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Mittag-Leffler distribution

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The Mittag-Leffler distributions are two families of probability distributions on the half-line [ 0 , ) {\displaystyle [0,\infty )} α ( 0 , 1 ] {\displaystyle \alpha \in (0,1]} or α [ 0 , 1 ] {\displaystyle \alpha \in } . Both are defined with the Mittag-Leffler function, named after Gösta Mittag-Leffler.

The Mittag-Leffler function

For any complex α {\displaystyle \alpha } whose real part is positive, the series

E α ( z ) := n = 0 z n Γ ( 1 + α n ) {\displaystyle E_{\alpha }(z):=\sum _{n=0}^{\infty }{\frac {z^{n}}{\Gamma (1+\alpha n)}}}

defines an entire function. For α = 0 {\displaystyle \alpha =0} , the series converges only on a disc of radius one, but it can be analytically extended to C { 1 } {\displaystyle \mathbb {C} \setminus \{1\}} .

First family of Mittag-Leffler distributions

The first family of Mittag-Leffler distributions is defined by a relation between the Mittag-Leffler function and their cumulative distribution functions.

For all α ( 0 , 1 ] {\displaystyle \alpha \in (0,1]} , the function E α {\displaystyle E_{\alpha }} is increasing on the real line, converges to 0 {\displaystyle 0} in {\displaystyle -\infty } , and E α ( 0 ) = 1 {\displaystyle E_{\alpha }(0)=1} . Hence, the function x 1 E α ( x α ) {\displaystyle x\mapsto 1-E_{\alpha }(-x^{\alpha })} is the cumulative distribution function of a probability measure on the non-negative real numbers. The distribution thus defined, and any of its multiples, is called a Mittag-Leffler distribution of order α {\displaystyle \alpha } .

All these probability distributions are absolutely continuous. Since E 1 {\displaystyle E_{1}} is the exponential function, the Mittag-Leffler distribution of order 1 {\displaystyle 1} is an exponential distribution. However, for α ( 0 , 1 ) {\displaystyle \alpha \in (0,1)} , the Mittag-Leffler distributions are heavy-tailed, with

E α ( x α ) x α Γ ( 1 α ) , x . {\displaystyle E_{\alpha }(-x^{\alpha })\sim {\frac {x^{-\alpha }}{\Gamma (1-\alpha )}},\quad x\to \infty .}

Their Laplace transform is given by:

E ( e λ X α ) = 1 1 + λ α , {\displaystyle \mathbb {E} (e^{-\lambda X_{\alpha }})={\frac {1}{1+\lambda ^{\alpha }}},}

which implies that, for α ( 0 , 1 ) {\displaystyle \alpha \in (0,1)} , the expectation is infinite. In addition, these distributions are geometric stable distributions. Parameter estimation procedures can be found here.

Second family of Mittag-Leffler distributions

The second family of Mittag-Leffler distributions is defined by a relation between the Mittag-Leffler function and their moment-generating functions.

For all α [ 0 , 1 ] {\displaystyle \alpha \in } , a random variable X α {\displaystyle X_{\alpha }} is said to follow a Mittag-Leffler distribution of order α {\displaystyle \alpha } if, for some constant C > 0 {\displaystyle C>0} ,

E ( e z X α ) = E α ( C z ) , {\displaystyle \mathbb {E} (e^{zX_{\alpha }})=E_{\alpha }(Cz),}

where the convergence stands for all z {\displaystyle z} in the complex plane if α ( 0 , 1 ] {\displaystyle \alpha \in (0,1]} , and all z {\displaystyle z} in a disc of radius 1 / C {\displaystyle 1/C} if α = 0 {\displaystyle \alpha =0} .

A Mittag-Leffler distribution of order 0 {\displaystyle 0} is an exponential distribution. A Mittag-Leffler distribution of order 1 / 2 {\displaystyle 1/2} is the distribution of the absolute value of a normal distribution random variable. A Mittag-Leffler distribution of order 1 {\displaystyle 1} is a degenerate distribution. In opposition to the first family of Mittag-Leffler distribution, these distributions are not heavy-tailed.

These distributions are commonly found in relation with the local time of Markov processes.

References

  1. H. J. Haubold A. M. Mathai (2009). Proceedings of the Third UN/ESA/NASA Workshop on the International Heliophysical Year 2007 and Basic Space Science: National Astronomical Observatory of Japan. Astrophysics and Space Science Proceedings. Springer. p. 79. ISBN 978-3-642-03325-4.
  2. D.O. Cahoy V.V. Uhaikin W.A. Woyczyński (2010). "Parameter estimation for fractional Poisson processes". Journal of Statistical Planning and Inference. 140 (11): 3106–3120. arXiv:1806.02774. doi:10.1016/j.jspi.2010.04.016.
  3. D.O. Cahoy (2013). "Estimation of Mittag-Leffler parameters". Communications in Statistics - Simulation and Computation. 42 (2): 303–315. arXiv:1806.02792. doi:10.1080/03610918.2011.640094.
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