“…The Fourier coefficients of λ with negative indices vanish (the integrals defining the Fourier coefficients and, more generally, the integrals ϕ dλ, where ϕ is a scalar function, are understood in the Gelfand sense: we mean the element x → ϕ d x, λ , x ∈ G, of G * ). By the main result of [6], there exists a G-measurable G * -valued function f such that λ(e) = e f dm for all Borel sets e ⊂ T (again, the integral is understood in a weak sense). Next, the scalar-valued function t → f (t) G * may fail to be measurable.…”