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Hermitian eigenvalues move by at most the spectral norm perturbation

Statement

Let A,E∈Cn×n be Hermitian, and order their real eigenvalues decreasingly as λ1(A)≥⋯≥λn(A), λ1(E)≥⋯≥λn(E), and likewise for A+E. Then for every 1≤k≤n,

∣λk(A+E)−λk(A)∣≤∥E∥2.

Facts & Assumptions

Given: Hermitian A,E and the ordered eigenvalues in the statement.

[F1]

Realification duplicates each Hermitian eigenvalue and preserves operator 2-norms (Realification preserves Hermitian spectra, norms, and congruence).

[F2]

Weyl's two-sided eigenvalue inequalities hold for real self-adjoint sums (Weyl inequalities bound the eigenvalues of a sum of self-adjoint endomorphisms).

[F3]

The operator norm is induced by the Euclidean vector norm (The operator norm is zero on the zero domain and otherwise is max_{||v||=1} ||Tv||).

Proof

1.1givenF1F2

Realify A and E. Their eigenvalues in decreasing order repeat each complex eigenvalue twice, so the 2k-th eigenvalue of R(A) is λk(A) and similarly for E and A+E. By [F2] with indices i=2k,j=1, the upper Weyl inequality gives λ2k(R(A+E))≤λ2k(R(A))+λ1(R(E)). With i=2k,j=2n, the lower inequality gives λ2k(R(A+E))≥λ2k(R(A))+λ2n(R(E)).

2.1givenF1F3step 1.1algebra∎

For a unit eigenvector u of the Hermitian E, ∣λ∣=∥Eu∥2≤∥E∥2 by [F3]. Hence −∥E∥2≤λ2n(R(E)) and λ1(R(E))≤∥E∥2 by [F1]. Step 1.1 places λk(A+E)−λk(A) between these two bounds, proving the result.

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