recurrence relation for $zeta(2n)$
$begingroup$
I found this formula. Is it correct?
For $ninBbb N, ngeq2$,
$$zeta(2n)=frac{2npi^{2n}}{Gamma(2n+2)}+sum_{k=0}^{n-2}(-1)^{k-n}frac{pi^{2n-2k-2}}{Gamma(2n-2k)}zeta(2k+2)$$
Here's my proof.
Assume $mgeq2$ is an even number. We start by finding the Fourier series expansion for $x^m$. We define
$$a_k(m)=frac1piint_{-pi}^{pi}x^mcos(kx)mathrm dx$$
$$b_k(m)=frac1piint_{-pi}^{pi}x^msin(kx)mathrm dx$$
Hence we know that
$$x^m=frac{a_0(m)}2+sum_{kgeq1}a_k(m)cos(kx)+b_k(m)sin(kx)$$
And because $m$ is even,
$$x^m=frac{pi^m}{m+1}+sum_{kgeq1}a_k(m)cos(kx)+b_k(m)sin(kx)$$
Next, we start on $b_k(m)$. We make the substitution $x=-t$, and after a little algebra,
$$b_k(m)=0$$
This is because $m$ is even, and thus $(-x)^m=x^m$. Hence we update our series
$$x^m=frac{pi^m}{m+1}+sum_{kgeq1}a_k(m)cos(kx)$$
For $a_k(m)$, I integrated by parts twice to find
$$a_k(m)=(-1)^{k}frac{2mpi^{m-2}}{k^2}-frac{m(m-1)}{k^2}a_k(m-2)$$
Which brought me to the formula
$$a_k(m)=sum_{v=0}^{frac{m}2-1}(-1)^{k+v}frac{2pi^{m-2-2v}}{k^{2+2v}}prod_{i=1}^{2v+1}(m+1-i)$$
Then, plugging $x=pi$ into the Fourier series,
$$pi^m=frac{pi^m}{m+1}+sum_{kgeq1}(-1)^ksum_{v=0}^{frac{m}2-1}(-1)^{k+v}frac{2pi^{m-2-2v}}{k^{2+2v}}prod_{i=1}^{2v+1}(m+1-i)$$
$$frac{mpi^m}{m+1}=sum_{kgeq1}sum_{v=0}^{frac{m}2-1}(-1)^{v}frac{2pi^{m-2-2v}}{k^{2+2v}}prod_{i=1}^{2v+1}(m+1-i)$$
$$frac{mpi^m}{m+1}=sum_{v=0}^{frac{m}2-1}(-1)^{v}2pi^{m-2-2v}prod_{i=1}^{2v+1}(m+1-i)sum_{kgeq1}frac1{k^{2+2v}}$$
$$frac{mpi^m}{m+1}=sum_{v=0}^{frac{m}2-1}(-1)^{v}2pi^{m-2-2v}zeta(2v+2)prod_{i=1}^{2v+1}(m+1-i)$$
Defining
$$c_v(m)=(-1)^v2prod_{i=1}^{2v+1}(m+1-i)$$
We have
$$frac{mpi^m}{m+1}=sum_{v=0}^{frac{m}2-1}pi^{m-2-2v}c_v(m)zeta(2v+2)$$
$$frac{mpi^m}{m+1}=c_{m/2-1}(m)zeta(m)+sum_{v=0}^{frac{m}2-2}pi^{m-2-2v}c_v(m)zeta(2v+2)$$
$$c_{m/2-1}(m)zeta(m)=frac{mpi^{m}}{m+1}-sum_{v=0}^{frac{m}2-2}pi^{m-2-2v}c_v(m)zeta(2v+2)$$
I then replace $m$ with $2n$ and $v$ with $k$ (because I like $k$ better):
$$c_{n-1}(2n)zeta(2n)=frac{2npi^{2n}}{2n+1}-sum_{k=0}^{n-2}pi^{2n-2-2k}c_k(2n)zeta(2k+2)$$
$$zeta(2n)=frac{2npi^{2n}}{(2n+1)c_{n-1}(2n)}-sum_{k=0}^{n-2}pi^{2n-2-2k}frac{c_k(2n)}{c_{n-1}(2n)}zeta(2k+2)$$
At this point I plugged some things into Wolfram Alpha and got
$$zeta(2n)=frac{2npi^{2n}}{Gamma(2n+2)}+sum_{k=0}^{n-2}(-1)^{k-n}frac{pi^{2n-2k-2}}{Gamma(2n-2k)}zeta(2k+2)$$
I have not seen this formula anywhere, and I don't have Mathematica or Wolfram Pro, so the only way for me to feel confident in this formula is by having you look at it. I don't think I broke any rules, so is this formula valid? Are there any alternate forms for it? Thanks.
