ΘρϵηΠατπ

Sigma Algebra
Suppose that X is a set. A collection 𝒮𝒫(X) is a σ-algebra on X if
  • 𝒮,
  • if E𝒮, then XE𝒮,
  • if E1,E2,𝒮 is a sequence, then k=1Ek𝒮.
Sigma Algebras are Closed under Standard Set Operations
Suppose that 𝒮 is a σ-algebra on X. Then
  • X𝒮,
  • if D,E𝒮, then DE𝒮, DE𝒮, and DE𝒮,
  • if E1,E2,𝒮, then k=1Ek𝒮.

Since 𝒮 and 𝒮 is closed under complements, X=X𝒮 by the definition of a σ-algebra.

If D,E𝒮, then DE𝒮 by closure under countable unions, using for all remaining terms. Also, DE=X((XD)(XE)), so DE𝒮. Finally, DE=D(XE), so DE𝒮.

If E1,E2,𝒮, then by De Morgan's law, k=1Ek=Xk=1(XEk). The right side belongs to 𝒮, again by the defining closure properties of a σ-algebra.

Measurable Space
A measurable space is an ordered pair (X,𝒮), where X is a set and 𝒮 is a σ-algebra on X.
Measurable Set
Suppose that (X,𝒮) is a measurable space. A set EX is 𝒮-measurable if E𝒮.
Smallest Sigma Algebra Containing a Collection
Suppose that X is a set and 𝒜𝒫(X). The intersection of all σ-algebras on X that contain 𝒜 is a σ-algebra on X.

Let 𝒯 be the intersection of all σ-algebras on X that contain 𝒜. This collection is nonempty because 𝒫(X) itself is a σ-algebra containing 𝒜.

Every σ-algebra in the intersection contains , so 𝒯. If E𝒯, then E belongs to every σ-algebra in the intersection, so XE belongs to every one of them, and hence XE𝒯. If E1,E2,𝒯, then each Ek belongs to every σ-algebra in the intersection, so k=1Ek belongs to every one of them, and hence belongs to 𝒯. Thus 𝒯 is a σ-algebra on X.

Borel σ-Algebra
The Borel σ-algebra on is the smallest σ-algebra on that contains every open subset of .
Borel Set
A Borel set is an element of the Borel σ-algebra.
Singletons are Borel Sets
For every x, the singleton set {x} is a Borel set.
The set {x}=(,x)(x,) is open. Since the Borel σ-algebra contains every open subset of , we have {x}. Since a σ-algebra is closed under set difference from the ambient set, {x}=({x}). Therefore {x} is a Borel set.
Inverse Image
Suppose that f:XY is a function and AY. The inverse image of A under f is f1(A):={xX:f(x)A}.
Algebra of Inverse Images
Suppose that f:XY. Then
  • f1(YA)=Xf1(A) for every AY,
  • f1(A𝒜A)=A𝒜f1(A) for every collection 𝒜𝒫(Y),
  • f1(A𝒜A)=A𝒜f1(A) for every collection 𝒜𝒫(Y).

We prove each identity by element chasing from the definition of inverse image.

For the complement identity, xf1(YA) if and only if f(x)YA, if and only if f(x)A, if and only if xXf1(A).

For unions, xf1(A𝒜A) if and only if f(x)A for some A𝒜, if and only if xf1(A) for some A𝒜, if and only if xA𝒜f1(A). The proof for intersections is the same with "for some" replaced by "for every".

Inverse Image of a Composition
Suppose that f:XY, g:YW, and AW. Then (gf)1(A)=f1(g1(A)).

For xX, we have x(gf)1(A) if and only if g(f(x))A, if and only if f(x)g1(A), if and only if xf1(g1(A)). Therefore the two sets are equal by set equality by elements.

Measurable Function
Suppose that (X,𝒮) is a measurable space. A function f:X is 𝒮-measurable if f1(B)𝒮 for every Borel set B.
Characteristic Function
Suppose that EX. The characteristic function of E is the function χE:X defined by χE(x)={1xE,0xE.
Ray Test for Measurability
Suppose that (X,𝒮) is a measurable space and f:X. If f1((a,))𝒮 for every a, then f is 𝒮-measurable.

Let 𝒯:={B:f1(B)𝒮}. By the algebra of inverse images and the definition of a σ-algebra, the collection 𝒯 is a σ-algebra on . By hypothesis, (a,)𝒯 for every a. The σ-algebra generated by these rays is the Borel σ-algebra, so every Borel set belongs to 𝒯. Hence f is 𝒮-measurable.

Borel Measurable Function
Suppose that X. A function f:X is Borel measurable if f1(B) is a Borel set for every Borel set B.
Continuous Functions are Borel Measurable
Every continuous real-valued function whose domain is a Borel subset of is Borel measurable.

