Eigenvalues of Robin Laplacians in infinite sectors
arXiv:1607.06848 · doi:10.1002/mana.201600314
Abstract
For , let denote the infinite planar sector of opening , \[ U_α=\big\{ (x_1,x_2)\in\mathbb R^2: \big|\arg(x_1+ix_2) \big|<α\big\}, \] and be the Laplacian in , , with the Robin boundary condition , where stands for the outer normal derivative and . The essential spectrum of does not depend on the angle and equals , and the discrete spectrum is non-empty iff . In this case we show that the discrete spectrum is always finite and that each individual eigenvalue is a continous strictly increasing function of the angle . In particular, there is just one discrete eigenvalue for . As approaches , the number of discrete eigenvalues becomes arbitrary large and is minorated by with a suitable , and the th eigenvalue of behaves as \[ E_n(T^γ_α)=-\dfrac{γ^2}{(2n-1)^2 α^2}+O(1) \] and admits a full asymptotic expansion in powers of . The eigenfunctions are exponentially localized near the origin. The results are also applied to -interactions on star graphs.
34 pages
References in corpus (4)
Cited by in corpus (6)
- On radial Schroedinger operators with a Coulomb potential
- Absence of eigenvalues of non-self-adjoint Robin Laplacians on the half-space
- Robin eigenvalues on domains with peaks
- Hydrogenoid spectra with central perturbations
- A numerical study of the Dirichlet-to-Neumann operator in planar domains
- On Schrödinger operators with -potentials supported on star graphs