Bourbaki

§ 6. Convexity inequalities

1. The convexity theorem

Theorem 1

— Let XX be a locally compact space, μ\mu a positive measure on XX, FF a real Banach space, DD a closed convex set in FF, and ff a function on XX such that f(X)⊂Df(X) \subset D. For every non-negligible integrable numerical function g⩾0g \geqslant 0 such that fgfg is integrable, the point ∫fg dμ∫g dμ\frac{\int fg\, d\mu}{\int g\, d\mu} belongs to DD.

For, let F′F' be the dual of FF and let ⟨z,a′⟩⩽α\langle z, a' \rangle \leqslant \alpha (a′∈F′,α∈Ra' \in F', \alpha \in \mathbf{R}) be a relation defining a closed half-space containing DD. Since fgfg is integrable, so is the numerical function ⟨fg,a′⟩=⟨f,a′⟩g\langle fg, a' \rangle = \langle f, a' \rangle g, and

∫⟨fg,a′⟩ dμ=⟨∫fg dμ,a′⟩ \int \langle fg, a' \rangle\, d\mu = \left\langle \int fg\, d\mu, a' \right\rangle

(§ 4, No. 2, Cor. 1 of Th. 1); but, by hypothesis, ⟨f(x),a′⟩⩽α\langle f(x), a' \rangle \leqslant \alpha for all x∈Xx \in X, therefore ⟨f(x)g(x),a′⟩⩽αg(x)\langle f(x)g(x), a' \rangle \leqslant \alpha g(x); on integrating, we have

⟨∫fg dμ,a′⟩⩽α∫g dμ. \left\langle \int fg\, d\mu, a' \right\rangle \leqslant \alpha \int g\, d\mu .

This proves that the point ∫fg dμ∫g dμ\frac{\int fg\, d\mu}{\int g\, d\mu} belongs to every closed half-space containing DD; but, by the Hahn–Banach theorem, DD is the intersection of the closed half-spaces containing it (TVS, II, §5, No. 3, Cor. 1 of Prop. 4), whence the theorem.

Corollary

— If the positive measure μ\mu has total mass equal to 1 and if ff is integrable, then ∫f dμ\int f\, d\mu belongs to the closed convex envelope of f(X)f(X) in FF.

It suffices to take for gg the constant function 1.

2. Inequality of the mean

We are going to sharpen Th. 1 for numerical measurable functions (finite or not).

Definition 1

— Let X be a locally compact space, μ\mu a measure on X. Given a numerical function f (finite or not), defined locally almost everywhere in X, we call maximum in measure, or μ\mu-maximum (resp. minimum in measure, or μ\mu-minimum) of the function f, and denote by M∞(f)M_\infty(f) (resp. m∞(f)m_\infty(f)), the infimum (resp. supremum) of the set of numbers α\alpha such that f(x)≤αf(x) \leq \alpha (resp. f(x)≥αf(x) \geq \alpha) locally almost everywhere (for μ\mu).

It follows at once from the definition that m∞(f)=−M∞(−f)m_\infty(f) = -M_\infty(-f), thus from every property of the maximum in measure one deduces a corresponding property of the minimum in measure.

For every α>M∞(f)\alpha > M_\infty(f), the set of x∈Xx \in X such that f(x)>αf(x) > \alpha is locally negligible; now, the set of x∈Xx \in X such that f(x)>M∞(f)f(x) > M_\infty(f) is the union of the sets where f(x)>rnf(x) > r_n, with rnr_n running over the set of rational numbers >M∞(f)> M_\infty(f); therefore f(x)≤M∞(f)f(x) \leq M_\infty(f) locally almost everywhere (§ 5, No. 2). Similarly f(x)≥m∞(f)f(x) \geq m_\infty(f) locally almost everywhere; it follows that m∞(f)≤M∞(f)m_\infty(f) \leq M_\infty(f) if the measure μ\mu is nonzero; moreover, the relation m∞(f)=M∞(f)m_\infty(f) = M_\infty(f) is equivalent to saying that ff is equal to a constant locally almost everywhere. It is clear that if the measure μ\mu is nonzero, then

inf⁡x∈Xf(x)≤m∞(f)≤M∞(f)≤sup⁡x∈Xf(x). \inf_{x \in X} f(x) \leq m_\infty(f) \leq M_\infty(f) \leq \sup_{x \in X} f(x).

If two functions f,gf, g are equal locally almost everywhere, then m∞(f)=m∞(g)m_\infty(f) = m_\infty(g) and M∞(f)=M∞(g)M_\infty(f) = M_\infty(g).

Finally, if ff and gg are two functions such that f+gf + g is defined locally almost everywhere, then

(1)

M∞(f+g)≤M∞(f)+M∞(g) M_\infty(f + g) \leq M_\infty(f) + M_\infty(g)
provided the second member is defined, as follows at once from Def. 1; similarly, if ff and gg are both ≥0\geq 0 and are such that fgfg is defined locally almost everywhere, then

(2)

M∞(fg)≤M∞(f)M∞(g) M_\infty(fg) \leq M_\infty(f) M_\infty(g)
provided the second member is defined.

If M∞(f)<+∞M_\infty(f) < +\infty, then f(x)<+∞f(x) < +\infty locally almost everywhere, but not necessarily almost everywhere. A numerical function ff is said to be bounded in measure (for the measure μ\mu) if it is defined and finite almost everywhere and if, moreover, the numbers m∞(f)m_\infty(f) and M∞(f)M_\infty(f) are both finite (the latter condition amounts to saying that M∞(∣f∣)<+∞M_\infty(|f|) < +\infty).

