2003 Volume 39 Issue 2 Pages 297-330
In this paper we consider the two-dimensional Schrödinger operatorof the form:
HV=−\frac{∂2}{∂x12}+(\frac{1}{i}\frac{∂}{∂x2}−b(x1))2+V(x1, x2),
where the magnetic field B(x1)=rot(0, b(x1)) is monotone increasing and steplike, namely the limits limx1→±∞ B(x1)=B± exist with 0<B−<B+<∞, and V is the slowly power-decaying electric potential. The spectrum σ(H0) of the unperturbed operator H0 (=HV with V=0) has the band structure and HV has the discrete spectrum in the gaps of the essential spectrum σess(HV)=σ(H0). The aim of this paper is to study the asymptotic distribution of the eigenvalues near the edges of the spectral gaps. Using the min-max argument, we prove that the classical Weyl-type asymptotic formula is satisfied under suitable assumptions on B and V.
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