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The title pretty much explains it, but let's provide more context:

Say we have a rational function $R(x)$ of degree $\le -2$. Then the series $\sum_{n\ge n_0} R(n)$ is convergent. The sum is very easy to evaluate if $R(x)$ happens to be a discrete difference: $$R(x) = S(x)-S(x+1)$$ for another rational fraction $S(x)$ of degree $\le -1$. There are some necessary and sufficient conditions for that, see for instance this question.

Recently there was another question on the site where some answers provided examples of series $\sum_{n\ge 1} R(n)$ with a rational sum, and $R(x)$ a rational fraction in $\mathbb{Q}(x)$. In all of the examples the sum was calculated using the fact that $R(x)$ is a discrete difference. Now the question whether there could not exist an example of a series as above with a rational sum where $R(x)$ is not a discrete difference.

Note that if the denominator of $R(n)$ has all roots integers such an example would (probably) not be possible, as this would imply some rational dependence among values of the zeta function at positive integers. We know that this is not possible for the values at even integers ( equivalent to $\pi$ is transcendental), and I do not expect that the all zeta values and $1$ would be linearly dependent over $\mathbb{Q}$. So an example would involve some other fractions. Would be happy to see an example, maybe a very simple one, that escapes me at the moment. Thank you for your interest!


$\bf{Added:}$ Calvin Lin just provided a very ingenious answer, using zeta sums at odd integers! While the question is thus answered, one could think what else is out there... " can you surprise me with a series $\sum_{n\ge 1} R(n) \in \mathbb{Q}$ in other ways ?"


$\bf{Added:}$ Building on the idea of Calvin Lin:

Say $T(n) = \frac{1}{n^k}$, $k>1$, then for $d\ge 2$ integer we have

$$\frac{1}{d^k} \sum_{n\ge 1} T(n) = \sum_{n\ge 1} \frac{1}{(d n)^k}=\sum_{n\equiv 0 \mod d} T(n)$$

and so $$(1-\frac{1}{d^k}) \sum_{n\ge 1} T(n) = \sum_{n\not \equiv 0 \mod d} T(n)$$

or

$$\sum_{n\ge 1}\left[ (1-\frac{1}{d^k}) T(n) - ( T(d(n-1) + 1) + T(d(n-1) + 2) + \cdot T(d(n-1) +(d-1)) ) \right] = 0$$

We could do other similar things. Let $p_1$, $p_2$, $\ldots$ $p_i$ be the prime factors of some $d\ge 2$ natural. Then we have

$$(1-\frac{1}{p_1^k})(1-\frac{1}{p_2^k}) \cdots (1-\frac{1}{p_i^k}) \sum_{n\ge 1}\frac{1}{n^k} - \sum_{(n,d) = 1} \frac{1}{n^k} = 0$$

and again we get an example. Note that we do get a series that is not a difference.

orangeskid
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    Given that $\sum 1/k^3 - \sum 8/[7(1+2k)^3] = 8/7$, would you accept $R(x) = \frac{1}{k^3} - \frac{ 8}{7 (1+2k)^3 } = \frac{ 48x^3 + 84 x^2 + 42x + 7 } { 7x^3 (2x+1)^3}$? (I believe that) It can't be partial fractioned into a telescoping series with a finite difference, though we're cancelling out $k$ with $2k, 2k+1$. – Calvin Lin Jan 10 '25 at 07:23
  • @Calvin Lin : Yes, that is a Good example... now I see... thank you!. – orangeskid Jan 10 '25 at 07:29
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    Besides CalvinLin's counter-example, I want to mention that all hyper-telelescoping patterns must be avoided altogether to avoid "trivial sums". For example: $$R(x)=S(x)-\frac{1}{3}S(x+1)-\frac{2}{3}S(x+2)$$ – Quý Nhân Jan 10 '25 at 07:35
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    @QuýNhân In your case, we could define $T(x) = S(x) + \frac{2}{3} S(x+1)$, then $T(x) - T(x-1) = S(x) - \frac{1}{3} S(x+1) - \frac{2}{3} S(x+2) = R(x)$ fulfills OP's condition. Hence my referencing "telescoping series with a finite difference", and why I created my example as such. (I used cubic just in case there were concerns, and could make quadratic work. Unfortunately the linear case doesn't.) – Calvin Lin Jan 10 '25 at 07:39
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    @CalvinLin Oh, how right you are. – Quý Nhân Jan 10 '25 at 07:41
  • In this case I suppose the degree of $P=f/g$ is defined as $\deg f - \deg g$? – Milten Jan 10 '25 at 08:41
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    The more common definition of the degree of a rational function is the maximum of the degrees of numerator and denominator. – Martin R Jan 10 '25 at 10:06
  • @Martin R: indeed, that would be the correct definition in some contexts, especially for complex analysis. The one specified by Milten 6 works well since it is invariant under the many writings of $R$ as a fraction, and also for calculus. – orangeskid Jan 10 '25 at 14:46

