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Starting with the famous Basel problem, Euler evaluated the Riemann zeta function for all even positive integers and the result is a compact expression involving Bernoulli numbers. However, the evaluation of the zeta function at odd positive integers (in terms of getting a closed form sum) is still open. There has been some progress in the form of Apery's theorem and other results such as "infinitely many of $\zeta(2n+1)$ are irrational" or "at least one of $\zeta(5),\zeta(7),\zeta(9)$ or $\zeta(11)$ is irrational".

Question(s): Is there a high level understanding for this disparity between even and odd integers? Is it a case of there being a simple expression for $\zeta(3)$ that is out there waiting for an ingenious attack like Euler did with $\zeta(2)$? Or is the belief that such a closed form summation is unlikely? Where do the many many proofs powerful enough to evaluate $\zeta(2n)$ stumble when it comes to evaluating $\zeta(2n+1)$?

Motivation: The Basel problem and Euler's solution are my all-time favorites for the sheer surprise factor and ingenuity of proof (what do $\pi$ and $\frac{sin(x)}{x}$ have to do with $\zeta(2)$??). However, I currently lack the more advanced analytical tools to appreciate the deeper results of this area. I have wondered for a while about the questions above and Internet search hasn't helped much. I would greatly appreciate any answers/references. Thanks.

Dinesh
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    If you don't know yet this list compiled by Wadim Zudilin, one of the researchers in this field, colects all the relevant papers concerning the subject http://wain.mi.ras.ru/zw/ "Several references and links devoted to the arithmetic study of values of the Riemann zeta function at positive integers and related constants are put on this page." – Américo Tavares Dec 03 '10 at 00:51
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    You can also look the 3Blue1Brown's Youtube explanation why $\pi$ appears in $\zeta(2)$. Here is the link: https://www.youtube.com/watch?v=d-o3eB9sfls – Stefan Gruenwald Apr 30 '20 at 02:44

8 Answers8

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The zeta function is defined as a sum over the positive integers, but as far as actually evaluating it, it turns out to be more natural to think of it as a sum over all nonzero integers; thus we should really be thinking about $\sum_{n \neq 0} \frac{1}{n^k}$. For $k$ even this is just $2 \zeta(k)$ and there are various ways to evaluate this more symmetric sum, e.g. by writing down a meromorphic function with the right poles, or a Fourier series with the right coefficients, etc. But for $k$ odd this is equal to zero, since terms cancel with their negatives! Written in this way, the zeta function at even integers reveals its alter ego as an Eisenstein series in one dimension.

This cancellation phenomenon occurs in Euler's classic "proof," since the infinite product for $\sin z$ that he uses has zeroes at all integer multiples of $\pi$, not just the positive ones. It also occurs in the general proof that proceeds by considering the generating function $\frac{z}{e^z - 1}$ for the Bernoulli numbers. As you might know, the closed form of $\zeta(2k)$ involves Bernoulli numbers, and again $\frac{z}{e^z - 1}$ has poles at $2 \pi i n$ for all nonzero integers $n$, not just the positive ones. I describe how this works in slightly more detail here.

Another way to think about the difference between the even and odd cases is that one can think of the even cases as $L^2$ norms of appropriate Fourier series; this is precisely how a standard proof of the evaluation of $\zeta(2)$ works. But for the odd cases we don't get an $L^2$ norm; instead we get a mysterious inner product.

Qiaochu Yuan
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    Thanks for the wonderful explanation. Do you have any thoughts on how likely a closed form summation is for $\zeta(2n+1)$? – Dinesh Dec 03 '10 at 00:22
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    @Dinesh: nope. The values of the zeta function at odd integers are related to some deep mathematics and I'm totally unqualified to comment on whether any of these deep approaches do or do not support the idea that there is a nice closed form. – Qiaochu Yuan Dec 03 '10 at 00:28
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    Can you expand on the mysterious inner product? – zerosofthezeta Dec 03 '13 at 21:09
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One expects that the numbers $\zeta(2n+1)$ are algebraically independent of one another, and of $\pi$, and so one should think of them as ``new'' numbers; you can't expect any closed form expression in terms of powers of $\pi$, say. Unfortunately, this conjecture seems very much out of reach at the moment.

For an explanation of why people believe this conjecture, one can see for example this answer to a related mathoverflow question.

