Bourbaki

§ 2. Vectorial measures

1. Definition of a vectorial measure

The definition of a measure given in Ch. III, §1, No. 3 may be generalized as follows:

Definition 1

Let F be a Hausdorff locally convex space over R. One calls vectorial measure on T with values in F every continuous linear mapping of the space K(T)\mathscr{K}(T) into F.

Def. 1 may also be expressed as follows: a vectorial measure on T with values in F is a linear mapping m of K(T)\mathscr{K}(T) into F such that, for every compact subset K of T, the restriction of m to K(T,K)\mathscr{K}(T, K) is continuous for the topology of uniform convergence. If f∈K(T)f \in \mathscr{K}(T), one also writes ∫fdm\int f dm or ∫f(t) dm(t)\int f(t)\,dm(t) instead of m(f)m(f). The measures with values in R\mathbf{R} are sometimes called real measures (Ch. III, §1, No. 5) or scalar measures on T.

Example

— 1) The identity mapping of K(T)\mathscr{K}(T) is a vectorial measure on T with values in K(T)\mathscr{K}(T).

2) Let H be a complex Hilbert space, L(H)\mathscr{L}(H) the normed algebra of continuous endomorphisms of H. Let A be a subalgebra of L(H)\mathscr{L}(H), commutative, closed, self-adjoint and containing the identity; one shows that there exist a compact space X and an isomorphism of the normed algebra A onto the algebra KC(X)=CC(X)\mathscr{K}_\mathbf{C}(X) = \mathscr{C}_\mathbf{C}(X) of continuous complex functions on X, equipped with the norm ∥f∥=sup⁡x∈X∣f(x)∣\|f\| = \sup_{x \in X} |f(x)|. The inverse isomorphism, restricted to K(X)\mathscr{K}(X), is a vectorial measure m on X, with values in L(H)\mathscr{L}(H), such that m(fg)=m(f)m(g)m(fg) = m(f)m(g).

Remark

— 1) For a linear mapping m of K(T)\mathscr{K}(T) into F to be a vectorial measure, it is necessary and sufficient that, for every compact subset K of T, the image under m of the unit ball ∥f∥≤1\|f\| \leq 1 of K(T,K)\mathscr{K}(T, K) be bounded in F. The notion of vectorial measure with values in F is therefore the same for all the Hausdorff locally convex topologies on F that admit the same bounded sets, and in particular for all the topologies compatible with the duality between F and F' (TVS, IV, §1, No. 1, Prop. 1).

2) Let T1T_1 be a locally compact space, F1F_1 a Hausdorff locally convex space over R\mathbf{R}, u a continuous linear mapping of K(T1)\mathscr{K}(T_1) into K(T)\mathscr{K}(T), and v a continuous linear mapping of F into F1F_1. If m is a vectorial measure on T with values in F, then v∘m∘uv \circ m \circ u is a vectorial measure on T1T_1 with values in F1F_1. In particular, if g is a continuous, finite numerical function on T, then f↦m(gf)f \mapsto m(gf) is a vectorial measure on T with values in F, which is denoted g⋅mg \cdot m; if h is a second continuous, finite numerical function on T, then g⋅(h⋅m)=(gh)⋅mg \cdot (h \cdot m) = (gh) \cdot m.

3) Since the space K(T)\mathscr{K}(T) is the direct limit of the Banach spaces K(T,K)\mathscr{K}(T, K), and is in particular barreled (TVS, III, §4, No. 1, Cor. of Prop. 2 and Cor. 3 of Prop. 3), in order that a linear mapping m of K(T)\mathscr{K}(T) into F be a vectorial measure, it is necessary and sufficient that, for every z′∈F′z' \in F', z′∘mz' \circ m be a scalar measure on T (TVS, II, §6, No. 4, Prop. 5 and IV, §1, No. 3, Prop. 7).

4) In view of Remark 1, Prop. 1 of Ch. III, §2, No. 1 and its proof are again valid for vectorial measures. One can therefore define the support of a vectorial measure m on T to be the complement of the largest open set U⊂TU \subset T such that the restriction of m to U is zero.

2. Integration with respect to a vectorial measure

Let mm be a vectorial measure on TT, with values in FF. For every z′∈F′z' \in F', the mapping z′∘mz' \circ m is a scalar measure on TT, depending linearly on z′z'. If ff is a numerical function defined on TT, we shall say, by an abuse of language, that the pair (f,m)(f, m) has the property PP if, for every z′∈F′z' \in F', the pair (f,∣z′∘m∣)(f, |z' \circ m|) has the property PP. For example, we shall say that ff is essentially integrable for mm if, for every z′∈F′z' \in F', the function ff is essentially integrable for ∣z′∘m∣|z' \circ m|. It comes to the same to say that ff is essentially integrable for each of the measures (z′∘m)+(z' \circ m)^+ and (z′∘m)−(z' \circ m)^- (Ch. V, §2, No. 2, Cor. 2 of Prop. 3).

Proposition 1

Let mm be a vectorial measure on TT with values in FF, ff a numerical function on TT that is essentially integrable for mm. The mapping*

z′↦∫f d(z′∘m)+−∫f d(z′∘m)− z' \mapsto \int f \, d(z' \circ m)^+ - \int f \, d(z' \circ m)^-
is a linear form on F′F'.

Denoting this mapping by Φ\Phi, it is immediate that Φ(λz′)=λΦ(z′)\Phi(\lambda z') = \lambda \Phi(z') for all λ∈R\lambda \in \mathbf{R}. Everything comes down to showing that Φ(y′+z′)=Φ(y′)+Φ(z′)\Phi(y' + z') = \Phi(y') + \Phi(z'). Set μ=∣y′∘m∣+∣z′∘m∣\mu = |y' \circ m| + |z' \circ m|; by the Lebesgue–Nikodym theorem, one can then write y′∘m=g⋅μy' \circ m = g \cdot \mu and z′∘m=h⋅μz' \circ m = h \cdot \mu, where gg and hh are two bounded and locally μ\mu-integrable numerical functions (Ch. V, §5, No. 5, Th. 2); moreover, (y′∘m)+=g+⋅μ(y' \circ m)^+ = g^+ \cdot \mu and (y′∘m)−=g−⋅μ(y' \circ m)^- = g^- \cdot \mu, and the analogous relations hold with y′y' replaced by z′z' (resp. y′+z′y' + z') and gg by hh (resp. g+hg + h). This being so, it is immediate that ff is essentially μ\mu-integrable (Ch. V, §2, No. 2, Cor. 1 of Prop. 3), and the relation to be proved reduces to (g+h)+−(g+h)−=(g+−g−)+(h+−h−)(g + h)^+ - (g + h)^- = (g^+ - g^-) + (h^+ - h^-), which is obvious.

Definition 2

Let mm be a vectorial measure on TT with values in FF, ff a numerical function on TT that is essentially integrable for mm. One calls integral of ff with respect to mm, and denotes by m(f)m(f) or ∫f dm\int f \, dm or again ∫f(t) dm(t)\int f(t) \, dm(t), the element of F′∗{F'}^* defined by

⟨z′,∫f dm⟩=∫f d(z′∘m)+−∫f d(z′∘m)−. \langle z', \int f \, dm \rangle = \int f \, d(z' \circ m)^+ - \int f \, d(z' \circ m)^-.

We observe that if f∈K(T)f \in \mathscr{K}(T), the element ∫f dm\int f \, dm so defined coincides with the element denoted likewise in No. 1, because the second member of (1) is then ∫f d(z′∘m)=z′(m(f))\int f \, d(z' \circ m) = z'(m(f)) by definition. Moreover, if in particular one applies Def. 2 to the case that F=RF = \mathbf{R}, one sees that for every z′∈F′z' \in F', f is essentially integrable for the real measure z′∘mz' \circ m, and that the second member of (1) may be written ∫fd(z′∘m)\int f d(z' \circ m).

Suppose now that ff is essentially integrable for mm, and let z′∈F′z' \in F'. Set μ=∣z′∘m∣\mu = |z' \circ m|; by the Lebesgue–Nikodym theorem, one can write z′∘m=g⋅μz' \circ m = g \cdot \mu, where gg is locally μ\mu-integrable and ∥g∥≤1\|g\| \leq 1, and the proof of Prop. 1 shows that ∫fd(z′∘m)=∫fgdμ\int f d(z' \circ m) = \int fg d\mu. Consequently,

∣∫fd(z′∘m)∣≤∫∣f∣d∣z′∘m∣. \left| \int f d(z' \circ m) \right| \leq \int |f| d|z' \circ m|.

It is clear that the set of finite numerical functions essentially integrable for mm is a vector space over R\mathbf{R}; we shall denote by L(m)\mathscr{L}(m) this space equipped with the coarsest locally convex topology making continuous all of the linear forms f↦∫fd(z′∘m)f \mapsto \int f d(z' \circ m), where z′z' runs over F′F'. Note that in general the locally convex space L(m)\mathscr{L}(m) is not Hausdorff.

Example

— Let us take for mm the identity mapping of K(T)\mathscr{K}(T) onto itself. Since the dual of K(T)\mathscr{K}(T) is the space M(T)\mathscr{M}(T) of scalar measures on TT, the functions f∈L(m)f \in \mathscr{L}(m) are those that are essentially integrable for every scalar measure μ\mu (cf. Exer. 1), and the integral ∫fdm\int f dm is the linear form μ↦∫fdμ\mu \mapsto \int f d\mu on M(T)\mathscr{M}(T). One cannot have ∫fdμ=0\int f d\mu = 0 for every measure μ∈M(T)\mu \in \mathscr{M}(T) unless f=0f = 0, as one sees on taking μ=εt\mu = \varepsilon_t, where tt is arbitrary in TT; in other words, the mapping f↦∫fdmf \mapsto \int f dm is an injection of L(m)\mathscr{L}(m) into the algebraic dual of M(T)\mathscr{M}(T), which extends the identity mapping of K(T)\mathscr{K}(T). The relation ∫fdm∈F=K(T)\int f dm \in F = \mathscr{K}(T) is therefore equivalent to f∈K(T)f \in \mathscr{K}(T).

Let uu be a continuous linear mapping of FF into a Hausdorff locally convex space GG, and let us denote again by uu its extension by bitransposition to a linear mapping of F′∗{F'}^* into G′∗{G'}^* (§ 1, No. 1). With this convention:

Proposition 2

Every numerical function* ff essentially integrable for mm is essentially integrable for u∘mu \circ m, and ∫fd(u∘m)=u(∫fdm)\int f d(u \circ m) = u(\int f dm).

The proposition is obvious, in view of the equality y′∘u∘m=tu(y′)∘my' \circ u \circ m = {}^t u(y') \circ m for all y∈G′y \in G'.

