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Contour integration with infinite poles

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Contour integration with infinite poles


contour integration of logarithm functionBest way to evaluate integral with contour integration?How many poles have to be inside the contour?Integral with contour integrationCan Cauchy principal values of functions with nonsimple poles be evaluated using complex contour integration methods?Are there real definite integrals which can only be evaluated by contour integration?Contour integral with two polesContour integration - complex analysis






.everyoneloves__top-leaderboard:empty,.everyoneloves__mid-leaderboard:empty,.everyoneloves__bot-mid-leaderboard:empty margin-bottom:0;








4












$begingroup$


I am trying to find the integral of the following expression:-
$$int_-infty^infty fracx^2e^k+e^x^2dx$$
I think this can be solved using contour integration. The poles will be the points with $z^2 = k+i(2n+1)pi$ according to me. But this results in infinite poles if you choose a contour covering the entire real axis. Does anybody have any insights to solve this integral?










share|cite|improve this question









$endgroup$









  • 1




    $begingroup$
    It is not a problem of infinitely poles. You can't use contour integration because the function doesn't $to 0$ for $|x|$ large on an half-plane.
    $endgroup$
    – reuns
    3 hours ago


















4












$begingroup$


I am trying to find the integral of the following expression:-
$$int_-infty^infty fracx^2e^k+e^x^2dx$$
I think this can be solved using contour integration. The poles will be the points with $z^2 = k+i(2n+1)pi$ according to me. But this results in infinite poles if you choose a contour covering the entire real axis. Does anybody have any insights to solve this integral?










share|cite|improve this question









$endgroup$









  • 1




    $begingroup$
    It is not a problem of infinitely poles. You can't use contour integration because the function doesn't $to 0$ for $|x|$ large on an half-plane.
    $endgroup$
    – reuns
    3 hours ago














4












4








4


1



$begingroup$


I am trying to find the integral of the following expression:-
$$int_-infty^infty fracx^2e^k+e^x^2dx$$
I think this can be solved using contour integration. The poles will be the points with $z^2 = k+i(2n+1)pi$ according to me. But this results in infinite poles if you choose a contour covering the entire real axis. Does anybody have any insights to solve this integral?










share|cite|improve this question









$endgroup$




I am trying to find the integral of the following expression:-
$$int_-infty^infty fracx^2e^k+e^x^2dx$$
I think this can be solved using contour integration. The poles will be the points with $z^2 = k+i(2n+1)pi$ according to me. But this results in infinite poles if you choose a contour covering the entire real axis. Does anybody have any insights to solve this integral?







integration complex-analysis contour-integration






share|cite|improve this question













share|cite|improve this question











share|cite|improve this question




share|cite|improve this question










asked 8 hours ago









Rishabh JainRishabh Jain

1958 bronze badges




1958 bronze badges










  • 1




    $begingroup$
    It is not a problem of infinitely poles. You can't use contour integration because the function doesn't $to 0$ for $|x|$ large on an half-plane.
    $endgroup$
    – reuns
    3 hours ago













  • 1




    $begingroup$
    It is not a problem of infinitely poles. You can't use contour integration because the function doesn't $to 0$ for $|x|$ large on an half-plane.
    $endgroup$
    – reuns
    3 hours ago








1




1




$begingroup$
It is not a problem of infinitely poles. You can't use contour integration because the function doesn't $to 0$ for $|x|$ large on an half-plane.
$endgroup$
– reuns
3 hours ago





$begingroup$
It is not a problem of infinitely poles. You can't use contour integration because the function doesn't $to 0$ for $|x|$ large on an half-plane.
$endgroup$
– reuns
3 hours ago











2 Answers
2






active

oldest

votes


















5














$begingroup$

Let's assume, for the moment, that $kleq 0$. Then we can rewrite our integral in the following way:



$$int_-infty^infty fracx^2e^k + e^x^2dx = e^-kint_-infty^infty fracx^2e^ke^-x^2e^ke^-x^2+1dx = e^-ksum_n=1^infty (-1)^n+1e^nkint_-infty^infty x^2e^-nx^2dx$$



Then, by Feynman's trick



$$= e^-ksum_n=1^infty (-1)^n+1 e^nkBiggr(-fracddnint_-infty^infty e^-nx^2dxBiggr) = e^-ksum_n=1^infty (-1)^n+1 e^nk left(-fracddnsqrtfracpinright)$$



$$ = -fracsqrtpi2e^-k sum_n=1^infty frac(-e^k)^nn^frac32 equiv -fracsqrtpi2e^-k textLi_frac32(-e^k)$$



