A particle of mass $m$ and charge $q$ is constrained to move in the $x y$ plane on a circular orbit of radius $\rho$ around the origin 0 , as in Problem 2, and a magnetic field, represented by the vector potential $\mathbf{A}=\Phi \hat{\mathbf{k}} \times \mathbf{r} /\left[2 \pi(\hat{\mathbf{k}} \times \mathbf{r})^2\right]$, is imposed.
(a) Show that the magnetic field approximates that of a long thin solenoid with flux $\Phi$ placed on the $z$ axis.
(b) Determine the energy spectrum in the presence of the field and show that it coincides with the spectrum for $\Phi=0$ if the flux assumes certain quantized values. Note that the energy levels depend on the strength of a magnetic field $\mathbf{B}$ which differs from zero only in a region into which the particle cannot penetrate (the AharonovBohm effect).