⋯⊗xp)=0(x1x2…xp)◃f=f▹(x1x2…xp)=0for p<n.(x1∧x2∧⋯∧xp)◃f=f▹(x1∧x2∧⋯∧xp)=0 \begin{cases} (x_1 \otimes x_2 \otimes \cdots \otimes x_p) \triangleleft f = f \triangleright (x_1 \otimes x_2 \otimes \cdots \otimes x_p) = 0 \\ (x_1 x_2 \ldots x_p) \triangleleft f = f \triangleright (x_1 x_2 \ldots x_p) = 0 \quad \text{for } p < n. \\ (x_1 \wedge x_2 \wedge \cdots \wedge x_p) \triangleleft f = f \triangleright (x_1 \wedge x_2 \wedge \cdots \wedge x_p) = 0 \end{cases}

For p≥np \geq n, we have respectively

(58) (x1⊗x2⊗⋯⊗xp)◃f=f(x1,…,xn)xn+1⊗⋯⊗xp(x_1 \otimes x_2 \otimes \cdots \otimes x_p) \triangleleft f = f(x_1, \ldots, x_n)x_{n+1} \otimes \cdots \otimes x_p

(59) (x1x2…xp)◃f=∑σf(xσ(1),…,xσ(n))xσ(n+1)⋯xσ(p)(x_1 x_2 \ldots x_p) \triangleleft f = \sum_{\sigma} f(x_{\sigma(1)}, \ldots, x_{\sigma(n)})x_{\sigma(n+1)} \cdots x_{\sigma(p)}

(60) (x1∧x2∧⋯∧xp)◃f=∑σεσf(xσ(1),…,xσ(n))xσ(n+1)∧⋯∧xσ(p)(x_1 \wedge x_2 \wedge \cdots \wedge x_p) \triangleleft f = \sum_{\sigma} \varepsilon_{\sigma} f(x_{\sigma(1)}, \ldots, x_{\sigma(n)})x_{\sigma(n+1)} \wedge \cdots \wedge x_{\sigma(p)}

(where, in (59) and (60), the summations are taken over the permutations σ∈Sp\sigma \in \mathfrak{S}_p which are increasing on each of the intervals [1,n][1, n] and [n+1,p][n+1, p] of N\mathbf{N}; and similarly

(61) f▹(x1⊗x2⊗⋯⊗xp)=f(xp−n+1,…,xp)x1⊗x2⊗⋯⊗xp−nf \triangleright (x_1 \otimes x_2 \otimes \cdots \otimes x_p) = f(x_{p-n+1}, \ldots, x_p)x_1 \otimes x_2 \otimes \cdots \otimes x_{p-n}

(62) f▹(x1x2…xp)=∑σf(xσ(p−n+1),…,xσ(p))xσ(1)⋯xσ(p−n)f \triangleright (x_1 x_2 \ldots x_p) = \sum_{\sigma} f(x_{\sigma(p-n+1)}, \ldots, x_{\sigma(p)})x_{\sigma(1)} \cdots x_{\sigma(p-n)}

(63) f▹(x1∧x2∧⋯∧xp)=∑σεσf(xσ(p−n+1),…,xσ(p))xσ(1)∧⋯∧xσ(p−n)f \triangleright (x_1 \wedge x_2 \wedge \cdots \wedge x_p) = \sum_{\sigma} \varepsilon_{\sigma} f(x_{\sigma(p-n+1)}, \ldots, x_{\sigma(p)})x_{\sigma(1)} \wedge \cdots \wedge x_{\sigma(p-n)}

(where, in (62) and (63), the summations are taken over the permutations σ∈Sp\sigma \in \mathfrak{S}_p which are increasing on each of the intervals [1,p−n][1, p-n] and [p−n+1,p][p-n+1, p] of N\mathbf{N}).

8. Inner products: case of bigebras

Let E be a graded bigebra (resp. skew graded bigebra) (no. 4, Definition 3); then the results of nos. 6 and 7 can be applied to define the right (resp. left) inner products x◃u∈Ex \triangleleft u \in E and u◃x∈E∗gru \triangleleft x \in E^{*gr} (resp. u▹x∈Eu \triangleright x \in E and x▹u∈E∗grx \triangleright u \in E^{*gr}) for all x∈Ex \in E and all u∈E∗gru \in E^{*\mathrm{gr}}. Thus an (E,E)(E, E)-bimodule structure and an (E∗gr,E∗gr)(E^{*\mathrm{gr}}, E^{*\mathrm{gr}})-bimodule structure are obtained on EE. Further:

Proposition 9

Let EE be a graded bigebra (resp. skew graded bigebra). For every element xx of degree 1 in EE, the left and right inner products by xx are derivations (resp. antiderivations) (§10§ 10, no. 2) of the algebra E∗grE^{*\mathrm{gr}}.

In the notation of no. 6, for every homogeneous element xx of degree 1 in a graded bigebra (resp. a skew graded bigebra) EE,

c(x)=x⊗1+1⊗x, c(x) = x \otimes 1 + 1 \otimes x,
by Proposition 5 of no. 3 and the fact that cc is a homomorphism of degree 0. Suppose first that EE is a graded bigebra. For all y∈Ey \in E, by definition
⟨(uv)&x,y⟩=⟨uv,xy⟩=m((u⊗v)(c(xy))) \langle (uv) \mathbin{\&} x, y \rangle = \langle uv, xy \rangle = m((u \otimes v)(c(xy)))
and since cc is an algebra homomorphism, c(xy)=c(x)c(y)c(xy) = c(x)c(y). Let c(y)=∑isi⊗tic(y) = \sum_i s_i \otimes t_i with sis_i and tit_i in EE; therefore
c(xy)=∑i(xsi)⊗ti+∑isi⊗(xti). c(xy) = \sum_i (xs_i) \otimes t_i + \sum_i s_i \otimes (xt_i).
Hence ⟨(uv)&x,y⟩=∑iu(xsi)v(ti)+∑iu(si)v(xti)\langle (uv) \mathbin{\&} x, y \rangle = \sum_i u(xs_i)v(t_i) + \sum_i u(s_i)v(xt_i). But we may write
∑iu(xsi)v(ti)=m(((u&x)⊗v)(c(y)))=⟨(u&x)v,y⟩ \sum_i u(xs_i)v(t_i) = m(((u \mathbin{\&} x) \otimes v)(c(y))) = \langle (u \mathbin{\&} x)v, y \rangle
and similarly
∑iu(si)v(xti)=m((u⊗(v&x))(c(y)))=⟨u(v&x),y⟩, \sum_i u(s_i)v(xt_i) = m((u \otimes (v \mathbin{\&} x))(c(y))) = \langle u(v \mathbin{\&} x), y \rangle,
whence, returning to the notation i(x)i(x) for the inner product.
(64)(64)
(i(x))(uv)=((i(x))(u))v+u((i(x))(v))(i(x))(uv) = ((i(x))(u))v + u((i(x))(v))
which proves that i(x)i(x) is a derivation in E∗grE^{*\mathrm{gr}}.

