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How to evaluate the integral $int_0^infty fraclog xx^p (x-1), dx$?


How many ways to calculate: $sum_n=-infty^+inftyfrac1(u+n)^2$ where $u not in BbbZ$Finding integral $int_0^infty fracx^alphalogx1-x^2dx$ using complex analysis - residuesHow much makes $sumlimits_i=-infty^infty frac1i2pi+x$?integral with $logleft(fracx+1x-1right)$Evaluating $frac1pi int_0^pi e^2costheta dtheta$How to evaluate improper integral $int_0^inftyfractan^-1xe^ax-1dx$?Evaluate $int_-infty^infty fraclog(1+x^2) dx1+x^2$ Using Complex AnalysisEvaluate $int_ - infty^infty fracdx1+x^2$ using complex integrationAn explanation or hints to evaluate $textPVint_0^infty frace^-x(x+log (x))1-e^-xdx$Evaluate log improper integral $int_a^infty -frac1c (1-x) x$.Integral $int_frac12^1 fracln xsqrtx^2+1dx$How to evaluate $int_-infty^inftyfracxarctanfrac1x log(1+x^2)1+x^2dx$A line integral involving $log zeta(s)$













3












$begingroup$



How to evaluate the integral
$$
I_p=int_0^infty fraclog xx^p (x-1), dx,?$$




Attempt:



My first idea was to find the area of convergence, which gives me $p in (0,1)$. Now let's consider the function $f(z) = fraclog^2 zz^p (z-1)$. Then we can use Cauchy theorem and residuals.



But I'm stuck here. Because there is no term to describe $I_1$. Any ideas?










share|cite|improve this question











$endgroup$











  • $begingroup$
    math.stackexchange.com/a/2843081/155436
    $endgroup$
    – Count Iblis
    Mar 18 at 0:18















3












$begingroup$



How to evaluate the integral
$$
I_p=int_0^infty fraclog xx^p (x-1), dx,?$$




Attempt:



My first idea was to find the area of convergence, which gives me $p in (0,1)$. Now let's consider the function $f(z) = fraclog^2 zz^p (z-1)$. Then we can use Cauchy theorem and residuals.



But I'm stuck here. Because there is no term to describe $I_1$. Any ideas?










share|cite|improve this question











$endgroup$











  • $begingroup$
    math.stackexchange.com/a/2843081/155436
    $endgroup$
    – Count Iblis
    Mar 18 at 0:18













3












3








3





$begingroup$



How to evaluate the integral
$$
I_p=int_0^infty fraclog xx^p (x-1), dx,?$$




Attempt:



My first idea was to find the area of convergence, which gives me $p in (0,1)$. Now let's consider the function $f(z) = fraclog^2 zz^p (z-1)$. Then we can use Cauchy theorem and residuals.



But I'm stuck here. Because there is no term to describe $I_1$. Any ideas?










share|cite|improve this question











$endgroup$





How to evaluate the integral
$$
I_p=int_0^infty fraclog xx^p (x-1), dx,?$$




Attempt:



My first idea was to find the area of convergence, which gives me $p in (0,1)$. Now let's consider the function $f(z) = fraclog^2 zz^p (z-1)$. Then we can use Cauchy theorem and residuals.



But I'm stuck here. Because there is no term to describe $I_1$. Any ideas?







integration complex-analysis






share|cite|improve this question















share|cite|improve this question













share|cite|improve this question




share|cite|improve this question








edited Mar 17 at 19:28









Jack

27.6k1782203




27.6k1782203










asked Mar 17 at 15:54









openspaceopenspace

3,3512822




3,3512822











  • $begingroup$
    math.stackexchange.com/a/2843081/155436
    $endgroup$
    – Count Iblis
    Mar 18 at 0:18
















  • $begingroup$
    math.stackexchange.com/a/2843081/155436
    $endgroup$
    – Count Iblis
    Mar 18 at 0:18















$begingroup$
math.stackexchange.com/a/2843081/155436
$endgroup$
– Count Iblis
Mar 18 at 0:18




$begingroup$
math.stackexchange.com/a/2843081/155436
$endgroup$
– Count Iblis
Mar 18 at 0:18










4 Answers
4






active

oldest

votes


















6












$begingroup$

We can take from here the following representation of the digamma function:
$$psi(s+1)=-gamma+int_0^1 frac1-x^s1-xdxRightarrow psi_1(s)=int_0^1 fracx^s-1ln xx-1dx$$
Now we are just one step away to solve it by splitting the integral into two pieces because we have:
$$int_1^infty fracln xx^p(x-1)dxoversetlarge x=frac1t=int_0^1 fract^p-1ln tt-1dt$$




$$int_0^infty fracln xx^p(x-1)dx=int_0^1 fracx^-pln xx-1dx+int_0^1fracx^p-1ln xx-1dx=psi_1(1-p)+psi_1(p)=boxedfracpi^2sin^2 (pi p)$$
Above follows by the the trigamma's reflection formula.






share|cite|improve this answer











$endgroup$












  • $begingroup$
    Nice solution. I posted one in which I avoid any reference to special functions and instead uses contour integration and makes use of the partial fraction expansion of the cotangent function. Let me know what you think.
    $endgroup$
    – Mark Viola
    Mar 18 at 3:26










  • $begingroup$
    @MarkViola that is cute and probably what OP intended to find (seeing the complex analysis tag)! I wish I knew to do that myself from scratch (I don't have a good knowledge of complex analysis).
    $endgroup$
    – Zacky
    Mar 18 at 9:47







  • 1




    $begingroup$
    Thank you. And I thought it might be of interest to you to see THESE derivations of the partial fraction representation of the cotangent function, which was key to my solution herein.
    $endgroup$
    – Mark Viola
    Mar 18 at 16:45


















4












$begingroup$

Well use $$Re s>0implies int_0^inftyfracue^-su1-e^-udu=sum_nge 0frac1(n+s)^2.$$With the substitution $u=ln x$ followed by the identity $int_Bbb Rg(u)du=int_0^infty [g(u)+g(-u)]du$, $$I_1=int_0^inftyfracu (e^-pu+e^-(1-p)u)1-e^-udu=sum_nge 0left(frac1(n+1-p)^2+frac1(n+p)^2right).$$
This is evaluated here as $pi^2csc^2pi p.$






share|cite|improve this answer











$endgroup$








  • 1




    $begingroup$
    That's beautiful! Thanks for your answer, I was quite interested in this problem.+1
    $endgroup$
    – Awe Kumar Jha
    Mar 17 at 17:02











