Wright omega function

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The Wright omega function along part of the real axis

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

ω(z)=WIm(z)π2π(ez).

It is simpler to be defined by its inverse function

z(ω)=ln(ω)+ω

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

Properties

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The Wright omega function satisfies the relation Wk(z)=ω(ln(z)+2πik).

It also satisfies the differential equation

dωdz=ω1+ω

wherever ω is analytic (as can be seen by performing separation of variables and recovering the equation ln(ω)+ω=z, and as a consequence its integral can be expressed as:

ωndz={ωn+11n+1+ωnnif n1,ln(ω)1ωif n=1.

Its Taylor series around the point a=ωa+ln(ωa) takes the form :

ω(z)=n=0+qn(ωa)(1+ωa)2n1(za)nn!

where

qn(w)=k=0n1n+1k(1)kwk+1

in which

nk

is a second-order Eulerian number.

Values

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ω(0)=W0(1)0.56714ω(1)=1ω(1±iπ)=1ω(13+ln(13)+iπ)=13ω(13+ln(13)iπ)=W1(13e13)2.237147028

Plots

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Notes

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  1. ^ Not to be confused with the Fox–Wright function, also known as Wright function.
  2. ^ This plot has been reported as incorrect; see Talk page.

References

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