Bourbaki

§ 7. Hermitian forms and ordered fields

Throughout this paragraph, let K denote a maximal ordered field (hence commutative and of characteristic zero; cf. chap. VI, § 2), and suppose that we are in one of the following three cases:

1°) A = K, J is the identity; 2°) A is the field K(i), obtained by adjunction to K of a square root i of −1, and, for every λ ∈ A, λ‾\overline{\lambda} is the conjugate of λ (chap. II, § 7, no 7). 3°) A is the quaternion field over K corresponding to the pair (−1, −1) (or, as we shall say for brevity, the quaternion field over K), and, for every λ ∈ A, λ‾\overline{\lambda} is the conjugate of λ (cf. chap. II, § 7, no 8 and chap. VIII, § 11, no 2).

If Φ is a hermitian form on E, we therefore have, in all cases, Φ(x,x)∈K\Phi(x, x) \in K for every x∈Ex \in E, since Φ(x,x)=Φ(x,x)‾\Phi(x, x) = \overline{\Phi(x, x)}.

1. Positive hermitian forms.

Definition 1

A hermitian form Φ\Phi on EE is said to be positive (resp. negative) if Φ(x,x)⩾0\Phi(x, x) \geqslant 0 (resp. Φ(x,x)⩽0\Phi(x, x) \leqslant 0) for every x∈Ex \in E.

When A=KA = K, one also says that the quadratic form

Q(x)=12Φ(x,x) Q(x) = \frac{1}{2} \Phi(x, x)
associated with Φ\Phi is positive (resp. negative).

Suppose EE is finite-dimensional over AA, and let (ei)(e_i) (i=1,…,ni = 1, \ldots, n) be an orthogonal basis of EE (§6§ 6, no 1, th. 1). For a hermitian form Φ\Phi on EE to be positive, it is necessary and sufficient that Φ(ei,ei)⩾0\Phi(e_i, e_i) \geqslant 0 for i=1,…,ni = 1, \ldots, n. Let Φ\Phi be a positive non-degenerate hermitian form on EE; since every positive element of KK is a square, hence of the form ρρ‾\rho \overline{\rho} (ρ∈A\rho \in A), there exist orthonormal bases for Φ\Phi in EE (§6§ 6, no 1, cor. 1 of th. 1).

Proposition 1

Suppose EE is finite-dimensional, and A=KA = K or A=K(i)A = K(i). If Φ\Phi is a positive non-degenerate hermitian form on EE, then the extensions of Φ\Phi to ⨂pE\bigotimes^p E and ∧pE\wedge^p E (p>0p > 0), as well as the inverse form of Φ\Phi, are positive non-degenerate hermitian forms.

This follows at once from the existence of an orthonormal basis of EE, and from prop. 2, §6§ 6, no 1.

Prop. 1 remains true if « positive non-degenerate » is replaced everywhere by « positive ».

Proposition 2

Let Φ\Phi be a positive hermitian form on EE. For x,yx, y in EE, one has

Φ(x,y)Φ(x,y)‾⩽Φ(x,x)Φ(y,y). \Phi(x, y) \overline{\Phi(x, y)} \leqslant \Phi(x, x) \Phi(y, y).

The inequality is indeed immediate when the vectors xx and yy are proportional. We may therefore suppose that xx and yy are linearly independent. Let A′A' be the (commutative) subfield K(Φ(x,y))K(\Phi(x, y)) of AA, FF the vector plane over A′A' generated by xx and yy, and ΦF\Phi_F the restriction of Φ\Phi to FF; the latter takes its values in A′A'. By Proposition 1, the discriminant of ΦF\Phi_F with respect to the basis (x,y)(x, y) is ⩾0\geqslant 0. Now this discriminant is Φ(x,x)Φ(y,y)−Φ(x,y)Φ(x,y)‾\Phi(x, x)\Phi(y, y) - \Phi(x, y)\overline{\Phi(x, y)}. Q.E.D.

Corollary

The set of isotropic vectors of E is the orthogonal subspace E0E^0 of E for Φ\Phi. In order that Φ\Phi be non-degenerate, it is necessary and sufficient that Φ(x,x)>0\Phi(x, x) > 0 for every x≠0x \neq 0.

Proposition 3

Suppose E finite-dimensional and A commutative (A=K\mathbf{A} = \mathbf{K} or A=K(i)\mathbf{A} = \mathbf{K}(i)). Let Φ\Phi be a hermitian form on E, X its matrix with respect to a basis (xj)(x_j) (j=1,…,nj = 1, \ldots, n) of E; for every subset H of {1,n}\{1, n\}, denote by XH,HX_{H, H} the minor of X obtained by deleting the rows and columns with indices j∉Hj \notin H (Chap. III, § 6, No. 3).

a) *If Φ\Phi is positive non-degenerate, then XH,H>0X_{H, H} > 0 for every subset H of {1,n}\{1, n\}.

b) *Conversely, if, on putting Hj={1,j}H_j = \{1, j\}, we have XHj,Hj>0X_{H_j, H_j} > 0 for j=1,…,nj = 1, \ldots, n, then Φ\Phi is positive non-degenerate.

Suppose first that Φ\Phi is positive non-degenerate. The elements (xj)(x_j) (j∈Hj \in H) form a basis of a subspace F of E, and the minor XH,HX_{H, H} is the discriminant of the restriction ΦF\Phi_F of Φ\Phi to F with respect to this basis; now, since ΦF(x,x)>0\Phi_F(x, x) > 0 for every x≠0x \neq 0 in F, ΦF\Phi_F is positive non-degenerate (Corollary to Proposition 2); hence XH,H>0X_{H, H} > 0 (Proposition 1). To prove b), let us note that, with the notation of Proposition 1, § 6, No. 1, the minor XHj,HjX_{H_j, H_j} is equal to Dj+1,j+1D_{j+1, j+1}; there therefore exists (Proposition 1, § 6, No. 1) an orthogonal basis (ej)(e_j) (j=1,…,nj = 1, \ldots, n) of E such that Φ(ej,ej)>0\Phi(e_j, e_j) > 0 for j=1,…,nj = 1, \ldots, n; consequently Φ\Phi is positive non-degenerate.

Remark

It follows from the existence of orthonormal bases that two non-degenerate positive hermitian forms on two vector spaces of the same finite dimension are equivalent (§ 1, no 6). Let then L be a finite-dimensional hermitian space over A, whose metric form is positive non-degenerate, and let V1V_1 and V2V_2 be two linear varieties of the same dimension in L (§ 6, no 6); since the restrictions of the metric form to the directions T1T_1 and T2T_2 of V1V_1 and V2V_2 on the one hand, and to the orthogonal subspaces T10T_1^0 and T20T_2^0 on the other hand, are equivalent, there exists a unitary automorphism uu of the space TT of the translations of LL such that u(T1)=T2u(T_1) = T_2 and u(T10)=T20u(T_1^0) = T_2^0; there therefore exists a displacement vv of LL such that v(V1)=V2v(V_1) = V_2. Let (a,b),(a′,b′)(a, b), (a', b') be two pairs of points of LL; for there to exist a displacement vv of LL such that v(a)=a′v(a) = a' and v(b)=b′v(b) = b', it is therefore necessary and sufficient (with the notation of § 6, no 6) that one has e(a,b)=e(a′,b′)e(a, b) = e(a', b'); the element e(a,b)\sqrt{e(a, b)} of AA (chap. VI, § 2, no 4) is called the distance between aa and bb in the hermitian space LL.

