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Paths in Polynomial Lemniscates: Proofs and Examples

Erdős #1041 75 pp Equations typeset from the exact TeX

Précis

For a monic trinomial with roots in the open unit disc, any two distinct roots are joined inside {|f|<1} by a path of length less than 2. For any squarefree monic polynomial of degree n2, an area-growth argument gives such a path when the least critical-value modulus μ is at most 13/25; scaling gives length less than (5/2)μ1/n inside {|f|<(25/13)μ}. The record develops this argument, an inverse-ray averaging estimate, and a construction using an isolated simple critical value, together with results for collinear roots and several coefficient families. A weighted Poisson identity gives a sharp mean bound on critical values; examples distinguish that bound from path-length control. The final sections examine inverse-sheet topology and refute an earlier spanning-tree estimate. These results do not prove the unrestricted length-2 assertion.

This paper owns the complete problem-specific reasoning surface for Erdős #1041, including all registered result families and their boundaries.

It is not authority for the validity of claims tagged Lean, which belongs to the cited kernel-checked source, or a solution to Erdős #1041, which remains open.

In this paper

The short note centres on the trinomial identity in Section 2. That proof does not use Newton flow. The area-growth comparison is proved here in Section 3. The other constructions are independent of that proof. This record provides their derivations and keeps failed estimates beside the witnesses that refute them.

Short-note passage Argument in this record
Section 3: small critical value Section 3: inverse-map lengths, packing, area growth and the rational certificate.
Supplement after Section 3: area estimate Section 4: regular-level selection, low and high lifts, and the adjacent-pair average.
Section 6: isolated critical value Section 6: the two-sheeted component, square-root map, Bergman segment bound and capacity estimate.
Sections 13–14: chords and collinear roots Section 8: the exact binomial chord calculation; Section 7.1: Chebyshev comparison and related extremal problems.
Section 15: critical-value means Section 8: the reflected derivative, weighted Poisson identity, boundary passage and equality cases.
Section 17: limits and examples Section 8, subsections Limits of contained paths at fixed degree and Blaschke-product examples and limits in varying degree.

The historical question

Problem 1.1 (Erdős #1041). Let f(z)=i=1n(zzi) be monic of degree n2, with ziD, the open unit disc. Must two of the roots be joined by a curve of length less than 2 lying in the open lemniscate {zC:|f(z)|<1}?

The open-disc hypothesis is essential for this formulation. For f(z)=z21, whose roots lie on the unit circle, every continuous path from 1 to 1 meets the imaginary axis. There |f(iy)|=1+y21, so no such path lies in the open unit lemniscate. Repeated roots, counted as distinct occurrences, give a constant path; the substantive case is therefore squarefree.

The problem numbering follows Bloom’s Erdős problem catalogue . A degree-seven counterexample to the unrestricted assertion has been reported to the author. Its proof is not reproduced or independently verified in this revision. We therefore refer to the displayed assertion as the historical question, not as an assertion that the unrestricted bound remains open. The original source is Problem 5 on printed p. 139 of Erdős–Herzog–Piranian [4]; the preceding paragraph records the known input that one component of the lemniscate contains at least two zeros.

The main constructions use different kinds of information. The trinomial identity controls a prescribed path directly. The area argument instead uses the number of roots in a sublevel component. Source comparisons for component counts and lemniscate topology accompany the inverse-sheet discussion in Section 11; the Newton-flow terminology is introduced in Section 9.

Two recent manuscripts are relevant. The 48-page manuscript posted by shtuka on 24 March 2026 [10] claims the unrestricted statement. Its Proposition 12 (p. 16, with proof continuing through p. 30) supplies the spanning-tree decomposition used in the final proof. The defect was located publicly in the problem’s discussion thread: on 25 March 2026 Tao observed that the invocation of Lemma 8 there is unjustified and that the flow lines need not organise into connected trees, and on 26 March 2026 the manuscript’s author agreed that the statement of Proposition 12 itself, not only its printed proof, is incorrect, and set the strategy aside. Section 11 records an independent diagnosis of the same local saddle defect, together with the Cassini obstruction to the printed global tree-length bound. That obstruction refutes the metric estimate used in the final proof, not Erdős #1041. Pendyala’s independent June 2026 preprint [11] proves the degree-four case through a finite four-point radial lemma and a short polygonal connector. That is the degree-four result directly comparable to the root-pair problem. Together with the cubic theorem established here, it settles these two degrees; it does not supply the general-degree conclusion. The all-degree estimates below either impose a bound on the least critical-value modulus or allow a larger length constant and containment level. They address different hypotheses from the quartic theorem.