In general, if f∈L(m)f \in \mathscr{L}(m), the integral ∫fdm\int f dm belongs to F′∗{F'}^* but not to FF (see the above Example). However:

Proposition 3

If the image under* mm of the set of f∈K(T)f \in \mathscr{K}(T) such that sup⁡t∈T∣f(t)∣≤1\sup_{t \in T} |f(t)| \leq 1 is weakly relatively compact in FF, then ∫fdm∈F\int f dm \in F for every bounded numerical function ff essentially integrable for mm.

Let AA be the set of f∈L(m)f \in \mathscr{L}(m) such that sup⁡t∈T∣f(t)∣≤1\sup_{t \in T} |f(t)| \leq 1, and let B=A∩K(T)B = A \cap \mathscr{K}(T); by hypothesis, m(B)m(B) is weakly relatively compact in FF, therefore it suffices to show that m(A)m(A) is contained in the closure (in F′∗{F'}^*) of m(B)m(B) for the topology σ(F′∗,F′)\sigma({F'}^*, F'); since m(B)m(B) is convex and balanced, it suffices to prove that the polar of m(B)m(B) in F′F' is contained in that of m(A)m(A) (TVS, II, §6, No. 3, Th. 1). Now, for a linear form z′∈F′z' \in F' to belong to (m(B))∘(m(B))^\circ, it is necessary and sufficient that ∣⟨z′,m(g)⟩∣=∣∫gd(z′∘m)∣≤1|\langle z', m(g)\rangle| = |\int g d(z'\circ m)| \leq 1 for every function g∈Bg \in B, which signifies that the scalar measure ∣z′∘m∣|z'\circ m| is bounded and of norm ≤1\leq 1 (Ch. III, §1, No. 8); but by (2) the latter condition implies that ∣⟨z′,m(f)⟩∣≤1|\langle z', m(f)\rangle| \leq 1 for every function f∈Af \in A, whence z′∈(m(A))∘z' \in (m(A))^\circ.

Corollary 1

If, for every compact subset K of T, the image under m of the set of f∈H(T,K)f \in \mathscr{H}(T, K) such that sup⁡t∈T∣f(t)∣≤1\sup_{t \in T} |f(t)| \leq 1 is weakly relatively compact in F, then ∫fdm∈F\int f dm \in F for every function f∈L(m)f \in \mathscr{L}(m) that is bounded and has compact support, and ∫fdm∈F′′\int f dm \in F'' for every function f∈L(m)f \in \mathscr{L}(m).

The first assertion may be deduced immediately from Prop. 3: if ff is bounded and has compact support, and if U is a relatively compact open neighborhood of the support of ff, then the restriction of mm to the subspace H(U)\mathscr{H}(U) is a measure mUm_U on U that satisfies the conditions of Prop. 3, and ∫fdmU=∫fdm\int f dm_U = \int f dm (Ch. V, §7, No. 1, Th. 1), therefore ∫fdm∈F\int f dm \in F.

Now let ff be any element of L(m)\mathscr{L}(m); for every compact subset K of T and every integer n>0n > 0, let fn,Kf_{n,K} be the numerical function on T defined as follows: if t∉Kt \notin K, fn,K(t)=0f_{n,K}(t) = 0; if t∈Kt \in K and ∣f(t)∣≤n|f(t)| \leq n, fn,K(t)=f(t)f_{n,K}(t) = f(t); finally, if t∈Kt \in K and ∣f(t)∣>n|f(t)| > n, fn,K(t)=nf(t)/∣f(t)∣f_{n,K}(t) = nf(t)/|f(t)|. It is clear that for every t∈Tt \in T, f(t)f(t) is the limit of fn,K(t)f_{n,K}(t) with respect to the product filter of the Fréchet filter by the section filter of the (increasing directed) ordered set of compact subsets of T. Since ∣fn,K∣≤∣f∣|f_{n,K}| \leq |f|, it follows from Lebesgue’s theorem and Prop. 10 of Ch. V, §1, No. 3, applied to each scalar measure ∣z′∘m∣|z'\circ m|, that fn,Kf_{n,K} converges to ff in L(m)\mathscr{L}(m) with respect to the preceding filter. Consequently, the integral ∫fdm\int f dm is in the closure in F′∗{F'}^* (for the topology σ(F′∗,F′)\sigma({F'}^*, F')) of the set M of m(fn,K)m(f_{n,K}). But the first part of the corollary shows that M⊂FM \subset F, and, on the other hand, for every z′∈F′z' \in F' one has ∣⟨z′,m(fn,K)⟩∣≤∫∣f∣d∣z′∘m∣|\langle z', m(f_{n,K})\rangle| \leq \int |f| d|z'\circ m|, which shows that M is bounded in FσF_\sigma, hence also in F (TVS, IV, §1, No. 1, Prop. 1). Lemma 1 of §1, No. 2 therefore shows that ∫fdm∈F′′\int f dm \in F''.

Corollary 2

If F is semi-reflexive, then ∫fdm∈F\int f dm \in F for every numerical function ff essentially integrable for mm.

3. Majorizable vectorial measures

Let qq be a lower semi-continuous semi-norm on F. We shall denote by Aq′A'_q the set of z′∈F′z' \in F' such that ∣⟨z′,x⟩∣≤q(x)|\langle z', x\rangle| \leq q(x) for all x∈Fx \in F. This is

the polar in F′F' of the set of x∈Fx \in F such that q(x)≤1q(x) \leq 1; for every x∈Fx \in F,

q(x)=sup⁡z′∈Aq′∣⟨x,z′⟩∣. q(x) = \sup_{z' \in A'_q} |\langle x, z' \rangle|.

Definition 3

Let mm be a vectorial measure on TT with values in FF. If qq is a lower semi-continuous semi-norm on FF, mm is said to be q-majorizable if there exists a positive measure μ\mu such that ∣z′∘m∣≤μ|z' \circ m| \leq \mu for every z′∈Aq′z' \in A'_q; the supremum of the measures ∣z′∘m∣|z' \circ m| as z′z' runs over Aq′A'_q (Ch. III, §2, No. 4, Th. 3) is then denoted q(m)q(m). One says that mm is majorizable if it is q-majorizable for every continuous semi-norm qq on FF.

If mm and m′m' are both q-majorizable, it is immediate that m+m′m + m' is also q-majorizable and that

q(m+m′)≤q(m)+q(m′). q(m + m') \leq q(m) + q(m').

When FF is a normed space, with norm denoted ∣x∣|x|, to say that mm is majorizable therefore means that the measures ∣z′∘m∣|z' \circ m|, where ∣z′∣≤1|z'| \leq 1, are bounded above1^1 by a same positive measure; one then denotes by ∣m∣|m| the supremum of this family of measures.

If F=RF = \mathbf{R}, the measure ∣m∣|m| corresponding to the Euclidean norm ∣x∣|x| on R\mathbf{R} coincides with the measure denoted by ∣m∣|m| in Ch. III, §1, No. 5.

Proposition 4

Let* (Fi)1≤i≤n(F_i)_{1 \leq i \leq n} *be a finite family of Hausdorff locally convex spaces, F=∏i=1nFiF = \prod_{i=1}^n F_i their product, qiq_i (1≤i≤n1 \leq i \leq n) a lower semi-continuous semi-norm on FiF_i, and qq the semi-norm on FF defined by q(x1,…,xn)=∑i=1nqi(xi)q(x_1, \ldots, x_n) = \sum_{i=1}^n q_i(x_i). If mim_i (1≤i≤n1 \leq i \leq n) is a vectorial measure on TT with values in FiF_i that is qiq_i*-majorizable*, then the measure m=(m1,…,mn)m = (m_1, \ldots, m_n) with values in FF is q-majorizable.

For, the dual F′F' may be identified with ∏i=1nFi′\prod_{i=1}^n F_i', in such a way that if x=(xi)∈Fx = (x_i) \in F, z′=(zi′)∈F′z' = (z_i') \in F', then ⟨x,z′⟩=∑i=1n⟨xi,zi′⟩\langle x, z' \rangle = \sum_{i=1}^n \langle x_i, z_i' \rangle. If ∣⟨x,z′⟩∣≤q(x)|\langle x, z' \rangle| \leq q(x) for every x∈Fx \in F, then in particular ∣⟨xi,zi′⟩∣≤qi(xi)|\langle x_i, z_i' \rangle| \leq q_i(x_i) for 1≤i≤n1 \leq i \leq n, and the converse is obvious, which shows that the set Aq′A'_q is the product of the Aqi′A'_{q_i}. Since by hypothesis ∣zi′∘mi∣≤qi(mi)|z_i' \circ m_i| \leq q_i(m_i) for zi′∈Aqi′z_i' \in A'_{q_i}, it follows that

∣z′∘m∣≤∑i=1n∣zi′∘mi∣≤∑i=1nqi(mi) |z' \circ m| \leq \sum_{i=1}^n |z_i' \circ m_i| \leq \sum_{i=1}^n q_i(m_i)
for every z′∈Aq′z' \in A'_q, which proves the proposition.

1^1 Majorées.

Corollary

— If the space F is finite-dimensional, then every vectorial measure m with values in F is majorizable. In order that a numerical function be essentially integrable for m, it is necessary and sufficient that it be essentially integrable for |m| (where |x| denotes any norm on F).

Proposition 5

— *Let q be a lower semi-continuous semi-norm on F. Let m be a q-majorizable measure, and let f be a function essentially integrable for m and such that ∫fdm∈F\int f dm \in F. Then

q(∫fdm)≤∫∙∣f∣dq(m). q\left( \int f dm \right) \leq \int^\bullet |f| dq(m).

For,

q(∫fdm)=sup⁡z′∈Aq′∣⟨z′,∫fdm⟩∣≤sup⁡z′∈Aq′∫∣f∣d∣z′∘m∣≤∫∙∣f∣dq(m) q\left( \int f dm \right) = \sup_{z' \in A'_q} \left| \langle z', \int f dm \rangle \right| \leq \sup_{z' \in A'_q} \int |f| d|z' \circ m| \leq \int^\bullet |f| dq(m)

by virtue of (1) and the relation ∣z′∘m∣≤q(m)|z' \circ m| \leq q(m) for z′∈Aq′z' \in A'_q.

Proposition 6

— *Let F be a quasi-complete, Hausdorff locally convex space, m a majorizable measure on T with values in F. If f is a numerical function essentially integrable for all of the measures q(m) (where q runs over the set of continuous semi-norms on F), then f is essentially integrable for m, and ∫fdm∈F\int f dm \in F.

We shall make use of the following auxiliary result. Let (μι)ι∈I(\mu_\iota)_{\iota \in I} be an increasing directed family of positive measures on T. Let us denote by L1((μι)ι∈I)\mathscr{L}^1((\mu_\iota)_{\iota \in I}) the vector space of finite numerical functions on T, essentially μι\mu_\iota-integrable for every ι∈I\iota \in I, equipped with the topology defined by the semi-norms f↦μι(∣f∣)f \mapsto \mu_\iota(|f|) (ι∈I\iota \in I). Let L0\mathscr{L}_0 be the linear subspace of L1((μι)ι∈I)\mathscr{L}^1((\mu_\iota)_{\iota \in I}) generated by the products gφKg \varphi_K, where g runs over the set of continuous finite numerical functions on T, and K over the set of compact subsets of T.

