Bourbaki

Remark 2

Tag 0DM4, permanent. Cite it as [Bourbaki, Tag 0DM4].

Algebra, chapter IX, § 7. Formes hermitiennes et corps ordonnés

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).

Bourbaki puts the proof directly after the statement, so what is above is the statement and its proof together.

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