Trinomials

Write Ef={zC:|f(z)|<1}. The first theorem gives a prescribed path between every pair of zeros of a trinomial, in every degree.

Theorem 2.1 (trinomial root connections). Let n,m be integers with 1m<n, and let f(z)=zn+azm+b have every zero in D. For every zero ζ, the segment [0,ζ] lies in Ef. Consequently any two zeros ζ1,ζ2 are joined in Ef by the broken line ζ10ζ2, of length |ζ1|+|ζ2|<2.

Proof. Vieta’s formula gives |b|<1. At a zero ζ the root equation ζn+aζm+b=0 eliminates the middle coefficient:

(1)f(tζ)=b(1tm)+ζn(tntm).

For 0t<1 the two scalar weights 1tm and tmtn are nonnegative and sum to 1tn, so

|f(tζ)||b|(1tm)+|ζ|n(tmtn)<1tn1.

At t=1 the value is zero. Concatenating two such segments gives the length assertion. ◻

The coefficient a carries no hypothesis; the root equation removes it before absolute values are taken. The conclusion concerns segments to zeros and makes no assertion that Ef is star-shaped.

The cancellation mechanism.

For f(z)=k=0nckzk and a zero ζ, put Sj=k=0jckζk. Finite summation by parts gives

(2)f(tζ)=j=0n1(tjtj+1)Sj(0t1),

since the coefficient of ckζk on the right is tktn and k<nckζk=cnζn. The weights in (2) are nonnegative and sum to 1tn, so the whole radial segment lies in the closed unit sublevel set whenever every partial sum lies in the closed unit disc. For a trinomial, Sj=b for j<m and Sj=ζn for mj<n; these two values may coincide. This is exactly the estimate above. With two intermediate coefficients, the root-disc hypothesis need not put every partial sum in the unit disc. The next example shows that a prescribed radial segment can then escape.

Example 2.2 (an escaping root spoke). Let 0<r<1 satisfy r6>320/327, and set

fr(z)=z6+15r2z415r4z2r6=(z2r2)(z4+65r2z2+r4).

Every zero has modulus r: for the quartic factor put z=rw, so that the squared roots solve v2+(6/5)v+1=0, whose two roots are complex conjugates of product one. Nevertheless

fr(r/2)=327320r6,

so the segment [0,r] leaves Efr. This rules out a universal assertion about every origin-to-zero segment. It exhibits no counterexample to the existence of some short connection.

Sources and scope.

The identity (2) is checked as the Abel summation identity, the constant-term bound as the constant-term estimate from the root-disc hypothesis, the radial estimate as containment along a trinomial root segment, and their combination with the length bound as the two segment inequalities and their length bound. Example 2.2 is checked as the sextic evaluation. What the kernel proves is the pair of radial inequalities and the bound |ζ1|+|ζ2|<2 on the sum of the two radii. Assembling those into a single rectifiable path object, and the passage to the one-dimensional Hausdorff measure used by the original formulation of the problem, are ordinary steps taken here. No novelty claim is made for this elementary trinomial argument.

A small least critical value

The next criterion restricts the smallest critical-value modulus, but places no condition on the coefficients or the root locations. Throughout this section

μ=minf(c)=0|f(c)|

is the least critical-value modulus.

Theorem 3.1 (a small least critical value forces a short connector). Let f be squarefree and monic of degree n2 with μ13/25. Then two distinct roots of f are joined inside {|f|<1} by a rectifiable curve of length strictly below 2. No hypothesis is placed on the locations of the roots, on the number of roots in any component, or on the capacity of any component.

For f(z)=znb with 0<|b|<1, the only critical point is 0 and μ=|b|. Thus this criterion includes |b|13/25 but excludes 13/25<|b|<1, although the trinomial theorem gives the required path in both ranges. Its value is that it also applies to polynomials with arbitrary coefficient patterns, including roots outside the unit disc. For example, (z3)n1/2, n2, has μ=1/2 and all its roots satisfy |z|>2. The required containment is |f(z)|<1, not |z|<1.