Proposition 1 (Inequality of the mean)

— *Let f be a measurable numerical function that is bounded in measure. For every integrable numerical function g⩾0g \geqslant 0, the function fgfg (defined almost everywhere) is integrable and

m∞(f)∫gd∣μ∣⩽∫fgd∣μ∣⩽M∞(f)∫gd∣μ∣. m_\infty(f) \int g d|\mu| \leqslant \int fg d|\mu| \leqslant M_\infty(f) \int g d|\mu|.

Moreover, two of the three members of the inequality (3) cannot be equal unless, in the set of x∈Xx \in X such that g(x)≠0g(x) \neq 0, f is equal to M∞(f)M_\infty(f) almost everywhere or equal to m∞(f)m_\infty(f) almost everywhere.

Indeed, fgfg is measurable (§ 5, No. 3, Cor. 5 of Th. 1); moreover, the inequality m∞(f)g(x)⩽f(x)g(x)⩽M∞(f)g(x)m_\infty(f)g(x) \leqslant f(x)g(x) \leqslant M_\infty(f)g(x) holds, not only locally almost everywhere, but even almost everywhere, because the set of points x∈Xx \in X where g(x)≠0g(x) \neq 0 is a countable union of integrable sets (§ 5, No. 6, Lemma 1). It follows that fgfg is integrable (§ 5, No. 6, Th. 5) and the inequality (3) holds. On the other hand, the function M∞(f)g−fgM_\infty(f)g - fg is almost everywhere defined and equal to (M∞(f)−f)g(M_\infty(f) - f)g; it is therefore ⩾0\geqslant 0 almost everywhere in XX; since the relation M∞(f)∫gd∣μ∣=∫fgd∣μ∣M_\infty(f) \int g d|\mu| = \int fg d|\mu| is equivalent to ∫(M∞(f)−f)gd∣μ∣=0\int (M_\infty(f) - f)g d|\mu| = 0, it can hold only if the function (M∞(f)−f)g(M_\infty(f) - f)g is negligible, which completes the proof.

Setting aside the trivial case that ∫gd∣μ∣=0\int g d|\mu| = 0, the inequality (3) may be deduced from Th. 1 of No. 1 applied to the interval D=[m∞(f),M∞(f)]D = [m_\infty(f), M_\infty(f)]. One can bring to Th. 1 of No. 1 the complements analogous to those of Prop. 1, that specify the case in which the point (∫fgdμ)/(∫gdμ)(\int fg d\mu)/(\int g d\mu) belongs to the boundary of D (Exer. 2).

3. The spaces LF∞L^\infty_F

Definition 2

For every mapping ff of XX into a Banach space FF, one sets N∞(f)=M∞(∣f∣)N_\infty(f) = M_\infty(|f|); ff is said to be bounded in measure (for the measure μ\mu) if N∞(f)N_\infty(f) is finite. The set of mappings of XX into FF that are measurable and bounded in measure is denoted LF∞(X,μ)\mathscr{L}_F^\infty(X, \mu) (or LF∞(μ)\mathscr{L}_F^\infty(\mu), or simply LF∞\mathscr{L}_F^\infty).

A function ff in LF∞\mathscr{L}_F^\infty may thus be characterized by the fact that there exists a bounded measurable function equal locally almost everywhere to ff.

It follows immediately from (1) that

N∞(f+g)⩽N∞(f)+N∞(g); N_\infty(f + g) \leqslant N_\infty(f) + N_\infty(g);

on the other hand, N∞(αf)=∣α∣N∞(f)N_\infty(\alpha f) = |\alpha| N_\infty(f) for every scalar α\alpha. The set LF∞\mathscr{L}_F^\infty is therefore a linear subspace of the space of all mappings of XX into FF, and N∞(f)N_\infty(f) is a semi-norm on this vector space. Let (fn)(f_n) be a sequence of functions in LF∞\mathscr{L}_F^\infty that converges to f∈LF∞f \in \mathscr{L}_F^\infty for the topology defined by the semi-norm N∞(f)N_\infty(f); for every integer mm, there exist a locally negligible set HmH_m and an integer n0n_0 such that ∣f(x)−fn(x)∣≤1/m|f(x) - f_n(x)| \leq 1/m for every integer n≥n0n \geq n_0 and every x∉Hmx \notin H_m (every countable union of locally negligible sets being locally negligible); the union HH of the HmH_m is locally negligible, and one sees that fn(x)f_n(x) tends uniformly to f(x)f(x) on the complement of the locally negligible set HH; the converse is immediate.

It is clear that every function equal locally almost everywhere to a function in LF∞\mathscr{L}_F^\infty belongs to LF∞\mathscr{L}_F^\infty. In particular, the locally negligible functions defined on XX with values in FF form a linear subspace NF∞\mathscr{N}_F^\infty of LF∞\mathscr{L}_F^\infty, characterized by the relation N∞(f)=0N_\infty(f) = 0 (the closure of 0 for the topology defined by N∞(f)N_\infty(f)). The Hausdorff space associated with LF∞\mathscr{L}_F^\infty, that is, the quotient space LF∞/NF∞\mathscr{L}_F^\infty / \mathscr{N}_F^\infty, is denoted LF∞(X,μ)L_F^\infty(X, \mu) (or LF∞(μ)L_F^\infty(\mu) or LF∞L_F^\infty); its topology is defined by the norm deduced from N∞N_\infty by passage to the quotient; the norm of a class f˙∈LF∞\dot{f} \in L_F^\infty is denoted N∞(f˙)N_\infty(\dot{f}), or also ∥f˙∥∞\| \dot{f} \|_\infty. When F=RF = \mathbf{R} (resp. C\mathbf{C}), we write L∞\mathscr{L}^\infty and L∞L^\infty in place of LR∞\mathscr{L}_\mathbf{R}^\infty and LR∞L_\mathbf{R}^\infty (resp. LC∞\mathscr{L}_\mathbf{C}^\infty and LC∞L_\mathbf{C}^\infty) if this can cause no confusion.

