Bourbaki

§ 3. Hermitian forms and quadratic forms

In all that follows in this Chapter, unless expressly stated otherwise, AA denotes a ring and EE a left AA-module. We suppose that AA is endowed with an involutive antiautomorphism JJ, denoted α→α‾\alpha \to \overline{\alpha}; we therefore have (α+β)=α‾+β‾(\alpha + \beta) = \overline{\alpha} + \overline{\beta}, (αβ)=β‾⋅α‾(\alpha \beta) = \overline{\beta} \cdot \overline{\alpha} and α‾=α\overline{\alpha} = \alpha whatever α,β\alpha, \beta in A may be. Unless expressly stated otherwise, the sesquilinear forms considered are right sesquilinear (§ 1, No. 2, def. 4) for this antiautomorphism.

1. Hermitian and ε\varepsilon-hermitian forms.

Definition 1

Let ε\varepsilon be an element of the center of A. A sesquilinear form Φ\Phi on E such that one has Φ(x,y)=εΦ(y,x)‾\Phi(x, y) = \varepsilon \overline{\Phi(y, x)} whatever xx and yy in E may be is called an ε\varepsilon-hermitian form. A 1-hermitian form (resp. (−1)-hermitian) is called hermitian (resp. antihermitian).

When J is the identity (which implies that A is commutative) a hermitian form (resp. antihermitian form) (for J) is nothing other than a symmetric (resp. antisymmetric) bilinear form (Chapter III, § 5, No. 1, def. 2). Recall that an alternating bilinear form (Chapter III, § 5, No. 2, def. 4) is antisymmetric; the converse is true if, in A, the relation 2a=02a = 0 implies a=0a = 0.

The orthogonality relation (§1,n°3§ 1, n° 3) with respect to an ε\varepsilon-hermitian form is obviously symmetric (cf. exerc. 1).

If α\alpha is an invertible element of A, the mapping T:λ→α−1λ‾αT : \lambda \to \alpha^{-1} \overline{\lambda} \alpha is an antiautomorphism of A, and one readily verifies that the form Φα\Phi \alpha is sesquilinear with respect to T. If, moreover, one has α=α‾\alpha = \overline{\alpha}, then T is involutive, and, if Φ\Phi is ε\varepsilon-hermitian, Φα\Phi \alpha is so also; indeed one has

(λT)T=α−1(α−1λα‾)α=α−1α‾λα−1‾α=λ (\lambda^T)^T = \alpha^{-1} (\overline{\alpha^{-1} \lambda \alpha}) \alpha = \alpha^{-1} \overline{\alpha} \lambda \overline{\alpha^{-1}} \alpha = \lambda
Φ(y,x)α=εΦ(x,y)‾α=ε(Φ(x,y)α)T. \Phi(y, x) \alpha = \varepsilon \overline{\Phi(x, y)} \alpha = \varepsilon (\Phi(x, y) \alpha)^T.

In particular, when A is a field, the elements α\alpha of the center of A such that α‾=α\overline{\alpha} = \alpha form a subfield K of A, and the ε\varepsilon-hermitian forms on E (for J) form a vector space over K.

Remark 1

If Φ\Phi is an ε\varepsilon-hermitian form on E, one has Φ(x,y)=εΦ(x,y)‾ε‾\Phi(x, y) = \varepsilon \overline{\Phi(x, y)} \overline{\varepsilon} whatever x,yx, y in E may be. Hence, if Φ\Phi takes invertible values, one has εε‾=1\varepsilon \overline{\varepsilon} = 1. 2) If there exists an invertible element ii of the center of A such that i‾=iε\overline{i} = i \varepsilon, then, for Φ\Phi to be ε\varepsilon-hermitian, it is necessary and sufficient that iΦi \Phi be hermitian.

The mapping (y,x)→Φ(x,y)‾(y, x) \to \overline{\Phi(x, y)} being sesquilinear for J, in order that Φ\Phi be ε\varepsilon-hermitian, it is necessary and sufficient that one have Φ(y,x)=εΦ(x,y)‾\Phi(y, x) = \varepsilon \overline{\Phi(x, y)} when xx and yy run through a system of generators of E. In particular, if E admits a finite basis (ei)1≤i≤n(e_i)_{1 \leq i \leq n}, in order that a sesquilinear form Φ\Phi on E be ε\varepsilon-hermitian, it is necessary and sufficient that its matrix R=(ρij)=(Φ(ei,ej))R = (\rho_{ij}) = (\Phi(e_i, e_j)) satisfy the relations ρji=ερij‾\rho_{ji} = \varepsilon \overline{\rho_{ij}} whatever i,ji, j may be, that is to say ′R=εR‾'R = \varepsilon \overline{R} ; a matrix RR possessing this property is said to be ε\varepsilon-hermitian. When ε=1\varepsilon = 1 (resp. −1-1) one says that RR is hermitian (resp. antihermitian) relative to the antiautomorphism J. When J is the identity (hence A commutative), a hermitian (resp. antihermitian) matrix RR is such that ′R=R'R = R (resp. ′R=−R'R = -R) ; it is then said that RR is a symmetric (resp. antisymmetric) matrix. In order that Φ\Phi be an alternating form, it is necessary and sufficient that its matrix be antisymmetric and, in addition, that the diagonal terms of RR all be zero; a matrix possessing these properties is said to be alternating.

Let Φ\Phi be a sesquilinear form on EE, and let sΦs_\Phi and dΦd_\Phi be the mappings of EE into E∗E^* associated with Φ\Phi on the left and on the right (§1§ 1, n° 6). In order that Φ\Phi be ε\varepsilon-hermitian, it is necessary and sufficient that ⟨x,sΦ(y)⟩=εˉ⟨x,dΦ(y)⟩\langle x, s_\Phi(y) \rangle = \bar{\varepsilon} \langle x, d_\Phi(y) \rangle for all elements x,yx, y of EE, hence that sΦ=εˉdΦs_\Phi = \bar{\varepsilon} d_\Phi, or again that ⟨x,dΦ(y)⟩=ε⟨x,sΦ(y)⟩\langle x, d_\Phi(y) \rangle = \varepsilon \langle x, s_\Phi(y) \rangle, hence that dΦ=εsΦd_\Phi = \varepsilon s_\Phi.