While these specific steps don't apply when $k>0$, we can use analytic continuation to extend the polylogarithm (and taking the antilimit).






share|cite|improve this answer











$endgroup$










  • 1




    $begingroup$
    Nice use of Feynman's trick. $to +1$
    $endgroup$
    – Claude Leibovici
    7 hours ago










  • $begingroup$
    Alternatively I think you could use the identity $$fracGamma(s/2)n^spi^s/2=int_0^infty x^s/2-1e^-n^2pi xdx,$$ instead of Feynman's trick since your integral is symmetric about $x=0$. You'd need to apply a change of variable and substitute a value for $s$ first.
    $endgroup$
    – Pixel
    6 hours ago



















2














$begingroup$

Using a CAS, I did not find any antiderivative. However, for the integral
$$int_-infty^infty fracx^2K+e^x^2,dx=-fracsqrtpi 2 K textLi_frac32(-K)$$ where appears the polylogarithm function.



$$int_-infty^infty fracx^2e^k+e^x^2,dx=-fracsqrtpi 2 e^-k ,textLi_frac32left(-e^kright)$$






share|cite|improve this answer









$endgroup$














  • $begingroup$
    Hmm, interesting. Originally, I came across the above integral while manipulating a function related to fermi-Dirac statistics. I think if we do go along the road of expanding the above function in terms of the infinite poles, we may end up in the polylogarithmic function only.
    $endgroup$
    – Rishabh Jain
    7 hours ago













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2 Answers
2






active

oldest

votes








2 Answers
2






active

oldest

votes









active

oldest

votes






active

oldest

votes









5














$begingroup$

Let's assume, for the moment, that $kleq 0$. Then we can rewrite our integral in the following way:



$$int_-infty^infty fracx^2e^k + e^x^2dx = e^-kint_-infty^infty fracx^2e^ke^-x^2e^ke^-x^2+1dx = e^-ksum_n=1^infty (-1)^n+1e^nkint_-infty^infty x^2e^-nx^2dx$$



Then, by Feynman's trick



$$= e^-ksum_n=1^infty (-1)^n+1 e^nkBiggr(-fracddnint_-infty^infty e^-nx^2dxBiggr) = e^-ksum_n=1^infty (-1)^n+1 e^nk left(-fracddnsqrtfracpinright)$$



$$ = -fracsqrtpi2e^-k sum_n=1^infty frac(-e^k)^nn^frac32 equiv -fracsqrtpi2e^-k textLi_frac32(-e^k)$$



While these specific steps don't apply when $k>0$, we can use analytic continuation to extend the polylogarithm (and taking the antilimit).






share|cite|improve this answer











$endgroup$










  • 1




    $begingroup$
    Nice use of Feynman's trick. $to +1$
    $endgroup$
    – Claude Leibovici
    7 hours ago










  • $begingroup$
    Alternatively I think you could use the identity $$fracGamma(s/2)n^spi^s/2=int_0^infty x^s/2-1e^-n^2pi xdx,$$ instead of Feynman's trick since your integral is symmetric about $x=0$. You'd need to apply a change of variable and substitute a value for $s$ first.
    $endgroup$
    – Pixel
    6 hours ago
















5














$begingroup$

Let's assume, for the moment, that $kleq 0$. Then we can rewrite our integral in the following way:



$$int_-infty^infty fracx^2e^k + e^x^2dx = e^-kint_-infty^infty fracx^2e^ke^-x^2e^ke^-x^2+1dx = e^-ksum_n=1^infty (-1)^n+1e^nkint_-infty^infty x^2e^-nx^2dx$$



Then, by Feynman's trick



$$= e^-ksum_n=1^infty (-1)^n+1 e^nkBiggr(-fracddnint_-infty^infty e^-nx^2dxBiggr) = e^-ksum_n=1^infty (-1)^n+1 e^nk left(-fracddnsqrtfracpinright)$$



$$ = -fracsqrtpi2e^-k sum_n=1^infty frac(-e^k)^nn^frac32 equiv -fracsqrtpi2e^-k textLi_frac32(-e^k)$$



While these specific steps don't apply when $k>0$, we can use analytic continuation to extend the polylogarithm (and taking the antilimit).






share|cite|improve this answer











$endgroup$










  • 1




    $begingroup$
    Nice use of Feynman's trick. $to +1$
    $endgroup$
    – Claude Leibovici
    7 hours ago










