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Canonical systems whose Weyl coefficients have dominating real part

Matthias Langer, Raphael Pruckner, Harald Woracek

Abstract

For a two-dimensional canonical system $y'(t)=zJH(t)y(t)$ on the half-line $(0,\infty)$ whose Hamiltonian $H$ is a.e. positive semi-definite, denote by $q_H$ its Weyl coefficient. De Branges' inverse spectral theorem states that the assignment $H\mapsto q_H$ is a bijection between Hamiltonians (suitably normalised) and Nevanlinna functions. The main result of the paper is a criterion when the singular integral of the spectral measure, i.e. Re $q_H(iy)$, dominates its Poisson integral Im $q_H(iy)$ for $y\to+\infty$. Two equivalent conditions characterising this situation are provided. The first one is analytic in nature, very simple, and explicit in terms of the primitive $M$ of $H$. It merely depends on the relative size of the off-diagonal entries of $M$ compared with the diagonal entries. The second condition is of geometric nature and technically more complicated, but explicit in terms of $H$ itself. It involves the relative size of the off-diagonal entries of $H$, a measurement for oscillations of the diagonal of $H$, and a condition on the speed and smoothness of the rotation of $H$.

Canonical systems whose Weyl coefficients have dominating real part

Abstract

For a two-dimensional canonical system on the half-line whose Hamiltonian is a.e. positive semi-definite, denote by its Weyl coefficient. De Branges' inverse spectral theorem states that the assignment is a bijection between Hamiltonians (suitably normalised) and Nevanlinna functions. The main result of the paper is a criterion when the singular integral of the spectral measure, i.e. Re , dominates its Poisson integral Im for . Two equivalent conditions characterising this situation are provided. The first one is analytic in nature, very simple, and explicit in terms of the primitive of . It merely depends on the relative size of the off-diagonal entries of compared with the diagonal entries. The second condition is of geometric nature and technically more complicated, but explicit in terms of itself. It involves the relative size of the off-diagonal entries of , a measurement for oscillations of the diagonal of , and a condition on the speed and smoothness of the rotation of .

Paper Structure

This paper contains 13 sections, 16 theorems, 109 equations.

Key Result

Theorem 1.1

Let $H$ be a Hamiltonian defined on the interval $(0,\infty)$ such that G1 holds and neither $h_1$ nor $h_2$ vanishes a.e. on some neighbourhood of the left endpoint $0$. Then the following statements are equivalent.

Theorems & Definitions (40)

  • Theorem 1.1
  • Remark 1.3
  • Theorem 1.4
  • Example 1.6
  • Example 1.7
  • Definition 2.1
  • Remark 2.2
  • Lemma 2.3
  • proof
  • Lemma 2.4
  • ...and 30 more