integration sequences-and-series recurrence-relations fourier-series riemann-zeta
$endgroup$
add a comment |
$begingroup$
I found this formula. Is it correct?
For $ninBbb N, ngeq2$,
$$zeta(2n)=frac{2npi^{2n}}{Gamma(2n+2)}+sum_{k=0}^{n-2}(-1)^{k-n}frac{pi^{2n-2k-2}}{Gamma(2n-2k)}zeta(2k+2)$$
Here's my proof.
Assume $mgeq2$ is an even number. We start by finding the Fourier series expansion for $x^m$. We define
$$a_k(m)=frac1piint_{-pi}^{pi}x^mcos(kx)mathrm dx$$
$$b_k(m)=frac1piint_{-pi}^{pi}x^msin(kx)mathrm dx$$
Hence we know that
$$x^m=frac{a_0(m)}2+sum_{kgeq1}a_k(m)cos(kx)+b_k(m)sin(kx)$$
And because $m$ is even,
$$x^m=frac{pi^m}{m+1}+sum_{kgeq1}a_k(m)cos(kx)+b_k(m)sin(kx)$$
Next, we start on $b_k(m)$. We make the substitution $x=-t$, and after a little algebra,
$$b_k(m)=0$$
This is because $m$ is even, and thus $(-x)^m=x^m$. Hence we update our series
$$x^m=frac{pi^m}{m+1}+sum_{kgeq1}a_k(m)cos(kx)$$
For $a_k(m)$, I integrated by parts twice to find
$$a_k(m)=(-1)^{k}frac{2mpi^{m-2}}{k^2}-frac{m(m-1)}{k^2}a_k(m-2)$$
Which brought me to the formula
$$a_k(m)=sum_{v=0}^{frac{m}2-1}(-1)^{k+v}frac{2pi^{m-2-2v}}{k^{2+2v}}prod_{i=1}^{2v+1}(m+1-i)$$
Then, plugging $x=pi$ into the Fourier series,
$$pi^m=frac{pi^m}{m+1}+sum_{kgeq1}(-1)^ksum_{v=0}^{frac{m}2-1}(-1)^{k+v}frac{2pi^{m-2-2v}}{k^{2+2v}}prod_{i=1}^{2v+1}(m+1-i)$$
$$frac{mpi^m}{m+1}=sum_{kgeq1}sum_{v=0}^{frac{m}2-1}(-1)^{v}frac{2pi^{m-2-2v}}{k^{2+2v}}prod_{i=1}^{2v+1}(m+1-i)$$
$$frac{mpi^m}{m+1}=sum_{v=0}^{frac{m}2-1}(-1)^{v}2pi^{m-2-2v}prod_{i=1}^{2v+1}(m+1-i)sum_{kgeq1}frac1{k^{2+2v}}$$
$$frac{mpi^m}{m+1}=sum_{v=0}^{frac{m}2-1}(-1)^{v}2pi^{m-2-2v}zeta(2v+2)prod_{i=1}^{2v+1}(m+1-i)$$
Defining
$$c_v(m)=(-1)^v2prod_{i=1}^{2v+1}(m+1-i)$$
We have
$$frac{mpi^m}{m+1}=sum_{v=0}^{frac{m}2-1}pi^{m-2-2v}c_v(m)zeta(2v+2)$$
$$frac{mpi^m}{m+1}=c_{m/2-1}(m)zeta(m)+sum_{v=0}^{frac{m}2-2}pi^{m-2-2v}c_v(m)zeta(2v+2)$$
$$c_{m/2-1}(m)zeta(m)=frac{mpi^{m}}{m+1}-sum_{v=0}^{frac{m}2-2}pi^{m-2-2v}c_v(m)zeta(2v+2)$$
I then replace $m$ with $2n$ and $v$ with $k$ (because I like $k$ better):
$$c_{n-1}(2n)zeta(2n)=frac{2npi^{2n}}{2n+1}-sum_{k=0}^{n-2}pi^{2n-2-2k}c_k(2n)zeta(2k+2)$$
$$zeta(2n)=frac{2npi^{2n}}{(2n+1)c_{n-1}(2n)}-sum_{k=0}^{n-2}pi^{2n-2-2k}frac{c_k(2n)}{c_{n-1}(2n)}zeta(2k+2)$$
At this point I plugged some things into Wolfram Alpha and got
$$zeta(2n)=frac{2npi^{2n}}{Gamma(2n+2)}+sum_{k=0}^{n-2}(-1)^{k-n}frac{pi^{2n-2k-2}}{Gamma(2n-2k)}zeta(2k+2)$$
