recurrence relation for $zeta(2n)$












3












$begingroup$


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.










share|cite|improve this question









$endgroup$












  • $begingroup$
    See math.uwaterloo.ca/~krdavids/M148/Apostol.pdf
    $endgroup$
    – FDP
    Dec 11 '18 at 12:58
















3












$begingroup$


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.










share|cite|improve this question









$endgroup$












  • $begingroup$
    See math.uwaterloo.ca/~krdavids/M148/Apostol.pdf
    $endgroup$
    – FDP
    Dec 11 '18 at 12:58














3












3








3





$begingroup$


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.










share|cite|improve this question









$endgroup$




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






share|cite|improve this question













share|cite|improve this question











share|cite|improve this question




share|cite|improve this question










asked Dec 11 '18 at 0:07









clathratusclathratus

4,084335




4,084335












  • $begingroup$
    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




$begingroup$
See math.uwaterloo.ca/~krdavids/M148/Apostol.pdf
$endgroup$
– FDP
Dec 11 '18 at 12:58










1 Answer
1






active

oldest

votes


















2












$begingroup$

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.






share|cite|improve this answer









$endgroup$









  • 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











Your Answer





StackExchange.ifUsing("editor", function () {
return StackExchange.using("mathjaxEditing", function () {
StackExchange.MarkdownEditor.creationCallbacks.add(function (editor, postfix) {
StackExchange.mathjaxEditing.prepareWmdForMathJax(editor, postfix, [["$", "$"], ["\\(","\\)"]]);
});
});
}, "mathjax-editing");

StackExchange.ready(function() {
var channelOptions = {
tags: "".split(" "),
id: "69"
};
initTagRenderer("".split(" "), "".split(" "), channelOptions);

StackExchange.using("externalEditor", function() {
// Have to fire editor after snippets, if snippets enabled
if (StackExchange.settings.snippets.snippetsEnabled) {
StackExchange.using("snippets", function() {
createEditor();
});
}
else {
createEditor();
}
});

function createEditor() {
StackExchange.prepareEditor({
heartbeatType: 'answer',
autoActivateHeartbeat: false,
convertImagesToLinks: true,
noModals: true,
showLowRepImageUploadWarning: true,
reputationToPostImages: 10,
bindNavPrevention: true,
postfix: "",
imageUploader: {
brandingHtml: "Powered by u003ca class="icon-imgur-white" href="https://imgur.com/"u003eu003c/au003e",
contentPolicyHtml: "User contributions licensed under u003ca href="https://creativecommons.org/licenses/by-sa/3.0/"u003ecc by-sa 3.0 with attribution requiredu003c/au003e u003ca href="https://stackoverflow.com/legal/content-policy"u003e(content policy)u003c/au003e",
allowUrls: true
},
noCode: true, onDemand: true,
discardSelector: ".discard-answer"
,immediatelyShowMarkdownHelp:true
});


}
});














draft saved

draft discarded


















StackExchange.ready(
function () {
StackExchange.openid.initPostLogin('.new-post-login', 'https%3a%2f%2fmath.stackexchange.com%2fquestions%2f3034679%2frecurrence-relation-for-zeta2n%23new-answer', 'question_page');
}
);

Post as a guest















Required, but never shown

























1 Answer
1






active

oldest

votes








1 Answer
1






active

oldest

votes









active

oldest

votes






active

oldest

votes









2












$begingroup$

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.






share|cite|improve this answer









$endgroup$









  • 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
















2












$begingroup$

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.






share|cite|improve this answer









$endgroup$









  • 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














2












2








2





$begingroup$

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.






share|cite|improve this answer









$endgroup$



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.







share|cite|improve this answer












share|cite|improve this answer



share|cite|improve this answer










answered Dec 11 '18 at 0:16









Jack D'AurizioJack D'Aurizio

1




1








  • 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














  • 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








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


















draft saved

draft discarded




















































Thanks for contributing an answer to Mathematics Stack Exchange!


  • Please be sure to answer the question. Provide details and share your research!

But avoid



  • Asking for help, clarification, or responding to other answers.

  • Making statements based on opinion; back them up with references or personal experience.


Use MathJax to format equations. MathJax reference.


To learn more, see our tips on writing great answers.




draft saved


draft discarded














StackExchange.ready(
function () {
StackExchange.openid.initPostLogin('.new-post-login', 'https%3a%2f%2fmath.stackexchange.com%2fquestions%2f3034679%2frecurrence-relation-for-zeta2n%23new-answer', 'question_page');
}
);

Post as a guest















Required, but never shown





















































Required, but never shown














Required, but never shown












Required, but never shown







Required, but never shown

































Required, but never shown














Required, but never shown












Required, but never shown







Required, but never shown







Popular posts from this blog

Wiesbaden

Marschland

Dieringhausen