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Research notes on every problem, and a library of the papers behind them. Built from the open erdos repository.

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We give the mathematical bridge for the claim. All computational steps below are author evidence, without an independent audit of the engine.

The two pencils and their coverage

For FD=z4−32z2−zF_D=z^4-\tfrac32z^2-z, FD′=4(z−1)(z+12)2F_D'=4(z-1)(z+\tfrac12)^2. Its critical values are −32-\tfrac32 at 11 and 316\tfrac3{16} at the double critical point −12-\tfrac12. For FE=z4−2z2F_E=z^4-2z^2, FE′=4z(z−1)(z+1)F_E'=4z(z-1)(z+1). Its critical values are −1-1 at 1,−11,-1 and 00 at 00. Denote the two ordered values of either quartic by fA<fBf_A<f_B, and put d=fB−fAd=f_B-f_A.

Every circle through these values has center on their perpendicular bisector. After conjugation, which preserves the integral because the quartics have real coefficients, it is represented by

R=d2sin⁡β,C=fA+fB2+iRcos⁡β,0<β≤π/2.R=\frac{d}{2\sin\beta},\qquad C=\frac{f_A+f_B}{2}+iR\cos\beta, \qquad 0<\beta\le\pi/2.

The value β=0\beta=0 represents the real line. Thus the compact interval [0,π/2][0,\pi/2] covers the entire pencil, including its line limit. The flattening parametrization used by the program is

σ(x)=fA+e−iβx1−iκx/2,κ=2sin⁡βd.\sigma(x)=f_A+\frac{e^{-i\beta}x}{1-i\kappa x/2},\qquad \kappa=\frac{2\sin\beta}{d}.

It has the displayed circle as its image when β>0\beta>0 and is the real line when β=0\beta=0.

The certified integral

The evidence account and the docstring and formulas of wiki/research/erdos_114/quartic_evidence/evidence/main.py specify the finite computation. The mathematical bounds it applies are the Crofton window estimate, certified inverse-root discs, the singular weight identity and the far-field factorization proved in the research sketch, under "Uniform estimates through the degenerations".

For the flatter circles it subtracts the reference density pointwise; for the other circles it bounds the nonnegative density integral and subtracts the exact reference integral. Every accepted bound is uniform both in its angle box and in its integration piece. All roots used in those bounds are included in four pairwise disjoint discs certified by Rouché's theorem. Singular windows use full preimage length bounds. The signed pieces share exact endpoints, and the signed tail is bounded as an integral, so no overlap of an unknown sign is discarded.

The full check accepts only if the angle boxes tile the specified interval and every upper bound is strictly below −1-1. Its last edge is checked to exceed π/2\pi/2. The retained computation gives 142 accepted boxes for FDF_D and 126 for FEF_E, with largest upper bounds less than −1.021-1.021 and −1.077-1.077, respectively. These quoted decimal bounds are rounded outward from the enclosures printed by the program. It follows that the integral is below −1-1 at every parameter in the two pencils.

Local inverse singularities have exponent at most 2/32/3 on these pencils, and the reference exponent is 3/43/4, so the finite singularities are integrable. The retained far-field estimate makes the signed difference absolutely integrable at the line's infinity as well.

Run the complete evidence from the repository root with

sh
uv run --no-sync python wiki/research/erdos_114/quartic_evidence/evidence/main.py

The full check uses 80-bit Arb and Acb balls and takes about forty-five minutes of one thread per pencil. The options --only double and --only equal partition it into its two required checks. The --quick option covers only selected boxes and cannot establish this claim. The approximate line values used in the controls test the implementation; the proof of the bounds comes from the certified enclosures themselves.

Passage to polynomial length

Let Γ\Gamma be a circle with center CC and radius RR, and set p(z)=R−1F(R1/4z)−C/Rp(z)=R^{-1}F(R^{1/4}z)-C/R. Inverse-branch integration gives

ℓ(p)=R−1/4∫ΓGF(σ) ∣dσ∣.\ell(p)=R^{-1/4}\int_\Gamma G_F(\sigma)\,|d\sigma|.

The inverse-derivative density of w4+fAw^4+f_A is ∣σ−fA∣−3/4|\sigma-f_A|^{-3/4}. Because fAf_A lies on Γ\Gamma, its preimage is, after rotation and the scale R1/4R^{1/4}, the lemniscate of z4−1z^4-1. Consequently its length is R1/4ℓ(z4−1)R^{1/4}\ell(z^4-1). Subtracting these two identities yields

ℓ(p)−ℓ(z4−1)=R−1/4I~(F,Γ)<−R−1/4.\ell(p)-\ell(z^4-1) =R^{-1/4}\widetilde I(F,\Gamma)<-R^{-1/4}.

This proves the length consequence. The argument covers the two collision pencils only and makes no assertion about all quartics.