2. The law of inertia.

Theorem 1 (« law of inertia »)

Suppose that AA satisfies the hypotheses at the beginning of this paragraph, and that EE is of finite dimension nn. Let Φ\Phi be a hermitian form on EE. Then:

a) There exists a decomposition of EE into a direct sum of the subspace E0E^0 orthogonal to EE, and of two subspaces E+E^+ and E−E^- such that the restriction of Φ\Phi to E+E^+ (resp. E−E^-) is positive (resp. negative) and non-degenerate.

b) There exists an orthogonal basis (ei)1≤i≤n(e_i)_{1 \leq i \leq n} of EE such that

Φ(∑i=1nξiei,∑i=1nηiei)=∑i=1sξiηi‾−∑i=s+1s+tξiηi‾. \Phi\left( \sum_{i=1}^n \xi_i e_i, \sum_{i=1}^n \eta_i e_i \right) = \sum_{i=1}^s \xi_i \overline{\eta_i} - \sum_{i=s+1}^{s+t} \xi_i \overline{\eta_i}.

c) The dimensions ss of E+E^+ and tt of E−E^- are the same for all the decompositions into a direct sum satisfying the conditions stated in a) ; the integer ss (resp. tt) is the maximum of the dimensions of the subspaces FF of EE such that the restriction of Φ\Phi to FF is positive (resp. negative) and non-degenerate.

d) The rank of Φ\Phi is s+ts + t.

e) If Φ\Phi is non-degenerate, its index is equal to inf⁡(s,t)\inf(s, t) (§ 4, no 2, def. 2).

Indeed, let (xi)(x_i) (i=1,…,ni = 1, \ldots, n) be an orthogonal basis of EE (§ 6, No. 1, Theorem 1); recall that Φ(x,x)∈K\Phi(x, x) \in K for every x∈Ex \in E. We may suppose that Φ(xi,xi)>0\Phi(x_i, x_i) > 0 for i=1,…,si = 1, \ldots, s, Φ(xi,xi)<0\Phi(x_i, x_i) < 0 for i=s+1,…,s+ti = s + 1, \ldots, s + t and Φ(xi,xi)=0\Phi(x_i, x_i) = 0 for i=s+t+1,…,ni = s + t + 1, \ldots, n. This proves a), since we take for E+E^+ (resp. E−E^-) the subspace generated by x1,…,xsx_1, \ldots, x_s (resp. by xs+1,…,xs+tx_{s+1}, \ldots, x_{s+t}), and E0E^0 is then generated by xs+t+1,…,xnx_{s+t+1}, \ldots, x_n. We deduce b) from this by observing that Φ(xi,xi)\Phi(x_i, x_i) is of the form ρρ‾\rho \overline{\rho} (resp.

- ρρˉ) (ρ∈A∗)\rho \bar{\rho} )\ (\rho \in A^*) for i=1,…,si = 1, \ldots, s (resp. i=s+1,…,s+ti = s + 1, \ldots, s + t). To prove c), consider a subspace P of E such that the restriction of Φ\Phi to P is positive and non-degenerate; we then have P∩(E−+E0)={0}P \cap (E^- + E^0) = \{0\}, and the sum P+E−+E0P + E^- + E^0 is therefore direct; we conclude that dim⁡P≤dim⁡E+=s\dim P \leq \dim E^+ = s, and this proves c). Assertion d) follows at once from a).

Suppose finally that Φ\Phi is non-degenerate, put q=inf⁡(s,t)q = \inf (s, t), and show that q is the index of Φ\Phi. With the notations of b), the vectors ei+es+ie_i + e_{s+i} (resp. ei−es+ie_i - e_{s+i}) (i=1,…,qi = 1, \ldots, q) generate a totally isotropic subspace F (resp. F′F'). Since K is of characteristic 0, F+F′F + F' is generated by e1,…,eq,es+1,…,es+qe_1, \ldots, e_q, e_{s+1}, \ldots, e_{s+q} and is therefore non-isotropic. The restriction of Φ\Phi to the subspace H=(F+F′)0H = (F + F')^0 is then positive (or negative) and non-degenerate, and H contains therefore no isotropic vector ≠0\neq 0. Since F0F^0 contains F and H, and since dim⁡(F+H)=codim⁡F′=codim⁡F\dim(F + H) = \operatorname{codim} F' = \operatorname{codim} F, we have F0=F+HF^0 = F + H. Thus an isotropic vector z orthogonal to F is necessarily in F, because, in the direct sum F+HF + H, the component of z in H is isotropic. Consequently F is a maximal totally isotropic subspace, and this proves e).

Definition 2

With the notations of Theorem 1, the pair (s,t)(s, t) is called the signature of Φ\Phi.

3. Reduction of a form with respect to a positive hermitian form.

In this No. we shall suppose that E is of finite dimension nn over AA, and we shall denote by Φ\Phi a non-degenerate positive hermitian form on E.

Since the linear mappings of E into E∗E^* associated with Φ\Phi are bijective, whatever the elements x,y,zx, y, z of E with y≠0y \neq 0, there exists one and only one element tt of E such that Φ(x,z)=Φ(t,y)‾\Phi(x, z) = \overline{\Phi(t, y)}. In particular, if A=KA = K or A=K(i)A = K(i) and if uu is a semilinear mapping for J of E into itself (chap. II, App. I, No. 1), there exists, for every x∈Ex \in E, one and only one element u∗(x)u^*(x) such that for every y∈Ey \in E, Φ(x,u(y))=Φ(u∗(x),y)‾\Phi(x, u(y)) = \overline{\Phi(u^*(x), y)}. It is immediately seen that u∗u^* is a semilinear mapping for J of E into itself; it is called the adjoint of uu.

Remark 1

When J is the identity, we recover the notion of adjoint of a homomorphism defined in § 1, No. 8.

Remark 2

Suppose still that A=KA = K or A=K(i)A = K(i). Let EJE^J be the right A-module defined in § 1, No. 2, Def. 5. The form Φ\Phi is a bilinear form on E×EJE \times E^J, ΦJ\Phi^J is a bilinear form on EJ×EE^J \times E, and uu is an A-linear mapping of E into EJE^J. The adjoint of this homomorphism, in the sense of § 1, No. 8, is an A-linear mapping of E into EJE^J; it is immediately seen that this coincides with the mapping u∗u^* defined above.

An endomorphism uu of E is said to be normal (for Φ\Phi) if uu∗=u∗uuu^* = u^*u.

Examples of normal endomorphisms: 1) the unitary automorphisms for Φ\Phi (§\S 6, No. 2), which are characterized by the relation u−1=u∗u^{-1} = u^* (§\S 1, No. 8, cor. of prop. 8); 2) the endomorphisms uu such that u∗=uu^* = u; these are called hermitian endomorphisms.

For every hermitian endomorphism uu of E, put Φu(x,y)=Φ(u(x),y)\Phi_u(x, y) = \Phi(u(x), y); we have

Φu(y,x)=Φ(u(y),x)=Φ(y,u(x))=Φ(u(x),y)‾=Φu(x,y)‾. \Phi_u(y, x) = \Phi(u(y), x) = \Phi(y, u(x)) = \overline{\Phi(u(x), y)} = \overline{\Phi_u(x, y)}.
which shows that Φu\Phi_u is a hermitian form on E. Conversely let Ψ\Psi be a hermitian form on E; since the mapping sΦs_\Phi of E into E∗E^* associated with Φ\Phi is bijective, there exists, for every x∈Ex \in E, one and only one element u(x)u(x) of E such that Ψ(x,y)=Φ(u(x),y)\Psi(x, y) = \Phi(u(x), y); it is easily verified that uu is a hermitian endomorphism of E. Thus u→Φuu \to \Phi_u is a canonical bijection of the set of hermitian endomorphisms of E onto the set of hermitian forms on E.

Suppose that A=KA = K or A=K(i)A = K(i); given a bilinear form Ψ\Psi on E, there exists, for every x∈Ex \in E, one and only one element u(x)u(x) of E such that Ψ(x,y)=Φ(u(x),y)‾\Psi(x, y) = \overline{\Phi(u(x), y)}; it is immediately seen that uu is a semilinear mapping (for J) of E into itself. Since Φ(u(x),y)=Φ(y,u(x))=Φ(u∗(y),x)‾\Phi(u(x), y) = \Phi(y, u(x)) = \overline{\Phi(u^*(y), x)}, we see that, for Ψ\Psi to be symmetric (resp. alternating), it is necessary and sufficient that u∗=uu^* = u (resp. u∗=−uu^* = -u).

Theorem 2

Let S be a set of endomorphisms of E (resp. of semilinear mappings of E into E when A = K or A = K(i)) stable under the mapping u → u*. Then, if V is a subspace of E stable under S, its orthogonal V⁰ is stable under S. On the other hand E is the direct sum of subspaces stable under S, minimal in the set of subspaces ≠ {0} and stable under S, and pairwise orthogonal.