Let Φ\Phi be an ε\varepsilon-hermitian form such that the mapping dΦd_\Phi of EE into E∗E^* associated on the right with Φ\Phi is bijective. For every endomorphism uu of EE one then has

u∗∗=εεˉu. u^{**} = \varepsilon \bar{\varepsilon} u.
Indeed, for all elements xx and yy of EE, one has
Φ(x,u∗∗(y))=Φ(u∗(x),y)=εΦ(y,u∗(x))‾=εΦ(u(y),x)‾=εΦ(x,u(y))εˉ=Φ(x,εεˉu(y)) \begin{align*} \Phi(x, u^{**(y)}) &= \Phi(u^*(x), y) = \varepsilon \overline{\Phi(y, u^*(x))} = \varepsilon \overline{\Phi(u(y), x)} \\ &= \varepsilon \Phi(x, u(y)) \bar{\varepsilon} = \Phi(x, \varepsilon \bar{\varepsilon} u(y)) \end{align*}
hence u∗∗(x)=εεˉu(x)u^{**(x)} = \varepsilon \bar{\varepsilon} u(x) since Φ\Phi is non-degenerate.

Si Φ\Phi est une forme ε\varepsilon-hermitienne telle que les applications sΦs_\Phi et dΦd_\Phi soient bijectives, alors la forme inverse Φ^\widehat{\Phi} de Φ\Phi (§1§ 1, No. 7) est une forme εˉ\bar{\varepsilon}-hermitienne. En effet, en posant s=sΦs = s_\Phi, d=dΦd = d_\Phi pour abréger, on déduit de d=εsd = \varepsilon s que s−1=εˉd−1s^{-1} = \bar{\varepsilon} d^{-1}, ss étant semilinear. Par suite, quels que soient u,vu, v dans EE, on a

Φ^(u,v)=Φ(s−1(u),d−1(v))=εˉΦ(d−1(u),d−1(v)), \widehat{\Phi}(u, v) = \Phi(s^{-1}(u), d^{-1}(v)) = \bar{\varepsilon} \Phi(d^{-1}(u), d^{-1}(v)),
d’où
Φ^(v,u)=εˉεΦ(d−1(u),d−1(v))‾=εˉΦ^(u,v)‾, \widehat{\Phi}(v, u) = \bar{\varepsilon} \varepsilon \overline{\Phi(d^{-1}(u), d^{-1}(v))} = \bar{\varepsilon} \overline{\widehat{\Phi}(u, v)},
puisque, ε\varepsilon est dans le center de AA.

Enfin, lorsque le ring AA est commutative, les prolongements canoniques d’une forme ε\varepsilon-hermitienne Φ\Phi aux puissances tensorielle et extérieure ⨂pE\bigotimes^p E et ∧pE\wedge^p E de EE sont des formes εp\varepsilon^p-hermitiennes, comme il résulte aussitôt des formules (35) et (37) du §1§ 1, No. 9.

2. Modules over a quadratic extension.

Soit KK un commutative ring. On prend pour AA l’extension quadratique A=K(i)A = K(i) avec i2=−1i^2 = -1, et pour JJ l’automorphisme λ + iμ → λ − iμ (λ∈K,μ∈K\lambda \in K, \mu \in K) (chap. II, § 7, No. 7). Si E est un A-module, nous noterons E0E_0 le K-module déduit de E par restriction de l’anneau des scalaires, et par j l’automorphisme x→ixx \to ix de E0E_0; on a évidemment j2=−Ij^2 = -I, où I est le mapping identique de E0E_0. Inversement soit E0E_0 un K-module et soit j un automorphism de E0E_0 tel que j2=−Ij^2 = -I; l’application λ+iμ→λI+μj\lambda + i\mu \to \lambda I + \mu j est évidemment un homomorphism de A dans le ring L(E0)\mathscr{L}(E_0) des endomorphisms de E0E_0; on a donc défini sur E0E_0 une structure de A-module, pour laquelle on a

(2)

(λ+iμ)x=λx+μj(x)(\lambda + i\mu)x = \lambda x + \mu j(x)
(x∈E0,λ∈K,μ∈K).(x \in E_0, \lambda \in K, \mu \in K).

If E′E' is another A-module, E0′E'_0 the K-module underlying E′E', j′j' the automorphism x′→ix′x' \to ix' of E0′E'_0, then the A-linear mappings f of E into E′E' are none other than the K-linear mappings of E0E_0 into E0′E'_0 such that f∘j=j′∘ff \circ j = j' \circ f. In particular, if we denote by E∗E^* and (E0)∗(E_0)^* the respective duals of E and E0E_0, and if f1f_1 and f2f_2 are two mappings of E into K, for the mapping x→f1(x)+if2(x)x \to f_1(x) + if_2(x) of E into A to be A-linear, it is necessary and sufficient that f1f_1 and f2f_2 belong to (E0)∗(E_0)^* and that one has f1∘j+i(f2∘j)=if1−f2f_1 \circ j + i(f_2 \circ j) = if_1 - f_2, that is to say f1=f2∘jf_1 = f_2 \circ j and f1∘j=−f2f_1 \circ j = -f_2. Since j is an automorphism of E0E_0 and since j2=−Ij^2 = -I, these two conditions are equivalent. Eliminating f1f_1 or f2f_2, one sees that the formulas

(3)

f(x)=f1(x)−if1(j(x))f(x) = f_1(x) - if_1(j(x))
(4)
f(x)=f2(j(x))+if2(x)f(x) = f_2(j(x)) + if_2(x)

(x∈E, f∈E∗, f1∈(E0)∗, f2∈(E0)∗)(x \in E,\ f \in E^*,\ f_1 \in (E_0)^*,\ f_2 \in (E_0)^*) establish two one-to-one correspondences between E∗E^* and (E0)∗(E_0)^*.

3. Bilinear forms associated with a Hermitian form.

We suppose here again that the ring A is the quadratic extension A=K(i)A = K(i) (where i2=−1i^2 = -1) of a commutative ring K, and that J is the automorphism λ+iμ→λ−iμ\lambda + i\mu \to \lambda - i\mu of A (λ∈K,μ∈K\lambda \in K, \mu \in K). Let E and E′E' be two A-modules, E0E_0 and E0′E'_0 the K-modules underlying E and E′E', j and j′j' the automorphisms x→ixx \to ix and x′→ix′x' \to ix' of E and E′E' (cf. n° 2). A K-bilinear form ff on E0×E0′E_0 \times E'_0 will be said to be invariant under j and j′j' if one has

(5)

f(j(x),j′(x′))=f(x,x′)f(j(x), j'(x')) = f(x, x')

for x∈E0x \in E_0 and x′∈E0′x' \in E'_0. Replacing xx by j(x)j(x), one sees that this condition is equivalent to

f(x,j′(x′))=−f(j(x),x′) f(x, j'(x')) = - f(j(x), x')

whatever x∈E0x \in E_0 and x′∈E0′x' \in E'_0 may be.

