$sum_n=1^inftyfrac1n^6=fracpi^6945$ by Fourier series of $x^2$

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Prove that
$$sum_n=1^inftyfrac1n^6=fracpi^6945$$ by the Fourier series of $x^2$.




By Parseval's identity, I can only show $sum_n=1^inftyfrac1n^4=fracpi^490$. Could you please give me some hints?







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  • 2




    I think you need to use the fourier series of x^3 to directly use Parseval's identity.
    – BenLaurense
    Sep 30 '16 at 16:20










  • ... or integrate the Fourier series of $x^2$, then apply Parseval's theorem. However, in order to implement this idea it is better to take a different quadratic polynomial, namely $B_2left(fracx2piright)$.
    – Jack D'Aurizio♦
    Sep 30 '16 at 16:57















up vote
4
down vote

favorite
4













Prove that
$$sum_n=1^inftyfrac1n^6=fracpi^6945$$ by the Fourier series of $x^2$.




By Parseval's identity, I can only show $sum_n=1^inftyfrac1n^4=fracpi^490$. Could you please give me some hints?







share|cite|improve this question

















  • 2




    I think you need to use the fourier series of x^3 to directly use Parseval's identity.
    – BenLaurense
    Sep 30 '16 at 16:20










  • ... or integrate the Fourier series of $x^2$, then apply Parseval's theorem. However, in order to implement this idea it is better to take a different quadratic polynomial, namely $B_2left(fracx2piright)$.
    – Jack D'Aurizio♦
    Sep 30 '16 at 16:57













up vote
4
down vote

favorite
4









up vote
4
down vote

favorite
4






4






Prove that
$$sum_n=1^inftyfrac1n^6=fracpi^6945$$ by the Fourier series of $x^2$.




By Parseval's identity, I can only show $sum_n=1^inftyfrac1n^4=fracpi^490$. Could you please give me some hints?







share|cite|improve this question














Prove that
$$sum_n=1^inftyfrac1n^6=fracpi^6945$$ by the Fourier series of $x^2$.




By Parseval's identity, I can only show $sum_n=1^inftyfrac1n^4=fracpi^490$. Could you please give me some hints?









share|cite|improve this question












share|cite|improve this question




share|cite|improve this question








edited Oct 1 '16 at 5:21









Parcly Taxel

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asked Sep 30 '16 at 16:14









Longitude

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  • 2




    I think you need to use the fourier series of x^3 to directly use Parseval's identity.
    – BenLaurense
    Sep 30 '16 at 16:20










  • ... or integrate the Fourier series of $x^2$, then apply Parseval's theorem. However, in order to implement this idea it is better to take a different quadratic polynomial, namely $B_2left(fracx2piright)$.
    – Jack D'Aurizio♦
    Sep 30 '16 at 16:57













  • 2




    I think you need to use the fourier series of x^3 to directly use Parseval's identity.
    – BenLaurense
    Sep 30 '16 at 16:20










  • ... or integrate the Fourier series of $x^2$, then apply Parseval's theorem. However, in order to implement this idea it is better to take a different quadratic polynomial, namely $B_2left(fracx2piright)$.
    – Jack D'Aurizio♦
    Sep 30 '16 at 16:57








2




2




I think you need to use the fourier series of x^3 to directly use Parseval's identity.
– BenLaurense
Sep 30 '16 at 16:20




I think you need to use the fourier series of x^3 to directly use Parseval's identity.
– BenLaurense
Sep 30 '16 at 16:20












... or integrate the Fourier series of $x^2$, then apply Parseval's theorem. However, in order to implement this idea it is better to take a different quadratic polynomial, namely $B_2left(fracx2piright)$.
– Jack D'Aurizio♦
Sep 30 '16 at 16:57





... or integrate the Fourier series of $x^2$, then apply Parseval's theorem. However, in order to implement this idea it is better to take a different quadratic polynomial, namely $B_2left(fracx2piright)$.
– Jack D'Aurizio♦
Sep 30 '16 at 16:57











1 Answer
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We may start from
$$ f_1(x) = sum_ngeq 1fracsin(nx)n tag1$$
that is the Fourier series of a sawtooth wave, equal to $fracpi-x2$ on the interval $I=(0,2pi)$.

