Differences

This shows you the differences between two versions of the page.

--- un:poisson-distribution [2023/06/20 09:45] – asad
+++ un:poisson-distribution [2023/10/22 05:16] (current) – removed asad
@@ Line 1: / Line 1: @@
-====== Poisson distribution ======
-A discrete [[probability distribution]] that expresses the probability of a given number of events occurring in a fixed interval of time or space when the events occur independently (non-correated) and at a constant given average rate. It is named after the French mathematician Siméon Denis Poisson (1781--1840).
-If the average (mean) rate is $\mu$, the probability of counting $x$ events in a single trial
-$$ P(x,\mu) = \frac{\mu^x}{x!} e^{-\mu} $$
-where $e$ is [[Euler's number]] and $x$ is a non-negative integer. The function is plotted below for three different means.
-https://colab.research.google.com/drive/1_Qwr1tiXnFgphLiypeGJcEmkLMMOHP41?usp=sharing|{{:un:poisson.png?nolink&750|}}]]
-For example, if $\mu=2.8$ (green curve) raindrops are falling on a tin roof on average per second, then the probability of hearing 4 raindrops in the next second $P(4,2.8) \approx 0.15$.
-The variance of Poisson distribution $\sigma^2=\mu$ and, hence, the standard deviation $\sigma=\sqrt{\mu}$.
-The fractional uncertainty in counting $N$ events
-$$ \frac{\sigma}{\mu} \approx \frac{1}{\sqrt{N}}. $$
-If $N$ photons have arrived in the detector of a telescope in $t$ seconds, then the //counts per second// $N/t$ has an uncertainty $\sigma/t \approx \sqrt{N}/t$.
-To decrease the uncertainty in measuring photons, we have to increase the number of photons by either increasing the size of the telescope of the exposure time.