“…The reason to have projection matrices P ϕ is the asymptotic behavior of solutions to (2). Indeed, de Branges, Krein and Langer [7,19] showed that solutions to (10)…”
Section: Schrödinger Canonical Systemsmentioning
confidence: 99%
“…It is well known that Weyl theory can be applied to a canonical system in a similar way to that for Schrödinger operators (see e.g. [2]). More precisely, it is possible to choose f n = (f n,1 , f n,2 ) t which are H n -integrable solutions to (10)…”
Section: Piecewise Linear Functionsmentioning
confidence: 99%
“…To be self-contained we are going to prove Proposition 5.1 by following the argument in [2]. The extension of his argument from H to H, however, is necessary, especially to deal with ∞.…”
Section: Appendix a Proof Of Proposition 51mentioning
confidence: 99%
“…The extension of his argument from H to H, however, is necessary, especially to deal with ∞. As a cost of this extension, the proof becomes much longer than that in [2].…”
Section: Appendix a Proof Of Proposition 51mentioning
We show that the Herglotz functions that arise as Weyl-Titchmarsh m functions of one-dimensional Schrödinger operators are dense in the space of all Herglotz functions with respect to uniform convergence on compact subsets of the upper half plane. This result is obtained as an application of de Branges theory of canonical systems.
“…The reason to have projection matrices P ϕ is the asymptotic behavior of solutions to (2). Indeed, de Branges, Krein and Langer [7,19] showed that solutions to (10)…”
Section: Schrödinger Canonical Systemsmentioning
confidence: 99%
“…It is well known that Weyl theory can be applied to a canonical system in a similar way to that for Schrödinger operators (see e.g. [2]). More precisely, it is possible to choose f n = (f n,1 , f n,2 ) t which are H n -integrable solutions to (10)…”
Section: Piecewise Linear Functionsmentioning
confidence: 99%
“…To be self-contained we are going to prove Proposition 5.1 by following the argument in [2]. The extension of his argument from H to H, however, is necessary, especially to deal with ∞.…”
Section: Appendix a Proof Of Proposition 51mentioning
confidence: 99%
“…The extension of his argument from H to H, however, is necessary, especially to deal with ∞. As a cost of this extension, the proof becomes much longer than that in [2].…”
Section: Appendix a Proof Of Proposition 51mentioning
We show that the Herglotz functions that arise as Weyl-Titchmarsh m functions of one-dimensional Schrödinger operators are dense in the space of all Herglotz functions with respect to uniform convergence on compact subsets of the upper half plane. This result is obtained as an application of de Branges theory of canonical systems.
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