By termwise integration, we get that
$$ forall xin I,quad sum_ngeq 1frac1-cos(nx)n^2 = frac2pi x-x^24$$
hence:
$$ forall xin I,quad f_2(x) = sum_ngeq 1fraccos(nx)n^2=fracpi^26-fracpi x2+fracx^24tag2 $$
$$ forall xin I,quad f_3(x) = sum_ngeq 1fracsin(nx)n^3=fracpi^2 x6-fracpi x^24+fracx^312tag3 $$
(the integration constants are computed from the fact that $f_j(x)$ has to have mean zero over $I$)
and by Parseval's theorem
$$ zeta(6) = frac1piint_0^2pif_3(x)^2,dx = frac2pi^69int_0^1left[x(x-1)(2x-1)right]^2,dx=colorredfracpi^6945.tag4$$
With the same approach it is not difficult to prove that for any $ngeq 1$, $zeta(2n)$ is a rational multiple of $pi^2nint_0^1B_n(x)^2,dx$, where $B_n(x)$ is a Bernoulli polynomial.






share|cite|improve this answer























  • it is not 100% clear that you substract the mean such that $f_j(x)$ has zero mean
    – reuns
    Sep 30 '16 at 16:40











  • @user1952009: the expression for $f_2(x)$ is derived from $f_2(x)=zeta(2)-sum_ngeq 1frac1-cos(nx)n^2$ and the expression for $f_3(x)$ is derived from $f_3(pi)=0$. Anyway, answer improved. Thanks for the suggestion.
    – Jack D'Aurizio♦
    Sep 30 '16 at 16:43











  • But where is the Fourier series of $x^2$?
    – Longitude
    Sep 30 '16 at 16:56










  • @Longitude: it is part of $(2)$. See my comment under your question.
    – Jack D'Aurizio♦
    Sep 30 '16 at 16:57










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1 Answer
1






active

oldest

votes








1 Answer
1






active

oldest

votes









active

oldest

votes






active

oldest

votes








up vote
3
down vote













We may start from
$$ f_1(x) = sum_ngeq 1fracsin(nx)n tag1$$
that is the Fourier series of a sawtooth wave, equal to $fracpi-x2$ on the interval $I=(0,2pi)$.

By termwise integration, we get that
$$ forall xin I,quad sum_ngeq 1frac1-cos(nx)n^2 = frac2pi x-x^24$$
hence:
$$ forall xin I,quad f_2(x) = sum_ngeq 1fraccos(nx)n^2=fracpi^26-fracpi x2+fracx^24tag2 $$
$$ forall xin I,quad f_3(x) = sum_ngeq 1fracsin(nx)n^3=fracpi^2 x6-fracpi x^24+fracx^312tag3 $$
(the integration constants are computed from the fact that $f_j(x)$ has to have mean zero over $I$)
and by Parseval's theorem
$$ zeta(6) = frac1piint_0^2pif_3(x)^2,dx = frac2pi^69int_0^1left[x(x-1)(2x-1)right]^2,dx=colorredfracpi^6945.tag4$$
With the same approach it is not difficult to prove that for any $ngeq 1$, $zeta(2n)$ is a rational multiple of $pi^2nint_0^1B_n(x)^2,dx$, where $B_n(x)$ is a Bernoulli polynomial.






share|cite|improve this answer























  • it is not 100% clear that you substract the mean such that $f_j(x)$ has zero mean
    – reuns
    Sep 30 '16 at 16:40











  • @user1952009: the expression for $f_2(x)$ is derived from $f_2(x)=zeta(2)-sum_ngeq 1frac1-cos(nx)n^2$ and the expression for $f_3(x)$ is derived from $f_3(pi)=0$. Anyway, answer improved. Thanks for the suggestion.
    – Jack D'Aurizio♦
    Sep 30 '16 at 16:43











  • But where is the Fourier series of $x^2$?
    – Longitude
    Sep 30 '16 at 16:56










  • @Longitude: it is part of $(2)$. See my comment under your question.
    – Jack D'Aurizio♦
    Sep 30 '16 at 16:57














up vote
3
down vote













We may start from
$$ f_1(x) = sum_ngeq 1fracsin(nx)n tag1$$
that is the Fourier series of a sawtooth wave, equal to $fracpi-x2$ on the interval $I=(0,2pi)$.

