MEASURE AND INTEGRATION D-MATH, ETH Z¨urich
Francesca Da Lio1
August 30, 2021
1Department of Mathematics, ETH Z¨urich, R¨amistrasse 101, 8092 Z¨urich, Switzerland. Abstract
The aim of this course is to provide notions of abstract measure and integration which are more general and robust than the classical notion of Jordan measure and Riemann integral. For a presentation of Jordan measure and Riemann integral we suggest to look at the lecture notes of Analysis I & II by Michael Struwe (https://people.math.ethz.ch/ struwe/Skripten). ∼ The concept of measure of a general set in Rn originated from the classical notion of volume of a cube in Rn as product of the length of its sides. Starting from this, by a covering process one can assign to any subset a nonnegative number which “quantifies its volume”. Such an association leads to the introduction of a set function called “Lebesgue measure” which is defined over all subsets of Rn. Although the Lebesgue measure was initially developed in Euclidean spaces, the theory is independent of the geometry of the background space and applies to abstract spaces as well. Measure theory is now applied to most areas of mathematics such as functional analysis, geometry, probability, dynamical systems and other domains of mathematics. All results presented here are classical and their presentation follows the one in Struwe’s lecture notes. The proofs are mostly inspired by those in the books by Evans & Gariepy, and by Cannarsa & D’Aprile. Some References
Robert G. Bartle. The elements of Integration and Lebesgue • Measure, Wiley Classics Library, 1995. Piermarco Cannarsa and Teresa D’Aprile. Introduction to • measure theory and functional analysis, Vol. 89, Springer, 2015. Lawrence Craig Evans and Ronald F. Gariepy. Measure theory • and fine properties of functions, revised edition, CRC Press, 2015. Gerald B. Folland. Modern Techniques and Their Applications, • second edition, John Wiley & Sons, INC, 1999. Lecture Notes by Prof. Michael Struwe, FS 13, • https://people.math.ethz.ch/ struwe/Skripten/AnalysisIII- ∼ FS2013-12-9-13.pdf
2 Contents
1 Measure Spaces 1 1.1 Algebras and σ-Algebras of Sets ...... 1 1.1.1 Notation and Preliminaries ...... 1 1.1.2 Algebras and σ-Algebras ...... 3 1.2 Measures ...... 6 1.2.1 Additive and σ-Additive Functions ...... 6 1.2.2 Measures and Measure Spaces ...... 8 1.2.3 Construction of Measures ...... 16 1.3 Lebesgue Measure ...... 21 1.4 Comparison between Lebesgue and Jordan Measure .. 27 1.5 An example of a non-measurable set ...... 29 1.6 An uncountable n-null set: the Cantor Triadic Set .. 32 L 1.7 Lebesgue-Stieltjes Measure ...... 34 1.8 Hausdorff Measures ...... 41 1.8.1 Examples of non-integer Hausdorff-dimension sets 48 1.9 Radon Measure ...... 52
2 Measurable Functions 55 2.1 Inverse Image of a Function ...... 55 2.2 Definition and Basic Properties ...... 55 2.3 Lusin’s and Egoroff’s Theorems ...... 61 2.4 Convergence in Measure ...... 66
3 Integration 69 3.1 Definitions and Basic Properties ...... 69 3.2 Comparison between Lebesgue and Riemann-Integral . 82 3.2.1 Review of Riemann Integral ...... 83 3.3 Convergence Results ...... 86
3 3.4 Application: Differentiation under integral sign .... 91 3.5 Absolute Continuity of Integrals ...... 92 3.6 Vitali’s Theorem ...... 94 3.7 The Lp(Ω, µ) spaces, 1 p ...... 100 ≤ ≤∞ 4 Product Measures and Multiple Integrals 118 4.1 Fubini’s Theorem ...... 118 4.2 Applications ...... 129 4.3 Convolution ...... 131 4.4 Application:Solution of the Laplace Equation ...... 139
5 Differentiation of Measures 142 5.1 Differentiability of Lebesgue Integrals ...... 142 5.2 Differentiation of Radon measures ...... 147 5.3 Differentiation of absolutely continuousfunctions . . . . 151
4 Chapter 1
Measure Spaces
In this chapter we develop measure theory from an abstract point of view in order to construct a large variety of measures on a generic space X. In the particular case of X = Rn, a special role is played by Radon measures which have important regularity properties.