Proposition 2

The space* LF∞\mathscr{L}_F^\infty is complete; the space LF∞L_F^\infty is a Banach space.

For, let (fn)(f_n) be a Cauchy sequence in LF∞\mathscr{L}_F^\infty; for every integer nn, there exists an integer knk_n such that N∞(fr−fs)≤1/nN_\infty(f_r - f_s) \leq 1/n for r≥knr \geq k_n and s≥kns \geq k_n; thus, there exists a locally negligible set ArsA_{rs} such that ∣fr(x)−fs(x)∣≤1/n|f_r(x) - f_s(x)| \leq 1/n for all x∉Arsx \notin A_{rs}. If AnA_n is the union of the sets ArsA_{rs} (for r≥knr \geq k_n and s≥kns \geq k_n), then AnA_n is locally negligible and, for every x∉Anx \notin A_n, ∣fr(x)−fs(x)∣≤1/n|f_r(x) - f_s(x)| \leq 1/n for all indices r≥kn,s≥knr \geq k_n, s \geq k_n. Let AA be the locally negligible set formed by the union of the AnA_n, and set gn(x)=fn(x)g_n(x) = f_n(x) for x∉Ax \notin A, gn(x)=0g_n(x) = 0 for x∈Ax \in A; then gng_n belongs to LF∞\mathscr{L}_F^\infty and, by the definition of AA, the sequence (gn)(g_n) converges uniformly on XX to a function gg. It follows that the function gg is measurable (§ 5, No. 4, Th. 2); moreover, gg is bounded on the set of x∈Xx \in X where ∣gk1(x)∣≤N∞(gk1)|g_{k_1}(x)| \leq N_\infty(g_{k_1}) and, since the complement of this set is locally negligible, gg belongs to LF∞\mathscr{L}_F^\infty. It is clear that in LF∞\mathscr{L}_F^\infty, the sequence (gn)(g_n) has limit gg, and the same is therefore true of the sequence (fn)(f_n), since N∞(fn−gn)=0N_\infty(f_n - g_n) = 0 for all nn. The second part of the proposition may be deduced immediately from this.

Remark

— 1) Every bounded continuous function ff on XX with values in FF belongs to LF∞\mathscr{L}_F^\infty, and

N∞(f)≤∥f∥=sup⁡x∈X∣f(x)∣. N_\infty(f) \leq \| f \| = \sup_{x \in X} |f(x)| .

In order that N∞(f)=∥f∥N_\infty(f) = \|f\| for every bounded continuous function ff, it is necessary and sufficient that the support of the measure μ\mu be equal to XX. For, if there exists a continuous function ff with negligible compact support and not identically zero, then N∞(f)=0N_\infty(f) = 0 and ∥f∥>0\|f\| > 0. Conversely, if the support of μ\mu is equal to XX then, for every bounded continuous function ff and every number α<∥f∥\alpha < \|f\|, the set of x∈Xx \in X such that ∣f(x)∣>α|f(x)| > \alpha is open and nonempty, hence has outer measure >0> 0, which shows that N∞(f)=∥f∥N_\infty(f) = \|f\|.

When the support of μ\mu is equal to XX, we may therefore identify the normed space Cb(X;F)C^b(X; F), of bounded continuous functions on XX with values in FF, with a subspace of the space LF∞L_F^\infty. Since LF∞L_F^\infty is not in general Hausdorff, the subspace Cb(X;F)C^b(X; F) is not in general closed in LF∞L_F^\infty, but its canonical image in LF∞L_F^\infty is a closed subspace of LF∞L_F^\infty (which can moreover be identified with Cb(X;F)C^b(X; F) in the case contemplated). In general, Cb(X;F)C^b(X; F) is distinct from LF∞L_F^\infty, that is, for an arbitrary bounded measurable function ff, there does not in general exist a continuous function gg equal to ff locally almost everywhere (§ 5, Exer. 12). This implies that the space H(X;F)\mathscr{H}(X; F) of mappings of XX into FF, continuous with compact support, is in general not dense in LF∞L_F^\infty, whereas it is dense in each of the spaces LFpL_F^p for 1≤p<+∞1 \leq p < +\infty (§ 3, No. 4. Def. 2).

2) It is immediate that the topology defined by the semi-norm N∞N_\infty is finer than the topology induced on LF∞L_F^\infty by the topology of convergence in measure (§ 5, No. 11).

4. Hölder’s inequality

In this No., pp and qq will denote two real numbers such that 1≤p≤+∞1 \leq p \leq +\infty, 1≤q≤+∞1 \leq q \leq +\infty, bound by the relation 1/p+1/q=11/p + 1/q = 1; thus q=p/(p−1)q = p/(p-1) if 1<p<+∞1 < p < +\infty, q=+∞q = +\infty if p=1p = 1, and q=1q = 1 if p=+∞p = +\infty; pp and qq will be called conjugate exponents. Note that the relation 1≤p≤21 \leq p \leq 2 is equivalent to 2≤q≤+∞2 \leq q \leq +\infty; p=qp = q only when pp and qq are equal to 2.

Theorem 2 (Hölder’s inequality)

— Let ff and gg be two numerical functions that are finite almost everywhere and are such that ff is equal almost everywhere to a function in LpL^p and gg to a function in LqL^q. Then, the function fgfg (defined almost everywhere) is integrable, and

N1(fg)≤Np(f)Nq(g). N_1(fg) \leq N_p(f) N_q(g).

