Using a paraxial analysis, Shelankov (1998 Europhys. Lett. 43 623) has show
n that charged particles in a beam of small angular width l/w, aimed at a m
agnetic flux line with quantum flux a, are deflected through an angle D pro
portional to sin(2 pi alpha)/w, vanishing in the classical limit and also v
anishing if the incident beam has zero intensity at the flux line. These pr
operties are confirmed by numerical calculations based on an exact solution
of the Schrodinger equation, and the paraxial wavefunction is obtained as
an asymptotic approximation for large iv. Paraxial theory suggests that the
same deflection will occur for a light beam reflected by a mirror containi
ng a step of height pi alpha. A theory of this optical phenomenon, based on
an exact solution (for which D is not periodic in alpha), shows that conve
rgence to the paraxial D is fast for alpha << 1, and slow for alpha near 1/
2.