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On generalization of Williamson's theorem to real symmetric matrices

Functional Analysis 2026-04-07 v2 Mathematical Physics math.MP Symplectic Geometry

Abstract

Williamson's theorem states that if AA is a 2n×2n2n \times 2n real symmetric positive definite matrix then there exists a 2n×2n2n \times 2n real symplectic matrix MM such that MTAM=DDM^T A M=D \oplus D, where DD is an n×nn \times n diagonal matrix with positive diagonal entries known as the symplectic eigenvalues of AA. The theorem is known to be generalized to 2n×2n2n \times 2n real symmetric positive semidefinite matrices whose kernels are symplectic subspaces of R2n\mathbb{R}^{2n}, in which case, some of the diagonal entries of DD are allowed to be zero. In this paper, we further generalize Williamson's theorem to 2n×2n2n \times 2n real symmetric matrices by allowing the diagonal elements of DD to be any real numbers, and thus extending the notion of symplectic eigenvalues to real symmetric matrices. Also, we provide an explicit description of symplectic eigenvalues, construct symplectic matrices achieving Williamson's theorem type decomposition, and establish perturbation bounds on symplectic eigenvalues for a class of 2n×2n2n \times 2n real symmetric matrices denoted by EigSpSm(2n)\operatorname{EigSpSm}(2n). The set EigSpSm(2n)\operatorname{EigSpSm}(2n) contains 2n×2n2n \times 2n real symmetric positive semidefinite whose kernels are symplectic subspaces of R2n\mathbb{R}^{2n}. Our perturbation bounds on symplectic eigenvalues for EigSpSm(2n)\operatorname{EigSpSm}(2n) generalize known perturbation bounds on symplectic eigenvalues of positive definite matrices given by Bhatia and Jain \textit{[J. Math. Phys. 56, 112201 (2015)]}.

Keywords

Cite

@article{arxiv.2408.04894,
  title  = {On generalization of Williamson's theorem to real symmetric matrices},
  author = {Hemant K. Mishra},
  journal= {arXiv preprint arXiv:2408.04894},
  year   = {2026}
}

Comments

21 pages; The revised version of the paper contains a new section dedicated to providing interpretations of the main results of the paper in a coordinate-free fashion. Several notations are modified to their standard counterparts and unnecessary emphasize on their descriptions are removed