MIT 6.041 Probability: Poisson Process I

Probability
MIT 6.041
Poisson Process
Exponential Distribution
Erlang Distribution
Notes on Poisson processes, the Bernoulli-to-Poisson limit, interarrival times, Erlang waiting times, and merging independent Poisson processes.
Author

Chao Ma

Published

August 5, 2026

A Poisson process is a continuous-time model for random arrivals.

It is the continuous analogue of a Bernoulli process: instead of checking whether an arrival happens in each discrete slot, we count arrivals over continuous time intervals.

Definition

Let \(N(t)\) be the number of arrivals by time \(t\). For an interval of length \(\tau\),

\[ P(k,\tau) = \Pr(N(t+\tau)-N(t)=k). \]

The process is characterized by three ideas:

  • Homogeneity: the distribution depends only on the interval length \(\tau\), not on where the interval starts.
  • Independent increments: numbers of arrivals in disjoint intervals are independent.
  • Small-interval behavior: in a tiny interval, either no arrival happens or one arrival happens; two or more arrivals are negligible.

For a fixed interval length \(\tau\),

\[ \sum_{k=0}^{\infty} P(k,\tau)=1. \]

Small Interval Probabilities

For a very small interval of length \(\delta\),

\[ P(k,\delta) \approx \begin{cases} 1-\lambda\delta, & k=0,\\ \lambda\delta, & k=1,\\ 0, & k>1. \end{cases} \]

Here \(\lambda\) is the arrival rate per unit time.

Intuition:

  • \(\lambda\delta\) is the approximate probability of one arrival in a tiny interval.
  • \(1-\lambda\delta\) is the approximate probability of no arrival.
  • The probability of more than one arrival in a tiny interval is approximately zero.

From Bernoulli to Poisson

The Poisson PMF can be derived as a limit of binomial probabilities.

Step 1: Discretize Time

Take an interval of length \(\tau\) and divide it into \(n\) small slots:

\[ \delta = \frac{\tau}{n}. \]

As \(n\to\infty\), the slot length \(\delta\to 0\).

Step 2: Match the Arrival Rate

Approximate each small slot as a Bernoulli trial with success probability

\[ p = \lambda\delta = \lambda\left(\frac{\tau}{n}\right) = \frac{\lambda\tau}{n}. \]

Then the expected number of arrivals in the whole interval is

\[ np = n\left(\frac{\lambda\tau}{n}\right) = \lambda\tau. \]

Step 3: Start from the Binomial PMF

If the \(n\) tiny slots are independent Bernoulli trials, then

\[ P(K_n=k) = \binom{n}{k}p^k(1-p)^{n-k}. \]

Substitute \(p=\lambda\tau/n\):

\[ P(K_n=k) = \binom{n}{k} \left(\frac{\lambda\tau}{n}\right)^k \left(1-\frac{\lambda\tau}{n}\right)^{n-k}. \]

Step 4: Take the Limit

For fixed \(k\),

\[ \binom{n}{k} = \frac{n(n-1)\cdots(n-k+1)}{k!}. \]

So

\[ P(K_n=k) = \frac{n(n-1)\cdots(n-k+1)}{k!} \left(\frac{\lambda\tau}{n}\right)^k \left(1-\frac{\lambda\tau}{n}\right)^n \left(1-\frac{\lambda\tau}{n}\right)^{-k}. \]

As \(n\to\infty\):

\[ \frac{n(n-1)\cdots(n-k+1)}{n^k}\to 1, \]

\[ \left(1-\frac{\lambda\tau}{n}\right)^n \to e^{-\lambda\tau}, \]

and

\[ \left(1-\frac{\lambda\tau}{n}\right)^{-k}\to 1. \]

Therefore,

\[ P(K=k) = \frac{(\lambda\tau)^k e^{-\lambda\tau}}{k!}, \qquad k=0,1,2,\ldots \]

From Bernoulli trials to the Poisson distribution.

Example: Email Arrivals

Suppose emails arrive according to a Poisson process with rate

\[ \lambda=5 \]

messages per hour. You check email every 30 minutes, so \(\tau=1/2\) and

\[ \lambda\tau = 5\cdot\frac{1}{2}=2.5. \]

The probability of no new messages is

\[ P(0,1/2) = \frac{(2.5)^0}{0!}e^{-2.5} = e^{-2.5} \approx 0.082. \]

The probability of exactly one new message is

\[ P(1,1/2) = \frac{(2.5)^1}{1!}e^{-2.5} = 2.5e^{-2.5} \approx 0.205. \]

Interarrival Times

Let \(X_i\) be the time between the \((i-1)\)st arrival and the \(i\)th arrival. For a Poisson process with rate \(\lambda\),

\[ X_i \sim \operatorname{Exponential}(\lambda), \qquad f_X(x)=\lambda e^{-\lambda x}, \quad x\ge 0. \]

The interarrival times are independent and identically distributed. This is the continuous-time memoryless structure behind the Poisson process.

Time of the kth Arrival

Let \(Y_k\) be the time from the start of the process until the \(k\)th arrival. Then

\[ Y_k = X_1 + X_2 + \cdots + X_k. \]

Because \(Y_k\) is the sum of \(k\) independent exponential random variables with rate \(\lambda\),

\[ Y_k \sim \operatorname{Erlang}(k,\lambda), \]

with density

\[ f_{Y_k}(y) = \frac{\lambda^k y^{k-1}e^{-\lambda y}}{(k-1)!}, \qquad y\ge 0. \]

For \(k=1\), this reduces to the exponential density:

\[ f_{Y_1}(y) = \lambda e^{-\lambda y}, \qquad y\ge 0. \]

Memorylessness

The exponential interarrival time is memoryless:

\[ \Pr(X>s+t\mid X>s)=\Pr(X>t). \]

Intuition: if no arrival has happened yet, the remaining waiting time has the same distribution as if the process just started.

Bernoulli and Poisson Relation

The Poisson process can be viewed as the limit of a Bernoulli process under rare events and many trials:

  • Divide continuous time into tiny slots of length \(\delta\).
  • Treat each slot as a Bernoulli trial with success probability \(p=\lambda\delta\).
  • Let \(\delta\to 0\) while keeping \(\lambda\tau\) fixed.
Concept Poisson process Bernoulli process
Time model Continuous Discrete
Arrival rate \(\lambda\) per unit time \(p\) per trial
Count distribution Poisson Binomial
First arrival time Exponential Geometric
Time to kth arrival Erlang Negative binomial

Merging

If two independent Poisson processes have rates \(\lambda_1\) and \(\lambda_2\), then their merged process is also Poisson.

The merged rate is

\[ \lambda_{\text{total}} = \lambda_1+\lambda_2. \]

Given that an arrival occurred in the merged process, the probability that it came from process 1 is proportional to its rate:

\[ \Pr(\text{from process 1}\mid \text{arrival}) = \frac{\lambda_1}{\lambda_1+\lambda_2}. \]

Takeaways

  • The Poisson process models random arrivals in continuous time.
  • Counts in a fixed interval follow a Poisson distribution.
  • Interarrival times are independent exponential random variables.
  • The time to the kth arrival follows an Erlang distribution.
  • Independent Poisson processes merge into another Poisson process with rates added.

Source: MIT 6.041 Probabilistic Systems Analysis and Applied Probability, Poisson Process I.