Bourbaki

Definition 6

Tag 09B4, permanent. Cite it as [Bourbaki, Tag 09B4].

Integration, VI, p. 34, § 2. Vectorial measures . "

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}.

Bourbaki puts the proof directly after the statement, so what is above is the statement and its proof together.

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