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By the definition of the gamma function: $$\Gamma(n)=\int_0^{\infty}{e^{-x}x^{n-1}dx}$$ Let $n = \frac{1}{2}$ and we get: $$\Gamma(\frac{1}{2})=\int_0^{\infty}{e^{-x}x^{-\frac{1}{2}}dx}$$ I tried to use integration by parts but treating $x^{-\frac{1}{2}}$ as $u$ or as $v$ both makes it needlessly complicated and doesn't seem to get me anywhere. I then tried the subtitution $u=e^{-x}$, where $x=-\ln(u)$ and $dx=-\frac{1}{u}du$ gives me this new integral: $$\int_1^0{\frac{u}{\sqrt{\ln(u)}}\cdot\frac{1}{u}du}=\int_1^0{-\frac{1}{\sqrt{-\ln(u)}}du}$$ However, I've not studied enough analysis to know if this integral is equivalent to $\int_0^1{-\frac{1}{\sqrt{-\ln(u)}}du}$ where I just swap the bounds like that, and even if I try to integrate it without particularly caring for the limits I get stuck. WolframAlpha gives the answer to this $u$ integral in terms of the imaginary error function, and it gives the answer to my original integral in terms of the very gamma function I started with! I know that $\Gamma(\frac{1}{2})=\sqrt{\pi}$ but I wanna figure out how we derive it!

tai
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