MathLabs

Worked solution: The Beukers–Calabi–Kolk double-integral proof (1993)

Step 1 of 6: Split into odd and even squares
In plain words

Sort the terms of ζ(2)\zeta(2) into two piles by whether the index is odd or even, the way you might sort socks by color. The even pile turns out to be an exact quarter-sized copy of the whole sum, so subtracting it away and solving for ζ(2)\zeta(2) leaves only the odd pile — the sum over 1,3,5,…1,3,5,\dots — to understand.

ζ(2)=∑n=1∞1n2=∑k=0∞1(2k+1)2+14∑m=1∞1m2 ⟹ ζ(2)=43∑k=0∞1(2k+1)2\zeta(2)=\sum_{n=1}^{\infty}\frac{1}{n^2}=\sum_{k=0}^{\infty}\frac{1}{(2k+1)^2}+\frac14\sum_{m=1}^{\infty}\frac{1}{m^2}\ \Longrightarrow\ \zeta(2)=\frac43\sum_{k=0}^{\infty}\frac{1}{(2k+1)^2}
Detailed analysis

Separating even indices n=2mn=2m from odd indices n=2k+1n=2k+1 turns the even part into 14ζ(2)\tfrac14\zeta(2) itself; solving for ζ(2)\zeta(2) reduces the whole problem to the sum over odd squares only, which matches a natural double integral in the next step.

Terms in this step
ζ(2)\zeta(2)
Standard shorthand for the value at 22 of the Riemann zeta function, ζ(s)=∑n=1∞1/ns\zeta(s)=\sum_{n=1}^\infty 1/n^s — here the infinite sum ∑1/n2\sum 1/n^2 from the Basel problem.
Knowledge used in this step