Proposition 1

Let Φ1\Phi_1 (resp. Φ2\Phi_2) be a K-bilinear form on E0×E0′E_0 \times E'_0, invariant under jj and j′j'. The mapping which to Φ1\Phi_1 (resp. Φ2\Phi_2) associates the mapping Φ\Phi of E×E′E \times E' into AA defined by

Φ(x,x′)=Φ1(x,x′)+iΦ1(x,j′(x′)) \Phi(x, x') = \Phi_1(x, x') + i \Phi_1(x, j'(x'))
(resp. Φ(x,x′)=−Φ2(x,j′(x′))+iΦ2(x,x′)\Phi(x, x') = - \Phi_2(x, j'(x')) + i \Phi_2(x, x'))

(x∈E,x′∈E)(x \in E, x' \in E), is an isomorphism of the K-vector space of K-bilinear forms on E0×E0′E_0 \times E'_0 invariant under jj and j′j' onto the K-vector space of sesquilinear forms on E×E′E \times E'. Suppose moreover that E=E′E = E'; for Φ\Phi to be hermitian, it is necessary and sufficient that Φ1\Phi_1 be symmetric (resp. that Φ2\Phi_2 be antisymmetric) (cf. Exercise 4).

Indeed every mapping Φ\Phi of E×E′E \times E' into AA can be written, in one and only one way, in the form Φ=Φ1+iΦ2\Phi = \Phi_1 + i \Phi_2, where Φ1\Phi_1 and Φ2\Phi_2 are mappings of E×E′E \times E' into KK. For the partial mapping x→Φ(x,x′)x \to \Phi(x, x') to be A-linear, it is necessary and sufficient, by the formula (3) (resp. (4)) of No. 2, that Φ1\Phi_1 (resp. Φ2\Phi_2) be K-linear in xx and that one have

Φ(x,x′)=Φ1(x,x′)−iΦ1(j(x),x′) \Phi(x, x') = \Phi_1(x, x') - i \Phi_1(j(x), x')
(resp. Φ(x,x′)=Φ2(j(x),x′)+iΦ2(x,x′)\Phi(x, x') = \Phi_2(j(x), x') + i \Phi_2(x, x')).

Analogously, for Φ‾(x,x′)\overline{\Phi}(x, x') to be A-linear in x′x', it is necessary and sufficient that Φ1\Phi_1 (resp. Φ2\Phi_2) be K-linear in x′x' and that one have

Φ(x,x′)=Φ1(x,x′)+iΦ1(x,j′(x′)) \Phi(x, x') = \Phi_1(x, x') + i \Phi_1(x, j'(x'))
(resp. Φ(x,x′)=−Φ2(x,j′(x′))+iΦ2(x,x′)\Phi(x, x') = - \Phi_2(x, j'(x')) + i \Phi_2(x, x')).

It follows immediately that, for Φ\Phi to be sesquilinear, it is necessary and sufficient that it be written in one or the other of the forms (9) and (11) (resp. (10) and (12)) with Φ1\Phi_1 (resp. Φ2\Phi_2) a K-bilinear form invariant under jj and j′j'.

It follows from this that, for a sesquilinear form Φ=Φ1+iΦ2\Phi = \Phi_1 + i \Phi_2 to be zero, it is necessary and sufficient that Φ1\Phi_1 (resp. Φ2\Phi_2) be zero. Now, if E=E′E = E', one has Φ(y,x)=Φ1(y,x)+iΦ2(y,x)\Phi(y, x) = \Phi_1(y, x) + i \Phi_2(y, x) and Φ(x,y)‾=Φ1(x,y)−iΦ2(x,y)\overline{\Phi(x, y)} = \Phi_1(x, y) - i \Phi_2(x, y); for these two expressions to be equal, in other words for Φ\Phi to be hermitian, it is necessary and sufficient therefore that Φ1\Phi_1 be symmetric (resp. that Φ2\Phi_2 be antisymmetric).

Remark 1

The formulas (7) and (8) show that, if x∈Ex \in E, in order that Φ(x,x′)=0\Phi(x, x') = 0 for all x′∈E′x' \in E', it is necessary and sufficient that Φ1(x,x′)=0\Phi_1(x, x') = 0 (resp. Φ2(x,x′)=0\Phi_2(x, x') = 0) for all x′∈E′x' \in E'. 2) The adjoint of an endomorphism uu of EE with respect to Φ\Phi (§1§ 1, n° 8) is the same as the adjoint of uu (considered as an endomorphism of E0E_0) with respect to Φ1\Phi_1 (resp. Φ2\Phi_2).

4. Quadratic forms.

Definition 2

We suppose that the ring AA is commutative. We say that a mapping QQ of EE into AA is a quadratic form on EE if 1) Q(αx)=α2Q(x)Q(\alpha x) = \alpha^2 Q(x) for α∈A\alpha \in A and x∈Ex \in E; 2) the mapping Φ:(x,y)→Q(x+y)−Q(x)−Q(y)\Phi : (x, y) \to Q(x + y) - Q(x) - Q(y) of E×EE \times E into AA is a bilinear form. The bilinear form Φ\Phi (which is necessarily symmetric) is called the bilinear form associated with QQ. If Φ\Phi is non-degenerate, we say that QQ is non-degenerate.

Since Q(2x)=4Q(x)Q(2x) = 4Q(x), it follows at once from 2) that

Φ(x,x)=2Q(x). \Phi(x, x) = 2Q(x).
In particular, if AA is a ring of characteristic 2, the form Φ\Phi is alternating.

We shall say that two elements (resp. two subsets) of EE are orthogonal relative to QQ if they are orthogonal relative to the bilinear form associated with Φ\Phi.

Let (xi)i∈I(x_i)_{i \in I} be a family of elements of EE and (ai)i∈I(a_i)_{i \in I} a family of elements of AA all but a finite number of which are zero. By induction on the number of indices ii for which ai≠0a_i \neq 0, one easily shows that

Q(∑iaixi)=∑iai2Q(xi)+∑{i,j}aiajΦ(xi,xj), Q(\sum_i a_i x_i) = \sum_i a_i^2 Q(x_i) + \sum_{\{i, j\}} a_i a_j \Phi(x_i, x_j),

the last summation being extended over the two-element subsets of I.

For every bilinear form ff on E×EE \times E, we define a quadratic form QQ by putting Q(x)=f(x,x)Q(x) = f(x, x); the bilinear form Φ\Phi associated with QQ is then defined by Φ(x,y)=f(x,y)+f(y,x)\Phi(x, y) = f(x, y) + f(y, x) for x,yx, y in EE. Moreover, if one supposes that the scalar 2 has an inverse 12\frac{1}{2} in AA, there exists one and only one symmetric bilinear form ff such that Q(x)=f(x,x)Q(x) = f(x, x), namely f=12Φf = \frac{1}{2} \Phi; the discriminant of ff with respect to a system S=(x1,…,xn)S = (x_1, \ldots, x_n) is also called the discriminant of QQ with respect to SS. There is therefore in this case a one-to-one correspondence between the quadratic forms and the symmetric bilinear forms on EE (cf. exerc. 6).

