For canonical systems, the start of the essential spectrum is at least half and at most about 2.62 times that of the diagonal system, with the 1/2 factor optimal; the diagonal value itself is pinned by limsup/liminf integrals of sin²φ.
Canonical systems with discrete spectrum
1 Pith paper cite this work. Polarity classification is still indexing.
abstract
We study spectral properties of two-dimensional canonical systems $y'(t)=zJH(t)y(t)$, $t\in[a,b)$, where the Hamiltonian $H$ is locally integrable on $[a,b)$, positive semidefinite, and Weyl's limit point case takes place at $b$. We answer the following questions explicitly in terms of $H$: Is the spectrum of the associated selfadjoint operator discrete ? If it is discrete, what is its asymptotic distribution ? Here asymptotic distribution means summability and limit superior conditions relative to comparison functions growing sufficiently fast. Making an analogy with complex analysis, this corresponds to convergence class and type w.r.t.\ proximate orders having order larger than $1$. It is a surprising fact that these properties depend only on the diagonal entries of $H$. In 1968 L.de~Branges posed the following question as a fundamental problem: Which Hamiltonians are the structure Hamiltonian of some\\ de~Branges space ? We give a complete and explicit answer.
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The essential spectrum of canonical systems
For canonical systems, the start of the essential spectrum is at least half and at most about 2.62 times that of the diagonal system, with the 1/2 factor optimal; the diagonal value itself is pinned by limsup/liminf integrals of sin²φ.