# Particular values of the Gamma function

The gamma function is an important special function in mathematics. Its particular values can be expressed in closed form for integer and half-integer arguments, but no simple expressions are known for the values at rational points in general. Other fractional arguments can be approximated through efficient infinite products, infinite series, and recurrence relations.

## Integers and half-integers

For positive integer arguments, the gamma function coincides with the factorial, that is,

${\displaystyle \Gamma (n)=(n-1)!\qquad n\in \mathbb {N} _{0},}$

and hence

{\displaystyle {\begin{aligned}\Gamma (1)&=1,\\\Gamma (2)&=1,\\\Gamma (3)&=2,\\\Gamma (4)&=6,\\\Gamma (5)&=24.\end{aligned}}}

For non-positive integers, the gamma function is not defined.

For positive half-integers, the function values are given exactly by

${\displaystyle \Gamma \left({\tfrac {n}{2}}\right)={\sqrt {\pi }}{\frac {(n-2)!!}{2^{\frac {n-1}{2}}}}\,,}$

or equivalently, for non-negative integer values of n:

{\displaystyle {\begin{aligned}\Gamma \left({\tfrac {1}{2}}+n\right)&={\frac {(2n-1)!!}{2^{n}}}\,{\sqrt {\pi }}={\frac {(2n)!}{4^{n}n!}}{\sqrt {\pi }}\\\Gamma \left({\tfrac {1}{2}}-n\right)&={\frac {(-2)^{n}}{(2n-1)!!}}\,{\sqrt {\pi }}={\frac {(-4)^{n}n!}{(2n)!}}{\sqrt {\pi }}\end{aligned}}}

where n!! denotes the double factorial. In particular,

 ${\displaystyle \Gamma \left({\tfrac {1}{2}}\right)\,}$ ${\displaystyle ={\sqrt {\pi }}\,}$ ${\displaystyle \approx 1.772\,453\,850\,905\,516\,0273\,,}$ ${\displaystyle \Gamma \left({\tfrac {3}{2}}\right)\,}$ ${\displaystyle ={\tfrac {1}{2}}{\sqrt {\pi }}\,}$ ${\displaystyle \approx 0.886\,226\,925\,452\,758\,0137\,,}$ ${\displaystyle \Gamma \left({\tfrac {5}{2}}\right)\,}$ ${\displaystyle ={\tfrac {3}{4}}{\sqrt {\pi }}\,}$ ${\displaystyle \approx 1.329\,340\,388\,179\,137\,0205\,,}$ ${\displaystyle \Gamma \left({\tfrac {7}{2}}\right)\,}$ ${\displaystyle ={\tfrac {15}{8}}{\sqrt {\pi }}\,}$ ${\displaystyle \approx 3.323\,350\,970\,447\,842\,5512\,,}$

and by means of the reflection formula,

 ${\displaystyle \Gamma \left(-{\tfrac {1}{2}}\right)\,}$ ${\displaystyle =-2{\sqrt {\pi }}\,}$ ${\displaystyle \approx -3.544\,907\,701\,811\,032\,0546\,,}$ ${\displaystyle \Gamma \left(-{\tfrac {3}{2}}\right)\,}$ ${\displaystyle ={\tfrac {4}{3}}{\sqrt {\pi }}\,}$ ${\displaystyle \approx 2.363\,271\,801\,207\,354\,7031\,,}$ ${\displaystyle \Gamma \left(-{\tfrac {5}{2}}\right)\,}$ ${\displaystyle =-{\tfrac {8}{15}}{\sqrt {\pi }}\,}$ ${\displaystyle \approx -0.945\,308\,720\,482\,941\,8812\,,}$

