“…The parameter N > 1 for the gaskets chosen here is a prime integer, while the initiator f(x; a) as well as the generator g(x; a) (Mandelbrot 1983) are given by the function ) in which the spatial frequencies used are u = wxo/ro c, v = wyo/r o c. Rewriting eqn (10) in the form (12) we immediately observe that qL(X O, t) at any given X o is a unifractal in time because the relationships (13 a,b) bear a strong analogy to eqns (9 a.b), Thus, it is seen that a dipole array which is bifractal in its spatial arrangement radiates a far-field which is also a bifractal in its spatial variations (Lakhtakia et al 1987). In addition, the time-dependent far-field response of this array turns out to a unifractal in time.…”