Vieta’s formulas and ζ(2)\zeta(2)

(This is Yan Sheng.)

At some point I came up with a new idea to prove the famous identityζ(2)n=11n2=π26.\zeta(2)\coloneqq\sum_{n=1}^\infty\frac1{n^2}=\frac{\pi^2}6.There is no shortage of existing proofs of this identity; see this math.SE question, or this collection of proofs compiled by Robin Chapman. I was inspired by this illuminating video, where 3Blue1Brown explains an elementary proof based on Euclidean geometry, by a physical interpretation involving systems of lighthouses. My new idea comes from trying to translate this proof into the complex plane.

Vieta’s formulas

The main idea in the video is to get an expression for the sum of inverse squared distances from the origin to the vertices of a certain regular nn-gon. We first observe that when viewed on the complex plane, the vertices of this nn-gon are the roots of some polynomial of degree nn, and the sum of inverse squares can be computed by Vieta’s formulas.

More explicitly, suppose that ρ1,ρ2,,ρn\rho_1,\rho_2,\ldots,\rho_n​ are the roots of the polynomialanzn+an1zn1++a1z+a0=0,a_nz^n+a_{n-1}z^{n-1}+\cdots+a_1z+a_0=0,with an0a_n\neq0 (so that there are nn roots) and a00a_0\neq0 (so the roots are nonzero), and we want to find the sum of inverse squares j1ρj2\sum_j\frac1{\rho_j^2}.

The astute reader might have noticed that this objective is different from the video, which computes j1ρj2\sum_j\frac1{\lvert\rho_j\rvert^2} instead. We chose this reformulation because it is easier to handle algebraically.

If we had wanted to find the sum of squares jρj2\sum_j\rho_j^2 instead, we could use the following calculation:jρj2=j,kρjρkj<kρjρkj>kρjρk=(jρj)22j<kρjρk=()(an1an)22an2an=an122anan2an2,()\begin{aligned} \sum_j\rho_j^2&=\sum_{j,k}\rho_j\rho_k-\sum_{j< k}\rho_j\rho_k-\sum_{j>k}\rho_j\rho_k\\ &=\left(\sum_j\rho_j\right)^2-2\sum_{j< k}\rho_j\rho_k\\ &\overset{(* )}=\left(-\frac{a_{n-1}}{a_n}\right)^2-2\frac{a_{n-2}}{a_n}\\ &=\frac{a_{n-1}^2-2a_na_{n-2}}{a_n^2},\qquad(\dagger) \end{aligned}where for ()(*) we used Vieta’s formulasjρj=an1an,j<kρjρk=an2an.\sum_j\rho_j=-\frac{a_{n-1}}{a_n},\qquad\sum_{j< k}\rho_j\rho_k=\frac{a_{n-2}}{a_n}.To get the sum of inverse squares instead, we need to apply the above formula to some polynomial with roots 1ρ1,1ρ2,,1ρn\frac1{\rho_1},\frac1{\rho_2},\ldots,\frac1{\rho_n}. But this is exactly what the reciprocal polynomial does: if we reverse the order of the coefficients of a polynomial, the roots of the new polynomial are the reciprocals of the original roots. To show this, note thatanρjn+an1ρjn1++a1ρj+a0=0    an+an1ρj++a1ρjn1+a0ρjn=0, \begin{aligned} a_n\rho_j^n+a_{n-1}\rho_j^{n-1}+\cdots+a_1\rho_j+a_0&=0\\ \implies a_n+\frac{a_{n-1}}{\rho_j}+\cdots+\frac{a_1}{\rho_j^{n-1}}+\frac{a_0}{\rho_j^n}&=0, \end{aligned}so the polynomial a0zn+a1zn1++an1z+an=0a_0z^n+a_1z^{n-1}+\cdots+a_{n-1}z+a_n=0 has roots 1ρj\frac1{\rho_j}. Now the formula ()(\dagger) applied to this polynomial givesj1ρj2=a122a0a2a02.\sum_j\frac1{\rho_j^2}=\frac{a_1^2-2a_0a_2}{a_0^2}.

An Eulerian “proof”

In the video, a sequence of regular polygons is chosen such that the vertices tend to the sequence of odd integers on the real line. In our reformulation, we should thus choose a sequence of polynomials fnf_n which tends to some power series ff with regularly spaced roots. For our purposes, we will choosef(z)=ez1z=1+12z+16z2+, \begin{aligned} f(z)&=\frac{e^z-1}z\\ &=1+\frac12z+\frac16z^2+\cdots, \end{aligned}which has roots 2πik2\pi ik for kZ\0k\in\mathbb Z\backslash{0}.

If we pretend that our sum-of-inverse-squares formula works not just for polynomials, but for general power series, then applying it to ff giveskZ\{0}1(2πik)2=(12)22(1)(16)1224π2k=11k2=112ζ(2)=π26, \begin{aligned} \sum_{k\in\mathbb Z\backslash\{0\}}\frac1{(2\pi ik)^2}&=\frac{(\frac12)^2-2(1)(\frac16)}{1^2}\\ -\frac2{4\pi^2}\sum_{k=1}^\infty\frac1{k^2}&=-\frac1{12}\\ \zeta(2)&=\frac{\pi^2}6, \end{aligned}which is a “proof” in the style of Euler that I think he might have enjoyed.

