Verification of $(-frac{1}{2})!$Proving $int_{0}^{infty} mathrm{e}^{-x^2} dx = frac{sqrt pi}{2}$A difficult...

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Verification of $(-frac{1}{2})!$


Proving $int_{0}^{infty} mathrm{e}^{-x^2} dx = frac{sqrt pi}{2}$A difficult integral $int_0^infty mathrm{d}tfrac{1}{t}frac{1}{t-s-mathrm{i}epsilon}frac{1}{X}lnfrac{1-X}{1+X} $Substitution of Differentials without IntegralsHow to find $int frac{e^{-x^2}}{x^2 + 1} dx$?Evaluate $lim_{n to infty} int_0^1 frac{dx}{x^n + 1}$Strange Limit in Proof of the Fresnel IntegralHow to transform $- int_{0}^{infty} ln(1 - x e^{-x}) mathrm{d}x$ into $sum_{n=1}^{infty} frac{n!}{n^{n+2}}$?$ int_2^{infty}frac{1}{xsqrt{x^2-4}}dx$ convergence verificationdivergence of $sum_{n=3}^infty frac{sqrt{n}+2}{n-2}$ verification/ alternative methodA naive change of integration limit













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$begingroup$


I was working on a proof for $(-frac{1}{2})!$ and my issue was with converting my bounds from variable to variable. As you will see, I kept my bounds in terms of $t$ throughout the calculation, but switched the bounds as one of my final steps.



$$int_{t=0}^{t=infty} t^{n}e^{-t}dt$$



$$int_{t=0}^{t=infty} t^{-frac{1}{2}}e^{-t}dt$$
$u=t^{-frac{1}{2}}$ $rightarrow$ $t=u^{-2},dt=-2u^{-3}du$
$$int_{t=0}^{t=infty} ue^{-u^{-2}}cdot -2u^{-2}u^{-1} du$$
$u^{-2}=v^{2}rightarrow v=u^{-1},u=v^{-1}rightarrow dv=-u^{-2}$
$$2int_{t=0}^{t=infty} e^{-v^{2}} dv$$
Recall: $$int_{0}^{infty} e^{-x^{2}} dx = frac{sqrt{pi}}{2}$$
Now for the bounds. I have kept them in terms of $t$, and now, after all of the substitutions, I can relate $v$ to $t$. I have $u=t^{-frac{1}{2}}$, and I also have $u=v^{-1}$, which gives me $v^{-1}=t^{-frac{1}{2}}$ which means that $v=t^{frac{1}{2}}$. When $t=0$, I get: $v=0^{frac{1}{2}}=0$, and when $t=infty$, I get: $v=infty^{frac{1}{2}}=infty$, so my bounds stay the same.
Finally: $$2int_{0}^{infty} e^{-v^{2}} dv=sqrt{pi}$$










share|cite|improve this question









$endgroup$








  • 1




    $begingroup$
    What's the problem? Seems fine.
    $endgroup$
    – Hobbyist
    Mar 19 at 14:42










  • $begingroup$
    Is my method for determining the bounds in terms of $t$ to $v$ ok?
    $endgroup$
    – ItIsLastThursday
    Mar 19 at 14:45






  • 1




    $begingroup$
    That's pretty much the standard proof that $Gamma(tfrac12)=sqrtpi$ that you normally see. There's no problem with your limits.
    $endgroup$
    – Hobbyist
    Mar 19 at 14:46










  • $begingroup$
    What do you try to achieve with the first substitution? Don't you think $t=v^2$ is enough?
    $endgroup$
    – Diger
    Mar 19 at 14:46










  • $begingroup$
    I realized that afterwards, but whatever.
    $endgroup$
    – ItIsLastThursday
    Mar 19 at 14:47
















0












$begingroup$


I was working on a proof for $(-frac{1}{2})!$ and my issue was with converting my bounds from variable to variable. As you will see, I kept my bounds in terms of $t$ throughout the calculation, but switched the bounds as one of my final steps.



