Wright Omega function

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Short description: Mathematical function
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)=W⌈Im(z)−π2π⌉(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 z≠x±iπ for x ≤ −1, of the equation y + ln(y) = z. Except on those two rays, the Wright omega function is continuous, even analytic.

Properties

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:

∫wndz={ωn+1−1n+1+ωnnif n≠−1,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)2n−1(z−a)nn!

where

qn(w)=∑k=0n−1⟨⟨n+1k⟩⟩(−1)kwk+1

in which

⟨⟨nk⟩⟩

is a second-order Eulerian number.

Values

ω(0)=W0(1)≈0.56714ω(1)=1ω(−1±iπ)=−1ω(−13+ln⁡(13)+iπ)=−13ω(−13+ln⁡(13)−iπ)=W−1(−13e−13)≈−2.237147028

Plots

Notes

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

References