## General rational arguments

In analogy with the half-integer formula,

{\displaystyle {\begin{aligned}\Gamma \left(n+{\tfrac {1}{3}}\right)&=\Gamma \left({\tfrac {1}{3}}\right){\frac {(3n-2)!!!}{3^{n}}}\\\Gamma \left(n+{\tfrac {1}{4}}\right)&=\Gamma \left({\tfrac {1}{4}}\right){\frac {(4n-3)!!!!}{4^{n}}}\\\Gamma \left(n+{\tfrac {1}{p}}\right)&=\Gamma \left({\tfrac {1}{p}}\right){\frac {{\big (}pn-(p-1){\big )}!^{(p)}}{p^{n}}}\end{aligned}}}

where n!(p) denotes the pth multifactorial of n. Numerically,

${\displaystyle \Gamma \left({\tfrac {1}{3}}\right)\approx 2.678\,938\,534\,707\,747\,6337}$
${\displaystyle \Gamma \left({\tfrac {1}{4}}\right)\approx 3.625\,609\,908\,221\,908\,3119}$
${\displaystyle \Gamma \left({\tfrac {1}{5}}\right)\approx 4.590\,843\,711\,998\,803\,0532}$
${\displaystyle \Gamma \left({\tfrac {1}{6}}\right)\approx 5.566\,316\,001\,780\,235\,2043}$
${\displaystyle \Gamma \left({\tfrac {1}{7}}\right)\approx 6.548\,062\,940\,247\,824\,4377}$
${\displaystyle \Gamma \left({\tfrac {1}{8}}\right)\approx 7.533\,941\,598\,797\,611\,9047}$ .

It is unknown whether these constants are transcendental in general, but Γ(1/3) and Γ(1/4) were shown to be transcendental by G. V. Chudnovsky. Γ(1/4) / 4π has also long been known to be transcendental, and Yuri Nesterenko proved in 1996 that Γ(1/4), π, and eπ are algebraically independent.

The number Γ(1/4) is related to the lemniscate constant S by

${\displaystyle \Gamma \left({\tfrac {1}{4}}\right)={\sqrt {{\sqrt {2\pi }}S}},}$

and it has been conjectured by Gramain that

${\displaystyle \Gamma \left({\tfrac {1}{4}}\right)={\sqrt[{4}]{4\pi ^{3}e^{2\gamma -\mathrm {\delta } +1}}}}$

where δ is the Masser–Gramain constant , although numerical work by Melquiond et al. indicates that this conjecture is false.[1]

Borwein and Zucker have found that Γ(n/24) can be expressed algebraically in terms of π, K(k(1)), K(k(2)), K(k(3)), and K(k(6)) where K(k(N)) is a complete elliptic integral of the first kind. This permits efficiently approximating the gamma function of rational arguments to high precision using quadratically convergent arithmetic-geometric mean iterations. No similar relations are known for Γ(1/5) or other denominators.

In particular, Γ(1/4) is given by

${\displaystyle \Gamma \left({\tfrac {1}{4}}\right)={\sqrt {\frac {(2\pi )^{\frac {3}{2}}}{AGM\left({\sqrt {2}},1\right)}}}}$, where AGM() is the arithmetic–geometric mean.

and Γ(1/6) is given by[2]

${\displaystyle \Gamma \left({\frac {1}{6}}\right)={\frac {2^{\frac {14}{9}}\cdot 3^{\frac {1}{3}}\cdot \pi ^{\frac {5}{6}}}{AGM\left(1+{\sqrt {3}},{\sqrt {8}}\right)^{\frac {2}{3}}}}.}$

Other formulas include the infinite products

${\displaystyle \Gamma \left({\tfrac {1}{4}}\right)=(2\pi )^{\frac {3}{4}}\prod _{k=1}^{\infty }\tanh \left({\frac {\pi k}{2}}\right)}$

and

${\displaystyle \Gamma \left({\tfrac {1}{4}}\right)=A^{3}e^{-{\frac {G}{\pi }}}{\sqrt {\pi }}2^{\frac {1}{6}}\prod _{k=1}^{\infty }\left(1-{\frac {1}{2k}}\right)^{k(-1)^{k}}}$

where A is the Glaisher-Kinkelin constant and G is Catalan's constant.