Suppose now that EE is a skew graded bigebra, that u∈Ep∗u \in E_p^*, v∈Eq∗v \in E_q^* and y∈Ery \in E_r; then we can write

c(y)=∑0≤j≤r(∑isij⊗ti,r−j) c(y) = \sum_{0 \leq j \leq r} \left( \sum_i s_{ij} \otimes t_{i,r-j} \right)
where the sijs_{ij} and tijt_{ij} belong to EjE_j; by definition of the product in Eg⊗AEE^g \otimes_A E, then
c(xy)=c(x)c(y)=∑0≤j≤r(∑i(xsij)⊗ti,r−j+(−1)j∑isij⊗(xti,r−j)) c(xy) = c(x)c(y) = \sum_{0 \leq j \leq r} \left( \sum_i (xs_{ij}) \otimes t_{i,r-j} + (-1)^j \sum_i s_{ij} \otimes (xt_{i,r-j}) \right)
whence this time
⟨(uv)&x,y⟩=∑0≤j≤r(∑iu(xsij)v(ti,r−j)+(−1)j∑iu(sij)v(xti,r−j)). \langle (uv) \mathbin{\&} x, y \rangle = \sum_{0 \leq j \leq r} \left( \sum_i u(xs_{ij})v(t_{i,r-j}) + (-1)^j \sum_i u(s_{ij})v(xt_{i,r-j}) \right).

Then also ∑0≤j≤r(∑iu(xsij)v(ti,r−j))=⟨(u⊔x)v,y⟩\sum_{0 \leq j \leq r} \left( \sum_i u(x s_{ij}) v(t_{i,r-j}) \right) = \langle (u \sqcup x)v, y \rangle. On the other hand, u(sij)=0u(s_{ij}) = 0 unless j=−pj = -p and hence we may also write

∑0≤j≤r(−1)j(∑iu(sij)v(xti,r−j))=(−1)p⟨u(v⊔x),y⟩. \sum_{0 \leq j \leq r} (-1)^j \left( \sum_i u(s_{ij}) v(x t_{i,r-j}) \right) = (-1)^p \langle u(v \sqcup x), y \rangle.
We therefore conclude that
(i(x))(uv)=((i(x))(u))v+(−1)pu((i(x))(v)), (i(x))(uv) = ((i(x))(u))v + (-1)^p u((i(x))(v)),
in other words i(x)i(x) is an antiderivation in E∗grE^{*gr}. The assertions relating to the left inner product by an element xx of degree 1 in EE are proved similarly.

Remark

(1) Let EE be a graded bigebra over AA and N,N′,N′′N, N', N'' three graded AA-modules. Let mm be an AA-bilinear mapping of N×N′N \times N' into N′′N''; for u∈HomgrA(E,N)u \in \mathrm{Homgr}_A(E, N) and v∈HomgrA(E,N′)v \in \mathrm{Homgr}_A(E, N'), let u.vu.v denote the graded homomorphism m∘(u⊗v)∘cm \circ (u \otimes v) \circ c of EE into N′′N''. On the other hand, let i(x)i(x) denote the (right or left) inner product by x∈Ex \in E in the AA-modules HomgrA(E,N)\mathrm{Homgr}_A(E, N), HomgrA(E,N′)\mathrm{Homgr}_A(E, N') and HomgrA(E,N′′)\mathrm{Homgr}_A(E, N''). Then, if xx is of degree 1,

(i(x))(u.v)=((i(x))(u)).v+u.((i(x))(v)) (i(x))(u.v) = ((i(x))(u)).v + u.((i(x))(v))
for all u∈HomgrA(E,N)u \in \mathrm{Homgr}_A(E, N) and v∈HomgrA(E,N′)v \in \mathrm{Homgr}_A(E, N').

Under the same conditions, if EE is a skew graded bigebra and uu is homogeneous of degree pp, then

(i(x))(u.v)=((i(x))(u)).v+(−1)pu.((i(x))(v)). (i(x))(u.v) = ((i(x))(u)).v + (-1)^p u.((i(x))(v)).
The proofs are the same as in Proposition 9.

(2) The same argument as in the above proof proves, more generally, that for all x∈Ex \in E, if c(x)=∑jxj′⊗xj′′c(x) = \sum_j x'_j \otimes x''_j, then, for all u,vu, v in E∗grE^{*gr}, the "Leibniz formula"

(i(x))(uv)=∑j(i(xj′))(u).(i(xj′′))(v) (i(x))(uv) = \sum_j (i(x'_j))(u).(i(x''_j))(v)
holds. In particular, for every primitive element of a graded bigebra EE, that is such that c(x)=x⊗1+1⊗xc(x) = x \otimes 1 + 1 \otimes x, i(x)i(x) is a derivation of E∗grE^{*gr}.

Proposition 10

Let EE be a graded bigebra (resp. skew graded bigebra). For every element ff of degree 1 in E∗grE^{*gr}, the left and right inner products are derivations (resp. antiderivations) of the algebra EE.

Let x∈Ep,y∈Eqx \in E_p, y \in E_q (p≥1,q≥1p \geq 1, q \geq 1). By Proposition 5 of no. 3, we can write

c(x)=x⊗1+∑1≤j≤p−1(∑ixij′⊗xij,p−j′′)+1⊗x c(x) = x \otimes 1 + \sum_{1 \leq j \leq p-1} \left( \sum_i x'_{ij} \otimes x''_{ij,p-j} \right) + 1 \otimes x
c(y)=y⊗1+∑1≤k≤q−1(∑iyi,k′⊗yi,q−k′′)+1⊗y c(y) = y \otimes 1 + \sum_{1 \leq k \leq q-1} \left( \sum_i y'_{i,k} \otimes y''_{i,q-k} \right) + 1 \otimes y

where xij′x'_{ij} and xij′′x''_{ij} belong to EjE_j, yik′y'_{ik} and yik′′y''_{ik} to EkE_k. If EE is a graded bigebra, the component of c(xy)=c(x)c(y)c(xy) = c(x)c(y) belonging to E1⊗EE_1 \otimes E, is equal to