  • $begingroup$
    Alternatively I think you could use the identity $$fracGamma(s/2)n^spi^s/2=int_0^infty x^s/2-1e^-n^2pi xdx,$$ instead of Feynman's trick since your integral is symmetric about $x=0$. You'd need to apply a change of variable and substitute a value for $s$ first.
    $endgroup$
    – Pixel
    6 hours ago














5














5










5







$begingroup$

Let's assume, for the moment, that $kleq 0$. Then we can rewrite our integral in the following way:



$$int_-infty^infty fracx^2e^k + e^x^2dx = e^-kint_-infty^infty fracx^2e^ke^-x^2e^ke^-x^2+1dx = e^-ksum_n=1^infty (-1)^n+1e^nkint_-infty^infty x^2e^-nx^2dx$$



Then, by Feynman's trick



$$= e^-ksum_n=1^infty (-1)^n+1 e^nkBiggr(-fracddnint_-infty^infty e^-nx^2dxBiggr) = e^-ksum_n=1^infty (-1)^n+1 e^nk left(-fracddnsqrtfracpinright)$$



$$ = -fracsqrtpi2e^-k sum_n=1^infty frac(-e^k)^nn^frac32 equiv -fracsqrtpi2e^-k textLi_frac32(-e^k)$$



While these specific steps don't apply when $k>0$, we can use analytic continuation to extend the polylogarithm (and taking the antilimit).






share|cite|improve this answer











$endgroup$



Let's assume, for the moment, that $kleq 0$. Then we can rewrite our integral in the following way:



$$int_-infty^infty fracx^2e^k + e^x^2dx = e^-kint_-infty^infty fracx^2e^ke^-x^2e^ke^-x^2+1dx = e^-ksum_n=1^infty (-1)^n+1e^nkint_-infty^infty x^2e^-nx^2dx$$



Then, by Feynman's trick



$$= e^-ksum_n=1^infty (-1)^n+1 e^nkBiggr(-fracddnint_-infty^infty e^-nx^2dxBiggr) = e^-ksum_n=1^infty (-1)^n+1 e^nk left(-fracddnsqrtfracpinright)$$



$$ = -fracsqrtpi2e^-k sum_n=1^infty frac(-e^k)^nn^frac32 equiv -fracsqrtpi2e^-k textLi_frac32(-e^k)$$



While these specific steps don't apply when $k>0$, we can use analytic continuation to extend the polylogarithm (and taking the antilimit).







share|cite|improve this answer














share|cite|improve this answer



share|cite|improve this answer








edited 7 hours ago

























answered 7 hours ago









Ninad MunshiNinad Munshi

2,6573 silver badges12 bronze badges




2,6573 silver badges12 bronze badges










  • 1




    $begingroup$
    Nice use of Feynman's trick. $to +1$
    $endgroup$
    – Claude Leibovici
    7 hours ago










  • $begingroup$
    Alternatively I think you could use the identity $$fracGamma(s/2)n^spi^s/2=int_0^infty x^s/2-1e^-n^2pi xdx,$$ instead of Feynman's trick since your integral is symmetric about $x=0$. You'd need to apply a change of variable and substitute a value for $s$ first.
    $endgroup$
    – Pixel
    6 hours ago













  • 1




    $begingroup$
    Nice use of Feynman's trick. $to +1$
    $endgroup$
    – Claude Leibovici
    7 hours ago










  • $begingroup$
    Alternatively I think you could use the identity $$fracGamma(s/2)n^spi^s/2=int_0^infty x^s/2-1e^-n^2pi xdx,$$ instead of Feynman's trick since your integral is symmetric about $x=0$. You'd need to apply a change of variable and substitute a value for $s$ first.
    $endgroup$
    – Pixel
    6 hours ago








1




1




$begingroup$
Nice use of Feynman's trick. $to +1$
$endgroup$
– Claude Leibovici
7 hours ago




$begingroup$
Nice use of Feynman's trick. $to +1$
$endgroup$
– Claude Leibovici
7 hours ago












$begingroup$
Alternatively I think you could use the identity $$fracGamma(s/2)n^spi^s/2=int_0^infty x^s/2-1e^-n^2pi xdx,$$ instead of Feynman's trick since your integral is symmetric about $x=0$. You'd need to apply a change of variable and substitute a value for $s$ first.
$endgroup$
– Pixel
6 hours ago





$begingroup$
Alternatively I think you could use the identity $$fracGamma(s/2)n^spi^s/2=int_0^infty x^s/2-1e^-n^2pi xdx,$$ instead of Feynman's trick since your integral is symmetric about $x=0$. You'd need to apply a change of variable and substitute a value for $s$ first.
$endgroup$
– Pixel
6 hours ago