C. H. Brown derived rapidly converging infinite series for particular values of the gamma function:[3]

{\displaystyle {\begin{aligned}{\frac {\left(\Gamma \left({\tfrac {1}{3}}\right)\right)^{6}}{12\pi ^{4}}}&={\frac {1}{{\sqrt {1}}0}}\sum _{k=0}^{\infty }{\frac {(6k)!(-1)^{k}}{(k!)^{3}(3k)!3^{k}160^{3k}}}\\{\frac {\left(\Gamma \left({\tfrac {1}{4}}\right)\right)^{4}}{128\pi ^{3}}}&={\frac {1}{\sqrt {u}}}\sum _{k=0}^{\infty }{\frac {(6k)!(2w)^{k}}{(k!)^{3}(3k)!6486^{3k}}}\end{aligned}}}

where,

{\displaystyle {\begin{aligned}u&=273+180{\sqrt {2}}\\v&=1+{\sqrt {2}}\\w&=-761\,354\,780+538\,359\,129{\sqrt {2}}={\frac {6486^{3}}{2\left(uv^{2}{\sqrt {2}}\right)^{3}}}\end{aligned}}}

equivalently,

${\displaystyle {\frac {\left(\Gamma \left({\tfrac {1}{4}}\right)\right)^{4}}{128\pi ^{3}}}={\frac {1}{\sqrt {u}}}\sum _{k=0}^{\infty }{\frac {(6k)!}{(k!)^{3}(3k)!}}{\frac {1}{(uv^{2}{\sqrt {2}})^{3k}}}.}$

The following two representations for Γ(3/4) were given by I. Mező[4]

${\displaystyle {\sqrt {\frac {\pi {\sqrt {e^{\pi }}}}{2}}}{\frac {1}{\Gamma ^{2}\left({\frac {3}{4}}\right)}}=i\sum _{k=-\infty }^{\infty }e^{\pi (k-2k^{2})}\vartheta _{1}\left({\frac {i\pi }{2}}(2k-1),e^{-\pi }\right),}$

and

${\displaystyle {\sqrt {\frac {\pi }{2}}}{\frac {1}{\Gamma ^{2}\left({\frac {3}{4}}\right)}}=\sum _{k=-\infty }^{\infty }{\frac {\vartheta _{4}(ik\pi ,e^{-\pi })}{e^{2\pi k^{2}}}},}$

where ϑ1 and ϑ4 are two of the Jacobi theta functions.

## Products

Some product identities include:

${\displaystyle \prod _{r=1}^{2}\Gamma \left({\tfrac {r}{3}}\right)={\frac {2\pi }{\sqrt {3}}}\approx 3.627\,598\,728\,468\,435\,7012}$
${\displaystyle \prod _{r=1}^{3}\Gamma \left({\tfrac {r}{4}}\right)={\sqrt {2\pi ^{3}}}\approx 7.874\,804\,972\,861\,209\,8721}$
${\displaystyle \prod _{r=1}^{4}\Gamma \left({\tfrac {r}{5}}\right)={\frac {4\pi ^{2}}{\sqrt {5}}}\approx 17.655\,285\,081\,493\,524\,2483}$
${\displaystyle \prod _{r=1}^{5}\Gamma \left({\tfrac {r}{6}}\right)=4{\sqrt {\frac {\pi ^{5}}{3}}}\approx 40.399\,319\,122\,003\,790\,0785}$
${\displaystyle \prod _{r=1}^{6}\Gamma \left({\tfrac {r}{7}}\right)={\frac {8\pi ^{3}}{\sqrt {7}}}\approx 93.754\,168\,203\,582\,503\,7970}$
${\displaystyle \prod _{r=1}^{7}\Gamma \left({\tfrac {r}{8}}\right)=4{\sqrt {\pi ^{7}}}\approx 219.828\,778\,016\,957\,263\,6207}$

In general:

${\displaystyle \prod _{r=1}^{n}\Gamma \left({\tfrac {r}{n+1}}\right)={\sqrt {\frac {(2\pi )^{n}}{n+1}}}}$
${\displaystyle {\frac {\Gamma \left({\tfrac {1}{5}}\right)\Gamma \left({\tfrac {4}{15}}\right)}{\Gamma \left({\tfrac {1}{3}}\right)\Gamma \left({\tfrac {2}{15}}\right)}}={\frac {{\sqrt {2}}\,{\sqrt[{20}]{3}}}{{\sqrt[{6}]{5}}\,{\sqrt[{4}]{5-{\frac {7}{\sqrt {5}}}+{\sqrt {6-{\frac {6}{\sqrt {5}}}}}}}}}}$[5]
${\displaystyle {\frac {\Gamma \left({\tfrac {1}{20}}\right)\Gamma \left({\tfrac {9}{20}}\right)}{\Gamma \left({\tfrac {3}{20}}\right)\Gamma \left({\tfrac {7}{20}}\right)}}={\frac {{\sqrt[{4}]{5}}\left(1+{\sqrt {5}}\right)}{2}}}$[6]

