If AA is compact and selfadjoint on a Hilbert space, there is an orthonormal basis of eigenvectors {ek}\{e_k\} with Aek=λkekAe_k=\lambda_k e_k, λkR\lambda_k\in\mathbb R, and λk0\lambda_k\to0.

Remarks

Key properties (paper use):

k(2λk/(λk2+1))1/2\prod_k (2\lambda_k/(\lambda_k^2+1))^{1/2} (Lemma 3.2).

  • Ensures existence of "eigensystems" used in continuity arguments (Lemma 2.4).
Examples
  • A diagonal operator on 2\ell^2 with diagonal entries λk0\lambda_k\to0.