Corollary 3.2 (scale-free form). Every squarefree monic f of degree n2 has two distinct roots joined inside {|f|<(25/13)μ} by a curve of length below 2((25/13)μ)1/n.

Proof. Apply Theorem 3.1 to snf(sz) with s=((25/13)μ)1/n, whose least critical-value modulus is 13/25, and scale back. Squarefreeness gives μ>0, so the scaling factor is positive. ◻

The proof has two steps. Failure of the length bound first forces the roots to be far apart in the hyperbolic metric of a sublevel component. Packing those roots gives a lower bound for their number. Averaging paths between adjacent boundary points then converts that root count into an area-growth inequality. The rational certificate shows that this growth would exceed Pólya’s area bound before the value level reaches 1.

Consequences of having no short path.

Assume no two distinct roots are joined inside {|f|<1} by a curve of length below 2. Choose a critical point at level μ and two descending inverse arcs into distinct one-root components of {|f|<μ}; below μ each component maps conformally onto the value disc, and distinct local inverse arcs at the first critical point enter distinct components, since two inverse images of a nearby regular value in one component would contradict its degree one. Their union is a compact connected set containing two roots. Fix a level t(μ,1) at which no critical value has modulus t, so that the level is regular. Let Ct be the component of {|f|<t} containing that set, let k2 be its root count, and put x=log(t/μ) and a=Area(Ct)/π; Pólya’s inequality [2] gives at2/n<1. The component is a Jordan domain. List its roots as ζ1,,ζk, choose a Riemann map φ:DCt, and write bj=φ1(ζj). The component-wise form of [8] is

f(φ(z))t=eiθj=1kzbj1bjz.

Indeed, regularity extends φ across the Jordan boundary. The quotient of the two sides without the phase has no zero or pole on the closed disc and has boundary modulus one. The maximum principle, applied to that quotient and its reciprocal, makes it a unimodular constant. The product has degree k, the root count of this component, not necessarily the full degree n. Distances between the bj below are hyperbolic distances in D, normalised by d(0,s)=2artanhs for 0s<1. Intrinsic distances in Ct are infima of Euclidean lengths of curves in that component.

The length estimate converts area into a bound for the image of a compact real interval I(1,1). Here is the coefficient calculation underlying the Bergman-kernel argument. Write φ(z)=0αz. Injectivity and the area formula give 0|α|2/(+1)=a. To express length as a linear integral, choose ω(x)=φ(x)/|φ(x)| on I; the denominator is nonzero because φ is conformal. Cauchy–Schwarz gives

length(φ(I))2=|0αIω(x)xdx|2a0(+1)|Iω(x)xdx|2.

Compactness of I permits termwise integration of the series. Since 0(+1)(xy)=(1xy)2>0 for real x,yI, taking absolute values in the resulting double integral yields

length(φ(I))2aIIdxdy(1xy)2.

This is precisely the positivity of the disc Bergman kernel K(z,w)=π1(1zw)2 on the real diameter. For I=[u,v](1,1), direct integration gives

uvuvdxdy(1xy)2=log(1uv)2(1u2)(1v2).

Thus I=[0,r] gives length(φ([0,r]))2alog(1/(1r2)). Moving two preimages to ±s and taking I=[s,s] instead gives

length(φ([s,s]))24aartanh(s2).

A pair of roots at hyperbolic distance d may be placed at ±tanh(d/4), so a connector shorter than 2 exists as soon as artanh(tanh2(d/4))<1/a. Failure therefore gives

(3)d(bi,bj)  D:=4artanhtanh(1/a),cosh(D/2)=e2/a.

There is also a point h in the chosen compact connected set whose intrinsic distance in Ct from every root is at least 1. Otherwise the open intrinsic balls of radius 1 about the roots would cover that set. Two balls with distinct centres cannot meet: paths from their centres to a common point would concatenate to length below 2. But a connected set containing two distinct roots cannot be covered by these disjoint open sets. This contradiction proves the assertion. Now choose the Riemann map with φ(0)=h, and continue to write bj=φ1(ζj). Put dj=d(0,bj) and λ(d)=logtanh(d/2). The one-root estimate at h gives tanh(dj/2)1e1/a. The centre h lies on the chosen inverse arcs, so 0<|f(h)|μ; it is not a root because its intrinsic distance from every root is at least 1. The Blaschke identity at 0 gives |f(h)|/t=j|bj|, hence jλ(dj)=log(t/|f(h)|)log(t/μ)=x. Together these estimates give

(4)λ(dj)δ(a)2,δ(a)=log(1e1/a),j=1kλ(dj)  x.
A lower bound for the number of roots.

