English

Block perturbation of symplectic matrices in Williamson's theorem

Functional Analysis 2024-08-22 v2 Mathematical Physics math.MP Quantum Physics

Abstract

Williamson's theorem states that for any 2n×2n2n \times 2n real positive definite matrix AA, there exists a 2n×2n2n \times 2n real symplectic matrix SS such that STAS=DDS^TAS=D \oplus D, where DD is an n×nn\times n diagonal matrix with positive diagonal entries which are known as the symplectic eigenvalues of AA. Let HH be any 2n×2n2n \times 2n real symmetric matrix such that the perturbed matrix A+HA+H is also positive definite. In this paper, we show that any symplectic matrix S~\tilde{S} diagonalizing A+HA+H in Williamson's theorem is of the form S~=SQ+O(H)\tilde{S}=S Q+\mathcal{O}(\|H\|), where QQ is a 2n×2n2n \times 2n real symplectic as well as orthogonal matrix. Moreover, QQ is in symplectic block diagonal\textit{symplectic block diagonal} form with the block sizes given by twice the multiplicities of the symplectic eigenvalues of AA. Consequently, we show that S~\tilde{S} and SS can be chosen so that S~S=O(H)\|\tilde{S}-S\|=\mathcal{O}(\|H\|). Our results hold even if AA has repeated symplectic eigenvalues. This generalizes the stability result of symplectic matrices for non-repeated symplectic eigenvalues given by Idel, Gaona, and Wolf [Linear Algebra Appl., 525:45-58, 2017\textit{Linear Algebra Appl., 525:45-58, 2017}].

Keywords

Cite

@article{arxiv.2307.01078,
  title  = {Block perturbation of symplectic matrices in Williamson's theorem},
  author = {Gajendra Babu and Hemant K. Mishra},
  journal= {arXiv preprint arXiv:2307.01078},
  year   = {2024}
}

Comments

13 pages, accepted in Canadian Mathematical Bulletin, the title shortened, some minor changes were made to the previous version and typos were fixed