  • $begingroup$
    Using the relation: $zeta(2, x)=psi_1(x)$ further simplification is avaible using the reflection formula for the trigamma function. I didn't find that formula for the Hurwitz Zeta function (on google), altough there must exist one.
    $endgroup$
    – Zacky
    Mar 17 at 18:22







  • 1




    $begingroup$
    @Zacky Thanks; fixed.
    $endgroup$
    – J.G.
    Mar 17 at 18:26










  • $begingroup$
    @J.G. Nice solution. I posted one in which I avoid any reference to special functions and instead uses contour integration and makes use of the partial fraction expansion of the cotangent function. Let me know what you think.
    $endgroup$
    – Mark Viola
    Mar 18 at 3:27










  • $begingroup$
    Your solution is fine; you might consider providing readers with a reference to your first equation since this is the thrust of the development. And I just thought it might be of interest to you to see THESE derivations of the partial fraction representation of the cotangent function.
    $endgroup$
    – Mark Viola
    Mar 18 at 16:42


















2












$begingroup$

The OP stated at the end of the posted question




Now let's consider the function $f(z) = fraclog^2 zz^p (z-1)$. Then we can use Cauchy theorem and residuals.




Rather than analyze a contour integral of $f(z)=fraclog^2 zz^p (z-1)$, we analyze the integral



$$I(p)=oint_C fraclog(z)z^p(z-1),dz$$



where $C$ is the classical keyhole contour where the branch cut for $log(z)$ is take along the positive real axis and $arg(z)in [0,2pi)$. Inasmuch as $fraclog(z)z^p(z-1)$ is analytic in and on $C$, Cauchy's Integral Theorem guarantees that



$$beginalign
0&=oint_C fraclog(z)z^p(z-1),dz\\
&=int_epsilon^R fraclog(x)x^p(x-1),dx+underbraceint_0^2pi fraclog(Re^iphi)R^pe^ipphi(Re^iphi-1),iRe^iphi,dphi_to 0,,textas,,Rto infty+int_R^1+nufraclog(x)+i2pix^pe^i2pi p(x-1),dx\\
&+underbraceint_2pi^pi fraclog(1+nu e^iphi)(1+nu e^iphi)^pnu e^iphi,inu e^iphi,dphi_to -ipi (i2pi )e^-i2pi p,,textas,,nuto0+int_1-nu^epsilon fraclog(x)+i2pix^pe^i2pi p(x-1),dx+underbraceint_2pi^0 fraclog(epsilon e^iphi)(epsilon e^iphi)^p(epsilon e^iphi-1),iepsilon e^iphi,dphi_to 0,,textas,,epsilonto 0tag1
endalign$$




Letting $epsilonto 0^+$, $Rto infty$, and $nu to 0^+$ in $(1)$, we obtain



$$(1-e^-i2pi p)int_0^infty fraclog(x)x^p(x-1),dx=i2pi e^-i2pi p,,textPVleft(int_0^infty frac1x^p(x-1),dxright)+(ipi)left(i2pi e^-i2pi p right)tag2$$



where $textPVleft(int_0^infty frac1x^p(x-1),dx+ipiright)$ denotes the Cauchy Principal Value (CPV) integral.




We can evaluate the CVP integral as follows.



$$beginalign
textPVint_0^infty frac1x^p(x-1),dx&=lim_nuto 0^+left(int_0^1-nufrac1x^p(x-1),dx+int_1+nu^inftyfrac1x^p(x-1),dxright)\\
&=lim_nuto 0^+left(-sum_n=0^inftyint_0^1-nux^n-p,dx+sum_n=0^inftyint_1+nu^infty x^-n-p-1,dxright)\\
&=sum_n=0^infty left(frac1n+p-frac1n-p+1right)tag3
endalign$$



The series on the right-hand side of $(3)$ is the partial fraction representation of $pi cot(pi p)$ for $pin (0,1)$ (SEE HERE).




Substituting $(3)$ into $(2)$, dividing both sides by $(1-e^-i2pi p)$, we find



$$int_0^infty fraclog(x)x^p(x-1),dx=fracpi^2sin^2(pi p)$$






share|cite|improve this answer











$endgroup$












  • $begingroup$
    @openspace Please let me know how I can improve my answer. I really want to give you the best answer I can. And feel free to up vote an answer as you see fit.
    $endgroup$
    – Mark Viola
    2 days ago



















0












$begingroup$

Too Long for comment



If $p≥2$ were some natural number, we could write the indefinite integral as,
$$
I = log x left[ log left( 1-frac 1x right) + sum_r=2^p frac 1(r-1)x^r-1 right] - text Li _2 left( frac 1x right) + sum_r=2^p frac 1(r-1)^2x^r-1 + C
$$

However, I don't know how this can be related to your problem, as you say $0<p<1$ which seems absurd.






share|cite|improve this answer









$endgroup$












  • $begingroup$
    web.archive.org/web/20110617053801/http://www.math.tu-berlin.de/…
    $endgroup$
    – Count Iblis
    Mar 18 at 0:13










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4 Answers
4






active

oldest

votes








4 Answers
4






active

oldest

votes









active

oldest

votes






active

oldest

votes









6












$begingroup$

We can take from here the following representation of the digamma function:
$$psi(s+1)=-gamma+int_0^1 frac1-x^s1-xdxRightarrow psi_1(s)=int_0^1 fracx^s-1ln xx-1dx$$
Now we are just one step away to solve it by splitting the integral into two pieces because we have:
$$int_1^infty fracln xx^p(x-1)dxoversetlarge x=frac1t=int_0^1 fract^p-1ln tt-1dt$$




$$int_0^infty fracln xx^p(x-1)dx=int_0^1 fracx^-pln xx-1dx+int_0^1fracx^p-1ln xx-1dx=psi_1(1-p)+psi_1(p)=boxedfracpi^2sin^2 (pi p)$$
Above follows by the the trigamma's reflection formula.






