On Titchmarsh-Weyl functions and eigenfunction expansions of first-order symmetric systems
arXiv:1303.6153 · doi:10.1007/s00020-013-2090-0
Abstract
We study general (not necessarily Hamiltonian) first-order symmetric systems $J y'(t)-B(t)y(t)=\D(t) f(t)$ on an interval $\cI=[a,b> $ with the regular endpoint . It is assumed that the deficiency indices $n_\pm(\Tmi)$ of the minimal relation $\Tmi$ in $\LI$ satisfy $n_-(\Tmi)\leq n_+(\Tmi)$. By using a Nevanlinna boundary parameter at the singular endpoint we define self-adjoint and -depending Nevanlinna boundary conditions which are analogs of separated self-adjoint boundary conditions for Hamiltonian systems. With a boundary value problem involving such conditions we associate the -function $m(\cd)$, which is an analog of the Titchmarsh-Weyl coefficient for the Hamiltonian system. By using -function we obtain the Fourier transform $V:\LI\to L^2(\Si)$ with the spectral function $\Si(\cd)$ of the minimally possible dimension. If is an isometry, then the (exit space) self-adjoint extension $\wt T$ of $\Tmi$ induced by the boundary problem is unitarily equivalent to the multiplication operator in $L^2(\Si)$; hence the spectrum of $\wt T$ is defined by the spectral function $\Si(\cd)$. We show that all the objects of the boundary problem are determined by the parameter , which enables us to parametrize all spectral function $\Si(\cd) $ immediately in terms of . Similar results for various classes of boundary problems were obtained by Kac and Krein, Fulton, Hinton and Shaw and other authors.