I have not seen this formula anywhere, and I don't have Mathematica or Wolfram Pro, so the only way for me to feel confident in this formula is by having you look at it. I don't think I broke any rules, so is this formula valid? Are there any alternate forms for it? Thanks.
integration sequences-and-series recurrence-relations fourier-series riemann-zeta
$endgroup$
$begingroup$
See math.uwaterloo.ca/~krdavids/M148/Apostol.pdf
$endgroup$
– FDP
Dec 11 '18 at 12:58
add a comment |
$begingroup$
I found this formula. Is it correct?
For $ninBbb N, ngeq2$,
$$zeta(2n)=frac{2npi^{2n}}{Gamma(2n+2)}+sum_{k=0}^{n-2}(-1)^{k-n}frac{pi^{2n-2k-2}}{Gamma(2n-2k)}zeta(2k+2)$$
Here's my proof.
Assume $mgeq2$ is an even number. We start by finding the Fourier series expansion for $x^m$. We define
$$a_k(m)=frac1piint_{-pi}^{pi}x^mcos(kx)mathrm dx$$
$$b_k(m)=frac1piint_{-pi}^{pi}x^msin(kx)mathrm dx$$
Hence we know that
$$x^m=frac{a_0(m)}2+sum_{kgeq1}a_k(m)cos(kx)+b_k(m)sin(kx)$$
And because $m$ is even,
$$x^m=frac{pi^m}{m+1}+sum_{kgeq1}a_k(m)cos(kx)+b_k(m)sin(kx)$$
Next, we start on $b_k(m)$. We make the substitution $x=-t$, and after a little algebra,
$$b_k(m)=0$$
This is because $m$ is even, and thus $(-x)^m=x^m$. Hence we update our series
$$x^m=frac{pi^m}{m+1}+sum_{kgeq1}a_k(m)cos(kx)$$
For $a_k(m)$, I integrated by parts twice to find
$$a_k(m)=(-1)^{k}frac{2mpi^{m-2}}{k^2}-frac{m(m-1)}{k^2}a_k(m-2)$$
Which brought me to the formula
$$a_k(m)=sum_{v=0}^{frac{m}2-1}(-1)^{k+v}frac{2pi^{m-2-2v}}{k^{2+2v}}prod_{i=1}^{2v+1}(m+1-i)$$
Then, plugging $x=pi$ into the Fourier series,
$$pi^m=frac{pi^m}{m+1}+sum_{kgeq1}(-1)^ksum_{v=0}^{frac{m}2-1}(-1)^{k+v}frac{2pi^{m-2-2v}}{k^{2+2v}}prod_{i=1}^{2v+1}(m+1-i)$$
$$frac{mpi^m}{m+1}=sum_{kgeq1}sum_{v=0}^{frac{m}2-1}(-1)^{v}frac{2pi^{m-2-2v}}{k^{2+2v}}prod_{i=1}^{2v+1}(m+1-i)$$
$$frac{mpi^m}{m+1}=sum_{v=0}^{frac{m}2-1}(-1)^{v}2pi^{m-2-2v}prod_{i=1}^{2v+1}(m+1-i)sum_{kgeq1}frac1{k^{2+2v}}$$
$$frac{mpi^m}{m+1}=sum_{v=0}^{frac{m}2-1}(-1)^{v}2pi^{m-2-2v}zeta(2v+2)prod_{i=1}^{2v+1}(m+1-i)$$
Defining
$$c_v(m)=(-1)^v2prod_{i=1}^{2v+1}(m+1-i)$$
We have
$$frac{mpi^m}{m+1}=sum_{v=0}^{frac{m}2-1}pi^{m-2-2v}c_v(m)zeta(2v+2)$$
$$frac{mpi^m}{m+1}=c_{m/2-1}(m)zeta(m)+sum_{v=0}^{frac{m}2-2}pi^{m-2-2v}c_v(m)zeta(2v+2)$$
$$c_{m/2-1}(m)zeta(m)=frac{mpi^{m}}{m+1}-sum_{v=0}^{frac{m}2-2}pi^{m-2-2v}c_v(m)zeta(2v+2)$$
I then replace $m$ with $2n$ and $v$ with $k$ (because I like $k$ better):