share|cite|improve this answer











$endgroup$












  • $begingroup$
    Nice solution. I posted one in which I avoid any reference to special functions and instead uses contour integration and makes use of the partial fraction expansion of the cotangent function. Let me know what you think.
    $endgroup$
    – Mark Viola
    Mar 18 at 3:26










  • $begingroup$
    @MarkViola that is cute and probably what OP intended to find (seeing the complex analysis tag)! I wish I knew to do that myself from scratch (I don't have a good knowledge of complex analysis).
    $endgroup$
    – Zacky
    Mar 18 at 9:47







  • 1




    $begingroup$
    Thank you. And I thought it might be of interest to you to see THESE derivations of the partial fraction representation of the cotangent function, which was key to my solution herein.
    $endgroup$
    – Mark Viola
    Mar 18 at 16:45















6












$begingroup$

We can take from here the following representation of the digamma function:
$$psi(s+1)=-gamma+int_0^1 frac1-x^s1-xdxRightarrow psi_1(s)=int_0^1 fracx^s-1ln xx-1dx$$
Now we are just one step away to solve it by splitting the integral into two pieces because we have:
$$int_1^infty fracln xx^p(x-1)dxoversetlarge x=frac1t=int_0^1 fract^p-1ln tt-1dt$$




$$int_0^infty fracln xx^p(x-1)dx=int_0^1 fracx^-pln xx-1dx+int_0^1fracx^p-1ln xx-1dx=psi_1(1-p)+psi_1(p)=boxedfracpi^2sin^2 (pi p)$$
Above follows by the the trigamma's reflection formula.






share|cite|improve this answer











$endgroup$












  • $begingroup$
    Nice solution. I posted one in which I avoid any reference to special functions and instead uses contour integration and makes use of the partial fraction expansion of the cotangent function. Let me know what you think.
    $endgroup$
    – Mark Viola
    Mar 18 at 3:26










  • $begingroup$
    @MarkViola that is cute and probably what OP intended to find (seeing the complex analysis tag)! I wish I knew to do that myself from scratch (I don't have a good knowledge of complex analysis).
    $endgroup$
    – Zacky
    Mar 18 at 9:47







  • 1




    $begingroup$
    Thank you. And I thought it might be of interest to you to see THESE derivations of the partial fraction representation of the cotangent function, which was key to my solution herein.
    $endgroup$
    – Mark Viola
    Mar 18 at 16:45













6












6








6





$begingroup$

We can take from here the following representation of the digamma function:
$$psi(s+1)=-gamma+int_0^1 frac1-x^s1-xdxRightarrow psi_1(s)=int_0^1 fracx^s-1ln xx-1dx$$
Now we are just one step away to solve it by splitting the integral into two pieces because we have:
$$int_1^infty fracln xx^p(x-1)dxoversetlarge x=frac1t=int_0^1 fract^p-1ln tt-1dt$$




$$int_0^infty fracln xx^p(x-1)dx=int_0^1 fracx^-pln xx-1dx+int_0^1fracx^p-1ln xx-1dx=psi_1(1-p)+psi_1(p)=boxedfracpi^2sin^2 (pi p)$$
Above follows by the the trigamma's reflection formula.






share|cite|improve this answer











$endgroup$



We can take from here the following representation of the digamma function:
$$psi(s+1)=-gamma+int_0^1 frac1-x^s1-xdxRightarrow psi_1(s)=int_0^1 fracx^s-1ln xx-1dx$$
Now we are just one step away to solve it by splitting the integral into two pieces because we have:
$$int_1^infty fracln xx^p(x-1)dxoversetlarge x=frac1t=int_0^1 fract^p-1ln tt-1dt$$




$$int_0^infty fracln xx^p(x-1)dx=int_0^1 fracx^-pln xx-1dx+int_0^1fracx^p-1ln xx-1dx=psi_1(1-p)+psi_1(p)=boxedfracpi^2sin^2 (pi p)$$
Above follows by the the trigamma's reflection formula.







share|cite|improve this answer














share|cite|improve this answer



share|cite|improve this answer








edited Mar 17 at 18:28

























answered Mar 17 at 18:20









ZackyZacky

7,75511062




7,75511062











  • $begingroup$
    Nice solution. I posted one in which I avoid any reference to special functions and instead uses contour integration and makes use of the partial fraction expansion of the cotangent function. Let me know what you think.
    $endgroup$
    – Mark Viola
    Mar 18 at 3:26










  • $begingroup$
    @MarkViola that is cute and probably what OP intended to find (seeing the complex analysis tag)! I wish I knew to do that myself from scratch (I don't have a good knowledge of complex analysis).
    $endgroup$
    – Zacky
    Mar 18 at 9:47







  • 1




    $begingroup$
    Thank you. And I thought it might be of interest to you to see THESE derivations of the partial fraction representation of the cotangent function, which was key to my solution herein.
    $endgroup$
    – Mark Viola
    Mar 18 at 16:45
















  • $begingroup$
    Nice solution. I posted one in which I avoid any reference to special functions and instead uses contour integration and makes use of the partial fraction expansion of the cotangent function. Let me know what you think.
    $endgroup$
    – Mark Viola
    Mar 18 at 3:26










  • $begingroup$
    @MarkViola that is cute and probably what OP intended to find (seeing the complex analysis tag)! I wish I knew to do that myself from scratch (I don't have a good knowledge of complex analysis).
    $endgroup$
    – Zacky
    Mar 18 at 9:47







  • 1




    $begingroup$
    Thank you. And I thought it might be of interest to you to see THESE derivations of the partial fraction representation of the cotangent function, which was key to my solution herein.
    $endgroup$
    – Mark Viola
    Mar 18 at 16:45















$begingroup$
Nice solution. I posted one in which I avoid any reference to special functions and instead uses contour integration and makes use of the partial fraction expansion of the cotangent function. Let me know what you think.
$endgroup$
– Mark Viola
Mar 18 at 3:26




