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Basic Notions of Lebesgue Integration

The main idea is to define in a simple and fast way the Lebesgue integral and the Lebesgue spaces, since they will be used in this site, both in the study of the universal approximation theorem and in the study of partial differential equations.

For ease of writing, the following sets will be introduced, R‾=R∪{−∞,+∞}\overline{\mathbb{R}} = \mathbb{R}\cup\{-\infty, +\infty\} and R‾+=R+∪{+∞}\overline{\mathbb{R}}^+ =\mathbb{R}^+\cup\{+\infty\}.

Some Definitions​

A σ-algebra\pmb{\sigma\text{-algebra}} is a collection Σ\Sigma of subsets of Rn\mathbb{R}^n with the properties:

  1. The empty set ∅\empty and Rn\mathbb{R}^n ∈\in Σ\Sigma;
  2. If A∈ΣA \in \Sigma, then its complement Ac∈ΣA^c \in \Sigma ;
  3. Aj∈ΣA_j\in\Sigma, j=1,2,...j=1,2,..., then ⋃j=1∞Aj∈Σ\bigcup_{j=1}^{\infty}A_j\in\Sigma.

A set A∈ΣA\in\Sigma is said to be measurable.


Let Σ\Sigma be a σ-algebra\sigma\text{-algebra}. A function μ:Σ→R‾+\mu:\Sigma\to\overline{\mathbb{R}}^+ is a measure if it has the properties:

  1. μ(∅)=0\mu(\empty)=0;
  2. μ\mu is a countably additive, that is, if Aj∈ΣA_j\in\Sigma, j=1,2,...j=1,2,..., are pairwise disjoint sets then
μ(⋃j=1∞Aj)=∑j=1∞μ(Aj).\mu\left(\bigcup_{j=1}^{\infty}A_j\right)=\sum_{j=1}^{\infty}\mu(A_j).

Let Σ\Sigma be a σ-algebra\sigma\text{-algebra} and a measure μ\mu on Σ\Sigma such that Aj={x∈Rn:ai≤xi≤bi,i=1,2,...,n}A_j=\{x\in\mathbb{R}^n:a_i\leq x_i\leq b_i, i=1,2,..., n\} and

μ(Aj)=∏i=1n(bi−ai).\mu(A_j)=\prod_{i=1}^n(b_i-a_i).

The elements of Σ\Sigma are called Lebesgue measurable subsets of Rn\mathbb{R}^n , and μ\mu is called the Lebesgue measure in Rn\mathbb{R}^n


Let A⊂RnA\sub\mathbb{R}^n. A function f:A→R‾f:A\to\overline{\mathbb{R}} is said measurable if the set

{x∈A:f(x)>α}\{x\in A: f(x)>\alpha\}

is measurable for every α∈R\alpha\in\mathbb{R}.

If ff is measurable then the functions ∣f∣|f| are measurable.

Construction of the integral​

Let A⊂RnA\sub\mathbb{R}^n. In the following sequence of elements we describe the construction of the integral of appropriate functions f:A→R‾.f: A \to \overline{\mathbb{R}}.

For any subset Aj⊂RnA_j\subset\mathbb{R}^n. The characteristic function χAj\chi_{A_j} of AjA_j is defined by,

χAj(x)={1 x∈Aj,0 x∉Aj.\chi_{A_j}(x)= \begin{cases} 1 & \ x \in A_j, \\ 0 & \ x \notin A_j. \end{cases}

A function ϕ:A→R\phi:A\to\mathbb{R} is simple if its range is a finite set of real numbers, this is ϕ(x)∈{α1,...,αm}\phi(x)\in \{ \alpha_1,...,\alpha_m \} , then

ϕ=∑j=1kαjχAj,\phi = \sum^k_{j=1}\alpha_j\chi_{A_j},

where Aj={x∈A:ϕ(x)=αj}A_j=\{x\in A: \phi(x)=\alpha_j \}, and ϕ\phi is measurable if and only if AjA_j are measurable, j=1,...,k.j=1,...,k.


For simple function ϕ\phi, where Aj⊂AA_j\sub A, AjA_j measurable, j=1,...,k.j=1,...,k. We define

∫Aϕ(x)dμ=∑j=1kαjμ(Aj).\int_A\phi(x)d\mu = \sum^k_{j=1}\alpha_j\mu(A_j).

If ff is measurable and non-negative and let the integral of ff be defined by

∫Afdμ=sup⁡{∫Aϕdμ:ϕ is simple and 0≤ϕ≤f}.\int_A f d\mu = \sup \left\{ \int_A\phi d\mu: \phi \ \text{is simple and } 0\leq\phi\leq f \right\}.

If ff is measurable and ∫A∣f∣dμ<∞\int_A |f| d\mu<\infty, then ff can be seen as f+−f−f^+-f⁻, where f+=max⁡(f,0)f^+=\max(f,0) and f−=−min⁡(f,0)f^-=-\min(f,0) are both measurable and non-negative and

∫Afdμ=∫Af+dμ−∫Af−dμ,\int_A f d\mu = \int_A f^+d\mu - \int_A f^- d\mu,

and μ\mu is the Lebesgue measure then it is said that ff is Lebesgue Integrable.

The Lebesgue Space​

Definition L1(Ω)L^1(\Omega)

Let equivalence relation ∼\sim on all Lebesgue Integrable functions of Ω⊂Rn\Omega \sub\mathbb{R}^n such

f∼g,f(x)=g(x) almost everywhere x∈Ω.f \sim g, \quad f(x)=g(x) \ \text{almost everywhere} \ x\in\Omega.

The generated equivalence class is denoted L1(Ω)\pmb{L^1(\Omega)}.

Definition Lp(Ω)L^p(\Omega)

Let Ω⊂Rn\Omega \sub\mathbb{R}^n and let p∈Np\in\mathbb{N}. Lp(Ω)\pmb{L^p(\Omega)} is the class equivalence (with equivalence relation ∼\sim) of all measurable functions f:Ω→Rf:\Omega\to\mathbb{R} with the property

∫Ω∣f∣pdμ<∞.\int_\Omega |f|^p d\mu<\infty.

References​

For the construction of the Lebesgue integral and the development of the Lebesgue spaces I was strongly inspired by 1 but adapted to the notation and concept used in 2, The exposition is intentionally detailed and self-contained to avoid requiring the reader to consult external references.

  1. B. P. Rynne and M. A. Youngson, Linear Functional Analysis, 2nd ed. London: Springer, 2008, pp. 20-28, 34.

  2. R. A. Adams and J. J. F. Fournier, Sobolev Spaces, 2nd ed. Amsterdam: Academic Press, 2003, pp. 13-16.