The Laplace–Stieltjes transform, named for PierreSimon Laplace and Thomas Joannes Stieltjes, is an integral transform similar to the Laplace transform. For realvalued functions, it is the Laplace transform of a Stieltjes measure, however it is often defined for functions with values in a Banach space. It is useful in a number of areas of mathematics, including functional analysis, and certain areas of theoretical and applied probability.
Contents

Realvalued functions 1

Vector measures 2

Related transforms 3

Probability distributions 4

Exponential distribution 4.1

Erlang distribution 4.2

Uniform distribution 4.3

References 5
Realvalued functions
The Laplace–Stieltjes transform of a realvalued function g is given by a Lebesgue–Stieltjes integral of the form

\int\mathrm{e}^{sx}\,dg(x)
for s a complex number. As with the usual Laplace transform, one gets a slightly different transform depending on the domain of integration, and for the integral to be defined, one also needs to require that g be of bounded variation on the region of integration. The most common are:

The bilateral (or twosided) Laplace–Stieltjes transform is given by


\{\mathcal{L}^*g\}(s) = \int_{\infty}^{\infty} \mathrm{e}^{sx}\,dg(x).

The unilateral (onesided) Laplace–Stieltjes transform is given by


\{\mathcal{L}^*g\}(s) = \int_{0^}^{\infty} \mathrm{e}^{sx}\,dg(x).

where the lower limit 0^{−} means


\lim_{\varepsilon\to 0^+}\int_{\varepsilon}^\infty.

This is necessary to ensure that the transform captures a possible jump in g(x) at x = 0, as is needed to make sense of the Laplace transform of the Dirac delta function.

More general transforms can be considered by integrating over a contour in the complex plane; see Zhavrid 2001.
The Laplace–Stieltjes transform in the case of a scalarvalued function is thus seen to be a special case of the Laplace transform of a Stieltjes measure. To wit,

\mathcal{L}^*g = \mathcal{L}(dg).
In particular, it shares many properties with the usual Laplace transform. For instance, the convolution theorem holds:

\{\mathcal{L}^*(g * h)\}(s) = \{\mathcal{L}^*g\}(s)\{\mathcal{L}^*h\}(s).
Often only real values of the variable s are considered, although if the integral exists as a proper Lebesgue integral for a given real value s = σ, then it also exists for all complex s with re(s) ≥ σ.
The Laplace–Stieltjes transform appears naturally in the following context. If X is a random variable with cumulative distribution function F, then the Laplace–Stieltjes transform is given by the expectation:

\{\mathcal{L}^*F\}(s) = \mathrm{E}\left[\mathrm{e}^{sX}\right].
Vector measures
Whereas the Laplace–Stieltjes transform of a realvalued function is a special case of the Laplace transform of a measure applied to the associated Stieltjes measure, the conventional Laplace transform cannot handle vector measures: measures with values in a Banach space. These are, however, important in connection with the study of semigroups that arise in partial differential equations, harmonic analysis, and probability theory. The most important semigroups are, respectively, the heat semigroup, RiemannLiouville semigroup, and Brownian motion and other infinitely divisible processes.
Let g be a function from [0,∞) to a Banach space X of strongly bounded variation over every finite interval. This means that, for every fixed subinterval [0,T] one has

\sup \sum_i \g(t_i)g(t_{i+1})\_X < \infty
where the supremum is taken over all partitions of [0,T]

0=t_0 < t_1<\cdots< t_n=T.
The Stieltjes integral with respect to the vector measure dg

\int_0^T e^{st}dg(t)
is defined as a Riemann–Stieltjes integral. Indeed, if π is the tagged partition of the interval [0,T] with subdivision 0 = t_{0} ≤ t_{1} ≤ ... ≤ t_{n} = T, distinguished points τ_{i}∈ [t_{i},t_{i+1}] and mesh size π = maxt_{i}− t_{i+1}, the Riemann–Stieltjes integral is defined as the value of the limit

\lim_{\pi\to 0} \sum_{i=0}^{n1}e^{s\tau_i}[g(t_{i+1})g(t_i)]
taken in the topology on X. The hypothesis of strong bounded variation guarantees convergence.
If in the topology of X the limit

\lim_{T\to\infty} \int_0^T e^{st}dg(t)
exists, then the value of this limit is the Laplace–Stieltjes transform of g.
Related transforms
The Laplace–Stieltjes transform is closely related to other integral transforms, including the Fourier transform and the Laplace transform. In particular, note the following:

If g has derivative g' then the Laplace–Stieltjes transform of g is the Laplace transform of g' .


\{\mathcal{L}^*g\}(s) = \{\mathcal{L}g'\}(s),

We can obtain the Fourier–Stieltjes transform of g (and, by the above note, the Fourier transform of g' ) by


\{\mathcal{F}^*g\}(s) = \{\mathcal{L}^*g\}(\mathrm{i}s), \quad s \in \mathbb{R}.
Probability distributions
If X is a continuous random variable with cumulative distribution function F(t) then moments of X can be computed using^{[1]}

\mathbb E [X^n] = (1)^n \left.\frac{\text{d}^n \{\mathcal{L}^*F\}(s)}{\text{d}s^n} \right_{s=0}.
Exponential distribution
For an exponentially distributed random variable Y with rate parameter λ the LST is,


\tilde Y(s) = \{\mathcal{L}^*F_Y\}(s) = \int_0^\infty e^{st} \lambda e^{\lambda t} dt = \frac{\lambda}{\lambda+s}
from which the first three moments can be computed as 1/λ, 2/λ^{2} and 6/λ^{3}.
Erlang distribution
For Z with Erlang distribution (which is the sum of n exponential distributions) we use the fact that the probability distribution of the sum of independent random variables is equal to the convolution of their probability distributions. So if


Z = Y_1 + Y_2 + \ldots + Y_n
with the Y_{i} independent then


\tilde Z(s) = \tilde Y_1(s) \cdot \tilde Y_2(s) \cdot \cdots \cdot \tilde Y_n(s)
therefore in the case where Z has an Erlang distribution,


\tilde Z(s) = \left( \frac{\lambda}{\lambda+s} \right)^n.
Uniform distribution
For U with uniform distribution on the interval (a,b), the transform is given by


\tilde U(s) = \int_a^b e^{st} \frac{1}{ba}\text{d}t = \frac{e^{sa}e^{sb}}{s(ba)}.
References

^ HarcholBalter, M. (2012). "Transform Analysis". Performance Modeling and Design of Computer Systems. p. 433.

Apostol, T.M. (1957), Mathematical Analysis (1st ed.), Reading, MA: AddisonWesley ; 2nd ed (1974) ISBN 0201002884.

Apostol, T.M. (1997), Modular Functions and Dirichlet Series in Number Theory (2nd ed.), New York: SpringerVerlag, .

Grimmett, G.R.; Stirzaker, D.R. (2001), Probability and Random Processes (3rd ed.), Oxford: Oxford University Press, .

.

Zhavrid, N.S. (2001), "Laplace transform", in Hazewinkel, Michiel, .
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