Let f1f_1 (resp. g1g_1) be a function in LpL^p (resp. LqL^q) to which ff (resp. gg) is equal almost everywhere; fgfg is equal almost everywhere to the function f1g1f_1 g_1, which is everywhere defined and finite, and which is measurable, being the product of two measurable functions (§ 5, No. 3, Cor. 5 of Th. 1). If 1<p<+∞1 < p < +\infty, Hölder’s inequality for the upper integral (Ch. I, No. 3, Prop. 4) yields the inequality (4), and the relation N1(fg)<+∞N_1(fg) < +\infty then shows that fgfg is integrable (§ 5, No. 6, Th. 5). If p=1p = 1, q=+∞q = +\infty, the inequality (4) and the fact that fgfg is integrable are immediate consequences of the inequality of the mean (No. 2, Prop. 1); thus the theorem is proved in all cases.

Corollary 1

— Let F,G,HF, G, H be three Banach spaces, and let (u,v)↦Φ(u,v)(u, v) \mapsto \Phi(u, v) be a continuous bilinear mapping of F×GF \times G into HH such that ∣Φ(u,v)∣≤∣u∣⋅∣v∣|\Phi(u, v)| \leq |u| \cdot |v|. If f∈LFpf \in \mathscr{L}_F^p and g∈LGqg \in \mathscr{L}_G^q, then the function Φ(f,g)\Phi(f, g) is integrable and

∣∫Φ(f,g) dμ∣≤∫∣Φ(f,g)∣ d∣μ∣≤Np(f)Nq(g). \left| \int \Phi(f, g)\, d\mu \right| \leq \int |\Phi(f, g)|\, d|\mu| \leq N_p(f) N_q(g).

For, Φ(f,g)\Phi(f, g) is measurable (§ 5, No. 3, Cor. 5 of Th. 1); since ∣Φ(f,g)∣≤∣f∣⋅∣g∣|\Phi(f, g)| \leq |f| \cdot |g|, the corollary follows from Th. 2 and the integrability criterion of § 5, No. 6, Th. 5.

Two special cases of Cor. 1 are important in applications:

Corollary 2

— Let FF be a real (resp. complex) Banach space, F′F' its strong dual (TVS, III, § 3, No. 1), and let (z,z′)↦⟨z,z′⟩(z, z') \mapsto \langle z, z' \rangle be the canonical bilinear form on F×F′F \times F'. If f∈LFpf \in \mathscr{L}_F^p and g∈LF′qg \in \mathscr{L}_{F'}^q, then the real (resp. complex) function ⟨f,g⟩\langle f, g \rangle is integrable and

∣∫⟨f,g⟩ dμ∣≤∫∣⟨f,g⟩∣ d∣μ∣≤Np(f)Nq(g). \left| \int \langle f, g \rangle\, d\mu \right| \leq \int |\langle f, g \rangle|\, d|\mu| \leq N_p(f) N_q(g).

For, ∣⟨z,z′⟩∣≤∣z∣⋅∣z′∣|\langle z, z' \rangle| \leq |z| \cdot |z'|.

When FF is a real or complex Hilbert space, one knows that it can be canonically identified with its dual F′F' (TVS, V, § 1, No. 7). Since the space LF2L_F^2 is complete, we have the following result:

Corollary 3

— Let μ\mu be a positive measure on XX, FF a real (resp. complex) Hilbert space. On the space LF2L_F^2, the symmetric (resp. Hermitian) form

(f~,g~)↦∫⟨f,g⟩ dμ (\widetilde{f}, \widetilde{g}) \mapsto \int \langle f, g \rangle\, d\mu

defines a Hilbert space structure, for which the norm is equal to ∥f~∥2\| \widetilde{f} \|_2.

Corollary 4

— Let FF be a Banach space, ff a function in LFp\mathscr{L}_F^p, and gg a numerical function belonging to Lq\mathscr{L}^q; then, the function fgfg is integrable and

∣∫fg dμ∣≤∫∣fg∣ d∣μ∣≤Np(f)Nq(g). \left| \int fg\, d\mu \right| \leq \int |fg|\, d|\mu| \leq N_p(f) N_q(g).

Corollary 5

— Let f1,f2,…,fnf_1, f_2, \ldots, f_n be n positive integrable functions, and let α1,α2,…,αn\alpha_1, \alpha_2, \ldots, \alpha_n be n numbers >0> 0 such that ∑i=1nαi=1\sum_{i=1}^n \alpha_i = 1; under these conditions, the function f1α1f2α2⋯fnαnf_1^{\alpha_1} f_2^{\alpha_2} \cdots f_n^{\alpha_n} is integrable and

∫f1α1f2α2⋯fnαnd∣μ∣⩽(∫f1d∣μ∣)α1(∫f2d∣μ∣)α2⋯(∫fnd∣μ∣)αn. \int f_1^{\alpha_1} f_2^{\alpha_2} \cdots f_n^{\alpha_n} d|\mu| \leqslant \left( \int f_1 d|\mu| \right)^{\alpha_1} \left( \int f_2 d|\mu| \right)^{\alpha_2} \cdots \left( \int f_n d|\mu| \right)^{\alpha_n}.

For, the product f1α1f2α2⋯fnαnf_1^{\alpha_1} f_2^{\alpha_2} \cdots f_n^{\alpha_n} is measurable, being the product of measurable functions (§ 5, No. 3, Th. 1 and its Cor. 5); since the inequality (8) is true for upper integrals (Ch. I, No. 2, Cor. of Prop. 2), the function f1α1f2α2⋯fnαnf_1^{\alpha_1} f_2^{\alpha_2} \cdots f_n^{\alpha_n} is integrable (§ 5, No. 6, Th. 5), whence the corollary.

