Fox–Wright function

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Template:Short description In mathematics, the Fox–Wright function (also known as Fox–Wright Psi function, not to be confused with Wright Omega function) is a generalisation of the generalised hypergeometric function pFq(z) based on ideas of Template:Harvs and Template:Harvs:

pΨq[(a1,A1)(a2,A2)…(ap,Ap)(b1,B1)(b2,B2)…(bq,Bq);z]=∑n=0∞Γ(a1+A1n)⋯Γ(ap+Apn)Γ(b1+B1n)⋯Γ(bq+Bqn)znn!.

Upon changing the normalisation

pΨq∗[(a1,A1)(a2,A2)…(ap,Ap)(b1,B1)(b2,B2)…(bq,Bq);z]=Γ(b1)⋯Γ(bq)Γ(a1)⋯Γ(ap)∑n=0∞Γ(a1+A1n)⋯Γ(ap+Apn)Γ(b1+B1n)⋯Γ(bq+Bqn)znn!

it becomes pFq(z) for A1...p = B1...q = 1.

The Fox–Wright function is a special case of the Fox H-function Template:Harv:

pΨq[(a1,A1)(a2,A2)…(ap,Ap)(b1,B1)(b2,B2)…(bq,Bq);z]=Hp,q+11,p[−z|(1−a1,A1)(1−a2,A2)…(1−ap,Ap)(0,1)(1−b1,B1)(1−b2,B2)…(1−bq,Bq)].

Wright function

The entire function Wλ,μ(z) is often called the Wright function.[1] It is the special case of 0Ψ1[…] of the Fox–Wright function. Its series representation is

Wλ,μ(z)=∑n=0∞znn!Γ(λn+μ),λ>−1.

This function is used extensively in fractional calculus. Recall that limλ→0Wλ,μ(z)=ez/Γ(μ). Hence, a non-zero λ with zero μ is the simplest nontrivial extension of the exponential function in such context.

Three properties were stated in Theorem 1 of Wright (1933)[2] and 18.1(30–32) of Erdelyi, Bateman Project, Vol 3 (1955)[3] (p. 212)

λzWλ,μ+λ(z)=Wλ,μ−1(z)+(1−μ)Wλ,μ(z)(a)ddzWλ,μ(z)=Wλ,μ+λ(z)(b)λzddzWλ,μ(z)=Wλ,μ−1(z)+(1−μ)Wλ,μ(z)(c)

Equation (a) is a recurrence formula. (b) and (c) provide two paths to reduce a derivative. And (c) can be derived from (a) and (b).

A special case of (c) is λ=−cα,μ=0. Replacing z with −xα, we have

xddxW−cα,0(−xα)=−1c[W−cα,−1(−xα)+W−cα,0(−xα)]

A special case of (a) is λ=−α,μ=1. Replacing z with −z, we have αzW−α,1−α(−z)=W−α,0(−z)

Two notations, Mα(z) and Fα(z), were used extensively in the literatures:

Mα(z)=W−α,1−α(−z),[1ex]⟹Fα(z)=W−α,0(−z)=αzMα(z).

M-Wright function

Mα(z) is known as the M-Wright function, entering as a probability density in a relevant class of self-similar stochastic processes, generally referred to as time-fractional diffusion processes.

Its properties were surveyed in Mainardi et al (2010).[4]

Its asymptotic expansion of Mα(z) for α>0 is Mα(rα)=A(α)r(α−1/2)/(1−α)e−B(α)r1/(1−α),r→∞, where A(α)=12π(1−α), B(α)=1−αα.

See also

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References

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