Can the Intriguing Harmonic Sum be Solved with Elementary Methods?

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The forum discussion centers on proving the harmonic sum identity $$\sum_{k\geq 1} \frac{H^2_k}{k^2}=\frac{17}{4}\zeta(4)=\frac{17\pi^4}{360}$$ using elementary methods, as opposed to complex techniques such as contour integration and Fourier series. Participants explore various approaches, including the use of generating functions and integration techniques. The discussion highlights the potential for an induction proof and the simplification of the integral $$\int^1_0 \frac{1-x^n}{1-x}\, dx$$ as a pathway to the solution.

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  • Understanding of harmonic numbers, specifically $$H_k = 1 + \frac{1}{2} + \frac{1}{3} + \cdots + \frac{1}{k}$$
  • Familiarity with the Riemann zeta function, particularly $$\zeta(4)$$
  • Knowledge of generating functions and their applications in series
  • Basic integration techniques, including integration by parts
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  • Research the properties and applications of harmonic numbers in number theory
  • Study the Riemann zeta function and its significance in mathematical analysis
  • Explore generating functions in combinatorial mathematics
  • Learn advanced integration techniques, including contour integration and Fourier analysis
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Mathematicians, students of advanced calculus, and anyone interested in number theory or series convergence will benefit from this discussion.

alyafey22
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This thread will be dedicated for a trial to prove the following

$$\sum_{k\geq 1} \frac{H^2_k}{k^2}=\frac{17}{4}\zeta(4)=\frac{17\pi^4}{360}$$

$$\mbox{where }\,\,H^2_k =\left( 1+\frac{1}{2}+\frac{1}{3}+\cdots \frac{1}{k}\right)^2$$​

In this paper the authors give solutions to the sum and others , but the process is quite complicated and uses contour integration , Fourier series and Parseal's thoerem , ... .

I believe we can solve it using elementary methods .
 
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ZaidAlyafey said:
This method will be dedicated for a trial to prove the following

$$\sum_{k\geq 1} \frac{H^2_k}{k^2}=\frac{17}{4}\zeta(4)=\frac{17\pi^4}{360}$$

$$\mbox{where }\,\,H^2_k =\left( 1+\frac{1}{2}+\frac{1}{3}+\cdots \frac{1}{k}\right)^2$$​

In this paper the authors give solutions to the sum and others , but the process is quite complicated and uses contour integration , Fourier series and Parseal's thoerem , ... .

I believe we can solve it using elementary methods .
The harmonic series has no explicit formula for its partial sum. But we can possibly deal with the sum
[math]\sum_{j = 1}^k \frac{1}{jk}[/math]

I don't recognize the series, but if there is one and we can break it down into partial sums I think there might be an outside chance of an induction proof.

Possible do you think?

-Dan
 
I am thinking of using the formula

$$\psi_0^2(k+1) = (H_k -\gamma)^2$$

or possibly solving the integral

$$\left( \int^1_0 \frac{1-x^n}{1-x}\, dx \right)^2 $$
 
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topsquark said:
The harmonic series has no explicit formula for its partial sum. But we can possibly deal with the sum
[math]\sum_{j = 1}^k \frac{1}{jk}[/math]

I don't recognize the series, but if there is one and we can break it down into partial sums I think there might be an outside chance of an induction proof.

Possible do you think?

-Dan
I don't possibly get your idea , could you elaborate ?
 
The "inner" sum (before we square it and take the sum of that) is the 1/jk summation. I was thinking if we could get an explicit formula for that in terms of k we might be able to get a partial sum expression to sum over the square of and proceed inductively. If it works the outer sum would still be nasty as all (Swear) to compute, but it might be a way forward.

-Dan

- - - Updated - - -

ZaidAlyafey said:
$$\left( \int^1_0 \frac{1-x^n}{1-x} \right)^2\, dx $$
There's a typo here. What integral is this?

