Concerning this sum $sum_{n=0}^{infty}frac{1}{4n+1}left[frac{1}{4^n}{2n choose...












10












$begingroup$


I was looking at this paper and saw this nice sum in section [12] of the paper,




$$sum_{n=0}^{infty}frac{1}{4n+1}left[frac{1}{4^n}{2n choose n}right]^2=frac{Gamma^4left(frac{1}{4}right)}{16pi^2}tag1$$




out of curiosity I conjectured the following two sums



$$begin{align*}
sum_{n=0}^{infty}frac{(-1)^n}{(2n-1)^2}left[frac{1}{4^n}{2n choose n}right]^2&=frac{4sqrt{2pi}}{Gamma^2left(frac{1}{4}right)}tag2\
sum_{n=0}^{infty}(-1)^nfrac{n^2}{(2n-1)^2}left[frac{1}{4^n}{2n choose n}right]^2&=-frac{Gamma^2left(frac{1}{4}right)}{8pisqrt{2pi}}tag3
end{align*}$$



I am unable to prove them.



How do we go about to prove these two sums?










share|cite|improve this question











$endgroup$








  • 2




    $begingroup$
    What made you conjecture them?
    $endgroup$
    – clathratus
    Jan 1 at 8:35










  • $begingroup$
    I suppose that,as in the linked paper, we would need to use hypergeometric functions first summing from $0$ to $p$.
    $endgroup$
    – Claude Leibovici
    Jan 1 at 9:15












  • $begingroup$
    +1 for link to the nice paper. May be Jack D'Aurizio can shed some light on your conjectured identities.
    $endgroup$
    – Paramanand Singh
    Jan 1 at 15:41












  • $begingroup$
    All the given series can be written in terms of the moments of $K(x)$ or $E(x)$, i.e. $int_{0}^{1}x^eta K(x),dx$ and $int_{0}^{1}x^eta E(x),dx$. Since the complete elliptic integrals have simple Fourier-Legendre expansions, these identities can be proved through harmonic analysis, too. That's the whole point of the paper in a nutshell ;)
    $endgroup$
    – Jack D'Aurizio
    Jan 1 at 20:28
















10












$begingroup$


I was looking at this paper and saw this nice sum in section [12] of the paper,




$$sum_{n=0}^{infty}frac{1}{4n+1}left[frac{1}{4^n}{2n choose n}right]^2=frac{Gamma^4left(frac{1}{4}right)}{16pi^2}tag1$$




out of curiosity I conjectured the following two sums



$$begin{align*}
sum_{n=0}^{infty}frac{(-1)^n}{(2n-1)^2}left[frac{1}{4^n}{2n choose n}right]^2&=frac{4sqrt{2pi}}{Gamma^2left(frac{1}{4}right)}tag2\
sum_{n=0}^{infty}(-1)^nfrac{n^2}{(2n-1)^2}left[frac{1}{4^n}{2n choose n}right]^2&=-frac{Gamma^2left(frac{1}{4}right)}{8pisqrt{2pi}}tag3
end{align*}$$



I am unable to prove them.



How do we go about to prove these two sums?










share|cite|improve this question











$endgroup$








  • 2




    $begingroup$
    What made you conjecture them?
    $endgroup$
    – clathratus
    Jan 1 at 8:35










  • $begingroup$
    I suppose that,as in the linked paper, we would need to use hypergeometric functions first summing from $0$ to $p$.
    $endgroup$
    – Claude Leibovici
    Jan 1 at 9:15












  • $begingroup$
    +1 for link to the nice paper. May be Jack D'Aurizio can shed some light on your conjectured identities.
    $endgroup$
    – Paramanand Singh
    Jan 1 at 15:41












  • $begingroup$
    All the given series can be written in terms of the moments of $K(x)$ or $E(x)$, i.e. $int_{0}^{1}x^eta K(x),dx$ and $int_{0}^{1}x^eta E(x),dx$. Since the complete elliptic integrals have simple Fourier-Legendre expansions, these identities can be proved through harmonic analysis, too. That's the whole point of the paper in a nutshell ;)
    $endgroup$
    – Jack D'Aurizio
    Jan 1 at 20:28














10












10








10


5



$begingroup$


I was looking at this paper and saw this nice sum in section [12] of the paper,




$$sum_{n=0}^{infty}frac{1}{4n+1}left[frac{1}{4^n}{2n choose n}right]^2=frac{Gamma^4left(frac{1}{4}right)}{16pi^2}tag1$$




out of curiosity I conjectured the following two sums



$$begin{align*}
sum_{n=0}^{infty}frac{(-1)^n}{(2n-1)^2}left[frac{1}{4^n}{2n choose n}right]^2&=frac{4sqrt{2pi}}{Gamma^2left(frac{1}{4}right)}tag2\
sum_{n=0}^{infty}(-1)^nfrac{n^2}{(2n-1)^2}left[frac{1}{4^n}{2n choose n}right]^2&=-frac{Gamma^2left(frac{1}{4}right)}{8pisqrt{2pi}}tag3
end{align*}$$



I am unable to prove them.



