Bourbaki

Proposition 3

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

Algebra, chapter IX, § 4. Sous-espaces totalement isotropes. Théorème de Witt

*Let Φ\Phi be a non-degenerate ε\varepsilon-hermitian form satisfying (T) (resp. the bilinear form associated with a non-degenerate quadratic form Q). Let F1F_1 and F2F_2 be two maximal totally isotropic (resp. totally singular) subspaces of E, one of them being finite-dimensional. Put F=F1∩F2F = F_1 \cap F_2. Let Si (i=1,2)S_i \ (i = 1, 2) be a supplementary subspace to FF in FiF_i; put S=S1+S2S = S_1 + S_2. Then there exist two subspaces G and H of E such that a) The subspaces G+F,SG + F, S and H are non-isotropic and pairwise orthogonal; b) E is the direct sum of F, S, G and H; c) There is no nonzero isotropic (resp. singular) vector in H; d) G is totally isotropic (resp. totally singular). Moreover F1F_1 and F2F_2 are both finite-dimensional and we have dim F1=dim⁡F2,dim⁡G=dim⁡F,dim⁡S1=dim⁡S2,codim⁡H=2dim⁡F1F_1 = \dim F_2, \dim G = \dim F, \dim S_1 = \dim S_2, \operatorname{codim} H = 2 \dim F_1.

First observe that, if NN is a maximal totally isotropic (resp. totally singular) subspace, then every isotropic (resp. singular) vector xx orthogonal to NN is an element of NN, since otherwise N+AxN + Ax would contradict the maximal character of NN. Hence if, for i=1, 2, xii = 1,\ 2,\ x_i is an isotropic (resp. singular) vector of Fi0F_i^0, we have xi∈Fix_i \in F_i. On the other hand, if yy is an element of S1S_1 orthogonal to S2S_2, it is orthogonal to F1F_1 since F1F_1 is totally isotropic, hence to FF, and consequently to F2=S2+FF_2 = S_2 + F. Since yy is isotropic (resp. singular) and is orthogonal to F2F_2, we have

y∈S1∩F2=S1∩F1∩F2=S1∩F={0}. y \in S_1 \cap F_2 = S_1 \cap F_1 \cap F_2 = S_1 \cap F = \{0\}.

One therefore has S1∩S20={0}S_1 \cap S_2^0 = \{0\}, and analogously S2∩S10={0}S_2 \cap S_1^0 = \{0\}. Since one of the two subspaces F1,F2F_1, F_2, for example F1F_1, is finite-dimensional, S1S_1 is finite-dimensional, and hence S10S_1^0 is of finite codimension (§1,n∘6,cor. 1 de la prop. 4§ 1, \mathrm{n}^\circ 6, \mathrm{cor.\ 1\ de\ la\ prop.\ 4}), and consequently S2S_2 is finite-dimensional since S2∩S10={0}S_2 \cap S_1^0 = \{0\}; moreover this shows that dim⁡S2⩽codim⁡S10=dim⁡S1\dim S_2 \leqslant \operatorname{codim} S_1^0 = \dim S_1; analogously dim⁡S1⩽dim⁡S2\dim S_1 \leqslant \dim S_2, whence dim⁡S1=dim⁡S2\dim S_1 = \dim S_2. Prop. 2 a) then shows that S=S1+S2S = S_1 + S_2 is non-isotropic.

Now the orthogonal NN of SS is non-isotropic (n∘1,cor. de la prop. 1\mathrm{n}^\circ 1, \mathrm{cor.\ de\ la\ prop.\ 1}) and contains FF; Cor. 1 of Prop. 2 therefore shows that there exists a subspace GG totally isotropic (resp. totally singular) of NN such that dim⁡G=dim⁡F\dim G = \dim F, that G∩F={0}G \cap F = \{0\} and that G+FG + F is non-isotropic. Thus d) is satisfied by GG. We shall then satisfy a) and b) by taking for HH the orthogonal of G+FG + F in NN. As for c), we note that, since HH is orthogonal to F1=S1+FF_1 = S_1 + F, there is no nonzero isotropic (resp. singular) vector in HH by virtue of what was noted at the beginning of the proof and of the fact that H∩F1={0}H \cap F_1 = \{0\}. Finally some of the assertions concerning dimensions have been proved along the way; the others follow from them trivially.

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

Cited by

Nothing.

Cites

Nothing.

Translated with machine help, not yet reviewed by a person.