“…In (12), the first moment m 1 is indexed by r and is thus an N =2 length vector. Note that in (5), Δϕ j = 2πj=N À 2π for j = 1,…,2N, but since e inΔϕ in ( 13) is 2π=n periodic, we have that e in 2πÀΔϕ ð Þ = e ÀinΔϕ , and hence, m 2 r,r 0 , Δϕ j = m 2 r,r 0 ,Δϕ j + N . Thus, Δϕ j for j = 1,…,N is redundant and we consider only Δϕ j for j = N + 1,…,2N, which enumerates 0,2π ½ .…”