How do we go about to prove these two sums?










share|cite|improve this question











$endgroup$




I was looking at this paper and saw this nice sum in section [12] of the paper,




$$sum_{n=0}^{infty}frac{1}{4n+1}left[frac{1}{4^n}{2n choose n}right]^2=frac{Gamma^4left(frac{1}{4}right)}{16pi^2}tag1$$




out of curiosity I conjectured the following two sums



$$begin{align*}
sum_{n=0}^{infty}frac{(-1)^n}{(2n-1)^2}left[frac{1}{4^n}{2n choose n}right]^2&=frac{4sqrt{2pi}}{Gamma^2left(frac{1}{4}right)}tag2\
sum_{n=0}^{infty}(-1)^nfrac{n^2}{(2n-1)^2}left[frac{1}{4^n}{2n choose n}right]^2&=-frac{Gamma^2left(frac{1}{4}right)}{8pisqrt{2pi}}tag3
end{align*}$$



I am unable to prove them.



How do we go about to prove these two sums?







sequences-and-series






share|cite|improve this question















share|cite|improve this question













share|cite|improve this question




share|cite|improve this question








edited Jan 7 at 0:02









mrtaurho

6,08771641




6,08771641










asked Jan 1 at 8:17









user583851user583851

518110




518110








  • 2




    $begingroup$
    What made you conjecture them?
    $endgroup$
    – clathratus
    Jan 1 at 8:35










  • $begingroup$
    I suppose that,as in the linked paper, we would need to use hypergeometric functions first summing from $0$ to $p$.
    $endgroup$
    – Claude Leibovici
    Jan 1 at 9:15












  • $begingroup$
    +1 for link to the nice paper. May be Jack D'Aurizio can shed some light on your conjectured identities.
    $endgroup$
    – Paramanand Singh
    Jan 1 at 15:41












  • $begingroup$
    All the given series can be written in terms of the moments of $K(x)$ or $E(x)$, i.e. $int_{0}^{1}x^eta K(x),dx$ and $int_{0}^{1}x^eta E(x),dx$. Since the complete elliptic integrals have simple Fourier-Legendre expansions, these identities can be proved through harmonic analysis, too. That's the whole point of the paper in a nutshell ;)
    $endgroup$
    – Jack D'Aurizio
    Jan 1 at 20:28














  • 2




    $begingroup$
    What made you conjecture them?
    $endgroup$
    – clathratus
    Jan 1 at 8:35










  • $begingroup$
    I suppose that,as in the linked paper, we would need to use hypergeometric functions first summing from $0$ to $p$.
    $endgroup$
    – Claude Leibovici
    Jan 1 at 9:15












  • $begingroup$
    +1 for link to the nice paper. May be Jack D'Aurizio can shed some light on your conjectured identities.
    $endgroup$
    – Paramanand Singh
    Jan 1 at 15:41












  • $begingroup$
    All the given series can be written in terms of the moments of $K(x)$ or $E(x)$, i.e. $int_{0}^{1}x^eta K(x),dx$ and $int_{0}^{1}x^eta E(x),dx$. Since the complete elliptic integrals have simple Fourier-Legendre expansions, these identities can be proved through harmonic analysis, too. That's the whole point of the paper in a nutshell ;)
    $endgroup$
    – Jack D'Aurizio
    Jan 1 at 20:28








2




2




$begingroup$
What made you conjecture them?
$endgroup$
– clathratus
Jan 1 at 8:35




$begingroup$
What made you conjecture them?
$endgroup$
– clathratus
Jan 1 at 8:35












$begingroup$
I suppose that,as in the linked paper, we would need to use hypergeometric functions first summing from $0$ to $p$.
$endgroup$
– Claude Leibovici
Jan 1 at 9:15






$begingroup$
I suppose that,as in the linked paper, we would need to use hypergeometric functions first summing from $0$ to $p$.
$endgroup$
– Claude Leibovici
Jan 1 at 9:15














$begingroup$
+1 for link to the nice paper. May be Jack D'Aurizio can shed some light on your conjectured identities.
$endgroup$
– Paramanand Singh
Jan 1 at 15:41