Cor. 2 of Th. 2 is sharpened by the following proposition:

Proposition 3

— Let μ\mu be a positive measure on X, F a real or complex Banach space, F' its strong dual, and (z,z′)↦⟨z,z′⟩(z, z') \mapsto \langle z, z' \rangle the canonical bilinear form on F×F′F \times F'.

1° For every function f∈LFpf \in \mathscr{L}_F^p (1≤p≤+∞1 \leq p \leq +\infty),

Np(f)=sup⁡∣∫⟨f,g⟩ dμ∣ N_p(f) = \sup \left| \int \langle f, g \rangle \, d\mu \right|

as g runs over the set of functions in LF′q\mathscr{L}_{F'}^q, such that Nq(g)≤1N_q(g) \leq 1.

2° For every function g∈LF′qg \in \mathscr{L}_{F'}^q (1≤q≤+∞1 \leq q \leq +\infty),

Nq(g)=sup⁡∣∫⟨f,g⟩ dμ∣ N_q(g) = \sup \left| \int \langle f, g \rangle \, d\mu \right|

as f runs over the set of functions in LFp\mathscr{L}_F^p such that Np(f)≤1N_p(f) \leq 1.

Let us first prove the relation (9); we distinguish between two cases.

(i) 1≤p<+∞1 \leq p < +\infty. The relation (9) being trivial when Np(f)=0N_p(f) = 0 (because f and ⟨f,g⟩\langle f, g \rangle are then negligible), we can always suppose, on multiplying f by a scalar, that Np(f)=1N_p(f) = 1. Suppose first that f is an integrable step function, f=∑k=1nakφAkf = \sum_{k=1}^n a_k \varphi_{A_k}, where the AkA_k are pairwise disjoint (§ 4, No. 9, Lemma). Thus ∑k=1n∣ak∣pμ(Ak)=1\sum_{k=1}^n |a_k|^p \mu(A_k) = 1 by hypothesis. For every ε>0\varepsilon > 0, there exists (for every index k) a vector ak′∈F′a'_k \in F' such that ∣ak′∣q=∣ak∣p|a'_k|^q = |a_k|^p if p>1p > 1 (resp. ∣ak′∣=1|a'_k| = 1 if p=1p = 1) and ⟨ak,ak′⟩≥(1−ε)∣ak∣⋅∣ak′∣\langle a_k, a'_k \rangle \geq (1 - \varepsilon)|a_k| \cdot |a'_k| (TVS, IV,

§1, No. 3, Prop. 8). Setting g=∑k=1nak′φAkg = \sum_{k=1}^n a_k' \varphi_{A_k}, we have ∑k=1n∣ak′∣qμ(Ak)=1\sum_{k=1}^n |a_k'|^q \mu(A_k) = 1 if p>1p > 1 (resp. sup⁡1≤k≤n∣ak′∣=1\sup_{1 \leq k \leq n} |a_k'| = 1 if p=1p = 1), thus Nq(g)=1N_q(g) = 1; on the other hand,

∫⟨f,g⟩dμ=∑k=1n⟨ak,ak′⟩μ(Ak)≥(1−ε)∑k=1n∣ak∣⋅∣ak′∣μ(Ak) \int \langle f, g \rangle d\mu = \sum_{k=1}^n \langle a_k, a_k' \rangle \mu(A_k) \geq (1 - \varepsilon) \sum_{k=1}^n |a_k| \cdot |a_k'| \mu(A_k)

and, since ∣ak′∣=∣ak∣p/q=∣ak∣p−1|a_k'| = |a_k|^{p/q} = |a_k|^{p-1} if p>1p > 1 (resp. ∣ak′∣=1|a_k'| = 1 if p=1p = 1), we have

∫⟨f,g⟩dμ≥(1−ε)∑k=1n∣ak∣pμ(Ak)=(1−ε)Np(f)=1−ε, \int \langle f, g \rangle d\mu \geq (1 - \varepsilon) \sum_{k=1}^n |a_k|^p \mu(A_k) = (1 - \varepsilon) N_p(f) = 1 - \varepsilon,

which proves the relation (9) in this case.

Let us pass to the case that ff is any element of LFp\mathscr{L}_F^p such that Np(f)=1N_p(f) = 1. For every ε>0\varepsilon > 0, there exists a step function f1∈LFpf_1 \in \mathscr{L}_F^p such that Np(f−f1)≤εN_p(f - f_1) \leq \varepsilon (§ 4, No. 10, Cor. 1 of Prop. 19). By what we have just seen, there exists a function g∈LFqg \in \mathscr{L}_F^q, such that Nq(g)=1N_q(g) = 1 and

∫⟨f1,g⟩dμ≥Np(f1)−ε≥1−2ε. \int \langle f_1, g \rangle d\mu \geq N_p(f_1) - \varepsilon \geq 1 - 2\varepsilon.

Now,

∫⟨f,g⟩dμ=∫⟨f1,g⟩dμ+∫⟨f−f1,g⟩dμ \int \langle f, g \rangle d\mu = \int \langle f_1, g \rangle d\mu + \int \langle f - f_1, g \rangle d\mu

and, by (6),

∣∫⟨f−f1,g⟩dμ∣≤Np(f−f1)Nq(g), \left| \int \langle f - f_1, g \rangle d\mu \right| \leq N_p(f - f_1) N_q(g),

whence

∣∫⟨f,g⟩dμ∣≥1−3ε, \left| \int \langle f, g \rangle d\mu \right| \geq 1 - 3\varepsilon,

which proves (9).

