“…The real part and, referring to (16), is therefore distributed with zero mean and variance Since the are independent, and assuming that the variance of the 's with respect to is small (i.e., the atoms are approximately of the same atomic number), the central limit theorem may be applied to (7) (provided that is large), so that (17) where is defined by (18) The same distribution applies to Equation (17) may be used to obtain and The real and imaginary parts are independent [16], so that (19) is a function of the amplitude but is independent of the phase and may be obtained as (20) Note that, referring to (8) and (18), is a function of in general. However, since the atomic electron densities are, to a very good approximation, spherically symmetric, so too are the atomic scattering factors in reciprocal space.…”