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Measure, Integration & Real Analysis, 2021a

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358 Chapter 11 Fourier <strong>Analysis</strong><br />

11.38 L p -norm of a convolution<br />

Suppose 1 ≤ p ≤ ∞, f ∈ L 1 (∂D), and g ∈ L p (∂D). Then<br />

‖ f ∗ g‖ p ≤‖f ‖ 1 ‖g‖ p .<br />

Proof<br />

We use the following result to estimate the norm in L p (∂D):<br />

11.39<br />

If F : ∂D → C is measurable and 1 ≤ p ≤ ∞, then<br />

{∫<br />

}<br />

‖F‖ p = sup |Fh| dσ : h ∈ L p′ (∂D) and ‖h‖ p ′ = 1 .<br />

∂D<br />

Hölder’s inequality (7.9) shows that the left side of the equation above is greater<br />

than or equal to the right side. The inequality in the other direction almost follows<br />

from 7.12, but7.12 would require the hypothesis that F ∈ L p (∂D) (and we want the<br />

equation above to hold even if ‖F‖ p = ∞). To get around this problem, apply 7.12<br />

to truncations of F and use the Monotone Convergence Theorem (3.11); the details<br />

of verifying 11.39 are left to the reader.<br />

Suppose h ∈ L p′ (∂D) and ‖h‖ p ′ = 1. Then<br />

∫<br />

∂D<br />

∫<br />

|( f ∗ g)(z)h(z)| dσ(z) ≤<br />

∫<br />

=<br />

∫<br />

≤<br />

∂D<br />

∂D<br />

∂D<br />

(∫<br />

∂D<br />

∫<br />

| f (w)|<br />

)<br />

| f (w)g(zw)| dσ(w)|h(z)| dσ(z)<br />

∂D<br />

|g(zw)h(z)| dσ(z) dσ(w)<br />

| f (w)|‖g‖ p ‖h‖ p ′ dσ(w)<br />

11.40<br />

= ‖ f ‖ 1 ‖g‖ p ,<br />

where the second line above follows from Tonelli’s Theorem (5.28) and the third line<br />

follows from Hölder’s inequality (7.9) and 11.17. Now11.39 (with F = f ∗ g) and<br />

11.40 imply that ‖ f ∗ g‖ p ≤‖f ‖ 1 ‖g‖ p .<br />

Order does not matter in convolutions, as we now prove.<br />

11.41 convolution is commutative<br />

Suppose f , g ∈ L 1 (∂D). Then f ∗ g = g ∗ f .<br />

Proof<br />

Suppose z ∈ ∂D is such that ( f ∗ g)(z) is defined. Then<br />

∫<br />

( f ∗ g)(z) =<br />

∂D<br />

∫<br />

f (w)g(zw) dσ(w) =<br />

∂D<br />

f (zζ)g(ζ) dσ(ζ) =(g ∗ f )(z),<br />

where the second equality follows from making the substitution ζ = zw (which<br />

implies that w = zζ); the invariance of the integral under this substitution is explained<br />

in connection with 11.17.<br />

<strong>Measure</strong>, <strong>Integration</strong> & <strong>Real</strong> <strong>Analysis</strong>, by Sheldon Axler

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