(ii) p=+∞p = +\infty. We may again restrict ourselves to the case that N∞(f)>0N_\infty(f) > 0. Let α\alpha be any number such that 0<α<N∞(f)0 < \alpha < N_\infty(f); by hypothesis, the set of x∈Xx \in X such that ∣f(x)∣>α|f(x)| > \alpha is measurable and is not locally negligible, therefore it contains a compact set KK of measure >0> 0. Since ff is measurable, there exists a compact set K1⊂KK_1 \subset K of measure >0> 0, such that the restriction of ff to K1K_1 is continuous. It follows that, for every ε>0\varepsilon > 0, there exists a partition of K1K_1 into a finite number of integrable sets, in each of which the oscillation of ff is ≤ε\leq \varepsilon; at least one of these sets AA has measure > 0. Let aa be one of the values of ff in AA; then ∣a∣>α|a| > \alpha and ∣f(x)−a∣≤ε|f(x) - a| \leq \varepsilon for all x∈Ax \in A. There exists a vector a′∈F′a' \in F' such that ∣a′∣=1|a'| = 1 and ∣⟨a,a′⟩∣≥∣a∣−ε|\langle a, a' \rangle| \geq |a| - \varepsilon; the function g=φA⋅a′/μ(A)g = \varphi_A \cdot a'/\mu(A) is integrable and N1(g)=1N_1(g) = 1; on the other hand,

∫⟨f,g⟩dμ=1μ(A)∫⟨f,a′⟩φAdμ. \int \langle f, g \rangle d\mu = \frac{1}{\mu(A)} \int \langle f, a' \rangle \varphi_A d\mu.

Now, one can write

∫⟨f,a′⟩φAdμ=⟨a,a′⟩μ(A)+∫⟨f−a,a′⟩φAdμ, \int \langle f, a' \rangle \varphi_A d\mu = \langle a, a' \rangle \mu(A) + \int \langle f - a, a' \rangle \varphi_A d\mu,

and since

∣⟨f−a,a′⟩φA∣≤εφA, |\langle f - a, a' \rangle \varphi_A| \leq \varepsilon \varphi_A,

we see that

∣∫⟨f,g⟩dμ∣≥∣⟨a,a′⟩∣−ε≥∣a∣−2ε>α−2ε; \left| \int \langle f, g \rangle d\mu \right| \geq |\langle a, a' \rangle| - \varepsilon \geq |a| - 2\varepsilon > \alpha - 2\varepsilon;

since ε\varepsilon is arbitrary and α\alpha is any number < N∞(f)N_\infty(f), the relation (9) is also verified in this case.

One argues in exactly the same manner to prove the relation (10), on considering separately the case 1≤q<+∞1 \leq q < +\infty and the case q=+∞q = +\infty, and using the fact that for every z′∈F′z' \in F', ∣z′∣=sup⁡∣z∣≤1∣⟨z,z′⟩∣|z'| = \sup_{|z| \leq 1} |\langle z, z' \rangle| by the definition of the norm in F′F'.

Remark

— 1) Let E\mathscr{E} be a dense linear subspace of LF′q\mathscr{L}_{F'}^q; then the formula (9) holds when gg runs over the intersection of E\mathscr{E} with the set BB of functions in LF′q\mathscr{L}_{F'}^q such that Nq(g)≤1N_q(g) \leq 1. For, it suffices to observe that the interior B∘\overset{\circ}{B} of BB is dense in BB and that B∘∩E\overset{\circ}{B} \cap \mathscr{E} is dense in B∘\overset{\circ}{B}, since B∘\overset{\circ}{B} is open. This remark applies in particular to the set E=K(X;F′)\mathscr{E} = \mathscr{K}(X; F') of continuous functions with compact support (with values in F′F') when 1≤q<+∞1 \leq q < +\infty, that is, 1<p≤+∞1 < p \leq +\infty. But in this case, the formula (9) is true as gg runs over B∩K(X;F′)B \cap \mathscr{K}(X; F'), even for p=1p = 1. For, we may, as above, restrict ourselves to the case that ff is a step function. We saw then that if N1(f)=1N_1(f) = 1, then for every ε>0\varepsilon > 0 there exists a step function g∈LF′∞g \in \mathscr{L}_{F'}^\infty such that ∣g(x)∣≤1|g(x)| \leq 1 for all x∈Xx \in X and ∣∫⟨f,g⟩dμ∣≥1−ε|\int \langle f, g \rangle d\mu| \geq 1 - \varepsilon. There exists a finite number of pairwise disjoint compact sets KiK_i such that gg has a constant value ai′a'_i on each KiK_i and such that, if KK is the union of the KiK_i, then ∫∣f∣φCKdμ≤ε\int |f| \varphi_{\mathscr{C}_K} d\mu \leq \varepsilon. Let UiU_i be a neighborhood of KiK_i such that the sets UiU_i are pairwise disjoint, and let hih_i be a continuous mapping of XX into [0,1][0, 1] with support contained in UiU_i and equal to 1 on KiK_i. Setting h=∑ai′hih = \sum a'_i h_i, we have h(x)=g(x)h(x) = g(x) on KK and ∣h(x)∣≤1|h(x)| \leq 1 on XX, therefore

∫∣⟨f,h⟩∣φCKdμ≤ε \int |\langle f, h \rangle| \varphi_{\mathscr{C}_K} d\mu \leq \varepsilon

and consequently ∣∫⟨f,h⟩dμ∣≥1−3ε|\int \langle f, h \rangle d\mu| \geq 1 - 3\varepsilon, which proves our assertion. Analogous remarks can be made for the formula (10).