1.1 Algebras and σ-Algebras of Sets
1.1.1 Notation and Preliminaries We denote by X a nonempty set, by (X)or2X the set of all subsets P of X and the empty set. For any subset A of X we denote by Ac its ∅ complement, i.e. Ac = x X x / A . (1.1.1) { ∈ | ∈ } For any A,B (X) we set ∈ P A B = A Bc. (1.1.2) \ ∩ Let (A ) be a sequence in (X). The De Morgan’s identity holds n n P ∞ c ∞ c An = An . (1.1.3) n=1 n=1 [ \
1 We define1
∞ ∞ lim sup An = Am n →∞ n=1 m=n \ [ (1.1.4) ∞ ∞ lim inf An = Am . n →∞ n=1 m=n [ \
If L = limsupn An = liminfn An, then we set L = limn An →∞ →∞ →∞ and we say that (An)n converges to L. Remark 1.1.1. Note that:
1. liminf An lim sup An. n ⊆ n →∞ →∞ 2. If (A ) is increasing (A A ,n N), then n n n ⊆ n+1 ∈ ∞ lim An = An . (1.1.5) n →∞ n=1 [ Proof. Since An is increasing we have
∞ ∞ A A , n N . m ⊆ m ∀ ∈ m=1 m=n [ [ Therefore
∞ ∞ ∞ lim sup An = Am = Am. n n=1 m=n m=1 →∞ \ [ [ ∞ On the other hand for every n N we have Am = An and ∈ m=n therefore T ∞ lim inf An = Am. n →∞ m=1 [ 1We can “think” about the limit supremum and infimum for sets in the following way:
lim sup An = x An, for infinitely many n n→∞ { ∈ }
lim inf An = x An, for all but finitely many n n→∞ { ∈ }
2 3. If (A ) is decreasing (A A ,n N), then n n n ⊇ n+1 ∈ ∞ lim An = An . (1.1.6) n →∞ n=1 \
1.1.2 Algebras and σ-Algebras
Definition 1.1.2. Let (X), is called an algebra in X A ⊆ P A if a) X . ∈ A b) A,B = A B . ∈ A ⇒ ∪ ∈ A c) A = Ac . ∈ A ⇒ ∈ A
Remark 1.1.3. If is an algebra and A, B , then A B and A ∈ A ∩ A B belong to . Therefore, the symmetric difference A ∆ B = \ A (A B) (B A) belongs to as well. is also stable under finite \ ∪ \ A A unions and intersections
A1 An A1,...,An = ∪···∪ ∈ A ∈ A ⇒ ( A1 An . ∩···∩ ∈ A
Definition 1.1.4. An algebra (X) is called a σ-algebra if E ⊆ P for any sequence (A ) of elements in , we have ∞ A . n n E n=1 n ∈ E S
Remark 1.1.5. If isa σ-algebra in X and (A ) , then ∞ A E n n ⊆ E n=1 n ∈ by De Morgan’s identity (1.1.3). Moreover one can show (easy E T exercise!) that:
lim inf An , lim sup An . (1.1.7) n ∈ E n ∈ E →∞ →∞
3 Exercise 1.1.6.
1. (X) and = , X are σ-algebras. (X) is the largest P A {∅ } P σ-algebra in X and the smallest. A
2. In X = [0, 1), the class consisting of and of all finite A0 ∅ unions of half-closed intervals of the form
n A = [a ,b ), 0 a
Ac = [0, a ) [b , a ) [b , 1) , 1 ∪ 1 2 ∪···∪ n ∈ A0 moreover, is stable under finite unions. It suffices to A0 observe that the union of two (not necessarily disjoint) intervals of the form [a, b) and [c, d) belongs to . A0
3. In an infinite set X, consider the class . A = A (X) A is finite, or Ac is finite , (1.1.8) A { ∈ P | } is an algebra. The only point that needs to be checked A is that is stable under a finite union. Let A,B . If A ∈ A A,B are both finite, then so is A B. In all other cases, ∪ (A B)c is finite. but not a σ-algebra. ∪ A
4. In an uncountable set X, consider the class
= A (X) A is countable or Ac is countable . E { ∈ P | } (1.1.9) Then is a σ-algebra which is strictly smaller than (X) E P (here “countable” stands for “at most countable”).