In the case of a free module, we have in addition the following result:

Proposition 2

Suppose that AA is commutative and that EE admits a basis (ei)i∈I(e_i)_{i \in I}. Then, for every quadratic form QQ on EE, there exists a bilinear form ff on E×EE \times E such that Q(x)=f(x,x)Q(x) = f(x, x) for every x∈Ex \in E. For every family (bij)(i,j)∈I×I(b_{ij})_{(i,j) \in I \times I} of scalars such that bij=bjib_{ij} = b_{ji} for (i,j)∈I×I(i, j) \in I \times I, there exists one and only one quadratic form QQ such that

Q(ei)=bii,Φ(ei,ej)=bij pour i≠j, Q(e_i) = b_{ii}, \quad \Phi(e_i, e_j) = b_{ij} \text{ pour } i \neq j,

where Φ\Phi denotes the bilinear form associated with QQ; then QQ is given by the formula

Q(∑iaiei)=∑{i,j}bijaiaj, Q(\sum_i a_i e_i) = \sum_{\{i,j\}} b_{ij} a_i a_j,

the last summation extending over the subsets {i,j}\{i, j\} of II having one or two elements.

En effet, comme the formula (16) is only a transcription of formula (14), the uniqueness of a quadratic form QQ satisfying (15) is proved. To prove its existence, let us first remark that there exists a family (bij′)(b'_{ij}) of elements of AA such that bii′=biib'_{ii} = b_{ii} and that bij′+bji′=bijb'_{ij} + b'_{ji} = b_{ij} for i≠ji \neq j; one obtains, for example, such a family by endowing II with an ordered set structure (Theory of Sets, Chapter III, § 2, No. 3, Theorem 1) and by setting bij′=bijb'_{ij} = b_{ij} for i<ji < j and bij′=0b'_{ij} = 0 for i>ji > j. Since the eie_i form a basis of EE, there exists a bilinear form ff on E×EE \times E such that f(ei,ej)=bij′f(e_i, e_j) = b'_{ij}; by setting Q′(x)=f(x,x)Q'(x) = f(x, x) and denoting by Φ′\Phi' the bilinear form associated with the quadratic form Q′Q', one obtains Q′(ei)=biiQ'(e_i) = b_{ii} and Φ′(ei,ej)=f(ei,ej)+f(ej,ei)=bij\Phi'(e_i, e_j) = f(e_i, e_j) + f(e_j, e_i) = b_{ij}. This proves our second assertion. As for the first, it follows immediately, since, by virtue of the uniqueness, if a quadratic form QQ satisfies (15), one has Q(x)=Q′(x)=f(x,x)Q(x) = Q'(x) = f(x, x).

The module EE endowed with the structure defined by a quadratic form QQ is called a quadratic module. A homomorphism of the quadratic module (E,Q)(E, Q) into a quadratic module (E′,Q′)(E', Q') is a linear mapping uu of EE into E′E' such that Q=Q′∘uQ = Q' \circ u; if Φ\Phi and Φ′\Phi' are the bilinear forms associated with QQ and Q′Q', one then has Φ(x,y)=Φ′(u(x),u(y))\Phi(x, y) = \Phi'(u(x), u(y)) for x∈E, y∈Ex \in E,\ y \in E; in other words Φ′\Phi' is the inverse image of Φ\Phi by uu (§ 1, No. 1). One says that two quadratic forms QQ and Q′Q' on two AA-modules EE and E′E' are equivalent if the corresponding quadratic modules are isomorphic.

Let (Ei,Qi)i∈I(E_i, Q_i)_{i \in I} be a family of quadratic modules, and let EE be the direct sum of the modules EiE_i. The external direct sum of the quadratic modules (Ei,Qi)(E_i, Q_i) is the quadratic module obtained by endowing EE with the quadratic form QQ defined by Q(∑ixi)=∑iQi(xi)Q(\sum_i x_i) = \sum_i Q_i(x_i) for xi∈Eix_i \in E_i. One also says that the quadratic form QQ is the external direct sum of the quadratic forms QiQ_i.

If the forms QiQ_i are non-degenerate, the same is true of QQ.

Let QQ be a quadratic form on the AA-module EE; if FF is a submodule of EE and if QQ is constant on each class modulo FF, the mapping Q‾\overline{Q} of E/FE/F into AA deduced from QQ by passing to the quotient is obviously a quadratic form, and the canonical mapping of EE onto E/FE/F is a homomorphism for the structures of quadratic modules. For QQ to be constant on each class modulo FF, it is necessary and sufficient that we have Q(x+y)=Q(x)Q(x + y) = Q(x) for x∈Ex \in E and y∈Fy \in F, that is, denoting by Φ\Phi the bilinear form associated with QQ, that we have Q(y)+Φ(x,y)=0Q(y) + \Phi(x, y) = 0 for y∈Fy \in F and x∈Ex \in E. Taking x=0x = 0, we see that we have Q(y)=0Q(y) = 0 for y∈Fy \in F, and therefore

Φ(x,y)=0\Phi(x, y) = 0 for x∈Ex \in E and y∈Fy \in F. In other words, if we call the kernel of the quadratic module (E,Q)(E, Q) the set NN of elements xx of EE such that Q(x)=0Q(x) = 0 and Φ(x,z)=0\Phi(x, z) = 0 for all z∈Ez \in E, for QQ to be constant on each class modulo FF, it is necessary and sufficient that FF be contained in the kernel NN of (E,Q)(E, Q). It is readily verified that NN is a submodule of EE. For QQ to be constant on each class modulo FF, it is therefore necessary and sufficient that FF be generated by elements of NN.

It is immediately seen that the kernel of the quadratic module ∣E/N|E/N is {0}\{0\}.

Proposition 3

Let hh be a homomorphism of AA into a commutative ring A′A'. For every quadratic form QQ on the AA-module EE, there exists one and only one quadratic form Q′Q' on the A′A'-module A′⊗AEA' \otimes_A E (chap. III, 2nd ed., App. II, No. 10) such that one has*

Q′(1⊗x)=h(Q(x)) Q'(1 \otimes x) = h(Q(x))
for every x∈Ex \in E. *Moreover the bilinear form Φ′\Phi' associated with Q′Q' is obtained by extension of the ring of scalars from the bilinear form Φ\Phi associated with QQ.