2) Let μ\mu be a positive measure on XX, ff a measurable function ≥0\geq 0 (finite or not) whose support is contained in a countable union of compact sets KnK_n. Then, for every pp such that 1≤p≤+∞1 \leq p \leq +\infty,

(11)Np(f)=sup⁡∫∗∣fg∣dμ, (11) \quad N_p(f) = \sup \int^* |fg| d\mu,

as gg runs over the set of functions in H(X;R)\mathscr{H}(X; \mathbf{R}) such that Nq(g)≤1N_q(g) \leq 1. For, the formula (11) is a special case of (9) when Np(f)<+∞N_p(f) < +\infty, since ff is then equivalent to a function in Lp\mathscr{L}^p (§ 5, No. 6, Th. 5). If Np(f)=+∞N_p(f) = +\infty, for every integer n>0n > 0 set fn=inf⁡(n,fφKn)f_n = \inf(n, f \varphi_{K_n}). Then

Np(fn)=sup⁡∫∗∣fng∣dμ≤sup⁡∫∗∣fg∣dμ, N_p(f_n) = \sup \int^* |f_n g| d\mu \leq \sup \int^* |f g| d\mu,

whence, on passing to the limit (assuming, as we may, that the sequence (Kn)(K_n) is increasing), we have sup⁡∫∗∣fg∣dμ=+∞\sup \int^* |f g| d\mu = +\infty (§ 1, No. 3, Th. 3).

Corollary

— *Let μ\mu be a positive measure on XX, FF a Banach space, F′F' its strong dual, and gg any function in LF′q\mathscr{L}^q_{F'}. Then, the linear form on LFpL^p_F, deduced from the linear form f↦∫⟨f,g⟩dμf \mapsto \int \langle f, g \rangle d\mu on LFp\mathscr{L}^p_F by passage to the quotient, is continuous and has norm Nq(g)N_q(g).

5. Application: relations between the spaces LFpL^p_F (1≤p≤+∞1 \leq p \leq +\infty)

Proposition 4

— *Let ff be a measurable function with values in a Banach space FF; the set II of numbers pp, such that 1≤p≤+∞1 \leq p \leq +\infty and Np(f)N_p(f) is finite, is either empty or is an interval of R‾\overline{\mathbf{R}}. If II is nonempty, the restriction to II of the mapping p↦Np(f)p \mapsto N_p(f) is continuous; moreover, if ff is not negligible, log⁡Np(f)\log N_p(f) is a convex function of 1/p1/p on Iˉ\bar{I}.

We already know (Ch. I, No. 3, Prop. 5) that the set JJ of finite numbers p≥1p \geq 1 such that Np(f)<+∞N_p(f) < +\infty is either empty or is an interval, and that log⁡Np(f)\log N_p(f) is a convex function of 1/p1/p on JJ (when ff is not negligible); this of course implies the continuity of p↦Np(f)p \mapsto N_p(f) on JJ.

If JJ is empty then either I=∅I = \varnothing or I={+∞}I = \{+\infty\}, and the proposition is obvious in this case; assume henceforth that JJ is nonempty. The proposition is also obvious if ff is negligible; assume henceforth that ff is not negligible. If s∈Js \in J then, for every finite number p>sp > s, ∣f∣p=∣f∣s∣f∣p−s|f|^p = |f|^s |f|^{p-s}, and the inequality of the mean shows that

(12)Np(f)≤(Ns(f))s/p(N∞(f))(p−s)/p. (12) \quad N_p(f) \leq (N_s(f))^{s/p} (N_\infty(f))^{(p-s)/p}.

Letting pp tend to +∞+\infty, it follows that

lim sup⁡p→+∞Np(f)≤N∞(f). \limsup_{p \to +\infty} N_p(f) \leq N_\infty(f).

This proves that if +∞∈I+\infty \in I then JJ contains arbitrarily large numbers; thus II is indeed an interval of R‾\overline{\mathbf{R}}, and I‾=J‾\overline{I} = \overline{J}. The proposition will be proved if we show that p↦Np(f)p \mapsto N_p(f) is continuous on J‾\overline{J}, and it suffices to establish continuity at the end-points of JJ. We can suppose, moreover, that JJ does not reduce to a point. Let rr and ss be the left and right end-points of JJ (r<s≤+∞r < s \leq +\infty). Let AA be the (measurable) set of x∈Xx \in X such that ∣f(x)∣≥1|f(x)| \geq 1; then

∫∣f∣pd∣μ∣=∫∣f∣pφAd∣μ∣+∫∣f∣pφCAd∣μ∣. \int |f|^p d|\mu| = \int |f|^p \varphi_A d|\mu| + \int |f|^p \varphi_{C_A} d|\mu|.

As p∈Jp \in J tends to rr, ∣f∣pφA|f|^p \varphi_A tends to ∣f∣rφA|f|^r \varphi_A while decreasing, and ∣f∣pφCA|f|^p \varphi_{C_A} tends to ∣f∣rφCA|f|^r \varphi_{C_A} while increasing. Thus ∫∣f∣pφCAd∣μ∣\int |f|^p \varphi_{C_A} d|\mu| tends to ∫∗∣f∣rφCAd∣μ∣\int^* |f|^r \varphi_{C_A} d|\mu| (§ 1, No. 3, Th. 3). On the other hand, ∣f∣pφA|f|^p \varphi_A is integrable for p∈Jp \in J, and ∫∣f∣pφAd∣μ∣\int |f|^p \varphi_A d|\mu| tends to ∫∣f∣rφAd∣μ∣\int |f|^r \varphi_A d|\mu| (§ 4, No. 3, Prop. 4). Therefore ∫∣f∣pd∣μ∣\int |f|^p d|\mu| tends to ∫∗∣f∣rd∣μ∣\int^* |f|^r d|\mu|, which proves the continuity of p↦Np(f)p \mapsto N_p(f) at rr.

