Proving the Gamma Function Integral for $\frac{1}{2}$

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Homework Help Overview

The discussion revolves around proving the integral representation of the Gamma function for the specific case of \(\Gamma\left(\frac{1}{2}\right)\), which is stated to equal \(\sqrt{\pi}\). Participants are exploring the relationship between different integral forms and attempting to connect the Gamma function with known results involving Gaussian integrals.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants are considering various methods to prove the statement, including the use of double integrals and substitutions. There is discussion about the differences in the forms of the integrals and the potential use of integration by parts. Some participants suggest using Laplace transforms as a method to approach the problem.

Discussion Status

The discussion is active, with participants sharing insights and hints. There is a recognition of the need for substitutions to connect the Gamma function to more familiar integral forms. While some methods have been proposed, there is no explicit consensus on a single approach, and participants are still exploring the problem.

Contextual Notes

Participants note the importance of correctly identifying the integral form of the Gamma function and the implications of fractional exponents in their reasoning. There is an acknowledgment of the constraints posed by the original problem and the need for careful manipulation of the integrals involved.

amcavoy
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I am wondering how the following statement holds true:

[tex]\Gamma\left(\frac{1}{2}\right)=\int_0^{\infty}e^{-x}x^{-\frac{1}{2}}\,dx=\sqrt{\pi}[/tex]

I know how to show that:

[tex]\int_0^{\infty}e^{-x^2}\,dx=\frac{\sqrt{\pi}}{2}[/tex]

But I can't seem to apply that method (converting to a double-integral) to the gamma function. Any ideas?

Thanks.
 
Last edited:
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[tex]\int_0^{+\infty} e^{-x^2} \, dx[/tex]

and

[tex]\int_0^{+\infty} e^{-x} x^{1/2} \, dx[/tex]

look a lot different... after all, one has [itex]-x^2[/itex] in the exponent, and the other has [itex]-x[/itex]...
 
Yeah, I just figured that since the results look similar, there may be a way to rearrange that gamma function to make it look like the other. --I guess not.

Would you suggest integration by parts to solve this? That is the only way I can think of, but it doesn't seem too promising because I can't get rid of that fractional exponent. Is there some sort of trick to this?

Thanks again.
 
Yeah, I just figured that since the results look similar, there may be a way to rearrange that gamma function to make it look like the other. --I guess not.
I never said you couldn't. :-p My post was a hint!
 
One method is to use Laplace Transforms:
First calculate:
[tex]\Gamma(x+1)=\int_0^{\infty}e^{-\beta}\beta^{x}d\beta[/tex]
let:
[tex]\beta=st[/tex]
[tex]\Gamma(x+1)=s^{x+1}\int_0^{\infty}e^{-st}t^x dt[/tex]
rearrange, equate to the Laplace transform of [itex]t^{x}[/itex] and then let x=-1/2. Can you finish it?
Also, shouldn't your integral have [itex]x^{-1/2}[/itex]?
 
yep

saltydog said:
One method is to use Laplace Transforms:
Also, shouldn't your integral have [itex]x^{-1/2}[/itex]?
Yes, it should, for [itex]\Gamma(z)=\int_{t=0}^{\infty}e^{-t}t^{z-1}dt[/itex] for [itex]z\in\mathbb{C}[/itex] such that [itex]\Re(z)>0[/itex].
Hence [itex]\Gamma\left(\frac{1}{2}\right)=\int_{t=0}^{\infty}e^{-t}t^{-\frac{1}{2}}dt[/itex], apply the substitution [itex]x=\sqrt t \Rightarrow dx=\frac{1}{2}t^{-\frac{1}{2}}dt[/itex] to get
[itex]\Gamma\left(\frac{1}{2}\right)=2\int_{t=0}^{\infty}e^{-x^{2}}dx = \sqrt\pi[/itex]
 
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Thanks a lot everyone for the help. I like that last substitution to change it into the form I am familiar with. Thank you :smile:
 
Do you understand why he thought to use that substitution in the first place? (Hint: my hint is why, though he probably knew it without my hint) Will you think to look at that next time you get stuck on an integral?
 
Hurkyl said:
Do you understand why he thought to use that substitution in the first place? (Hint: my hint is why, though he probably knew it without my hint) Will you think to look at that next time you get stuck on an integral?
Yes, thank you both very much.
 

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