Unproved elliptic-integral moment identity involving derivatives

From papers

Let K(x)K(x) and E(x)E(x) denote the complete elliptic integrals of the first and second kinds, respectively, and let K(x)K'(x) and E(x)E'(x) denote their complementary counterparts. The integrals are taken over 0x10\leq x\leq 1. Elliptic-integral moment conjecture.

01(2K(x)24E(x)K(x)+3E(x)2K(x)E(x))dx=0.\int_0^1 \left(2K(x)^2-4E(x)K(x)+3E(x)^2-K'(x)E'(x)\right)\,\mathrm{d}x=0.

The paper states that this is the only entry in its tables for which the authors do not possess a proof, so its status remains open.

Progress summary

Open

The identity remains an open conjecture, with no publicly verified proof or disproof found.

The identity was posed in the 2011 paper Moments of Products of Elliptic Integrals. The authors stated that it was the sole unproved entry in their tables and that proving it would determine five related moments, while they had derived only four relations.

Known results

  • The 2011 paper derives four relations among the five relevant moments, leaving this identity as the missing relation.
  • A 2013 follow-up settles several conjectures from the earlier paper and gives additional elliptic-integral moment evaluations, but does not identify this specific identity as settled.

Current status (as of August 2026): The conjectured identity remains open; no verified proof, disproof, or claim specifically resolving it was found.

Sources
Sources & referencesView supporting material

Primary source

James Wan, “Moments of Products of Elliptic Integrals”, arXiv:1101.1132 (2011).

Solutions 1

Proof

Proof

Here the primes denote complementary modulus, not differentiation:

K(x)=K(1x2)K'(x)=K(\sqrt{1-x^2}) and E(x)=E(1x2)E'(x)=E(\sqrt{1-x^2}).

First consider the complementary moment. Make the substitution

t=(1x)/(1+x)t=(1-x)/(1+x),

so that

x=(1t)/(1+t)x=(1-t)/(1+t), dx=2dt/(1+t)2\quad dx=-2\,dt/(1+t)^2,

and

1x2=2t/(1+t)\sqrt{1-x^2}=2\sqrt{t}/(1+t).

The Landen formulas give

K(2t/(1+t))=(1+t)K(t)K(2\sqrt{t}/(1+t))=(1+t)K(t)

and

E(2t/(1+t))=(2E(t)(1t2)K(t))/(1+t)E(2\sqrt{t}/(1+t)) =\bigl(2E(t)-(1-t^2)K(t)\bigr)/(1+t).

Consequently,

01K(x)E(x)dx=01(4K(t)E(t)(1+t)22(1t)1+tK(t)2)dt.\int_0^1 K'(x)E'(x)\,dx = \int_0^1 \left( \frac{4K(t)E(t)}{(1+t)^2} -\frac{2(1-t)}{1+t}K(t)^2 \right)dt.

Subtracting this from the other three terms in the conjectured integral and renaming tt as xx, it remains to prove

01F(x)dx=0,\int_0^1 F(x)\,dx=0,

where

F(x)=41+xK(x)2(4+4(1+x)2)K(x)E(x)+3E(x)2.F(x)= \frac{4}{1+x}K(x)^2 -\left(4+\frac{4}{(1+x)^2}\right)K(x)E(x) +3E(x)^2.

Use the standard derivative identities

dKdx=E(1x2)Kx(1x2),dEdx=EKx.\frac{dK}{dx} = \frac{E-(1-x^2)K}{x(1-x^2)}, \qquad \frac{dE}{dx} = \frac{E-K}{x}.

Define

G(x)=(x1)(2K(x)22x+2x+1K(x)E(x)+x+2x+1E(x)2).G(x)=(x-1)\left( 2K(x)^2 -2\frac{x+2}{x+1}K(x)E(x) +\frac{x+2}{x+1}E(x)^2 \right).

Direct differentiation using the two identities above, followed by collecting the coefficients of K2K^2, KEKE, and E2E^2, gives

dGdx=F(x).\frac{dG}{dx}=F(x).

At x=0x=0, since K(0)=E(0)=π/2K(0)=E(0)=\pi/2,

G(0)=2(K(0)E(0))2=0.G(0)=-2\bigl(K(0)-E(0)\bigr)^2=0.

As x1x\to1^-, we have E(x)1E(x)\to1 and

K(x)=O(log11x).K(x)=O\left(\log\frac1{1-x}\right).

The factor x1x-1 in GG therefore implies G(x)0G(x)\to0, because

(1x)log211x0.(1-x)\log^2\frac1{1-x}\longrightarrow0.

The same estimates show that the improper integrals converge. Applying the fundamental theorem of calculus first on compact subintervals and then passing to the endpoints gives

01F(x)dx=G(1)G(0)=0.\int_0^1F(x)\,dx=G(1^-)-G(0)=0.

Together with the Landen substitution, this proves

01(2K(x)24E(x)K(x)+3E(x)2K(x)E(x))dx=0.\int_0^1 \left( 2K(x)^2-4E(x)K(x)+3E(x)^2-K'(x)E'(x) \right)dx=0.

Sources:

Original conjecture: https://arxiv.org/abs/1101.1132

Landen transformation: https://dlmf.nist.gov/19.8.E12

Derivative identities: https://dlmf.nist.gov/19.4.E1 https://dlmf.nist.gov/19.4.E2

Endpoint asymptotics: https://dlmf.nist.gov/19.12

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