Landau distribution

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Landau distribution with mode at 2 and sigma of 1

In probability theory, the Landau distribution[1] is a probability distribution named after Lev Landau. Because of the distribution's long tail, the moments of the distribution, like mean or variance, are undefined. The distribution is a special case of the stable distribution.

Definition

The probability density function of a standard version of the Landau distribution is defined by the complex integral

p(x)={\frac  {1}{2\pi i}}\int _{{c-i\infty }}^{{c+i\infty }}\!e^{{s\log s+xs}}\,ds,

where c is any positive real number, and log refers to the logarithm base e, the natural logarithm. The result does not change if c changes. For numerical purposes it is more convenient to use the following equivalent form of the integral,

p(x)={\frac  {1}{\pi }}\int _{0}^{\infty }\!e^{{-t\log t-xt}}\sin(\pi t)\,dt.

The full family of Landau distributions is obtained by extending the standard distribution to a location-scale family.

This distribution is a special case of the stable distribution with parameters α = 1, and β = 1.[2]

The characteristic function may be expressed as:

\varphi (t;\mu ,c)=\exp \!{\Big [}\;it\mu -|c\,t|(1+{\tfrac  {2i}{\pi }}\log(|t|)){\Big ]}.

where μ and c are real, which yields a Landau distribution shifted by μ and scaled by c.[3]

Related distributions

References

  1. Landau, L. (1944). "On the energy loss of fast particles by ionization". J. Phys. (USSR) 8: 201. 
  2. Gentle, James E. (2003). Random Number Generation and Monte Carlo Methods. Statistics and Computing (2nd ed.). New York, NY: Springer. p. 196. doi:10.1007/b97336. ISBN 978-0-387-00178-4. 
  3. Meroli, S. (2011). "Energy loss measurement for charged particles in very thin silicon layers". JINST 6: 6013. 


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