∑ixi,1′⊗xi,p−1′′y+∑iyi,1′⊗xyi,q−1′′ \sum_i x'_{i,1} \otimes x''_{i,p-1}y + \sum_i y'_{i,1} \otimes xy''_{i,q-1}
and hence by definition
(xy)←f=∑if(xi,1′)xi,p−1′′y+∑if(yi,1′)xyi,q−1′′ (xy) \leftarrow f = \sum_i f(x'_{i,1})x''_{i,p-1}y + \sum_i f(y'_{i,1})xy''_{i,q-1}
=(x←f)y+x(y←f) = (x \leftarrow f)y + x(y \leftarrow f)
and the right inner product by ff is a derivation. If on the other hand EE is a skew graded bigebra, the component of c(xy)c(xy) belonging to E1⊗EE_1 \otimes E is equal to
∑ixi,1′⊗xi,p−1′′y+(−1)p∑iyi,1′⊗xyi,q−1′′ \sum_i x'_{i,1} \otimes x''_{i,p-1}y + (-1)^p \sum_i y'_{i,1} \otimes xy''_{i,q-1}
and this time we obtain
(xy)←f=(x←f)y+(−1)px(y←f) (xy) \leftarrow f = (x \leftarrow f)y + (-1)^p x(y \leftarrow f)
which shows that i(f)i(f) is then an antiderivation. The argument is similar for the left inner product by ff.

Example

Propositions 9 and 10 apply in particular to the graded bigebra S(M)S(M) and the skew graded bigebra Λ(M)\Lambda(M). The inner products by elements of degree 1 in S(M)S(M) (resp. S(M)∗grS(M)^{*gr}) are derivations which commute with one another, since S(M)S(M) (resp. S(M)∗grS(M)^{*gr}) is commutative.

Similarly, the inner products by elements of degree 1 in Λ(M)\Lambda(M) (resp. Λ(M)∗gr\Lambda(M)^{*gr}) are antiderivations, which are of zero square, for the square of an element of degree 1 in the algebra Λ(M)\Lambda(M) (resp. Λ(M)∗gr\Lambda(M)^{*gr}) is zero.

9. Inner products between T(M)T(M) and T(M∗)T(M^*), S(M)S(M) and S(M∗)S(M^*), Λ(M)\Lambda(M) and Λ(M∗)\Lambda(M^*)

The right inner product defines on T(M)T(M) (resp. S(M)S(M), resp. Λ(M)\Lambda(M)) a right module structure over the algebra T(M)∗grT(M)^{*gr} (resp. S(M)∗grS(M)^{*gr}, resp. Λ(M)∗gr\Lambda(M)^{*gr}) (no. 7, Examples). Using the canonical homomorphisms θT\theta_T (resp. θS\theta_S, resp. θΛ\theta_\Lambda) of no. 5, we derive a right T(M∗)T(M^*)-module structure on T(M)T(M) a right S(M∗)S(M^*)-module structure on S(M)S(M) a left Λ(M∗)\Lambda(M^*)-module structure on Λ(M)\Lambda(M).

The external law of any of these structures is also denoted by

(z∗,t)↦i(z∗)⋅t (z^*, t) \mapsto i(z^*) \cdot t

(by an abuse of language); we also write t≺z∗t \prec z^* instead of i(z∗).ti(z^*) . t in the case of T(M)T(M) or S(M)S(M); on the other hand, we write z∗≺tz^* \prec t in the case of Λ(M)\Lambda(M) and say that this is a left inner product of tt by z∗z^*, since then we have a left Λ(M∗)\Lambda(M^*)-module law. For z∗z^* homogeneous of degree nn and tt homogeneous of degree pp, i(z∗).t=0i(z^*) . t = 0 if p<np < n and, for xi∈Mx_i \in M (1≤i≤p1 \leq i \leq p), xj∗∈M∗x_j^* \in M^* (1≤j≤n1 \leq j \leq n) and p≥np \geq n, by virtue of formulae (58), (59) and (60) of no. 7,

(66)i(x1∗⊗x2∗⊗⋯⊗xn∗).(x1⊗x2⊗⋯⊗xp) (66)\quad i(x_1^* \otimes x_2^* \otimes \cdots \otimes x_n^*) . (x_1 \otimes x_2 \otimes \cdots \otimes x_p)
=(∏j=1n⟨xj∗,xj⟩)xn+1⊗⋯⊗xp = \left( \prod_{j=1}^n \langle x_j^*, x_j \rangle \right) x_{n+1} \otimes \cdots \otimes x_p
(67)i(x1∗x2∗…xn∗).(x1x2…xp)=∑σ(∏j=1n⟨xj∗,xσ(j)⟩)xσ(n+1)⋯xσ(p) (67)\quad i(x_1^* x_2^* \ldots x_n^*) . (x_1 x_2 \ldots x_p) = \sum_\sigma \left( \prod_{j=1}^n \langle x_j^*, x_{\sigma(j)} \rangle \right) x_{\sigma(n+1)} \cdots x_{\sigma(p)}
(68)i(x1∗∧x2∗∧⋯∧xn∗).(x1∧x2∧⋯∧xp) (68)\quad i(x_1^* \wedge x_2^* \wedge \cdots \wedge x_n^*) . (x_1 \wedge x_2 \wedge \cdots \wedge x_p)
=(−1)n(n−1)/2∑σεσ(∏j=1n⟨xj∗,xσ(j)⟩)xσ(n+1)∧⋯∧xσ(p) = (-1)^{n(n-1)/2} \sum_\sigma \varepsilon_\sigma \left( \prod_{j=1}^n \langle x_j^*, x_{\sigma(j)} \rangle \right) x_{\sigma(n+1)} \wedge \cdots \wedge x_{\sigma(p)}

where, the formulae (67) and (68), σ\sigma runs through the set of permutations σ∈Sp\sigma \in \mathfrak{S}_p which are increasing on the intervals {1,n}\{1, n\} and {n+1,p}\{n + 1, p\}.

We can also write, in the inner product notation,

⟨t≺u∗,v∗⟩=⟨t,θT(u∗v∗)⟩for t∈T(M),u∗,v∗ in T(M∗) \langle t \prec u^*, v^* \rangle = \langle t, \theta_T(u^* v^*) \rangle \quad \text{for } t \in T(M), u^*, v^* \text{ in } T(M^*)
⟨t≺u∗,v∗⟩=⟨t,θS(u∗v∗)⟩for t∈S(M),u∗,v∗ in S(M∗) \langle t \prec u^*, v^* \rangle = \langle t, \theta_S(u^* v^*) \rangle \quad \text{for } t \in S(M), u^*, v^* \text{ in } S(M^*)
⟨v∗,u∗≺t⟩=⟨θΛ(u∗∧v∗),t⟩ for t∈Λ(M),u∗,v∗ in Λ(M∗). \langle v^*, u^* \prec t \rangle = \langle \theta_\Lambda(u^* \wedge v^*), t \rangle \text{ for } t \in \Lambda(M), u^*, v^* \text{ in } \Lambda(M^*).

