Lebesgue–Stieltjes integration

In measure-theoretic analysis and related branches of mathematics, Lebesgue–Stieltjes integration generalizes both Riemann–Stieltjes and Lebesgue integration, preserving the many advantages of the former in a more general measure-theoretic framework. The Lebesgue–Stieltjes integral is the ordinary Lebesgue integral with respect to a measure known as the Lebesgue–Stieltjes measure, which may be associated to any function of bounded variation on the real line. The Lebesgue–Stieltjes measure is a regular Borel measure, and conversely every regular Borel measure on the real line is of this kind.

Lebesgue–Stieltjes integrals, named for Henri Leon Lebesgue and Thomas Joannes Stieltjes, are also known as Lebesgue–Radon integrals or just Radon integrals, after Johann Radon, to whom much of the theory is due. They find common application in probability and stochastic processes, and in certain branches of analysis including potential theory.

Definition

The Lebesgue–Stieltjes integral

\int _{a}^{b}f(x)\,dg(x)

is defined when $f:\left[a,b\right]\rightarrow \mathbb {R}$ is Borel-measurable and bounded and $g:\left[a,b\right]\rightarrow \mathbb {R}$ is of bounded variation in $[a, b]$ and right-continuous, or when $f$ is non-negative and $g$ is monotone and right-continuous. To start, assume that $f$ is non-negative and $g$ is monotone non-decreasing and right-continuous. Define $w ((s, t]) = g (t) - g (s)$ and $w ({a}) = 0$ (Alternatively, the construction works for $g$ left-continuous, $w ([s, t)) = g (t) - g (s)$ and $w ({b}) = 0$ ).

By Carathéodory's extension theorem, there is a unique Borel measure $μ g$ on $[a, b]$ which agrees with $w$ on every interval $I$ . The measure $μ g$ arises from an outer measure (in fact, a metric outer measure) given by

\mu _{g}(E)=\inf \left\{\sum _{i}\mu _{g}(I_{i})\ :\ E\subseteq \bigcup _{i}I_{i}\right\}

the infimum taken over all coverings of $E$ by countably many semiopen intervals. This measure is sometimes called^[1] the Lebesgue–Stieltjes measure associated with $g$ .

The Lebesgue–Stieltjes integral

\int _{a}^{b}f(x)\,dg(x)

is defined as the Lebesgue integral of $f$ with respect to the measure $μ g$ in the usual way. If $g$ is non-increasing, then define

\int _{a}^{b}f(x)\,dg(x):=-\int _{a}^{b}f(x)\,d(-g)(x),

the latter integral being defined by the preceding construction.

If $g$ is of bounded variation and $f$ is bounded, then it is possible to write

dg(x)=dg_{1}(x)-dg_{2}(x)

where $g 1 (x) = V x a g$ is the total variation of $g$ in the interval $[a, x]$ , and $g 2 (x) = g 1 (x) - g (x)$ . Both $g 1$ and $g 2$ are monotone non-decreasing. Now the Lebesgue–Stieltjes integral with respect to $g$ is defined by

\int _{a}^{b}f(x)\,dg(x)=\int _{a}^{b}f(x)\,dg_{1}(x)-\int _{a}^{b}f(x)\,dg_{2}(x),

where the latter two integrals are well-defined by the preceding construction.

Daniell integral

An alternative approach (Hewitt & Stromberg 1965) is to define the Lebesgue–Stieltjes integral as the Daniell integral that extends the usual Riemann–Stieltjes integral. Let $g$ be a non-decreasing right-continuous function on $[a, b]$ , and define $I (f)$ to be the Riemann–Stieltjes integral

I(f)=\int _{a}^{b}f(x)\,dg(x)

for all continuous functions $f$ . The functional $I$ defines a Radon measure on $[a, b]$ . This functional can then be extended to the class of all non-negative functions by setting

{\begin{aligned}{\overline {I}}(h)&=\sup \left\{I(f)\ :\ f\in C[a,b],0\leq f\leq h\right\}\\{\overline {\overline {I}}}(h)&=\inf \left\{I(f)\ :\ f\in C[a,b],h\leq f\right\}.\end{aligned}}

For Borel measurable functions, one has

{\overline {I}}(h)={\overline {\overline {I}}}(h),

and either side of the identity then defines the Lebesgue–Stieltjes integral of $h$ . The outer measure $μ g$ is defined via

\mu _{g}(A):={\overline {I}}(\chi _{A})={\overline {\overline {I}}}(\chi _{A})

where $χ A$ is the indicator function of $A$ .

Integrators of bounded variation are handled as above by decomposing into positive and negative variations.

Example

Suppose that $γ : [a, b] \to R 2$ is a rectifiable curve in the plane and $ρ : R 2 \to [0, \infty)$ is Borel measurable. Then we may define the length of $γ$ with respect to the Euclidean metric weighted by ρ to be

\int _{a}^{b}\rho (\gamma (t))\,d\ell (t),

where $\ell (t)$ is the length of the restriction of $γ$ to $[a, t]$ . This is sometimes called the $ρ$ -length of $γ$ . This notion is quite useful for various applications: for example, in muddy terrain the speed in which a person can move may depend on how deep the mud is. If $ρ (z)$ denotes the inverse of the walking speed at or near $z$ , then the $ρ$ -length of $γ$ is the time it would take to traverse $γ$ . The concept of extremal length uses this notion of the $ρ$ -length of curves and is useful in the study of conformal mappings.

