抄録
Density correlation function 〈ρ·ρ〉kω is calculated on the basis of phenomenological equations of macroscopic variables ρ, s, j, Ψ, Ψ*, near Tλ. In particular the “central peak” due to fluctuations in the amplitude of the condensate field Ψ is carefully investigated. It is concluded, however, that the “central peak” is far less important than the contributions from second sound in the regime kξ<1. The final expression obtained for 〈ρ·ρ〉kω is compared with that of Kretzen and Mikeska and that of Hohenberg.