$begingroup$
+1 for link to the nice paper. May be Jack D'Aurizio can shed some light on your conjectured identities.
$endgroup$
– Paramanand Singh
Jan 1 at 15:41














$begingroup$
All the given series can be written in terms of the moments of $K(x)$ or $E(x)$, i.e. $int_{0}^{1}x^eta K(x),dx$ and $int_{0}^{1}x^eta E(x),dx$. Since the complete elliptic integrals have simple Fourier-Legendre expansions, these identities can be proved through harmonic analysis, too. That's the whole point of the paper in a nutshell ;)
$endgroup$
– Jack D'Aurizio
Jan 1 at 20:28




$begingroup$
All the given series can be written in terms of the moments of $K(x)$ or $E(x)$, i.e. $int_{0}^{1}x^eta K(x),dx$ and $int_{0}^{1}x^eta E(x),dx$. Since the complete elliptic integrals have simple Fourier-Legendre expansions, these identities can be proved through harmonic analysis, too. That's the whole point of the paper in a nutshell ;)
$endgroup$
– Jack D'Aurizio
Jan 1 at 20:28










1 Answer
1






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oldest

votes


















10












$begingroup$

From the beautiful answer by @robjohn, we learn
begin{equation}
sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}frac{r^{2k-1}}{(2k-1)^2}
=frac2{pi r}int_0^1frac{left(rxarcsin(rx)+sqrt{1-r^2x^2}right),mathrm{d}x}{sqrt{1-x^2}}
end{equation}

Plugging in $r=i$,
begin{align}
sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}frac{(-1)^k}{(2k-1)^2}
&=frac{2}{pi}int_0^1frac{left(ixarcsin(ix)+sqrt{1+x^2}right),mathrm{d}x}{sqrt{1-x^2}}\
&=frac{2}{pi}int_0^1frac{sqrt{1+x^2}-xsinh^{-1}(x)}{sqrt{1-x^2}},mathrm{d}x\
&=frac{2}{pi}int_0^1left[ frac{sqrt{1+x^2}}{sqrt{1-x^2}}-frac{sqrt{1-x^2}}{sqrt{1+x^2}}right],mathrm{d}x\
&=frac{4}{pi}int_0^1 frac{x^2}{sqrt{1-x^4}},mathrm{d}x\
&=frac{1}{pi}Bleft( frac{3}{4},frac{1}{2} right)\
&=frac{4sqrt{2pi}}{Gamma^2left( frac{1}{4} right)}
end{align}

(the integration of the $sinh^{-1}$ term was made by parts).



For the second expression, we decompose
begin{equation}
frac{n^2}{left( 2n-1 right)^2}=frac{1}{4}+frac{1}{2}frac{1}{2n-1}+frac{1}{4}frac{1}{left( 2n-1 right)^2}
end{equation}

From the linked answer we have also
begin{equation}
sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}frac{r^{2k-1}}{2k-1}
=frac1{pi r}int_0^1frac{-sqrt{1-r^2x},mathrm{d}x}{sqrt{x(1-x)}}
end{equation}

and thus, with $r=i$
begin{align}
sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}frac{(-1)^k}{2k-1}
&=-frac1{pi }int_0^1frac{sqrt{1+x},mathrm{d}x}{sqrt{x(1-x)}}\
&=-frac2{pi }int_0^1frac{sqrt{1+t^2}}{sqrt{1-t^2}},mathrm{d}t\
&=-frac{2sqrt{2}}{pi}Eleft( frac{1}{sqrt{2}} right)\
&=-frac{2sqrt{2}}{pi}left[ frac{Gamma^2left( frac{1}{4} right)}{8sqrt{pi}}+frac{pi^{3/2}}{Gamma^2left( frac{1}{4} right)}right]
end{align}

where the singular value $k_1$ for the elliptic integral is used. We may also express from the answer
begin{equation}
sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}r^{2k}
=frac1piint_0^1frac{mathrm{d}x}{sqrt{1-r^2x}sqrt{x(1-x)}}
end{equation}

which, with $r=i$ again, gives
begin{align}
sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}(-1)^{k}
&=frac1piint_0^1frac{mathrm{d}x}{sqrt{1+x}sqrt{x(1-x)}}\
&=frac2piint_0^1frac{dt}{sqrt{1-t^4}}\
&=frac{1}{2pi}Bleft(frac{1}{4}, frac{1}{2} right)\
&=frac{sqrt{2pi}}{2Gamma^2left(frac{3}{4}right)}
end{align}

