Lebesgue measure (updating)
My personal motivation(s):
- want to know when it is allowed to swap limit and sum.
- want to know when it is allowed to swap limit and integral.
- want to know what the Lebesgue integral is.
- want to make a base for probability theory.
σ-algebra
Suppose a set X and its power set P(X).
The “measure” will be defined for some elements of P(X) later.
Σ⊆P(X) is σ-algebra if
- ϕ,X∈Σ,
- A∈Σ⟹Ac:=X∖A∈Σ, and
- {Ai}i∈N⟹⋃iAi∈Σ. (i could be countable infinite).
The Σ is called (A-)measurable set.
The condition 2 is a difference from the definitioin of a tpological space.
Note that, we could have more than one σ-algebra for a set, depends on how to choose the subset of its power set.
Theorem: conjunction of σ-algebras
Arbitrary numbers of conjunction of sigma algebra ⋂iΣi is also a σ-algebra.
Generated σ-algebra
Let F∈P(X). There exists a unique smallest σ-algebra which contains every set in F. This σ-algebra is called “σ-algebra benerated by the family F”, denoted by σ(F).
Borel (σ-)algebra
Let (X,τ) be a topological space. A Borel σ-algebra of X, B(X), is defined by
B(X):=σ(τ)
Measure space
Let (X,Σ) be an measurable set.
A map μ:Σ→[0,∞] is caleed measure if
- μ(ϕ)=0
- μ(∞⋂k=1Ek)=∞∑k=1μ(Ek), where {Ek}∞k=1 is any countable collection of pairwise disjoint sets (Ei∩Ej=ϕ if i≠j for all i,j)
(X,Σ,μ) is called measure space (cf. measurable space).
The second property is called σ-additivity.
Note that,
- In general, two elements of σ-algebra can have joint elements.
Examples of measure
Counting measure
μ(A)={|A|,if A is finite ∞,if A is infinite
Dirac measure
For p∈X,
δp(Σ)={1,if p∈Σ 0,else
Almost everywhere
“Almost everywhere” is a mathmatical terminology.
If (X,Σ,μ) is a measure space, a property P is said to hold almost everywhere in X if there exists a set N∈Σ with μ(N)=0, and ∀x∈X∖N have the property P.
Vitali set
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Measurable function (measurable map)
Let (X1,Σ1) and (X2,Σ2) be measurable spaces.
A function f:X1→X2 is called measurable map if f−1(A2)∈Σ1 for all A2∈Σ2.
This map “preserve” the structure of measure spaces.
Properties
- When f and g is measurable functions, then g⋅f also.
- f±g also.
Indicator function
The indicator function of a subset A of a set X is a function 1A:X→{0,1}, defined as
1A(x):={1, if x∈A, 0, if x∉A.
If A contains x, it returns true (1), otherwise false (0).
In Physics, it is frequently called “characteristic function” and denote χA.
Simple function and its representation
Simple function
Let (X,Σ) and (R,B(R)) be a measurable spaces. The topology is the standard topology on R.
A measurable function f:X→R is called a simple function if the image of the entire set has the finite number of elements:
f(X)={f1,f2,⋯,fN|fi∈R} for some N∈N
Note that, by definition of measurable functions, f−1({fi})∈Σ where {fi}∈B(R).
When you imagine X as a simple finite set, most pre-images in B(R) are ϕ.
The simple functions are closed under addition and multiplication.
Representation of a simple function
We can write the equivalent simple function as follows:
f=∑fi∈f(X)fi⋅1f−1({fi})
For example:
f(a1)=∑fi∈f(X)fi⋅[1f−1({fi})(a1)]
Integral of a measurable function
When the measurable space is induced a measure μ, which always returns finite values, the integral of a measurable function f with respect to μ is defined as follows:
∫Xfdμ:=sup{∑hi∈h(X)z⋅μ(h−1({hi})) | h is a simple function, and 0≤h≤f}
- f and h take the same set X which has the same σ-algebra.
- The differences between f and h is, f is just a measurable function where h is a simple function.
- By definition, h−1({hi})≠h−1({hj}) when i≠j (pairwise disjoint).
- This integral is defined with supremum.
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Reference
- https://www.youtube.com/watch?v=xZ69KEg7ccU&list=PLBh2i93oe2qvMVqAzsX1Kuv6-4fjazZ8j&index=1
- https://www.youtube.com/watch?v=ot253Lhx2_o
- https://web.ma.utexas.edu/users/gordanz/notes/lebesgue_integration.pdf
Partition of a set
A partition of a set X is a set of subsets {Pi} of X such that:
- {Pi} is pairwise disjoint: ∀Pi,Pj,Pi∩Pj=ϕ when Pi≠P2,
- The union of {Pi} forms the whole set X: ⋃iPi=X
- None of the elements of S is empty: ∀Pi,Pi≠ϕ.
When the number of partition is finite, the partition is called finite expansion.