Lemma 1

— *When L0\mathscr{L}_0 and K(T)\mathscr{K}(T) are equipped with the topology induced by that of L1((μι)ι∈I)\mathscr{L}^1((\mu_\iota)_{\iota \in I}): a) each element of L0\mathscr{L}_0 is in the closure of some bounded subset of K(T)\mathscr{K}(T); b) each element of L1((μι)ι∈I)\mathscr{L}^1((\mu_\iota)_{\iota \in I}) is in the closure of some bounded subset of L0\mathscr{L}_0.

To prove a), we may restrict ourselves to the case of an element of the form f=gφKf = g \varphi_K (g∈C(T)g \in \mathscr{C}(T)), K compact in T). It is immediate (by virtue of Urysohn’s theorem) that ff is in the closure of the set B of functions of the form ghgh, where h describes the set of continuous mappings of T into [0,1][0,1] that are equal to 1 on K and to 0 on the complement of a fixed compact neighborhood H of K. Moreover, the set B is bounded, because μι(∣gh∣)≤μι(∣fφH∣)\mu_\iota(|gh|) \leq \mu_\iota(|f\varphi_H|) for every function h having the preceding properties.

Let us now prove b); we may restrict ourselves to the case of an element f≥0f \geq 0 of L1((μι)ι∈I)\mathscr{L}^1((\mu_\iota)_\iota \in I). For every ι∈I\iota \in I and every ε>0\varepsilon > 0, there exists a compact subset K(ι,ε)K(\iota, \varepsilon) of T such that the restriction of ff to K(ι,ε)K(\iota, \varepsilon) is continuous and ∣μι(∣f−fφK(ι,ε)∣)∣≤ε|\mu_\iota(|f - f\varphi_{K(\iota, \varepsilon)}|)| \leq \varepsilon. It is clear that ff is in the closure of the set C of fφK(ι,ε)f\varphi_{K(\iota, \varepsilon)} (where ι∈I, ε>0\iota \in I,\ \varepsilon > 0). By virtue of Urysohn’s theorem, the set C in contained in L0\mathscr{L}_0; moreover, it is bounded, because μκ(fφK(ι,ε))≤μκ(f)\mu_\kappa(f\varphi_{K(\iota, \varepsilon)}) \leq \mu_\kappa(f) for all ι∈I, κ∈I\iota \in I,\ \kappa \in I and ε>0\varepsilon > 0.

Let us now prove Prop. 6: for every function g∈K(T)g \in \mathscr{K}(T) and every continuous seminorm q on F, q(∫g dm)≤∫∣g∣ d(q(m))q\left( \int g\,dm \right) \leq \int |g|\,d(q(m)) (Prop. 5), which implies that the mapping g↦∫g dmg \mapsto \int g\,dm of K(T)\mathscr{K}(T) into F is continuous when K(T)\mathscr{K}(T) is equipped with the topology induced by that of L1((q(m))q∈Q)\mathscr{L}^1((q(m))_{q \in Q}) (Q the set of continuous semi-norms on F). Consequently, by the preceding lemma and Prop. 10 of TVS, III, §1, No. 6, this mapping may be extended by continuity, first to a continuous linear mapping v0v_0 of L0\mathscr{L}_0 into F, then to a continuous linear mapping vv of L1((q(m))q∈Q)\mathscr{L}^1((q(m))_{q \in Q}) into F. Moreover, for every z′∈F′z' \in F' the relation ⟨z′,v(f)⟩=∫f d(z′∘m)\langle z', v(f) \rangle = \int f\,d(z' \circ m) holds, by the definition of vv, for every f∈K(T)f \in \mathscr{K}(T); since ∣z′∘m∣≤q(m)|z' \circ m| \leq q(m) for q(z)=∣⟨z′,z⟩∣q(z) = |\langle z', z \rangle|, the mapping f↦∫f d(z′∘m)f \mapsto \int f\,d(z' \circ m) is continuous on L1((q(m))q∈Q)\mathscr{L}^1((q(m))_{q \in Q}), therefore again by continuity, the relation ⟨z′,v(f)=∫f d(z′∘m)\langle z', v(f) = \int f\,d(z' \circ m) holds for every function f∈L1((q(m))q∈Q)f \in \mathscr{L}^1((q(m))_{q \in Q}). It follows that v(f)=∫f dmv(f) = \int f\,dm, which completes the proof.

4. Vectorial measures with base μ\mu

Definition 4

Let μ\mu be a positive measure on T. A vectorial measure mm on T, with values in F, is said to be a measure with base μ\mu if there exists a mapping ff of T into F, scalarly locally μ\mu-integrable, such that m(g)=∫gf dμm(g) = \int gf\,d\mu for every function g∈K(T)g \in \mathscr{K}(T). One then says that ff is a density of mm with respect to μ\mu, and one writes m=f⋅μm = f \cdot \mu.

It is immediate that if f1f_1 and f2f_2 are two densities of mm with respect to μ\mu, then f1−f2f_1 - f_2 is scalarly locally μ\mu-negligible (Ch. V, §5, No. 3, Cor. 2 of Prop. 3); recall that in general this does not imply that f1−f2f_1 - f_2 is zero locally almost everywhere (cf. §1, Exer. 12 and No. 1, Remark 2).

Let mm be a measure with base μ\mu, of density ff. For a numerical function gg to be essentially integrable for mm, it is necessary and sufficient that gfgf be scalarly essentially μ\mu-integrable (Ch. V, §5, No. 3, Th. 1).

Proposition 7

— Let ff be a mapping scalarly locally integrable with respect to a positive measure μ\mu on TT, such that, for every function g∈K(T)g \in \mathscr{K}(T), one has ∫gf dμ∈F\int gf\,d\mu \in F. Then the mapping g↦∫gf dμg \mapsto \int gf\,d\mu of K(T)\mathscr{K}(T) into FF is a vectorial measure on TT, with base μ\mu and density ff with respect to μ\mu.

For (No. 1, Remark 3), it suffices to show that, setting m(g)=∫gf dμm(g) = \int gf\,d\mu, z′∘mz' \circ m is a scalar measure for every z′∈F′z' \in F'. But since z′(m(g))=∫g⟨z′,f⟩ dμz'(m(g)) = \int g\langle z', f \rangle\,d\mu, one has z′∘m=⟨z′,f⟩⋅μz' \circ m = \langle z', f \rangle \cdot \mu, whence our assertion.

Proposition 8

— Let μ\mu be a positive measure on TT, mm a measure on TT with values in FF, with base μ\mu and density ff with respect to μ\mu. Let qq be a lower semi-continuous semi-norm on FF.

a) If, for every compact subset KK of TT, the upper integral ∫K∗(q∘f) dμ\int_K^*(q \circ f)\,d\mu is finite, then mm is qq-majorizable.

b) If mm is qq-majorizable, then q(m)q(m) has base μ\mu; if in addition ff is μ\mu-measurable as a mapping of TT into FσF_\sigma, then q∘fq \circ f is locally μ\mu-integrable and q(m)=(q∘f)⋅μq(m) = (q \circ f) \cdot \mu.

a) For every finite subset JJ of Aq′A'_q, let us denote by λJ\lambda_J the supremum of the measures ∣z′∘m∣|z' \circ m|, where z′z' runs over JJ; if gJ=sup⁡z′∈J∣⟨z′,f⟩∣g_J = \sup_{z' \in J} |\langle z', f \rangle| then λJ=gJ⋅μ\lambda_J = g_J \cdot \mu (Ch. V, §5, No. 2, Prop. 2). For every relatively compact open subset UU of TT, let λJ,U\lambda_{J,U} be the restriction of λJ\lambda_J to UU; let us first show that as JJ runs over the directed set F\mathfrak{F} of finite subsets of Aq′A'_q, the family (λJ,U)(\lambda_{J,U}) is bounded above in M(U)\mathscr{M}(U). Indeed, for every function h≥0h \geq 0 in K(U)K(U),

∫h dλJ,U=∫hgJ dμ≤∫∗(q∘f)h dμ≤∥h∥∫U∗(q∘f) dμ, \int h\,d\lambda_{J,U} = \int hg_J\,d\mu \leq \int^*(q \circ f)h\,d\mu \leq \|h\| \int_U^*(q \circ f)\,d\mu,

whence our assertion (Ch. II, §2, No. 2). Let νU\nu_U be the supremum of this family of measures in M(U)\mathscr{M}(U). If U′U' is a second relatively compact open subset of TT such that U⊂U′U \subset U', then νU\nu_U is the restriction of νU′\nu_{U'} to UU, as follows immediately from the expression of the supremum of an increasing directed set of measures (Ch. II, §2, No. 2) and the fact that λJ,U\lambda_{J,U} is the restriction to UU of λJ,U′\lambda_{J,U'}. Thus there is one and only one positive measure ν\nu whose restriction to each UU is νU\nu_U (Ch. III, §2, No. 1, Prop. 1), and it is clear that ν=q(m)\nu = q(m).

b) Since the measures λJ\lambda_J have base μ\mu, so does their supremum q(m)q(m) (Ch. V, §5, No. 5, Th. 2). If ff is μ\mu-measurable for the topology σ(F,F′)\sigma(F, F') on FF, it follows at once from the definitions that the mapping g:t↦(gJ(t))J∈Fg : t \mapsto (g_J(t))_{J \in \mathfrak{F}} of TT into the product space RF\mathbf{R}^\mathfrak{F} is μ\mu-measurable. The restriction of q∘f=sup⁡J∈FgJq \circ f = \sup_{J \in \mathfrak{F}} g_J to every compact subset of TT on which gg is continuous is lower semi-continuous; consequently q∘fq \circ f is μ\mu-measurable (Ch. IV, §5, No. 5, Cor. of Prop. 8 and No. 10, Prop. 15). Let KK be a compact subset of T; it admits a partition consisting of a μ\mu-negligible set and a sequence (Kn)(K_n) of compact sets on which gg is continuous. Then ∫Kn∗(q∘f) dμ=sup⁡J∫KngJ dμ≤∫Kndq(m)\int_{K_n}^*(q \circ f)\, d\mu = \sup_J \int_{K_n} g_J\, d\mu \leq \int_{K_n} dq(m) for all nn (Ch. IV, §1, No. 1, Th. 1 and Ch. V, §7, No. 1, Prop. 1), whence ∫K∗(q∘f) dμ=∑n∫Kn∗(q∘f) dμ≤∫Kdq(m)\int_K^*(q \circ f)\, d\mu = \sum_n \int_{K_n}^*(q \circ f)\, d\mu \leq \int_K dq(m). But this proves that q∘fq \circ f is locally μ\mu-integrable and that λJ≤(q∘f)⋅μ≤q(m)\lambda_J \leq (q \circ f) \cdot \mu \leq q(m) for all J∈FJ \in \mathscr{F}; whence, by definition, q(m)=(q∘f)⋅μq(m) = (q \circ f) \cdot \mu.

