Factorial
Using integration by parts ,
Î
(
z
)
=
â«
0
â
t
z
â
1
d
(
e
â
t
d
t
)
{\displaystyle \Gamma (z)=\int _{0}^{\infty }t^{z-1}d(e^{-t}dt)}
=
[
t
z
â
1
(
â
e
â
t
)
]
0
â
â
â«
0
â
(
z
â
1
)
t
(
z
â
2
)
(
â
e
â
t
)
d
t
.
{\displaystyle =\left[t^{z-1}(-e^{-t})\right]_{0}^{\infty }-\int _{0}^{\infty }(z-1)t^{(z-2)}(-e^{-t})dt.}
At
t
=
0
{\displaystyle t=0}
,
t
z
â
1
(
â
e
â
t
)
{\displaystyle t^{z-1}(-e^{-t})}
goes to 0. Using L'Hopital's rule , it's easy to show that
lim
t
â
â
t
z
â
1
e
t
=
0
{\displaystyle \lim _{t\to \infty }{\frac {t^{z-1}}{e^{t}}}=0}
.
So,
=
(
z
â
1
)
â«
0
â
t
(
z
â
1
)
â
1
e
â
t
d
t
{\displaystyle =(z-1)\int _{0}^{\infty }t^{(z-1)-1}e^{-t}dt}
=
(
z
â
1
)
Î
(
z
â
1
)
.
{\displaystyle =(z-1)\Gamma (z-1).}
Thus,
Î
(
z
)
=
(
z
â
1
)
Î
(
z
â
1
)
.
{\displaystyle \Gamma (z)=(z-1)\Gamma (z-1).}
Using this, and the fact that
Î
(
1
)
=
1
{\displaystyle \Gamma (1)=1}
, then we can get the factorial function. For
n
{\displaystyle n}
a positive integer,
Î
(
n
)
=
(
n
â
1
)
!
.
{\displaystyle \Gamma (n)=(n-1)!.}
z=1/2
For z=1/2,
Î
(
1
/
2
)
=
â«
0
â
t
â
1
/
2
e
â
t
d
t
{\displaystyle \Gamma (1/2)=\int _{0}^{\infty }t^{-1/2}e^{-t}dt}
Substituting
x
=
t
1
/
2
{\displaystyle x=t^{1/2}}
,
=
â«
0
â
(
1
x
)
e
â
x
2
(
2
x
d
x
)
{\displaystyle =\int _{0}^{\infty }({\frac {1}{x}})e^{-x^{2}}(2xdx)}
=
2
â«
0
â
e
â
x
2
d
x
{\displaystyle =2\int _{0}^{\infty }e^{-x^{2}}dx}
=
â«
â
â
â
e
â
x
2
d
x
{\displaystyle =\int _{-\infty }^{\infty }e^{-x^{2}}dx}
where in the last line we used the fact that
e
â
x
2
{\displaystyle e^{-x^{2}}}
is an even function. The integral is called the Gaussian integral and has a well known value of
Ï
{\displaystyle {\sqrt {\pi }}}
.
Thus,
Î
(
1
/
2
)
=
Ï
.
{\displaystyle \Gamma (1/2)={\sqrt {\pi }}.}