Then,
begin{align}
S&=sum_{n=0}^{infty}frac{(-1)^nn^2}{(2n-1)^2}left[frac{1}{4^n}{2n choose n}right]^2\
&=frac{sqrt{2pi}}{8Gamma^2left(frac{3}{4}right)}
-frac{sqrt{2}}{pi}left[ frac{Gamma^2left( frac{1}{4} right)}{8sqrt{pi}}+frac{pi^{3/2}}{Gamma^2left( frac{1}{4} right)}right]+frac{sqrt{2pi}}{Gamma^2left( frac{1}{4} right)}
end{align}

Using the reflection formula $Gamma(3/4)Gamma(1/4)=pisqrt{2}$, we obtain finally
begin{equation}
S=-frac{Gamma^2left( frac{1}{4} right)}{8sqrt2pi^{3/2}}
end{equation}

as expected.



Edit (simpler derivation for the second expression)



For the second expression, it is easier to leave the integrals unevaluated in the decomposition:
begin{equation}
S=int_0^1left[frac{1}{2pi}frac{1}{sqrt{1-x^4}}-frac{1}{pi}sqrt{frac{1+x^2}{1-x^2}}+frac{1}{pi}frac{x^2}{sqrt{1-x^4}} right],dx
end{equation}

or
begin{align}
S&=-frac{1}{2pi}int_0^1frac{dx}{sqrt{1-x^4}}\
&=-frac{1}{8pi}int_0^1 left( 1-u right)^{-1/2}u^{-3/4},du\
&=-frac{Bleft( frac{1}{4},frac{1}{2} right)}{8pi}
end{align}

and the result follows from the $Gamma$ reflection formula.






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    10












    $begingroup$

    From the beautiful answer by @robjohn, we learn
    begin{equation}
    sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}frac{r^{2k-1}}{(2k-1)^2}
    =frac2{pi r}int_0^1frac{left(rxarcsin(rx)+sqrt{1-r^2x^2}right),mathrm{d}x}{sqrt{1-x^2}}
    end{equation}

    Plugging in $r=i$,
    begin{align}
    sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}frac{(-1)^k}{(2k-1)^2}
    &=frac{2}{pi}int_0^1frac{left(ixarcsin(ix)+sqrt{1+x^2}right),mathrm{d}x}{sqrt{1-x^2}}\
    &=frac{2}{pi}int_0^1frac{sqrt{1+x^2}-xsinh^{-1}(x)}{sqrt{1-x^2}},mathrm{d}x\
    &=frac{2}{pi}int_0^1left[ frac{sqrt{1+x^2}}{sqrt{1-x^2}}-frac{sqrt{1-x^2}}{sqrt{1+x^2}}right],mathrm{d}x\
    &=frac{4}{pi}int_0^1 frac{x^2}{sqrt{1-x^4}},mathrm{d}x\
    &=frac{1}{pi}Bleft( frac{3}{4},frac{1}{2} right)\
    &=frac{4sqrt{2pi}}{Gamma^2left( frac{1}{4} right)}
    end{align}

    (the integration of the $sinh^{-1}$ term was made by parts).



    For the second expression, we decompose
    begin{equation}
    frac{n^2}{left( 2n-1 right)^2}=frac{1}{4}+frac{1}{2}frac{1}{2n-1}+frac{1}{4}frac{1}{left( 2n-1 right)^2}
    end{equation}

    From the linked answer we have also
    begin{equation}
    sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}frac{r^{2k-1}}{2k-1}
    =frac1{pi r}int_0^1frac{-sqrt{1-r^2x},mathrm{d}x}{sqrt{x(1-x)}}
    end{equation}

    and thus, with $r=i$
    begin{align}
    sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}frac{(-1)^k}{2k-1}
    &=-frac1{pi }int_0^1frac{sqrt{1+x},mathrm{d}x}{sqrt{x(1-x)}}\
    &=-frac2{pi }int_0^1frac{sqrt{1+t^2}}{sqrt{1-t^2}},mathrm{d}t\
    &=-frac{2sqrt{2}}{pi}Eleft( frac{1}{sqrt{2}} right)\
    &=-frac{2sqrt{2}}{pi}left[ frac{Gamma^2left( frac{1}{4} right)}{8sqrt{pi}}+frac{pi^{3/2}}{Gamma^2left( frac{1}{4} right)}right]
    end{align}

    where the singular value $k_1$ for the elliptic integral is used. We may also express from the answer
    begin{equation}
    sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}r^{2k}
    =frac1piint_0^1frac{mathrm{d}x}{sqrt{1-r^2x}sqrt{x(1-x)}}
    end{equation}

    which, with $r=i$ again, gives
    begin{align}
    sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}(-1)^{k}
    &=frac1piint_0^1frac{mathrm{d}x}{sqrt{1+x}sqrt{x(1-x)}}\
    &=frac2piint_0^1frac{dt}{sqrt{1-t^4}}\
    &=frac{1}{2pi}Bleft(frac{1}{4}, frac{1}{2} right)\
    &=frac{sqrt{2pi}}{2Gamma^2left(frac{3}{4}right)}
    end{align}