4 Definition 1.1.7. Let (X). The intersection of all σ- K ⊆ P algebras including K is called the σ-algebra generated by K and will be denoted by σ( ). K
Exercise 1.1.8. Let (X). Verify that the intersection of σ- K ⊆ P algebras containing is actually a σ-algebra and it is the smallest K σ-algebra including . K
Example 1.1.9. 1. Let (X,d) be a metric space. The σ-algebra generated by all open sets of X is called the Borel σ-algebra of X and is denoted by (X). The elements of (X) are called Borel sets. B B 2. Let X = R and be the set of all half-closed intervals [a, b) I with a b. We show that σ( )= (R). ≤ I B “σ( ) (R)” : this follows from the fact that I ⊆B ∞ 1 [a, b)= a , b . − n n=1 \ “ (R) σ( )”: Let V be an open set in R, then it is a countable B ⊆ I union of some family of open intervals. Indeed, let (qk) be the sequence including all rational numbers of V and denote by Ik the largest open interval contained in V and containing q . We clearly have ∞ I k ∪k=0 k ⊂ V , but also the opposite inclusion holds: it suffices to consider, for any x V , r > 0 such that (x r, x + r) V, and k such that ∈ − ⊂ q (x r, x + r) to obtain that (x r, x + r) I , by the maximality k ∈ − − ⊂ k of I and then x I . k ∈ k Any open interval (a, b) can be represented as
∞ 1 1 (a, b)= a + ,b
5 1.2 Measures
1.2.1 Additive and σ-Additive Functions
Definition 1.2.1. Let (X) be an algebra and µ: A ⊆ P A → [0, + ] with µ( )=0. ∞ ∅ i) We say that µ is additive if for any finite family A ,...,A of mutually disjoint sets, we have 1 n ∈ A n n µ Ak = µ(Ak). (1.2.1) k=1 k=1 [ P ii) We say that µ is σ-additive if, for any sequence (A ) n n ⊆ A of mutually disjoint sets such that ∞ A , we have k=1 k ∈ A S ∞ ∞ µ Ak = µ(Ak). (1.2.2) k=1 k=1 [ P
6 Remark 1.2.2.
1. If µ is σ-additive function on then it is also additive. A 2. If µ is additive on , it is monotone with respect to the A inclusion: indeed, if A,B and B A, then µ(A) = ∈ A ⊆ µ(B)+ µ(A B). Therefore, µ(A) µ(B). \ ≥ 3. Let µ be additive on and let (A ) be mutually A n n ⊆ A disjoint sets such that ∞ A . Then k=1 k ∈ A n ∞ S n µ A µ A = µ(A ) n N, (1.2.3) k ≥ k k ∀ ∈ k=1 k=1 k=1 [ [ P therefore ∞ µ A ∞ µ(A ). (1.2.4) k ≥ k k=1 k=1 [ P 4. Any σ-additive function µ on is σ-subadditive, that is, A for any sequence (A ) in such that ∞ A n n A k=1 k ∈ A ∞ S µ A ∞ µ(A ). k ≤ k k=1 k=1 [ P
Indeed, let (An)n be such that n∞=1 An and define ⊆ A n 1 ∈ A B = A and B = A − A . Then B are mutually 1 1 n n \ k=1 k ∈ AS n disjoint, µ(B ) µ(A ) for all n N and n ≤ n S ∈ ∞ ∞ Bi = Ai. i=1 i=1 [ [ Therefore
∞ ∞ µ A = µ B = ∞ µ(B ) ∞ µ(A ). (1.2.5) i i i ≤ i i=1 i=1 i=1 i=1 [ [ P P
5. In view of points 3 and 4 an additive function is σ-additive if and only if it is σ-subadditive.
7 Definition 1.2.3. A σ-additive function µ on an algebra A ⊆ (X) is said to be P finite, if µ(X) < + ; • ∞ σ-finite, if there exists a sequence (A ) such that • n n ⊆ A ∞ A = X and µ(A ) < + n N. n n ∞ ∀ ∈ n=1 [
Exercise 1.2.4. In X = N consider the algebra
= A (X) A is finite or Ac is finite . (1.2.6) A ∈ P | The function µ: [0, + ] defined as • A→ ∞ # A if A is finite µ(A)= (1.2.7) ( if Ac is finite ∞ is σ-additive (# A = number of elements of A). The function ν: A [0, + ] defined as ν( )=0 and • → ∞ ∅ 1 n if A is finite ν(A)= n A 2 (1.2.8) ∈ P if Ac is finite ∞ is additive but not σ-additive.
