Wrapped Lévy distribution explained

In probability theory and directional statistics, a wrapped Lévy distribution is a wrapped probability distribution that results from the "wrapping" of the Lévy distribution around the unit circle.

Description

The pdf of the wrapped Lévy distribution is

fWL

infty
(\theta;\mu,c)=\sum\sqrt{
n=-infty
c
2\pi
}\,\frac

where the value of the summand is taken to be zero when

\theta+2\pin-\mu\le0

,

c

is the scale factor and

\mu

is the location parameter. Expressing the above pdf in terms of the characteristic function of the Lévy distribution yields:

fWL(\theta;\mu,c)=

1
2\pi
infty
\sum
n=-infty

e-in(\theta-\mu)-\sqrt{c|n|(1-isgn{n})}=

1
2\pi

\left(1+

infty
2\sum
n=1

e-\sqrt{cn

}\cos\left(n(\theta-\mu) - \sqrt\,\right)\right)

In terms of the circular variable

z=ei\theta

the circular moments of the wrapped Lévy distribution are the characteristic function of the Lévy distribution evaluated at integer arguments:

\langle

n\rangle=\int
z
\Gamma

ein\thetafWL(\theta;\mu,c)d\theta=ei(1-isgn(n))}.

where

\Gamma

is some interval of length

2\pi

. The first moment is then the expectation value of z, also known as the mean resultant, or mean resultant vector:

\langlez\rangle=ei\mu-\sqrt{c(1-i)}

The mean angle is

\theta\mu=Arg\langlez\rangle=\mu+\sqrt{c}

and the length of the mean resultant is

R=|\langlez\rangle|=e-\sqrt{c

}

See also

References