Wright omega function
{{Short description|Mathematical function}}
{{Use American English|date = March 2019}}
In mathematics, the Wright omega function or Wright function,Not to be confused with the Fox–Wright function, also known as Wright function. denoted ω, is defined in terms of the Lambert W function as:
:
It is simpler to be defined by its inverse function
:
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 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 .
It also satisfies the differential equation
:
wherever ω is analytic (as can be seen by performing separation of variables and recovering the equation , and as a consequence its integral can be expressed as:
:
\int \omega^n \, dz =
\begin{cases}
\frac{\omega^{n+1} -1 }{n+1} + \frac{\omega^n}{n} & \mbox{if } n \neq -1, \\
\ln(\omega) - \frac{1}{\omega} & \mbox{if } n = -1.
\end{cases}
Its Taylor series around the point takes the form :
:
where
:
\begin{matrix}
n+1 \\
k
\end{matrix}
\bigg \rangle \! \! \bigg \rangle (-1)^k w^{k+1}
in which
:
\begin{matrix}
n \\
k
\end{matrix}
\bigg \rangle \! \! \bigg \rangle
Values
:
\begin{array}{lll}
\omega(0) &= W_0(1) &\approx 0.56714 \\
\omega(1) &= 1 & \\
\omega(-1 \pm i \pi) &= -1 & \\
\omega(-\frac{1}{3} + \ln \left ( \frac{1}{3} \right ) + i \pi ) &= -\frac{1}{3} & \\
\omega(-\frac{1}{3} + \ln \left ( \frac{1}{3} \right ) - i \pi ) &= W_{-1} \left ( -\frac{1}{3} e^{-\frac{1}{3}} \right ) &\approx -2.237147028 \\
\end{array}
Plots
Image:WrightOmegaRe.png|
Image:WrightOmegaIm.png|
Image:WrightOmegaAbs.png|
Notes
{{reflist|group=note}}
References
- [https://www.uwo.ca/apmaths/faculty/jeffrey/pdfs/wrightomega.pdf "The Wright ω function", Robert Corless and David Jeffrey]