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The interior-maximum qualification in equation (33)


Source. Bernstein 1931, equations (32)--(33), printed p. 1040 / PDF p. 16, with the setup on printed p. 1039 / PDF p. 15, in the complete source. Equation (33) displays

F(ξ)>12log⁡n−O(log⁡log⁡log⁡n)F(\xi)>\frac12\log n-O(\log\log\log n)

when the maximum of the nodal polynomial's modulus on a fixed interval is attained at an interior point. This page preserves that source claim and separates it from the version completely derived below.

A version with explicit uniform hypotheses. Fix I=[α,β]⊆[−1,1]I=[\alpha,\beta]\subseteq[-1,1] of length L>0L>0 and 0<η≤L/20<\eta\le L/2. For each degree dd, suppose there is a point

ξ∈[α+η,β−η],∣A(ξ)∣=max⁡I∣A∣,\xi\in[\alpha+\eta,\beta-\eta], \qquad |A(\xi)|=\max_I|A|,

where AA is the nodal polynomial for d+1d+1 distinct nodes in [−1,1][-1,1]. Put M=max⁡IFM=\max_I F and m=⌊d/2⌋m=\lfloor d/2\rfloor. For all sufficiently large dd, uniformly in the nodes,

M>12log⁡ηm2log⁡(2log⁡d)=12log⁡d−OI,η(log⁡log⁡log⁡d).(H)M>\frac12\log\frac{\eta m}{2\log(2\log d)} =\frac12\log d-O_{I,\eta}(\log\log\log d). \tag{H}

In the case M≤log⁡dM\le\log d, the finite right side is also a lower bound for F(ξ)F(\xi) itself.

Proof. If M>log⁡dM>\log d, (H) is immediate for d≥16d\ge16, because η≤1\eta\le1, m≤d/2m\le d/2, and log⁡(2log⁡d)>1\log(2\log d)>1 make its right side less than log⁡d\log d. Otherwise the local gap companion applies with

D=2log⁡(2M)m≤D0=2log⁡(2log⁡d)m.D=\frac{2\log(2M)}m \le D_0=\frac{2\log(2\log d)}m.

Take dd large enough that D0<η/2D_0<\eta/2. There is a first node u<α+Du<\alpha+D in II and a last node v>β−Dv>\beta-D in II. Hence ξ−u>η/2\xi-u>\eta/2 and v−ξ>η/2v-\xi>\eta/2. The consecutive nodes surrounding ξ\xi belong to this block and have gap δ<D\delta<D. Equation (T2) on the telescoping page therefore gives

F(ξ)>14log⁡4(ξ−u)(v−ξ)δ2>12log⁡ηD≥12log⁡ηD0.F(\xi)> \frac14\log\frac{4(\xi-u)(v-\xi)}{\delta^2} >\frac12\log\frac{\eta}{D} \ge\frac12\log\frac{\eta}{D_0}.

This is (H). Its asymptotic form follows as on the all-cases local-bound page. All inequalities remain valid when II touches ±1\pm1.

Unresolved source implication. Equation (32) retains the factor (ξ−ap)(aq−ξ)(\xi-a_p)(a_q-\xi). The assertion that ξ\xi is an interior point, for each degree separately, does not by itself give a degree-independent positive lower bound for these two distances. For example, the logical condition α<ξd<β\alpha<\xi_d<\beta permits ξd−α→0\xi_d-\alpha\to0; this observation is not a counterexample involving nodal polynomials.

The source's displayed passage from (32) to (33) does not explicitly provide the additional uniform-distance estimate. This compilation does not prove or refute (33) under its bare interiority wording. The exact remaining obligation is to justify the necessary product control from the nodal-maximum hypotheses, or to state an appropriate additional hypothesis. The theorem (H) above uses the explicit sufficient hypothesis of uniform separation. It is not presented as an author-issued correction.

Proof scope. The uniformly separated version has a complete rewritten proof, reviewed on 6 September 2026 as component C7 of the local-chain review, which passed it conditionally on the (T1) correction now present in equation (32). The bare-interiority source implication and the claim at a selected nodal maximum in the large-MM case remain unresolved. Neither is needed for the completed 1/41/4 local-maximum argument. No sharp 2/π2/\pi or formal credit follows.

Bears on. Problem 1153, qualified historical bound.