From those products can be deduced other values, for example, from the former equations for ${\displaystyle \prod _{r=1}^{3}\Gamma \left({\tfrac {r}{4}}\right)}$, ${\displaystyle \Gamma \left({\tfrac {1}{4}}\right)}$ and ${\displaystyle \Gamma \left({\tfrac {2}{4}}\right)}$, can be deduced:

${\displaystyle \Gamma \left({\tfrac {3}{4}}\right)=\left({\tfrac {\pi }{2}}\right)^{\tfrac {1}{4}}{AGM\left({\sqrt {2}},1\right)}^{\tfrac {1}{2}}}$

## Imaginary and complex arguments

The gamma function on the imaginary unit i = −1 returns , :

${\displaystyle \Gamma (i)=(-1+i)!\approx -0.1549-0.4980i.}$

It may also be given in terms of the Barnes G-function:

${\displaystyle \Gamma (i)={\frac {G(1+i)}{G(i)}}=e^{-\log G(i)+\log G(1+i)}.}$

The gamma function with complex arguments returns

${\displaystyle \Gamma (1+i)=i\Gamma (i)\approx 0.498-0.155i}$
${\displaystyle \Gamma (1-i)=-i\Gamma (-i)\approx 0.498+0.155i}$
${\displaystyle \Gamma ({\tfrac {1}{2}}+{\tfrac {1}{2}}i)\approx 0.818\,163\,9995-0.763\,313\,8287\,i}$
${\displaystyle \Gamma ({\tfrac {1}{2}}-{\tfrac {1}{2}}i)\approx 0.818\,163\,9995+0.763\,313\,8287\,i}$
${\displaystyle \Gamma (5+3i)\approx 0.016\,041\,8827-9.433\,293\,2898\,i}$
${\displaystyle \Gamma (5-3i)\approx 0.016\,041\,8827+9.433\,293\,2897\,i.}$

## Other constants

The gamma function has a local minimum on the positive real axis

${\displaystyle x_{\mathrm {min} }=1.461\,632\,144\,968\,362\,341\,262\ldots \,}$

with the value

${\displaystyle \Gamma \left(x_{\mathrm {min} }\right)=0.885\,603\,194\,410\,888\ldots \,}$ .

Integrating the reciprocal gamma function along the positive real axis also gives the Fransén–Robinson constant.

On the negative real axis, the first local maxima and minima (zeros of the digamma function) are:

Approximate local extrema of Γ(x)
x Γ(x) OEIS
−0.5040830082644554092582693045 −3.5446436111550050891219639933
−1.5734984731623904587782860437 2.3024072583396801358235820396
−2.6107208684441446500015377157 −0.8881363584012419200955280294
−3.6352933664369010978391815669 0.2451275398343662504382300889
−4.6532377617431424417145981511 −0.0527796395873194007604835708
−5.6671624415568855358494741745 0.0093245944826148505217119238
−6.6784182130734267428298558886 −0.0013973966089497673013074887
−7.6877883250316260374400988918 0.0001818784449094041881014174
−8.6957641638164012664887761608 −0.0000209252904465266687536973
−9.7026725400018637360844267649 0.0000021574161045228505405031

The inverse of the gamma function gives out this interesting result :

${\displaystyle \int \limits _{1}^{\infty }{\frac {1}{\Gamma (x)}}dx\simeq 2.2665345076\dots }$ also equivalent to ${\displaystyle \int \limits _{0}^{\infty }{\frac {1}{\Gamma (x+1)}}dx=\int \limits _{0}^{\infty }{\frac {1}{x!}}dx\simeq 2.2665345076\dots }$