Testing only consecutive pairs in angular order loses essential information. For k=2m, put m points at hyperbolic radius dlow and m at radius dlow+D, alternating in cyclic order. The reverse triangle inequality separates every consecutive pair by at least D, regardless of the angular gaps, whereas

jλ(dj)=m(λ(dlow)+λ(dlow+D))(m).

The even number of points is needed for cyclic alternation. These point configurations test only the consecutive-pair constraints; they need not satisfy separation for nonconsecutive pairs or arise from a polynomial component. To use the missing pairwise information, we impose the packing bound on every circle centred at the origin.

Lemma 3.3 (circle-slice packing). Under (3), for every r>0,

j=1kw(dj,r)π,w(d,r)=arccos(clampcoshdcoshrcosh(D/2)sinhdsinhr),

where clamp truncates its argument to [1,1].

Proof. The open balls Bj=Bhyp(bj,D/2) are pairwise disjoint, since a common point would force d(bi,bj)<D. Fix r>0. By the hyperbolic law of cosines the point of the hyperbolic circle of radius r at angle θ lies in Bj exactly when coshdjcoshrsinhdjsinhrcos(θθj)<cosh(D/2). The set of angles satisfying this inequality has measure 2w(dj,r): clamping gives measure zero for an empty intersection and 2π for a full circle, with tangent endpoint sets of measure zero. The intersections of the balls with this circle are disjoint, so their angular measures sum to at most 2π. ◻

Theorem 3.4 (a lower bound for the number of roots). Fix radii r1,,rp>0 and weights σ1,,σp0, put Σ=iσi and

U=supddlow(a)[λ(d)iσiw(d,ri)],λ(dlow(a))=δ(a)2.

If U>0, then failure forces k(xπΣ)/U.

Proof. By (4), Lemma 3.3 and the radius bound,

xjλ(dj)=j[λ(dj)iσiw(dj,ri)]+iσijw(dj,ri)kU+πΣ.

The weighted sum of circle-slice inequalities is a dual certificate: it bounds the contribution of every permitted root configuration without having to optimise over all configurations directly. The weights give a usable bound only when Σ and the supremum U have rigorous bounds. In particular, checking the expression on a finite grid does not bound the supremum between grid points. Zero weights recover only the individual bound k2x/δ(a); nonzero weights incorporate the circle-packing information and can improve the result. A certificate at area aa also applies at a. Indeed, dlow(a)dlow(a), so the admissible range of d only shrinks. Also D(a)D(a), which enlarges every slice angle w(d,ri) at fixed d,ri. Since the weights are nonnegative, the expression defining U can only decrease. Thus the same certified pair (Σ,U) remains valid. The numerical comparison also uses two bounds that do not involve chosen weights. They are useful where the circle-slice certificate is weaker. We derive them here so that every root-count input to the comparison is visible.

Two further root-count bounds.

Order the distances as d1dk. The triangle inequality gives djDd1 for j2. The function λ is decreasing and convex, since λ(d)=1/sinhd and λ(d)=coshd/sinh2d>0. On [dlow,D/2], the convex function λ(d)+(k1)λ(Dd) takes its maximum at an endpoint. If d1D/2, each summand is at most λ(D/2) instead. (The definitions give dlow<D/2.) Thus

xjλ(dj)max{δ(a)2+(k1)λ(Ddlow),kλ(D/2)},

and consequently

kmin{1+xδ(a)/2λ(Ddlow),xλ(D/2)}.

The minimum is essential: the two expressions arise from alternative positions of the nearest root, not from simultaneous restrictions.

For the second bound, integrate over the disjoint hyperbolic balls of radius D/2. Put E=e2/a1, so each ball has hyperbolic area 2πE. At most one contains the origin; its contribution to jλ(dj) is at most δ(a)/2. On every other ball, log|z| is harmonic. To average it, first move the ball’s centre to 0 by a disc automorphism. Hyperbolic area is invariant under this change of coordinates and has radial density 4/(1|z|2)2 there. The ordinary mean-value property on each centred Euclidean circle therefore gives hyperbolic area mean λ(dj). If the original ball has 0 on its boundary, use increasing smaller concentric balls and monotone convergence.