    Then,
    begin{align}
    S&=sum_{n=0}^{infty}frac{(-1)^nn^2}{(2n-1)^2}left[frac{1}{4^n}{2n choose n}right]^2\
    &=frac{sqrt{2pi}}{8Gamma^2left(frac{3}{4}right)}
    -frac{sqrt{2}}{pi}left[ frac{Gamma^2left( frac{1}{4} right)}{8sqrt{pi}}+frac{pi^{3/2}}{Gamma^2left( frac{1}{4} right)}right]+frac{sqrt{2pi}}{Gamma^2left( frac{1}{4} right)}
    end{align}

    Using the reflection formula $Gamma(3/4)Gamma(1/4)=pisqrt{2}$, we obtain finally
    begin{equation}
    S=-frac{Gamma^2left( frac{1}{4} right)}{8sqrt2pi^{3/2}}
    end{equation}

    as expected.



    Edit (simpler derivation for the second expression)



    For the second expression, it is easier to leave the integrals unevaluated in the decomposition:
    begin{equation}
    S=int_0^1left[frac{1}{2pi}frac{1}{sqrt{1-x^4}}-frac{1}{pi}sqrt{frac{1+x^2}{1-x^2}}+frac{1}{pi}frac{x^2}{sqrt{1-x^4}} right],dx
    end{equation}

    or
    begin{align}
    S&=-frac{1}{2pi}int_0^1frac{dx}{sqrt{1-x^4}}\
    &=-frac{1}{8pi}int_0^1 left( 1-u right)^{-1/2}u^{-3/4},du\
    &=-frac{Bleft( frac{1}{4},frac{1}{2} right)}{8pi}
    end{align}

    and the result follows from the $Gamma$ reflection formula.






    share|cite|improve this answer











    $endgroup$


















      10












      $begingroup$

      From the beautiful answer by @robjohn, we learn
      begin{equation}
      sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}frac{r^{2k-1}}{(2k-1)^2}
      =frac2{pi r}int_0^1frac{left(rxarcsin(rx)+sqrt{1-r^2x^2}right),mathrm{d}x}{sqrt{1-x^2}}
      end{equation}

      Plugging in $r=i$,
      begin{align}
      sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}frac{(-1)^k}{(2k-1)^2}
      &=frac{2}{pi}int_0^1frac{left(ixarcsin(ix)+sqrt{1+x^2}right),mathrm{d}x}{sqrt{1-x^2}}\
      &=frac{2}{pi}int_0^1frac{sqrt{1+x^2}-xsinh^{-1}(x)}{sqrt{1-x^2}},mathrm{d}x\
      &=frac{2}{pi}int_0^1left[ frac{sqrt{1+x^2}}{sqrt{1-x^2}}-frac{sqrt{1-x^2}}{sqrt{1+x^2}}right],mathrm{d}x\
      &=frac{4}{pi}int_0^1 frac{x^2}{sqrt{1-x^4}},mathrm{d}x\
      &=frac{1}{pi}Bleft( frac{3}{4},frac{1}{2} right)\
      &=frac{4sqrt{2pi}}{Gamma^2left( frac{1}{4} right)}
      end{align}

      (the integration of the $sinh^{-1}$ term was made by parts).



      For the second expression, we decompose
      begin{equation}
      frac{n^2}{left( 2n-1 right)^2}=frac{1}{4}+frac{1}{2}frac{1}{2n-1}+frac{1}{4}frac{1}{left( 2n-1 right)^2}
      end{equation}