1.2.2 Measures and Measure Spaces Let X be a set.
8 Definition 1.2.5. A mapping µ: (X) [0, + ] is called a P → ∞ measure on X if i) µ( )=0 and ∅ ∞ ∞ ii) µ(A) µ(Ak) whenever A Ak. ≤ k=1 ⊆ k=1 P S
Warning: Most texts call such a mapping µ an outer measure reserving the name measure for µ restricted to the collection of µ-measurable subsets of X (see below).
Remark 1.2.6. The condition ii) in Definition 1.2.5 implies the sub- additivity and the monotonicity.
Definition 1.2.7. Let µ be a measure on X and A X, then µ ⊆ restricted to A written µ A is the measure defined by
(µ A)(B)= µ(A B) B X. (1.2.9) ∩ ∀ ⊆
Definition 1.2.8. [Carath´eodory criterion of measurability] A X is called µ-measurable if for all ⊆ B X ⊆ µ(B)= µ(B A)+ µ(B A). (1.2.10) ∩ \
Remark 1.2.9. 1) If µ(A) = 0, then A is µ-measurable. Indeed, let B X. By the subadditivity, we have ⊆ µ(B) µ(B A)+ µ(B A). (1.2.11) ≤ ∩ \ 9 On the other hand, we have
µ(B A)+ µ(B A) µ(A)+ µ(B)= µ(B), (1.2.12) ∩ \ ≤ which yields the claim. 2) By the subadditivity the condition (1.2.10) is equivalent to
µ(B) µ(B A)+ µ (B A). ≥ ∩ \
Theorem 1.2.10. Let µ: (X) [0, + ] be a measure. P → ∞ Then the set
Σ= A X: A is µ-measurable { ⊆ } is a σ-algebra.
Proof. We proceed by steps.
i) X Σ: B X, it holds ∈ ∀ ⊆ µ(B X)+ µ(B X)= µ(B)+ µ( )= µ(B). (1.2.13) ∩ \ ∅
ii) A Σ= Ac Σ: B X it holds ∈ ⇒ ∈ ∀ ∈ B Ac = B A, B Ac = B A. (1.2.14) ∩ \ \ ∩ Therefore
µ(B Ac)+ µ(B Ac)= µ(B A)+ µ(B A)= µ(B). (1.2.15) ∩ \ \ ∩
iii) Let A ,...,A Σ. By induction on m we show that m A 1 m ∈ k=1 k ∈ Σ. S m = 1 is trivial. m 1 − (induction step) m 1= m: Let A = Ak. − ⇒ k=1 S
10 By inductive hypothesis, we assume A is µ-measurable. Thus, for B X, we have ∀ ⊆ µ(B)= µ(B A)+ µ(B A). (1.2.16) ∩ \
Since Am is also µ-measurable, we have
µ(B A)= µ (B A) Am + µ (B A) Am \ \ ∩ \ \ (1.2.17) = µ (B A) A + µ B (A A ) . \ ∩ m \ ∪ m Now we observe that
B (A A )=(B A) [(B A) A ]. ∩ ∪ m ∩ ∪ \ ∩ m Thus by (1.2.17)
µ(B)= µ(B A)+ µ(B A) ∩ \ = µ(B A)+ µ (B A) A + µ (B A) A ∩ \ ∩ m \ \ m µ B (A A ) + µ B (A A ) ≥ ∩ ∪ m \ ∪ m (1.2.18) m From Remark 1.2.9 it follows that A Am = Ak Σ. ∪ k=1 ∈ S iv) Let (Ak)k N Σ. We show that A = k∞=1 Ak is µ-measurable. ∈ ⊂ We may suppose that A A = , k = ℓ, otherwise we consider k ∩ ℓ ∅ 6 S A = A , A = A A , A = A (A A ) 1 1 2 2 \ 1 3 3 \ 1 ∪ 2 n 1 − (1.2.19) Ae = A e A . e n n \ k k[=1 We cane note that ∞ ∞ Ak = Ak. k[=1 k[=1 e Since each Am is µ-measurable, we have
11 m m m µ B A = µ B A A + µ B A A ∩ k ∩ k ∩ m ∩ k \ m k=1 k=1 k=1 [ m 1 [ [ − = µ(B A )+ µ B A ∩ m ∩ k k=1 [m 1 m 1 − − = µ(B Am)+ µ B Ak Am 1 + µ B Ak Am 1 ∩ ∩ ∩ − ∩ \ − k=1 k=1 [ m 2 [ − = µ(B Am)+ µ(B Am 1)+ µ B Ak ∩ ∩ − ∩ k=1 ... [ (1.2.20) m = µ(B Ak). k=1 ∩ P By using the monotonicity of µ, we get
m m µ(B)= µ B A + µ B A ∩ k \ k k=1 k=1 (1.2.21) m [ [ µ(B Ak)+ µ(B A) ≥ k=1 ∩ \ P We let m + : → ∞ ∞ µ(B) µ(B Ak)+ µ(B A) ≥ k=1 ∩ \ µP(B A)+ µ(B A) ≥ ∩ \ by the σ-subadditivity. Therefore A Σ, by the Remark 1.2.9 ∈
Definition 1.2.11. If µ: (X) [0, + ] is a measure on X, P → ∞ Σ is the σ-algebra of µ-measurable sets, then (X, Σ, µ) is called a Measure Space.