There are m=k1 nonexceptional balls if one contains the origin, and m=k otherwise. Their union has area 2πmE. Each superlevel set of log|z| is a centred ball, so its intersection with any set of this area has area at most the smaller of the two areas. The centred ball of area 2πmE attains that upper bound at every superlevel. Integrating these intersection areas over the superlevel parameter therefore bounds the integral over the union by the integral over that centred ball. Its radius R satisfies coshR=1+mE. With v=coshr1, the identity logtanh(r/2)=12log(1+2/v) reduces the radial integral to (2E)10mElog(1+2/v)dv. Evaluating it gives

12πEBhyp(0,R)log|z|dAhyp=mE2log(1+2/(mE))+log(1+mE/2)E1+log(1+mE/2)E,

where the improper integral is finite because vlogv0 as v0, and the last inequality uses log(1+u)u for u>0. Adding the possible exceptional contribution and inverting each case yields

kmin{1+2E(eE(xδ(a)/2)11),2E(eEx11)}.

Again the minimum accounts for the two possible cases. This estimate uses area rearrangement, whereas the preceding one uses only ordered distances; neither replaces the circle-slice inequalities.

The comparison takes the maximum of 2, 2x/δ(a), these two bounds, and the certified circle-slice bounds. Each may first be rounded up because k is an integer. Any of these estimates derived with an upper bound for a remains valid at the actual smaller area: the root configuration still satisfies the weaker separation and radius conditions at that upper bound.

From the root count to an area contradiction.

At a direction avoiding the finitely many critical-value arguments, lift the value radius from 0 to teiθ from each of the k roots in Ct and split each lift at level μ. Put A0=Area(Ct{|f|<μ}). This is the sum of the areas of the k one-root components inside Ct, not of all the root components of f; in particular, 0A0πa. On each of these components f/μ is conformal, since it is a proper map with no critical point onto a simply connected disc. Take ψ(z)=0γz to be its inverse, so f(ψ(z))=μz and ψ(0) is the selected root. The radial curves in this coordinate therefore trace exactly the required value-ray lifts. Cauchy–Schwarz in the radial variable and Parseval give

meanθ(01|ψ(reiθ)|dr)212|γ|2211|γ|2=Area(component)π.

First stop the radial integrals short of the unit circle, then pass to the endpoint by monotone convergence. Thus no smoothness of the boundary at level μ is assumed. Summing the k square-root area bounds gives a mean total low lift length at most kA0/π. At a regular intermediate level u, let AC(u) be the area of Ct{|f|<u} and PC(u) its total boundary length. The argument principle and the coarea formula give

(5)PC(u)22πkuAC(u),

because |dz|=ud(argf)/|f| on the level curve, its total argument variation is 2πk, and Cauchy–Schwarz applies. Integrating PC(u)/(2πu) from μ to t bounds the mean high lift length by kx(πaA0)/(2π). Cauchy–Schwarz combines the low and high bounds as

kA0π+kx(πaA0)2πka(1+x/2).

Choose a direction whose total lift length is at most ka(x+2)/2. Order its k boundary endpoints cyclically and join each adjacent pair using the two lifts and the intervening boundary arc. Each path lies in Ct{|f|<1} and, under failure, has length at least 2. Each lift occurs twice in the sum of these lengths, while the boundary occurs once. Therefore

2k2ka(x+2)+PC(t).

Now let t=μex vary, and write a(x)=Area(Cμex)/π for the component containing the chosen first pair; its root count k may increase at later mergers. On a regular interval, a(x)=tAC(t)/π. Applying (5) at the outer level and rearranging therefore gives

(6)a(x)  12π2[2k2a(x)(x+2)]+2

on each regular interval for the component containing the selected pair, using the largest of the root-count bounds just derived. At merger levels this component only gains area, which strengthens the integrated comparison. Pólya’s inequality caps a at 1 until the level reaches 1, so a trajectory forced past that cap before t=1 contradicts the assumption.