The same reasoning may be applied at the point ss if s<+∞s < +\infty. Finally, suppose that s=+∞s = +\infty. In view of (13), it suffices to prove that

lim inf⁡p→+∞Np(f)≥N∞(f). \liminf_{p \to +\infty} N_p(f) \geq N_\infty(f).

Now, let aa be a number such that 0<a<N∞(f)0 < a < N_\infty(f). Since, by hypothesis, there exist finite values of pp such that Np(f)<+∞N_p(f) < +\infty, the set AA of x∈Xx \in X such that ∣f(x)∣≥a|f(x)| \geq a, which is measurable and non-negligible, is integrable by virtue of the inequality φA≤(∣f∣/a)p\varphi_A \leq (|f|/a)^p; moreover, we infer from this inequality that Np(f)≥a⋅(∣μ∣(A))1/pN_p(f) \geq a \cdot (|\mu|(A))^{1/p}; letting pp tend to +∞+\infty, it follows that lim inf⁡p→+∞Np(f)≥a\liminf_{p \to +\infty} N_p(f) \geq a, which completes the proof.

Corollary

— If r,s,pr, s, p *are three numbers such that

1≤r<p<s≤+∞, 1 \leq r < p < s \leq +\infty,

then the intersection LFr∩LFs\mathscr{L}_F^r \cap \mathscr{L}_F^s is contained in LFp\mathscr{L}_F^p.

Note that in general the topologies induced on the intersection LFr∩LFs\mathscr{L}_F^r \cap \mathscr{L}_F^s by the topologies of the LFp\mathscr{L}_F^p (r<p<sr < p < s) are distinct. If no further hypothesis is made on μ\mu, the topologies induced on LFr∩LFs\mathscr{L}_F^r \cap \mathscr{L}_F^s by those of LFr\mathscr{L}_F^r and LFs\mathscr{L}_F^s are in general not comparable (in other words, the ratio Nr(f)/Ns(f)N_r(f)/N_s(f) can take arbitrarily large values and arbitrarily small values in LFr∩LFs\mathscr{L}_F^r \cap \mathscr{L}_F^s; cf. Exer. 8).

Prop. 4 may be sharpened when μ\mu is a bounded measure:

Proposition 5

— Let μ\mu be a bounded measure, and let ff be a μ\mu-measurable function with values in a Banach space FF. The set I of numbers pp such that 1≤p≤+∞1 \leq p \leq +\infty and Np(f)N_p(f) is finite, is either empty or is an interval with left end-point p=1p = 1 and containing this point; moreover, (∣μ∣(X))−1/pNp(f)(|\mu|(X))^{-1/p} N_p(f) is an increasing function of pp on I.

This is an immediate consequence of Prop. 4 above and of the Cor. of Prop. 4 of Ch. I, No. 3.

Corollary

— If the measure μ\mu is bounded, the relation r<sr < s implies LFs⊂LFr\mathscr{L}_F^s \subset \mathscr{L}_F^r; moreover, the topology of convergence in mean of order ss is finer than the topology of convergence in mean of order rr (on LFs\mathscr{L}_F^s).

One can show that in general the topology of convergence in mean of order ss is strictly finer than the topology of convergence in mean of order rr (Exer. 8).

Proposition 6

— Let XX be a discrete space, μ\mu the measure on XX defined by placing a mass +1+1 at each point of XX. If ff is a mapping of XX into the Banach space FF, the set I of numbers pp such that 1≤p≤+∞1 \leq p \leq +\infty and Np(f)N_p(f) is finite, is either empty or is an interval with right end-point +∞+\infty and containing this point; moreover, Np(f)N_p(f) is a decreasing function of pp on I.

For, μ∗(∣f∣)=∑x∈X∣f(x)∣\mu^*(|f|) = \sum_{x \in X} |f(x)| for every function ff (§ 1, No. 1, Example), and N∞(f)=∥f∥=sup⁡x∈X∣f(x)∣N_\infty(f) = \|f\| = \sup_{x \in X} |f(x)|; if there exists a number α>0\alpha > 0 such that ∣f(x)∣≥α|f(x)| \geq \alpha for infinitely many values of x∈Xx \in X, then Np(f)=+∞N_p(f) = +\infty for every finite pp; in the contrary case, there exists an x0∈Xx_0 \in X such that ∣f(x0)∣=∥f∥|f(x_0)| = \|f\|, whence

N∞(f)=∣f(x0)∣≤Np(f) N_\infty(f) = |f(x_0)| \leq N_p(f)

for every finite pp. Since the function log⁡Np(f)\log N_p(f) is convex with respect to 1/p1/p and takes its smallest value at the point +∞+\infty, it is necessarily a decreasing function of pp on I (FRV, I, § 4, No. 3, Prop. 5), which completes the proof.

Corollary

— If XX is discrete and the measure μ\mu is defined by a mass +1+1 at each point of XX, then the relation r<sr < s implies LFr⊂LFs\mathscr{L}_F^r \subset \mathscr{L}_F^s; moreover, the topology of convergence in mean of order rr is finer than the topology of convergence in mean of order ss (on LFr\mathscr{L}_F^r).

Exercises

See the exercises for § 6.

Transcribed from the printed volume. Not translated.