Now we don’t need the functions to be bounded or supported on a set with finite measure. We extend the definition of the integral to non-negative measurable functions (f ≥ 0 f \ge 0 f ≥ 0 ).
One way is to approximate f f f by a sequence of truncated functions.
Define:
h n = ( f ∧ n ) 1 E n h_n = (f \wedge n) \mathbf{1}_{E_n} h n = ( f ∧ n ) 1 E n
where E n ↑ Ω E_n \uparrow \Omega E n ↑ Ω is a sequence of sets with μ ( E n ) < ∞ \mu(E_n) < \infty μ ( E n ) < ∞ for all n n n ; and f ∧ n = min ( f , n ) f \wedge n = \min(f, n) f ∧ n = min ( f , n ) .
We approximate f f f by clipping its height at n n n and restricting its domain to a set E n E_n E n of finite measure. Shown: h 1 = ( f ∧ 1 ) 1 E 1 h_1 = (f \wedge 1) \mathbf{1}_{E_1} h 1 = ( f ∧ 1 ) 1 E 1 and h 2 = ( f ∧ 2 ) 1 E 2 h_2 = (f \wedge 2) \mathbf{1}_{E_2} h 2 = ( f ∧ 2 ) 1 E 2 .
Lemma
lim n → ∞ ∫ h n d μ = ∫ f d μ \lim_{n \to \infty} \int h_n \, d\mu = \int f \, d\mu n → ∞ lim ∫ h n d μ = ∫ f d μ
Existence of Limit :
Since n n n increases and E n E_n E n expands, h n h_n h n is a non-decreasing sequence (h n ≤ h n + 1 h_n \le h_{n+1} h n ≤ h n + 1 ).
Thus ∫ h n d μ \int h_n \, d\mu ∫ h n d μ is non-decreasing, so the limit lim n → ∞ ∫ h n d μ \lim_{n \to \infty} \int h_n \, d\mu lim n → ∞ ∫ h n d μ exists.
Lower Bound :
Let h ∈ H h \in H h ∈ H be any function in the class defined above. Let M M M be its bound (h ≤ M h \le M h ≤ M ).
Since h h h is supported on a set of finite measure, let E = { x : h ( x ) > 0 } E = \{x : h(x) > 0\} E = { x : h ( x ) > 0 } with μ ( E ) < ∞ \mu(E) < \infty μ ( E ) < ∞ .
For any n ≥ M n \ge M n ≥ M :
∫ E n h n d μ = ∫ E n ( f ∧ n ) d μ ≥ ∫ E n h d μ \int_{E_n} h_n \, d\mu = \int_{E_n} (f \wedge n) \, d\mu \ge \int_{E_n} h \, d\mu ∫ E n h n d μ = ∫ E n ( f ∧ n ) d μ ≥ ∫ E n h d μ
(since on E n E_n E n , h n = f ∧ n ≥ h ∧ n = h h_n = f \wedge n \ge h \wedge n = h h n = f ∧ n ≥ h ∧ n = h because h ≤ f h \le f h ≤ f and h ≤ M ≤ n h \le M \le n h ≤ M ≤ n ).
Decomposition :
∫ E n h d μ = ∫ h d μ − ∫ E n c h d μ \int_{E_n} h \, d\mu = \int h \, d\mu - \int_{E_n^c} h \, d\mu ∫ E n h d μ = ∫ h d μ − ∫ E n c h d μ
Consider the term ∫ E n c h d μ \int_{E_n^c} h \, d\mu ∫ E n c h d μ . Since h h h is supported on E E E :
∫ E n c h d μ = ∫ E n c ∩ E h d μ ≤ ∫ E n c ∩ E M d μ = M μ ( E ∩ E n c ) = M μ ( E ∖ E n ) \int_{E_n^c} h \, d\mu = \int_{E_n^c \cap E} h \, d\mu \le \int_{E_n^c \cap E} M \, d\mu = M \mu(E \cap E_n^c) = M \mu(E \setminus E_n) ∫ E n c h d μ = ∫ E n c ∩ E h d μ ≤ ∫ E n c ∩ E M d μ = M μ ( E ∩ E n c ) = M μ ( E ∖ E n )
As E n ↑ Ω E_n \uparrow \Omega E n ↑ Ω , we have E ∖ E n ↓ ∅ E \setminus E_n \downarrow \emptyset E ∖ E n ↓ ∅ , so μ ( E ∖ E n ) → 0 \mu(E \setminus E_n) \to 0 μ ( E ∖ E n ) → 0 (since μ ( E ) < ∞ \mu(E) < \infty μ ( E ) < ∞ ).
Thus, ∫ E n c h d μ → 0 \int_{E_n^c} h \, d\mu \to 0 ∫ E n c h d μ → 0 .
Inequality :
So we have lim n → ∞ ∫ h n d μ ≥ ∫ h d μ \lim_{n \to \infty} \int h_n \, d\mu \ge \int h \, d\mu lim n → ∞ ∫ h n d μ ≥ ∫ h d μ .
Since this holds for any h ∈ H h \in H h ∈ H , taking the supremum over all such h h h :
lim n → ∞ ∫ h n d μ ≥ sup h ∈ H ∫ h d μ = ∫ f d μ \lim_{n \to \infty} \int h_n \, d\mu \ge \sup_{h \in H} \int h \, d\mu = \int f \, d\mu n → ∞ lim ∫ h n d μ ≥ h ∈ H sup ∫ h d μ = ∫ f d μ
Equality :
On the other hand, since each h n ∈ H h_n \in H h n ∈ H (it is bounded by n n n and supported on E n E_n E n ), by definition:
∫ h n d μ ≤ ∫ f d μ ⟹ lim n → ∞ ∫ h n d μ ≤ ∫ f d μ \int h_n \, d\mu \le \int f \, d\mu \implies \lim_{n \to \infty} \int h_n \, d\mu \le \int f \, d\mu ∫ h n d μ ≤ ∫ f d μ ⟹ n → ∞ lim ∫ h n d μ ≤ ∫ f d μ
Combining both inequalities, we get the result.
Exercise 7
Prove that Properties 1-6 also hold for non-negative measurable functions.