We leave to the reader the task of finding explicitly the analogous formulae for left inner products, this time using formulae (61), (62) and (63).

The above can be applied with MM replaced by its dual M∗M^*; M∗M^* must then be replaced by the bidual M∗∗M^{**} and T(M∗)T(M^*), for example, thus has a right module structure over the algebra T(M∗∗)T(M^{**}). But the canonical mapping cM:M→M∗∗c_M : M \to M^{**} defines an algebra homomorphism T(cM):T(M)→T(M∗∗)T(c_M) : T(M) \to T(M^{**}), by means of which T(M∗)T(M^*) has a right T(M)T(M)-*module* structure. Similarly S(M∗)S(M^*) (resp. Λ(M∗)\Lambda(M^*)) has a right S(M)S(M)-*module* (resp. left Λ(M)\Lambda(M)-*module*) structure. The explicit formulae giving the external laws of these modules are derived immediately from the above by exchanging the roles of MM and M∗M^*. Note that, for all x∈Mx \in M, i(x)i(x) is always a derivation (resp. antiderivation of zero square) of the graded algebra S(M∗)S(M^*) (resp. Λ(M∗)\Lambda(M^*)).

Proposition 11

The canonical homomorphism* θT:T(M∗)→T(M)∗gr\theta_T : T(M^*) \to T(M)^{*gr} (resp. θS:S(M)→S(M)∗gr\theta_S : S(M) \to S(M)^{*gr}, resp. θΛ:Λ(M∗)→Λ(M)∗gr\theta_\Lambda : \Lambda(M^*) \to \Lambda(M)^{*gr}) is a right T(M)T(M)-*module* (resp. right S(M)S(M)-*module*, resp. left Λ(M)\Lambda(M)-*module*) *homomorphism.

We show first that, for z∗∈T(M∗)z^* \in T(M^*) and t∈T(M)t \in T(M),

θT(z∗∧t)=θT(z∗)∧t. \theta_T(z^* \wedge t) = \theta_T(z^*) \wedge t.

Since MM is a generating system of the algebra T(M)T(M), we need only prove (69) when t=x∈Mt = x \in M; moreover we can restrict our attention to the case where z∗=x1∗⊗x2∗⊗⋯⊗xp∗z^* = x_1^* \otimes x_2^* \otimes \cdots \otimes x_p^*, where the xj∗∈M∗x_j^* \in M^*, and then, by (66) with the roles of MM and M∗M^* interchanged, z∗∧x=⟨x,x1∗⟩x2∗⊗⋯⊗xp∗z^* \wedge x = \langle x, x_1^* \rangle x_2^* \otimes \cdots \otimes x_p^*. Therefore, for all y2,…,ypy_2, \ldots, y_p in MM,

⟨θT(z∗∧x),y2⊗y3⊗⋯⊗yp⟩=⟨x,x1∗⟩∏j=2p⟨yj,xj∗⟩=⟨θT(z∗),x⊗y2⊗⋯⊗yp⟩=⟨θT(z∗)∧x,y2⊗⋯⊗yp⟩ \begin{align*} \langle \theta_T(z^* \wedge x), y_2 \otimes y_3 \otimes \cdots \otimes y_p \rangle &= \langle x, x_1^* \rangle \prod_{j=2}^p \langle y_j, x_j^* \rangle \\ &= \langle \theta_T(z^*), x \otimes y_2 \otimes \cdots \otimes y_p \rangle \\ &= \langle \theta_T(z^*) \wedge x, y_2 \otimes \cdots \otimes y_p \rangle \end{align*}

whence (69).

We prove secondly that for z∗∈S(M∗)z^* \in S(M^*) and t∈S(M)t \in S(M),

θS(z∗∧t)=θS(z∗)∧t. \theta_S(z^* \wedge t) = \theta_S(z^*) \wedge t.

As above, we can limit ourselves to the case t=x∈Mt = x \in M. But further, here i(x)i(x) is a derivation of S(M∗)S(M^*) and a derivation of S(M)∗grS(M)^{*gr}. Therefore (§ 10, no. 7, Corollary to Proposition 9) it suffices to verify (70) for z∗=x∗∈M∗z^* = x^* \in M^*, since M∗M^* is a generating system of S(M∗)S(M^*); but this is trivial, the two sides then being equal to ⟨x∗,x⟩\langle x^*, x \rangle. A similar argument proves the relation

θ∧(t∧z∗)=t∧θ∧(z∗) \theta_\wedge(t \wedge z^*) = t \wedge \theta_\wedge(z^*)

for z∗∈Λ(M∗)z^* \in \Lambda(M^*) and t∈Λ(M)t \in \Lambda(M): observe then that, for x∈Mx \in M, i(x)i(x) is an antiderivation in Λ(M∗)\Lambda(M^*) as well as in Λ(M)∗gr\Lambda(M)^{*gr} and use § 10, no. 7, Corollary to Proposition 9. There is an analogous result for left inner products.

10. Explicit form of inner products in the case of a finitely generated free module

Let MM be a finitely generated free AA-module, (ei)1≤i≤n(e_i)_{1 \leq i \leq n} a basis of MM and (ei∗)1≤i≤n(e_i^*)_{1 \leq i \leq n} the dual basis of M∗M^*. For every finite sequence s=(i1,…,ip)s = (i_1, \ldots, i_p) of elements of {1,n}\{1, n\}, let es=ei1⊗ei2⊗⋯⊗eipe_s = e_{i_1} \otimes e_{i_2} \otimes \cdots \otimes e_{i_p} (resp. es∗=ei1∗⊗⋯⊗eip∗e_s^* = e_{i_1}^* \otimes \cdots \otimes e_{i_p}^*). We know (§ 5, no. 5, Theorem 1) that the ese_s form a basis of the AA-module T(M)T(M) and the es∗e_s^* a basis of the AA-module T(M∗)T(M^*). If s,ts, t are two finite sequences of elements of {1,n}\{1, n\}, let s.ts.t denote the sequence obtained as follows: if s=(i1,…,ip)s = (i_1, \ldots, i_p) and t=(j1,…,jq)t = (j_1, \ldots, j_q), s.ts.t is the sequence (i1,…,ip,j1,…,jq)(i_1, \ldots, i_p, j_1, \ldots, j_q) with p+qp + q terms. Then es.t=es⊗ete_{s.t} = e_s \otimes e_t. It then follows from (66) that

{es∧et∗=0if s is not of the form t.uet.u∧et∗=eu. \begin{cases} e_s \wedge e_t^* = 0 & \text{if } s \text{ is not of the form } t.u \\ e_{t.u} \wedge e_t^* = e_u. \end{cases}

