English

Characterization of Weyl functions in the class of operator-valued generalized Nevanlinna functions

Functional Analysis 2025-03-25 v5 Classical Analysis and ODEs

Abstract

We provide the necessary and sufficient conditions for a generalized Nevanlinna function QQ (QNκ(H)Q\in N_{\kappa }\left( \mathcal{H} \right)) to be a Weyl function (also known as a Weyl-Titchmarch function). We also investigate an important subclass of Nκ(H)N_{\kappa }(\mathcal{H}), the functions that have a boundedly invertible derivative at infinity Q():=limzzQ(z)Q'\left( \infty \right):=\lim \limits_{z \to \infty}{zQ(z)}. These functions are regular and have the operator representation Q(z)=Γ~+(Az)1Γ~,zρ(A)Q\left( z \right)=\tilde{\Gamma}^{+}\left( A-z \right)^{-1}\tilde{\Gamma},z\in \rho \left( A \right), where AA is a bounded self-adjoint operator in a Pontryagin space K\mathcal{K}. We prove that every such strict function QQ is a Weyl function associated with the symmetric operator S:=A(IP)KS:=A_{\vert (I-P)\mathcal{K}}, where PP is the orthogonal projection, P:=Γ~(Γ~+Γ~)1Γ~+P:=\tilde{\Gamma} \left( \tilde{\Gamma}^{+} \tilde{\Gamma} \right)^{-1} \tilde{\Gamma}^{+} . Additionally, we provide the relation matrices of the adjoint relation S+S^{+} of SS, and of A^\hat{A}, where A^\hat{A} is the representing relation of Q^:=Q1\hat{Q}:=-Q^{-1}. We illustrate our results through examples, wherein we begin with a given function QNκ(H)Q\in N_{\kappa }\left( \mathcal{H} \right) and proceed to determine the closed symmetric linear relation SS and the boundary triple Π\Pi so that QQ becomes the Weyl function associated with Π\Pi.

Keywords

Cite

@article{arxiv.2102.06931,
  title  = {Characterization of Weyl functions in the class of operator-valued generalized Nevanlinna functions},
  author = {Muhamed Borogovac},
  journal= {arXiv preprint arXiv:2102.06931},
  year   = {2025}
}

Comments

23 pages, Accepted in Sarajevo Journal of Mathematics