Poisson Process
Overview
The Poisson distribution arises naturally as a limit of the binomial distribution when the number of trials becomes large and the success probability becomes small, such that the expected number of successes remains constant. This is a key idea in stochastic processes and models real-world arrivald such as radioactive decay, call arrivals, and queue arrivals.
Let Xn∼Bin(n,p) denote a binomial random variable, where:
- n is the number of independent Bernoulli trials.
- p is the probability of success.
- λ=np is the expected number of successes.
We are interested in the behavior of Xn as n→∞, such that λ=np is held constant.
Let Xn∼Bin(n,λ/n). Then:
n→∞limP(Xn=k)=k!e−λλk,for all k∈{0,1,2,....}.
P(Xn=k)=(kn)(nλ)k(1−nλ)n−k=k!n(n−1)…(n−k+1)⋅(nkλk)⋅(1−nλ)n⋅(1−nλ)−k.
Using the limits:
- nkn(n−1)…(n−k+1)→1,
- (1−nλ)n→e−λ,
- (1−nλ)−k→1,
the expression converges to:
k!λke−λ.
This proves convergence in distribution to the Poisson distribution.
Theorem: Superposition
Let X∼Poisson(λ1t),Y∼Poisson(λ2t), then:
P(X+Y=k)=i=0∑kP(X=i)P(Y=k−i)
=e−(λ1+λ2)ti=0∑ki!(λ1t)i⋅(k−i)!(λ2t)k−i
=k!e−(λ1+λ2)ti=0∑k(ik)(λ1t)i(λ2t)k−i=k!e−(λ1+λ2)t(λ1t+λ2t)k
=k!(λ1+λ2)ktke−(λ1+λ2)t.
This is the PMF of a Poisson((λ1+λ2)t) process.
Inter-arrival Times in a Poisson Process
Let T1,T2,… be arrival times in a homogeneous Poisson process with rate λ.
Define inter-arrival times Sn=Tn−Tn−1 (with T0=0).
Theorem: Exponential Inter-arrival Times
Each Sn∼Exp(λ), and the Sn are i.i.d. (independent and identically distributed).
Proof:
The probability that no event occurs in the interval [0,t] is:
P(S1>t)=P(N(t)=0)=e−λt
So the Cumulative Distribution Function (CDF) of S1 is:
FS1(t)=P(S1≤t)=1−P(S1>t)=1−e−λt
The Probability Density Function (PDF) is the derivative of the CDF:
fS1(t)=dtd(1−e−λt)=λe−λt,t≥0
By the memoryless property of the Poisson process, the process effectively "restarts" after each arrival. This means the time until the next arrival (S2) is independent of the previous waiting time and follows the same distribution. Hence, S2,S3,⋯∼Exp(λ) i.i.d.