$begingroup$
Nice solution. I posted one in which I avoid any reference to special functions and instead uses contour integration and makes use of the partial fraction expansion of the cotangent function. Let me know what you think.
$endgroup$
– Mark Viola
Mar 18 at 3:26












$begingroup$
@MarkViola that is cute and probably what OP intended to find (seeing the complex analysis tag)! I wish I knew to do that myself from scratch (I don't have a good knowledge of complex analysis).
$endgroup$
– Zacky
Mar 18 at 9:47





$begingroup$
@MarkViola that is cute and probably what OP intended to find (seeing the complex analysis tag)! I wish I knew to do that myself from scratch (I don't have a good knowledge of complex analysis).
$endgroup$
– Zacky
Mar 18 at 9:47





1




1




$begingroup$
Thank you. And I thought it might be of interest to you to see THESE derivations of the partial fraction representation of the cotangent function, which was key to my solution herein.
$endgroup$
– Mark Viola
Mar 18 at 16:45




$begingroup$
Thank you. And I thought it might be of interest to you to see THESE derivations of the partial fraction representation of the cotangent function, which was key to my solution herein.
$endgroup$
– Mark Viola
Mar 18 at 16:45











4












$begingroup$

Well use $$Re s>0implies int_0^inftyfracue^-su1-e^-udu=sum_nge 0frac1(n+s)^2.$$With the substitution $u=ln x$ followed by the identity $int_Bbb Rg(u)du=int_0^infty [g(u)+g(-u)]du$, $$I_1=int_0^inftyfracu (e^-pu+e^-(1-p)u)1-e^-udu=sum_nge 0left(frac1(n+1-p)^2+frac1(n+p)^2right).$$
This is evaluated here as $pi^2csc^2pi p.$






share|cite|improve this answer











$endgroup$








  • 1




    $begingroup$
    That's beautiful! Thanks for your answer, I was quite interested in this problem.+1
    $endgroup$
    – Awe Kumar Jha
    Mar 17 at 17:02











  • $begingroup$
    Using the relation: $zeta(2, x)=psi_1(x)$ further simplification is avaible using the reflection formula for the trigamma function. I didn't find that formula for the Hurwitz Zeta function (on google), altough there must exist one.
    $endgroup$
    – Zacky
    Mar 17 at 18:22







  • 1




    $begingroup$
    @Zacky Thanks; fixed.
    $endgroup$
    – J.G.
    Mar 17 at 18:26










  • $begingroup$
    @J.G. Nice solution. I posted one in which I avoid any reference to special functions and instead uses contour integration and makes use of the partial fraction expansion of the cotangent function. Let me know what you think.
    $endgroup$
    – Mark Viola
    Mar 18 at 3:27










  • $begingroup$
    Your solution is fine; you might consider providing readers with a reference to your first equation since this is the thrust of the development. And I just thought it might be of interest to you to see THESE derivations of the partial fraction representation of the cotangent function.
    $endgroup$
    – Mark Viola
    Mar 18 at 16:42















4












$begingroup$

Well use $$Re s>0implies int_0^inftyfracue^-su1-e^-udu=sum_nge 0frac1(n+s)^2.$$With the substitution $u=ln x$ followed by the identity $int_Bbb Rg(u)du=int_0^infty [g(u)+g(-u)]du$, $$I_1=int_0^inftyfracu (e^-pu+e^-(1-p)u)1-e^-udu=sum_nge 0left(frac1(n+1-p)^2+frac1(n+p)^2right).$$
This is evaluated here as $pi^2csc^2pi p.$






share|cite|improve this answer











$endgroup$








  • 1




    $begingroup$
    That's beautiful! Thanks for your answer, I was quite interested in this problem.+1
    $endgroup$
    – Awe Kumar Jha
    Mar 17 at 17:02











  • $begingroup$
    Using the relation: $zeta(2, x)=psi_1(x)$ further simplification is avaible using the reflection formula for the trigamma function. I didn't find that formula for the Hurwitz Zeta function (on google), altough there must exist one.
    $endgroup$
    – Zacky
    Mar 17 at 18:22







  • 1




    $begingroup$
    @Zacky Thanks; fixed.
    $endgroup$
    – J.G.
    Mar 17 at 18:26










  • $begingroup$
    @J.G. Nice solution. I posted one in which I avoid any reference to special functions and instead uses contour integration and makes use of the partial fraction expansion of the cotangent function. Let me know what you think.
    $endgroup$
    – Mark Viola
    Mar 18 at 3:27










  • $begingroup$
    Your solution is fine; you might consider providing readers with a reference to your first equation since this is the thrust of the development. And I just thought it might be of interest to you to see THESE derivations of the partial fraction representation of the cotangent function.
    $endgroup$
    – Mark Viola
    Mar 18 at 16:42













4












4








4





$begingroup$

Well use $$Re s>0implies int_0^inftyfracue^-su1-e^-udu=sum_nge 0frac1(n+s)^2.$$With the substitution $u=ln x$ followed by the identity $int_Bbb Rg(u)du=int_0^infty [g(u)+g(-u)]du$, $$I_1=int_0^inftyfracu (e^-pu+e^-(1-p)u)1-e^-udu=sum_nge 0left(frac1(n+1-p)^2+frac1(n+p)^2right).$$
This is evaluated here as $pi^2csc^2pi p.$






share|cite|improve this answer











$endgroup$



Well use $$Re s>0implies int_0^inftyfracue^-su1-e^-udu=sum_nge 0frac1(n+s)^2.$$With the substitution $u=ln x$ followed by the identity $int_Bbb Rg(u)du=int_0^infty [g(u)+g(-u)]du$, $$I_1=int_0^inftyfracu (e^-pu+e^-(1-p)u)1-e^-udu=sum_nge 0left(frac1(n+1-p)^2+frac1(n+p)^2right).$$
This is evaluated here as $pi^2csc^2pi p.$







share|cite|improve this answer














share|cite|improve this answer



share|cite|improve this answer








edited Mar 18 at 17:44

























answered Mar 17 at 16:57









J.G.J.G.

