Suppose that the density fluctuations δ(r) in the early universe constitute a Gaussian field with a power spectrum P(k) that equals zero above some maximum wavenumber kmax. This maximum wavenumber corresponds to a minimum length scale rmin=2π/kmax and a minimum mass scale Mmin=(4π/3)ρmrmin3. Show that for M<Mmin, the mean square mass fluctuation, ⟨(δM/M)2⟩, is equal to σδ2 for the density field.