Similarly, the symmetric algebra S(M)S(M) has as basis the set of monomials eαe^\alpha with α∈Nn\alpha \in \mathbf{N}^n (§ 6, no. 6, Theorem 1) and S(M∗)S(M^*) the set of monomials e∗αe^{*\alpha} with α∈Nn\alpha \in \mathbf{N}^n; recall (no. 5) that uαu_\alpha, for ∣α∣=k|\alpha| = k, denotes the element of the basis of (Sk(M))∗(S^k(M))^*, dual to the basis (eα)∣α∣=k(e^\alpha)_{|\alpha|=k} of Sk(M)S^k(M); the uαu_\alpha, for α∈Nn\alpha \in \mathbf{N}^n, therefore form a basis of S(M)∗grS(M)^{*gr}. The definition of right inner product by eβe^\beta in S(M)∗grS(M)^{*gr} as the transpose of multiplication by eβe^\beta in S(M)S(M) then shows that

{uα⊥eβ=0if α≱βuα⊥eβ=uα−βif α≥β. \begin{cases} u_\alpha \perp e^\beta = 0 & \text{if } \alpha \not\geq \beta \\ u_\alpha \perp e^\beta = u_{\alpha-\beta} & \text{if } \alpha \geq \beta. \end{cases}

(73)

Similarly, since S(M)S(M) is here canonically identified with the graded dual of S(M)∗grS(M)^{*gr}, i(uβ)i(u_\beta) is the graded transpose of multiplication by uβu^\beta in S(M)∗grS(M)^{*gr} and hence from the multiplication table (33) (no. 5) of the basis (uα)(u_\alpha) we deduce that

{eα⊥uβ=0if α≱βeα⊥uβ=(β,α−β)eα−βif α≥β. \begin{cases} e^\alpha \perp u_\beta = 0 & \text{if } \alpha \not\geq \beta \\ e^\alpha \perp u_\beta = (\beta, \alpha - \beta)e^{\alpha-\beta} & \text{if } \alpha \geq \beta. \end{cases}

(74)

As for the right inner product of an element of S(M)S(M) by an element of S(M∗)S(M^*), the definition of this product (no. 9) and formula (34) of no. 5 allow us to deduce from (74) the formulae

{eα⊥e∗β=0if α≱βeα⊥e∗β=α!(α−β)!eα−βif α≥β. \begin{cases} e^\alpha \perp e^{*\beta} = 0 & \text{if } \alpha \not\geq \beta \\ e^\alpha \perp e^{*\beta} = \frac{\alpha!}{(\alpha-\beta)!} e^{\alpha-\beta} & \text{if } \alpha \geq \beta. \end{cases}

(75)

There are analogous formulae for the inner product of an element of S(M∗)S(M^*) by an element of S(M)S(M) interchanging the roles of MM and M∗M^* (since M∗∗M^{**} is here identified with MM).

Remark

Being given the basis (ei)1≤i≤n(e_i)_{1 \leq i \leq n} allows us to identify the algebra S(M)S(M) with the polynomial algebra A[X1,…,Xn]A[X_1, \ldots, X_n] (§ 6, no. 6); formula (75) shows that the inner product by e∗αe^{*\alpha} is just the differential operator Dα=D1α1D2α2…DnαnD^\alpha = D_1^{\alpha_1}D_2^{\alpha_2}\ldots D_n^{\alpha_n}, where Di=∂/∂XiD_i = \partial/\partial X_i for 1≤i≤n1 \leq i \leq n (§ 10, no. 11, Example).

Consider finally the exterior algebra Λ(M)\Lambda(M), which has as basis the set of elements eJe_J, where JJ runs through the set of subsets of the interval {1,n}\{1, n\} of N\mathbf{N} (§ 7, no. 8, Theorem 1); similarly Λ(M∗)\Lambda(M^*) has as basis the elements eJ∗e_J^*. It follows from formula (68) of no. 9 that

{eK∗∧eJ=0if K∉JeK∗∧eJ=(−1)p(p−1)/2ρK,J−KeJ−Kif K⊂J and p=Card⁡(K), \begin{cases} e_K^* \wedge e_J = 0 & \text{if } K \notin J \\ e_K^* \wedge e_J = (-1)^{p(p-1)/2} \rho_{K, J-K} e_{J-K} & \text{if } K \subset J \text{ and } p = \operatorname{Card}(K), \end{cases}

(76)

where ρK,J−K\rho_{K, J-K} is the number defined by formula (19) of § 7, no. 8. There are analogous formulae with the roles of MM and M∗M^* interchanged.

11. Isomorphisms between ∧p(M)\wedge^p(M) and ∧n−p(M∗)\wedge^{n-p}(M^*) for an nn-dimensional free module m

Proposition 12

Let M be a free A-module of dimension n; let e∈∧n(M)e \in \wedge^n(M) be an element forming a basis of ∧n(M)\wedge^n(M) and let e∗e^* be the element of ∧n(M∗)\wedge^n(M^*) such that {(−1)n(n−1)/2θ∧(e∗)}\{(-1)^{n(n-1)/2} \theta_{\wedge}(e^*)\} is the dual basis of {e}\{e\} in (∧n(M))∗(\wedge^n(M))^*. Let ϕ:∧(M∗)→∧(M)\phi : \wedge(M^*) \to \wedge(M) be the mapping z↦z∧e∗z \mapsto z \wedge e^* and ϕ′:∧(M∗)→∧(M)\phi' : \wedge(M^*) \to \wedge(M) the mapping z∗↦z∗∧ez^* \mapsto z^* \wedge e. Let ϕp\phi_p (resp. ϕp′\phi'_p) be the restriction of ϕ\phi (resp. ϕ′\phi') to ∧p(M)\wedge^p(M) (resp. ∧p(M∗)\wedge^p(M^*)). Then:

(i) *The mapping ϕ\phi is a left ∧(M)\wedge(M)-module isomorphism and the mapping ϕ′\phi' is a left ∧(M∗)\wedge(M^*)-module isomorphism; moreover the mappings ϕ\phi and ϕ′\phi' are inverses of one another.

(ii) *The mapping ϕp\phi_p is an isomorphism of the A-module ∧p(M)\wedge^p(M) onto the A-module ∧n−p(M∗)\wedge^{n-p}(M^*) and the mapping ϕp′\phi'_p is an isomorphism of the A-module ∧p(M∗)\wedge^p(M^*) onto the A-module ∧n−p(M)\wedge^{n-p}(M).