32.1k23250




32.1k23250







  • 1




    $begingroup$
    That's beautiful! Thanks for your answer, I was quite interested in this problem.+1
    $endgroup$
    – Awe Kumar Jha
    Mar 17 at 17:02











  • $begingroup$
    Using the relation: $zeta(2, x)=psi_1(x)$ further simplification is avaible using the reflection formula for the trigamma function. I didn't find that formula for the Hurwitz Zeta function (on google), altough there must exist one.
    $endgroup$
    – Zacky
    Mar 17 at 18:22







  • 1




    $begingroup$
    @Zacky Thanks; fixed.
    $endgroup$
    – J.G.
    Mar 17 at 18:26










  • $begingroup$
    @J.G. Nice solution. I posted one in which I avoid any reference to special functions and instead uses contour integration and makes use of the partial fraction expansion of the cotangent function. Let me know what you think.
    $endgroup$
    – Mark Viola
    Mar 18 at 3:27










  • $begingroup$
    Your solution is fine; you might consider providing readers with a reference to your first equation since this is the thrust of the development. And I just thought it might be of interest to you to see THESE derivations of the partial fraction representation of the cotangent function.
    $endgroup$
    – Mark Viola
    Mar 18 at 16:42












  • 1




    $begingroup$
    That's beautiful! Thanks for your answer, I was quite interested in this problem.+1
    $endgroup$
    – Awe Kumar Jha
    Mar 17 at 17:02











  • $begingroup$
    Using the relation: $zeta(2, x)=psi_1(x)$ further simplification is avaible using the reflection formula for the trigamma function. I didn't find that formula for the Hurwitz Zeta function (on google), altough there must exist one.
    $endgroup$
    – Zacky
    Mar 17 at 18:22







  • 1




    $begingroup$
    @Zacky Thanks; fixed.
    $endgroup$
    – J.G.
    Mar 17 at 18:26










  • $begingroup$
    @J.G. Nice solution. I posted one in which I avoid any reference to special functions and instead uses contour integration and makes use of the partial fraction expansion of the cotangent function. Let me know what you think.
    $endgroup$
    – Mark Viola
    Mar 18 at 3:27










  • $begingroup$
    Your solution is fine; you might consider providing readers with a reference to your first equation since this is the thrust of the development. And I just thought it might be of interest to you to see THESE derivations of the partial fraction representation of the cotangent function.
    $endgroup$
    – Mark Viola
    Mar 18 at 16:42







1




1




$begingroup$
That's beautiful! Thanks for your answer, I was quite interested in this problem.+1
$endgroup$
– Awe Kumar Jha
Mar 17 at 17:02





$begingroup$
That's beautiful! Thanks for your answer, I was quite interested in this problem.+1
$endgroup$
– Awe Kumar Jha
Mar 17 at 17:02













$begingroup$
Using the relation: $zeta(2, x)=psi_1(x)$ further simplification is avaible using the reflection formula for the trigamma function. I didn't find that formula for the Hurwitz Zeta function (on google), altough there must exist one.
$endgroup$
– Zacky
Mar 17 at 18:22





$begingroup$
Using the relation: $zeta(2, x)=psi_1(x)$ further simplification is avaible using the reflection formula for the trigamma function. I didn't find that formula for the Hurwitz Zeta function (on google), altough there must exist one.
$endgroup$
– Zacky
Mar 17 at 18:22





1




1




$begingroup$
@Zacky Thanks; fixed.
$endgroup$
– J.G.
Mar 17 at 18:26




$begingroup$
@Zacky Thanks; fixed.
$endgroup$
– J.G.
Mar 17 at 18:26












$begingroup$
@J.G. Nice solution. I posted one in which I avoid any reference to special functions and instead uses contour integration and makes use of the partial fraction expansion of the cotangent function. Let me know what you think.
$endgroup$
– Mark Viola
Mar 18 at 3:27




$begingroup$
@J.G. Nice solution. I posted one in which I avoid any reference to special functions and instead uses contour integration and makes use of the partial fraction expansion of the cotangent function. Let me know what you think.
$endgroup$
– Mark Viola
Mar 18 at 3:27












$begingroup$
Your solution is fine; you might consider providing readers with a reference to your first equation since this is the thrust of the development. And I just thought it might be of interest to you to see THESE derivations of the partial fraction representation of the cotangent function.
$endgroup$
– Mark Viola
Mar 18 at 16:42




$begingroup$
Your solution is fine; you might consider providing readers with a reference to your first equation since this is the thrust of the development. And I just thought it might be of interest to you to see THESE derivations of the partial fraction representation of the cotangent function.
$endgroup$
– Mark Viola
Mar 18 at 16:42











2












$begingroup$

The OP stated at the end of the posted question




Now let's consider the function $f(z) = fraclog^2 zz^p (z-1)$. Then we can use Cauchy theorem and residuals.




Rather than analyze a contour integral of $f(z)=fraclog^2 zz^p (z-1)$, we analyze the integral



$$I(p)=oint_C fraclog(z)z^p(z-1),dz$$



where $C$ is the classical keyhole contour where the branch cut for $log(z)$ is take along the positive real axis and $arg(z)in [0,2pi)$. Inasmuch as $fraclog(z)z^p(z-1)$ is analytic in and on $C$, Cauchy's Integral Theorem guarantees that



$$beginalign
0&=oint_C fraclog(z)z^p(z-1),dz\\
&=int_epsilon^R fraclog(x)x^p(x-1),dx+underbraceint_0^2pi fraclog(Re^iphi)R^pe^ipphi(Re^iphi-1),iRe^iphi,dphi_to 0,,textas,,Rto infty+int_R^1+nufraclog(x)+i2pix^pe^i2pi p(x-1),dx\\
&+underbraceint_2pi^pi fraclog(1+nu e^iphi)(1+nu e^iphi)^pnu e^iphi,inu e^iphi,dphi_to -ipi (i2pi )e^-i2pi p,,textas,,nuto0+int_1-nu^epsilon fraclog(x)+i2pix^pe^i2pi p(x-1),dx+underbraceint_2pi^0 fraclog(epsilon e^iphi)(epsilon e^iphi)^p(epsilon e^iphi-1),iepsilon e^iphi,dphi_to 0,,textas,,epsilonto 0tag1
endalign$$




Letting $epsilonto 0^+$, $Rto infty$, and $nu to 0^+$ in $(1)$, we obtain



$$(1-e^-i2pi p)int_0^infty fraclog(x)x^p(x-1),dx=i2pi e^-i2pi p,,textPVleft(int_0^infty frac1x^p(x-1),dxright)+(ipi)left(i2pi e^-i2pi p right)tag2$$



where $textPVleft(int_0^infty frac1x^p(x-1),dx+ipiright)$ denotes the Cauchy Principal Value (CPV) integral.




