Note on set theory - Real Analysis

Notes on Lebesgue measure and integration

Set Theory

Set $X$ is a collection of objects. Class $C$ is a set of sets ("2nd-order set"). Space $(X, \cdots)$ is a set with certain structure.

Countability

countable set; equivalence of sets; power of a set; power of a countable set; power of the continuum

Set Operations

union; intersection; complement, relative complement/set difference, absolute complement; symmetric difference

The Cartesian product or direct product $A \times B$ of two sets $A, B$ is the set of all tuples $(a,b)$ composed of elements of the two sets: $A \times B = \{ (a,b) \mid a \in A, b \in B \}$.

Set Relations

inclusion; equality

Function or mapping (in short, map) $f: X \to Y$ from set $X$ to set $Y$ is a set of ordered pairs $(x,y)$ such that $\forall x \in X$, $\exists! y \in Y$: $(x,y) \in f$; in other definitions, the set $f$ is also called the graph of the function, and $f(x) = y$ is equivalent notation for $(x, y) \in f$. Transformation $u: X \to X$ is a mapping of a set to itself. Operator $A: X \to Y$ is a function/mapping from a space $X$ to another space $Y$, especially when $X$ and $Y$ are both vector spaces; the operation commonly denoted as $Ax = y$. Functional is an operator from a vector space $X$ of functions to a scalar field $\mathbb{F}$, usually $\mathbb{R}$ or $\mathbb{C}$. Correspondence or binary relation $(R, A, B)$ between two sets $A$ and $B$ is any subset of the Cartesian product $A \times B$. Morphism $\alpha \in H_{\mathcal{K}}(A, B)$ of a category $\mathcal{K}$ is a mapping from an object $A$ in the category into another $B$.

Measurable Space

An algebra over a set is a class of subsets of the set that is closed under all finite set operations: for a set $X$, a non-empty subset $\mathcal{F}$ of the power set $2^X$ that is closed under (absolute) complementation and closed under union and/or intersection.

Any set algebra $\mathcal{F}$ is a subalgebra of the power set of the underlying set $X$. (Boolean Algebra)

A sigma-algebra is an algebra closed under countable unions and/or intersections. A sigma-algebra $\Sigma$ of a set $X$ is:

  1. a non-empty subset of the power set $2^X$;
  2. closed under (absolute) complementation;
  3. closed under countable unions and/or intersections.

By De Morgan's laws, closure under countable unions is equivalent to closure under countable intersections.

Smallest sigma-algebra containing a subset of the power set is the intersection of all sigma-algebras containing it. Given a class of subsets $S \subset 2^X$, the smallest sigma-algebra containing $S$ is $\Sigma = \bigcap \{ \mathcal{F} : S \subset \mathcal{F}, \mathcal{F} \text{ is a sigma-algebra of } X \}$. The smallest sigma-algebra containing $S$ is also called the sigma-algebra generated by $S$.

Borel sigma-algebra $\mathcal{B}$ is the smallest sigma-algebra containing a topology $T$.

A field of sets $(X, \mathcal{F})$ is a set $X$ with an algebra $\mathcal{F}$ over the set. The word "field" in "field of sets" is not used with the meaning of "field" from field theory.

A field of sets $(X,\Sigma)$ is a measurable space if the underlying algebra is a sigma-algebra.

Measure Space

A measure (测度, size) is a non-negative function on a sigma-algebra that is countably additive. Given a sigma-algebra $\Sigma$, function $\mu: \Sigma \to \mathbb{R}_{\ge 0}$ is a measure if it satisfies:

  1. Non-negativity: $\mu(E)\geq 0, \forall E \in \Sigma$;
  2. Null empty set: $\mu(\emptyset) =0$;
  3. Countable additivity: $\forall E_i \in \Sigma, E_i \cap E_j = \emptyset, i \ne j, i, j \in \mathbb{N} : \mu\left(\bigcup_{i \in \mathbb{N}} E_i\right ) = \sum_{i \in \mathbb{N}} \mu\left(E_i\right)$

A finite measure is a measure that assigns the entire domain set a finite value. A sigma-finite measure is a measure where the entire domain set is a countable union of measurable sets with finite measure.