Indeed let V be a subspace of E stable under S; whatever x ∈ V⁰, y ∈ V and u ∈ S, we have u*(y) ∈ V, whence Φ(y,u(x))=Φ(u∗(y),x)=0\Phi(y, u(x)) = \Phi(u*(y), x) = 0 (resp. Φ(y,u(x))=Φ(u∗(y),x)‾=0\Phi(y, u(x)) = \overline{\Phi(u^*(y), x)} = 0), and consequently u(x) ∈ V⁰; thus V⁰ is stable under S, which proves our first assertion. For the second we shall proceed by induction on the dimension n of E, the case n = 0 being trivial. For n ≠ 0 there exists a subspace V ≠ {0} of E stable under S and minimal, for example a stable subspace ≠ {0} of minimal dimension. It then suffices to apply the induction hypothesis to V⁰, since the adjoint of the restriction of u to V⁰ (with respect to the restriction of Φ\Phi) is identical with the restriction to V⁰ of the adjoint of u.

Corollary 1

Suppose that A = K or that A = K(i). Let B be a subalgebra of LA(E)\mathscr{L}_A(E), stable under the mapping u → u*. Then E is a semisimple B-module, and is the direct sum of simple submodules pairwise orthogonal. The algebra B is semisimple.

Indeed, since every B-submodule V of E has a supplement, for example V⁰, the B-module V is semisimple (chap. VIII, § 3, No. 3, prop. 7). Since every B-submodule ≠ {0} and minimal in E is simple, E is the direct sum of simple submodules pairwise orthogonal. Finally B is a semisimple algebra, since it admits a semisimple and faithful module E whose contramodule is of finite type (chap. VIII, § 5, No. 1, prop. 3).

Corollary 2

The assumptions and notations being those of cor. 1, suppose in addition that the algebra B is commutative. Then all its elements are semisimple (normal) endomorphisms of E. When A = K (resp. A = K(i)), E is the direct sum of simple B-submodules pairwise orthogonal, which are vector spaces of dimension 1 or 2 (resp. 1) over A.

The first assertion follows from chap. VIII, § 9, No. 1, prop. 2, since B is semisimple. On the other hand every simple B-module is isomorphic to a B-module of the form B/m, where m is a maximal ideal of B, hence to a commutative field L of finite degree over A; when A = K (resp. A = K(i)), the field L is necessarily isomorphic to K or K(i) (resp. K(i)), since K(i) is algebraically closed (chap. VI, § 2, No. 6, th. 3).

Proposition 4

Let u be a normal endomorphism of E. When A is equal to K(i) or to the quaternion field over K, there exists an orthonormal basis (for Φ) of E formed by eigenvectors of u. When A = K, u is semisimple and E is direct sum of stable subspaces for u, pairwise orthogonal, and of dimension 1 or 2.

First examine the case where A is commutative (A = K or A = K(i)). Then the subalgebra B = A[u, u*] of LA(E)\mathscr{L}_A(E) is commutative since u is normal; it is stable under the mapping φ→φ∗\varphi \to \varphi^* by virtue of formulas (32) and (33) of § 1, No. 8. The assertion concerning the case A = K then follows immediately from cor. 2 of th. 2. When A = K(i), this corollary also shows that E is direct sum of vector subspaces AxiAx_i (i=1,…,ni = 1, \ldots, n) of dimension 1, pairwise orthogonal and stable for u; if one puts ei=(Φ(xi,xi))−1/2xie_i = (\Phi(x_i, x_i))^{-1/2} x_i, (ei)(e_i) is the orthonormal basis sought.

When A is the quaternion field over K, it will suffice similarly to prove, by virtue of th. 2, that every minimal element of the set of subspaces ≠{0}\neq \{0\} of E stable for u and u∗u^* is of dimension 1. Now such a subspace V necessarily contains an eigenvector x≠0x \neq 0 of u (*), as is seen by observing that the quaternion field A contains K(i) as an algebraically closed subfield, and by restricting to K(i) the field of

(*) If E is a left vector space over a noncommutative field A, and u an endomorphism of E, one still says that a vector x≠0x \neq 0 of E is an eigenvector for u if there exists a∈Aa \in A such that u(x)=axu(x) = ax; the scalar a is then called an eigenvalue of u. One will note that, for every b≠0b \neq 0 in A, the vector bxbx is an eigenvector for u, and that the corresponding eigenvalue is bab−1bab^{-1}.

scalars of V. It remains therefore only to show that the eigenvector x of u is also an eigenvector of u*. Put u(x)=axu(x) = ax (a∈Aa \in A); one then has Φ(u(x),x)=aΦ(x,x)=Φ(x,x)a=Φ(x,a‾x)\Phi(u(x), x) = a\Phi(x, x) = \Phi(x, x)a = \Phi(x, \overline{a}x) since Φ(x,x)\Phi(x, x) belongs to the center of A, and on the other hand Φ(u(x),x)=Φ(x,u∗(x))\Phi(u(x), x) = \Phi(x, u^*(x)); it follows that one has Φ(x,u∗(x)−a‾x)=0\Phi(x, u^*(x) - \overline{a}x) = 0, and one can therefore write u∗(x)=a‾x+zu^*(x) = \overline{a}x + z, where z is a vector orthogonal to x. One therefore has

Φ(u∗(x),u∗(x))=a‾aΦ(x,x)+Φ(z,z)=Φ(u(x),u(x))+Φ(z,z). \Phi(u^*(x), u^*(x)) = \overline{a}a\Phi(x, x) + \Phi(z, z) = \Phi(u(x), u(x)) + \Phi(z, z).

Now, since u is normal, one has

Φ(u(x),u(x))=Φ(x,u∗u(x))=Φ(x,uu∗(x))=Φ(uu∗(x),x)=Φ(u∗(x),u∗(x)). \begin{align*} \Phi(u(x), u(x)) &= \Phi(x, u^*u(x)) = \Phi(x, uu^*(x)) \\ &= \Phi(uu^*(x), x) = \Phi(u^*(x), u^*(x)). \end{align*}

Consequently one has Φ(z,z)=0\Phi(z, z) = 0, which, by assumption, entails z=0z = 0 and u∗(x)=a‾xu^*(x) = \overline{a}x. QED.

Remark

It follows from th. 2 that the eigenspaces relative to two distinct eigenvalues of u are orthogonal.

Proposition 5

Let u be a hermitian endomorphism of E. The eigenvalues of u belong to K, and there exists an orthonormal basis of E formed of eigenvectors of u.

When A is equal to K(i) or to the quaternion field over K, it suffices, by virtue of prop. 4, to prove the first assertion; now, if x is an eigenvector ≠0\neq 0 of u and a the corresponding eigenvalue, one has, by virtue of the assumption u=u∗u = u^*,

aΦ(x,x)=Φ(u(x),x)=Φ(x,u(x))=Φ(x,x)a‾; a\Phi(x, x) = \Phi(u(x), x) = \Phi(x, u(x)) = \Phi(x, x)\overline{a} ;

as Φ(x,x)\Phi(x, x) is a nonzero element of the center of A, it follows that a=a‾a = \overline{a}, hence a∈Ka \in K. Consequently a hermitian matrix has all its eigenvalues in K. Suppose now that A is equal to K. The matrix M of u with respect to an orthonormal basis of E is then symmetric; it is therefore a hermitian matrix if one considers it as a matrix over K(i). The first part of the proof then shows that this matrix has all its eigenvalues in K, and admits therefore, if E≠{0}E \neq \{0\}, nonzero eigenvectors in E. It follows that every stable subspace for u and minimal is necessarily of dimension 1, and the conclusion follows immediately, as in prop. 4.

Proposition 6

a) Let Ψ\Psi be a hermitian form (resp. symmetric bilinear form if A=K\mathbf{A} = \mathbf{K} or A=K(i)\mathbf{A} = \mathbf{K}(i)) on EE. There exists a basis of EE which is orthonormal for Φ\Phi and orthogonal for Ψ\Psi.

b) Suppose A=K\mathbf{A} = \mathbf{K} or A=K(i)\mathbf{A} = \mathbf{K}(i), and let Ψ\Psi be an alternating bilinear form on EE. There exists a basis of EE which is orthonormal for Φ\Phi and with respect to which the matrix of Ψ\Psi is of the form

(0a100…0−a1000…0000a2…000−a20…0⋯⋯⋯⋯). \begin{pmatrix} 0 & a_1 & 0 & 0 \ldots 0 \\ -a_1 & 0 & 0 & 0 \ldots 0 \\ 0 & 0 & 0 & a_2 \ldots 0 \\ 0 & 0 & -a_2 & 0 \ldots 0 \\ \cdots & \cdots & \cdots & \cdots \end{pmatrix}.

where the aia_i are ⩾0\geqslant 0 in K.