We first prove that, if there exists a quadratic form Q′Q' satisfying (17), it is unique and the bilinear form Φ′\Phi' associated with Q′Q' is obtained by extension of the ring of scalars from the form Φ\Phi associated with QQ. Indeed this last assertion follows from the fact that one has

Φ′(1⊗x,1⊗y)=Q′(1⊗x+1⊗y)−Q′(1⊗x)−Q′(1⊗y)=h(Φ(x,y)) \Phi'(1 \otimes x, 1 \otimes y) = Q'(1 \otimes x + 1 \otimes y) - Q'(1 \otimes x) - Q'(1 \otimes y) = h(\Phi(x, y))
for x∈E,y∈Ex \in E, y \in E. The formula (14) then shows that one has
Q′(∑iai′⊗xi)=∑iai′2h(Q(xi))+∑{i,j}ai′aj′h(Φ(xi,xj)) Q'(\sum_i a'_i \otimes x_i) = \sum_i a'_i{}^2 h(Q(x_i)) + \sum_{\{i, j\}} a'_i a'_j h(\Phi(x_i, x_j))
for ai′∈A′a'_i \in A' and xi∈Ex_i \in E, which proves the uniqueness of Q′Q'.

To prove the existence of Q′Q', we shall first suppose that the module EE admits a basis (ei)i∈I(e_i)_{i \in I}. There then exist elements bijb_{ij} of AA such that bij=bjib_{ij} = b_{ji} and that Q(∑iaiei)=∑{i,j}bijaiajQ(\sum_i a_i e_i) = \sum_{\{i, j\}} b_{ij} a_i a_j for ai∈Aa_i \in A (prop. 2). Since the elements 1⊗Aei1 \otimes_A e_i form a basis of the

A'-module A′⊗AEA' \otimes_A E, we define a quadratic form Q′Q' on this latter module by putting

Q′(∑iai′⊗ei)=∑{i,j}ai′aj′h(bij) Q'(\sum_i a'_i \otimes e_i) = \sum_{\{i,j\}} a'_i a'_j h(b_{ij})
for ai′∈A′a'_i \in A'; whence, for x=∑iaiei∈Ex = \sum_i a_i e_i \in E
Q′(1⊗x)=Q′(∑ih(ai)⊗ei)=∑{i,j}h(ai)h(aj)h(bij)=h(Q(x)), Q'(1 \otimes x) = Q'(\sum_i h(a_i) \otimes e_i) = \sum_{\{i,j\}} h(a_i) h(a_j) h(b_{ij}) = h(Q(x)),
which proves the existence of Q′Q' in this case.

Let us now pass to the general case. Let (xi)i∈I(x_i)_{i \in I} be a system of generators of EE, A(t)A^{(t)} the module of formal linear combinations of elements of II (Chap. II, § 1, No. 8), and (ei)i∈I(e_i)_{i \in I} the canonical basis of A(t)A^{(t)}. The linear mapping uu of A(t)A^{(t)} into EE defined by u(ei)=xiu(e_i) = x_i is surjective since the elements xix_i generate EE. It follows (Chap. III, 2nd ed., App. II, No. 5, Prop. 4) that the mapping 1⊗u1 \otimes u of A′⊗A(t)A' \otimes A^{(t)} into A′⊗EA' \otimes E is surjective, and that its kernel P′P' is generated by the elements of the form 1⊗p1 \otimes p with u(p)=0u(p) = 0. Let then Q1′Q'_1 be the extension to A′⊗AA(t)A' \otimes_A A^{(t)} of the quadratic form Q1=Q∘uQ_1 = Q \circ u on A(t)A^{(t)}. If pp is an element of A(t)A^{(t)} such that u(p)=0u(p) = 0, we have Q1′(1⊗p)=h(Q1(p))=0Q'_1(1 \otimes p) = h(Q_1(p)) = 0 and (denoting by Φ1′\Phi'_1 the bilinear form associated with Q1′Q'_1) Φ1′(1⊗p,1⊗x)=h(Φ(u(p),u(x)))=0\Phi'_1(1 \otimes p, 1 \otimes x) = h(\Phi(u(p), u(x))) = 0 for all x∈A(t)x \in A^{(t)}. Thus, if u(p)=0u(p) = 0 (p∈A(t)p \in A^{(t)}), then 1⊗p1 \otimes p belongs to the kernel of the quadratic module A′⊗AA(t)A' \otimes_A A^{(t)}, and there exists consequently, as we have seen above, a quadratic form Q′Q' on A′⊗AEA' \otimes_A E such that Q1′=Q′∘(1⊗u)Q'_1 = Q' \circ (1 \otimes u). Since uu is surjective, we see that Q′Q' satisfies condition (17). Q.E.D.

The quadratic form Q′Q', whose existence and uniqueness are assured by Prop. 3, is called the extension of QQ to A′⊗AEA' \otimes_A E (with respect to hh). One also says that Q′Q' is obtained from QQ by extension of the ring of scalars.

Exercises. — 1) Let AA be a field, EE a left vector space over AA, Φ\Phi a sesquilinear form on EE (for an antiautomorphism JJ of AA). Assume that the rank (finite or infinite) of Φ\Phi is ⩾2\geqslant 2, and that the relations Φ(x,y)=0\Phi(x, y) = 0 and Φ(y,x)=0\Phi(y, x) = 0 are equivalent. a) Now prove that there exists λ≠0\lambda \neq 0 in AA such that one has Φ(y,x)=λ(Φ(x,y))J\Phi(y, x) = \lambda (\Phi(x, y))^J. (Use exerc. 8 of § 1). b) Now prove that there exists α∈A\alpha \in A such that the sesquilinear form Φα\Phi \alpha (for the antiautomorphism ξ→α−1ξJα\xi \to \alpha^{-1} \xi^J \alpha) is hermitian or alternating.

(First note that one has ξJ2=λ−1ξλ−J\xi^{J^2} = \lambda^{-1} \xi \lambda^{-J} and λλJ=λJλ=1\lambda \lambda^J = \lambda^J \lambda = 1. Then distinguish two cases according as ξ+ξJλ−1=0\xi + \xi^J \lambda^{-1} = 0 for every ξ∈A\xi \in A or not; in the second case, prove that every element ≠0\neq 0 of the form α=ξ+ξJλ−1\alpha = \xi + \xi^J \lambda^{-1} answers the question).

2) Let Φ\Phi be an ε\varepsilon-hermitian sesquilinear form on a finite-dimensional vector space EE over a field AA.

a) Now prove that for every vector subspace MM of EE, one has (M0)0=M+E0(M^0)^0 = M + E^0 and dim⁡M0+dim⁡M=dim⁡E+dim⁡(M∩E0)\dim M^0 + \dim M = \dim E + \dim (M \cap E^0).

b) If M1,M2M_1, M_2 are two vector subspaces of EE, now prove that one has dim⁡(M1∩M20)+dim⁡(M2+M10)=dim⁡E+dim⁡(M1∩E0)\dim (M_1 \cap M_2^0) + \dim (M_2 + M_1^0) = \dim E + \dim (M_1 \cap E^0) (consider the canonical mapping of EE onto E/E0E/E^0).