      From the linked answer we have also
      begin{equation}
      sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}frac{r^{2k-1}}{2k-1}
      =frac1{pi r}int_0^1frac{-sqrt{1-r^2x},mathrm{d}x}{sqrt{x(1-x)}}
      end{equation}

      and thus, with $r=i$
      begin{align}
      sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}frac{(-1)^k}{2k-1}
      &=-frac1{pi }int_0^1frac{sqrt{1+x},mathrm{d}x}{sqrt{x(1-x)}}\
      &=-frac2{pi }int_0^1frac{sqrt{1+t^2}}{sqrt{1-t^2}},mathrm{d}t\
      &=-frac{2sqrt{2}}{pi}Eleft( frac{1}{sqrt{2}} right)\
      &=-frac{2sqrt{2}}{pi}left[ frac{Gamma^2left( frac{1}{4} right)}{8sqrt{pi}}+frac{pi^{3/2}}{Gamma^2left( frac{1}{4} right)}right]
      end{align}

      where the singular value $k_1$ for the elliptic integral is used. We may also express from the answer
      begin{equation}
      sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}r^{2k}
      =frac1piint_0^1frac{mathrm{d}x}{sqrt{1-r^2x}sqrt{x(1-x)}}
      end{equation}

      which, with $r=i$ again, gives
      begin{align}
      sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}(-1)^{k}
      &=frac1piint_0^1frac{mathrm{d}x}{sqrt{1+x}sqrt{x(1-x)}}\
      &=frac2piint_0^1frac{dt}{sqrt{1-t^4}}\
      &=frac{1}{2pi}Bleft(frac{1}{4}, frac{1}{2} right)\
      &=frac{sqrt{2pi}}{2Gamma^2left(frac{3}{4}right)}
      end{align}

      Then,
      begin{align}
      S&=sum_{n=0}^{infty}frac{(-1)^nn^2}{(2n-1)^2}left[frac{1}{4^n}{2n choose n}right]^2\
      &=frac{sqrt{2pi}}{8Gamma^2left(frac{3}{4}right)}
      -frac{sqrt{2}}{pi}left[ frac{Gamma^2left( frac{1}{4} right)}{8sqrt{pi}}+frac{pi^{3/2}}{Gamma^2left( frac{1}{4} right)}right]+frac{sqrt{2pi}}{Gamma^2left( frac{1}{4} right)}
      end{align}

      Using the reflection formula $Gamma(3/4)Gamma(1/4)=pisqrt{2}$, we obtain finally
      begin{equation}
      S=-frac{Gamma^2left( frac{1}{4} right)}{8sqrt2pi^{3/2}}
      end{equation}

      as expected.



      Edit (simpler derivation for the second expression)



      For the second expression, it is easier to leave the integrals unevaluated in the decomposition:
      begin{equation}
      S=int_0^1left[frac{1}{2pi}frac{1}{sqrt{1-x^4}}-frac{1}{pi}sqrt{frac{1+x^2}{1-x^2}}+frac{1}{pi}frac{x^2}{sqrt{1-x^4}} right],dx
      end{equation}

      or
      begin{align}
      S&=-frac{1}{2pi}int_0^1frac{dx}{sqrt{1-x^4}}\
      &=-frac{1}{8pi}int_0^1 left( 1-u right)^{-1/2}u^{-3/4},du\
      &=-frac{Bleft( frac{1}{4},frac{1}{2} right)}{8pi}
      end{align}

      and the result follows from the $Gamma$ reflection formula.






      share|cite|improve this answer











      $endgroup$
















        10












        10








        10





        $begingroup$

        From the beautiful answer by @robjohn, we learn
        begin{equation}
        sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}frac{r^{2k-1}}{(2k-1)^2}
        =frac2{pi r}int_0^1frac{left(rxarcsin(rx)+sqrt{1-r^2x^2}right),mathrm{d}x}{sqrt{1-x^2}}
        end{equation}

        Plugging in $r=i$,
        begin{align}
        sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}frac{(-1)^k}{(2k-1)^2}
        &=frac{2}{pi}int_0^1frac{left(ixarcsin(ix)+sqrt{1+x^2}right),mathrm{d}x}{sqrt{1-x^2}}\
        &=frac{2}{pi}int_0^1frac{sqrt{1+x^2}-xsinh^{-1}(x)}{sqrt{1-x^2}},mathrm{d}x\
        &=frac{2}{pi}int_0^1left[ frac{sqrt{1+x^2}}{sqrt{1-x^2}}-frac{sqrt{1-x^2}}{sqrt{1+x^2}}right],mathrm{d}x\
        &=frac{4}{pi}int_0^1 frac{x^2}{sqrt{1-x^4}},mathrm{d}x\
        &=frac{1}{pi}Bleft( frac{3}{4},frac{1}{2} right)\
        &=frac{4sqrt{2pi}}{Gamma^2left( frac{1}{4} right)}
        end{align}

        (the integration of the $sinh^{-1}$ term was made by parts).