Remark

Suppose that there exists in Aq′A_q' a countable subset D that is dense for σ(F′,F)\sigma(F', F); then, the function q∘fq \circ f is always μ\mu-measurable, because q(f(t))=sup⁡z′∈D∣⟨z′,f(t)⟩∣q(f(t)) = \sup_{z' \in D} |\langle z', f(t) \rangle| (Ch. IV, §5, No. 4, Cor. 1 of Th. 2). Then, for every compact subset K of T, ∫K∗(q∘f) dμ=sup⁡J∫KgJ dμ\int_K^*(q \circ f)\, d\mu = \sup_J \int_K g_J\, d\mu, where J runs over the countable directed set of finite subsets of D (Ch. IV, §1, No. 1, Cor. of Th. 3); thus, one sees that in this case the condition that ∫K∗(q∘f) dμ<+∞\int_K^*(q \circ f)\, d\mu < +\infty for every compact subset K of T is necessary and sufficient for m to be qq-majorizable.

Proposition 9

— *Let F be a finite-dimensional Banach space. Every measure m on T with values in F is a measure with base ∣m∣|m|. If m=f⋅∣m∣m = f \cdot |m|, then ∣f(t)∣=1|f(t)| = 1 locally almost everywhere for ∣m∣|m|. For m to have base μ\mu, it is necessary and sufficient that ∣m∣|m| have base μ\mu, and if m=g⋅μm = g \cdot \mu then ∣m∣=∣g∣⋅μ|m| = |g| \cdot \mu.

Let (ei)1≤i≤n(e_i)_{1 \leq i \leq n} and (ei′)1≤i≤n(e'_i)_{1 \leq i \leq n} be dual bases of F and F' (A, II, §2, No. 6) with ∣ei′∣=1|e'_i| = 1 for all i. Then ∣ei′∘m∣≤∣m∣|e'_i \circ m| \leq |m| for every index i, therefore (Ch. V, §5, No. 5, Th. 2) ei′∘m=hi⋅∣m∣e'_i \circ m = h_i \cdot |m|, where hih_i is bounded and ∣m∣|m|-measurable. Setting h=∑i=1nhi⋅eih = \sum_{i=1}^n h_i \cdot e_i, we therefore have m=h⋅∣m∣m = h \cdot |m|. If m=f⋅∣m∣m = f \cdot |m|, Prop. 8 shows that ∣m∣=∣f∣⋅∣m∣|m| = |f| \cdot |m|, whence ∣f(t)∣=1|f(t)| = 1 locally almost everywhere for ∣m∣|m| (Ch. V, §5, No. 3, Cor. 2 of Prop. 3). The final assertion follows at once from Prop. 8.

Remark

If z=∑i=1nzieiz = \sum_{i=1}^n z_i e_i then ψ(z1,…,zn)=∣z∣\psi(z_1, \ldots, z_n) = |z| is a positively homogeneous continuous function on Rn\mathbf{R}^n. Setting μi=ei′∘m=hi⋅∣m∣\mu_i = e'_i \circ m = h_i \cdot |m|, by definition (Ch. V, §5, No. 9) ψ(μ1,…,μn)=ψ(h1,…,hn)⋅∣m∣=∣h∣⋅∣m∣=∣m∣\psi(\mu_1, \ldots, \mu_n) = \psi(h_1, \ldots, h_n) \cdot |m| = |h| \cdot |m| = |m|.

5. The Dunford–Pettis theorem

Let μ\mu be a positive measure on T. A vectorial measure m on T, with values in F, is said to be scalarly of base μ\mu (or to have base μ\mu scalarly) if, for every z′∈F′z' \in F', the scalar measure z′∘mz' \circ m has base μ\mu. If a vectorial measure mm with values in FF has base μ\mu, then it has base μ\mu scalarly: for, if m=f⋅μm = f \cdot \mu then z′∘m=⟨z′,f⟩⋅μz' \circ m = \langle z', f \rangle \cdot \mu for every z′∈F′z' \in F'. But there exist vectorial measures that are scalarly of base μ\mu without having base μ\mu (Exer. 17), and, on the other hand, there exist vectorial measures that are not scalarly of base ν\nu for any positive measure ν\nu; note however that every majorizable measure mm with values in a normed space is scalarly of base ∣m∣|m|, by virtue of the Lebesgue–Nikodym theorem.

Example

— Let us take for mm the identity mapping of H(T)\mathscr{H}(T). To say that mm is scalarly of base μ\mu means that every real measure on TT has base μ\mu. In particular, the point measure εt\varepsilon_t (t∈Tt \in T) must have base μ\mu, which requires that μ({t})>0\mu(\{t\}) > 0 for every t∈Tt \in T, and implies in particular that every compact subset of TT is countable.

In this No. we are going to prove a result that generalizes one of the consequences of the Lebesgue–Nikodym theorem, namely, that the dual of L1(μ)L^1(\mu) is L∞(μ)L^\infty(\mu) (Ch. V, §5, No. 8, Th. 4), and that gives a sufficient condition for a vectorial measure that is scalarly of base μ\mu to have base μ\mu.

Let π\pi be the canonical mapping of L∞(μ)\mathscr{L}^\infty(\mu) onto L∞(μ)L^\infty(\mu). We shall say that a linear subspace GG of L∞L^\infty has the lifting property if there exists a linear mapping ρ\rho of GG into L∞(μ)\mathscr{L}^\infty(\mu) (called a lifting of GG) such that π∘ρ\pi \circ \rho is the identity on GG and ∣ρ(f)(t)∣≤N∞(f)|\rho(f)(t)| \leq N_\infty(f) for all t∈Tt \in T and f∈Gf \in G.

One proves that if μ\mu is Lebesgue measure on Rn\mathbf{R}^n, the entire space L∞(Rn,μ)L^\infty(\mathbf{R}^n, \mu) has the lifting property (Exer. 18).

Lemma 2

Every separable subspace* GG of the Banach space L∞(T,μ)L^\infty(T, \mu) has the lifting property.

By the hypothesis, there exists a countable dense subset HH of GG that is a linear subspace with respect to the field Q\mathbf{Q} of rational numbers; let (hn)(h_n) be a (countable) basis of HH over Q\mathbf{Q}. For every integer nn, let hn′h'_n be an element of L∞\mathscr{L}^\infty such that π(hn′)=hn\pi(h'_n) = h_n, and let ρ′\rho' be the Q\mathbf{Q}-linear mapping of HH into L∞\mathscr{L}^\infty defined by ρ′(hn)=hn′\rho'(h_n) = h'_n; it is clear that π∘ρ′\pi \circ \rho' is the identity on HH. Moreover, for every h∈Hh \in H one has ∣ρ′(h)(t)∣≤N∞(h)|\rho'(h)(t)| \leq N_\infty(h) except at the points tt of a locally negligible set A(h)A(h). Let AA be the union of the A(h)A(h) for h∈Hh \in H, which is also locally negligible. For every h∈Hh \in H, denote by ρ(h)\rho(h) the function h′′∈L∞h'' \in \mathscr{L}^\infty such that h′′(t)=ρ′(h)(t)h''(t) = \rho'(h)(t) if t∉At \notin A, and h′′(t)=0h''(t) = 0 if t∈At \in A. It is clear that ρ\rho is a Q\mathbf{Q}-linear mapping of HH into the subspace B\mathscr{B} of bounded functions in L∞\mathscr{L}^\infty, such that π∘ρ\pi \circ \rho is the identity on HH and such that ∣ρ(h)(t)∣≤N∞(h)|\rho(h)(t)| \leq N_\infty(h) for all h∈Hh \in H and t∈Tt \in T. Since B\mathscr{B} is a Banach space for the norm ∥f∥=sup⁡t∈T∣f(t)∣\|f\| = \sup_{t \in T} |f(t)| (Ch. IV, §5, No. 4, Th. 2), ρ\rho may be extended to a continuous R\mathbf{R}-linear mapping, again denoted ρ\rho, of GG into B\mathscr{B}, which is obviously a lifting of GG.

Definition 5

— Let F be a Hausdorff locally convex space, Fs′F'_s its dual equipped with the topology σ(F′,F)\sigma(F', F). We denote by LFs′∞\mathscr{L}_{F'_s}^\infty the vector space of mappings ff of T into Fs′F'_s, such that ff is scalarly μ\mu-measurable and is equal scalarly locally almost everywhere (for μ\mu) to a mapping of T into an equicontinuous subset of F′F'. We denote by LFs′∞L_{F'_s}^\infty the quotient space of LFs′∞\mathscr{L}_{F'_s}^\infty by the space of scalarly locally μ\mu-negligible mappings of T into Fs′F'_s.

When F satisfies the hypotheses of §1, No. 5, Prop. 13, the functions in LFs′∞\mathscr{L}_{F'_s}^\infty are μ\mu-measurable for the weak topology σ(F′,F)\sigma(F', F), but are not necessarily measurable for the strong topology on F′F', even if F is a Banach space (§1, Exer. 17). Under the same conditions, the scalarly locally μ\mu-negligible mappings of T into Fs′F'_s are identical to the locally μ\mu-negligible mappings of T into Fs′F'_s (§1, No. 1, Remark 2).

When F is a separable normed space, the elements of LFs′∞\mathscr{L}_{F'_s}^\infty are the mappings ff of T into Fs′F'_s such that ff is scalarly μ\mu-measurable and ∣f∣|f| is bounded in measure; one can then define a normed space structure on the space LFs′∞L_{F'_s}^\infty, by equipping it with the norm N∞N_\infty (Ch. IV, §6, No. 3).

Lemma 3

Let F be a Hausdorff locally convex space, ff an element of LFs′∞\mathscr{L}_{F'_s}^\infty. For every z∈Fz \in F, one has ⟨z,f⟩∈L∞\langle z, f \rangle \in \mathscr{L}^\infty, and the linear mapping z↦π(⟨z,f⟩)z \mapsto \pi(\langle z, f \rangle) of F into L∞L^\infty is continuous; if, moreover, F is a normed space, then N∞(⟨z,f⟩)≤∣z∣⋅sup⁡t∈T∣f(t)∣N_\infty(\langle z, f \rangle) \leq |z| \cdot \sup_{t \in T} |f(t)|.