12 Exercise 1.2.12. 1. Let x X. Define, for every A (X) ∈ ∈ P 1 x A δx(A)= ∈ (1.2.22) 0 x / A. ∈ Then δ is a measure on (X), called the Dirac measure x P at x. 2. For every A (X) we define ∈ P #A if A is finite µ(A)= (1.2.23) + otherwise ; ∞ µ is a measure on (X) and it is called the counting P measure. Every A is µ-measurable. 3. µ: (X) [0, + ], µ( ) = 0, µ(A) = 1, A = . In this P → ∞ ∅ 6 ∅ case, A X is µ-measurable A = or A = X. ⊆ ⇐⇒ ∅
13 Theorem 1.2.13. Let (X, Σ, µ) be a Measure Space and let A Σ, k N. Then the following conditions hold: k ∈ ∈ ∞ i) σ-additivity: Aj Aℓ = (j = ℓ) = µ Ak = ∩ ∅ 6 ⇒ k=1 ∞ S µ(Ak). k=1 P ii) Continuity from below: A A A 1 ⊆ 2 ⊆ ··· ⊆ k ⊂ ∞ Ak+1 ... = µ Ak = lim µ(Ak). ⊆ ⇒ k + k=1 → ∞ S iii) Continuity from above: A A A 1 ⊇ 2 ⊇ ··· ⊇ k ⊇ A ..., µ(A ) < + . Then k+1 ⊇ 1 ∞ ∞ µ Ak = lim µ(Ak). k + → ∞ k\=1
Proof. i) In the proof of Theorem 1.2.10 we showed that B X: ∀ ⊆ m m µ B A = µ(B A ) m. (1.2.24) ∩ k ∩ k ∀ k=1 k=1 [ P By taking B = X, we get in particular
m m µ Ak = µ(Ak). (1.2.25) k=1 k=1 [ P By using the monotonicity and the σ-subadditivity, we get m ∞ µ Ak lim µ Ak ≥ m + k=1 → ∞ k=1 [ m [ = lim µ(Ak) (1.2.26) m + → ∞ k=1 ∞ P ∞ = µ(Ak) µ Ak k=1 ≥ k=1 P S 14 ii) Consider the pairwise disjoint family of sets Ak = Ak Ak 1, \ − A1 = A1: e e A3
e
A2
e A1
Fig. 1.1 e
By using i), we get m ∞ µ( k∞=1Ak)= µ( k∞=1Ak)= µ(Ak)= lim µ(Ak) m + ∪ ∪ k=1 → ∞ k=1 m P P = lim e µ(Ak) µe(Ak 1)+ µ(A1) e m + − → ∞ k=2 − = lim µP(Am). m + → ∞ (1.2.27) iii) One considers A = A A ,k N. We have k 1 \ k ∈ = A A .... (1.2.28) e ∅ 1 ⊆ 2 ⊆ We observe that k N ∀ ∈ e e µ(A1)= µ(Ak)+ µ(Ak). Thus e µ(A1) lim µ(Ak)= lim µ(Ak) − k + k + → ∞ → ∞ ∞ e ∞ = µ Ak = µ A1 Ak ii) \ (1.2.29) k[=1 k\=1 e ∞ = µ(A ) µ A . 1 − k k\=1 15 We can conclude.
