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{{Short description|Random process in probability theory}}  
{{Short description|Random process in probability theory}}{{One source|date=March 2026}}
A '''compound Poisson process''' is a continuous-time [[Stochastic process|stochastic process]] with jumps. The jumps arrive randomly according to a [[Poisson process]] and the size of the jumps is also random, with a specified probability distribution. To be precise, a compound Poisson process, parameterised by a rate <math>\lambda > 0</math> and jump size distribution ''G'', is a process <math>\{\,Y(t) : t \geq 0 \,\}</math> given by
A '''compound Poisson process''' is a continuous-time [[Stochastic process|stochastic process]] with jumps. The jumps arrive randomly according to a [[Poisson process]] and the size of the jumps is also random, with a specified probability distribution. To be precise, a compound Poisson process, parameterised by a rate <math>\lambda > 0</math> and jump size distribution ''G'', is a process <math>\{\,Y(t) : t \geq 0 \,\}</math> given by


:<math>Y(t) = \sum_{i=1}^{N(t)} D_i</math>
:<math>Y(t) = \sum_{i=1}^{N(t)} D_i</math>


where, <math> \{\,N(t) : t \geq 0\,\}</math> is the counting variable of a [[Poisson process]] with rate <math>\lambda</math>, and <math> \{\,D_i : i \geq 1\,\}</math> are independent and identically distributed random variables, with distribution function ''G'', which are also independent of <math> \{\,N(t) : t \geq 0\,\}.\,</math>
where, <math> \{\,N(t) : t \geq 0\,\}</math> is the counting variable of a [[Poisson process]] with rate <math>\lambda</math>, and <math> \{\,D_i : i \geq 1\,\}</math> are independent and identically distributed random variables, with distribution function ''G'', which are also independent of <math> \{\,N(t) : t \geq 0\,\}.\,</math><ref>{{Cite book |last=Ross |first=Sheldon M. |title=Stochastic processes |date=1996 |publisher=Wiley |isbn=978-0-471-12062-9 |edition=2nd |series=Wiley series in probability and statistics |location=New York}}</ref>


When <math> D_i </math> are non-negative integer-valued random variables, then this compound Poisson process is known as a '''stuttering Poisson process.''' {{source needed|date=December 2024}}
When <math> D_i </math> are non-negative integer-valued random variables, then this compound Poisson process is known as a '''stuttering Poisson process.''' {{source needed|date=December 2024}}
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* Campbell's formula for the moment generating function of a compound Poisson process
* Campbell's formula for the moment generating function of a compound Poisson process


{{Stochastic processes}}
== References ==
{{Reflist}}{{Stochastic processes}}


{{DEFAULTSORT:Compound Poisson Process}}
{{DEFAULTSORT:Compound Poisson Process}}

Latest revision as of 23:27, 15 April 2026

Short description: Random process in probability theory

A compound Poisson process is a continuous-time stochastic process with jumps. The jumps arrive randomly according to a Poisson process and the size of the jumps is also random, with a specified probability distribution. To be precise, a compound Poisson process, parameterised by a rate λ>0 and jump size distribution G, is a process {Y(t):t0} given by

Y(t)=i=1N(t)Di

where, {N(t):t0} is the counting variable of a Poisson process with rate λ, and {Di:i1} are independent and identically distributed random variables, with distribution function G, which are also independent of {N(t):t0}.[1]

When Di are non-negative integer-valued random variables, then this compound Poisson process is known as a stuttering Poisson process. [citation needed]

Properties of the compound Poisson process

The expected value of a compound Poisson process can be calculated using a result known as Wald's equation as:

E(Y(t))=E(D1++DN(t))=E(N(t))E(D1)=E(N(t))E(D)=λtE(D).

Making similar use of the law of total variance, the variance can be calculated as:

var(Y(t))=E(var(Y(t)N(t)))+var(E(Y(t)N(t)))=E(N(t)var(D))+var(N(t)E(D))=var(D)E(N(t))+E(D)2var(N(t))=var(D)λt+E(D)2λt=λt(var(D)+E(D)2)=λtE(D2).

Lastly, using the law of total probability, the moment generating function can be given as follows:

Pr(Y(t)=i)=nPr(Y(t)=iN(t)=n)Pr(N(t)=n)
E(esY)=iesiPr(Y(t)=i)=iesinPr(Y(t)=iN(t)=n)Pr(N(t)=n)=nPr(N(t)=n)iesiPr(Y(t)=iN(t)=n)=nPr(N(t)=n)iesiPr(D1+D2++Dn=i)=nPr(N(t)=n)MD(s)n=nPr(N(t)=n)enln(MD(s))=MN(t)(ln(MD(s)))=eλt(MD(s)1).

Exponentiation of measures

Let N, Y, and D be as above. Let μ be the probability measure according to which D is distributed, i.e.

μ(A)=Pr(DA).

Let δ0 be the trivial probability distribution putting all of the mass at zero. Then the probability distribution of Y(t) is the measure

exp(λt(μδ0))

where the exponential exp(ν) of a finite measure ν on Borel subsets of the real line is defined by

exp(ν)=n=0ν*nn!

and

ν*n=ν**νn factors

is a convolution of measures, and the series converges weakly.

See also

References

  1. Ross, Sheldon M. (1996). Stochastic processes. Wiley series in probability and statistics (2nd ed.). New York: Wiley. ISBN 978-0-471-12062-9. 

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