-Dan
 
We can use the following generating function

$$\sum_{n\geq 1} H^2_n x^n = \frac{\log^2(1-x)+\operatorname{Li}_2(x)}{1-x}$$

$$\sum_{n\geq 1} H^2_n x^{n-1} = \frac{\log^2(1-x)}{1-x}+\frac{\log^2(1-x)}{x}+\frac{\operatorname{Li}_2(x)}{1-x}+\frac{\operatorname{Li}_2(x)}{x}$$

By integrating we get

$$\sum_{n\geq 1}\frac{ H^2_n }{n}x^{n} = -\frac{\log^3(1-x)}{3}+\int^x_0 \frac{\log^2(1-x)}{x}\, dx+\int^x_0 \frac{\operatorname{Li}_2(x)}{1-x}\, dx+\operatorname{Li}_3(x)$$

$$\int^{x}_0 \frac{\operatorname{Li}_2(x)}{1-x}\, dx= -\log(1-x) \operatorname{Li}_2(x)- \int^x_0 \frac{\log^2(1-x)}{x}$$

Hence we have

$$\sum_{n\geq 1}\frac{ H^2_n }{n}x^{n} = -\frac{\log^3(1-x)}{3}-\log(1-x) \operatorname{Li}_2(x)+\operatorname{Li}_3(x)$$

By integrating we get

$$\sum_{n\geq 1}\frac{ H^2_n }{n^2}x^{n} = -\frac{1}{3}\int^x_0 \frac{\log^3(1-x)}{x}\, dx+\frac{ \operatorname{Li}^2_2(x)}{2}+\operatorname{Li}_4(x)$$

Of course this a generalization of the harmonic sum , an attempt to solve the integral will be made later .
 
Let us solve

$$\int^x_0 \frac{\log^3(1-t)}{t}\, dt$$

If we start by parts we get

$$\int^x_0 \frac{\log^3(1-t)}{t}\, dt = \log^3(1-x)\log(x) +3 \int^x_0 \frac{\log^2(1-t) \log(t)}{1-t} \, dt $$

Integrating by parts again we get

$$\int^x_0 \frac{\log^3(1-t)}{t}\, dt = \log^3(1-x)\log(x) +3 \left(\log^2(1-x)\operatorname{Li}_2(1-x)+2 \int^x_0 \frac{\log(1-t) \operatorname{Li}_2(1-t)}{1-t} \right)$$

Simplifying we get

$$\int^x_0 \frac{\log^3(1-t)}{t}\, dt = \log^3(1-x)\log(x)+3 \log^2(1-x)\operatorname{Li}_2(1-x)+6 \int^x_0 \frac{\log(1-t) \operatorname{Li}_2(1-t)}{1-t}\, dt $$

By parts for the third time

$$\int^x_0 \frac{\log^3(1-t)}{t}\, dt = \log^3(1-x)\log(x)+3 \log^2(1-x)\operatorname{Li}_2(1-x)-6 \operatorname{Li}_3(1-x) \log(1-x) +6\operatorname{Li}_4(1-x) -6\zeta(4)$$
 
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So that becomes

\begin{align}
\sum_ {n\geq 1}\frac{ H^2_n }{n^2}x^{n} &= \frac{\pi^4}{45}-\frac{1}{3}\log^3(1-x)\log(x)- \log^2(1-x)\operatorname{Li}_2(1-x)+2 \operatorname{Li}_3(1-x) \log(1-x) \\& \, -2\operatorname{Li}_4(1-x)+\frac{ \operatorname{Li}^2_2(x)}{2}+\operatorname{Li}_4(x )
\end{align}

Putting $x =1$ most of the terms will go BAAAA... m and we are left with

$$ \sum_{n\geq 1}\frac{ H^2_n }{n^2} =\frac{\pi^4}{45}+\frac{\zeta^{\, 2}(2)}{2}+\zeta(4)=\frac{\pi^4}{45}+ \frac{\pi^4}{72}+\frac{\pi^4}{90}=\frac{17 \pi^4}{360}$$

Wasn't that nice !
 
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