Hadamard's gamma function

In mathematics, Hadamard's gamma function, named after Jacques Hadamard, is an extension of the factorial function, different from the classical gamma function (it is an instance of a pseudogamma function). This function, with its argument shifted down by 1, interpolates the factorial and extends it to real and complex numbers in a different way than Euler's gamma function. It is defined as:

H(x)={\frac {1}{\Gamma (1-x)}}\,{\dfrac {d}{dx}}\left\{\ln \left({\frac {\Gamma ({\frac {1}{2}}-{\frac {x}{2}})}{\Gamma (1-{\frac {x}{2}})}}\right)\right\},

where $Γ(x)$ denotes the classical gamma function. If $n$ is a positive integer, then:

H(n)=\Gamma (n)=(n-1)!

Properties

Unlike the classical gamma function, Hadamard's gamma function $H (x)$ is an entire function, i.e. it has no poles in its domain. It satisfies the functional equation

H(x+1)=xH(x)+{\frac {1}{\Gamma (1-x)}},

with the understanding that ${\tfrac {1}{\Gamma (1-x)}}$ is taken to be $0$ for positive integer values of $x$ .

Representations

Hadamard's gamma can also be expressed as

H(x)={\frac {\psi \left(1-{\frac {x}{2}}\right)-\psi \left({\frac {1}{2}}-{\frac {x}{2}}\right)}{2\Gamma (1-x)}}={\frac {\Phi \left(-1,1,-x\right)}{\Gamma (-x)}}

where $\Phi$ is the Lerch zeta function, and as

H(x)=\Gamma (x)\left[1+{\frac {\sin(\pi x)}{2\pi }}\left\{\psi \left({\dfrac {x}{2}}\right)-\psi \left({\dfrac {x+1}{2}}\right)\right\}\right],

where $ψ (x)$ denotes the digamma function.

References

Hadamard, M. J. (1894), Sur L'Expression Du Produit 1·2·3· · · · ·(n−1) Par Une Fonction Entière (PDF) (in French), Œuvres de Jacques Hadamard, Centre National de la Recherche Scientifiques, Paris, 1968
Srivastava, H. M.; Junesang, Choi (2012). Zeta and Q-Zeta Functions and Associated Series and Integrals. Elsevier insights. p. 124. ISBN 978-0-12-385218-2.
"Introduction to the Gamma Function". The Wolfram Functions Site. Wolfram Research, Inc. Retrieved 27 February 2016.

Properties

Representations

See also

References