When Ψ\Psi is hermitian, our assertion follows at once from Prop. 5 and the canonical correspondence between hermitian forms on EE and hermitian endomorphisms for Φ\Phi. In the two other cases, let uu be the semilinear mapping of EE into itself defined at the beginning of this No. by the formula Ψ(x,y)=Φ(u(x),y)‾\Psi(x, y) = \overline{\Phi(u(x), y)}. Then u2u^2 is an A\mathbf{A}-linear mapping; when Ψ\Psi is symmetric (resp. alternating), one has u=u∗u = u^* (resp. u=−u∗u = -u^*), hence u2u^2 is hermitian; whence also

Φ(u2(x),x)=Φ(x,u2(x))‾=Φ(u∗(x),u(x))=Φ(u(x),u(x)) \Phi(u^2(x), x) = \overline{\Phi(x, u^2(x))} = \Phi(u^*(x), u(x)) = \Phi(u(x), u(x))
(resp. −Φ(u(x),u(x))-\Phi(u(x), u(x)));

this shows that the hermitian form (x,y)→Φ(u2(x),y)(x, y) \to \Phi(u^2(x), y) is positive (resp. negative). Apply then Theorem 2, and let VV be a minimal element of the family of the subspaces ≠{0}\neq \{0\} of EE stable for uu and for u∗u^*. Since u2u^2 is a hermitian endomorphism, VV contains a proper vector x≠0x \neq 0 of u2u^2; put u2(x)=axu^2(x) = ax, where a∈Ka \in \mathbf{K} (Prop. 5).

When Ψ\Psi is symmetric, the inequality Φ(u2(x),x)⩾0\Phi(u^2(x), x) \geqslant 0 shows that one has a⩾0a \geqslant 0. Put y=a1/2x+u(x)y = a^{1/2}x + u(x); one has u(y)=a1/2u(x)+ax=a1/2yu(y) = a^{1/2}u(x) + ax = a^{1/2}y, and AyAy is stable for uu and u∗=uu^* = u. If y=0y = 0, AxAx is stable for uu and u∗u^*; in all cases, VV is a subspace of dimension 1, and our conclusion follows at once from Theorem 2.

When Ψ\Psi is alternating, one has a⩽0a \leqslant 0; put

y=(−a)1/2x+u(x),z=(−a)1/2x−u(x). y = (-a)^{1/2}x + u(x), \quad z = (-a)^{1/2}x - u(x).

One has u(y)=−(−a)1/2z, u(z)=(−a)1/2yu(y) = -(-a)^{1/2}z, \ u(z) = (-a)^{1/2}y and

Φ(y,z)=−aΦ(x,x)−Φ(u(x),u(x))=−Φ(ax,x)+Φ(u2(x),x)=0. \Phi(y, z) = -a\Phi(x, x) - \Phi(u(x), u(x)) = -\Phi(ax, x) + \Phi(u^2(x), x) = 0.

If y=z=0y = z = 0, we have a=0a = 0 and u(x)=0u(x) = 0, hence AxAx is stable under uu and u∗u^*, VV is of dimension 1, and the matrix of the restriction of Ψ\Psi to VV is zero since Ψ\Psi is alternating. Otherwise, yy and zz are both ≠0\neq 0, they generate VV, and since they are orthogonal, VV is of dimension 2 and the matrix of the restriction of Ψ\Psi to VV is of the form (0b−b0)\begin{pmatrix} 0 & b \\ -b & 0 \end{pmatrix}. Finally, by virtue of the formula Ψ′(x′,y′)=Φ(u(x′),y′)‾\Psi'(x', y') = \overline{\Phi(u(x'), y')}, we have Ψ′(x′,y′)=0\Psi'(x', y') = 0 when x′x' and y′y' belong to two subspaces stable under uu and orthogonal for Φ\Phi. This proves the existence of an orthonormal basis of EE (for Φ\Phi) with respect to which the matrix of Ψ\Psi has the indicated form. Q.E.D.

Exercises. — 1) Suppose that the hypotheses at the beginning of § 7 are satisfied; let Φ\Phi be a positive Hermitian form on EE.

a) In order that Φ(x,x)Φ(y,y)=Φ(x,y)Φ(x,y)‾\Phi(x, x)\Phi(y, y) = \Phi(x, y)\overline{\Phi(x, y)}, it is necessary and sufficient that xx and yy be linearly dependent or that the plane generated by xx and yy be isotropic.

b) Suppose that, for every x∈Ex \in E, Φ(x,x)\Phi(x, x) is a square in KK. Now prove that for any two vectors x,yx, y of EE, we have

Φ(x+y,x+y)≤Φ(x,x)+Φ(y,y). \sqrt{\Phi(x + y, x + y)} \leq \sqrt{\Phi(x, x)} + \sqrt{\Phi(y, y)}.

If Φ\Phi is non-degenerate, the two members of this inequality can be equal only if αx+βy=0\alpha x + \beta y = 0, where α\alpha and β\beta are two elements of KK, not both zero and such that αβ≤0\alpha \beta \leq 0.

2) Suppose A=KA = K or A=K(i)A = K(i). Let XX be a Hermitian square matrix of order nn over AA, such that for every nonempty subset HH of {1,n}\{1, n\}, we have XH,H≥0X_{H, H} \geq 0 (notations of Proposition 3 of No. 1).

a) Let λ\lambda be an element >0> 0 of KK; now prove that the matrix X+λIX + \lambda I is positive non-degenerate (use Proposition 3 of No. 1, reasoning by induction on nn).

b) Deduce that the Hermitian matrix XX is positive.

Remark 3

One assumes that A=KA = K or A=K(i)A = K(i) and that EE is finite-dimensional. Let Φ1,Φ2\Phi_1, \Phi_2 be two positive hermitian forms on EE, and let V=(αij),W=(βij)V = (\alpha_{ij}), W = (\beta_{ij}) be the matrices of these forms with respect to the same basis (ei)(e_i) of EE. Show that the hermitian form Φ\Phi whose matrix (γij)(\gamma_{ij}) with respect to (ei)(e_i) is such that γij=αijβij\gamma_{ij} = \alpha_{ij}\beta_{ij} for every pair of indices, is positive; moreover, if Φ1\Phi_1 and Φ2\Phi_2 are non-degenerate, the same is true of Φ\Phi. (In the calculation of Φ(x,x)\Phi(x, x), express the αij\alpha_{ij} in terms of the values Φ1(ci,ci)\Phi_1(c_i, c_i) for an orthogonal basis (ci)(c_i) of EE relative to Φ1\Phi_1.)

Remark 4

One assumes that A=KA = K or A=K(i)A = K(i). Let RR be a hermitian matrix of order nn over AA; one says that RR has signature (s,t)(s, t) if the hermitian form on AnA^n having RR as matrix with respect to the canonical basis, has signature (s,t)(s, t). Let Δk\Delta_k denote the principal minor of RR obtained by deleting in RR the rows and columns of index >k> k; one assumes that Δs+t≠0\Delta_{s+t} \neq 0 and that, for no index k<s+tk < s + t, Δk\Delta_k and Δk+1\Delta_{k+1} are simultaneously zero (cf. § 6, exerc. 1 b)). Show that if Δk=0\Delta_k = 0 for some k<s+tk < s + t, Δk−1\Delta_{k-1} and Δk+1\Delta_{k+1} have opposite signs (method of exerc. 1 a) of § 6) and that the number s−ts - t is equal to

sgn⁡Δ1+sgn⁡(Δ1Δ2)+⋯+sgn⁡(Δs+t−1Δs+t) \operatorname{sgn} \Delta_1 + \operatorname{sgn} (\Delta_1 \Delta_2) + \cdots + \operatorname{sgn} (\Delta_{s+t-1} \Delta_{s+t})

(use exerc. 2 of § 6).