Integration by parts

A function $f$ is said to be "regular" at a point $a$ if the right and left hand limits $f (a +)$ and $f (a -)$ exist, and the function takes at $a$ the average value

f(a)={\frac {f(a-)+f(a+)}{2}}.

Given two functions $U$ and $V$ of finite variation, if at each point either at least one of $U$ or $V$ is continuous or $U$ and $V$ are both regular, then an integration by parts formula for the Lebesgue–Stieltjes integral holds:^[2]

\int _{a}^{b}U\,dV+\int _{a}^{b}V\,dU=U(b+)V(b+)-U(a-)V(a-),\qquad -\infty <a<b<\infty .

Here the relevant Lebesgue–Stieltjes measures are associated with the right-continuous versions of the functions $U$ and $V$ ; that is, to ${\textstyle {\tilde {U}}(x)=\lim _{t\to x^{+}}U(t)}$ and similarly ${\tilde {V}}(x).$ The bounded interval $(a, b)$ may be replaced with an unbounded interval $(-\infty, b)$ , $(a, \infty)$ or $(-\infty, \infty)$ provided that $U$ and $V$ are of finite variation on this unbounded interval. Complex-valued functions may be used as well.

An alternative result, of significant importance in the theory of stochastic calculus is the following. Given two functions $U$ and $V$ of finite variation, which are both right-continuous and have left-limits (they are càdlàg functions) then

U(t)V(t)=U(0)V(0)+\int _{(0,t]}U(s-)\,dV(s)+\int _{(0,t]}V(s-)\,dU(s)+\sum _{u\in (0,t]}\Delta U_{u}\Delta V_{u},

where $Δ U t = U (t) - U (t -)$ . This result can be seen as a precursor to Itô's lemma, and is of use in the general theory of stochastic integration. The final term is $Δ U (t)Δ V (t) = d [U, V],$ which arises from the quadratic covariation of $U$ and $V$ . (The earlier result can then be seen as a result pertaining to the Stratonovich integral.)

Related concepts

Lebesgue integration

When $g (x) = x$ for all real $x$ , then $μ g$ is the Lebesgue measure, and the Lebesgue–Stieltjes integral of $f$ with respect to $g$ is equivalent to the Lebesgue integral of $f$ .

Riemann–Stieltjes integration and probability theory

Where $f$ is a continuous real-valued function of a real variable and $v$ is a non-decreasing real function, the Lebesgue–Stieltjes integral is equivalent to the Riemann–Stieltjes integral, in which case we often write

\int _{a}^{b}f(x)\,dv(x)

for the Lebesgue–Stieltjes integral, letting the measure $μ v$ remain implicit. This is particularly common in probability theory when $v$ is the cumulative distribution function of a real-valued random variable $X$ , in which case

\int _{-\infty }^{\infty }f(x)\,dv(x)=\mathrm {E} [f(X)].

(See the article on Riemann–Stieltjes integration for more detail on dealing with such cases.)

Notes

^ Halmos (1974), Sec. 15
^ Hewitt, Edwin (May 1960). "Integration by Parts for Stieltjes Integrals". The American Mathematical Monthly. 67 (5): 419–423. doi:10.2307/2309287. JSTOR 2309287.

References

Halmos, Paul R. (1974), Measure Theory, Berlin, New York: Springer-Verlag, ISBN 978-0-387-90088-9
Hewitt, Edwin; Stromberg, Karl (1965), Real and abstract analysis, Springer-Verlag.
Saks, Stanisław (1937) Theory of the Integral.
Shilov, G. E., and Gurevich, B. L., 1978. Integral, Measure, and Derivative: A Unified Approach, Richard A. Silverman, trans. Dover Publications. ISBN 0-486-63519-8.

[1] Halmos (1974), Sec. 15

[2] Hewitt, Edwin (May 1960). "Integration by Parts for Stieltjes Integrals". The American Mathematical Monthly. 67 (5): 419–423. doi:10.2307/2309287. JSTOR 2309287.

[1]

[2]

v t e Integrals
Types of integrals	Riemann integral Lebesgue integral Burkill integral Bochner integral Daniell integral Darboux integral Henstock–Kurzweil integral Haar integral Hellinger integral Khinchin integral Kolmogorov integral Lebesgue–Stieltjes integral Pettis integral Pfeffer integral Riemann–Stieltjes integral Regulated integral
Integration techniques	Substitution Trigonometric Euler Weierstrass By parts Partial fractions Euler's formula Inverse functions Changing order Reduction formulas Parametric derivatives Differentiation under the integral sign Laplace transform Contour integration Laplace's method Numerical integration Simpson's rule Trapezoidal rule Risch algorithm
Improper integrals	Gaussian integral Dirichlet integral Fermi–Dirac integral complete incomplete Bose–Einstein integral Frullani integral Common integrals in quantum field theory
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