“…The transferred momentum q is a 3 − d vector in the liquid, but it is only defined in two dimensions in the J E −k,−ω J E k,ω term. We overcame the same difficulty in Eq.s (45,47), by considering the convolution (with k− integration) as in Eq. (56) of Subsection III.B, which corresponds to averaging in space, but by assuming that the fluctuation correlations are localized within a volume ∼ ã2 .…”