Poisson process
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| Tomasz Downarowicz (2008), Scholarpedia, 3(11):3922. | revision #52355 [link to/cite this article] | |||||||||||||||||||
Contents |
The definition
A Poisson process is a homogeneous signal process with continuous time characterized by two properties:
1. The probability of two or more signals arriving at the same time (trajectories with jumps by more than one unit) is zero, and
2. The increments
are stochastically independent,
for any natural
and every
.
These properties imply that for every
the distribution of
is the Poisson distribution with parameter
for some real parameter
and so:
The expected value of
is
, thus
is interpreted as the average number of signals per unit of time and called the intensity.
If
, then the process is the trivial zero process, so it is natural to assume that
. In such a case the distribution of the waiting time
can be easily computed as follows
The expected value of
is
.
Interpretation
The Poisson process models the signals arriving by pure chance, independently from each-other, yet maintaining a constant intensity (expected number of signals per unit of time). It is widely used to model some processes in reality, for example incoming telephone calls, malfunctions of some device, etc. The interpretation is best understood via approximation, as described below.
Approximating the Poisson process
Poisson process can be obtained as the limit process in at least two ways; via Bernoulli schemes, and via independent signals on a bounded interval.
Bernoulli schemes
Consider an infinite sequence of 0-1 Bernoulli trials (i.e., i.i.d. 0-1 valued random variables) performed at equal (small) time distances
, where the probability of success (i.e., of 1) is
. It is clear that the generated signal process is homogeneous and satisfies both postulates in the definition of the Poisson process (of intensity
). The only difference is that it has discrete time with increment
rather than continuous time. The probability of exactly
successes observed in time
(for simplicity take
a multiple of
), is, by an elementary combinatorial formula, equal to
Letting
go to zero we arrive at a process with continuous time. On the other hand, applying elementary calculus the above formula is seen to converge to the formula for the Poisson distribution.
Independent signals in a bounded interval
Now consider the interval of time
where
is very large. Suppose for simplicity that
is an integer and consider
independent variables with the uniform distribution on
. These variables interpreted as times of arrivals of signals form a process satisfying both conditions postulated in the definition of the Poisson process (of intensity
) but only for
. Now, for
and
, the probability of exactly
signals in time
equals
This time we let
grow to infinity, and once again, we obtain the formula for the Poisson distribution.