Remark 5

One assumes that A=KA = K or A=K(i)A = K(i); let R,SR, S be two hermitian matrices over AA, of signatures (s,t)(s, t) and (s′,t′)(s', t') respectively (exerc. 4); show that the matrix R⊗SR \otimes S is a hermitian matrix of signature (ss′+tt′,st′+s′t)(ss' + tt', st' + s't).

Remark 6

Let KK be a maximal ordered field, LL a simple algebra of finite rank over KK. If (s,t)(s, t) is the signature of the symmetric bilinear form (x,y)→Tr⁡L/K(xy)(x, y) \to \operatorname{Tr}_{L/K}(xy) on LL, now prove that one has: s−t=ms - t = m if LL is isomorphic to a matrix algebra of order mm over KK; s−t=0s - t = 0 if LL is isomorphic to a matrix algebra over the field K(i)K(i); s−t=−2ms - t = -2m if LL is isomorphic to a matrix algebra of order mm over the quaternion field over KK.

Remark 7

We suppose that AA satisfies the conditions at the beginning of § 7 and that EE is of finite dimension nn. Let Φ\Phi be a non-degenerate positive hermitian form on EE. a) Now prove that every similitude for Φ\Phi can be written in one and only one way as the product of a homothety of ratio ⩾0\geqslant 0 in KK, and of a unitary transformation. b) For every basis (ai)1≤i≤n(a_i)_{1 \leq i \leq n} of EE, show that there exists one and only one orthonormal basis (ei)1≤i≤n(e_i)_{1 \leq i \leq n} of EE satisfying the following conditions: 1° for every mm such that 1≤m≤n1 \leq m \leq n, the subspace generated by a1,…,ama_1, \ldots, a_m is identical with the subspace generated by e1,…,eme_1, \ldots, e_m; 2° one has Φ(ai,ei)≥0\Phi(a_i, e_i) \geq 0 in KK, for every index ii (cf. § 6, no 1, prop. 1). c) Deduce from b) that for every invertible square matrix MM of order nn over AA, there exists one and only one pair of matrices (L,U)(L, U) of order nn, such that UU is a unitary matrix, that L=(λij)L = (\lambda_{ij}) has only zeros below its diagonal and diagonal terms λii\lambda_{ii} belonging to KK and >0> 0, and finally that M=LUM = LU.

Remark 8

On suppose A=KA = K; soit LL un espace hermitien de dimension finie sur AA, dont la forme métrique est positive non dégénérée. Soient M,NM, N deux parties de LL, uu une bijection de MM sur NN telle que l’on ait e(u(a),u(b))=e(a,b)e(u(a), u(b)) = e(a, b) quels que soient les points a,ba, b de MM. Montrer qu’il existe un déplacement dont la restriction à MM soit égale à uu (raisonner par récurrence sur la dimension de la variété linéaire affine engendrée par MM, comme dans le procédé d’orthogonalisation de Gram-Schmidt). La proposition s’étend-elle au cas où A est égal à K(i) ou au corps des quaternions sur K ?

Remark 9

On suppose remplies les conditions du n° 3, et en outre que A est le corps des quaternions sur K. Soit u un endomorphisme normal de E. Montrer que E est somme directe de sous-espaces F_k (1 \leq k \leq r), deux à deux orthogonaux, tels que dans chacun des F_k il existe une base orthonormale (e_{ik}) (1 \leq i \leq n_k) et que l’on ait u(e_{ik}) = \lambda_k e_{ik} pour 1 \leq i \leq n_k, deux \lambda_k d’indices distincts n’étant pas transformés l’un de l’autre par un automorphisme intérieur de A. En outre, si (F'_k) est une seconde décomposition de E ayant les mêmes propriétés, avec un système (\lambda'_k) de valeurs propres, on a F'_k = F_k (à une permutation près des indices) et \lambda'_k = \alpha_k \lambda_k \alpha_k^{-1}; l’ensemble des vecteurs propres de u pour la valeur propre \lambda_k est le sous-espace sur le commutant A_k de \lambda_k dans A, engendré par les e_{ik} (1 \leq i \leq n_k).

Remark 10

On suppose remplies les conditions du n° 3, et en outre que A est égal à K(i) ou au corps des quaternions sur K. Soit u un endomorphisme normal de E.

a) Montrer que pour qu’un sous-espace vectoriel F de E soit tel que u(F) \subset F, il faut et il suffit que F soit engendré par des vecteurs propres de u ; on a alors u(F^0) \subset F^0 et u^*(F) \subset F.

b) Pour que u soit unitaire (resp. pour que u^* = u, u^* = -u), il faut et il suffit que pour toute valeur propre \lambda de u, on ait \lambda \overline{\lambda} = 1 (resp. \overline{\lambda} = \lambda, \overline{\lambda} = -\lambda).

c) On dit qu’un endomorphisme hermitien u de E est positif (resp. positif et non dégénéré) si la forme hermitienne (x, y) \to \Phi(u(x), y) qui lui correspond canoniquement est positive (resp. positive et non dégénérée) ; il faut et il suffit pour cela que toutes les valeurs propres de u soient \geq 0 (resp. > 0).

d) Montrer que pour tout entier m > 0, il existe un endomorphisme normal v de E tel que v^m = u. Si u est hermitien positif, il existe un seul endomorphisme hermitien positif v tel que v^m = u, et il existe un polynôme f \in K[X] tel que v = f(u) ; ce dernier résultat est aussi valable lorsque A = K.

Remark 11

On suppose remplies les conditions du n° 3, et en outre que A = K. Soit u un endomorphisme normal de E.

a) Soit V un élément minimal de l’ensemble des sous-espaces de E non réduits à 0, stables pour u et u* ; montrer que si V est de dimension 2, la restriction de u à V est une similitude directe de multiplicateur > 0.

b) Montrer que tout sous-espace de E stable pour u est aussi stable pour u*. (Soit E_0 l’espace vectoriel obtenu à partir de E par extension à K(i) du corps des scalaires ; \Phi est la restriction à E d’une forme hermitienne positive non dégénérée sur E_0 et u la restriction à E d’un endomorphisme normal u_0 de E_0 (pour cette forme) ; en outre E est l’ensemble des x \in E_0 invariants par une bijection semi-linéaire involutive j de E_0, et on a u_0j = ju_0. Appliquer alors l’exerc. 10 a.).

Remark 12

On suppose remplies les conditions du n° 3, et en outre que A est égal à K(i) ou au corps des quaternions sur K. Montrer que pour tout endomorphisme uu de EE, il existe une base orthonormale de EE par rapport à laquelle la matrice de uu n’ait que des zéros au-dessous de la diagonale. (Procéder par récurrence sur la dimension de EE, en considérant un vecteur propre de uu.)

Remark 13

Soient AA un corps vérifiant les conditions du début du § 7, E,FE, F deux espaces vectoriels de dimension finie sur AA, Φ\Phi (resp. Ψ\Psi) une forme hermitienne positive non dégénérée sur EE (resp. FF). Montrer que, pour toute application linéaire uu de EE dans FF, l’adjoint u∗u^* de uu (pour Φ\Phi et Ψ\Psi; cf. § 1, no 8) est tel que u∗uu^*u et uu∗uu^* soient des endomorphismes hermitiens positifs (exerc. 10 c)) de EE et FF respectivement.

Remark 14

On suppose remplies les conditions du no 3. Soient uu un endomorphisme de EE, h1,h2h_1, h_2 les deux endomorphismes hermitiens positifs de EE, tels que l’on ait h12=u∗u,h22=uu∗h_1^2 = u^*u, h_2^2 = uu^* (exerc. 13 et 10 d)).

a) Montrer qu’il existe un endomorphisme unitaire ν\nu tel que u=νh1=h2νu = \nu h_1 = h_2 \nu et en particulier que h1h_1 et h2h_2 sont semblables (remarquer que u(0)=h1‾(0)u(0) = \overline{h_1}(0) et que si VV est le sous-espace orthogonal à u‾(0)\overline{u}(0), on a Φ(u(x),u(x))=Φ(h1(x),h1(x))\Phi(u(x), u(x)) = \Phi(h_1(x), h_1(x)) pour tout x∈Vx \in V. Pour que ν\nu soit déterminé de façon unique, il faut et il suffit que uu soit bijective. Pour qu’on puisse prendre ν\nu permutable avec h1h_1, il faut et il suffit que uu soit normal.

b) Deduce from a) that every square matrix MM of order nn over AA can be written UDVUDV, where UU and VV are unitary matrices and DD a diagonal matrix whose elements are ⩾0\geqslant 0, and whose squares are the eigenvalues of MM∗MM^*.