Matt E
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    @ Matt E: Thanks for the explanation. Its fascinating that each of $\zeta(3),\zeta(5),\dots$ is likely to be a "new" irrational number. – Dinesh Dec 04 '10 at 00:14
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    Why do you expect them to be algebraically independent of pi, when the even ones aren't? – Peter Webb Sep 12 '15 at 12:31
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    Your question: " Is there a high level understanding for this disparity between even and odd integers?" is much deeper that you could think. It is at the heart of current advanced research on the "special values of L-functions of motives". I recommend the recent book of Proceedings of the Pune conference , "The Bloch-Kato conjecture for the Riemann Zeta function", ed. Coates & al., London Math. Soc. LNS 418 (2015). – nguyen quang do May 20 '16 at 06:24
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    From the preface :"The values of Zeta(s) at even positive integers and odd negative integers have been known since the time of Euler. However, its values at odd positive integers remains mysterious to this day. The Bloch-Kato conjectures provide a conjectural framework to understand the special values of all motivic L-functions. The principal aim of this workshopwas to prove the B-K conjecture in the simplest "non critical" example, i.e. the values of Riemann Zeta(s) at odd positive integers." – nguyen quang do May 20 '16 at 06:27
  • To make things short : 1) The "critical values" of Zeta(s) are its values at all even positive and (via the functional equation) odd negative integers are classically known (Euler, etc.) to be given by precise formulae involving Bernouilli numbers 2) The "non critical values" are the values at all odd positive and (again via the functional eq.) all even negative integers. However, the latter are null (the so called simple "trivial zeroes"), and the mystery actually lies in the first terms of the Taylor expansions . – nguyen quang do May 20 '16 at 06:39
  • @Dinesh What is proved now : these special values are rational numbers; up to sign and a power of 2, the numerators (denominators) are resp. the orders of the K-groups of Z of even (odd) index in Quillen's K-theory. Of course there are conjectures extending this to number fields, which in some way generalize the class number formula ) with Riemann replaced by Dedekind. Again, this has been proved for abelian fields. – nguyen quang do May 20 '16 at 06:45
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Have you looked at this ICM paper before. Ramanujan has found out some wierd formula. The paper is not viable to read. But I guess, this will give some idea about the progress made regarding this problem.

Added: Try emailing Prof. Bruce Berndt. Since this is related to Ramanujan, I am sure he might be knowing something along these lines. Another good source of information which I am sure you would like to read are: -

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Where do the many many proofs powerful enough to evaluate ζ(2n) stumble when it comes to evaluating ζ(2n+1)?

Another method of evaluating $ \zeta(2n) \ $ not mentioned yet is by applying Parseval's Theorem to the Fourier series of the Bernoulli Polynomials. The Fourier coefficients of $ B_n\ $ have the form $ c_k = (constants)\cdot \frac{1}{k} $. By Parseval's Theorem, $$ \int_0^1 |B_n(t)|^2 dt = \sum_{k\neq0} |c_k|^2 $$ $$ (constant) = (more\ constants) \sum_{k\neq0} \frac{1}{k^{2n}} $$ (Note that the constants depend upon n)
The reason this method falls apart for odd integers is that, since Parseval's Theorem involves squaring the coefficients, so there is no way to get odd powers into the sum.

Riley E
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  • This is equivalent to the proof using the generating function for the Bernoulli numbers, and I mentioned that one could use Parseval's theorem in my answer; the Fourier series you mention comes from the poles of that function. – Qiaochu Yuan Jan 04 '11 at 13:56
  • Sorry about that. I only noticed the reference to the generating function and not the reference to the Fourier series. – Riley E Jan 04 '11 at 17:39
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Riemann Zeta at Even Integers

One reason why $\zeta(2k)$ has a nice closed form is because $$ \require{enclose} \newcommand{\Res}{\operatorname*{Res}} \lim_{R\to\infty}\int_{|z|=R}\frac{\pi\cot(\pi z)}{z^{2k}}\,\mathrm{d}z=0\tag1 $$ and the residue of $\pi\cot(\pi z)$ is $1$ at each integer. Since the integral in $(1)$ is $2\pi i$ times the sum of the residues inside $|z|=R$, we get $$ \zeta(2k)=-\tfrac12\Res_{z=0}\frac{\pi\cot(\pi z)}{z^{2k}}\tag2 $$ As shown in this answer, we can find a recurrence for the coefficients of $z\cot(z)$ which leads to a recurrence for $\zeta(2k)$.

This approach fails if we use $2k+1$ in place of $2k$. Summing over the reciprocals of all non-zero integers with odd exponent yields a sum of $0$. This agrees with the fact that the residue of an even function at $z=0$ is $0$.


An Alternating Approach

The function $\pi\sec(\pi z)$ has a residue $(-1)^n$ at $z=n-\frac12$ for $n\in\mathbb{Z}$. This gives opposite residues at $z=n-\frac12$ and $z=-n+\frac12$. This is good for summing odd functions. $$ \begin{align} 0 &=\frac1{2\pi i}\lim_{R\to\infty}\int_{|z|=R}\frac{\pi\sec(\pi z)}{z^{2k+1}}\,\mathrm{d}z\\ &=\Res_{z=0}\frac{\pi\sec(\pi z)}{z^{2k+1}}+2\sum_{n=1}^\infty\frac{(-1)^n}{\left(\small{n-\frac12}\right)^{2k+1}}\\ &=\Res_{z=0}\frac{\pi\sec(\pi z)}{z^{2k+1}}+4^{k+1}\sum_{n=1}^\infty\frac{(-1)^n}{(2n-1)^{2k+1}}\\ &=\Res_{z=0}\frac{\pi\sec(\pi z)}{z^{2k+1}}-4^{k+1}\beta(2k+1) \end{align} $$ where $\beta(s)$ is the Dirichlet beta Function. Some values and a recursion for all even arguments can be found in this answer.