2 Answers2

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Verify that $$ \sum_{k=1}^\infty \frac{1}{k^2} = \frac{4}{3} + \frac{4}{3} \sum_{k=1}^\infty \frac{1}{(1+2k)^2}.$$
(Split the LHS into odd and even $k$. We can rearrange terms as the sum is finite).

Hence we have

$$ \sum_{k=1}^\infty \frac{ 1}{k^2} - \frac{ 4}{3(1+2k)^2 } = \sum_{k=1}^\infty \frac { 8k^2 + 12k + 3 } { 3k^2 ( 2k+1) ^2 } = \frac{4}{3}.$$

Then this cannot be partial fractioned into a telescoping series using terms that are a finite distance away.


Note: Technically, I haven't definitively proved that there isn't a simple $S(x)$ of finite degree such that $\frac { 8k^2 + 12k + 3 } { 3k^2 ( 2k+1) ^2 } = S(k) - S(k+1). $
We could of course have $S(k) = \sum_{j=k}^\infty \frac { 8j^2 + 12j + 3 } { 3j^2 ( 2j+1) ^2 } $, which doesn't evaluate to a "nice form" per Eric's comment.

Calvin Lin
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    What a beautiful idea! – orangeskid Jan 10 '25 at 07:38
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    I believe the fact that this series does not telescope follows from the answer of orangeskid linked in the question, since the partial fraction expansion $$\frac{8k^2+12k+3}{3k^2(2k+1)^2}=\frac1{k^2}-\frac1{3(k+\frac12)^2}$$ has coefficients which don't sum to zero. – Carl Schildkraut Jan 10 '25 at 08:14
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    Mathematica tells me $S(k) = C + \frac{1}{3}\left( 3 \psi^{(1)}(k) - \psi^{(1)}(k+1/2) - 4 \right)$, where $\psi^{(1)}$ is a polygamma function, $\psi^{(1)}(x) = \psi'(x) = (\Gamma'(x)/\Gamma(x))'$. It's fairly easy to see the $4/3$ in this solution and I suspect the offset $\psi$s are implementing the even-odd split you intended. I haven't read enough about the Galois theory of difference equations to know how contorted the inhomogeneous term has to be to obstruct solvability (or even if that's possible). – Eric Towers Jan 10 '25 at 08:16
  • Carl is right, yes indeed, more precisely, in every fixed degree and $\mathbb{Z}$ orbit ( under translation) for the roots at the denom, the sums are $0$. When the roots are all integers that is equivalent to $0$ sums. Note that in degree $-1$ the sums over all roots are $0$ ( some residue theorem, if $\deg R \le -2$). So here you got roots $0$ and $-1/2$ so they are in different orbits. Moreover, $1$ and $-1/3$ are $\ne 0$ so not a difference. It works for all combinations like this from zetas. – orangeskid Jan 10 '25 at 14:41
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I will prove CalvinLin's sum can't be turned (directly) into a telelescoping sum. $$\frac{4}{3}=\sum_{k=1}^{\infty}\left(\frac{ 1}{k^2} - \frac{ 4}{3(2k+1)^2 }\right)=\sum_{k=1}^{\infty}R(k)$$ Where $R(k)=\frac{8k^2+12k+3}{3k^2(2k+1)^2}$. We will prove by contradiction. First, let's assume: $\ \exists S(x)\in \mathbb{Q}(x):S(x)-S(x+1)=R(x)$ (*)

