Simple function
In the mathematical field of real analysis, a simple function is a real (or complex)-valued function over a subset of the real line, similar to a step function. Simple functions are sufficiently "nice" that using them makes mathematical reasoning, theory, and proof easier. For example, simple functions attain only a finite number of values. Some authors also require simple functions to be measurable, as used in practice.
A basic example of a simple function is the floor function over the half-open interval [1, 9), whose only values are {1, 2, 3, 4, 5, 6, 7, 8}. A more advanced example is the Dirichlet function over the real line, which takes the value 1 if x is rational and 0 otherwise. (Thus the "simple" of "simple function" has a technical meaning somewhat at odds with common language.) All step functions are simple.
Simple functions are used as a first stage in the development of theories of integration, such as the Lebesgue integral, because it is easy to define integration for a simple function and also it is straightforward to approximate more general functions by sequences of simple functions.
Definition
[edit ]Formally, a simple function is a finite linear combination of indicator functions of measurable sets. More precisely, let (X, Σ) be a measurable space. Let A1, ..., An ∈ Σ be a sequence of disjoint measurable sets, and let a1, ..., an be a sequence of real or complex numbers. A simple function is a function {\displaystyle f\colon X\to \mathbb {C} } of the form
- {\displaystyle f(x)=\sum _{k=1}^{n}a_{k}{\mathbf {1} }_{A_{k}}(x),}
where {\displaystyle {\mathbf {1} }_{A}} is the indicator function of the set A.
Properties of simple functions
[edit ]The sum, difference, and product of two simple functions are again simple functions, and multiplication by constant keeps a simple function simple; hence it follows that the collection of all simple functions on a given measurable space forms a commutative algebra over {\displaystyle \mathbb {C} }.
Integration of simple functions
[edit ]If a measure {\displaystyle \mu } is defined on the space {\displaystyle (X,\Sigma )}, the integral of a simple function {\displaystyle f\colon X\to \mathbb {R} } with respect to {\displaystyle \mu } is defined to be
- {\displaystyle \int _{X}fd\mu =\sum _{k=1}^{n}a_{k}\mu (A_{k}),}
if all summands are finite.
Relation to Lebesgue integration
[edit ]The above integral of simple functions can be extended to a more general class of functions, which is how the Lebesgue integral is defined. This extension is based on the following fact.
- Theorem. Any non-negative measurable function {\displaystyle f\colon X\to \mathbb {R} ^{+}} is the pointwise limit of a monotonic increasing sequence of non-negative simple functions.
It is implied in the statement that the sigma-algebra in the co-domain {\displaystyle \mathbb {R} ^{+}} is the restriction of the Borel σ-algebra {\displaystyle {\mathfrak {B}}(\mathbb {R} )} to {\displaystyle \mathbb {R} ^{+}}. The proof proceeds as follows. Let {\displaystyle f} be a non-negative measurable function defined over the measure space {\displaystyle (X,\Sigma ,\mu )}. For each {\displaystyle n\in \mathbb {N} }, subdivide the co-domain of {\displaystyle f} into {\displaystyle 2^{2n}+1} intervals, {\displaystyle 2^{2n}} of which have length {\displaystyle 2^{-n}}. That is, for each {\displaystyle n}, define
- {\displaystyle I_{n,k}=\left[{\frac {k-1}{2^{n}}},{\frac {k}{2^{n}}}\right)} for {\displaystyle k=1,2,\ldots ,2^{2n}}, and {\displaystyle I_{n,2^{2n}+1}=[2^{n},\infty )},
which are disjoint and cover the non-negative real line ({\displaystyle \mathbb {R} ^{+}\subseteq \cup _{k}I_{n,k},\forall n\in \mathbb {N} }).
Now define the sets
- {\displaystyle A_{n,k}=f^{-1}(I_{n,k}),円} for {\displaystyle k=1,2,\ldots ,2^{2n}+1,}
which are measurable ({\displaystyle A_{n,k}\in \Sigma }) because {\displaystyle f} is assumed to be measurable.
Then the increasing sequence of simple functions
- {\displaystyle f_{n}=\sum _{k=1}^{2^{2n}+1}{\frac {k-1}{2^{n}}}{\mathbf {1} }_{A_{n,k}}}
converges pointwise to {\displaystyle f} as {\displaystyle n\to \infty }. Note that, when {\displaystyle f} is bounded, the convergence is uniform.