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[parent] evaluating the gamma function at 1/2 (Derivation)

In the entry on the gamma function it is mentioned that $\Gamma(1/2) = \sqrt{\pi}$ . In this entry we reduce the proof of this claim to the problem of computing the area under the bell curve. First note that by definition of the gamma function,

$\displaystyle \Gamma(1/2)$ $\displaystyle = \int_0^{\infty} e^{-x} x^{-1/2}\,dx$    
  $\displaystyle = 2\int_0^{\infty} e^{-x} \frac{1}{2\sqrt{x}}\,dx.$    

Performing the substitution $u = \sqrt{x}$ , we find that $du = \frac{1}{2\sqrt{x}}\,dx$ , so$$ \Gamma(1/2) = 2\int_0^{\infty} e^{-u^2}\,du = \int_{\mathbb{R}} e^{-u^2}\,du,$$ where the last equality holds because $e^{-u^2}$ is an even function. Since the area under the bell curve is $\sqrt{\pi}$ , it follows that $\Gamma(1/2) = \sqrt{\pi}$ .




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See Also: area under Gaussian curve, Laplace transform of power function


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Cross-references: even function, area under the bell curve, proof, gamma function
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This is version 1 of evaluating the gamma function at 1/2, born on 2007-04-19.
Object id is 9223, canonical name is EvaluatingTheGammaFunctionAt12.
Accessed 1572 times total.

Classification:
AMS MSC33B15 (Special functions :: Elementary classical functions :: Gamma, beta and polygamma functions)
 30D30 (Functions of a complex variable :: Entire and meromorphic functions, and related topics :: Meromorphic functions, general theory)

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