TheoremBase

If one seminorm vanishes the product is zero almost everywhere. Otherwise Young's inequality applied pointwise to the normalized functions and integrated gives the bound; the case p = q = 2 then gives the Cauchy-Schwarz inequality.

Proof

Throughout, fgfg and ∣fg∣|fg| are measurable (Arithmetic of Measurable Real- and [0,∞]-Valued Maps (i)), ∣fg∣∈M+|fg|\in\mathcal{M}^{+} (Linearity and Monotonicity of the Lebesgue Integral, and the Integrability Criterion (iv)), integrals of nonnegative functions are taken in M+\mathcal{M}^{+}, and products in [0,∞][0,\infty] of real numbers are the products in R\mathbb{R} (Addition and Multiplication on [0,∞] (ii)). By Linearity and Monotonicity of the Lebesgue Integral, and the Integrability Criterion (iv), fg∈L1(μ)fg\in\mathcal{L}^{1}(\mu) as soon as ∫∣fg∣ dμ<∞\int|fg|\,d\mu<\infty.

Hölder's inequality. Write A=∥f∥pA=\|f\|_{p} and B=∥g∥qB=\|g\|_{q}.

Case A=0A=0 or B=0B=0. Say A=0A=0; the case B=0B=0 is the same with ff and gg exchanged. By Elementary Properties of the p-Seminorm (vii), f(x)=0f(x)=0 for almost every xx, and at each such xx also ∣f(x)g(x)∣=0|f(x)g(x)|=0; so ∣fg∣=0|fg|=0 almost everywhere (Null Sets and Properties Holding Almost Everywhere (vi)), and ∫∣fg∣ dμ=0\int|fg|\,d\mu=0 by The Lebesgue Integral and Null Sets (iv). Hence fg∈L1(μ)fg\in\mathcal{L}^{1}(\mu) and ∫∣fg∣ dμ=0≤AB\int|fg|\,d\mu=0\le AB.

Case A,B>0A,B>0. Let x∈Xx\in X. Young's inequality (Conjugate Exponents and Young's Inequality (ii)) with a=∣f(x)∣/Aa=|f(x)|/A and b=∣g(x)∣/Bb=|g(x)|/B, together with ap=∣f(x)∣p/Apa^{p}=|f(x)|^{p}/A^{p} and bq=∣g(x)∣q/Bqb^{q}=|g(x)|^{q}/B^{q} (Properties of Real Powers (v)), gives

1AB ∣f(x)g(x)∣≤1pAp ∣f(x)∣p+1qBq ∣g(x)∣q.\frac{1}{AB}\,|f(x)g(x)|\le\frac{1}{pA^{p}}\,|f(x)|^{p}+\frac{1}{qB^{q}}\,|g(x)|^{q} .

The three coefficients are positive real numbers. Integrating, by Basic Properties of the Integral of Nonnegative Measurable Maps (iv), Linearity and Monotonicity of the Lebesgue Integral, and the Integrability Criterion (i) and Basic Properties of the Integral of Nonnegative Measurable Maps (iii), and using ∫∣f∣p dμ=Ap\int|f|^{p}\,d\mu=A^{p} and ∫∣g∣q dμ=Bq\int|g|^{q}\,d\mu=B^{q} (Elementary Properties of the p-Seminorm (ii)), we get

1AB∫∣fg∣ dμ≤1pAp∫∣f∣p dμ+1qBq∫∣g∣q dμ=1p+1q=1.\frac{1}{AB}\int|fg|\,d\mu\le\frac{1}{pA^{p}}\int|f|^{p}\,d\mu+\frac{1}{qB^{q}}\int|g|^{q}\,d\mu=\frac{1}{p}+\frac{1}{q}=1 .

If ∫∣fg∣ dμ\int|fg|\,d\mu were ∞\infty, the left side would be ∞\infty (Addition and Multiplication on [0,∞] (ii)); so ∫∣fg∣ dμ\int|fg|\,d\mu is a real number (Small Facts about [0,∞]: Zero, Finiteness and Sums of Zeros (ii)), fg∈L1(μ)fg\in\mathcal{L}^{1}(\mu), and multiplying by AB>0AB>0 gives

∫∣fg∣ dμ≤∥f∥p ∥g∥q.\int|fg|\,d\mu\le\|f\|_{p}\,\|g\|_{q} .

The Cauchy-Schwarz inequality. The exponents p=q=2p=q=2 satisfy 1/2+1/2=11/2+1/2=1, so (i) gives fg∈L1(μ)fg\in\mathcal{L}^{1}(\mu) and ∫∣fg∣ dμ≤∥f∥2∥g∥2\int|fg|\,d\mu\le\|f\|_{2}\|g\|_{2}. By Linearity and Monotonicity of the Lebesgue Integral, and the Integrability Criterion (x), ∣fg∣∈L1(μ)|fg|\in\mathcal{L}^{1}(\mu) and ∣∫fg dμ∣≤∫∣fg∣ dμ\bigl|\int fg\,d\mu\bigr|\le\int|fg|\,d\mu, the integral of ∣fg∣|fg| as an element of L1(μ)\mathcal{L}^{1}(\mu); it equals the integral in M+\mathcal{M}^{+} by Linearity and Monotonicity of the Lebesgue Integral, and the Integrability Criterion (vi). Hence

∣∫fg dμ∣≤∥f∥2 ∥g∥2.\Bigl|\int fg\,d\mu\Bigr|\le\|f\|_{2}\,\|g\|_{2} .

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