Let X be a Borel set, and let f:X be continuous. By the ray test for measurability, it is enough to prove that f1((a,)) is Borel for each a.

If xf1((a,)), then by continuity, there is δx+ such that f(y)>a whenever yX(xδx,x+δx). Therefore f1((a,))=Xxf1((a,))(xδx,x+δx). The union is open in , hence Borel, and its intersection with the Borel set X is Borel by closure of σ-algebras under intersections. Thus f is Borel measurable.

Increasing Function
Suppose that X and f:X. The function f is increasing if f(x)f(y) whenever x,yX and x<y.
Strictly Increasing Function
Suppose that X and f:X. The function f is strictly increasing if f(x)<f(y) whenever x,yX and x<y.
Increasing Functions are Borel Measurable
Every increasing real-valued function whose domain is a Borel subset of is Borel measurable.

Let X be Borel and let f:X be increasing. By the ray test, it is enough to show that f1((a,)) is Borel for each a.

If this inverse image is empty, it is Borel. Otherwise let b=inff1((a,)). Since f is increasing, the set f1((a,)) is either X(b,) or X[b,). Both are Borel because X is Borel and the Borel σ-algebra is closed under intersections. Therefore f is Borel measurable.

Composition of Measurable Functions
Suppose that (X,𝒮) is a measurable space and f:X is 𝒮-measurable. If g is a Borel measurable real-valued function on a subset of that contains the range of f, then gf is 𝒮-measurable.

Let B be a Borel set. By the inverse image formula for a composition, (gf)1(B)=f1(g1(B)). Since g is Borel measurable, g1(B) is Borel. Since f is 𝒮-measurable, the right side belongs to 𝒮. Thus gf is 𝒮-measurable.

Algebraic Operations with Measurable Functions
Suppose that (X,𝒮) is a measurable space and f,g:X are 𝒮-measurable. Then f+g, fg, and fg are 𝒮-measurable. If g(x)0 for every xX, then f/g is 𝒮-measurable.

For addition, fix a. We have (f+g)1((a,))=r(f1((r,))g1((ar,))). The equality follows because if f(x)+g(x)>a, then some rational r lies between ag(x) and f(x). The right side belongs to 𝒮 because f and g are measurable, is countable, and 𝒮 is a σ-algebra. Thus f+g is measurable by the ray test.

The function g is measurable because it is the composition of g with the continuous function xx, using continuous functions are Borel measurable and composition of measurable functions. Hence fg=f+(g) is measurable.

The square of a measurable function is measurable for the same composition reason, using xx2. Since fg=(f+g)2f2g22, the product fg is measurable. If g(x)0 for all x, then 1/g is the composition of g with the continuous function x1/x on {0}, so 1/g is measurable. Therefore f/g=f(1/g) is measurable.

Pointwise Limit of Measurable Functions is Measurable
Suppose that (X,𝒮) is a measurable space and f1,f2,:X are 𝒮-measurable. If f(x):=limkfk(x) exists for every xX, then f is 𝒮-measurable.

Let a. We claim that f1((a,))=j=1m=1k=mfk1((a+1j,)). If f(x)>a, choose j with f(x)>a+1/j. Since fk(x)f(x), eventually fk(x)>a+1/j, putting x in the right side. Conversely, if x is in the right side, then for some j,m, all km satisfy fk(x)>a+1/j, so taking limits gives f(x)a+1/j>a.

The right side belongs to 𝒮 because each fk is measurable and 𝒮 is closed under countable unions and intersections. By the ray test, f is measurable.

Borel Subsets of the Extended Real Line
A subset C[,] is Borel if C is a Borel subset of .
Extended Real-Valued Measurable Function
Suppose that (X,𝒮) is a measurable space. A function f:X[,] is 𝒮-measurable if f1(B)𝒮 for every Borel set B[,].
Extended Ray Test for Measurability
Suppose that (X,𝒮) is a measurable space and f:X[,]. If f1((a,])𝒮 for every a, then f is 𝒮-measurable.

Let 𝒯:={B[,]:f1(B)𝒮}. The algebra of inverse images shows that 𝒯 is a σ-algebra on [,]. By hypothesis, it contains every ray (a,]. These rays generate the Borel subsets of the extended real line, so every Borel B[,] belongs to 𝒯. Therefore f is 𝒮-measurable.

Infimum and Supremum of Measurable Functions
Suppose that (X,𝒮) is a measurable space and f1,f2,:X[,] are 𝒮-measurable. Define g(x):=inf{fk(x):k+}andh(x):=sup{fk(x):k+}. Then g and h are 𝒮-measurable.

For h, note that for every a, h1((a,])=k=1fk1((a,]). The right side belongs to 𝒮, so h is measurable by the extended ray test.

For g, observe that g(x)=sup{fk(x):k1}. Each fk is measurable as a composition with xx, and the supremum result just proved applies. Therefore g is measurable.