“…We use a simple but physically reasonable model [22,23,24,25,26] which treats the fullerene as a spherical shell of a finite width, ∆R = R 2 − R 1 (where R 1,2 are the inner and the outer radii of the molecule, respectively). Interaction with an incident electron leads to the variation of the volume electron density, occurring inside the shell, and of the surface electron densities at the inner and the outer surfaces of the shell.…”