It is clear by definition that ⟨z,f⟩\langle z, f \rangle is μ\mu-measurable and bounded in measure; replacing if necessary ff by a function belonging to the same class of LFs′∞L_{F'_s}^\infty, we can suppose in addition that f(T)⊂V∘f(T) \subset V^\circ, where V is a balanced convex neighborhood of 0 in F (which does not modify ⟨z,f⟩\langle z, f \rangle except on a locally negligible set, depending on zz). Then the relation z∈Vz \in V implies that ∣⟨z,f(t)⟩∣≤1|\langle z, f(t) \rangle| \leq 1 for all t∈Tt \in T, which proves the continuity of z↦π(⟨z,f⟩)z \mapsto \pi(\langle z, f \rangle). The final assertion is obvious.

Lemma 4

Let F be a Hausdorff locally convex space, ff an element of LFs′∞\mathscr{L}_{F'_s}^\infty. For every numerical function g∈L‾1g \in \overline{\mathscr{L}}^1, the function gfgf is scalarly essentially μ\mu-integrable and ∫gf dμ∈F′\int gf\, d\mu \in F'.

For every z∈Fz \in F, ⟨z,f⟩\langle z, f \rangle belongs to L∞\mathscr{L}^\infty, whence the first assertion. One can suppose moreover, without modifying ∫gf dμ\int gf\, d\mu, that f(T)⊂V∘f(T) \subset V^\circ, where V is a balanced convex neighborhood of 0 in F. Then the relation z∈Vz \in V implies ∣⟨z,f(t)⟩∣≤1|\langle z, f(t) \rangle| \leq 1 for all t∈Tt \in T, whence ∣⟨z,∫gf dμ⟩∣=∣∫⟨z,f⟩g dμ∣≤N‾1(g)|\langle z, \int gf\, d\mu \rangle| = |\int \langle z, f \rangle g\, d\mu| \leq \overline{N}_1(g), which proves that ∫gf dμ∈F′\int gf\, d\mu \in F'.

Theorem 1

— Let F be a Hausdorff locally convex space that contains a countable dense subset. For every function f∈LFs′∞f \in \mathscr{L}_{F'_s}^\infty and every z∈Fz \in F, let vf(z)=π(⟨z,f⟩)∈L∞v_f(z) = \pi(\langle z, f \rangle) \in L^\infty; the mapping f↦vff \mapsto v_f defines, by passage to the quotient, a linear bijection of LF′∞L_{F'}^\infty onto the space L(F;L∞)\mathscr{L}(F; L^\infty) of continuous linear mappings of FF into L∞L^\infty. *If FF is a normed space, this bijection is an isometry.

In view of Lemma 3, the first assertion will be demonstrated if one proves that for every continuous mapping uu of FF into L∞L^\infty, there exists a function f∈LF′∞f \in \mathscr{L}_{F'}^\infty such that π(⟨z,f⟩)=u(z)\pi(\langle z, f \rangle) = u(z) for all z∈Fz \in F, and that the class of ff in LF′∞L_{F'}^\infty is uniquely determined by this condition. The second point is immediate, because if π(⟨z,f⟩)=π(⟨z,f1⟩)\pi(\langle z, f \rangle) = \pi(\langle z, f_1 \rangle) for all z∈Fz \in F, then f1−ff_1 - f is scalarly locally negligible. On the other hand, there exists a lifting ρ\rho of u(F)u(F) into L∞\mathscr{L}^\infty (Lemma 2). For every t∈Tt \in T, the mapping z↦ρ(u(z))(t)z \mapsto \rho(u(z))(t) is a continuous linear form on FF, that is, an element f(t)f(t) of F′F'. The function ff is scalarly μ\mu-measurable since ⟨z,f⟩=ρ(u(z))∈L∞\langle z, f \rangle = \rho(u(z)) \in \mathscr{L}^\infty for every z∈Fz \in F; one has π(⟨z,f⟩)=u(z)\pi(\langle z, f \rangle) = u(z); finally, for every t∈Tt \in T and every zz belonging to the inverse image VV under uu of the unit ball of L∞L^\infty,

∣⟨z,f(t)⟩∣=∣ρ(u(z))(t)∣≤N∞(u(z))≤1, |\langle z, f(t) \rangle| = |\rho(u(z))(t)| \leq N_\infty(u(z)) \leq 1,

which shows that f(t)∈V∘f(t) \in V^\circ for all t∈Tt \in T.

If, moreover, FF is a normed space, the foregoing shows that

sup⁡t∈T∣f(t)∣≤∥u∥. \sup_{t \in T} |f(t)| \leq \|u\|.

But on the other hand (Lemma 3), N∞(u(z))≤∣z∣⋅sup⁡t∈T∣f(t)∣N_\infty(u(z)) \leq |z| \cdot \sup_{t \in T} |f(t)|, and this inequality continues to hold when ff is modified arbitrarily on a locally negligible set. It follows that ∥u∥=N∞(∣f∣)\|u\| = N_\infty(|f|).

Corollary 1

Let FF be a Hausdorff locally convex space containing a countable dense subset. For every function f∈LF′∞f \in \mathscr{L}_{F'}^\infty, every z∈Fz \in F and every function g∈L1g \in \mathscr{L}^1, let Φf(z,g~)=∫⟨z,f(t)⟩g(t) dμ(t)\Phi_f(z, \tilde{g}) = \int \langle z, f(t) \rangle g(t)\, d\mu(t). The mapping f↦Φff \mapsto \Phi_f defines, by passage to the quotient, a linear bijection of LF′∞L_{F'}^\infty onto the space B(F,L1)\mathscr{B}(F, L^1) of continuous bilinear forms on F×L1F \times L^1. *If FF is a normed space, this bijection is an isometry.

One can suppose that f(T)f(T) is an equicontinuous subset of F′F'. It is then clear that Φf\Phi_f is separately continuous, and, with the notations of Th. 1 and the Appendix, one has (taking into account the fact that L∞L^\infty is the dual of L1L^1 (Ch. V, §5, No. 8, Th. 4)) lΦf=vf^l \Phi_f = v_f. The corollary then follows from Th. 1 above and from the Appendix, No. 1, Prop. 1 and its corollary.

Corollary 2 (Dunford–Pettis theorem)

— Let FF be a Hausdorff locally convex space containing a countable dense subset. For every function f∈LF′∞f \in \mathscr{L}_{F'}^\infty and every function g∈L1g \in \mathscr{L}^1, let wf(g~)=∫gf dμ∈F′w_f(\tilde{g}) = \int gf\, d\mu \in F' (Lemma 4). The mapping f↦wff \mapsto w_f defines, by passage to the quotient, a linear bijection of LFs∞L_{F_s}^\infty onto the space R(L1,F′)\mathscr{R}(L^1, F') of linear mappings uu of L1L^1 into F′F' such that the image under uu of the unit ball of L1L^1 is an equicontinuous subset of F′F'. *If FF is a normed space (in which case R(L1,F′)\mathscr{R}(L^1, F') is the space of continuous linear mappings of L1L^1 into the strong dual of FF), the bijection f↦wff \mapsto w_f is an isometry.

Taking into account the fact that L∞L^\infty is the dual of L1L^1, this follows from the preceding corollary and from the Appendix, No. 1, Prop. 1 and its corollary.

Remark

— It is clear that the mappings u∈R(L1,F′)u \in \mathscr{R}(L^1, F') are continuous for every G\mathscr{G}-topology on F′F' (G\mathscr{G} a covering of FF by bounded subsets). Conversely, if FF is assumed moreover to be barreled, then every continuous linear mapping of L1L^1 into F′F' equipped with an G\mathscr{G}-topology transforms the unit ball of L1L^1 into a bounded subset of F′F', which is therefore equicontinuous (TVS, III, §4, No. 2, Th. 1).

Corollary 3

Let FF be a Hausdorff locally convex space containing a countable dense subset, mm a vectorial measure on TT with values in the weak dual F′F' of FF. If the image under mm of the set BB of functions gg in K(T)\mathscr{K}(T) such that μ(∣g∣)≤1\mu(|g|) \leq 1 is contained in a closed and convex equicontinuous subset H′H' of F′F', then mm has base μ\mu and there exists a density ff of mm with respect to μ\mu such that f(t)∈H′f(t) \in H' for all t∈Tt \in T.

The hypothesis implies that mm is continuous when K(T)\mathscr{K}(T) is equipped with the topology induced by that of L1(μ)\mathscr{L}^1(\mu) (defined by the semi-norm N1N_1); it may therefore be extended to a continuous linear mapping uu of L1(μ)\mathscr{L}^1(\mu) into the completion GG of the weak dual of FF; but since H′H' is a compact subset of GG and the image under uu of the set B‾\overline{B} of f∈L1f \in \mathscr{L}^1 such that N1(f)≤1N_1(f) \leq 1 is contained in the closure of H′H' in GG, one has u(B‾)⊂H′u(\overline{B}) \subset H', therefore uu maps L1\mathscr{L}^1 into F′F'. Since the relation N1(f)≤εN_1(f) \leq \varepsilon implies that u(f)∈εH′u(f) \in \varepsilon H', one has u(g)=0u(g) = 0 if gg is μ\mu-negligible, and Cor. 2 may therefore be applied to the mapping of L1L^1 into F′F' obtained from uu by passing to the quotient; whence the corollary.

Corollary 4

Let FF be a separable normed space, and mm a measure on TT with values in the strong dual F′F', majorizable for the norm of F′F'. Then mm is a measure with base ∣m∣|m|, and if m=f⋅∣m∣m = f \cdot |m| then ∣f(t)∣=1|f(t)| = 1 locally almost everywhere for ∣m∣|m|.

By hypothesis, for every z∈Fz \in F such that ∣z∣≤1|z| \leq 1, one has ∣⟨z,m(g)⟩∣≤∣m∣(∣g∣)|\langle z, m(g) \rangle| \leq |m|(|g|) for every function g∈K(T)g \in \mathscr{K}(T), consequently ∣m(g)∣≤∣m∣(∣g∣)|m(g)| \leq |m|(|g|) (TVS, IV, §2, No. 4, formula (1)). Since every ball in F′F' is equicontinuous, Cor. 3 is applicable and shows that mm has base ∣m∣|m|; moreover, if m=f⋅∣m∣m = f \cdot |m| then ff is ∣m∣|m|-measurable for σ(F′,F)\sigma(F', F) (§1, No. 5, Prop. 13) and ∣m∣=∣f∣⋅∣m∣|m| = |f| \cdot |m| (No. 4, Prop. 8), which proves the corollary (Ch. V, §5, No. 3, Cor. 2 of Prop. 3).

If this corollary is applied to the case that FF if finite-dimensional, one recovers as a special case the first part of Prop. 9.

6. Dual of the space LF1L^1_F (F a separable Banach space)

Proposition 10

— *Let F be a separable Banach space. For every function f∈L‾F1f \in \overline{\mathscr{L}}^1_F and every function g∈LFs′∞g \in \mathscr{L}_{F'_s}^\infty, the numerical function ⟨f,g⟩:t↦⟨f(t),g(t)⟩\langle f, g \rangle : t \mapsto \langle f(t), g(t) \rangle is essentially μ\mu-integrable, and

∣∫⟨f,g⟩ dμ∣≤N‾1(f)N∞(g). \left| \int \langle f, g \rangle \, d\mu \right| \leq \overline{N}_1(f) N_\infty(g) .