Lemma 1: $\exists c\in\mathbb{R}:\lim_{x\to\infty}S(x)=c$
Proof: Since $S(x)$ is rational function, the limit is either finite or infinte (exists) and If $\lim_{x\to\infty}S(x)=\infty\implies S(x)\sim P(x)$ for some non-constant polynomial $P(x)$, hence $R(x)=S(x)-S(x+1)\sim P(x)-P(x+1)\not\to 0$, contradicts convergence of $\sum_{k=1}^{\infty}R(k)$.
The case $\lim_{x\to\infty}S(x)=-\infty$ is dealt simililarly.

Fact 2: $\forall S(x)$ (satisfies lemma 1), we can rechoose $S_1(x)=S(x)-c-4/3$ so that $\lim_{x\to\infty}S_1(x)=-4/3$

By Fact 2, we are supposed to find $S(x)$ satisfying $S(x)-S(x+1)=R(x)$ and $\lim_{x\to\infty}S(x)=S(\infty)=-4/3$, so that: $$\frac{4}{3}=\sum_{k=1}^{\infty}R(k)=\sum_{k=1}^{\infty}\left(S(k)-S(k+1)\right)=S(1)-S(\infty)=S(1)+\frac{4}{3}$$ $$\implies S(1)=0 $$ We rewrite $S(x)$ as: $S(x)=(x-1)^m G(x)$ for some positive integer $m$, and rational $G(x)$ where $G(1)$ is a finite constant.
We have $R(x)=(x-1)^m G(x)-x^m G(x+1)\ \ (2)$. From here, consider limit: $$\lim_{x\to 0}\left(R(x)-(x-1)^m G(x)\right)=\lim_{x\to 0}-x^m G(x+1)=0$$ But $R(x)\sim \frac{1}{x^2}$ as $x\to 0$, we deduce $G(x)= H_0(x)/x^2$ for some rational $H_0(x)$ defined at $0$ and $1$. Substitute back to $(2)$: $$R(x)=\frac{(x-1)^m H_0(x)}{x^2}-\frac{x^m H_0(x+1)}{(x+1)^2}$$ Now consider limit: $$\lim_{x\to -1}\left(R(x)+\frac{x^m H_0(x+1)}{(x+1)^2}\right)=\lim_{x\to -1}\frac{(x-1)^m H_0(x)}{x^2}$$ The function of limit on LHS $\sim \frac{1}{(x+1)^2}$ as $x\to -1$ hence $H_0(x)\sim \frac{1}{(x+1)^2}\implies H_{0}(x)=H_{1}(x)/(x+1)^2$ for some rational $H_{1}(x)$ defined at $1,0,-1$. We continue this argument inductively by consider limit $x\to -N$, we eventually find out that $G(x)=\frac{H_{N}(x)}{x^2(x+1)^2...(x+N)^2}$ for some rational $H_{N}(x)$ defined at $1,0,-1,...,-N$. Since $N$ is unbounded, this means $G(x)$ will have unbounded number of poles at negative integers, contradicts $G(x)\in \mathbb{Q}(x)$.

So $\not\exists S(x)$ and our initial assumption (*) is false.

Quý Nhân
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    The $S$ you chose is $S(x) = \frac{1}{3}\left( 3 \psi^{(1)}(x) - \psi^{(1)}(x+1/2) - 4 \right)$ which indeed has infinitely many poles. – Gary Jan 10 '25 at 11:03
  • What you wrote is very interesting! Btw, have you checked the first link in the question, there are given conditions for the existence of such an $S(x)$, that can be read from the decomposition in partial fractions. – orangeskid Jan 10 '25 at 14:36
  • @orangeskid I'm aware of it, very nice result indeed. Thanks for mentioning. – Quý Nhân Jan 10 '25 at 20:03