We can evaluate the CVP integral as follows.



$$beginalign
textPVint_0^infty frac1x^p(x-1),dx&=lim_nuto 0^+left(int_0^1-nufrac1x^p(x-1),dx+int_1+nu^inftyfrac1x^p(x-1),dxright)\\
&=lim_nuto 0^+left(-sum_n=0^inftyint_0^1-nux^n-p,dx+sum_n=0^inftyint_1+nu^infty x^-n-p-1,dxright)\\
&=sum_n=0^infty left(frac1n+p-frac1n-p+1right)tag3
endalign$$



The series on the right-hand side of $(3)$ is the partial fraction representation of $pi cot(pi p)$ for $pin (0,1)$ (SEE HERE).




Substituting $(3)$ into $(2)$, dividing both sides by $(1-e^-i2pi p)$, we find



$$int_0^infty fraclog(x)x^p(x-1),dx=fracpi^2sin^2(pi p)$$






share|cite|improve this answer











$endgroup$












  • $begingroup$
    @openspace Please let me know how I can improve my answer. I really want to give you the best answer I can. And feel free to up vote an answer as you see fit.
    $endgroup$
    – Mark Viola
    2 days ago
















2












$begingroup$

The OP stated at the end of the posted question




Now let's consider the function $f(z) = fraclog^2 zz^p (z-1)$. Then we can use Cauchy theorem and residuals.




Rather than analyze a contour integral of $f(z)=fraclog^2 zz^p (z-1)$, we analyze the integral



$$I(p)=oint_C fraclog(z)z^p(z-1),dz$$



where $C$ is the classical keyhole contour where the branch cut for $log(z)$ is take along the positive real axis and $arg(z)in [0,2pi)$. Inasmuch as $fraclog(z)z^p(z-1)$ is analytic in and on $C$, Cauchy's Integral Theorem guarantees that



$$beginalign
0&=oint_C fraclog(z)z^p(z-1),dz\\
&=int_epsilon^R fraclog(x)x^p(x-1),dx+underbraceint_0^2pi fraclog(Re^iphi)R^pe^ipphi(Re^iphi-1),iRe^iphi,dphi_to 0,,textas,,Rto infty+int_R^1+nufraclog(x)+i2pix^pe^i2pi p(x-1),dx\\
&+underbraceint_2pi^pi fraclog(1+nu e^iphi)(1+nu e^iphi)^pnu e^iphi,inu e^iphi,dphi_to -ipi (i2pi )e^-i2pi p,,textas,,nuto0+int_1-nu^epsilon fraclog(x)+i2pix^pe^i2pi p(x-1),dx+underbraceint_2pi^0 fraclog(epsilon e^iphi)(epsilon e^iphi)^p(epsilon e^iphi-1),iepsilon e^iphi,dphi_to 0,,textas,,epsilonto 0tag1
endalign$$




Letting $epsilonto 0^+$, $Rto infty$, and $nu to 0^+$ in $(1)$, we obtain



$$(1-e^-i2pi p)int_0^infty fraclog(x)x^p(x-1),dx=i2pi e^-i2pi p,,textPVleft(int_0^infty frac1x^p(x-1),dxright)+(ipi)left(i2pi e^-i2pi p right)tag2$$



where $textPVleft(int_0^infty frac1x^p(x-1),dx+ipiright)$ denotes the Cauchy Principal Value (CPV) integral.




We can evaluate the CVP integral as follows.



$$beginalign
textPVint_0^infty frac1x^p(x-1),dx&=lim_nuto 0^+left(int_0^1-nufrac1x^p(x-1),dx+int_1+nu^inftyfrac1x^p(x-1),dxright)\\
&=lim_nuto 0^+left(-sum_n=0^inftyint_0^1-nux^n-p,dx+sum_n=0^inftyint_1+nu^infty x^-n-p-1,dxright)\\
&=sum_n=0^infty left(frac1n+p-frac1n-p+1right)tag3
endalign$$



The series on the right-hand side of $(3)$ is the partial fraction representation of $pi cot(pi p)$ for $pin (0,1)$ (SEE HERE).




Substituting $(3)$ into $(2)$, dividing both sides by $(1-e^-i2pi p)$, we find



$$int_0^infty fraclog(x)x^p(x-1),dx=fracpi^2sin^2(pi p)$$






share|cite|improve this answer











$endgroup$












  • $begingroup$
    @openspace Please let me know how I can improve my answer. I really want to give you the best answer I can. And feel free to up vote an answer as you see fit.
    $endgroup$
    – Mark Viola
    2 days ago














2












2








2





$begingroup$

The OP stated at the end of the posted question




Now let's consider the function $f(z) = fraclog^2 zz^p (z-1)$. Then we can use Cauchy theorem and residuals.




Rather than analyze a contour integral of $f(z)=fraclog^2 zz^p (z-1)$, we analyze the integral



$$I(p)=oint_C fraclog(z)z^p(z-1),dz$$



where $C$ is the classical keyhole contour where the branch cut for $log(z)$ is take along the positive real axis and $arg(z)in [0,2pi)$. Inasmuch as $fraclog(z)z^p(z-1)$ is analytic in and on $C$, Cauchy's Integral Theorem guarantees that



$$beginalign
0&=oint_C fraclog(z)z^p(z-1),dz\\
&=int_epsilon^R fraclog(x)x^p(x-1),dx+underbraceint_0^2pi fraclog(Re^iphi)R^pe^ipphi(Re^iphi-1),iRe^iphi,dphi_to 0,,textas,,Rto infty+int_R^1+nufraclog(x)+i2pix^pe^i2pi p(x-1),dx\\
&+underbraceint_2pi^pi fraclog(1+nu e^iphi)(1+nu e^iphi)^pnu e^iphi,inu e^iphi,dphi_to -ipi (i2pi )e^-i2pi p,,textas,,nuto0+int_1-nu^epsilon fraclog(x)+i2pix^pe^i2pi p(x-1),dx+underbraceint_2pi^0 fraclog(epsilon e^iphi)(epsilon e^iphi)^p(epsilon e^iphi-1),iepsilon e^iphi,dphi_to 0,,textas,,epsilonto 0tag1
endalign$$