$$c_{n-1}(2n)zeta(2n)=frac{2npi^{2n}}{2n+1}-sum_{k=0}^{n-2}pi^{2n-2-2k}c_k(2n)zeta(2k+2)$$
$$zeta(2n)=frac{2npi^{2n}}{(2n+1)c_{n-1}(2n)}-sum_{k=0}^{n-2}pi^{2n-2-2k}frac{c_k(2n)}{c_{n-1}(2n)}zeta(2k+2)$$
At this point I plugged some things into Wolfram Alpha and got
$$zeta(2n)=frac{2npi^{2n}}{Gamma(2n+2)}+sum_{k=0}^{n-2}(-1)^{k-n}frac{pi^{2n-2k-2}}{Gamma(2n-2k)}zeta(2k+2)$$
I have not seen this formula anywhere, and I don't have Mathematica or Wolfram Pro, so the only way for me to feel confident in this formula is by having you look at it. I don't think I broke any rules, so is this formula valid? Are there any alternate forms for it? Thanks.
integration sequences-and-series recurrence-relations fourier-series riemann-zeta
$endgroup$
I found this formula. Is it correct?
For $ninBbb N, ngeq2$,
$$zeta(2n)=frac{2npi^{2n}}{Gamma(2n+2)}+sum_{k=0}^{n-2}(-1)^{k-n}frac{pi^{2n-2k-2}}{Gamma(2n-2k)}zeta(2k+2)$$
Here's my proof.
Assume $mgeq2$ is an even number. We start by finding the Fourier series expansion for $x^m$. We define
$$a_k(m)=frac1piint_{-pi}^{pi}x^mcos(kx)mathrm dx$$
$$b_k(m)=frac1piint_{-pi}^{pi}x^msin(kx)mathrm dx$$
Hence we know that
$$x^m=frac{a_0(m)}2+sum_{kgeq1}a_k(m)cos(kx)+b_k(m)sin(kx)$$
And because $m$ is even,
$$x^m=frac{pi^m}{m+1}+sum_{kgeq1}a_k(m)cos(kx)+b_k(m)sin(kx)$$
Next, we start on $b_k(m)$. We make the substitution $x=-t$, and after a little algebra,
$$b_k(m)=0$$
This is because $m$ is even, and thus $(-x)^m=x^m$. Hence we update our series
$$x^m=frac{pi^m}{m+1}+sum_{kgeq1}a_k(m)cos(kx)$$
For $a_k(m)$, I integrated by parts twice to find
$$a_k(m)=(-1)^{k}frac{2mpi^{m-2}}{k^2}-frac{m(m-1)}{k^2}a_k(m-2)$$
Which brought me to the formula
$$a_k(m)=sum_{v=0}^{frac{m}2-1}(-1)^{k+v}frac{2pi^{m-2-2v}}{k^{2+2v}}prod_{i=1}^{2v+1}(m+1-i)$$
Then, plugging $x=pi$ into the Fourier series,
$$pi^m=frac{pi^m}{m+1}+sum_{kgeq1}(-1)^ksum_{v=0}^{frac{m}2-1}(-1)^{k+v}frac{2pi^{m-2-2v}}{k^{2+2v}}prod_{i=1}^{2v+1}(m+1-i)$$
$$frac{mpi^m}{m+1}=sum_{kgeq1}sum_{v=0}^{frac{m}2-1}(-1)^{v}frac{2pi^{m-2-2v}}{k^{2+2v}}prod_{i=1}^{2v+1}(m+1-i)$$
$$frac{mpi^m}{m+1}=sum_{v=0}^{frac{m}2-1}(-1)^{v}2pi^{m-2-2v}prod_{i=1}^{2v+1}(m+1-i)sum_{kgeq1}frac1{k^{2+2v}}$$
$$frac{mpi^m}{m+1}=sum_{v=0}^{frac{m}2-1}(-1)^{v}2pi^{m-2-2v}zeta(2v+2)prod_{i=1}^{2v+1}(m+1-i)$$
Defining
$$c_v(m)=(-1)^v2prod_{i=1}^{2v+1}(m+1-i)$$
We have
$$frac{mpi^m}{m+1}=sum_{v=0}^{frac{m}2-1}pi^{m-2-2v}c_v(m)zeta(2v+2)$$