Remark 1.2.14. If µ(A )=+ , then iii) in Theorem 1.2.13 1 ∞ may be false. Consider #A if A is finite µ(A)= + otherwise . ∞ Take A := m N : m n . We have µ(A )=+ and n { ∈ ≥ } 1 ∞ ∞ µ Ak =0 = lim µ(Ak). 6 k + → ∞ k\=1
1.2.3 Construction of Measures Let X = . 6 ∅ Definition 1.2.15. Let (X). is called a covering of K ⊆ P K X if i) . ∅∈K ∞ ii) (Kj)j N : X = Kj. ∃ ∈ ⊆K j=1 S
Example 1.2.16. The open intervals I = n (a ,b ), a b R k=1 k k k ≤ k ∈ are a covering of X = Rn. Each algebra (X) is a covering QA ⊆ P for X, since , X . ∅ ∈ A
16 Theorem 1.2.17. Let be a covering for X, λ: K K → [0, + ] with λ( )=0. Then ∞ ∅ ∞ ∞ µ(A) = inf λ(Kj): Kj , A Kj (1.2.30) j=1 ∈K ⊆ j=1 n P S o is a measure on X.
Proof of Theorem 1.2.17. We observe that µ 0, µ( ) = 0. We show ≥ ∅ that it is σ-subadditive. Let A ∞ A . The inequality µ(A) ⊆ k=1 k ≤ ∞ µ(A ) is trivial if the right-hand side is infinite. Therefore k=1 k S assume that ∞ µ(A ) is finite. For any k N and any ε > 0 P k=1 k ∈ there exists (K ) such that Pj,k j ⊆K ∞ ε A K and ∞ λ(K ) µ(A )+ . k ⊆ j,k j,k ≤ k 2k j=1 j=1 [ P Since A K . By definition of µ, we have ⊂ j,k j,k
S ∞ µ(A) λ(Kj,k) µ(Ak)+ ε. (1.2.31) ≤ j,k ≤ k=1 P P We let ε 0 and the σ-subadditivity follows. →
Exercise 1.2.18. X = , = , X , λ: [0, + ], λ( )= 0, 6 ∅ K {∅ } K → ∞ ∅ λ(X) = 1. The measure on X induced by λ is exactly the measure µ defined by µ( )=0 and µ(A)=1if A = . ∅ 6 ∅
If = (X) is an algebra and λ: [0, + ] is additive, K A ⊆ P A → ∞ a natural question is: is the measure µ defined in Theorem 1.2.17 a σ-additive extension of λ? We will give a sufficient condition in order for this to hold.
17 Definition 1.2.19. Let (X) be an algebra. A mapping λ: A ⊆ P [0, + ] is called a pre-measure if A→ ∞ i) λ( )=0. ∅ ii) λ(A) = ∞ λ(A ) for every A such that A = k=1 k ∈ A ∞ A , A mutually disjoint. k=1 k Pk ∈ A
λ isS called σ-finite if there exists a covering X = k∞=1 Sk, S and λ(S ) < + , k (we may assume without loss k ∈ A k ∞ ∀ S of generality the Sk’s are mutually disjoint).
