Moyal Distribution#
Univariate, Continuous, Asymmetric, Unbounded, Light-tailed
The Moyal distribution is a continuous probability distribution that was proposed by the physicist J. E. Moyal in 1955 as an approximation to the Landau distribution. The Moyal distribution is characterized by two parameters: the location parameter \(\mu\) and the scale parameter \(\sigma\).
The Moyal distribution is used in high-energy physics to model the energy loss, and the number of ion pairs produced, by ionization for fast charged particles.
Key properties and parameters#
Support |
\(x \in (-\infty, \infty)\) |
Mean |
\(\mu + \sigma\left(\gamma + \log 2\right)\), where \(\gamma\) is the Euler-Mascheroni constant |
Variance |
\(\frac{\pi^{2}}{2}\sigma^{2}\) |
Parameters:
\(\mu\) (loc): The location parameter.
\(\sigma\) (scale): The scale parameter.
Probability Density Function (PDF)#
where \(z = \frac{x - \mu}{\sigma}\).
Cumulative Distribution Function (CDF)#
where erf is the error function and \(z = \frac{x - \mu}{\sigma}\).