Letting $epsilonto 0^+$, $Rto infty$, and $nu to 0^+$ in $(1)$, we obtain



$$(1-e^-i2pi p)int_0^infty fraclog(x)x^p(x-1),dx=i2pi e^-i2pi p,,textPVleft(int_0^infty frac1x^p(x-1),dxright)+(ipi)left(i2pi e^-i2pi p right)tag2$$



where $textPVleft(int_0^infty frac1x^p(x-1),dx+ipiright)$ denotes the Cauchy Principal Value (CPV) integral.




We can evaluate the CVP integral as follows.



$$beginalign
textPVint_0^infty frac1x^p(x-1),dx&=lim_nuto 0^+left(int_0^1-nufrac1x^p(x-1),dx+int_1+nu^inftyfrac1x^p(x-1),dxright)\\
&=lim_nuto 0^+left(-sum_n=0^inftyint_0^1-nux^n-p,dx+sum_n=0^inftyint_1+nu^infty x^-n-p-1,dxright)\\
&=sum_n=0^infty left(frac1n+p-frac1n-p+1right)tag3
endalign$$



The series on the right-hand side of $(3)$ is the partial fraction representation of $pi cot(pi p)$ for $pin (0,1)$ (SEE HERE).




Substituting $(3)$ into $(2)$, dividing both sides by $(1-e^-i2pi p)$, we find



$$int_0^infty fraclog(x)x^p(x-1),dx=fracpi^2sin^2(pi p)$$






share|cite|improve this answer











$endgroup$



The OP stated at the end of the posted question




Now let's consider the function $f(z) = fraclog^2 zz^p (z-1)$. Then we can use Cauchy theorem and residuals.




Rather than analyze a contour integral of $f(z)=fraclog^2 zz^p (z-1)$, we analyze the integral



$$I(p)=oint_C fraclog(z)z^p(z-1),dz$$



where $C$ is the classical keyhole contour where the branch cut for $log(z)$ is take along the positive real axis and $arg(z)in [0,2pi)$. Inasmuch as $fraclog(z)z^p(z-1)$ is analytic in and on $C$, Cauchy's Integral Theorem guarantees that



$$beginalign
0&=oint_C fraclog(z)z^p(z-1),dz\\
&=int_epsilon^R fraclog(x)x^p(x-1),dx+underbraceint_0^2pi fraclog(Re^iphi)R^pe^ipphi(Re^iphi-1),iRe^iphi,dphi_to 0,,textas,,Rto infty+int_R^1+nufraclog(x)+i2pix^pe^i2pi p(x-1),dx\\
&+underbraceint_2pi^pi fraclog(1+nu e^iphi)(1+nu e^iphi)^pnu e^iphi,inu e^iphi,dphi_to -ipi (i2pi )e^-i2pi p,,textas,,nuto0+int_1-nu^epsilon fraclog(x)+i2pix^pe^i2pi p(x-1),dx+underbraceint_2pi^0 fraclog(epsilon e^iphi)(epsilon e^iphi)^p(epsilon e^iphi-1),iepsilon e^iphi,dphi_to 0,,textas,,epsilonto 0tag1
endalign$$




Letting $epsilonto 0^+$, $Rto infty$, and $nu to 0^+$ in $(1)$, we obtain



$$(1-e^-i2pi p)int_0^infty fraclog(x)x^p(x-1),dx=i2pi e^-i2pi p,,textPVleft(int_0^infty frac1x^p(x-1),dxright)+(ipi)left(i2pi e^-i2pi p right)tag2$$



where $textPVleft(int_0^infty frac1x^p(x-1),dx+ipiright)$ denotes the Cauchy Principal Value (CPV) integral.




We can evaluate the CVP integral as follows.



$$beginalign
textPVint_0^infty frac1x^p(x-1),dx&=lim_nuto 0^+left(int_0^1-nufrac1x^p(x-1),dx+int_1+nu^inftyfrac1x^p(x-1),dxright)\\
&=lim_nuto 0^+left(-sum_n=0^inftyint_0^1-nux^n-p,dx+sum_n=0^inftyint_1+nu^infty x^-n-p-1,dxright)\\
&=sum_n=0^infty left(frac1n+p-frac1n-p+1right)tag3
endalign$$



The series on the right-hand side of $(3)$ is the partial fraction representation of $pi cot(pi p)$ for $pin (0,1)$ (SEE HERE).




Substituting $(3)$ into $(2)$, dividing both sides by $(1-e^-i2pi p)$, we find



$$int_0^infty fraclog(x)x^p(x-1),dx=fracpi^2sin^2(pi p)$$







share|cite|improve this answer














share|cite|improve this answer



share|cite|improve this answer








edited Mar 18 at 16:10

























answered Mar 18 at 3:24









Mark ViolaMark Viola

134k1278176




134k1278176











  • $begingroup$
    @openspace Please let me know how I can improve my answer. I really want to give you the best answer I can. And feel free to up vote an answer as you see fit.
    $endgroup$
    – Mark Viola
    2 days ago

















  • $begingroup$
    @openspace Please let me know how I can improve my answer. I really want to give you the best answer I can. And feel free to up vote an answer as you see fit.
    $endgroup$
    – Mark Viola
    2 days ago
















$begingroup$
@openspace Please let me know how I can improve my answer. I really want to give you the best answer I can. And feel free to up vote an answer as you see fit.
$endgroup$
– Mark Viola
2 days ago





$begingroup$
@openspace Please let me know how I can improve my answer. I really want to give you the best answer I can. And feel free to up vote an answer as you see fit.
$endgroup$
– Mark Viola
2 days ago