A dead end?

To make the argument rigorous, we need polynomials fnf_n whose roots all lie on a circle, with fnff_n\to f as nn\to\infty; a very nice choice is given byfn(z)=(1+zn)n1z=1+(n2)n2z+(n3)n3z2+, \begin{aligned} f_n(z)&=\frac{(1+\frac zn)^n-1}z\\ &=1+\frac{\binom n2}{n^2}z+\frac{\binom n3}{n^3}z^2+\cdots, \end{aligned}which has roots at n(e2πik/n1)n(e^{2\pi ik/n}-1) for nkn\nmid k, ie. lying on a circle with radius nn centred at z=nz=-n. As a sanity check, note that for fixed kk, we have n(e2πik/n1)2πikn(e^{2\pi ik/n}-1)\to2\pi ik; hence the roots of fnf_n “tend pointwise” to the roots of ff.

However, this is not enough to show that the sum-of-inverse-squares of the nn roots of fnf_n tends to the sum-of-inverse-squares of the roots of ff. This is where our argument falls short of the geometric proof, which had good control on the error of the finite approximation.

A tour de force

To finish the argument, we have to abandon our initial hopes for a quick proof, and get some exact expressions from the sum-of-inverse-squares formula.

We fix nn, and set ω=e2πi/n\omega=e^{2\pi i/n}. Then the roots of fnf_n are ρk,nn(ωk1)\rho_{k,n}\coloneqq n(\omega^k-1) for 1kn11\leq k\leq n-1. Note that1n(1ωk1+12)=12nωk+1ωk1=12nωk/2+ωk/2ωk/2ωk/2=i2ncotkπn. \begin{aligned} \frac1n\left(\frac1{\omega^k-1}+\frac12\right)&=\frac1{2n}\frac{\omega^k+1}{\omega^k-1}\\ &=\frac1{2n}\frac{\omega^{k/2}+\omega^{-k/2}}{\omega^{k/2}-\omega^{-k/2}}\\ &=-\frac i{2n}\cot\frac{k\pi}n. \end{aligned}Hence1ρk,n=12n(1icotkπn)1ρk,n2=14n2(1cot2kπn+2icotkπn). \begin{aligned} \frac1{\rho_{k,n}}&=\frac1{2n}\left(-1-i\cot\frac{k\pi}n\right)\\ \frac1{\rho_{k,n}^2}&=\frac1{4n^2}\left(1-\cot^2\frac{k\pi}n+2i\cot\frac{k\pi}n\right). \end{aligned}We can sum this over kk, take the real part, and compare with the sum-of-inverse-squares formula to obtain14n2k=1n1(1cot2kπn)=((n2)n2)22(1)((n3)n3)12=(n1)(n5)12n2k=1n1cot2kπn=(n1)(n2)3k=1(n1)/2cot2kπn=(n1)(n2)6, \begin{aligned} \frac1{4n^2}\sum_{k=1}^{n-1}\left(1-\cot^2\frac{k\pi}n\right)&=\frac{(\frac{\binom n2}{n^2})^2-2(1)(\frac{\binom n3}{n^3})}{1^2}\\ &=-\frac{(n-1)(n-5)}{12n^2}\\ \sum_{k=1}^{n-1}\cot^2\frac{k\pi}n&=\frac{(n-1)(n-2)}3\\ \sum_{k=1}^{(n-1)/2}\cot^2\frac{k\pi}n&=\frac{(n-1)(n-2)}6, \end{aligned}since cot2(πθ)=cot2θ\cot^2(\pi-\theta)=\cot^2\theta.

Now we are in the position to finish as in Cauchy’s proof of the identity, by invoking the following trick: adding 1 to each term above givesk=1(n1)/2csc2kπn=(n1)(n+1)6.\sum_{k=1}^{(n-1)/2}\csc^2\frac{k\pi}n=\frac{(n-1)(n+1)}6.By the elementary inequality sinθ<θ<tanθ\sin\theta<\theta<\tan\theta for θ(0,π2)\theta\in(0,\frac\pi2), we havecot2θ<1θ2<csc2θk=1(n1)/2cot2kπn<k=1(n1)/2n2k2π2<k=1(n1)/2csc2kπnπ26(n1)(n2)n2<k=1(n1)/21k2<π26(n1)(n+1)n2, \begin{gathered} \cot^2\theta< \frac1{\theta^2}< \csc^2\theta\\ \sum_{k=1}^{(n-1)/2}\cot^2\frac{k\pi}n< \sum_{k=1}^{(n-1)/2}\frac{n^2}{k^2\pi^2}< \sum_{k=1}^{(n-1)/2}\csc^2\frac{k\pi}n\\ \frac{\pi^2}6\frac{(n-1)(n-2)}{n^2}< \sum_{k=1}^{(n-1)/2}\frac1{k^2}< \frac{\pi^2}6\frac{(n-1)(n+1)}{n^2}, \end{gathered}and we finish by taking nn\to\infty.

Exercise: Can we calculate ζ(4)n=11n4\zeta(4)\coloneqq\sum_{n=1}^\infty\frac1{n^4} similarly? How annoying is it going to be?

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