No positive initial area has to be assumed. While a1, for 0<x3/105 the bound k2 alone gives

a(x)12π2(222(2+3/105))2>130

at regular levels. For example, the last inequality follows using π<22/7, 2>140/99 and 2(2+3/105)<20001/10000. Integration, including the nonnegative merger jumps, gives a(3/105)>106. This is the universal starting bound used by the certificate.

The comparison is integrated cell by cell without assuming that the independently certified lower bounds increase with the table index. On a cell [x,xr], suppose a(x)aι and choose a trial upper bound m for the area. Let g be a certified lower bound for the right side of (6) throughout that cell under the trial assumption am. If m<aι+(xrx)g, then a(xr)>m. Indeed, the contrary assumption a(xr)m would imply am throughout the cell by monotonicity. Integrating the differential inequality, with the nonnegative merger jumps, would then give a(xr)>m, a contradiction.

Certificate.

The comparison gives an upper bound X on the logarithmic time needed for the forced area to exceed 1. It therefore gives a contradiction whenever μeX<1. The stated constant 13/25 is a convenient rational choice with room to spare, not an optimality claim. The companion program check_erdos1041_angular_budget_closure.py evaluates every accepted inequality in exact rational arithmetic, with directed rounding on the transcendental evaluations. Its fixed rational brackets for π and log2 have different elementary checks: Machin’s identity π=16arctan(1/5)4arctan(1/239) for the former, and log2=2j03(2j+1)/(2j+1) for the latter. Alternating-series bounds and a geometric tail bound, respectively, suffice to verify them. The full replay uses 18 area-table levels, 14 radii in each weighted bound, 126 attempted choices of weights, maximum step 1/400, and the initial lower area 106 at x=3/105. Only accepted rational certificates enter the comparison; its early steps may be shorter than 1/400. The recorded full replay certifies

X=6357628895991000000000000<0.6357629,1325eX<1,

which gives Theorem 3.1. The recorded quick-mode replay gives X=664373027131/1000000000000 and the weaker threshold 51/100. The floating optimiser proposes weights but supplies no proof. The argument uses only the subsequently certified rational bounds on their sum and on the supremum U. Each accepted pair supplies a weight sum Σ and a certified upper bound for the supremum U in Theorem 3.4. For orientation, the recorded quick-mode pairs at a=1, rounded to six decimal places, are (0.085674,0.045865), (0.126361,0.021829), (0.163157,0.010513) and (0.208928,0.004318), giving kU+πΣ approximately 0.4526, 0.5716, 0.6808 and 0.7945 at k=4,8,16,32, respectively. These rounded pairs do not themselves certify an inequality; the comparison uses the unrounded rational values and their directed bounds. To bound the supremum over d, the checker subdivides intervals and bounds each term in the direction needed for an upper bound. The function λ is decreasing. For fixed r, the slice angle w(d,r) has no strict interior minimum. Indeed, before clipping the angle to 0 or π, its cosine is

H(d)=coshdcoshrcosh(D/2)sinhdsinhr,H(d)=cosh(D/2)coshdcoshrsinh2dsinhr.

The numerator of H is increasing. Thus H has at most one interior minimum, and w=arccosH has at most one interior maximum; clipping preserves the endpoint-minimum property. On an interval [d,d+], therefore,

λ(d)iσiw(d,ri)λ(d)iσimin{w(d,ri),w(d+,ri)}.

Beyond d=maxiri+D/2, all the slice angles vanish, so only the decreasing function λ remains. These are interval bounds, not values sampled on a grid. The closing inequality is independently checkable: with X=635762889599/1012 and eXj14Xj/j!+(X15/15!)/(1X/16), rational arithmetic gives (13/25)eX<0.982000386<1. The same majorant also gives

5291000eX<0.998996547<1.

Thus the recorded full certificate in fact gives the path conclusion for μ529/1000, without changing the geometric argument or its hypotheses. This is an arithmetic consequence of the recorded stopping time, not a new certificate replay. We retain 13/25 in the theorem and its scaling corollaries as the simpler constant.

Sources and scope.