        For the second expression, we decompose
        begin{equation}
        frac{n^2}{left( 2n-1 right)^2}=frac{1}{4}+frac{1}{2}frac{1}{2n-1}+frac{1}{4}frac{1}{left( 2n-1 right)^2}
        end{equation}

        From the linked answer we have also
        begin{equation}
        sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}frac{r^{2k-1}}{2k-1}
        =frac1{pi r}int_0^1frac{-sqrt{1-r^2x},mathrm{d}x}{sqrt{x(1-x)}}
        end{equation}

        and thus, with $r=i$
        begin{align}
        sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}frac{(-1)^k}{2k-1}
        &=-frac1{pi }int_0^1frac{sqrt{1+x},mathrm{d}x}{sqrt{x(1-x)}}\
        &=-frac2{pi }int_0^1frac{sqrt{1+t^2}}{sqrt{1-t^2}},mathrm{d}t\
        &=-frac{2sqrt{2}}{pi}Eleft( frac{1}{sqrt{2}} right)\
        &=-frac{2sqrt{2}}{pi}left[ frac{Gamma^2left( frac{1}{4} right)}{8sqrt{pi}}+frac{pi^{3/2}}{Gamma^2left( frac{1}{4} right)}right]
        end{align}

        where the singular value $k_1$ for the elliptic integral is used. We may also express from the answer
        begin{equation}
        sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}r^{2k}
        =frac1piint_0^1frac{mathrm{d}x}{sqrt{1-r^2x}sqrt{x(1-x)}}
        end{equation}

        which, with $r=i$ again, gives
        begin{align}
        sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}(-1)^{k}
        &=frac1piint_0^1frac{mathrm{d}x}{sqrt{1+x}sqrt{x(1-x)}}\
        &=frac2piint_0^1frac{dt}{sqrt{1-t^4}}\
        &=frac{1}{2pi}Bleft(frac{1}{4}, frac{1}{2} right)\
        &=frac{sqrt{2pi}}{2Gamma^2left(frac{3}{4}right)}
        end{align}

        Then,
        begin{align}
        S&=sum_{n=0}^{infty}frac{(-1)^nn^2}{(2n-1)^2}left[frac{1}{4^n}{2n choose n}right]^2\
        &=frac{sqrt{2pi}}{8Gamma^2left(frac{3}{4}right)}
        -frac{sqrt{2}}{pi}left[ frac{Gamma^2left( frac{1}{4} right)}{8sqrt{pi}}+frac{pi^{3/2}}{Gamma^2left( frac{1}{4} right)}right]+frac{sqrt{2pi}}{Gamma^2left( frac{1}{4} right)}
        end{align}

        Using the reflection formula $Gamma(3/4)Gamma(1/4)=pisqrt{2}$, we obtain finally
        begin{equation}
        S=-frac{Gamma^2left( frac{1}{4} right)}{8sqrt2pi^{3/2}}
        end{equation}

        as expected.



        Edit (simpler derivation for the second expression)



        For the second expression, it is easier to leave the integrals unevaluated in the decomposition:
        begin{equation}
        S=int_0^1left[frac{1}{2pi}frac{1}{sqrt{1-x^4}}-frac{1}{pi}sqrt{frac{1+x^2}{1-x^2}}+frac{1}{pi}frac{x^2}{sqrt{1-x^4}} right],dx
        end{equation}

        or
        begin{align}
        S&=-frac{1}{2pi}int_0^1frac{dx}{sqrt{1-x^4}}\
        &=-frac{1}{8pi}int_0^1 left( 1-u right)^{-1/2}u^{-3/4},du\
        &=-frac{Bleft( frac{1}{4},frac{1}{2} right)}{8pi}
        end{align}

        and the result follows from the $Gamma$ reflection formula.






        share|cite|improve this answer











        $endgroup$



        From the beautiful answer by @robjohn, we learn
        begin{equation}
        sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}frac{r^{2k-1}}{(2k-1)^2}
        =frac2{pi r}int_0^1frac{left(rxarcsin(rx)+sqrt{1-r^2x^2}right),mathrm{d}x}{sqrt{1-x^2}}
        end{equation}

        Plugging in $r=i$,
        begin{align}
        sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}frac{(-1)^k}{(2k-1)^2}
        &=frac{2}{pi}int_0^1frac{left(ixarcsin(ix)+sqrt{1+x^2}right),mathrm{d}x}{sqrt{1-x^2}}\
        &=frac{2}{pi}int_0^1frac{sqrt{1+x^2}-xsinh^{-1}(x)}{sqrt{1-x^2}},mathrm{d}x\
        &=frac{2}{pi}int_0^1left[ frac{sqrt{1+x^2}}{sqrt{1-x^2}}-frac{sqrt{1-x^2}}{sqrt{1+x^2}}right],mathrm{d}x\
        &=frac{4}{pi}int_0^1 frac{x^2}{sqrt{1-x^4}},mathrm{d}x\
        &=frac{1}{pi}Bleft( frac{3}{4},frac{1}{2} right)\
        &=frac{4sqrt{2pi}}{Gamma^2left( frac{1}{4} right)}
        end{align}

        (the integration of the $sinh^{-1}$ term was made by parts).



