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Let pp be a local maximizer as in the claim, and suppose that aa is a critical value with ∣a∣≠1|a|\ne1. Choose a disc U=D(a,r)U=D(a,r) whose closure misses the unit circle and all other distinct critical values.

The source premise

We use the construction in the proof of Eremenko and Hayman's Lemma 5, pp. 5--6 of the authors' corrected preprint identified on the source card. Choose a smooth function Φ\Phi supported in UU with Φ(a)=1\Phi(a)=1 and put ϕλ(w)=w+λΦ(w)\phi_\lambda(w)=w+\lambda\Phi(w). For λ\lambda in a sufficiently small complex disc about zero, the source constructs quasiconformal maps ψλ\psi_\lambda, with ψ0(z)=z\psi_0(z)=z and

ψλ(z)=z+o(1)(z→∞),pλ=ϕλ∘p∘ψλ−1.\psi_\lambda(z)=z+o(1)\quad(z\to\infty),\qquad p_\lambda=\phi_\lambda\circ p\circ\psi_\lambda^{-1}.

The pλp_\lambda are monic quartics, continuous in their coefficients, and their critical values are those of pp with aa replaced by a+λa+\lambda. Multiplicities are preserved; all critical points with value aa move in this way. The maps ψλ\psi_\lambda are conformal off p−1(U‾)p^{-1}(\overline U), depend holomorphically on λ\lambda at each such point, and are conformal on a common neighborhood of E(p)E(p). The source gives

E(pλ)=ψλ(E(p)),ℓ(pλ)=∫E(p)∣ψλ′(z)∣ ∣dz∣.(1)E(p_\lambda)=\psi_\lambda(E(p)),\qquad \ell(p_\lambda)=\int_{E(p)}|\psi_\lambda'(z)|\,|dz|. \tag{1}

The function hz(λ)=ψλ′(z)h_z(\lambda)=\psi_\lambda'(z) is holomorphic in λ\lambda for each zz in that neighborhood, with hz(0)=1h_z(0)=1. On compact subsets the needed parameter and spatial continuity follow from the source's analytic-dependence construction and the Cauchy formula in zz.

This local construction is used as an external source premise. Its formulas, normalization, support, analytic dependence and length formula were read in proof on 2026-10-15 against pp. 5--7 of the corrected preprint identified on the source card, including the page images and transcription; the Beltrami existence and analytic-dependence theorems cited there are not re-proved here. The source's continuation along arcs is not used.

Constancy of length forces a trivial deformation

By (1), λ↦ℓ(pλ)\lambda\mapsto\ell(p_\lambda) is subharmonic. Local maximality of pp, and continuity of the coefficients of pλp_\lambda, make it at most ℓ(p)\ell(p) in a small disc. The maximum principle makes it constant there.

Fix a circle ∣λ∣=ρ|\lambda|=\rho contained in that disc. For each z∈E(p)z\in E(p) the mean-value inequality gives

12π∫02π∣hz(ρeiθ)∣ dθ≥1.\frac1{2\pi}\int_0^{2\pi}|h_z(\rho e^{i\theta})|\,d\theta\ge1.

Integrating over E(p)E(p) and using (1) and constancy shows equality for arclength-almost every z∈E(p)z\in E(p). Equality forces hz≡1h_z\equiv1 in ∣λ∣<ρ|\lambda|<\rho: the mean of hzh_z is hz(0)=1h_z(0)=1, and equality in the triangle inequality says that its boundary values lie on the nonnegative real axis almost everywhere. Continuity makes the boundary imaginary part zero everywhere, the harmonic maximum principle makes it zero in the disc, and the open mapping theorem makes hzh_z constant.

We next check the spatial component on which this equality holds. The open set

Ω=C∖p−1(U‾)={z:∣p(z)−a∣>r}\Omega=\mathbb C\setminus p^{-1}(\overline U) =\{z:|p(z)-a|>r\}

is connected. Indeed it contains a neighborhood of infinity, and a bounded component would have ∣p−a∣=r|p-a|=r on its boundary and ∣p−a∣>r|p-a|>r inside, contradicting the maximum modulus principle for the polynomial p−ap-a. Since U‾\overline U misses the unit circle, E(p)⊂ΩE(p)\subset\Omega.

Fix ∣λ∣<ρ|\lambda|<\rho. The holomorphic function ψλ′−1\psi_\lambda'-1 on Ω\Omega vanishes at arclength-almost every point of E(p)E(p). The latter contains a regular arc: take any unit value that is not one of the finitely many critical values and apply the inverse function theorem. Zeros on that arc have an accumulation point in Ω\Omega. The identity theorem therefore gives ψλ′≡1\psi_\lambda'\equiv1 on Ω\Omega. Connectedness gives ψλ(z)=z+bλ\psi_\lambda(z)=z+b_\lambda there, and the principal normalization at infinity forces bλ=0b_\lambda=0.

For z∈Ωz\in\Omega we have ϕλ(p(z))=p(z)\phi_\lambda(p(z))=p(z), so the defining identity for pλp_\lambda now gives pλ(z)=p(z)p_\lambda(z)=p(z). Polynomial identity implies pλ=pp_\lambda=p everywhere. For a sufficiently small nonzero λ\lambda, however, a+λa+\lambda is a critical value of pλp_\lambda and is not a critical value of pp, since UU contains no other such value. This is a contradiction.

Thus a local maximizing quartic has no critical value off the unit circle, as claimed. The argument is author-recorded; it does not assert an independent audit of the source construction.