(iii) *If we write B(u,v∗)=⟨u,θ∧(v∗)⟩B(u, v^*) = \langle u, \theta_{\wedge}(v^*) \rangle for u∈∧(M)u \in \wedge(M) and v∗∈∧(M∗)v^* \in \wedge(M^*) then, for u∗∈∧p(M∗)u^* \in \wedge^p(M^*) and v∗∈∧n−p(M∗)v^* \in \wedge^{n-p}(M^*),

B(ϕp′(u∗),v∗)=(−1)p(n−p)B(u∗,ϕn−p′(v∗)). B(\phi'_p(u^*), v^*) = (-1)^{p(n-p)} B(u^*, \phi'_{n-p}(v^*)).

The fact that ϕ\phi is ∧(M)\wedge(M)-linear and ϕ′\phi' is ∧(M∗)\wedge(M^*)-linear follows from the formulae (u∧v)∧e∗=u∧(v∧e∗)(u \wedge v) \wedge e^* = u \wedge (v \wedge e^*) and (u∗∧v∗)∧e=u∗∧(v∗∧e)(u^* \wedge v^*) \wedge e = u^* \wedge (v^* \wedge e) (no. 6, formula (37)), using the fact that θ∧\theta_{\wedge} is an isomorphism of ∧(M∗)\wedge(M^*) onto the opposite algebra to ∧(M)∗\wedge(M)^*. On the other hand there exists a basis (ei)1≤i≤n(e_i)_{1 \leq i \leq n} of M such that

e=e1∧e2∧⋯∧enande∗=(−1)n(n−1)/2e1∗∧e2∗∧⋯∧en∗, e = e_1 \wedge e_2 \wedge \cdots \wedge e_n \quad \text{and} \quad e^* = (-1)^{n(n-1)/2} e_1^* \wedge e_2^* \wedge \cdots \wedge e_n^*,

where (ei∗)(e_i^*) is the basis dual to (ei)(e_i). We write I={1,n}I = \{1, n\}; it follows from (76) that, for every subset J of I with p elements,

{ϕ(eJ)=(−1)n(n−1)/2+p(p−1)/2ρJ,I−JeI∗Jϕ′(eJ∗)=(−1)p(p−1)/2ρJ,I−JeI−J. \begin{cases} \phi(e_J) = (-1)^{n(n-1)/2 + p(p-1)/2} \rho_{J, I-J} e_I^* J \\ \phi'(e_J^*) = (-1)^{p(p-1)/2} \rho_{J, I-J} e_{I-J}. \end{cases}

This proves that ϕ\phi and ϕ′\phi' are bijective; moreover ρJ,I−JρI−J,J=(−1)p(n−p)\rho_{J, I-J} \rho_{I-J, J} = (-1)^{p(n-p)} (§ 7, no. 8, formula (21)); as the number

n(n−1)2+p(p−1)2+(n−p)(n−p−1)2+p(n−p)=n(n−1) \frac{n(n-1)}{2} + \frac{p(p-1)}{2} + \frac{(n-p)(n-p-1)}{2} + p(n-p) = n(n-1)

is even, it follows that ϕ\phi and ϕ′\phi' are inverses of one another. Finally, to prove (77), it suffices to take u∗=eJ∗u^* = e_J^* and v∗=eI−J∗v^* = e_{I-J}^*; the verification also follows from the definition of θ∧\theta_{\wedge}, formulae (78) and the relation ρJ,I−JρI−J,J=(−1)p(n−p)\rho_{J, I-J} \rho_{I-J, J} = (-1)^{p(n-p)} (§ 7, no. 8, formula (21)). Note that, for u∗∈∧p(M∗)u^* \in \wedge^p(M^*) and v∗∈∧n−p(M∗)v^* \in \wedge^{n-p}(M^*),

B(\phi_p'(u^*), v^*) is, to within a sign, the coefficient of u∗∧v∗u^* \wedge v^* with respect to the basis {e∗}\{e^*\} of Λn(M∗)\Lambda^n(M^*).

Proposition 13

With the hypotheses and notation of Proposition 11, for every endomorphism g of the A-module M.

(79)(79)
(det⁡g)ϕ=Λ(tg)∘ϕ∘Λ(g).(\det g)\phi = \Lambda^{(tg)} \circ \phi \circ \Lambda(g).

Clearly Λ(tg)=θΛ−1∘(tΛ(g))∘θΛ\Lambda^{(tg)} = \theta_{\Lambda}^{-1} \circ (t\Lambda(g)) \circ \theta_{\Lambda}; since Λ(g)\Lambda(g) is an endomorphism of the algebra Λ(M)\Lambda(M) and by definition, for all

z∈Λ(M),θΛ(Λ(g)(z)⊥e∗)=θΛ(e∗)⊥θΛ(Λ(g)(z)),z \in \Lambda(M), \quad \theta_{\Lambda}(\Lambda(g)(z) \perp e^*) = \theta_{\Lambda}(e^*) \perp \theta_{\Lambda}(\Lambda(g)(z)),
we deduce from formula (42) of no. 6 that
((θΛ−1∘(tΛ(g))∘θΛ)∘ϕ∘Λ(g))(z)=θΛ−1(tΛ(g)(θΛ(e∗))⊥z)=z⊥(Λ(tg)(e∗))=(det⁡g)(z⊥e∗)=(det⁡g)ϕ(z) ((\theta_{\Lambda}^{-1} \circ (t\Lambda(g)) \circ \theta_{\Lambda}) \circ \phi \circ \Lambda(g))(z) = \theta_{\Lambda}^{-1}(t\Lambda(g)(\theta_{\Lambda}(e^*)) \perp z) = z \perp (\Lambda^{(tg)}(e^*)) = (\det g)(z \perp e^*) = (\det g)\phi(z)
taking account of § 8, no. 4, Proposition 8.

Corollary

For every automorphism g of E,*

(80)(80)
Λ(tg−1)=(det⁡g)−1ϕ∘(Λ(g))∘ϕ−1.\Lambda^{(tg^{-1})} = (\det g)^{-1}\phi \circ (\Lambda(g)) \circ \phi^{-1}.

12. Application to the subspace associated with a p-vector

Let K be a field and E a vector space over K. Recall that with every pp-vector z∈Λp(E)z \in \Lambda^p(E) is associated a finite-dimensional subspace MzM_z of E, namely the smallest vector subspace M of E such that z∈Λp(M)z \in \Lambda^p(M) (§ 7, no. 2, Corollary to Proposition 4).

Proposition 14

(i) *The orthogonal of MzM_z in E∗E^* is the set of x∗∈E∗x^* \in E^* such that x∗⊥z=0x^* \perp z = 0.