0












$begingroup$

Too Long for comment



If $p≥2$ were some natural number, we could write the indefinite integral as,
$$
I = log x left[ log left( 1-frac 1x right) + sum_r=2^p frac 1(r-1)x^r-1 right] - text Li _2 left( frac 1x right) + sum_r=2^p frac 1(r-1)^2x^r-1 + C
$$

However, I don't know how this can be related to your problem, as you say $0<p<1$ which seems absurd.






share|cite|improve this answer









$endgroup$












  • $begingroup$
    web.archive.org/web/20110617053801/http://www.math.tu-berlin.de/…
    $endgroup$
    – Count Iblis
    Mar 18 at 0:13















0












$begingroup$

Too Long for comment



If $p≥2$ were some natural number, we could write the indefinite integral as,
$$
I = log x left[ log left( 1-frac 1x right) + sum_r=2^p frac 1(r-1)x^r-1 right] - text Li _2 left( frac 1x right) + sum_r=2^p frac 1(r-1)^2x^r-1 + C
$$

However, I don't know how this can be related to your problem, as you say $0<p<1$ which seems absurd.






share|cite|improve this answer









$endgroup$












  • $begingroup$
    web.archive.org/web/20110617053801/http://www.math.tu-berlin.de/…
    $endgroup$
    – Count Iblis
    Mar 18 at 0:13













0












0








0





$begingroup$

Too Long for comment



If $p≥2$ were some natural number, we could write the indefinite integral as,
$$
I = log x left[ log left( 1-frac 1x right) + sum_r=2^p frac 1(r-1)x^r-1 right] - text Li _2 left( frac 1x right) + sum_r=2^p frac 1(r-1)^2x^r-1 + C
$$

However, I don't know how this can be related to your problem, as you say $0<p<1$ which seems absurd.






share|cite|improve this answer









$endgroup$



Too Long for comment



If $p≥2$ were some natural number, we could write the indefinite integral as,
$$
I = log x left[ log left( 1-frac 1x right) + sum_r=2^p frac 1(r-1)x^r-1 right] - text Li _2 left( frac 1x right) + sum_r=2^p frac 1(r-1)^2x^r-1 + C
$$

However, I don't know how this can be related to your problem, as you say $0<p<1$ which seems absurd.







share|cite|improve this answer












share|cite|improve this answer



share|cite|improve this answer










answered Mar 17 at 16:39









Awe Kumar JhaAwe Kumar Jha

570113




570113











  • $begingroup$
    web.archive.org/web/20110617053801/http://www.math.tu-berlin.de/…
    $endgroup$
    – Count Iblis
    Mar 18 at 0:13
















  • $begingroup$
    web.archive.org/web/20110617053801/http://www.math.tu-berlin.de/…
    $endgroup$
    – Count Iblis
    Mar 18 at 0:13















$begingroup$
web.archive.org/web/20110617053801/http://www.math.tu-berlin.de/…
$endgroup$
– Count Iblis
Mar 18 at 0:13




$begingroup$
web.archive.org/web/20110617053801/http://www.math.tu-berlin.de/…
$endgroup$
– Count Iblis
Mar 18 at 0:13

















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Kathakali Contents Etymology and nomenclature History Repertoire Songs and musical instruments Traditional plays Styles: Sampradayam Training centers and awards Relationship to other dance forms See also Notes References External links Navigation menueThe Illustrated Encyclopedia of Hinduism: A-MSouth Asian Folklore: An EncyclopediaRoutledge International Encyclopedia of Women: Global Women's Issues and KnowledgeKathakali Dance-drama: Where Gods and Demons Come to PlayKathakali Dance-drama: Where Gods and Demons Come to PlayKathakali Dance-drama: Where Gods and Demons Come to Play10.1353/atj.2005.0004The Illustrated Encyclopedia of Hinduism: A-MEncyclopedia of HinduismKathakali Dance-drama: Where Gods and Demons Come to PlaySonic Liturgy: Ritual and Music in Hindu Tradition"The Mirror of Gesture"Kathakali Dance-drama: Where Gods and Demons Come to Play"Kathakali"Indian Theatre: Traditions of PerformanceIndian Theatre: Traditions of PerformanceIndian Theatre: Traditions of PerformanceIndian Theatre: Traditions of PerformanceMedieval Indian Literature: An AnthologyThe Oxford Companion to Indian TheatreSouth Asian Folklore: An Encyclopedia : Afghanistan, Bangladesh, India, Nepal, Pakistan, Sri LankaThe Rise of Performance Studies: Rethinking Richard Schechner's Broad SpectrumIndian Theatre: Traditions of PerformanceModern Asian Theatre and Performance 1900-2000Critical Theory and PerformanceBetween Theater and AnthropologyKathakali603847011Indian Theatre: Traditions of PerformanceIndian Theatre: Traditions of PerformanceIndian Theatre: Traditions of PerformanceBetween Theater and AnthropologyBetween Theater and AnthropologyNambeesan Smaraka AwardsArchivedThe Cambridge Guide to TheatreRoutledge International Encyclopedia of Women: Global Women's Issues and KnowledgeThe Garland Encyclopedia of World Music: South Asia : the Indian subcontinentThe Ethos of Noh: Actors and Their Art10.2307/1145740By Means of Performance: Intercultural Studies of Theatre and Ritual10.1017/s204912550000100xReconceiving the Renaissance: A Critical ReaderPerformance TheoryListening to Theatre: The Aural Dimension of Beijing Opera10.2307/1146013Kathakali: The Art of the Non-WorldlyOn KathakaliKathakali, the dance theatreThe Kathakali Complex: Performance & StructureKathakali Dance-Drama: Where Gods and Demons Come to Play10.1093/obo/9780195399318-0071Drama and Ritual of Early Hinduism"In the Shadow of Hollywood Orientalism: Authentic East Indian Dancing"10.1080/08949460490274013Sanskrit Play Production in Ancient IndiaIndian Music: History and StructureBharata, the Nāṭyaśāstra233639306Table of Contents2238067286469807Dance In Indian Painting10.2307/32047833204783Kathakali Dance-Theatre: A Visual Narrative of Sacred Indian MimeIndian Classical Dance: The Renaissance and BeyondKathakali: an indigenous art-form of Keralaeee

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