Given a pre-measure λ, we obtain as above a measure µ defined by
∞ ∞ µ(A) = inf λ(Ak): A Ak, Ak . (1.2.32) k=1 ⊆ k=1 ∈ A n P S o
Theorem 1.2.20. (Carath´eodory-Hahn extension) Let λ: [0, + ] be a pre-measure on X, µ be defined as in A → ∞ (1.2.32). Then it holds: i) µ: (X) [0, + ] is a measure. P → ∞ ii) µ(A)= λ(A) A . ∀ ∈ A iii) A is µ-measurable. ∀ ∈ A
Proof of Theorem 1.2.20. i) It follows from Theorem 1.2.17. ii) Let A . Clearly it holds µ(A) λ(A). ∈ A ≤ For the opposite inequality, let A ∞ A , A mutually disjoint, ⊆ k=1 k k A . We set A = A A . Clearly, A are mutually k ∈ A k k ∩ ∈S A k disjoint and A = k∞=1 Ak. Since λ is a pre-measure, it follows e e S ∞ ∞ λ(A)=e λ(Ak) λ(Ak). (1.2.33) k=1 ≤ k=1 P P 18 e Thus ∞ ∞ λ(A) inf λ(Ak) A Ak, Ak ≤ k=1 ⊆ k=1 ∈ A (1.2.34) n o = µ(A).P S iii) Let A and B X be arbitrary. For every ε > 0 choose ∈ A ⊆ B , k N with B ∞ B and k ∈ A ∈ ⊆ k=1 k ∞ S λ(Bk) µ(B)+ ε. k=1 ≤ P Since A,B , we have k ∈ A λ(B )= λ(B A)+ λ(B A). (1.2.35) k k ∩ k \ Moreover, we have
∞ B A B A ∩ ⊆ k ∩ k=1 [ (1.2.36) ∞ B A (B A). \ ⊆ k \ k[=1 Thus, by definition of µ, we have
µ(B A)+ µ(B A) ∞ λ(B A)+ ∞ λ(B A) ∩ \ ≤ k ∩ k \ k=1 k=1 (1.2.37) P∞ P = λ(Bk) µ(B)+ ε k=1 ≤ P We let ε 0 and we conclude the proof. →
Theorem 1.2.21. (Uniqueness of Charath´eodory- Hahn extension) Let λ: [0, + ] be as in Theorem 1.2.20 and σ- A → ∞ finite, µ be the measure induced by λ, Σ be the σ-algebra of the µ-measurable sets and let µ: (X) [0, + ] be P → ∞ another measure with µ = λ. Then µ Σ = µ, namely the |A | Charath´eodory-Hahn extension is unique.e e e
19 Proof. i). Let A ∞ A with A , k N. From the σ-sub- ⊆ ∪k=1 k k ∈ A ∈ additivity ofµ ˜ it follows
µ˜(A) Σ∞ µ˜(A )=Σ∞ λ(A ). ≤ k=1 k k=1 k
By taking the infimum over all (Ak)k we obtain µ˜(A) µ(A). (1.2.38) ≤ ii) We show that if A Σ then also the inverse inequality holds. To ∈ this purpose we consider first of all the case there is S such that ∈ A A S and λ(S) < + . ⊆ ∞ By i) we get
µ˜(S A) µ(S A) µ(S)= λ(S) < . (1.2.39) \ ≤ \ ≤ ∞ Since A Σ, S Σ it follows by the sub-additivity ofµ ˜ that ∈ ∈A⊂ µ˜(A)+˜µ(S A) µ(A)+ µ(S A)= µ(S) \ ≤ \ = λ(S)=˜µ(S) µ˜(A)+˜µ(S A).(1.2.40) ≤ \ From (1.2.39) and (1.2.40) it follows that µ(A)=˜µ(A).
Suppose now that X = k∞=1Sk where (Sk)k N are mutually disjoint, ∪ ∈ S , λ(S ) < , for all k N. We consider the disjoint union k ∈ A k ∞ ∈ A = ∞ A , A = A S , k N. For every m it holds ∪k=1 k k ∩ k ∈ µ˜( m A )= µ( m A ). ∪k=1 k ∪k=1 k By taking the limit m + we get → ∞ m m µ˜(A) lim µ˜( k=1Ak)= lim µ( k=1Ak)= µ(A). m m ≥ →∞ ∪ →∞ ∪ We can conclude the proof.
Remark 1.2.22. i) From Theorem 1.2.21 it is not clear if every A Σ is also µ˜-measurable. ∈ ii) In general the statement of Theorem 1.2.21 cannot be improved as the following example shows.
20 Example 1.2.23. Let X = [0, 1], = , X and λ: A {∅ } A → [0, + ], µ as in the exercise 1.2.18 . We have Σ = , X . ∞ {∅ } We will see in the next section that Lebesgue measure 1 is also L an extension of λ but 1([0, 1/2])= 1/2 = µ([0, 1/2])= 1. L 6
1.3 Lebesgue Measure
Lebesgue measure is the extension of “volume” of the so-called elementary sets.
Definition 1.3.1. i) For a =(a ,...,a ), b =(b ,...,b ) Rn we set 1 n 1 n ∈ n (ai,bi) if ai vol (a, b) = vol (a, b] = vol [a, b) = vol [a, b] n (bi ai) + if ai