        For the second expression, we decompose
        begin{equation}
        frac{n^2}{left( 2n-1 right)^2}=frac{1}{4}+frac{1}{2}frac{1}{2n-1}+frac{1}{4}frac{1}{left( 2n-1 right)^2}
        end{equation}

        From the linked answer we have also
        begin{equation}
        sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}frac{r^{2k-1}}{2k-1}
        =frac1{pi r}int_0^1frac{-sqrt{1-r^2x},mathrm{d}x}{sqrt{x(1-x)}}
        end{equation}

        and thus, with $r=i$
        begin{align}
        sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}frac{(-1)^k}{2k-1}
        &=-frac1{pi }int_0^1frac{sqrt{1+x},mathrm{d}x}{sqrt{x(1-x)}}\
        &=-frac2{pi }int_0^1frac{sqrt{1+t^2}}{sqrt{1-t^2}},mathrm{d}t\
        &=-frac{2sqrt{2}}{pi}Eleft( frac{1}{sqrt{2}} right)\
        &=-frac{2sqrt{2}}{pi}left[ frac{Gamma^2left( frac{1}{4} right)}{8sqrt{pi}}+frac{pi^{3/2}}{Gamma^2left( frac{1}{4} right)}right]
        end{align}

        where the singular value $k_1$ for the elliptic integral is used. We may also express from the answer
        begin{equation}
        sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}r^{2k}
        =frac1piint_0^1frac{mathrm{d}x}{sqrt{1-r^2x}sqrt{x(1-x)}}
        end{equation}

        which, with $r=i$ again, gives
        begin{align}
        sum_{k=0}^inftyfrac{binom{2k}{k}^2}{16^k}(-1)^{k}
        &=frac1piint_0^1frac{mathrm{d}x}{sqrt{1+x}sqrt{x(1-x)}}\
        &=frac2piint_0^1frac{dt}{sqrt{1-t^4}}\
        &=frac{1}{2pi}Bleft(frac{1}{4}, frac{1}{2} right)\
        &=frac{sqrt{2pi}}{2Gamma^2left(frac{3}{4}right)}
        end{align}

        Then,
        begin{align}
        S&=sum_{n=0}^{infty}frac{(-1)^nn^2}{(2n-1)^2}left[frac{1}{4^n}{2n choose n}right]^2\
        &=frac{sqrt{2pi}}{8Gamma^2left(frac{3}{4}right)}
        -frac{sqrt{2}}{pi}left[ frac{Gamma^2left( frac{1}{4} right)}{8sqrt{pi}}+frac{pi^{3/2}}{Gamma^2left( frac{1}{4} right)}right]+frac{sqrt{2pi}}{Gamma^2left( frac{1}{4} right)}
        end{align}

        Using the reflection formula $Gamma(3/4)Gamma(1/4)=pisqrt{2}$, we obtain finally
        begin{equation}
        S=-frac{Gamma^2left( frac{1}{4} right)}{8sqrt2pi^{3/2}}
        end{equation}

        as expected.



        Edit (simpler derivation for the second expression)



        For the second expression, it is easier to leave the integrals unevaluated in the decomposition:
        begin{equation}
        S=int_0^1left[frac{1}{2pi}frac{1}{sqrt{1-x^4}}-frac{1}{pi}sqrt{frac{1+x^2}{1-x^2}}+frac{1}{pi}frac{x^2}{sqrt{1-x^4}} right],dx
        end{equation}

        or
        begin{align}
        S&=-frac{1}{2pi}int_0^1frac{dx}{sqrt{1-x^4}}\
        &=-frac{1}{8pi}int_0^1 left( 1-u right)^{-1/2}u^{-3/4},du\
        &=-frac{Bleft( frac{1}{4},frac{1}{2} right)}{8pi}
        end{align}

        and the result follows from the $Gamma$ reflection formula.







        share|cite|improve this answer














        share|cite|improve this answer



        share|cite|improve this answer








        edited Jan 7 at 20:15

























        answered Jan 1 at 18:44









        Paul EntaPaul Enta

        5,36111434




        5,36111434






























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