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5 Gamma FunctionProperties

§5.4 Special Values and Extrema

Contents
  1. §5.4(i) Gamma Function
  2. §5.4(ii) Psi Function
  3. §5.4(iii) Extrema

§5.4(i) Gamma Function

5.4.1
\Gamma\left(1\right)=1,
n!=\Gamma\left(n+1\right).

(The second line of Formula (5.4.2) also applies when n=-1.)

5.4.6 \Gamma\left(\tfrac{1}{2}\right)=\pi^{1/2}\\
=1.77245\;38509\;05516\;02729\;\dots,
5.4.7 \Gamma\left(\tfrac{1}{3}\right)=2.67893\;85347\;07747\;63365\;\dots,
5.4.8 \Gamma\left(\tfrac{2}{3}\right)=1.35411\;79394\;26400\;41694\;\dots,
5.4.9 \Gamma\left(\tfrac{1}{4}\right)=3.62560\;99082\;21908\;31193\;\dots,
5.4.10 \Gamma\left(\tfrac{3}{4}\right)=1.22541\;67024\;65177\;64512\;\dots.
5.4.11 \Gamma'\left(1\right)=-\gamma.

§5.4(ii) Psi Function

5.4.12
\psi\left(1\right)=-\gamma,
\psi'\left(1\right)=\tfrac{1}{6}\pi^{2},

For higher derivatives of \psi\left(z\right) at z=1 and z=\frac{1}{2}, see §5.15.

5.4.14 \psi\left(n+1\right)=\sum_{k=1}^{n}\frac{1}{k}-\gamma,
5.4.15 \psi\left(n+\tfrac{1}{2}\right)=-\gamma-2\ln 2+2\left(1+\tfrac{1}{3}+\dots+%
\tfrac{1}{2n-1}\right),n=1,2,\dots.

If p,q are integers with 0<p<q, then

§5.4(iii) Extrema

Table 5.4.1: \Gamma'\left(x_{n}\right)=\psi\left(x_{n}\right)=0.
n x_{n} \Gamma\left(x_{n}\right)
0 1.46163 21449 68362 34126 0.88560 31944 10888 70028
1 −0.50408 30082 64455 40926 −3.54464 36111 55005 08912
2 −1.57349 84731 62390 45878 2.30240 72583 39680 13582
3 −2.61072 08684 44144 65000 −0.88813 63584 01241 92010
4 −3.63529 33664 36901 09784 0.24512 75398 34366 25044
5 −4.65323 77617 43142 44171 −0.05277 96395 87319 40076
6 −5.66716 24415 56885 53585 0.00932 45944 82614 85052
7 −6.67841 82130 73426 74283 −0.00139 73966 08949 76730
8 −7.68778 83250 31626 03744 0.00018 18784 44909 40419
9 −8.69576 41638 16401 26649 −0.00002 09252 90446 52667
10 −9.70267 25400 01863 73608 0.00000 21574 16104 52285

Compare Figure 5.3.1.

As n\to\infty,

5.4.20 x_{n}=-n+\frac{1}{\pi}\operatorname{arctan}\left(\frac{\pi}{\ln n}\right)+O%
\left(\frac{1}{n(\ln n)^{2}}\right).

For error bounds for this estimate see Walker (2007, Theorem 5).