# Reciprocal gamma function

In mathematics, the **reciprocal gamma function** is the function

where Γ(*z*) denotes the gamma function. Since the gamma function is meromorphic and nonzero everywhere in the complex plane, its reciprocal is an entire function. As an entire function, it is of order 1 (meaning that log log |1/Γ(*z*)| grows no faster than log |*z*|), but of infinite type (meaning that log |1/Γ(*z*)| grows faster than any multiple of |*z*|, since its growth is approximately proportional to |*z*| log |*z*| in the left-hand plane).

The reciprocal is sometimes used as a starting point for numerical computation of the gamma function, and a few software libraries provide it separately from the regular gamma function.

Karl Weierstrass called the reciprocal gamma function the "factorielle" and used it in his development of the Weierstrass factorization theorem.

## Infinite product expansion

Following from the infinite product definitions for the gamma function, due to Euler and Weierstrass respectively, we get the following infinite product expansion for the reciprocal gamma function:

where *γ* ≈ 0.577216... is the Euler–Mascheroni constant. These expansions are valid for all complex numbers *z*.

## Taylor series

Taylor series expansion around 0 gives

where *γ* is the Euler–Mascheroni constant. For *n* > 2, the coefficient *a*_{n} for the *z*^{n} term can be computed recursively as[1]

where *ζ*(*s*) is the Riemann zeta function. An integral representation was recently found by Fekih-Ahmed for these coefficients:[2]

For small values, these give the following values:

n |
a_{n} |
---|---|

1 | +1.0000000000000000000000000000000000000000 |

2 | +0.5772156649015328606065120900824024310422 |

3 | −0.6558780715202538810770195151453904812798 |

4 | −0.0420026350340952355290039348754298187114 |

5 | +0.1665386113822914895017007951021052357178 |

6 | −0.0421977345555443367482083012891873913017 |

7 | −0.0096219715278769735621149216723481989754 |

8 | +0.0072189432466630995423950103404465727099 |

9 | −0.0011651675918590651121139710840183886668 |

10 | −0.0002152416741149509728157299630536478065 |

11 | +0.0001280502823881161861531986263281643234 |

12 | −0.0000201348547807882386556893914210218184 |

13 | −0.0000012504934821426706573453594738330922 |

14 | +0.0000011330272319816958823741296203307449 |

15 | −0.0000002056338416977607103450154130020573 |

16 | +0.0000000061160951044814158178624986828553 |

17 | +0.0000000050020076444692229300556650480600 |

18 | −0.0000000011812745704870201445881265654365 |

19 | +0.0000000001043426711691100510491540332312 |

20 | +0.0000000000077822634399050712540499373114 |

21 | −0.0000000000036968056186422057081878158781 |

22 | +0.0000000000005100370287454475979015481323 |

23 | −0.0000000000000205832605356650678322242954 |

24 | −0.0000000000000053481225394230179823700173 |

25 | +0.0000000000000012267786282382607901588938 |

26 | −0.0000000000000001181259301697458769513765 |

27 | +0.0000000000000000011866922547516003325798 |

28 | +0.0000000000000000014123806553180317815558 |

29 | −0.0000000000000000002298745684435370206592 |

30 | +0.0000000000000000000171440632192733743338 |

An approximation for can be found in the above cited work of Fekih-Ahmed:

where , and is the minus first branch of the Lambert W function.

## Asymptotic expansion

As |*z*| goes to infinity at a constant arg(*z*) we have:

## Contour integral representation

An integral representation due to Hermann Hankel is

where *H* is the Hankel contour, that is, the path encircling 0 in the positive direction, beginning at and returning to positive infinity with respect for the branch cut along the positive real axis. According to Schmelzer & Trefethen, numerical evaluation of Hankel's integral is the basis of some of the best methods for computing the gamma function.

## Integral representations at the positive integers

For positive integers , there is an integral for the reciprocal factorial function given by [3]

- .

Similarly, for any real and we have the next integral for the reciprocal gamma function along the real axis in the form of [4]:

where the particular case when provides a corresponding relation for the reciprocal double factorial function, .

## Integral along the real axis

Integration of the reciprocal gamma function along the positive real axis gives the value

which is known as the Fransén–Robinson constant.

## References

- Wrench, J.W. (1968). Concerning two series for the gamma function.
*Mathematics of Computation*,*22*, 617–626. and

Wrench, J.W. (1973). Erratum: Concerning two series for the gamma function.*Mathematics of Computation*,*27*, 681–682. - Fekih-Ahmed, L. (2014). On the Power Series Expansion of the Reciprocal Gamma Function .
*HAL archives*, https://hal.archives-ouvertes.fr/hal-01029331v1 - Graham, Knuth, and Patashnik (1994).
*Concrete Mathematics*. Addison-Wesley. p. 566.CS1 maint: multiple names: authors list (link) - "Integral formula for ".
*Math Stack Exchange*.

- Thomas Schmelzer & Lloyd N. Trefethen, Computing the Gamma function using contour integrals and rational approximations
- Mette Lund, An integral for the reciprocal Gamma function
- Milton Abramowitz & Irene A. Stegun,
*Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables* - Eric W. Weisstein,
*Gamma Function*, MathWorld