Poisson Process

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)X_n \sim \text{Bin}(n, p) denote a binomial random variable, where:

  • nn is the number of independent Bernoulli trials.
  • pp is the probability of success.
  • λ=np\lambda = np is the expected number of successes.

We are interested in the behavior of XnX_n as n→∞n \to \infty, such that λ=np\lambda = np is held constant.

Let Xn∼Bin(n,λ/n)X_n \sim \text{Bin}(n, \lambda/n). Then:

lim⁡n→∞P(Xn=k)=e−λλkk!,for all k∈{0,1,2,....}. \begin{equation} \lim_{n \to \infty} \mathbb{P}(X_n = k) = \frac{e^{-\lambda} \lambda^k}{k!}, \quad \text{for all } k \in \{0,1,2,....\}. \end{equation}

P(Xn=k)=(nk)(λn)k(1−λn)n−k=n(n−1)…(n−k+1)k!⋅(λknk)⋅(1−λn)n⋅(1−λn)−k. \begin{equation} \begin{aligned} \mathbb{P}(X_n = k) &= \binom{n}{k} \left(\frac{\lambda}{n}\right)^k \left(1 - \frac{\lambda}{n}\right)^{n - k} \\ &= \frac{n(n-1)\dots(n-k+1)}{k!} \cdot \left(\frac{\lambda^k}{n^k}\right) \cdot \left(1 - \frac{\lambda}{n}\right)^n \cdot \left(1 - \frac{\lambda}{n}\right)^{-k}. \end{aligned} \end{equation}

Using the limits:

  • n(n−1)…(n−k+1)nk→1\frac{n(n-1)\dots(n-k+1)}{n^k} \to 1,
  • (1−λn)n→e−λ\left(1 - \frac{\lambda}{n}\right)^n \to e^{-\lambda},
  • (1−λn)−k→1\left(1 - \frac{\lambda}{n}\right)^{-k} \to 1,

the expression converges to:

λke−λk!. \begin{equation} \frac{\lambda^k e^{-\lambda}}{k!}. \end{equation}

This proves convergence in distribution to the Poisson distribution.

1: Superposition

Let X∼Poisson(λ1t),Y∼Poisson(λ2t)X \sim \text{Poisson}(\lambda_1 t), Y \sim \text{Poisson}(\lambda_2 t), then:

P(X+Y=k)=∑i=0kP(X=i)P(Y=k−i) \begin{equation} \mathbb{P}(X + Y = k) = \sum_{i=0}^{k} \mathbb{P}(X = i) \mathbb{P}(Y = k - i) \end{equation}

=e−(λ1+λ2)t∑i=0k(λ1t)ii!⋅(λ2t)k−i(k−i)! = e^{-(\lambda_1 + \lambda_2)t} \sum_{i=0}^k \frac{(\lambda_1 t)^i}{i!} \cdot \frac{(\lambda_2 t)^{k - i}}{(k - i)!}

=e−(λ1+λ2)tk!∑i=0k(ki)(λ1t)i(λ2t)k−i=e−(λ1+λ2)tk!(λ1t+λ2t)k = \frac{e^{-(\lambda_1 + \lambda_2)t}}{k!} \sum_{i=0}^{k} \binom{k}{i} (\lambda_1 t)^i (\lambda_2 t)^{k - i} = \frac{e^{-(\lambda_1 + \lambda_2)t}}{k!} (\lambda_1 t + \lambda_2 t)^k

=(λ1+λ2)ktkk!e−(λ1+λ2)t. = \frac{(\lambda_1 + \lambda_2)^k t^k}{k!} e^{-(\lambda_1 + \lambda_2)t}.

This is the PMF of a Poisson((λ1+λ2)t)\text{Poisson}((\lambda_1 + \lambda_2)t) process.

2: Inter-arrival Times in a Poisson Process

Let T1,T2,…T_1, T_2, \dots be arrival times in a homogeneous Poisson process with rate λ\lambda. Define inter-arrival times Sn=Tn−Tn−1S_n = T_n - T_{n - 1} (with T0=0T_0 = 0).

Exponential Inter-arrival Times

Each Sn∼Exp(λ)S_n \sim \text{Exp}(\lambda), and the SnS_n are i.i.d. (independent and identically distributed).

Proof: The probability that no event occurs in the interval [0,t][0, t] is:

P(S1>t)=P(N(t)=0)=e−λt \begin{equation} \mathbb{P}(S_1 > t) = \mathbb{P}(N(t) = 0) = e^{-\lambda t} \end{equation}

So the Cumulative Distribution Function (CDF) of S1S_1 is:

FS1(t)=P(S1≤t)=1−P(S1>t)=1−e−λt \begin{equation} F_{S_1}(t) = \mathbb{P}(S_1 \le t) = 1 - \mathbb{P}(S_1 > t) = 1 - e^{-\lambda t} \end{equation}

The Probability Density Function (PDF) is the derivative of the CDF:

fS1(t)=ddt(1−e−λt)=λe−λt,t≥0 \begin{equation} f_{S_1}(t) = \frac{d}{dt}(1 - e^{-\lambda t}) = \lambda e^{-\lambda t}, \quad t \ge 0 \end{equation}

By the memoryless property of the Poisson process, the process effectively "restarts" after each arrival. This means the time until the next arrival (S2S_2) is independent of the previous waiting time and follows the same distribution. Hence, S2,S3,⋯∼Exp(λ)S_2, S_3, \dots \sim \text{Exp}(\lambda) i.i.d.