Remark 15

Suppose that the conditions of No. 3 are satisfied. Show that every positive Hermitian matrix HH over AA can be written in the form LL∗LL^*, where L=(λij)L = (\lambda_{ij}) has only zeros below its diagonal and diagonal terms belonging to KK and ⩾0\geqslant 0; moreover LL is uniquely determined by these conditions when HH is invertible (cf. exerc. 10 d) and 7 c)).

Remark 16

Suppose that the conditions of No. 3 are satisfied and in addition that A=K(i)A = K(i). Let uu be an endomorphism of EE.

a) The set of eigenvalues of uu is contained in the set UU of the values of Φ(x,u(x))\Phi(x, u(x)) when xx runs through the set of elements of EE such that Φ(x,x)=1\Phi(x, x) = 1.

b) A subset CC of A=K(i)A = K(i) is said to be convex if, for every pair of elements (ξ,η)∈C2(\xi, \eta) \in C^2 and every τ∈K\tau \in K such that 0⩽τ⩽10 \leqslant \tau \leqslant 1 one has τξ+(1−τ)η∈C\tau \xi + (1-\tau)\eta \in C. Show that the set UU is convex. (Reduce to the case where n=2n = 2; by writing uu in the form ν+iω\nu + i\omega, where ν\nu and ω\omega are hermitian, and by replacing if necessary uu by λu\lambda u, where λ∈A\lambda \in A and λλ‾=1\lambda \overline{\lambda} = 1, show that everything reduces to proving the following property. Let f(ξ1,ξ2)=ξ1ξ‾1+ξ2ξ‾2f(\xi_1, \xi_2) = \xi_1 \overline{\xi}_1 + \xi_2 \overline{\xi}_2, g(ξ1,ξ2)=aξ1ξ‾1+bξ2ξ‾2g(\xi_1, \xi_2) = a \xi_1 \overline{\xi}_1 + b \xi_2 \overline{\xi}_2 (a∈K,b∈Ka \in K, b \in K), h(ξ1,ξ2)=αξ1ξ‾1+βξ1ξ‾2+βξ2ξ‾1+γξ2ξ‾2h(\xi_1, \xi_2) = \alpha \xi_1 \overline{\xi}_1 + \beta \xi_1 \overline{\xi}_2 + \beta \xi_2 \overline{\xi}_1 + \gamma \xi_2 \overline{\xi}_2 (α∈K,γ∈K,β∈A\alpha \in K, \gamma \in K, \beta \in A); let (η1,η2)∈A2,(ζ1,ζ2)∈A2(\eta_1, \eta_2) \in A^2, (\zeta_1, \zeta_2) \in A^2 be such that f(η1,η2)=f(ζ1,ζ2)=1f(\eta_1, \eta_2) = f(\zeta_1, \zeta_2) = 1, g(η1,η2)=g(ζ1,ζ2)=1g(\eta_1, \eta_2) = g(\zeta_1, \zeta_2) = 1, h(η1,η2)>0h(\eta_1, \eta_2) > 0, h(ζ1,ζ2)<0h(\zeta_1, \zeta_2) < 0; there then exists (theta1,theta2)∈A2(theta_1, theta_2) \in A^2 such that f(θ1,θ2)=1f(\theta_1, \theta_2) = 1, g(θ1,θ2)=1g(\theta_1, \theta_2) = 1 and h(θ1,θ2)=0h(\theta_1, \theta_2) = 0. One will begin by observing that for every pair (ξ1,ξ2)(\xi_1, \xi_2), there exists μ∈A\mu \in A such that μμ‾=1\mu \overline{\mu} = 1 and βμξ1ξ‾2+βμξ2ξ‾1=0\beta \mu \xi_1 \overline{\xi}_2 + \beta \mu \xi_2 \overline{\xi}_1 = 0, which will make it possible to reduce to the case where β=0\beta = 0; use prop. 5 of Chap. VI, § 2, No. 5.)

c) Show that if uu is normal, UU is the smallest convex set containing all the eigenvalues of uu. Give an example where uu is not normal but where UU still has the preceding property. (Take as eigenvalues of uu the elements ±1±i\pm 1 \pm i as simple eigenvalues, and 0 as a double eigenvalue.)

Remark 17

Suppose the conditions of No. 3 are satisfied; for every ξ∈A\xi \in A, denote by ∣ξ∣|\xi| the element ρ⩾0\rho \geqslant 0 of K such that ρ2=ξξ‾\rho^2 = \xi \overline{\xi} (absolute value of ξ\xi). For every square matrix M=(αij)M = (\alpha_{ij}) over A, put f(M)=max⁡i∣αii∣f(M) = \max_i |\alpha_{ii}|, g(M)=max⁡i,j∣αij∣g(M) = \max_{i,j} |\alpha_{ij}|, and denote by φ(M)\varphi(M) the largest absolute value of the eigenvalues of MM (one will show that this definition has a meaning when A is the field of quaternions over K).

a) Let A,B,DA, B, D be three square matrices of order nn over A. Show that if DD is diagonal, one has

g2(ADB∗)≤f2(D)f(AA∗)f(BB∗) g^2(ADB^*) \leq f^2(D)f(AA^*)f(BB^*)
(use inequality (1) of No. 1). Deduce that
g(ABB∗A∗)≤f(AA∗)φ(BB∗) g(ABB^*A^*) \leq f(AA^*)\varphi(BB^*)
(apply Prop. 5 to the hermitian matrix BB∗BB^*). Deduce that, for mm arbitrary square matrices AiA_i (1≤i≤m1 \leq i \leq m) over A, one has
g2(A1A2…Am)≤f(A1A1∗)φ(A2A2∗)…φ(Am−1Am−1∗)f(Am∗Am) g^2(A_1A_2\ldots A_m) \leq f(A_1A_1^*)\varphi(A_2A_2^*)\ldots\varphi(A_{m-1}A_{m-1}^*)f(A_m^*A_m)
φ2(A1A2…Am)≤φ(A1A1∗)φ(A2A2∗)…φ(AmAm∗) \varphi^2(A_1A_2\ldots A_m) \leq \varphi(A_1A_1^*)\varphi(A_2A_2^*)\ldots\varphi(A_mA_m^*)
g2(A1A2…Am)≤φ(A1A1∗)…φ(AmAm∗). g^2(A_1A_2\ldots A_m) \leq \varphi(A_1A_1^*)\ldots\varphi(A_mA_m^*).
(For (3), reason by induction from (2). For (4), use Ex. 12; finally deduce (5) from (3).)

Show that inequality (3) no longer necessarily holds when Am∗AmA_m^*A_m is replaced there by AmAm∗A_mA_m^* (observe that one may have f(A∗A)≠f(AA∗)f(A^*A) \neq f(AA^*)), or when φ(AiAi∗)\varphi(A_iA_i^*) is replaced by f(AiAi∗)f(A_iA_i^*) for 2≤i≤m−12 \leq i \leq m-1 (take all the AiA_i equal to the square matrix whose all elements are 1).

b) Let uu be a normal endomorphism of E; if λ\lambda is an eigenvalue of uu (element of K(i)K(i) when A=KA = K), λ‾\overline{\lambda} is an eigenvalue of u∗uu^*u. For every normal matrix MM (matrix of a normal endomorphism of E with respect to an orthonormal basis), one therefore has φ2(M)=φ(MM∗)\varphi^2(M) = \varphi(MM^*). Deduce that one also has g(M)≤φ(M)g(M) \leq \varphi(M), and more generally, if M1,…,MmM_1, \ldots, M_m are normal,

g(M1…Mm)≤φ(M1)…φ(Mm) g(M_1\ldots M_m) \leq \varphi(M_1)\ldots\varphi(M_m)
φ(M1…Mm)≤φ(M1)…φ(Mm) \varphi(M_1\ldots M_m) \leq \varphi(M_1)\ldots\varphi(M_m)
(use (4) and (5)).

c) Show that if HH is a positive hermitian matrix over A, one has f(H)=g(H)≤φ(H)f(H) = g(H) \leq \varphi(H) (use (3) and b), by writing H=AA∗H = AA^*.