The analytic chain above is ordinary mathematics. Its general inputs are the Riemann mapping theorem, the Bergman kernel, the argument principle, the coarea formula, and Pólya’s area inequality Area{|f|t}πt2/n [1], [2]. The exact rational certificate is checked by a separate exact-arithmetic program, not by the Lean kernel. The two additional root-count bounds above are the ordered-distance estimate in the earlier distance comparison and the area-rearrangement estimate in the hyperbolic packing argument. Their derivations above are part of the analytic proof. No complete Lean proof or independent review of this theorem is claimed. The finite summation implication identified in the companion paper assumes the geometric inequalities; it does not formalise the analytic chain or the certificate replay. Prior art for the assembled statement is unassessed. No novelty is claimed for the slice inequality, which follows directly from disjointness of the balls and the hyperbolic law of cosines. The public source of record is AngularBudgetLowCriticalClosure.md, which carries the full analytic argument, the table of certified weighted bounds and the instructions for replaying the certificate. The stopping-time test requires μ<eX; the stated 13/25 theorem and the 529/1000 consequence are two rational cutoffs within that range. Other theorems apply to some polynomials outside it, so failure of this numerical test does not identify the class left untreated by all the results. Fixed-degree arguments remain stronger at n=4 and n=5, where the corresponding thresholds are 61/100 and 139/250; from n=6 on the all-degree constant 13/25 is the better statement. These threshold arguments do not settle the unrestricted root-connector conclusion.

Corollary 3.5 (scaled low-critical connection). Every squarefree monic polynomial f of degree n2 has two distinct zeros joined by a rectifiable curve of length less than (5/2)μ1/n in {|f|<(25/13)μ}, where μ=minf(c)=0|f(c)|.

Proof. For n3, apply Theorem 3.1 to g(z)=snf(sz) with s=((25/13)μ)1/n. Its least critical modulus is 13/25; rescaling gives length less than 2(25/13)1/nμ1/n<(5/2)μ1/n, since 25/13<(5/4)3. For n=2, write f(z)=(zh)2d2. The two radial segments through h have total length 2|d|=2μ1/2 and lie in the closed level μ, which is inside the stated open level. ◻

The next section gives a different construction whose estimates retain the root count and capacity of the chosen component.

A path estimate from area and boundary length

Corollary 3.5 has both a smaller length constant and a smaller containment level than the next theorem: 5/2<71/10 and 25/13<2. The independent area argument below is useful for a different reason: it keeps the root count and component capacity in the length estimate. Its μ1/2 corollaries illustrate that geometric dependence; their ranges are already covered by Theorem 3.1. For a monic degree-n polynomial put

Kt={z:|f(z)|t},μ=minf(c)=0|f(c)|,ρ=μ1/n.

Theorem 4.1 (a uniform path bound at level 2μ). For every monic polynomial f of degree n2, two zero occurrences are joined by a possibly degenerate path of length at most

7110ρ

inside K2μ. If f is squarefree, their locations are distinct. If μ1/2, the construction may be chosen inside {|f|<1} with length at most 5.7.

The constant is the rationally certified specialization of a two-parameter bound. If the selected component contains k2 roots, then for every r(0,1) and λ>1 the proof constructs a path in Kλμ whose length is at most

(CF)2k(2r(1r)2+λ1/n(log(λ/r)+πlogλ))ρ.

For n3, the choice λ=2, r=3/20 makes the bracket less than 71/10: the largest case is n=3, where exact rational bounds give 66517563/9392500<71/10. Degree two has the exact root-segment bound 2ρ.

Proof. A repeated zero gives the constant path, so assume f is squarefree and μ>0. Degree two is the segment of length 2ρ in Kμ; assume n3. Put T=λμ, let CT be the component of KT containing a critical point at level μ, and write A(σ)=Area(KσCT). We will first choose a regular level t, then a direction in the value plane, and finally an adjacent pair of roots. This order ensures that the three estimates below apply to the same path.

At a regular level σ, a component C containing k roots has |dz|=σdφ/|f| on its boundary and total argument variation 2πk. Cauchy–Schwarz, followed by the coarea formula, gives

(CF1)H1(C)22πkσA(σ).

Here A sums the area derivatives of all the components in CT, so it bounds the contribution from C. Pólya’s inequality A(T)πT2/n [2] and averaging with respect to dσ/σ on (μ,T) give a regular level t such that tA(t)πT2/n/logλ. The component Ct containing the chosen first merger has k2 roots and

H1(Ct)π2k/logλT1/n.

Averaging over levels avoids estimating the area derivative at the critical level itself.

