Abstract

We explicitly compute the spectrum and eigenfunctions of the magnetic Schrödinger operator H(A,V)=(i+A)2+V in L2(2), with Aharonov-Bohm vector potential, A(x1,x2)=α(x2,x1)/|x|2, and either quadratic or Coulomb scalar potential V. We also determine sharp constants in the CLR inequality, both dependent on the fractional part of α and both greater than unity. In the case of quadratic potential, it turns out that the LT inequality holds for all γ1 with the classical constant, as expected from the nonmagnetic system (harmonic oscillator).