*For every class g˙∈LFs′∞\dot{g} \in L_{F'_s}^\infty, let θ(g˙)\theta(\dot{g}) be the continuous linear form on LF1L^1_F deduced from the linear form f↦∫⟨f,g⟩ dμf \mapsto \int \langle f, g \rangle \, d\mu on L‾F1\overline{\mathscr{L}}^1_F by passage to the quotient; then θ\theta is a linear isometry of LFs′∞L_{F'_s}^\infty onto the strong dual (LF1)′(L^1_F)' of the Banach space LF1L^1_F.

For every compact subset K of T and every ε>0\varepsilon > 0, there exists a compact subset K′K' of K such that μ(K−K′)≤ε\mu(K - K') \leq \varepsilon and the restriction of ff (resp. gg) to K′K' is a continuous mapping of K′K' into F (resp. into Fs′F'_s); consequently g(K′)g(K') is weakly compact, hence equicontinuous on F′F' (TVS, III, §4, No. 2, Th. 1 or IV, §1, Exer. 10). Now, the restriction of the canonical bilinear form on F×F′F \times F' to the product of F and an equicontinuous subset of F′F' is continuous for the product topology of the topology of F and σ(F′,F)\sigma(F', F) (GT, X, §2, No. 1, Cor. 4 of Prop. 1); it follows that the restriction of ⟨f,g⟩\langle f, g \rangle to K′K' is continuous, hence that ⟨f,g⟩\langle f, g \rangle is μ\mu-measurable. Moreover,

∣⟨f(t),g(t)⟩∣≤∣f(t)∣⋅∣g(t)∣≤∣f(t)∣N∞(g) |\langle f(t), g(t) \rangle| \leq |f(t)| \cdot |g(t)| \leq |f(t)| N_\infty(g)

locally almost everywhere, consequently ⟨f,g⟩\langle f, g \rangle is essentially μ\mu-integrable and the inequality (3) holds (Ch. IV, §5, No. 6, Th. 5 and Ch. V, §1, No. 3, Lemma).

It remains to show that θ\theta is a surjective isometry. Let uu be a continuous linear form on LF1L^1_F. The mapping (h~,z)↦u(h~z)(\tilde{h}, z) \mapsto u(\tilde{h}z) is a continuous bilinear form on L1×FL^1 \times F, because

∣u(h~z)∣≤∥u∥⋅N1(hz)≤∥u∥⋅∣z∣⋅N1(h). |u(\tilde{h}z)| \leq \|u\| \cdot N_1(hz) \leq \|u\| \cdot |z| \cdot N_1(h) .

By Cor. 1 of Th. 1 of No. 5, there exists a mapping gg of T into F′F', belonging to LFs′∞\mathscr{L}_{F'_s}^\infty, such that ∣g(t)∣≤∥u∥|g(t)| \leq \|u\| for all t∈Tt \in T and such that u(h~z)=∫⟨hz,g⟩ dμu(\tilde{h}z) = \int \langle hz, g \rangle \, d\mu for every function h∈L1h \in \mathscr{L}^1 with class h~\tilde{h} in L1L^1 and every z∈Fz \in F. In other words, the linear forms uu and θ(g˙)\theta(\dot{g}) coincide on the subspace of LF1L^1_F generated by the elements of the form h~z\tilde{h}z (h~∈L1,z∈F\tilde{h} \in L^1, z \in F). Since this subspace is dense in LF1L^1_F (Ch. IV, §3, No. 5, Prop. 10), it follows that u=θ(g˙)u = \theta(\dot{g}), which already proves that θ\theta is surjective. Moreover, by (3), ∥θ(g˙)∥≤N∞(g)≤∥u∥=∥θ(g˙)∥\| \theta(\dot{g}) \| \leq N_\infty(g) \leq \| u \| = \| \theta(\dot{g}) \|, whence ∥θ(g˙)∥=N∞(g)\| \theta(\dot{g}) \| = N_\infty(g), and this concludes the proof.

7. Integration of a vector-valued function with respect to a vectorial measure

Proposition 11

— Let F,G,HF, G, H be three Banach spaces, Φ\Phi a continuous bilinear mapping of F×GF \times G into HH. Let mm be a majorizable vectorial measure on TT, with values in GG. Then there exists one and only one continuous linear mapping IΦ,mI_{\Phi,m} of L‾F1(∣m∣)\overline{\mathscr{L}}^1_F(|m|) into HH such that, for every z∈Fz \in F and every numerical function hh integrable for ∣m∣|m|, one has IΦ,m(hz)=Φ(z,∫hdm)I_{\Phi,m}(hz) = \Phi(z, \int h dm). *Moreover,

∣IΦ,m(f)∣≤∥Φ∥∫∣f∣d∣m∣ |I_{\Phi,m}(f)| \leq \| \Phi \| \int |f| d|m|

for every function f∈L‾F1(∣m∣)f \in \overline{\mathscr{L}}^1_F(|m|).

If there exists such a mapping, its value for a step function ff over the ∣m∣|m|-integrable sets is uniquely determined: for, it is known that one can then write f=∑iaiφXif = \sum_i a_i \varphi_{X_i}, where the XiX_i are ∣m∣|m|-integrable and disjoint, and the ai∈Fa_i \in F (Ch. IV, §4, No. 9, Lemma). The value of IΦ,m(f)I_{\Phi,m}(f) must therefore be equal to ∑iΦ(ai,∫φXidm)\sum_i \Phi(a_i, \int \varphi_{X_i} dm). Now, we have (No. 3, Prop. 5)

∣∑iΦ(ai,∫φXidm)∣≤∥Φ∥⋅∑i∣ai∣⋅∣m∣(Xi)=∥Φ∥∫∣f∣d∣m∣, \left| \sum_i \Phi \left( a_i, \int \varphi_{X_i} dm \right) \right| \leq \| \Phi \| \cdot \sum_i |a_i| \cdot |m|(X_i) = \| \Phi \| \int |f| d|m|,

which shows first of all that the element ∑iΦ(ai,∫φXidm)\sum_i \Phi(a_i, \int \varphi_{X_i} dm) of HH does not depend on the particular expression of ff in the form ∑iaiφXi\sum_i a_i \varphi_{X_i}, hence that we may denote it by IΦ,m(f)I_{\Phi,m}(f). One verifies immediately that the mapping IΦ,mI_{\Phi,m} so defined is linear on the space EF\mathscr{E}_F of step functions over the ∣m∣|m|-integrable sets: for, it suffices to write two functions f,gf, g of EF\mathscr{E}_F in the form f=∑iaiφXif = \sum_i a_i \varphi_{X_i} and g=∑ibiφXig = \sum_i b_i \varphi_{X_i} with the same finite family of pairwise disjoint ∣m∣|m|-integrable sets XiX_i (which is possible by virtue of the Lemma of Ch. IV, §4, No. 9). The inequality (5) then shows that IΦ,mI_{\Phi,m} is continuous on EF\mathscr{E}_F, and since this subspace is dense in L‾F1\overline{\mathscr{L}}^1_F (Ch. IV, §4, No. 10, Cor. 1 of Prop. 19 and Ch. V, §1, No. 3), one deduces from this the existence and uniqueness of IΦ,mI_{\Phi,m}, as well as the inequality (4).

One says that IΦ,m(f)I_{\Phi,m}(f) is the integral of ff with respect to mm (relative to the bilinear mapping Φ\Phi); when the value of the bilinear mapping Φ\Phi at the point (x,y)(x,y) is denoted xyxy, we shall write ∫f dm\int f\,dm instead of IΦ,m(f)I_{\Phi,m}(f).

With the notations of No. 6, the integral ∫⟨f,g⟩ dμ\int \langle f, g \rangle\,d\mu is none other than IΦ,m(f)I_{\Phi,m}(f) with Φ(x,x′)=⟨x,x′⟩\Phi(x,x') = \langle x, x' \rangle and m=g⋅μm = g \cdot \mu.

Corollary

If* mm and m′m' are two majorizable measures on TT, with values in GG, then IΦ,m+m′=IΦ,m+IΦ,m′I_{\Phi,m+m'} = I_{\Phi,m} + I_{\Phi,m'} and IΦ,λm=λIΦ,mI_{\Phi,\lambda m} = \lambda I_{\Phi,m} for every scalar λ\lambda.

The second assertion is immediate. The first signifies that for every function ff that is both ∣m∣|m|-integrable and ∣m′∣|m'|-integrable,

IΦ,m+m′(f)=IΦ,m(f)+IΦ,m′(f). I_{\Phi,m+m'}(f) = I_{\Phi,m}(f) + I_{\Phi,m'}(f).

The function ff is (∣m∣+∣m′∣)(|m| + |m'|)-integrable (Ch. V, §2, No. 2, Cor. 1 of Prop. 3), hence a fortiori (∣m+m′∣)(|m + m'|)-integrable, and the first member of (6) is indeed meaningful. To show (6), it suffices to do so for ff a step function over the (∣m∣+∣m′∣)(|m| + |m'|)-integrable sets, since the set of these functions is dense in LF1(∣m∣+∣m′∣)\mathscr{L}_F^1(|m| + |m'|) and the two members of (6) are continuous in the latter space, by virtue of (4). But for f=aφXf = a \varphi_X, where XX is (∣m∣+∣m′∣)(|m| + |m'|)-integrable, the two members of (6) reduce to Φ(a,∫φX dm)+Φ(a,∫φX dm′)\Phi(a, \int \varphi_X\,dm) + \Phi(a, \int \varphi_X\,dm'), whence the corollary.

Remark

— When mm is of the form bμb\mu, where b∈Gb \in G and μ\mu is a real measure on TT,

IΦ,m(f)=∫Φ(f(t),b) dμ(t) I_{\Phi,m}(f) = \int \Phi(f(t), b)\,d\mu(t)

for every function f∈LF1(μ)f \in \mathscr{L}_F^1(\mu), because both members are continuous on this space and coincide when ff is a step function over the ∣μ∣|\mu|-integrable sets.

8. Complex measures

Definition 6

One calls complex measure on* TT every continuous linear form on the complex vector space KC(T)\mathscr{K}_C(T).\footnote{Cf. Ch. III, §1, No. 3, Def. 2.}

The space MC(T)\mathscr{M}_C(T) of complex measures on TT is thus the dual of the Hausdorff locally convex space KC(T)\mathscr{K}_C(T).