Remark 18

The conditions of No. 3 are assumed to be satisfied.

a) For every endomorphism uu of EE, let (ei)(e_i) be an orthonormal basis of EE formed by eigenvectors of u∗uu^*u, and let ρi\rho_i be the eigenvalue of u∗uu^*u corresponding to the vector eie_i; put s(u)=(∑i=1nρi)1/2s(u) = (\sum_{i=1}^n \rho_i)^{1/2} (square root of Tr⁡(u∗u)\operatorname{Tr}(u^*u) when AA is commutative); one has s(u∗)=s(u)s(u^*) = s(u). If u,vu, v are two endomorphisms of EE, U,VU, V their matrices with respect to the same orthonormal basis of EE, show that for the matrix UV∗+VU∗UV^* + VU^*, with elements in KK, one has (Tr⁡(UV∗+VU∗))2≤4s(u)s(v)(\operatorname{Tr}(UV^* + VU^*))^2 \leq 4s(u)s(v) (observe that (u∗+λv∗)(u+λv)(u^* + \lambda v^*)(u + \lambda v) is positive hermitian for every λ∈K\lambda \in K); deduce that s(u+v)≤s(u)+s(v)s(u + v) \leq s(u) + s(v). If in addition AA is commutative, one has

∣Tr⁡(uv)∣2≤s(u)s(v)and∣Tr⁡(u)∣≤ns(u) |\operatorname{Tr}(uv)|^2 \leq s(u)s(v) \quad \text{and} \quad |\operatorname{Tr}(u)| \leq \sqrt{n}s(u)

(write uu as a product by using Ex. 14 b)).

b) Suppose in addition that AA is commutative (thus equal to KK or K(i)K(i)). If H1,H2H_1, H_2 are two square matrices hermitian positive, now prove that one has Tr⁡(H1H2)≥0\operatorname{Tr}(H_1H_2) \geq 0 (reduce to the case where H2H_2 is a diagonal matrix). Deduce that one has (notations of Exercise 17)

∣Tr⁡(H1H2)∣≤φ(H1)Tr⁡(H2)≤Tr⁡(H1)Tr⁡(H2). |\operatorname{Tr}(H_1H_2)| \leq \varphi(H_1)\operatorname{Tr}(H_2) \leq \operatorname{Tr}(H_1)\operatorname{Tr}(H_2).

Conclude from these inequalities that for two arbitrary endomorphisms u,vu, v of EE, one has then s(uv)≤s(u)s(v)s(uv) \leq s(u)s(v).

c) Assuming still that AA is commutative, let ∏i=1n(x−λi)\prod_{i=1}^n (x - \lambda_i) be the decomposition into linear factors of the characteristic polynomial of an arbitrary endomorphism uu of EE; now prove that one has ∑i=1n∣λi∣2≤(s(u))2\sum_{i=1}^n |\lambda_i|^2 \leq (s(u))^2 and that, for the two members of this inequality to be equal, it is necessary and sufficient that uu be normal (use Exercise 12).

Remark 19

Suppose that the conditions of No. 3 are satisfied. Let MM be a square matrix of order nn over AA; now prove that for every square submatrix NN of MM (obtained by deleting in MM a certain number of rows and the columns having the same indices as these rows), one has (notations of Exercise 17) φ2(N)≤φ(MM∗)\varphi^2(N) \leq \varphi(MM^*) (apply suitably formula (4) of Exercise 17). If in particular MM is a normal matrix, φ(N)≤φ(M)\varphi(N) \leq \varphi(M) (cf. Exercise 17 b)).

Remark 20

Suppose that the conditions of No. 3 are satisfied and in addition that AA is equal to KK or to K(i)K(i). Apply the results of Exercises 17 to 19 to the extension of Φ\Phi to the pp-th exterior powers (§ 1, No. 9) and to the pp-th exterior powers of the endomorphisms or matrices considered. In particular, now prove that, if ∏i=1n(X−λi)\prod_{i=1}^n (X - \lambda_i) and ∏i=1n(X−ρi2)\prod_{i=1}^n (X - \rho_i^2) are the decompositions into linear factors of the characteristic polynomials of an endomorphism uu of EE and of the endomorphism u∗uu^*u, and if one supposes ∣λi∣⩾∣λi+1∣|\lambda_i| \geqslant |\lambda_{i+1}| and ρi⩾ρi+1⩾0\rho_i \geqslant \rho_{i+1} \geqslant 0 for 1⩽i⩽n−11 \leqslant i \leqslant n-1, one has

∣λ1λ2…λh∣⩽ρ1ρ2…ρh |\lambda_1 \lambda_2 \ldots \lambda_h| \leqslant \rho_1 \rho_2 \ldots \rho_h
for 1⩽h⩽n−11 \leqslant h \leqslant n-1 and ∣λ1λ2…λn∣=ρ1ρ2…ρn|\lambda_1 \lambda_2 \ldots \lambda_n| = \rho_1 \rho_2 \ldots \rho_n.

Remark 21

Suppose that the conditions of No. 3 are satisfied. Let uu be a hermitian endomorphism of EE and let ∏i=1n(X−λi)\prod_{i=1}^n (X-\lambda_i) be the decomposition into linear factors of its characteristic polynomial; suppose λi⩾λi+1\lambda_i \geqslant \lambda_{i+1} for 1⩽i⩽n−11 \leqslant i \leqslant n-1.

a) Now prove that the greatest (resp. the least) of the eigenvalues λi\lambda_i in KK is equal to the greatest (resp. the least) of the values of Φ(u(x),x)\Phi(u(x), x) when xx ranges over the set of the x∈Ex \in E such that Φ(x,x)=1\Phi(x, x) = 1. (Reason directly, or apply Exercise 16 c) by reducing to the case where A=K(i)A = K(i) (§3§ 3, Exercise 4).)

b) Let Ψv\Psi_v be the restriction to a vector subspace VV of EE of the hermitian form Ψ′\Psi' associated with uu, and let uvu_v be the hermitian endomorphism of VV associated with Ψv\Psi_v. Now prove that λk\lambda_k is the smallest of the largest eigenvalues of the uvu_v, when VV runs through the set of vector subspaces of EE of dimension n−k+1n-k+1 (use prop. 5).

Remark 22

Suppose that the conditions of No. 3 are fulfilled, and in addition that AA is equal to K(i)K(i) or to the field of quaternions over KK. Let u,vu, v be two normal endomorphisms of EE; let (Ei)1⩽i⩽r(E_i)_{1 \leqslant i \leqslant r} (resp. (Fj)1⩽j⩽s(F_j)_{1 \leqslant j \leqslant s}) be the decomposition of EE into a direct sum of pairwise orthogonal subspaces, such that in EiE_i (resp. FjF_j) there is an orthonormal basis formed of eigenvectors of uu (resp. vv) for the same eigenvalue λi\lambda_i (resp. μj\mu_j), and that λh\lambda_h and λi\lambda_i (resp. μj\mu_j and μk\mu_k) are not transformed into one another by an inner automorphism of AA if h≠ih \neq i (resp. j≠kj \neq k) (cf. prop. 4 and exerc. 9). In order that an endomorphism ww of EE be such that uw=vwuw = vw, it is necessary and sufficient that for every jj (1⩽j⩽s1 \leqslant j \leqslant s), w(Fj)w(F_j) be contained in one of the EiE_i and that the image by ww of every eigenvector of vv corresponding to the eigenvalue μj\mu_j be an eigenvector of uu corresponding to the eigenvalue μj\mu_j (which in particular implies that μj\mu_j and λi\lambda_i are transformed into one another by an inner automorphism of AA). Deduce that if this is so, then u∗w=wv∗u^*w = wv^*.

