“…One must remember that the whole problem is solved as an initial value problem, so that the knowledge of every function near the time origin is essential for finding the solution. To overcome this difficulty a different series expansion for the electric field components appearing in the right-hand side of equations (3), ( 4) and (5) has been derived (NALESSO, 1984) and then an approximate expression has been used which is valid when the elapsed time is shorter than the resistive diffusion time through a plane slab zd = A:,UOO.M for modes with long wavelengths ( A l k + 1) or, less restrictively, for short wavelengths, when t < AlrwpooM.…”