$$frac{mpi^m}{m+1}=c_{m/2-1}(m)zeta(m)+sum_{v=0}^{frac{m}2-2}pi^{m-2-2v}c_v(m)zeta(2v+2)$$
$$c_{m/2-1}(m)zeta(m)=frac{mpi^{m}}{m+1}-sum_{v=0}^{frac{m}2-2}pi^{m-2-2v}c_v(m)zeta(2v+2)$$
I then replace $m$ with $2n$ and $v$ with $k$ (because I like $k$ better):
$$c_{n-1}(2n)zeta(2n)=frac{2npi^{2n}}{2n+1}-sum_{k=0}^{n-2}pi^{2n-2-2k}c_k(2n)zeta(2k+2)$$
$$zeta(2n)=frac{2npi^{2n}}{(2n+1)c_{n-1}(2n)}-sum_{k=0}^{n-2}pi^{2n-2-2k}frac{c_k(2n)}{c_{n-1}(2n)}zeta(2k+2)$$
At this point I plugged some things into Wolfram Alpha and got
$$zeta(2n)=frac{2npi^{2n}}{Gamma(2n+2)}+sum_{k=0}^{n-2}(-1)^{k-n}frac{pi^{2n-2k-2}}{Gamma(2n-2k)}zeta(2k+2)$$
I have not seen this formula anywhere, and I don't have Mathematica or Wolfram Pro, so the only way for me to feel confident in this formula is by having you look at it. I don't think I broke any rules, so is this formula valid? Are there any alternate forms for it? Thanks.
integration sequences-and-series recurrence-relations fourier-series riemann-zeta
integration sequences-and-series recurrence-relations fourier-series riemann-zeta
asked Dec 11 '18 at 0:07
clathratusclathratus
4,9711438
4,9711438
$begingroup$
See math.uwaterloo.ca/~krdavids/M148/Apostol.pdf
$endgroup$
– FDP
Dec 11 '18 at 12:58
add a comment |
$begingroup$
See math.uwaterloo.ca/~krdavids/M148/Apostol.pdf
$endgroup$
– FDP
Dec 11 '18 at 12:58
$begingroup$
See math.uwaterloo.ca/~krdavids/M148/Apostol.pdf
$endgroup$
– FDP
Dec 11 '18 at 12:58
$begingroup$
See math.uwaterloo.ca/~krdavids/M148/Apostol.pdf
$endgroup$
– FDP
Dec 11 '18 at 12:58
add a comment |
1 Answer
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$begingroup$
It is correct, but it can be proved with considerably fewer efforts. Since Euler's work it is well-known that
$$ sum_{ngeq 1} zeta(2n) z^{2n} = frac{1-pi z cot(pi z)}{2} $$
hence the values of the $zeta$ function at the positive even integers are related to the coefficients of the Maclaurin series of $pi z cot(pi z)$, or $zcoth z$, or $frac{z}{e^z-1}$. So we have an explicit relation between $zeta(2n)$ and the Bernoulli number $B_{2n}$. Since the reciprocal of the (exponential) generating function of Bernoulli numbers is
$$ frac{e^z-1}{z} = sum_{ngeq 0}frac{z^{n}}{(n+1)!} $$
by considering the Cauchy product between $frac{e^z-1}{z}$ and $frac{z}{e^z-1}$ we may easily derive the recurrence relation for Bernoulli numbers (with even index). This recurrence, translated in terms of $zeta(2n)$, is exactly your identity.