3) Let KK be a commutative ring, ff a monic polynomial of K[X]K[X], of degree n⩾1n \geqslant 1; let AA be the quotient algebra K[X]/(f)K[X]/(f) admitting as basis over KK the elements 1,ξ,ξ2,…,ξn−11, \xi, \xi^2, \ldots, \xi^{n-1} (chap. IV, § 1, no 5, prop. 4). Now prove that the datum of an AA-module EE is equivalent to the datum of a KK-module E0E_0 and of a KK-endomorphism jj of E0E_0 such that f(j)=0f(j) = 0. For every u∈E∗u \in E^*, one sets u(x)=∑k=0n−1uk(x)ξku(x) = \sum_{k=0}^{n-1} u_k(x) \xi^k; prove that if α0=f(0)\alpha_0 = f(0) is invertible in KK, the mapping u→u0u \to u_0 is a KK-isomorphism of E∗E^* onto (E0)∗(E_0)^*, whose inverse isomorphism is to be made explicit.

¶ 4) a) Let AA be a ring (commutative or not), σ\sigma an automorphism of AA such that there exists an invertible element γ∈A\gamma \in A satisfying γσ=γ\gamma^\sigma = \gamma, and such that ξσ2=γξγ−1\xi^{\sigma^2} = \gamma \xi \gamma^{-1} for all ξ∈A\xi \in A. Let BB be a left AA-module having a basis of two elements (e1,e2)(e_1, e_2); now prove that a ring structure is defined on BB by taking as multiplication in BB the law of composition

(ξe1+ηe2)(ξ′e1+η′e2)=(ξξ′+ηη′γ)e1+(ηξ′σ+ξη′)e2. (\xi e_1 + \eta e_2)(\xi' e_1 + \eta' e_2) = (\xi \xi' + \eta \eta' \gamma) e_1 + (\eta {\xi'}^\sigma + \xi \eta') e_2.

For this ring structure, e1e_1 is the unit element (which we identify with the unit element 1 of AA); if we put e2=ρe_2 = \rho, we have ρ2=γ\rho^2 = \gamma and ρξ=ξσρ\rho \xi = \xi^\sigma \rho for all ξ∈A\xi \in A; moreover, BB is a right AA-module, of which 1 and ρ\rho form a basis. If AA is a field, a necessary and sufficient condition for BB to be a field is that γ\gamma not be of the form λσλ\lambda^\sigma \lambda (where λ∈A\lambda \in A). (Cf. Chapter VIII, § 12, exerc. 8).

b) Let JJ be an involutory antiautomorphism of AA. Suppose that there exists an invertible element δ∈A\delta \in A satisfying the following conditions:

(1) δJ=δ,δσδ=γγJ,(ξJ)σ=δ(ξσ)Jδ−1\delta^J = \delta, \quad \delta^\sigma \delta = \gamma \gamma^J, \quad (\xi^J)^\sigma = \delta (\xi^\sigma)^J \delta^{-1} for all ξ∈A\xi \in A.

Now prove that JJ can be extended to an involutory antiautomorphism of BB (again denoted by JJ) by putting

(2)

(ξ+ηρ)J=ξJ+γ−1δσ(ηJ)σρ. (\xi + \eta \rho)^J = \xi^J + \gamma^{-1} \delta^\sigma (\eta^J)^\sigma \rho.

If, moreover, AA and BB are fields and if σ\sigma is not an inner automorphism, now prove that the conditions (1) are necessary for the existence of an extension of JJ to an involutory antiautomorphism of BB (putting ρJ=α+βρ\rho^J = \alpha + \beta \rho, with α,β\alpha, \beta in AA, now prove that necessarily α=0\alpha = 0, by writing the condition (ρξ)J=ξJρJ(\rho \xi)^J = \xi^J \rho^J for all ξ∈A\xi \in A).

c) Suppose the conditions (1) are satisfied and the involutive antiautomorphism J extended to B by (2). Let F be a unitary B-module, E the unitary A-module deduced from F by restriction to A of the ring of scalars; the mapping j:x→ρxj : x \to \rho x is then a bijective semilinear mapping of E onto itself, relative to the automorphism σ\sigma of A and such that j2(x)=γxj^2(x) = \gamma x. Let Φ\Phi be a hermitian form on F (for J); for x∈Ex \in E, y∈Ey \in E, put Φ(x,y)=Φ1(x,y)+Φ2(x,y)ρ\Phi(x, y) = \Phi_1(x, y) + \Phi_2(x, y)\rho, where Φ1(x,y)∈A\Phi_1(x, y) \in A, Φ2(x,y)∈A\Phi_2(x, y) \in A. Now prove that Φ1\Phi_1 is a hermitian form on E (for J), such that

Φ1(j(x),j(y))=(Φ1(x,y))σδ; \Phi_1(j(x), j(y)) = (\Phi_1(x, y))^{\sigma \delta};
we have Φ2(x,y)=Φ1(x,j(y))δ−1\Phi_2(x, y) = \Phi_1(x, j(y))\delta^{-1}, Φ2\Phi_2 is a sesquilinear form on E for the antiautomorphism (in general non-involutive) ξ→(ξJ)σ\xi \to (\xi^J)^{\sigma}, such that
Φ2(j(x),j(y))=(Φ2(x,y))σδσ \Phi_2(j(x), j(y)) = (\Phi_2(x, y))^{\sigma \delta^{\sigma}}
and
Φ2(y,x)=γJδ−1((Φ2(x,y))J)σ. \Phi_2(y, x) = \gamma^J \delta^{-1}((\Phi_2(x, y))^J)^{\sigma}.

Conversely. In order that Φ\Phi be non-degenerate, it is necessary and sufficient that Φ1\Phi_1 or Φ2\Phi_2 be non-degenerate. Special case where B is a quaternion algebra over a commutative ring K, corresponding to a pair (α,β)(\alpha, \beta) of elements of K, β\beta being invertible, A the subalgebra K+KuK + Ku of B, and J and σ\sigma the mapping ξ→ξˉ\xi \to \bar{\xi} (chap. II, § 7, no 8).

d) Let uu be an automorphism of the A-module E. In order that uu be an automorphism of the B-module F, leaving the form Φ\Phi invariant, it is necessary and sufficient that uu satisfy any two of the following three conditions: 1° uu leaves Φ1\Phi_1 invariant; 2° uu leaves Φ2\Phi_2 invariant; 3° uu commutes with jj.

