dstefan
06-05-2008, 11:33 PM
Chapter 2, Problem 2:
Let f : (0, \infty) \to {\mathbb R} denote the Gamma function, i.e., let
f(\alpha) ~=~ \int_0^{\infty} x^{\alpha-1} ~e^{-x} ~dx.
(i) Show that f(\alpha) is well defined for any \alpha > 0.
(ii) Prove, using integration by parts, that f(\alpha) = (\alpha-1) ~f(\alpha-1) for any \alpha > 1. Show that f(1) = 1 and conclude that, for any positive integer n, f(n) = (n-1)!
Solution:
(i) We must show that both
\int_0^1 x^{\alpha-1} ~e^{-x} ~dx ~=~ \lim_{t \searrow 0} \int_t^1 x^{\alpha-1} ~e^{-x} ~dx
and
\int_1^{\infty} x^{\alpha-1} ~e^{-x} ~dx ~=~ \lim_{t \to \infty} \int_1^t x^{\alpha-1} ~e^{-x} ~dx
exist and are finite.
(ii) It is easy to see that
f(1)~=~ \int_0^{\infty} e^{-x} ~dx~=~ \lim_{t \to \infty} \int_0^t e^{-x} ~dx~=~ \lim_{t \to \infty} \left( 1 - e^{-t} \right)~=~ 1.
By integration by parts, and, for now, by abuse of notation, we find that
f(\alpha) = \int_0^{\infty} x^{\alpha-1} ~e^{-x} ~dx = - x^{\alpha-1} ~e^{-x} \left|_{x=0}^{x \to \infty} \right. ~+~ (\alpha-1) ~\int_0^{\infty} x^{\alpha-2} ~e^{-x} ~dx = (\alpha-1) f(\alpha-1),
since
\lim_{x \searrow 0} x^{\alpha-1} ~e^{-x} = \lim_{x \searrow 0} x^{\alpha-1} ~=~ 0
for \alpha > 1 and
\lim_{x \to \infty} x^{\alpha-1} ~e^{-x} = \lim_{x \to \infty} \frac{x^{\alpha-1}}{e^x} = 0
For any positive integer n > 1, we find that f(n) = (n-1) f(n-1). Since f(1) = 1, it follows by induction that f(n) = (n-1)!
Let f : (0, \infty) \to {\mathbb R} denote the Gamma function, i.e., let
f(\alpha) ~=~ \int_0^{\infty} x^{\alpha-1} ~e^{-x} ~dx.
(i) Show that f(\alpha) is well defined for any \alpha > 0.
(ii) Prove, using integration by parts, that f(\alpha) = (\alpha-1) ~f(\alpha-1) for any \alpha > 1. Show that f(1) = 1 and conclude that, for any positive integer n, f(n) = (n-1)!
Solution:
(i) We must show that both
\int_0^1 x^{\alpha-1} ~e^{-x} ~dx ~=~ \lim_{t \searrow 0} \int_t^1 x^{\alpha-1} ~e^{-x} ~dx
and
\int_1^{\infty} x^{\alpha-1} ~e^{-x} ~dx ~=~ \lim_{t \to \infty} \int_1^t x^{\alpha-1} ~e^{-x} ~dx
exist and are finite.
(ii) It is easy to see that
f(1)~=~ \int_0^{\infty} e^{-x} ~dx~=~ \lim_{t \to \infty} \int_0^t e^{-x} ~dx~=~ \lim_{t \to \infty} \left( 1 - e^{-t} \right)~=~ 1.
By integration by parts, and, for now, by abuse of notation, we find that
f(\alpha) = \int_0^{\infty} x^{\alpha-1} ~e^{-x} ~dx = - x^{\alpha-1} ~e^{-x} \left|_{x=0}^{x \to \infty} \right. ~+~ (\alpha-1) ~\int_0^{\infty} x^{\alpha-2} ~e^{-x} ~dx = (\alpha-1) f(\alpha-1),
since
\lim_{x \searrow 0} x^{\alpha-1} ~e^{-x} = \lim_{x \searrow 0} x^{\alpha-1} ~=~ 0
for \alpha > 1 and
\lim_{x \to \infty} x^{\alpha-1} ~e^{-x} = \lim_{x \to \infty} \frac{x^{\alpha-1}}{e^x} = 0
For any positive integer n > 1, we find that f(n) = (n-1) f(n-1). Since f(1) = 1, it follows by induction that f(n) = (n-1)!