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Measure, Integration & Real Analysis, 2021a

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Section 3B Limits of Integrals & Integrals of Limits 91<br />

Proof Suppose ε > 0. Let h : X → [0, ∞) be a simple S-measurable function such<br />

that 0 ≤ h ≤ g and ∫ ∫<br />

g dμ − h dμ < ε 2 ;<br />

the existence of a function h with these properties follows from 3.9. Let<br />

H = max{h(x) : x ∈ X}<br />

and let δ > 0 be such that Hδ <<br />

2 ε .<br />

Suppose B ∈Sand μ(B) < δ. Then<br />

∫ ∫<br />

∫<br />

g dμ = (g − h) dμ +<br />

B<br />

≤<br />

B<br />

∫<br />

B<br />

h dμ<br />

(g − h) dμ + Hμ(B)<br />

< ε 2 + Hδ<br />

as desired.<br />

< ε,<br />

Some theorems, such as Egorov’s Theorem (2.85) have as a hypothesis that the<br />

measure of the entire space is finite. The next result sometimes allows us to get<br />

around this hypothesis by restricting attention to a key set of finite measure.<br />

3.29 integrable functions live mostly on sets of finite measure<br />

Suppose (X, S, μ) is a measure space, g : X → [0, ∞] is S-measurable, and<br />

∫ g dμ < ∞. Then for every ε > 0, there exists E ∈Ssuch that μ(E) < ∞ and<br />

∫<br />

X\E<br />

g dμ < ε.<br />

Proof<br />

3.30<br />

Suppose ε > 0. Let P be an S-partition A 1 ,...,A m of X such that<br />

∫<br />

g dμ < ε + L(g, P).<br />

Let E be the union of those A j such that inf g > 0. Then μ(E) < ∞ (because<br />

A j<br />

otherwise ∫ we would have L(g, P) = ∞, which contradicts the hypothesis that<br />

g dμ < ∞). Now<br />

∫ ∫ ∫<br />

g dμ = g dμ − χ E<br />

g dμ<br />

X\E<br />

< ( ε + L(g, P) ) −L(χ E<br />

g, P)<br />

= ε,<br />

where the second line follows from 3.30 and the definition of the integral of a<br />

nonnegative function, and the last line holds because inf g = 0 for each A j not<br />

A<br />

contained in E.<br />

j<br />

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

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