$$int_{t=0}^{t=infty} t^{n}e^{-t}dt$$



$$int_{t=0}^{t=infty} t^{-frac{1}{2}}e^{-t}dt$$
$u=t^{-frac{1}{2}}$ $rightarrow$ $t=u^{-2},dt=-2u^{-3}du$
$$int_{t=0}^{t=infty} ue^{-u^{-2}}cdot -2u^{-2}u^{-1} du$$
$u^{-2}=v^{2}rightarrow v=u^{-1},u=v^{-1}rightarrow dv=-u^{-2}$
$$2int_{t=0}^{t=infty} e^{-v^{2}} dv$$
Recall: $$int_{0}^{infty} e^{-x^{2}} dx = frac{sqrt{pi}}{2}$$
Now for the bounds. I have kept them in terms of $t$, and now, after all of the substitutions, I can relate $v$ to $t$. I have $u=t^{-frac{1}{2}}$, and I also have $u=v^{-1}$, which gives me $v^{-1}=t^{-frac{1}{2}}$ which means that $v=t^{frac{1}{2}}$. When $t=0$, I get: $v=0^{frac{1}{2}}=0$, and when $t=infty$, I get: $v=infty^{frac{1}{2}}=infty$, so my bounds stay the same.
Finally: $$2int_{0}^{infty} e^{-v^{2}} dv=sqrt{pi}$$










share|cite|improve this question









$endgroup$








  • 1




    $begingroup$
    What's the problem? Seems fine.
    $endgroup$
    – Hobbyist
    Mar 19 at 14:42










  • $begingroup$
    Is my method for determining the bounds in terms of $t$ to $v$ ok?
    $endgroup$
    – ItIsLastThursday
    Mar 19 at 14:45






  • 1




    $begingroup$
    That's pretty much the standard proof that $Gamma(tfrac12)=sqrtpi$ that you normally see. There's no problem with your limits.
    $endgroup$
    – Hobbyist
    Mar 19 at 14:46










  • $begingroup$
    What do you try to achieve with the first substitution? Don't you think $t=v^2$ is enough?
    $endgroup$
    – Diger
    Mar 19 at 14:46










  • $begingroup$
    I realized that afterwards, but whatever.
    $endgroup$
    – ItIsLastThursday
    Mar 19 at 14:47














0












0








0





$begingroup$


I was working on a proof for $(-frac{1}{2})!$ and my issue was with converting my bounds from variable to variable. As you will see, I kept my bounds in terms of $t$ throughout the calculation, but switched the bounds as one of my final steps.



$$int_{t=0}^{t=infty} t^{n}e^{-t}dt$$



$$int_{t=0}^{t=infty} t^{-frac{1}{2}}e^{-t}dt$$
$u=t^{-frac{1}{2}}$ $rightarrow$ $t=u^{-2},dt=-2u^{-3}du$
$$int_{t=0}^{t=infty} ue^{-u^{-2}}cdot -2u^{-2}u^{-1} du$$
$u^{-2}=v^{2}rightarrow v=u^{-1},u=v^{-1}rightarrow dv=-u^{-2}$
$$2int_{t=0}^{t=infty} e^{-v^{2}} dv$$
Recall: $$int_{0}^{infty} e^{-x^{2}} dx = frac{sqrt{pi}}{2}$$
Now for the bounds. I have kept them in terms of $t$, and now, after all of the substitutions, I can relate $v$ to $t$. I have $u=t^{-frac{1}{2}}$, and I also have $u=v^{-1}$, which gives me $v^{-1}=t^{-frac{1}{2}}$ which means that $v=t^{frac{1}{2}}$. When $t=0$, I get: $v=0^{frac{1}{2}}=0$, and when $t=infty$, I get: $v=infty^{frac{1}{2}}=infty$, so my bounds stay the same.
Finally: $$2int_{0}^{infty} e^{-v^{2}} dv=sqrt{pi}$$










share|cite|improve this question









$endgroup$




I was working on a proof for $(-frac{1}{2})!$ and my issue was with converting my bounds from variable to variable. As you will see, I kept my bounds in terms of $t$ throughout the calculation, but switched the bounds as one of my final steps.