By termwise integration, we get that
$$ forall xin I,quad sum_ngeq 1frac1-cos(nx)n^2 = frac2pi x-x^24$$
hence:
$$ forall xin I,quad f_2(x) = sum_ngeq 1fraccos(nx)n^2=fracpi^26-fracpi x2+fracx^24tag2 $$
$$ forall xin I,quad f_3(x) = sum_ngeq 1fracsin(nx)n^3=fracpi^2 x6-fracpi x^24+fracx^312tag3 $$
(the integration constants are computed from the fact that $f_j(x)$ has to have mean zero over $I$)
and by Parseval's theorem
$$ zeta(6) = frac1piint_0^2pif_3(x)^2,dx = frac2pi^69int_0^1left[x(x-1)(2x-1)right]^2,dx=colorredfracpi^6945.tag4$$
With the same approach it is not difficult to prove that for any $ngeq 1$, $zeta(2n)$ is a rational multiple of $pi^2nint_0^1B_n(x)^2,dx$, where $B_n(x)$ is a Bernoulli polynomial.






share|cite|improve this answer























  • it is not 100% clear that you substract the mean such that $f_j(x)$ has zero mean
    – reuns
    Sep 30 '16 at 16:40











  • @user1952009: the expression for $f_2(x)$ is derived from $f_2(x)=zeta(2)-sum_ngeq 1frac1-cos(nx)n^2$ and the expression for $f_3(x)$ is derived from $f_3(pi)=0$. Anyway, answer improved. Thanks for the suggestion.
    – Jack D'Aurizio♦
    Sep 30 '16 at 16:43











  • But where is the Fourier series of $x^2$?
    – Longitude
    Sep 30 '16 at 16:56










  • @Longitude: it is part of $(2)$. See my comment under your question.
    – Jack D'Aurizio♦
    Sep 30 '16 at 16:57












up vote
3
down vote










up vote
3
down vote









We may start from
$$ f_1(x) = sum_ngeq 1fracsin(nx)n tag1$$
that is the Fourier series of a sawtooth wave, equal to $fracpi-x2$ on the interval $I=(0,2pi)$.

By termwise integration, we get that
$$ forall xin I,quad sum_ngeq 1frac1-cos(nx)n^2 = frac2pi x-x^24$$
hence:
$$ forall xin I,quad f_2(x) = sum_ngeq 1fraccos(nx)n^2=fracpi^26-fracpi x2+fracx^24tag2 $$
$$ forall xin I,quad f_3(x) = sum_ngeq 1fracsin(nx)n^3=fracpi^2 x6-fracpi x^24+fracx^312tag3 $$
(the integration constants are computed from the fact that $f_j(x)$ has to have mean zero over $I$)
and by Parseval's theorem
$$ zeta(6) = frac1piint_0^2pif_3(x)^2,dx = frac2pi^69int_0^1left[x(x-1)(2x-1)right]^2,dx=colorredfracpi^6945.tag4$$
With the same approach it is not difficult to prove that for any $ngeq 1$, $zeta(2n)$ is a rational multiple of $pi^2nint_0^1B_n(x)^2,dx$, where $B_n(x)$ is a Bernoulli polynomial.






share|cite|improve this answer















We may start from
$$ f_1(x) = sum_ngeq 1fracsin(nx)n tag1$$
that is the Fourier series of a sawtooth wave, equal to $fracpi-x2$ on the interval $I=(0,2pi)$.

