Bourbaki

Lemma 4

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

Lie Groups and Lie Algebras, chapter V, § 3. Groups of displacements generated by reflections

Let Q=(qij)Q = (q_{ij}) be a real, symmetric, square matrix of order nn such that: a) qij≤0q_{ij} \leq 0 for i≠ji \neq j; b) there does not exist a partition of {1,2,…,n}\{1, 2, \ldots, n\} into two non-empty subsets I and J such that (i,j)∈I×J(i, j) \in I \times J implies qij=0q_{ij} = 0; c) the quadratic form q(x1,…,xn)=∑i,jqijxixjq(x_1, \ldots, x_n) = \sum_{i,j} q_{ij} x_i x_j on Rn\mathbf{R}^n is positive.

Then: (i) The kernel N of q is of dimension 0 or 1. If dim⁡N=1\dim N = 1, N is generated by a vector all of whose coordinates are > 0. (ii) The smallest eigenvalue of Q is of multiplicity 1 and a corresponding eigenvector has all its coordinates > 0 or all its coordinates < 0.

Since q is a positive quadratic form, the kernel N of q is the set of isotropic vectors for q (Algebra, Chap. IX, § 7, no. 1, Cor. of Prop. 2). Let a1,…,ana_1, \ldots, a_n be the canonical basis of Rn\mathbf{R}^n. If ∑iciai∈N\sum_i c_i a_i \in N, Lemma 3 shows that we also have ∑i∣ci∣ai∈N\sum_i |c_i| a_i \in N, and hence ∑iqji∣ci∣=0\sum_i q_{ji} |c_i| = 0 for all j. Let I be the set of i such that ci≠0c_i \neq 0. If j∉Ij \notin I, then qji∣ci∣≤0q_{ji} |c_i| \leq 0 for i∈Ii \in I and qji∣ci∣=0q_{ji} |c_i| = 0 for i∉Ii \notin I, so qji=0q_{ji} = 0 for j∉Ij \notin I and i∈Ii \in I. Assumption b) thus implies that either I=∅I = \varnothing or I={1,…,n}I = \{1, \ldots, n\}. Consequently, every non-zero vector in N has all its coordinates ≠0\neq 0. If dim⁡N≥2\dim N \geq 2, the intersection of N with the hyperplane with equation xi=0x_i = 0 would be of dimension ≥1\geq 1, contrary to what we have just shown. The preceding argument also shows that, if dim⁡N=1\dim N = 1, then N contains a vector all of whose coordinates are > 0. This proves (i).

On the other hand, we know that the eigenvalues of Q are real (Algebra, Chap. IX, § 7, no. 3, Prop. 5) and positive since q is positive. Let λ\lambda be the smallest of them. The matrix Q′=Q−λInQ' = Q - \lambda I_n is then the matrix of a degenerate positive form q′q' and the off-diagonal elements of Q′Q' are the same as those of Q. Consequently, Q′Q' satisfies conditions a), b) and c) of the statement of the lemma. Since the kernel N′N' of q′q' is the eigenspace of Q corresponding to the eigenvalue λ\lambda, assertion (ii) follows from (i).

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

Cited by

Cites

  • Algebra, Chap. IX, § 7, no. 1, Cor. of Prop. 2 not yet on this site: A IX
  • Algebra, Chap. IX, § 7, no. 3, Prop. 5 not yet on this site: A IX
  • Lemma 3
Transcribed from the printed volume. Not translated.