$endgroup$
2
$begingroup$
Or probably, even more directly, I wouldn't be at all surprised if the recurrence turned out to follow from $sin(pi z) sum zeta(2n) z^{2n} = frac{sin(pi z) - pi z cos (pi z)}{2}$, substituting the Taylor series for $sin$ and $cos$.
$endgroup$
– Daniel Schepler
Dec 11 '18 at 0:22
$begingroup$
@DanielSchepler, oh, sure, nice way to put it.
$endgroup$
– Jack D'Aurizio
Dec 11 '18 at 0:35
add a comment |
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$begingroup$
It is correct, but it can be proved with considerably fewer efforts. Since Euler's work it is well-known that
$$ sum_{ngeq 1} zeta(2n) z^{2n} = frac{1-pi z cot(pi z)}{2} $$
hence the values of the $zeta$ function at the positive even integers are related to the coefficients of the Maclaurin series of $pi z cot(pi z)$, or $zcoth z$, or $frac{z}{e^z-1}$. So we have an explicit relation between $zeta(2n)$ and the Bernoulli number $B_{2n}$. Since the reciprocal of the (exponential) generating function of Bernoulli numbers is
$$ frac{e^z-1}{z} = sum_{ngeq 0}frac{z^{n}}{(n+1)!} $$
by considering the Cauchy product between $frac{e^z-1}{z}$ and $frac{z}{e^z-1}$ we may easily derive the recurrence relation for Bernoulli numbers (with even index). This recurrence, translated in terms of $zeta(2n)$, is exactly your identity.
$endgroup$
2
$begingroup$
Or probably, even more directly, I wouldn't be at all surprised if the recurrence turned out to follow from $sin(pi z) sum zeta(2n) z^{2n} = frac{sin(pi z) - pi z cos (pi z)}{2}$, substituting the Taylor series for $sin$ and $cos$.
$endgroup$
– Daniel Schepler
Dec 11 '18 at 0:22
$begingroup$
@DanielSchepler, oh, sure, nice way to put it.
$endgroup$
– Jack D'Aurizio
Dec 11 '18 at 0:35
add a comment |
$begingroup$
It is correct, but it can be proved with considerably fewer efforts. Since Euler's work it is well-known that
$$ sum_{ngeq 1} zeta(2n) z^{2n} = frac{1-pi z cot(pi z)}{2} $$
hence the values of the $zeta$ function at the positive even integers are related to the coefficients of the Maclaurin series of $pi z cot(pi z)$, or $zcoth z$, or $frac{z}{e^z-1}$. So we have an explicit relation between $zeta(2n)$ and the Bernoulli number $B_{2n}$. Since the reciprocal of the (exponential) generating function of Bernoulli numbers is
$$ frac{e^z-1}{z} = sum_{ngeq 0}frac{z^{n}}{(n+1)!} $$
by considering the Cauchy product between $frac{e^z-1}{z}$ and $frac{z}{e^z-1}$ we may easily derive the recurrence relation for Bernoulli numbers (with even index). This recurrence, translated in terms of $zeta(2n)$, is exactly your identity.
$endgroup$
2
$begingroup$
Or probably, even more directly, I wouldn't be at all surprised if the recurrence turned out to follow from $sin(pi z) sum zeta(2n) z^{2n} = frac{sin(pi z) - pi z cos (pi z)}{2}$, substituting the Taylor series for $sin$ and $cos$.
$endgroup$
– Daniel Schepler
Dec 11 '18 at 0:22
$begingroup$
@DanielSchepler, oh, sure, nice way to put it.