(ii) The subspace MzM_z associated with z is the image of Λp−1(E∗)\Lambda^{p-1}(E^*) under the mapping λz:u∗↦u∗⊥z\lambda_z : u^* \mapsto u^* \perp z of Λp−1(E∗)\Lambda^{p-1}(E^*) into E.

Let N denote the image of λz\lambda_z. For x∗∈E∗x^* \in E^* and u∗∈Λp−1(E∗)u^* \in \Lambda^{p-1}(E^*),

⟨θΛ(x∗),u∗⊥z⟩=⟨θΛ(u∗∧x∗),z⟩=(−1)p−1⟨θΛ(x∗∧u∗),z⟩=(−1)p−1⟨θΛ(u∗),x∗⊥z⟩. \langle \theta_{\Lambda}(x^*), u^* \perp z \rangle = \langle \theta_{\Lambda}(u^* \wedge x^*), z \rangle = (-1)^{p-1} \langle \theta_{\Lambda}(x^* \wedge u^*), z \rangle \\ = (-1)^{p-1} \langle \theta_{\Lambda}(u^*), x^* \perp z \rangle.
Therefore, for x∗x^* to be orthogonal to N, it is necessary and sufficient that x∗⊥zx^* \perp z be orthogonal to θΛ(Λ(E∗))\theta_{\Lambda}(\Lambda(E^*)). Now, the latter condition is equivalent to saying that x∗⊥z=0x^* \perp z = 0; for let (eλ)λ∈L(e_{\lambda})_{\lambda \in L} be a basis of E; giving L a total ordering, it has been seen (§ 7, no. 8, Theorem 1) that the eJe_J, for J running through the set F(L)\mathscr{F}(L) of finite subsets of L, form a basis of Λ(E)\Lambda(E); it then follows from formula (30) of no. 5 that the elements θ∧(eJ∗)\theta_{\wedge}(e_J^*) are, to within a sign, the coordinate forms on ∧(E)\wedge(E) relative to the basis (eJ)(e_J); whence our assertion.

The orthogonal of N therefore consists of the x∗∈E∗x^* \in E^* such that x∗⊥z=0x^* \perp z = 0 and the conclusion of (i) will therefore follow from (ii).

We show first that N⊂MzN \subset M_z. Let M be a vector subspace of E such that z∈∧(M)z \in \wedge(M) and let j:M→Ej : M \to E be the canonical injection; let μz\mu_z denote the mapping v∗↦v∗⊥zv^* \mapsto v^* \perp z of ∧p−1(M∗)\wedge^{p-1}(M^*) into M; it follows from formula (60) of no. 7 that there is a canonical factorization

λz:∧p−1(E∗)→∧p−1(tj)∧p−1(M∗)→μzM→jE \lambda_z : \wedge^{p-1}(E^*) \xrightarrow{\wedge^{p-1}(t_j)} \wedge^{p-1}(M^*) \xrightarrow{\mu_z} M \xrightarrow{j} E

which proves that N⊂MN \subset M and hence N⊂MzN \subset M_z by definition of MzM_z. It remains to verify that N=MzN = M_z. Suppose the converse: there would then exist a basis (ei)1≤i≤n(e_i)_{1 \leq i \leq n} of MzM_z and an element x∗∈E∗x^* \in E^* such that ⟨x∗,e1⟩=1,⟨x∗,ej⟩=0\langle x^*, e_1 \rangle = 1, \langle x^*, e_j \rangle = 0 for 2≤j≤n2 \leq j \leq n and such that x∗x^* is orthogonal to N and hence x∗⊥z=0x^* \perp z = 0. We write z=∑HaHeHz = \sum_H a_H e_H, where the sum is taken over the subsets of {1,n}\{1, n\} with pp elements. By (68) (no. 9),

x∗⊥eH=0if 1∉Hx∗⊥e{1}∪H=eHif H⊂{2,n} x^* \perp e_H = 0 \quad \text{if } 1 \notin H \\ x^* \perp e_{\{1\} \cup H} = e_H \quad \text{if } H \subset \{2, n\}

which shows that the relation x∗⊥z=0x^* \perp z = 0 implies aH=0a_H = 0 for 1∈H1 \in H. But this is impossible, for zz would then belong to ∧p(M′)\wedge^p(M'), where M′M' is the subspace of M generated by e2,…,ene_2, \ldots, e_n.

13. Pure pp-vectors. Grassmannians

Let K be a field and E a vector space over K. A pp-vector z∈∧p(E)z \in \wedge^p(E) is called pure (or sometimes decomposable) if it is non-zero and there exist vectors x1,…,xpx_1, \ldots, x_p in E such that z=x1∧x2∧⋯∧xpz = x_1 \wedge x_2 \wedge \cdots \wedge x_p. For this, it is necessary and sufficient that the subspace MzM_z associated with zz (which is always of dimension ≥p\geq p for z≠0z \neq 0) be exactly of dimension pp (since ∧p(Mz)\wedge^p(M_z) is then of dimension 1). In particular, every non-zero scalar, every non-zero element of E=∧1(E)E = \wedge^1(E), every non-zero element of ∧n(E)\wedge^n(E), when E is of dimension nn, is pure.

Proposition 15

Let E be a vector space of dimension n and let e be an element ≠0\neq 0 of ∧n(E)\wedge^n(E) (hence forming a basis of this vector space). Let ϕ:∧(E)→∧(E∗)\phi : \wedge(E) \to \wedge(E^*) be the vector space isomorphism associated with e (no. 11, Proposition 12). If z is a pure element of ∧p(E)\wedge^p(E), then ϕ(z)\phi(z) is a pure element of ∧n−p(E∗)\wedge^{n-p}(E^*) and the subspaces associated with z and ϕ(z)\phi(z) are orthogonal.

The cases p=0p = 0 and p=np = n are trivial. Suppose therefore that 1≤p≤n−11 \leq p \leq n - 1 and let z=x1∧⋯∧xp≠0z = x_1 \wedge \cdots \wedge x_p \neq 0. Then there exists a basis (ei)1≤i≤n(e_i)_{1 \leq i \leq n} of E such that ei=xie_i = x_i for 1≤i≤p1 \leq i \leq p and e=e1∧e2∧⋯∧ene = e_1 \wedge e_2 \wedge \cdots \wedge e_n. It then follows from formula (78) of no. 11 that ϕ(z)=±ep+1∗∧⋯∧en∗\phi(z) = \pm e_{p+1}^* \wedge \cdots \wedge e_n^*, whence the proposition.

Corollary

If E is of dimension n, every non-zero (n−1)(n-1)-vector E is pure.