A Unilateral Attack on Zeta

The function $\pi\tan(\pi z)$ has a residue $-1$ at $z=n-\frac12$ for $n\in\mathbb{Z}$. This gives identical residues at $z=n-\frac12$ and $z=-n+\frac12$. This is good for summing even functions. $$ \begin{align} 0 &=\frac1{2\pi i}\lim_{R\to\infty}\int_{|z|=R}\frac{\pi\tan(\pi z)}{z^{2k}}\,\mathrm{d}z\\ &=\Res_{z=0}\frac{\pi\tan(\pi z)}{z^{2k}}+2\sum_{n=1}^\infty\frac{-1}{\left(\small{n-\frac12}\right)^{2k}}\\ &=\Res_{z=0}\frac{\pi\tan(\pi z)}{z^{2k}}-2^{2k+1}\sum_{n=1}^\infty\frac1{(2n-1)^{2k}}\\ &=\Res_{z=0}\frac{\pi\tan(\pi z)}{z^{2k}}-\left(2^{2k+1}-2\right)\zeta(2k) \end{align} $$ where $\zeta(s)$ is the Riemann zeta Function.


A Unified Result

The following is a rational multiple of $\pi^k$ $$ \sum_{n=0}^\infty\frac{(-1)^{nk}}{(2n+1)^k} $$ This evaluates to $\beta(k)$ for odd $k$ and $\left(1-2^{-k}\right)\zeta(k)$ for even $k$.

robjohn
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$$\DeclareMathOperator{sinc}{sinc}$$ To piggy-back off of the discussion from @Matt E above, I would like to add that there is probably good reason to believe that all odd integer values for $\zeta(s)$ are algebraically independent of each other, but not necessarily of $\pi$. Euler evaluated the $\sinc(x)$ function to obtain a closed form value for $\zeta(2)$. You can also see this function in the product formula:

$$f(x) = \prod_{k=1}^\infty 1 -\frac{x^2}{k^2 \pi^2} = \frac{\sin(x)}{x}$$

If we look at a similar function for $\zeta(4)$, we obtain:

$$f(x) = \prod_{k=1}^\infty 1 -\frac{x^4}{k^4 \pi^4} = \frac{\sin(x) \sinh(x)}{x^2}$$

There are other transcendental functions associated with the higher, even integer values for $\zeta(s)$. Given these transcendental functions, i.e. the $\sinc(x)$ function and the function involving the hyperbolic $\sin$ associated with $\zeta(4)$, you can simply take the absolute value of the second term in each of their Taylor series expansions and set $x = \pi$. You then obtain the closed form values for $\zeta(2)$ and $\zeta(4)$. You can similarly perform this for the higher, even values for $\zeta(s)$.

The question: Is there a transcendental function that we can similarly use to obtain the value for $\zeta(3)$? We do know this, using the gamma function:

$$f(x) = \prod_{k=1}^\infty 1 -\frac{x^3}{k^3 \pi^3} = \frac{1}{\Gamma(1 - \frac{x}{\pi}) \Gamma(1 + \frac{(-1)^{(1/3)} x}{\pi}) \Gamma(1 - \frac{(-1)^{(2/3)} x}{\pi})}$$

If you look at the second term of the series expansion for this inverted "multi-gamma" function above, we obtain:

$$\frac{x^3 ψ^2(1)}{2 \pi^3}$$ where $ψ^n(x)$ is $n^{\text{th}}$ derivative of the digamma function.

When you set $x = \pi$, you can see that it cancels out with the $\pi^3$ in the denominator and you're left with the digamma function value divided by 2, which is $\zeta(3)$. So it seems that $\pi^3$ is kind of related to $\zeta(3)$, but not in a way that's tangible. My opinion is that there is most likely another transcendental quantity involved along with $\pi$, one that may need to be discovered, or one that is in lieu of $\pi$. That is, $\pi$ might be a stepping stone, so to speak, to reach another transcendental which is then involved with a closed form value for $\zeta(3)$.

D S
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Relation of the Eisenstein series, zeta functions at even and odd numbers can see from 11.17 page 117 of "Automorphic forms on $Sl_2(R)$" of Borel gives a formula: $$c(s) = {\pi ^{1/2}}\frac{{\zeta (s)}}{{\zeta (s + 1)}}\frac{{\Gamma (s/2)}}{{\Gamma ((1 + s)/2)}}$$ where $c(s)$ comes from constant term of Eisenstein series $E(s,z)_P$: $$E{(s,z)_P} = {y^{(1 + s)/2}} + c(s){y^{(1 - s)/2}}$$ with $z=x+iy$.

Nguyen Dang Son
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For where $m∈ℤ^+$,

$$ζ(2m+1)=(-1)^{m}2^{2m+1}π^{2m}\left(∫_1^{∞}\frac{z^{-2m-1}}{e^{z}-1}dz+∑_{k=0}^{∞}\frac{B_{k}}{k!}\frac{1}{k-2m-1}\right)$$

where $B_{k}$ is the $k$-th Bernoulli number.
It is not "closed form" but I found this and I wonder what I found. I hope someone tell me if it has a meaning instead of saying rubbish.

Bob Dobbs
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