“…It follows that, in the limit of small ω, X (ω) ∼ 2λ/(ω ε S ); i.e., it depends only on λ. From the frequency dependence of X (ω), in the limit of ω → 0, we obtain λ, and hence N , assuming for ε the one reported in ref . Increasing the frequency, the resistance decreases and then presents a new plateau, characterized by a resistance R ′ ∼ λ 2 d /( ε D f S ), where D f = ( D p + D m )/2 is the diffusion coefficient for the free diffusion.…”