EDITs
- extension to alternating sums (6)
- extension to general sums with parameter $x$ (8)
- extension to general sums with two parameters (11)
Extended post
The relation
$$\sum _{k=1}^{n } \left(\frac{H_k^{(p)}}{k^q}+\frac{H_k^{(q)}}{k^p}\right)=H_n^{(p)} H_n^{(q)}+H_n^{(p+q)}\tag{1}$$
where $H_k^{(p)} = \sum_{j=1}^k j^{-p}$, is a nice and important symmetry relation with various applications. Notice the finite upper index $n$. The proof is not hard.
Corollary 1
If $q = p$ the relation simplifies to
$$\sum _{k=1}^n \frac{H_k^{(p)}}{k^p}= \frac{1}{2}\left( (H_n^{(p)})^2+H_n^{(2p)} \right)\tag{2}$$
Corollary 2
In the limit $n \to \infty$ (1) turns into
$$\sum _{k=1}^{\infty } \left( \frac{H_k^{(p)}}{k^q}+\frac{H_k^{(q)}}{k^p}\right)=\zeta(p)\zeta(q)+ \zeta(p+q)\tag{3}$$
where
$$\zeta(s) = \lim_{n\to \infty } \, H_n^{(s)}=\sum_{k=1}^\infty k^{-s}\tag{3a}$$
is the Riemann zeta function.
For $q=p$ formula (3) gives the analogue to (2)
$$\sum _{k=1}^{\infty } \frac{H_k^{(p)}}{k^p}=\frac{1}{2}\left(\zeta(p)^2+ \zeta(2p)\right)\tag{4}$$
This formula was also given in [1], and there it was claimed that it is valid for real $p$.
Alternating sums
A similar relation can be derived for alternating sums.
Define
$$A_n^{(p)}= \sum_{k=1}^n (-1)^k \frac{1}{k^p}\tag{5}$$
then the basic relation is
$$\sum _{k=1}^{n} (-1)^k \frac{H_k^{(p)}}{k^q} +\sum _{k=1}^{n} \frac{A_k^{(q)}}{k^p} = H_n^{(p)} A_n^{(q)}+A_n^{(p+q)}\tag{6}$$
From (6) other corollaries and formulas can be derived in a manner similar to the one for the non-alternating sums described above.
Generalized relation with parameter $x$
It can be shown with similar methods as before that a more general relation holds from which the two formulas discussed before are special cases.
Let
$$H_n^{(p)}(x) = \sum_{k=1}^n \frac{x^k}{k^p}\tag{7}$$
$H_n^{(p)}$ is understood as $H_n^{(p)}(+1)$ and we have $H_n^{(p)}(-1)=A_n^{(p)}$ (c.f. (5)).
Then the relation is
$$\sum_{k=1}^n \left(x^k \frac{H_k^ {(p)}(1)}{k^q} + \frac{H_k^{(q)}(x)}{k^p}\right)=H_n^{(p)}(1)H_n^{(q)}(x)+ H_n^{(p+q)}(x)\tag{8}$$
Notice that this relation has lost the symmetry.
For $x=1$ and $x=-1$ we recover the relations (1) and (6), respectively.
In the limit $n\to\infty$ we encounter on the right hand side the polylog function
$$\lim_{n\to\infty}\, H_n^{(p)}(x)=\sum_{k=1}^\infty \frac{x^k}{k^p} = Li_p(x)\tag{9}$$
so that we have
$$\sum_{k=1}^{\infty} \left(x^k \frac{H_k^ {(p)}(1)}{k^q} + \frac{H_k^{(q)}(x)}{k^p}\right)=Li_p(1)Li_q(x)+ Li_{p+q}(x)\tag{10}$$
Note "added in proof"
The special case $x=-1$ of relation (10) can be uncovered (it is there more or less conceiled) from [2], page 33, where it is called "shuffle relation". We now have here an elementary proof of a generalization it.
Generalized relation with two parameters $x$ and $y$
We can even go one final step further and write down this two-parametric symmetry relation
$$\sum_{k=1}^n \frac{x^k}{k^q}\sum_{m=1}^k \frac{y^m}{m^p} + \sum_{k=1}^n \frac{y^k}{k^p}\sum_{m=1}^k \frac{x^m}{m^q}=\left( \sum_{k=1}^n \frac{x^k}{k^q}\right)\left( \sum_{k=1}^n \frac{y^k}{k^p}\right)+ \sum_{k=1}^n \frac{(x y)^k}{k^{p+q}}\tag{11}$$
This relation includes the various cases of alternating and non-alternating sums for apropriate choices of $x$ and $y$.
In the limit $n\to\infty$ we obtain
$$\sum_{k=1}^\infty \frac{x^k}{k^q}\sum_{m=1}^k \frac{y^m}{m^p} + \sum_{k=1}^\infty \frac{y^k}{k^p}\sum_{m=1}^k \frac{x^m}{m^q}=\text{Li}_q(x) \text{Li}_p(y)+ \text{Li}_{p+q}(x y)\tag{12}$$
The zeta functions of (3) have been generalized to polylog functions.
Question
Prove (1), (6), (8), (11) and (12)
References