$endgroup$
– Jack D'Aurizio
Dec 11 '18 at 0:35
add a comment |
$begingroup$
It is correct, but it can be proved with considerably fewer efforts. Since Euler's work it is well-known that
$$ sum_{ngeq 1} zeta(2n) z^{2n} = frac{1-pi z cot(pi z)}{2} $$
hence the values of the $zeta$ function at the positive even integers are related to the coefficients of the Maclaurin series of $pi z cot(pi z)$, or $zcoth z$, or $frac{z}{e^z-1}$. So we have an explicit relation between $zeta(2n)$ and the Bernoulli number $B_{2n}$. Since the reciprocal of the (exponential) generating function of Bernoulli numbers is
$$ frac{e^z-1}{z} = sum_{ngeq 0}frac{z^{n}}{(n+1)!} $$
by considering the Cauchy product between $frac{e^z-1}{z}$ and $frac{z}{e^z-1}$ we may easily derive the recurrence relation for Bernoulli numbers (with even index). This recurrence, translated in terms of $zeta(2n)$, is exactly your identity.
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It is correct, but it can be proved with considerably fewer efforts. Since Euler's work it is well-known that
$$ sum_{ngeq 1} zeta(2n) z^{2n} = frac{1-pi z cot(pi z)}{2} $$
hence the values of the $zeta$ function at the positive even integers are related to the coefficients of the Maclaurin series of $pi z cot(pi z)$, or $zcoth z$, or $frac{z}{e^z-1}$. So we have an explicit relation between $zeta(2n)$ and the Bernoulli number $B_{2n}$. Since the reciprocal of the (exponential) generating function of Bernoulli numbers is
$$ frac{e^z-1}{z} = sum_{ngeq 0}frac{z^{n}}{(n+1)!} $$
by considering the Cauchy product between $frac{e^z-1}{z}$ and $frac{z}{e^z-1}$ we may easily derive the recurrence relation for Bernoulli numbers (with even index). This recurrence, translated in terms of $zeta(2n)$, is exactly your identity.
answered Dec 11 '18 at 0:16
Jack D'AurizioJack D'Aurizio
292k33284672
292k33284672
2
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Or probably, even more directly, I wouldn't be at all surprised if the recurrence turned out to follow from $sin(pi z) sum zeta(2n) z^{2n} = frac{sin(pi z) - pi z cos (pi z)}{2}$, substituting the Taylor series for $sin$ and $cos$.
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– Daniel Schepler
Dec 11 '18 at 0:22
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@DanielSchepler, oh, sure, nice way to put it.
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– Jack D'Aurizio
Dec 11 '18 at 0:35
add a comment |
2
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Or probably, even more directly, I wouldn't be at all surprised if the recurrence turned out to follow from $sin(pi z) sum zeta(2n) z^{2n} = frac{sin(pi z) - pi z cos (pi z)}{2}$, substituting the Taylor series for $sin$ and $cos$.
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– Daniel Schepler
Dec 11 '18 at 0:22
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@DanielSchepler, oh, sure, nice way to put it.
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– Jack D'Aurizio
Dec 11 '18 at 0:35
2
2
$begingroup$
Or probably, even more directly, I wouldn't be at all surprised if the recurrence turned out to follow from $sin(pi z) sum zeta(2n) z^{2n} = frac{sin(pi z) - pi z cos (pi z)}{2}$, substituting the Taylor series for $sin$ and $cos$.
$endgroup$
– Daniel Schepler
Dec 11 '18 at 0:22
$begingroup$
Or probably, even more directly, I wouldn't be at all surprised if the recurrence turned out to follow from $sin(pi z) sum zeta(2n) z^{2n} = frac{sin(pi z) - pi z cos (pi z)}{2}$, substituting the Taylor series for $sin$ and $cos$.
$endgroup$
– Daniel Schepler
Dec 11 '18 at 0:22
$begingroup$
@DanielSchepler, oh, sure, nice way to put it.
$endgroup$
– Jack D'Aurizio
Dec 11 '18 at 0:35
$begingroup$
@DanielSchepler, oh, sure, nice way to put it.
$endgroup$
– Jack D'Aurizio
Dec 11 '18 at 0:35
add a comment |
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See math.uwaterloo.ca/~krdavids/M148/Apostol.pdf
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– FDP
Dec 11 '18 at 12:58