5) Let AA be a commutative ring, EE an AA-module, (xi)i∈I(x_i)_{i \in I} a system of generators of EE; let RR be the submodule of the module A(1)A^{(1)} formed by the elements (yi)i∈I(y_i)_{i \in I} such that ∑iyixi=0\sum_i y_i x_i = 0, and let (aλ)λ∈L(a_{\lambda})_{\lambda \in L} be a system of generators of RR (with aλ=(aλi)i∈Ia_{\lambda} = (a_{\lambda i})_{i \in I}). Let (bij)(b_{ij}) be a family of elements of AA (i∈I,j∈I)(i \in I, j \in I). In order that there exist a quadratic form QQ such that Q(xi)=biiQ(x_i) = b_{ii} and Φ(xi,xj)=bij\Phi(x_i, x_j) = b_{ij} for i≠ji \neq j (Φ\Phi denoting the bilinear form associated with QQ), it is necessary and sufficient that bij=bjib_{ij} = b_{ji} whatever i,ji, j in II, and that, whatever λ∈L\lambda \in L and i∈Ii \in I, one has

∑{i,j}bijaλiaλj=∑j≠ibijaλj+2biiaλi=0; \sum_{\{i, j\}} b_{ij} a_{\lambda i} a_{\lambda j} = \sum_{j \neq i} b_{ij} a_{\lambda j} + 2b_{ii} a_{\lambda i} = 0;
one then has Q(∑aixi)=∑{i,j}bijaiajQ(\sum a_i x_i) = \sum_{\{i, j\}} b_{ij} a_i a_j. Deduce a new proof of Proposition 3 of No. 4. (Notice that the xi′=1⊗xix'_i = 1 \otimes x_i form a system of generators of A′⊗AEA' \otimes_A E, and that the a-module A′⊗AEA' \otimes_A E is isomorphic to A′(1)/R′{A'}^{(1)}/R', where A′(1){A'}^{(1)} is identified with A′⊗AA(1)A' \otimes_A A^{(1)} and R′R' is generated by the image of R by the canonical mapping of A(1)A^{(1)} into A′(1){A'}^{(1)}.

6) Let AA be a commutative ring of characteristic 2, EE a free AA-module, A\mathscr{A} (resp. S\mathscr{S}, Q\mathscr{Q}) the AA-module of alternating bilinear forms (resp. symmetric bilinear forms, quadratic forms) on EE. One has A⊂S\mathscr{A} \subset \mathscr{S}; one defines in addition a linear mapping ω\omega of S\mathscr{S} into Q\mathscr{Q}, and a linear mapping θ\theta of Q\mathscr{Q} into A\mathscr{A} as follows: for every bilinear form Φ∈S\Phi \in \mathscr{S}, ω(Φ)\omega(\Phi) is the quadratic form x→Φ(x,x)x \to \Phi(x, x), and for every quadratic form Q∈QQ \in \mathscr{Q}, θ(Q)\theta(Q) is the bilinear form associated with QQ, which is alternating. Show that ω(0)=A\omega(0) = \mathscr{A}, θ(Q)=A\theta(\mathscr{Q}) = \mathscr{A} and θ(0)=ω(S)\theta(0) = \omega(\mathscr{S}).

¶ 7) Let AA be a commutative ring, E,FE, F two AA-modules. A mapping QQ of EE into FF is said to be quadratic if it satisfies the following conditions: 1∘1^\circ Q(αx)=α2Q(x)Q(\alpha x) = \alpha^2 Q(x) for α∈A,x∈E\alpha \in A, x \in E; 2∘2^\circ the mapping (x,y)→Q(x+y)−Q(x)−Q(y)(x, y) \to Q(x + y) - Q(x) - Q(y) of E×EE \times E into FF is bilinear. If ff is a linear mapping of an AA-module E1E_1 into EE, Q∘fQ \circ f is a quadratic mapping of E1E_1 into FF.

a) Let EE be an AA-module, A(E)A^{(E)} the module of formal linear combinations of the elements of EE with coefficients in AA (chap. II, § 1, no 8), and for every x∈Ex \in E, let εx\varepsilon_x be the corresponding element of the canonical basis of A(E)A^{(E)}. Let Γ2(E)\Gamma^2(E) be the quotient of A(E)×(E⊗AE)A^{(E)} \times (E \otimes_A E) by the submodule RR generated by the elements (εx+y−εx−εy,−x⊗y)(\varepsilon_{x+y} - \varepsilon_x - \varepsilon_y, -x \otimes y) and (ελx−λ2εx,0)(\varepsilon_{\lambda x} - \lambda^2 \varepsilon_x, 0), for x∈E,y∈E,λ∈Ax \in E, y \in E, \lambda \in A. For every x∈Ex \in E, put γ(x)=φ(εx,0)\gamma(x) = \varphi(\varepsilon_x, 0), denoting by φ\varphi the canonical mapping of A(E)×(E⊗E)A^{(E)} \times (E \otimes E) onto Γ2(E)\Gamma^2(E); γ\gamma is called the canonical mapping of EE into Γ2(E)\Gamma^2(E). Prove that γ\gamma is a quadratic mapping of EE into Γ2(E)\Gamma^2(E) and that, for every quadratic mapping QQ of EE into an AA-module FF, there exists one and only one linear mapping qq of Γ2(E)\Gamma^2(E) into FF such that Q=q∘γQ = q \circ \gamma (in other words, (Γ2(E),γ)(\Gamma^2(E), \gamma) is a solution of a universal mapping problem; cf. Ens., chap. IV, § 3).

Pour every couple of AA-modules E,E′E, E' and every linear mapping ff of EE into E′E', now prove that, if γ′\gamma' denotes the canonical mapping of E′E' into Γ2(E′)\Gamma^2(E'), there exists one and only one linear mapping fˉ\bar{f} of Γ2(E)\Gamma^2(E) into Γ2(E′)\Gamma^2(E') such that γ′∘f=fˉ∘γ\gamma' \circ f = \bar{f} \circ \gamma.

b) Suppose that EE is direct sum of two submodules M,NM, N. Define a canonical isomorphism of Γ2(E)\Gamma^2(E) onto the direct sum of the modules Γ2(M),Γ2(N)\Gamma^2(M), \Gamma^2(N) and M⊗NM \otimes N (show that this direct sum is solution of the same universal mapping problem as Γ2(E)\Gamma^2(E)).

c) Let FF be a submodule of EE, jj the canonical injection of FF into EE. Define a canonical isomorphism of Γ2(E/F)\Gamma^2(E/F) onto

Γ2(E)/(jˉ(Γ2(F))+ψ(E×F)), \Gamma^2(E)/(\bar{j}(\Gamma^2(F)) + \psi(E \times F)),

where ψ(x,y)=φ(0,x⊗j(y))\psi(x, y) = \varphi(0, x \otimes j(y)) for x∈E,y∈Fx \in E, y \in F. (Same method).

d) Let A′A' be a commutative ring, hh a homomorphism of AA into A′A'. Define a canonical isomorphism of Γ2(A′⊗AE)\Gamma^2(A' \otimes_A E) onto A′⊗AΓ2(E)A' \otimes_A \Gamma^2(E) (same method).

e) There exists one and only one linear mapping ss of Γ2(E)\Gamma^2(E) into E⊗EE \otimes E such that s(γ(x))=x⊗xs(\gamma(x)) = x \otimes x for all x∈Ex \in E; show that if EE is a free module, s is an isomorphism onto the submodule of symmetric tensors of order 2 on E.

f) Suppose that A=ZA = \mathbf{Z} and that E is a finite cyclic group of order n. Show that Γ2(E)\Gamma^2(E) is a cyclic group of order n if n is odd, of order 2n2n if n is even. (First remark that if a is a generator of E, γ(a)\gamma(a) is a generator of Γ2(E)\Gamma^2(E), and that γ(−ha)=γ(ha)\gamma(-ha) = \gamma(ha) for every integer h; deduce from this that if n is odd, nγ(a)=0n\gamma(a) = 0 by taking h=(n−1)/2h = (n-1)/2; show in the same way that 2nγ(a)=02n\gamma(a) = 0 if n is even. Finally prove that if n is odd (resp. even), there exists a quadratic mapping Q of E into a cyclic group of order n (resp. 2n2n) applying a to a generator of this group).

