  We consider a one-dimensional loop of circumference $L$ crossed by a constant
magnetic flux $\Phi$ and connected to an infinite lead with coupling parameter
$\epsilon$. Assuming that the initial state $\psi_0$ of the particle is
confined inside the loop and evolves freely, we analyse the time evolution of
the nonescape probability $P(\psi_0,L,\Phi,\epsilon,t)$, which is the
probability that the particle will still be inside the loop at some later time
$t$.