Proposition 16

For an element z≠0z \neq 0 of ⋀p(E)\bigwedge^p(E) to be pure, it is necessary and sufficient that, for all u∗∈⋀p−1(E∗)u^* \in \bigwedge^{p-1}(E^*),

(u∗⊥z)∧z=0. (u^* \perp z) \wedge z = 0.

The case p=0p = 0 is trivial and we assume p≥1p \geq 1. If z=x1∧⋯∧xpz = x_1 \wedge \cdots \wedge x_p, formula (68) (no. 9) with n=p−1n = p - 1 shows that u∗⊥zu^* \perp z is a linear combination of the xix_i (1≤i≤p1 \leq i \leq p), whence (81). If on the other hand the subspace MzM_z associated with zz is of dimension >p> p, consider a basis (ej)1≤j≤n(e_j)_{1 \leq j \leq n} of this subspace with n>pn > p. It follows from no. 11, Proposition 13 that each of the eje_j is of the form u∗⊥zu^* \perp z for some u∗∈⋀p−1(E∗)u^* \in \bigwedge^{p-1}(E^*) and relation (81) therefore implies ej∧z=0e_j \wedge z = 0 for 1≤j≤n1 \leq j \leq n. It follows that in the expression z=∑HaHeHz = \sum_H a_H e_H (where H runs through the set of subsets of {1,n}\{1, n\} with pp elements) all the coefficients aHa_H are zero, whence z=0z = 0, contrary to the hypothesis.

The criterion of Proposition 16 is equivalent to writing conditions (81) when u∗u^* runs through a basis of ⋀p−1(E∗)\bigwedge^{p-1}(E^*). In particular, suppose that E is of finite dimension nn and let (ei)1≤i≤n(e_i)_{1 \leq i \leq n} be a basis of E. Conditions (81) are then equivalent to the conditions

(82−(J,H))(82-(J, H))
⟨eJ∗,(eH∗⊥eI)∧z⟩=0 \langle e_J^*, (e_H^* \perp e_I) \wedge z \rangle = 0
for all subsets J, H of {1,n}\{1, n\} such that Card(J)=p+1\mathrm{Card}(J) = p + 1 and Card(H)=p−1\mathrm{Card}(H) = p - 1. Now, if I and I' are two subsets of {1,n}\{1, n\} with pp elements, formulae (76) of no. 10 and multiplication table (20) of § 7, no. 8 show that

⟨eJ∗,⟨eH∗⊥eI⟩∧eI′⟩=0 \langle e_J^*, \langle e_H^* \perp e_I \rangle \wedge e_{I'} \rangle = 0
unless there exists an i∈{1,n}i \in \{1, n\} such that I−H={i}I - H = \{i\} and J−I′={i}J - I' = \{i\}, in which case

(83)(83)
⟨eJ∗,(eH∗⊥eI)∧eI′⟩=(−1)(p−1)(p−2)/2εi,J,H \langle e_J^*, (e_H^* \perp e_I) \wedge e_{I'} \rangle = (-1)^{(p-1)(p-2)/2} \varepsilon_{i, J, H}
where εi,J,H=ρ{i},Hρ{i},I′\varepsilon_{i, J, H} = \rho_{\{i\}, H} \rho_{\{i\}, I'}; it can then be said that for i∈J∩CHi \in J \cap C H, εi,J,H\varepsilon_{i, J, H} is equal to +1+1 if the number of element of J which are <i< i and the number of elements of H which are <i< i have the same parity, and −1-1 otherwise.

It follows immediately that if we write z=∑IaIeIz = \sum_I a_I e_I, where I runs through the set of subsets of {1,n}\{1, n\} with pp elements, relation (82–(J, H)) is equivalent to the relation

∑i∈J∪CHεi,J,HaJ−{i}aH∪{i}=0. \sum_{i \in J \cup C_H} \varepsilon_{i, J, H} a_{J-\{i\}} a_{H \cup \{i\}} = 0.

Relations (84) are called Grassman’s relations; these are therefore necessary and sufficient conditions (when J describes the set of subsets with p+1p + 1 elements and H the set of subsets with p−1p - 1 elements of {1,n}\{1, n\}) for an element z≠0z \neq 0 of ⋀p(E)\bigwedge^p(E) to be pure.

Note that relations (84) are not independent. For example, for n=4n = 4 and p=2p = 2, Grassmann’s relations reduce to the single relation

a12a34−a13a24+a14a23=0. a_{12} a_{34} - a_{13} a_{24} + a_{14} a_{23} = 0.

Let Dp(E)D_p(E) be the subset of ⋀p(E)\bigwedge^p(E) consisting of the pure pp-vectors; clearly Dp(E)D_p(E) is saturated with respect to the equivalence relation between uu and vv: “there exists λ∈K∗\lambda \in K^* such that v=λuv = \lambda u” and two elements u,vu, v of Dp(E)D_p(E) are equivalent under this relation if and only if the subspaces MuM_u and MvM_v of E which are associated with them are the same. Therefore we thus obtain a canonical bijection of the set of p-dimensional vector subspaces of E onto the image Gp(E)G_p(E) of Dp(E)D_p(E) in the projective space P(⋀p(E))\mathbf{P}(\bigwedge^p(E)) associated with ⋀p(E)\bigwedge^p(E). The subset Gp(E)G_p(E) of P(⋀p(E))\mathbf{P}(\bigwedge^p(E)) is called the Grassmannian of index pp of the vector space E. When E is finite-dimensional and (ei)1≤i≤n(e_i)_{1 \leq i \leq n} is a basis of E, the Grassmannian of index pp is the set of points of P(⋀p(E))\mathbf{P}(\bigwedge^p(E)) for which a system of homogeneous coordinates (aI)(a_I) (relative to the basis (eI)(e_I) of ⋀p(E)\bigwedge^p(E)) satisfies Grassmann’s relations (84).

When E=KnE = K^n, we sometimes write Gn,p(K)G_{n,p}(K) instead of Gp(Kn)G_p(K^n), so that Gn,1(K)=Pn−1(K)G_{n,1}(K) = P_{n-1}(K). The mapping M↦M0M \mapsto M^0, which associates with every pp-dimensional subspace of KnK^n the orthogonal subspace in E∗E^* (identified with KnK^n under the choice of basis dual to the canonical basis of KnK^n) therefore defines a canonical bijection of Gn,p(K)G_{n,p}(K) onto Gn,n−p(K)G_{n,n-p}(K); Proposition 15 shows that this bijection is the restriction to Gn,p(K)G_{n,p}(K) of a canonical isomorphism of the projective space P(⋀p(Kn))\mathbf{P}(\bigwedge^p(K^n)) onto the projective space P(⋀n−p(Kn))\mathbf{P}(\bigwedge^{n-p}(K^n)).

Exercises

See the exercises for § 11.

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