8) Let A be a commutative field, E, F two vector spaces over A. Let g be a mapping of E into F, such that there exist three mappings a,b,ca, b, c of E×EE \times E into F, satisfying the identity

g(λx+μy)=λ2a(x,y)+λμb(x,y)+μ2c(x,y) g(\lambda x + \mu y) = \lambda^2 a(x, y) + \lambda \mu b(x, y) + \mu^2 c(x, y)

whatever x,yx, y in E, λ,μ\lambda, \mu in A.

a) Show that one has a(x,y)=g(x),c(x,y)=g(y),b(y,x)=b(x,y)a(x, y) = g(x), c(x, y) = g(y), b(y, x) = b(x, y) and b(λx,y)=λb(x,y)b(\lambda x, y) = \lambda b(x, y); moreover, if one sets

d(x,y,z)=b(x+y,z)−b(x,z)−b(y,z) d(x, y, z) = b(x + y, z) - b(x, z) - b(y, z)

show that one has d(x,y,z)=d(y,z,x)=d(z,x,y)d(x, y, z) = d(y, z, x) = d(z, x, y) and conclude that d(λx,μy,vz)=λμvd(x,y,z)d(\lambda x, \mu y, v z) = \lambda \mu v d(x, y, z).

b) Deduce from a) that if A≠F2A \neq \mathbf{F}_2, one necessarily has d(x,y,z)=0d(x, y, z) = 0 and consequently that g is a quadratic mapping (Exercise 7). On the contrary, if A=F2A = \mathbf{F}_2 and if dim E ⩾3\geqslant 3, show that there exist mappings g of E into A, satisfying (4) and for which d(x,y,z)d(x, y, z) is not identically zero.

9) Let A be a commutative ring, E an A-module having a basis of n elements, Φ\Phi a symmetric bilinear form on E. Let e be an element of ⋀nE\bigwedge^n E forming a basis of this module, Δ\Delta the discriminant of Φ\Phi with respect to e, φp\varphi_p the canonical isomorphism of ⋀pE\bigwedge^p E onto ⋀n−pE∗\bigwedge^{n-p} E^* relative to e (Chapter III, § 8, No. 5). For x∈⋀pEx \in \bigwedge^p E, let d(p)(x)=φn−p−1(dΦ(p)(x))d_{(p)}(x) = \varphi_{n-p}^{-1}(d_{\Phi_{(p)}}(x)); show that the mapping d(p)d_{(p)} of ⋀pE\bigwedge^p E into ⋀n−pE\bigwedge^{n-p} E has the following properties:

a) For every x∈⋀pEx \in \bigwedge^p E, d(n−p)(d(p)(x))=(−1)p(n−p)Δxd_{(n-p)}(d_{(p)}(x)) = (-1)^{p(n-p)} \Delta x.

b) For every pair of elements x,yx, y of ⋀pE\bigwedge^p E, one has

x∧d(p)(y)=Φ(p)(x,y)eandΦ(n−p)(d(p)(x),d(p)(y))=ΔΦ(p)(x,y). x \wedge d_{(p)}(y) = \Phi_{(p)}(x, y)e \quad \text{and} \quad \Phi_{(n-p)}(d_{(p)}(x), d_{(p)}(y)) = \Delta \Phi_{(p)}(x, y).

c) Suppose in addition that A is a field and that Φ\Phi is non-degenerate. Then, if x is a decomposable p-vector ≠0\neq 0 corresponding to a subspace F of E (Chapter III, § 7, No. 3), d(p)(x)d_{(p)}(x) is a decomposable (n−p)(n-p)-vector ≠0\neq 0 corresponding to the subspace F0F^0 orthogonal to F.

d) Extend the preceding results to the case where (A being a commutative ring), Φ is an ε-hermitian sesquilinear form for an involutive automorphism J ≠ 1 of A.

10) a) Let A be a commutative ring, E an A-module having a basis of 3 elements, Φ a symmetric bilinear form on E. With the notation of Exercise 9, for two arbitrary elements x, y of E, put x∧‾y=d(2)(x∧y)x \overline{\wedge} y = d_{(2)}(x \wedge y), and say that this element is the vector product of x and y (relative to Φ\Phi and to the basis e of ⋀3E\bigwedge^3 E). Show that (x,y)→x∧‾y(x, y) \to x \overline{\wedge} y is an alternating bilinear mapping of E×EE \times E into E, and that x∧‾yx \overline{\wedge} y is orthogonal to x and to y.

b) Let α, β be two invertible elements of A, B the quaternion algebra over A corresponding to the pair (α,β\alpha, \beta) (Chapter II, § 7, No. 8), 1, u, v, ω the canonical basis of B over A; let E be the submodule of B having u, v, ω as basis. Show that if x, y are two quaternions belonging to E, one has

xy=Φ(x,y)+x∧‾y xy = \Phi(x, y) + x \overline{\wedge} y
where Φ is a symmetric bilinear form on E, such that the linear mappings associated with Φ are bijective, and x∧‾yx \overline{\wedge} y is the vector product of x and y relative to the form Φ and to the basis α−1β−1u∧v∧ω\alpha^{-1}\beta^{-1}u \wedge v \wedge \omega of ⋀3E\bigwedge^3 E.

11) Let Φ be a non-degenerate ε-hermitian sesquilinear form on a finite-dimensional vector space E. A vector subspace M of E is said to be weakly orthogonal to a vector subspace N (relative to Φ) if one of the two subspaces M, N° contains the other.

a) Show that the relation "M is weakly orthogonal to N" is symmetric.

b) If M and N are weakly orthogonal, M° and N° are weakly orthogonal.

c) If M and N are weakly orthogonal and if M∩N={0}M \cap N = \{0\}, M and N are orthogonal.

Machine translation of the English, by gpt-5-mini, gpt-5-6-mini, against glossary version 34. Not checked by a person. That model is a cut down version of the one the rest of this language was written by.