Dirichlet and Neumann Eigenvalues for Half-Plane Magnetic Hamiltonians

preprint2012arXivOpen access

Abstract

Let H0,DH_{0, D} (resp., H0,NH_{0,N}) be the Schroedinger operator in constant magnetic field on the half-plane with Dirichlet (resp., Neumann) boundary conditions, and let Hℓ:=H0,ℓ−VH_\ell : = H_{0, \ell} - V, ℓ=D,N\ell =D,N, where the scalar potential VV is non negative, bounded, does not vanish identically, and decays at infinity. We compare the distribution of the eigenvalues of HDH_D and HNH_N below the respective infima of the essential spectra. To this end, we construct effective Hamiltonians which govern the asymptotic behaviour of the discrete spectrum of HℓH_\ell near inf⁡σess(Hℓ)=inf⁡σ(H0,ℓ)\inf σ_{ess}(H_\ell) = \inf σ(H_{0,\ell}), ℓ=D,N\ell = D,N. Applying these Hamiltonians, we show that σdisc(HD)σ_{disc}(H_D) is infinite even if VV has a compact support, while σdisc(HN)σ_{disc}(H_N) could be finite or infinite depending on the decay rate of VV.

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