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MEASURE · 1

Sigma-algebras and measures

8 concepts · 15 questions

Why Riemann integration is not enough, σ-algebras and Borel sets, measures and their basic properties, and null sets.

Overview 1The plan of this section

The Riemann integral handles continuous functions on intervals but behaves badly under limits: a pointwise limit of Riemann integrable functions (e.g. indicators of finite subsets of Q∩[0,1]\mathbb{Q}\cap[0, 1], increasing to 1Q\mathbf{1}_{\mathbb{Q}}) need not be Riemann integrable. Lebesgue's theory measures sets first, then integrates.

  1. σ-algebras (Def. 1.1) and Borel sets (Def. 1.2).
  2. Measures (Def. 1.3) with examples (Example 1.4) and basic properties including continuity (Prop. 1.5).
  3. Null sets and almost everywhere (Def. 1.6).

Measure sets first, then integrate: σ-algebras, measures, continuity of measure, null sets.

Definition 1.1σ-algebras

A σ-algebra on a set XX is a collection F\mathcal{F} of subsets containing XX, closed under complements and under countable unions (hence countable intersections). (X,F)(X, \mathcal{F}) is a measurable space and members of F\mathcal{F} are measurable sets.

σ-algebra: contains XX, closed under complements and countable unions.

Definition 1.2Generated σ-algebras and Borel sets

For any collection C\mathcal{C} of subsets, σ(C)\sigma(\mathcal{C}), the intersection of all σ-algebras containing C\mathcal{C}, is the smallest σ-algebra containing it. The Borel σ-algebra B(R)\mathcal{B}(\mathbb{R}) is generated by the open sets; it is also generated by the intervals (a,b](a, b], or by the rays (−∞,a](-\infty, a].

Borel sets: the σ-algebra generated by open sets (equivalently, by intervals).

Definition 1.3Measures

A measure on (X,F)(X, \mathcal{F}) is μ:F→[0,∞]\mu: \mathcal{F}\to[0, \infty] with μ(∅)=0\mu(\emptyset) = 0 and countable additivity: μ(⨆An)=∑μ(An)\mu\big(\bigsqcup A_n\big) = \sum\mu(A_n) for pairwise disjoint AnA_n. (X,F,μ)(X, \mathcal{F}, \mu) is a measure space; a probability space if μ(X)=1\mu(X) = 1.

Measure: μ(∅)=0\mu(\emptyset) = 0, countably additive on disjoint sets; values in [0,∞][0, \infty].

Example 1.4Examples of measures

  • Counting measure on P(X)\mathcal{P}(X): μ(A)=∣A∣\mu(A) = |A| (possibly ∞\infty).
  • Dirac measure δx(A)=1\delta_x(A) = 1 if x∈Ax\in A, else 00.
  • Discrete probability: μ(A)=∑x∈Apx\mu(A) = \sum_{x\in A}p_x with px≥0p_x\ge0, ∑px=1\sum p_x = 1.
  • Lebesgue measure on B(R)\mathcal{B}(\mathbb{R}) with λ((a,b])=b−a\lambda((a, b]) = b - a (constructed later: see Section 2).

Counting, Dirac, discrete probability, Lebesgue.

Proposition 1.5Basic properties of measures

For measurable sets: (a) monotonicity A⊆B⇒μ(A)≤μ(B)A\subseteq B\Rightarrow\mu(A)\le\mu(B); (b) countable subadditivity μ(⋃An)≤∑μ(An)\mu(\bigcup A_n)\le\sum\mu(A_n); (c) continuity from below: An↑AA_n\uparrow A ⇒ μ(An)→μ(A)\mu(A_n)\to\mu(A); (d) continuity from above: An↓AA_n\downarrow A and μ(A1)<∞\mu(A_1) < \infty ⇒ μ(An)→μ(A)\mu(A_n)\to\mu(A).

Monotone, countably subadditive, continuous from below; from above if finite.

Proof

Definition 1.6Null sets and almost everywhere

NN is a null set if N⊆AN\subseteq A for some measurable AA with μ(A)=0\mu(A) = 0. A property holds almost everywhere (a.e.) if it fails only on a null set. Countable unions of null sets are null. A measure space is complete if every subset of a measure-zero set is measurable.

Null: inside a measure-zero set. a.e.: except on a null set. Countable unions of null sets are null.

Check 1.7Check: verifying a measure

  • Check the domain is a σ-algebra (countable unions, complements).
  • Check μ(∅)=0\mu(\emptyset) = 0 and countable additivity on disjoint sets.
  • For limits of sets use continuity, remembering the finiteness condition from above.

σ-algebra; μ(∅)=0\mu(\emptyset) = 0; countable additivity; continuity (finite from above).