If mm is a complex measure on TT, its restriction to K(T)\mathscr{K}(T) is a vectorial measure on TT with values in C\mathbf{C} (regarded as a vector space over R\mathbf{R});

m is determined by this restriction, since if f=f1+if2∈HC(T)f = f_1 + i f_2 \in \mathscr{H}_\mathbf{C}(T), the real part f1f_1 and the imaginary part f2f_2 of ff are in H(T)\mathscr{H}(T), and m(f)=m(f1)+im(f2)m(f) = m(f_1) + i m(f_2). Conversely, for every vectorial measure m0m_0 on T with values in C\mathbf{C}, the formula m(f)=m0(f1)+im0(f2)m(f) = m_0(f_1) + i m_0(f_2) defines a complex measure mm, the only one on T whose restriction to H(T)\mathscr{H}(T) is m0m_0. We shall therefore henceforth identify a complex measure with its restriction to H(T)\mathscr{H}(T); such a measure mm is of the form m=μ1+iμ2m = \mu_1 + i \mu_2, where μ1\mu_1 and μ2\mu_2 are two real measures on T, which are called, respectively, the real part and the imaginary part of mm. The support of mm is the union of the supports of μ1\mu_1 and μ2\mu_2. One knows that mm is majorizable (No. 3, Cor. of Prop. 4); we shall call absolute value of mm the positive measure ∣m∣|m| corresponding to the absolute value ∣x1+ix2∣=x12+x22|x_1 + i x_2| = \sqrt{x_1^2 + x_2^2} on C\mathbf{C}. One has ∣m∣=(μ12+μ22)1/2|m| = (\mu_1^2 + \mu_2^2)^{1/2} (No. 4, Remark following Prop. 9),3^3 and ∣μ1∣≤∣m∣|\mu_1| \leq |m|, ∣μ2∣≤∣m∣|\mu_2| \leq |m|, ∣m∣≤∣μ1∣+∣μ2∣|m| \leq |\mu_1| + |\mu_2|; moreover, mm is a measure with base ∣m∣|m|, and one can write m=h⋅∣m∣m = h \cdot |m|, where h∈LC∞(∣m∣)h \in \mathscr{L}_\mathbf{C}^\infty(|m|) and ∣h(t)∣=1|h(t)| = 1 locally almost everywhere for ∣m∣|m| (No. 4, Prop. 9).4^4 The supports of mm and ∣m∣|m| are the same.

For every mapping ff of T into a complex Banach space F, essentially integrable with respect to ∣m∣|m|, one can define (No. 7) the integral of ff with respect to mm (corresponding to the R-bilinear mapping (x,λ)↦λx(x, \lambda) \mapsto \lambda x of F×CF \times \mathbf{C} into F), which will be denoted ∫f dm\int f \, dm; it follows at once from the uniqueness property of Prop. 11 that (with the preceding notations) ∫f dm=∫f dμ1+i∫f dμ2=∫fh d∣m∣\int f \, dm = \int f \, d\mu_1 + i \int f \, d\mu_2 = \int f h \, d|m|. We therefore have m(f)=∫f dmm(f) = \int f \, dm for f∈HC(T)f \in \mathscr{H}_\mathbf{C}(T). We say that ff is essentially integrable with respect to mm if it is so for ∣m∣|m|;5^5 mappings that are mm-integrable, mm-measurable, locally mm-integrable, mm-negligible or locally mm-negligible are defined similarly. We write

LFp(T,m)(resp. L‾Fp(T,m), LFp(T,m)) \mathscr{L}_F^p(T, m) \quad \text{(resp. } \overline{\mathscr{L}}_F^p(T, m), \ L_F^p(T, m) \text{)}
instead of LFp(T,∣m∣)\mathscr{L}_F^p(T, |m|) (resp. L‾Fp(T,∣m∣), LFp(T,∣m∣)\overline{\mathscr{L}}_F^p(T, |m|), \ L_F^p(T, |m|)); these are complex vector spaces.

For ff to be mm-integrable (resp. essentially mm-integrable), it is necessary and sufficient that ff be integrable (resp. essentially integrable) with respect to each of the four measures μ1+,μ1−,μ2+,μ2−\mu_1^+, \mu_1^-, \mu_2^+, \mu_2^-, by virtue of the inequalities between ∣m∣,∣μ1∣,∣μ2∣|m|, |\mu_1|, |\mu_2| and the relations ∣μk∣=μk++μk−|\mu_k| = \mu_k^+ + \mu_k^- (Ch. V, §2, No. 2, Prop. 3 and its Cor. 1).

If ff is essentially mm-integrable (resp. mm-integrable), then ∣f∣|f| is essen-

--- 3^3In particular, this definition of ∣m∣|m| coincides with that in Ch. III, §1, No. 6 (cf. Ch. V, §5, No. 9). 4^4Cf. Ch. V, §5, No. 5, Cor. 3 of Th. 2 for a sharper statement. 5^5Cf. Ch. V, §1, remarks at the end of No. 3.

tially ∣m∣|m|-integrable (resp. ∣m∣|m|-integrable), and it follows from Prop. 11 that

∣∫f dm∣≤∫∣f∣ d∣m∣. \left| \int \mathbf{f}\, dm \right| \leq \int |\mathbf{f}| \, d|m|.

Let F and G be two complex Banach spaces, uu a continuous linear mapping of F into G. If f\mathbf{f} is an essentially mm-integrable (resp. mm-integrable) mapping of T into F, then u∘fu \circ \mathbf{f} is essentially mm-integrable (resp. mm-integrable) and ∫(u∘f) dm=u(∫f dm)\int (u \circ \mathbf{f})\, dm = u(\int \mathbf{f}\, dm); this follows at once from the foregoing and the analogous proposition for essentially ∣m∣|m|-integrable functions (Ch. IV, §4, No. 2, Th. 1 and Ch. V, §1, No. 3, Lemma and Def. 3).

Let mm be a complex measure on T and let hh be a locally mm-integrable complex function. For every function f∈KC(T)f \in \mathscr{K}_C(T), the function fhfh is mm-integrable and the mapping f↦∫fh dmf \mapsto \int fh\, dm is a complex measure, denoted h⋅mh \cdot m and called the measure with density hh with respect to mm. If m=g⋅∣m∣m = g \cdot |m|, it is clear that h⋅m=hg⋅∣m∣h \cdot m = hg \cdot |m|; since, moreover, ∣g(t)∣=1|g(t)| = 1 locally almost everywhere for ∣m∣|m|, for f\mathbf{f} to be essentially integrable for n=h⋅mn = h \cdot m it is necessary and sufficient that fhfh be essentially mm-integrable, in which case ∫f dn=∫(fh) dm\int \mathbf{f}\, dn = \int (\mathbf{f}h)\, dm. Moreover, ∣h⋅m∣=∣h∣⋅∣m∣|h \cdot m| = |h| \cdot |m|. We again say that every measure of the form h⋅mh \cdot m is a complex measure with base mm; two complex measures m,m′m, m' are said to be equivalent if each has a density with respect to the other, or, what amounts to the same, if m′=h⋅mm' = h \cdot m with hh locally mm-integrable and h(t)≠0h(t) \neq 0 locally almost everywhere for ∣m∣|m|. It is clear that mm and ∣m∣|m| are equivalent and that, for mm and m′m' to be equivalent, it is necessary and sufficient that ∣m∣|m| and ∣m′∣|m'| be so.

If mm and m′m' are two complex measures on T, and f\mathbf{f} is a function with values in a complex Banach space F, essentially integrable (resp. integrable) for both mm and m′m', then, for any complex numbers λ\lambda and λ′\lambda', f\mathbf{f} is essentially integrable (resp. integrable) for λm+λ′m′\lambda m + \lambda' m', and

∫f d(λm+λ′m′)=λ∫f dm+λ′∫f dm′. \int \mathbf{f}\, d(\lambda m + \lambda' m') = \lambda \int \mathbf{f}\, dm + \lambda' \int \mathbf{f}\, dm'.

For, this follows from the Cor. of Prop. 11 of No. 7.

In addition, it follows from the definitions that

∣λm+λ′m′∣≤∣λ∣⋅∣m∣+∣λ′∣⋅∣m′∣. |\lambda m + \lambda' m'| \leq |\lambda| \cdot |m| + |\lambda'| \cdot |m'|.

One calls conjugate measure of a complex measure mm the complex measure m‾\overline{m} defined by m‾(f)=m(f‾)\overline{m}(f) = m(\overline{f}) for f∈KC(T)f \in \mathscr{K}_C(T). If m=μ1+iμ2m = \mu_1 + i \mu_2, where μ1\mu_1 and μ2\mu_2 are real measures, then m‾=μ1−iμ2\overline{m} = \mu_1 - i \mu_2 and ∣m‾∣=∣m∣|\overline{m}| = |m|; if m=h⋅∣m∣m = h \cdot |m| then m‾=h‾⋅∣m∣\overline{m} = \overline{h} \cdot |m|. If ff is an essentially mm-integrable (resp.

m-integrable) function with complex values, then f‾\overline{f} is essentially m‾\overline{m}-integrable (resp. m‾\overline{m}-integrable) and

∫f‾ dm‾=∫f dm‾. \int \overline{f}\, d\overline{m} = \overline{\int f\, dm}.

Proposition 12

Let m be a complex measure on T, p and q conjugate exponents (Ch. IV, §6, No. 4). The bilinear form (f,g)↦∫fg dm(f,g) \mapsto \int fg\, dm is defined and continuous on the product LCp(m)×LCq(m)\mathscr{L}_C^p(m) \times \mathscr{L}_C^q(m); the inequality ∣∫fg dm∣≤Np(f)Nq(g)|\int fg\, dm| \leq N_p(f)N_q(g) holds, and Nq(g)N_q(g) is the norm of the continuous linear form on LCp(m)\mathscr{L}_C^p(m) deduced from the linear form f↦∫fg dmf \mapsto \int fg\, dm by passage to the quotient.

Moreover, if 1≤p<+∞1 \leq p < +\infty, then every continuous linear form on the complex vector space LCp(m)\mathscr{L}_C^p(m) is of the type f↦∫fg dmf \mapsto \int fg\, dm, where gg is a function in LCq(m)\mathscr{L}_C^q(m), whose class in LCq(m)\mathscr{L}_C^q(m) is uniquely determined.

Since m=h⋅∣m∣m = h \cdot |m|, where ∣h(t)∣=1|h(t)| = 1 locally almost everywhere, the first assertion follows at once from Hölder’s inequality (Ch. IV, §6, No. 4, Th. 2); the second derives from Prop. 3 of Ch. IV, §6, No. 4. Finally, if uu is a continuous linear form on LCp\mathscr{L}_C^p, its restriction to the (real) subspace Lp\mathscr{L}^p of LCp\mathscr{L}_C^p is a continuous R\mathbf{R}-linear mapping of Lp\mathscr{L}^p into C\mathbf{C}; if 1≤p<+∞1 \leq p < +\infty, it is therefore of the type f↦∫fg1 d∣m∣+i∫fg2 d∣m∣f \mapsto \int fg_1\, d|m| + i \int fg_2\, d|m|, where g1g_1 and g2g_2 belong to Lq\mathscr{L}^q (Ch. V, §5, No. 8, Th. 4); whence the final assertion, on setting g=(g1+ig2)h−1g = (g_1 + ig_2)h^{-1}.

