Difference between revisions of "Gamma function"

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<math>\Gamma(z) = \int_{0}^{\infty}t^{z-1}e^{-t}dt</math>
 
<math>\Gamma(z) = \int_{0}^{\infty}t^{z-1}e^{-t}dt</math>
  
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== Relations and values ==
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===Factorial===
 
Using [[Integration_by_parts|integration by parts]],
 
Using [[Integration_by_parts|integration by parts]],
  
 
<math>\Gamma(z) = \int_{0}^{\infty}t^{z-1}d(e^{-t}dt)</math>
 
<math>\Gamma(z) = \int_{0}^{\infty}t^{z-1}d(e^{-t}dt)</math>
−
:<math>= \left[t^{z-1}(-e^{-t}) \right]_0^{\infty}- \int_{0}^{\infty}(z-1)t^{(z-2)}(-e^{-t})dt</math>
+
:<math>= \left[t^{z-1}(-e^{-t}) \right]_0^{\infty}- \int_{0}^{\infty}(z-1)t^{(z-2)}(-e^{-t})dt.</math>
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At <math>t=0</math>, <math>t^{z-1}(-e^{-t})</math> goes to 0.  Using [[L'Hopital's rule]], it's easy to show that <math>\lim_{t\to \infty} \frac{t^{z-1}}{e^{t}} = 0</math>.
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So,
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:<math>=(z-1) \int_{0}^{\infty}t^{(z-1)-1}e^{-t}dt</math>
 
:<math>=(z-1) \int_{0}^{\infty}t^{(z-1)-1}e^{-t}dt</math>
 
:<math>=(z-1) \Gamma(z-1).</math>
 
:<math>=(z-1) \Gamma(z-1).</math>
 
Thus,  
 
Thus,  
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:<math> \Gamma (z) = (z-1) \Gamma(z-1)</math>
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:<math> \Gamma (z) = (z-1) \Gamma(z-1).</math>
  
 
Using this, and the the fact that <math>\Gamma(0)=1</math>, then we can get the [[Factorial|factorial]]. For <math>n</math> a positive integer,
 
Using this, and the the fact that <math>\Gamma(0)=1</math>, then we can get the [[Factorial|factorial]]. For <math>n</math> a positive integer,
  
 
:<math> \Gamma(n) = (n-1)!. </math>
 
:<math> \Gamma(n) = (n-1)!. </math>
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===z=1/2===
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For z=1/2,
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:<math> \Gamma(1/2) = \int_{0}^{\infty}t^{-1/2}e^{-t}dt </math>
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Substituting <math>x=t^{1/2}</math>,
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 +
:<math>=\int_{0}^{\infty} (\frac{1}{x}) e^{-x^2} (2xdx )</math>
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:<math>=2 \int_{0}^{\infty} e^{-x^2}dx </math>
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:<math>= \int_{-\infty}^{\infty} e^{-x^2}dx </math>
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where in the last line we used the fact that the function <math>e^{-x^2}</math> is even. The integral is called the Gaussian integral and has a well known value of <math>\sqrt\pi</math>.
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Thus,
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:<math> \Gamma(1/2) = \sqrt\pi. </math>
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 +
  
 
[[category:mathematics]]
 
[[category:mathematics]]

Revision as of 21:05, June 5, 2010

The Gamma funciton is defined as

Relations and values

Factorial

Using integration by parts,

At , goes to 0. Using L'Hopital's rule, it's easy to show that .

So,

Thus,

Using this, and the the fact that , then we can get the factorial. For a positive integer,

z=1/2

For z=1/2,

Substituting ,

where in the last line we used the fact that the function is even. The integral is called the Gaussian integral and has a well known value of .

Thus,