نتایج جستجو برای: weyl titchmarsh m function

تعداد نتایج: 1689316  

Journal: :Journal of Mathematical Analysis and Applications 2004

2003
FRITZ GESZTESY

We construct a class of matrix-valued Schrödinger operators with prescribed finite-band spectra of maximum spectral multiplicity. The corresponding matrix potentials are shown to be stationary solutions of the KdV hierarchy. The methods employed in this paper rely on matrix-valued Herglotz functions, Weyl–Titchmarsh theory, pencils of matrices, and basic inverse spectral theory for matrix-value...

2000
FRITZ GESZTESY BARRY SIMON

We provide a new short proof of the following fact, first proved by one of us in 1998: If two Weyl-Titchmarsh m-functions, m j (z), of two Schrödinger operators H j = − d 2 dx 2 + q j , j = 1, 2 in L 2 ((0, R)), 0 < R ≤ ∞, are exponentially close, that is, |m 1 (z) − m 2 (z)| = |z|→∞ O(e −2 Im(z 1/2)a), 0 < a < R, then q 1 = q 2 a.e. on [0, a]. The result applies to any boundary conditions at x...

Journal: :SIAM Journal of Applied Mathematics 2015
Jon Wilkening Antoine J. Cerfon

We develop a spectrally accurate numerical method to compute solutions of a model PDE used in plasma physics to describe diffusion in velocity space due to Fokker–Planck collisions. The solution is represented as a discrete and continuous superposition of normalizable and nonnormalizable eigenfunctions via the spectral transform associated with a singular Sturm–Liouville operator. We present a ...

2007
BARRY SIMON

We continue the study of the A-amplitude associated to a half-line d2 Schrodinger operator, -=t 4 in L2((0, b ) ) , b 5 oo.A is related to the iieylTitchmarsh m-function via m(-fi2) = A(a)e-2ff" d c x + ~ ( e ( ~ ~ & ) " ) -6-J: for all E > 0. We discuss five issues here. First, we extend the theory to general q in L1((O, a ) ) for all a , including q's which are limit circle at infinity. Secon...

2000
FRITZ GESZTESY

We continue the study of the A-amplitude associated to a half-line Schrödinger operator, − d dx + q in L((0, b)), b ≤ ∞. A is related to the Weyl-Titchmarsh m-function via m(−κ2) = −κ− ∫ a 0 A(α)e −2ακ dα+O(e) for all ε > 0. We discuss five issues here. First, we extend the theory to general q in L((0, a)) for all a, including q’s which are limit circle at infinity. Second, we prove the followi...

Journal: :Journal of Differential Equations 2022

We consider canonical systems (with 2 p × Hamiltonians H ( x ) ≥ 0 ), which correspond to matrix string equations. Direct and inverse problems are solved in terms of Titchmarsh–Weyl spectral functions related S -nodes. Procedures for solving given.

2011
Jonathan Eckhardt Gerald Teschl

We provide an abstract framework for singular one-dimensional Schrödinger operators with purely discrete spectra to show when the spectrum plus norming constants determine such an operator completely. As an example we apply our findings to prove a new uniqueness results for perturbed quantum mechanical harmonic oscillators. In addition, we also show how to establish a Hochstadt–Liebermann type ...

2012
Jonathan Eckhardt Gerald Teschl

We provide an abstract framework for singular one-dimensional Schrödinger operators with purely discrete spectra to show when the spectrum plus norming constants determine such an operator completely. As an example we apply our findings to prove new uniqueness results for perturbed quantum mechanical harmonic oscillators. In addition, we also show how to establish a Hochstadt–Lieberman type res...

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