9. Bounded complex measures⁶

For every complex measure mm on TT, one sets

∥m∥=sup⁡∥f∥≤1, f∈HC(T)∣m(f)∣. \|m\| = \sup_{\|f\| \leq 1,\, f \in \mathscr{H}_C(T)} |m(f)|.

One says that mm is bounded if ∥m∥<+∞\|m\| < +\infty; it comes to the same to say that mm is continuous on HC(T)\mathscr{H}_C(T) equipped with the topology of uniform convergence, hence can be extended to a continuous linear form (of norm ∥m∥\|m\|) on the Banach space HC(T)\mathscr{H}_C(T) of continuous complex functions tending to 0 at infinity.

Lemma 5

Let m be a complex measure on T, f an m-integrable complex function. Then ∫∣f∣ d∣m∣=sup⁡∣∫fh dm∣\int |f|\, d|m| = \sup |\int fh\, dm|, as h runs over the set of functions in HC(T)\mathscr{H}_C(T) such that ∣h(t)∣≤1|h(t)| \leq 1 for all t∈Tt \in T*.

⁶Cf. Ch. III, §1, No. 8.

If m=g⋅∣m∣m = g \cdot |m|, then ∫∣f∣d∣m∣=∫∣fg∣d∣m∣\int |f| d|m| = \int |f g| d|m| and ∫fh dm=∫fgh d∣m∣\int f h \, dm = \int f g h \, d|m|. Set ζ(t)=0\zeta(t) = 0 when f(t)g(t)=0f(t)g(t) = 0, and ζ(t)=f(t)g(t)∣f(t)g(t)∣\zeta(t) = \frac{f(t)g(t)}{|f(t)g(t)|} when f(t)g(t)≠0f(t)g(t) \neq 0; ζ\zeta is ∣m∣|m|-measurable, thus for every ε>0\varepsilon > 0 there exists a compact subset K of T such that ∫T−K∣f∣ d∣m∣≤ε\int_{T-K} |f| \, d|m| \leq \varepsilon, the restriction of ζ\zeta to K is continuous, and ∣ζ(t)∣=1|\zeta(t)| = 1 on K. Therefore, by virtue of Urysohn’s theorem, there exists a continuous function ζ1\zeta_1 defined on T, with complex values, such that ζ1=ζ\zeta_1 = \zeta on K and such that ∣ζ1(t)∣≤2|\zeta_1(t)| \leq 2 and ζ1(t)≠0\zeta_1(t) \neq 0 for every t∈Tt \in T; setting h(t)=ζ1(t)/∣ζ1(t)∣h(t) = \zeta_1(t)/|\zeta_1(t)|, we see that hh is continuous on T, coincides with ζ\zeta on K, and is such that ∣h(t)∣=1|h(t)| = 1 for all t∈Tt \in T. Finally, let uu be a continuous mapping of T into [0,1][0,1], equal to 1 on K and with compact support; setting h1=h−1uh_1 = h^{-1}u, we have

∣∫fh1 dm−∫∣f∣ d∣m∣∣≤2∫T−K∣f∣ d∣m∣≤2ε, \left| \int f h_1 \, dm - \int |f| \, d|m| \right| \leq 2 \int_{T-K} |f| \, d|m| \leq 2\varepsilon ,
which proves the lemma.

Proposition 13

— *Let m be a complex measure, and μ=∣m∣\mu = |m|. For m to be bounded, it is necessary and sufficient that μ\mu be bounded, in which case ∥m∥=∥μ∥\|m\| = \|\mu\|.

We have m=g⋅μm = g \cdot \mu, where gg is μ\mu-measurable and ∣g(t)∣=1|g(t)| = 1 for all t∈Tt \in T. If μ\mu is bounded then, for every function f∈KC(T)f \in \mathscr{K}_\mathbf{C}(T),

∣m(f)∣=∣∫fg dμ∣≤N∞(fg)∥μ∥=∥f∥⋅∥μ∥, |m(f)| = \left| \int f g \, d\mu \right| \leq N_\infty(fg)\|\mu\| = \|f\| \cdot \|\mu\|,
therefore mm is bounded and ∥m∥≤∥μ∥\|m\| \leq \|\mu\|. If mm is bounded, then for every f∈KC(T)f \in \mathscr{K}_\mathbf{C}(T) we have, on taking into account Lemma 5,
∣μ(f)∣≤∥f∥⋅∥m∥, |\mu(f)| \leq \|f\| \cdot \|m\|,
therefore μ\mu is bounded and ∥μ∥≤∥m∥\|\mu\| \leq \|m\|. Whence the proposition.

Corollary

— *Let m be a bounded complex measure. Every function f∈LF∞(m)f \in \mathscr{L}_\mathbf{F}^\infty(m) is then m-integrable, and ∣∫f dm∣≤N∞(f)∥m∥\left| \int f \, dm \right| \leq N_\infty(f)\|m\|.

For, ff is mm-measurable and, setting μ=∣m∣\mu = |m|, we have

∫∗∣f∣ dμ≤N∞(f)∥μ∥=N∞(f)∥m∥, \int^* |f| \, d\mu \leq N_\infty(f)\|\mu\| = N_\infty(f)\|m\|,
therefore ff is ∣m∣|m|-integrable (Ch. IV, §5, No. 6, Th. 5) and
∣∫f dm∣≤∫∣f∣ dμ≤N∞(f)∥m∥. \left| \int f \, dm \right| \leq \int |f| \, d\mu \leq N_\infty(f)\|m\|.

10. Image of a complex measure; induced complex measure; product of complex measures\footnote{Cf. Ch. V, §6, No. 4; Ch. IV, §5, No. 7 and Ch. V, §7; Ch. III, §4 and Ch. V, §8, Nos. 2–5.}

Let mm be a complex measure on TT, and let π\pi be a mapping of TT into a locally compact space XX. We shall say that π\pi is mm-proper if π\pi is ∣m∣|m|-proper (Ch. V, §6, No. 1, Def. 1); it is then immediate that for every function f∈HC(X)f \in \mathscr{H}_C(X), the function f∘πf \circ \pi is essentially mm-integrable and

∣∫(f∘π) dm∣≤∫∣f∘π∣ d∣m∣=∫∣f∣ d(π(∣m∣)), \left| \int (f \circ \pi)\, dm \right| \leq \int |f \circ \pi|\, d|m| = \int |f|\, d(\pi(|m|)),

therefore the mapping f↦∫(f∘π) dmf \mapsto \int (f \circ \pi)\, dm is continuous on HC(X)\mathscr{H}_C(X), in other words is a complex measure on XX, which is denoted π(m)\pi(m) and called the image of mm under π\pi. Moreover, it follows from (8) that ∣π(m)∣≤π(∣m∣)|\pi(m)| \leq \pi(|m|). If mm and m′m' are two complex measures on TT and if π\pi is both mm-proper and m′m'-proper, then π\pi is (λm+λ′m′)(\lambda m + \lambda' m')-proper for any complex scalars λ,λ′\lambda, \lambda', and π(λm+λ′m′)=λπ(m)+λ′π(m′)\pi(\lambda m + \lambda' m') = \lambda \pi(m) + \lambda' \pi(m').

Let YY be a locally compact subspace of TT. For every function f∈HC(Y)f \in \mathscr{H}_C(Y), the function f′f' on TT, defined by f′(t)=f(t)f'(t) = f(t) if t∈Yt \in Y and by f′(t)=0f'(t) = 0 if t∉Yt \notin Y, is mm-integrable (Ch. IV, §5, No. 7); it is immediate that the mapping f↦∫f′ dmf \mapsto \int f'\, dm is a complex measure on YY, called the measure induced on YY by mm and denoted mYm_Y. If m=g⋅∣m∣m = g \cdot |m|, it is clear that mY=gY⋅∣m∣Ym_Y = g_Y \cdot |m|_Y, where gYg_Y is the restriction to YY of the function gg, which is locally integrable for ∣m∣Y|m|_Y (Ch. V, §7, No. 1); moreover, since ∣gY∣=1|g_Y| = 1 locally almost everywhere for ∣m∣Y|m|_Y (Ch. V, §7, No. 1, Cor. 1 of Prop. 1), we have ∣mY∣=∣m∣Y|m_Y| = |m|_Y.\footnote{Cf. Ch. IV, §5, No. 7, Lemma 3.}

Let TT and T′T' be two locally compact spaces, mm (resp. m′m') a complex measure on TT (resp. T′T'). Write m=g⋅∣m∣m = g \cdot |m| and m′=g′⋅∣m′∣m' = g' \cdot |m'|. The function g⊗g′g \otimes g' is locally integrable on T×T′T \times T' for the positive measure ∣m∣⊗∣m′∣|m| \otimes |m'| (Ch. V, §8, No. 5, Prop. 10), and one verifies immediately that if gg (resp. g′g') is replaced by a function g1g_1 (resp. g1′g'_1) equal to gg (resp. g′g') locally almost everywhere for ∣m∣|m| (resp. ∣m′∣|m'|), then g1⊗g1′g_1 \otimes g'_1 is equal to g⊗g′g \otimes g' locally almost everywhere for ∣m∣⊗∣m′∣|m| \otimes |m'|. The complex measure (g⊗g′)⋅(∣m∣⊗∣m′∣)(g \otimes g') \cdot (|m| \otimes |m'|) on T×T′T \times T' therefore depends only on mm and m′m'; it is denoted m⊗m′m \otimes m' and is called the product measure of mm and m′m'. Since ∣g⊗g′∣=1|g \otimes g'| = 1 locally almost everywhere for ∣m∣⊗∣m′∣|m| \otimes |m'| (Ch. V, §8, No. 2, Prop. 4), we have ∣m⊗m′∣=∣m∣⊗∣m′∣|m \otimes m'| = |m| \otimes |m'|.\footnote{Cf. Ch. III, §4, No. 2, Prop. 3.}

The reader will easily verify that all of the propositions proved in Ch. V relative to the image of a positive measure, the measure induced by a positive measure, and the product of positive measures, except those in which upper integrals or essential upper integrals intervene, remain valid when the positive measures are replaced by arbitrary complex measures.

Finally, one defines as in §1 the concept of scalarly essentially m-integrable function for a complex measure m; for a function f to have this property, it is necessary and sufficient that f be scalarly essentially integrable with respect to ∣μ1∣|\mu_1| and ∣μ2∣|\mu_2|, where μ1\mu_1 and μ2\mu_2 are the real and imaginary parts of mm, in which case ∫fdm=∫fdμ1+i∫fdμ2\int f dm = \int f d\mu_1 + i \int f d\mu_2. We leave to the reader the task of carrying over the results of §1 to complex measures.

Exercises

See the exercises for § 2.

Transcribed from the printed volume. Not translated.