Remark 23

Suppose that the conditions of No. 3 are fulfilled. Let uu and vv be two endomorphisms of EE.

a) Suppose that uu and uvuv are normal. In order that vuvu be normal, it is necessary and sufficient that vv and u∗uu^*u be commutable. (To see that the condition is necessary, use the relation u(vu)=(uv)uu(vu) = (uv)u and exerc. 22; to see that it is sufficient, use exerc. 14 a) and 10 d).)

b) Suppose that u,vu, v and uvuv are normal; let β\beta be the greatest eigenvalue of uu∗uu^*, and let FF be the subspace of EE formed by the eigenvectors of uu∗uu^* corresponding to the eigenvalue β\beta. Now prove that v(F)⊂Fv(F) \subset F. (Remark that for every normal endomorphism uu and every x∈Ex \in E, one has

Φ(u(x),u(x))=Φ(u∗(x),u∗(x)). \Phi(u(x), u(x)) = \Phi(u^*(x), u^*(x)).
)

Reduce to the case where A is equal to K(i) or to the quaternion field over K; F then admits a basis formed by eigenvectors for u (and u*); remark that for such a vector z, one has Φ(u∗uv(z),v(z))=βΦ(v(z),v(z))\Phi(u^*u v(z), v(z)) = \beta \Phi(v(z), v(z)). Deduce that νu is normal (reason by induction on the number of distinct eigenvalues of u∗uu^*u). If h (resp. h′h') is the positive hermitian endomorphism such that h2=uu∗h^2 = uu^* (resp. h′2=νν∗{h'}^2 = \nu \nu^*) and if one sets u=hu1,ν=h′ν1u = hu_1, \nu = h'\nu_1, where u1u_1 and ν1\nu_1 are unitary, h permutable with u1u_1 and h′h' with ν1\nu_1 (exerc. 14 a)), prove that the pairs (h,h′),(h,ν1)(h, h'), (h, \nu_1) and (h′,u1)(h', u_1) are permutable; converse. Deduce that umνn,νnum,uν∗u^m \nu^n, \nu^n u^m, u \nu^* and ν∗u\nu^* u are then normal (mm and nn arbitrary integers >0> 0).

Remark 24

Suppose that the conditions of No. 3 are fulfilled. Let Γ\Gamma be a group of automorphisms of E such that every u∈Γu \in \Gamma is normal. Now prove that there exists a decomposition of E into direct sum of subspaces EkE_k (1≤k≤r1 \leq k \leq r) pairwise orthogonal, such that the restriction to EkE_k of every u∈Γu \in \Gamma is of the form λkνk\lambda_k \nu_k, where λk\lambda_k is an element >0> 0 of K and where νk\nu_k is a unitary endomorphism of EkE_k (decompose each u∈Γu \in \Gamma in the form hνh \nu, where ν\nu is unitary, h positive hermitian and h2=uu∗h^2 = uu^* (exerc. 14 a)); use exerc. 23 b) and apply cor. 2 of th. 2 to the algebra generated by the hermitian endomorphisms h corresponding to the u∈Γu \in \Gamma. Deduce that if Γ\Gamma is finite, the elements u∈Γu \in \Gamma are unitary.

Remark 25

Suppose that A=KA = K (maximal ordered field). Let L be an euclidean space of dimension nn over A, whose metric form is positive non-degenerate.

Let S be a non-degenerate affine quadric in L (§ 6, exerc. 25). If S admits a center aa and if one takes aa for origin in L, now prove that there exists an orthonormal basis (ei)(e_i) for L such that, with respect to this basis, S has for equation λ1ξ12+⋯+λnξn2=1\lambda_1 \xi_1^2 + \cdots + \lambda_n \xi_n^2 = 1. Moreover, if two orthonormal bases have this property, the elements λi∈K\lambda_i \in K corresponding to them are the same up to order.

If S has no center, show that there exists a point bb of S and (taking bb as origin) an orthonormal basis for L such that, with respect to this basis, S has the equation λ1ξ12+⋯+λn−1ξn−12+ξn=0\lambda_1 \xi_1^2 + \cdots + \lambda_{n-1} \xi_{n-1}^2 + \xi_n = 0. (If S‾\overline{S} is the projective quadric such that S=L∩S‾S = L \cap \overline{S}, determine bb by the condition that the line passing through bb and cc be perpendicular to the tangent hyperplane to S at the point bb, where c is the (at infinity) pole with respect to S‾\overline{S} of the hyperplane at infinity H0H_0).

Remark 26

a) Let K be a commutative field, S a subset of K such that K is a maximal S-orderable field (chap. VI, § 2, exerc. 8). Let ff be a polynomial of K[X]K[X], L its field of roots. Show that if, for every (total) order structure on K compatible with its ring structure, L admits a structure of an ordered extension of K, then necessarily L=KL = K. (Argue by contradiction: proceeding as in exerc. 8 e) of chap. VI, § 2, reduce to the case where one would have [L:K]=2[L : K] = 2. Conclude by observing that if b∈Kb \in K is not a square, there exists a total order structure on K, compatible with its ring structure, for which b<0b < 0 (cf. chap. VI, § 2, no. 3, lemma of th. 1)).

b) Extend the results of No. 3 (with the exception of prop. 6) to the case where K is a maximal S-orderable field (). (Begin by proving the analogue of prop. 5, using a). Establish next the analogue of cor. 2 of th. 2 for the case where the commutative algebra B consists of hermitian endomorphisms, using prop. 10 of chap. VIII, § 9, no. 4. Pass to the case of a normal endomorphism u for A = K(i), observing that one can then write u=v+iwu = v + i w, where v and w are hermitian and permutable. Finally, if A is the field of quaternions over K, E0 the space E considered as a vector space of dimension 2n over K(i), and if one sets Φ(x,y)=Φ1(x,y)+Φ2(x,y)i\Phi(x, y) = \Phi_1(x, y) + \Phi_2(x, y)i, where Φ1\Phi_1 and Φ2\Phi_2 take their values in K(i), observe that if u is normal for Φ\Phi, it is also normal for Φ1\Phi_1.)

Remark 27

Let K be a maximal ordered field, E a vector space of dimension n over K, Φ\Phi a non-degenerate symmetric bilinear form on E, of signature (s, t) distinct from (n, 0) and from (0, n). Let (ei)(e_i) be an orthogonal basis for Φ\Phi, such that Φ(ei,ei)=1\Phi(e_i, e_i) = 1 for 1≤i≤s1 \leq i \leq s, Φ(ei,ei)=−1\Phi(e_i, e_i) = -1 for s+1≤i≤ns+1 \leq i \leq n. For every orthogonal transform u∈U(Φ)u \in \mathbf{U}(\Phi), let

U=(MNPQ) U = \begin{pmatrix} M & N \\ P & Q \end{pmatrix}

be the matrix of u with respect to (ei)(e_i), written in the form of a square tableau of matrices corresponding to the partition of (1,n)(1, n) into (1,s)(1, s) and (s+1,n)(s+1, n).

a) Prove the relations

tM⋅M−tP⋅P=IstQ⋅Q−tN⋅N=IttM⋅N−tP⋅Q=0. \begin{align*} {}^tM \cdot M - {}^tP \cdot P &= I_s \\ {}^tQ \cdot Q - {}^tN \cdot N &= I_t \\ {}^tM \cdot N - {}^tP \cdot Q &= 0. \end{align*}

b) Let R be a matrix over K with t rows and s columns, such that Is−tR⋅RI_s - {}^tR \cdot R is the matrix of a positive non-degenerate hermitian form (on KsK^s). Show that det⁡(M+λNR)\det(M + \lambda NR) does not change sign for −1≤λ≤1-1 \leq \lambda \leq 1 in K (show, using a), that t(M+λNR)(M+λNR){}^t(M + \lambda NR)(M + \lambda NR) is the matrix of a positive non-degenerate symmetric form).

c) Put σ(u)=σ(U)=sgn⁡(det⁡M)\sigma(u) = \sigma(U) = \operatorname{sgn}(\det M); show that, for any two elements u,vu, v of the orthogonal group U(Φ)\mathbf{U}(\Phi), one has σ(uv)=σ(u)σ(v)\sigma(uv) = \sigma(u)\sigma(v) (use a) and b)). Deduce that the commutator group of the special orthogonal group SU(Φ)\mathbf{SU}(\Phi) is distinct from SU(Φ)\mathbf{SU}(\Phi) (cf. § 10, exerc. 9).

Machine translation of the English, by 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.