By termwise integration, we get that
$$ forall xin I,quad sum_ngeq 1frac1-cos(nx)n^2 = frac2pi x-x^24$$
hence:
$$ forall xin I,quad f_2(x) = sum_ngeq 1fraccos(nx)n^2=fracpi^26-fracpi x2+fracx^24tag2 $$
$$ forall xin I,quad f_3(x) = sum_ngeq 1fracsin(nx)n^3=fracpi^2 x6-fracpi x^24+fracx^312tag3 $$
(the integration constants are computed from the fact that $f_j(x)$ has to have mean zero over $I$)
and by Parseval's theorem
$$ zeta(6) = frac1piint_0^2pif_3(x)^2,dx = frac2pi^69int_0^1left[x(x-1)(2x-1)right]^2,dx=colorredfracpi^6945.tag4$$
With the same approach it is not difficult to prove that for any $ngeq 1$, $zeta(2n)$ is a rational multiple of $pi^2nint_0^1B_n(x)^2,dx$, where $B_n(x)$ is a Bernoulli polynomial.







share|cite|improve this answer















share|cite|improve this answer



share|cite|improve this answer








edited Sep 30 '16 at 16:45


























answered Sep 30 '16 at 16:32









Jack D'Aurizio♦

269k30261625




269k30261625











  • it is not 100% clear that you substract the mean such that $f_j(x)$ has zero mean
    – reuns
    Sep 30 '16 at 16:40











  • @user1952009: the expression for $f_2(x)$ is derived from $f_2(x)=zeta(2)-sum_ngeq 1frac1-cos(nx)n^2$ and the expression for $f_3(x)$ is derived from $f_3(pi)=0$. Anyway, answer improved. Thanks for the suggestion.
    – Jack D'Aurizio♦
    Sep 30 '16 at 16:43











  • But where is the Fourier series of $x^2$?
    – Longitude
    Sep 30 '16 at 16:56










  • @Longitude: it is part of $(2)$. See my comment under your question.
    – Jack D'Aurizio♦
    Sep 30 '16 at 16:57
















  • it is not 100% clear that you substract the mean such that $f_j(x)$ has zero mean
    – reuns
    Sep 30 '16 at 16:40











  • @user1952009: the expression for $f_2(x)$ is derived from $f_2(x)=zeta(2)-sum_ngeq 1frac1-cos(nx)n^2$ and the expression for $f_3(x)$ is derived from $f_3(pi)=0$. Anyway, answer improved. Thanks for the suggestion.
    – Jack D'Aurizio♦
    Sep 30 '16 at 16:43











  • But where is the Fourier series of $x^2$?
    – Longitude
    Sep 30 '16 at 16:56










  • @Longitude: it is part of $(2)$. See my comment under your question.
    – Jack D'Aurizio♦
    Sep 30 '16 at 16:57















it is not 100% clear that you substract the mean such that $f_j(x)$ has zero mean
– reuns
Sep 30 '16 at 16:40





it is not 100% clear that you substract the mean such that $f_j(x)$ has zero mean
– reuns
Sep 30 '16 at 16:40













@user1952009: the expression for $f_2(x)$ is derived from $f_2(x)=zeta(2)-sum_ngeq 1frac1-cos(nx)n^2$ and the expression for $f_3(x)$ is derived from $f_3(pi)=0$. Anyway, answer improved. Thanks for the suggestion.
– Jack D'Aurizio♦
Sep 30 '16 at 16:43





@user1952009: the expression for $f_2(x)$ is derived from $f_2(x)=zeta(2)-sum_ngeq 1frac1-cos(nx)n^2$ and the expression for $f_3(x)$ is derived from $f_3(pi)=0$. Anyway, answer improved. Thanks for the suggestion.
– Jack D'Aurizio♦
Sep 30 '16 at 16:43













But where is the Fourier series of $x^2$?
– Longitude
Sep 30 '16 at 16:56




But where is the Fourier series of $x^2$?
– Longitude
Sep 30 '16 at 16:56












@Longitude: it is part of $(2)$. See my comment under your question.
– Jack D'Aurizio♦
Sep 30 '16 at 16:57




@Longitude: it is part of $(2)$. See my comment under your question.
– Jack D'Aurizio♦
Sep 30 '16 at 16:57












 

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