$$int_{t=0}^{t=infty} t^{n}e^{-t}dt$$



$$int_{t=0}^{t=infty} t^{-frac{1}{2}}e^{-t}dt$$
$u=t^{-frac{1}{2}}$ $rightarrow$ $t=u^{-2},dt=-2u^{-3}du$
$$int_{t=0}^{t=infty} ue^{-u^{-2}}cdot -2u^{-2}u^{-1} du$$
$u^{-2}=v^{2}rightarrow v=u^{-1},u=v^{-1}rightarrow dv=-u^{-2}$
$$2int_{t=0}^{t=infty} e^{-v^{2}} dv$$
Recall: $$int_{0}^{infty} e^{-x^{2}} dx = frac{sqrt{pi}}{2}$$
Now for the bounds. I have kept them in terms of $t$, and now, after all of the substitutions, I can relate $v$ to $t$. I have $u=t^{-frac{1}{2}}$, and I also have $u=v^{-1}$, which gives me $v^{-1}=t^{-frac{1}{2}}$ which means that $v=t^{frac{1}{2}}$. When $t=0$, I get: $v=0^{frac{1}{2}}=0$, and when $t=infty$, I get: $v=infty^{frac{1}{2}}=infty$, so my bounds stay the same.
Finally: $$2int_{0}^{infty} e^{-v^{2}} dv=sqrt{pi}$$







integration proof-verification improper-integrals factorial






share|cite|improve this question













share|cite|improve this question











share|cite|improve this question




share|cite|improve this question










asked Mar 19 at 14:40









ItIsLastThursdayItIsLastThursday

364




364








  • 1




    $begingroup$
    What's the problem? Seems fine.
    $endgroup$
    – Hobbyist
    Mar 19 at 14:42










  • $begingroup$
    Is my method for determining the bounds in terms of $t$ to $v$ ok?
    $endgroup$
    – ItIsLastThursday
    Mar 19 at 14:45






  • 1




    $begingroup$
    That's pretty much the standard proof that $Gamma(tfrac12)=sqrtpi$ that you normally see. There's no problem with your limits.
    $endgroup$
    – Hobbyist
    Mar 19 at 14:46










  • $begingroup$
    What do you try to achieve with the first substitution? Don't you think $t=v^2$ is enough?
    $endgroup$
    – Diger
    Mar 19 at 14:46










  • $begingroup$
    I realized that afterwards, but whatever.
    $endgroup$
    – ItIsLastThursday
    Mar 19 at 14:47














  • 1




    $begingroup$
    What's the problem? Seems fine.
    $endgroup$
    – Hobbyist
    Mar 19 at 14:42










  • $begingroup$
    Is my method for determining the bounds in terms of $t$ to $v$ ok?
    $endgroup$
    – ItIsLastThursday
    Mar 19 at 14:45






  • 1




    $begingroup$
    That's pretty much the standard proof that $Gamma(tfrac12)=sqrtpi$ that you normally see. There's no problem with your limits.
    $endgroup$
    – Hobbyist
    Mar 19 at 14:46










  • $begingroup$
    What do you try to achieve with the first substitution? Don't you think $t=v^2$ is enough?
    $endgroup$
    – Diger
    Mar 19 at 14:46










  • $begingroup$
    I realized that afterwards, but whatever.
    $endgroup$
    – ItIsLastThursday
    Mar 19 at 14:47








1




1




$begingroup$
What's the problem? Seems fine.
$endgroup$
– Hobbyist
Mar 19 at 14:42




$begingroup$
What's the problem? Seems fine.
$endgroup$
– Hobbyist
Mar 19 at 14:42












$begingroup$
Is my method for determining the bounds in terms of $t$ to $v$ ok?
$endgroup$
– ItIsLastThursday
Mar 19 at 14:45




$begingroup$
Is my method for determining the bounds in terms of $t$ to $v$ ok?
$endgroup$
– ItIsLastThursday
Mar 19 at 14:45




1




1




$begingroup$
That's pretty much the standard proof that $Gamma(tfrac12)=sqrtpi$ that you normally see. There's no problem with your limits.
$endgroup$
– Hobbyist
Mar 19 at 14:46




$begingroup$
That's pretty much the standard proof that $Gamma(tfrac12)=sqrtpi$ that you normally see. There's no problem with your limits.
$endgroup$
– Hobbyist
Mar 19 at 14:46












$begingroup$
What do you try to achieve with the first substitution? Don't you think $t=v^2$ is enough?
$endgroup$
– Diger
Mar 19 at 14:46




$begingroup$
What do you try to achieve with the first substitution? Don't you think $t=v^2$ is enough?
$endgroup$
– Diger
Mar 19 at 14:46












$begingroup$
I realized that afterwards, but whatever.
$endgroup$
– ItIsLastThursday
Mar 19 at 14:47




$begingroup$
I realized that afterwards, but whatever.
$endgroup$
– ItIsLastThursday
Mar 19 at 14:47










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