A measure space is a measurable space possessing a measure: $(X, \Sigma, \mu)$.

Lebesgue Measure Space

A complete measure space is a measure space $(X, \Sigma, \mu)$ in which every subset of every null set is measurable: $S \subseteq N \in \Sigma, \mu(N) = 0 \Rightarrow S \in \Sigma$. It follows that those sets have measure zero.

The completion of a measure space is the smallest extension $(X, \Sigma_0, \mu_0)$ of the measure space $(X, \Sigma, \mu)$ such that the former is complete:

  1. Construct the class $Z$ of all subsets of measure zero subsets of $(X, \Sigma, \mu)$.
  2. Generate the sigma-algebra $\Sigma_0$ from $\Sigma \cup Z$.
  3. Extend the measure $\mu$ to $\Sigma_0$ such that $\forall C \in \Sigma_0$, $\mu_0 (C) = \inf \{ \mu (D) \mid C \subseteq D \in \Sigma \}$.

Lebesgue measure $\lambda$ (or $n$-volume) is the completion of the Borel measure on $\mathbb{R}^n$ (interval lengths and their products).

Lebesgue measure space $(\mathbb{R}^n, \mathcal{L}, \lambda)$ is the $n$-product of real numbers associated with the Lebesgue measure and all its Lebesgue measurable subsets.

Product Measure Space

The product sigma-algebra $\mathcal{S}\times\mathcal{T}$ is the smallest sigma-algebra of product space $S \times T$ containing all measurable rectangles. A product set $A \times B$ is a measurable rectangle if $A \in \mathcal{S}, B \in \mathcal{T}$.

The product measure $\mu\times\theta$ is a measure on the product measurable space that satisfies

$$(\mu\times\theta)(A\times B) = \mu(A) \theta(B), \forall A \in \mathcal{S}, B \in \mathcal{T}$$

Such product measures always exist, guaranteed by Hahn–Kolmogorov theorem. If the constituent measure spaces are sigma-finite, then product measure is uniquely defined:

$$(\mu\times\theta)(Q) = \int_S \mathrm{d}\theta \int_T \mathbf{1}_Q(s,t) \mathrm{d} \mu = \int_T \mathrm{d} \mu \int_S \mathbf{1}_Q(s,t) \mathrm{d} \theta, \forall Q \in \mathcal{S}\times\mathcal{T}$$

A product measure space of two measure spaces $(S,\mathcal{S},\mu)$ and $(T,\mathcal{T},\theta)$ is denoted as $(S\times T, \mathcal{S}\times\mathcal{T}, \mu\times\theta)$.

Even if both constituent measure spaces are complete, their product measure space still might not be complete. Denote the completion of product measure space as $(S \times T, (\mathcal{S}\times\mathcal{T})^{} , \mu\times\theta)$, where the *extended product measure** can be defined in a similar fashion.

Misc

Haar measure, Hausdorff measure

Integration

Integration on product space

Fubini Theorem establishes a connection between multiple integral and iterated integrals.

Theorem (Fubini): Given $(S,\mathcal{S},\mu)$ and $(T,\mathcal{T},\theta)$ are sigma-finite measure spaces, and $f: S\times T \to \mathbb{R}$ is a measurable function w.r.t. $(\mathcal{S} \times \mathcal{T}, \mathcal{B})$. If $f\geq 0$ or $\int_S \, \mathrm{d} \mu \left(\int_T |f| \,\mathrm{d} \theta \right) < \infty$, then:

$$\int_{S \times T} f \,\mathrm{d}(\mu \times \theta) = \int_S \, \mathrm{d} \mu \left(\int_T f \,\mathrm{d} \theta \right) = \int_T \,\mathrm{d} \theta \left( \int_S f \, \mathrm{d} \mu \right)$$

Reference

Wikibooks: Measure Theory


🏷 Category=Analysis