Let f be a universally measurable function on the spectrum of u.
a) The set Df is a dense vector subspace of E. The mapping f(u):y↦ evy(f) of Df into E is linear and coincides with 1E if f=1;
b) Let g∈Lu(Sp(u)). For every y∈Df and every x∈Dg, one has fg∈L1(Sp(u),μx,y), and
⟨g(u)x∣f(u)y⟩=∫gfμx,y(7)
Sp(u)
c) Suppose that E=L2(X,μ) where X is a locally compact topological space and μ a positive measure on X, and that u=mh, where h:X→C is μ-measurable. One has f(mh)=mf∘h.
According to Theorem 1 of IV, p. 266, one may suppose that one is in the situation of assertion c), that is to say that E=L2(X,μ) and u=mh, where X is a locally compact topological space, μ a positive measure on X and h:X→C is μ-measurable. We shall denote by φ the class in L2(X,μ) of a function φ∈L2(X,μ).
Let S = Sp(mh). We denote by μφ1,φ2 (resp. μφ) the spectral measure of (φ1,φ2) (resp. of φ) relative to mh for every (φ1,φ2)∈L2(X,μ)2 (resp. every φ∈L2(X,μ)).
Let φ∈L2(X,μ). The spectral measure μφ is equal to the image measure h(∣φ∣2⋅μ) on S (Lemma 4 of IV, p. 269). Since the function f is μφ-measurable, one has φ∈Df if and only if the integrals
∫S∗∣f∣2dμφ=∫S∗∣f∣2h(∣φ∣2dμ)=∫X∗∣f∘h∣2∣φ∣2dμ
are finite (INT, V, p. 70, § 6, no2, prop. 2). This means that Df is the domain of the multiplication operator mf∘h, which is a dense subspace of E (prop. 5 of IV, p. 232).
The restriction of evφ to classes of functions g∈K(S) is the mapping which to a class g associates the element g(mh)(φ)=mg∘h(φ) (lemma 4 of IV, p. 269). The mapping evφ therefore coincides with the isometric mapping of L2(S,μφ) into L2(X,μ) deduced by passing to quotients from the mapping g↦(g∘h)⋅φ of L2(S,μφ) into L2(X,μ).
In particular, therefore, we have evφ(f)=mf∘h(φ), so that the mapping f(mh) of Df into E coincides with the partial operator mf∘h. This proves assertion c); if f=1, we find evφ(1)=φ, which also concludes the proof of a).
Let us prove assertion b). Let φ1 and φ2 be functions such that φ1∈Df and φ2∈Dg. We then have (INT, V, loc. cit.)
∫S∗∣fg∣∣μφ1,φ2∣=∫X∗∣(f∘h)(g∘h)φ1φ2∣dμ
⩽∥(f∘h)φ1∥∥(g∘h)φ2∥
which is finite; hence fg∈L1(S,μφ1,φ2). Moreover, we then have