Wright omega function explained

In mathematics, the Wright omega function or Wright function,[1] denoted ω, is defined in terms of the Lambert W function as:

\omega(z)=

W
\lceil
Im(z)-\pi
2\pi
\rceil

(ez).

Uses

One of the main applications of this function is in the resolution of the equation z = ln(z), as the only solution is given by z = e-ω(π i).

y = ω(z) is the unique solution, when

zx\pmi\pi

for x ≤ -1, of the equation y + ln(y) = z. Except for those two values, the Wright omega function is continuous, even analytic.

Properties

The Wright omega function satisfies the relation

Wk(z)=\omega(ln(z)+2\piik)

.

It also satisfies the differential equation

d\omega
dz

=

\omega
1+\omega

wherever ω is analytic (as can be seen by performing separation of variables and recovering the equation

ln(\omega)+\omega=z

), and as a consequence its integral can be expressed as:

\int\omegandz=\begin{cases}

\omegan+1-1
n+1

+

\omegan
n

&ifn-1,\\ ln(\omega)-

1
\omega

&ifn=-1. \end{cases}

Its Taylor series around the point

a=\omegaa+ln(\omegaa)

takes the form :

\omega(z)=

+infty
\sum
n=0
qn(\omegaa)
2n-1
(1+\omega
a)
(z-a)n
n!

where

qn(w)=

n-1
\sum
k=0

\langle \langle\begin{matrix} n+1\\ k \end{matrix} \rangle \rangle(-1)kwk+1

in which

\langle \langle\begin{matrix} n\\ k \end{matrix} \rangle \rangle

is a second-order Eulerian number.

Values

\begin{array}{lll} \omega(0)&=W0(1)&0.56714\\ \omega(1)&=1&\\ \omega(-1\pmi\pi)&=-1&\\ \omega(-

1
3

+ln\left(

1
3

\right)+i\pi)&=-

1
3

&\\ \omega(-

1
3

+ln\left(

1
3

\right)-i\pi)&=W-1\left(-

1
3
-1
3
e

\right)&-2.237147028\\ \end{array}

References

Notes and References

  1. Not to be confused with the Fox–Wright function, also known as Wright function.