2














$begingroup$

Using a CAS, I did not find any antiderivative. However, for the integral
$$int_-infty^infty fracx^2K+e^x^2,dx=-fracsqrtpi 2 K textLi_frac32(-K)$$ where appears the polylogarithm function.



$$int_-infty^infty fracx^2e^k+e^x^2,dx=-fracsqrtpi 2 e^-k ,textLi_frac32left(-e^kright)$$






share|cite|improve this answer









$endgroup$














  • $begingroup$
    Hmm, interesting. Originally, I came across the above integral while manipulating a function related to fermi-Dirac statistics. I think if we do go along the road of expanding the above function in terms of the infinite poles, we may end up in the polylogarithmic function only.
    $endgroup$
    – Rishabh Jain
    7 hours ago















2














$begingroup$

Using a CAS, I did not find any antiderivative. However, for the integral
$$int_-infty^infty fracx^2K+e^x^2,dx=-fracsqrtpi 2 K textLi_frac32(-K)$$ where appears the polylogarithm function.



$$int_-infty^infty fracx^2e^k+e^x^2,dx=-fracsqrtpi 2 e^-k ,textLi_frac32left(-e^kright)$$






share|cite|improve this answer









$endgroup$














  • $begingroup$
    Hmm, interesting. Originally, I came across the above integral while manipulating a function related to fermi-Dirac statistics. I think if we do go along the road of expanding the above function in terms of the infinite poles, we may end up in the polylogarithmic function only.
    $endgroup$
    – Rishabh Jain
    7 hours ago













2














2










2







$begingroup$

Using a CAS, I did not find any antiderivative. However, for the integral
$$int_-infty^infty fracx^2K+e^x^2,dx=-fracsqrtpi 2 K textLi_frac32(-K)$$ where appears the polylogarithm function.



$$int_-infty^infty fracx^2e^k+e^x^2,dx=-fracsqrtpi 2 e^-k ,textLi_frac32left(-e^kright)$$






share|cite|improve this answer









$endgroup$



Using a CAS, I did not find any antiderivative. However, for the integral
$$int_-infty^infty fracx^2K+e^x^2,dx=-fracsqrtpi 2 K textLi_frac32(-K)$$ where appears the polylogarithm function.



$$int_-infty^infty fracx^2e^k+e^x^2,dx=-fracsqrtpi 2 e^-k ,textLi_frac32left(-e^kright)$$







share|cite|improve this answer












share|cite|improve this answer



share|cite|improve this answer










answered 7 hours ago









Claude LeiboviciClaude Leibovici

136k11 gold badges64 silver badges146 bronze badges




136k11 gold badges64 silver badges146 bronze badges














  • $begingroup$
    Hmm, interesting. Originally, I came across the above integral while manipulating a function related to fermi-Dirac statistics. I think if we do go along the road of expanding the above function in terms of the infinite poles, we may end up in the polylogarithmic function only.
    $endgroup$
    – Rishabh Jain
    7 hours ago
















  • $begingroup$
    Hmm, interesting. Originally, I came across the above integral while manipulating a function related to fermi-Dirac statistics. I think if we do go along the road of expanding the above function in terms of the infinite poles, we may end up in the polylogarithmic function only.
    $endgroup$
    – Rishabh Jain
    7 hours ago















$begingroup$
Hmm, interesting. Originally, I came across the above integral while manipulating a function related to fermi-Dirac statistics. I think if we do go along the road of expanding the above function in terms of the infinite poles, we may end up in the polylogarithmic function only.
$endgroup$
– Rishabh Jain
7 hours ago




$begingroup$
Hmm, interesting. Originally, I came across the above integral while manipulating a function related to fermi-Dirac statistics. I think if we do go along the road of expanding the above function in terms of the infinite poles, we may end up in the polylogarithmic function only.
$endgroup$
– Rishabh Jain
7 hours ago


















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Кастелфранко ди Сопра Становништво Референце Спољашње везе Мени за навигацију43°37′18″ СГШ; 11°33′32″ ИГД / 43.62156° СГШ; 11.55885° ИГД / 43.62156; 11.5588543°37′18″ СГШ; 11°33′32″ ИГД / 43.62156° СГШ; 11.55885° ИГД / 43.62156; 11.558853179688„The GeoNames geographical database”„Istituto Nazionale di Statistica”проширитиууWorldCat156923403n850174324558639-1cb14643287r(подаци)