Choose a direction avoiding all critical-value arguments. Lift its radial segment from each of the k roots to Ct, splitting each lift at value modulus rμ. Below μ, the inverse branches of f/μ are univalent. Their derivatives at 0 are μ/f(zi), where zi ranges over the roots. The area formula for their disjoint images gives

(CF2)iμ2|f(zi)|2ρ2.

Indeed, the squared derivative at the centre is at most the image area divided by π, and the total image area is at most πμ2/n. Koebe distortion and Cauchy–Schwarz therefore bound the sum of the lengths below rμ, uniformly in the direction. Write ihigh(θ) for the length of the ith piece above rμ in direction θ. At an intermediate regular level, apply (CF1) to all the lower components contained in Ct; their root counts sum to k. Integrating their total perimeter with measure dσ/(2πσ) gives the mean of iihigh. Cauchy–Schwarz in σ, using an area increment at most Area(Ct)πT2/n, gives

12π02πiihigh(θ)dθkArea(Ct)2πlogtrμk2T1/nlog(λ/r).

Choose a direction avoiding the critical-value arguments at which the sum is at most this bound. The excluded directions form a finite set and hence have measure zero.

Order its k endpoints cyclically on Ct. Each adjacent pair of endpoints gives a path consisting of two lifted segments and the intervening boundary arc. In the sum over these k paths, every lifted segment occurs twice and the boundary arcs partition Ct. Thus some pair has length at most the sum of the following three bounds:

2kiilow2rρk(1r)2,2kiihigh2klog(λ/r)T1/n,H1(Ct)k2kπT1/nlogλ.

The first holds in every direction, the second in the direction just chosen, and the third at the previously selected level. Substituting T1/n=λ1/nρ proves (CF). For the final assertion, the repeated-zero case is already a constant path, and in degree two the root segment has length 2ρ=2μ2. For n3, take λ=2 and r=3/20. Since k2 and μ1/2, (CF) gives

length602289μ1/n+(2μ)1/n(log(40/3)+πlog2)602289+log(40/3)+πlog2=5.676476<5.7.

Here 2μ1, and the mean-value choice may be taken at a regular level strictly below the top of its positive-measure window. Thus the entire path lies in {|f|<1}. ◻

The bracket (CF) retains two quantities that the constant 71/10 discards, namely the root count k of the selected component through the factor 2/k, and the capacity of that component through the area input. Keeping either one turns the constant-factor theorem into the target conclusion on an explicit region.

The number of roots in the first merged component can be much smaller than the degree. At a first merger caused by one simple critical point it is 2, so the following thresholds do not apply. For znb, however, all n roots merge at the same level, giving k0=n. For example, n17 and 0<|b|1/2 satisfy the first pair of hypotheses. These conditions illustrate what the area argument gains from simultaneous mergers; the preceding 13/25 theorem already covers these three ranges without requiring a large root count.

Corollary 4.2 (a criterion using the number of roots at the first merger). Let f be monic with every root in the open unit disc, let c be a critical point with |f(c)|=μ, and let k0 be the number of roots, counted with multiplicity, in the component of Kμ containing c. Then Erdős #1041 holds for f in each of the three cases

μ12 and k017,μ14 and k012,μ18 and k010.

Proof. If μ=0, a repeated zero gives the constant path. Assume henceforth μ>0. Every selected component Ct in the proof of Theorem 4.1 contains the first-merge component, so kk0. For the first case take λ=2, r=13/100; then (2μ)1/n1 and ρ1, and the exact bounds 2<283/200, log(200/13)<5/3 and π/log2<(22/7)/(104/125)=1375/364 make the bracket in (CF) at most 15668813/2755116, whose square is 3412570881068535/7590664173456<34. Hence k017 gives squared length below (2/17)34=4. For the second case take λ=4, r=3/25: the bracket is below 6075221/1273888, whose square is 242038665078215/1622790636544<24, and 2/k01/6 gives squared length below 4. For the third take λ=8, r=11/100: the bracket is below 55629121/12475575, whose square is 2018200328379859/155639971580625<20, and 2/k01/5 again gives squared length below 4. In each case λμ1, so the freedom in the choice of the regular level t keeps t<1 and the containment strict. ◻

The next criterion uses logarithmic capacity, a measure of the size of a compact set that scales linearly under dilation. It compares the size of one component with that of the entire polynomial sublevel set. If that sublevel set is connected, the ratio κ below is 1; a cutoff such as κ1/3 therefore requires a genuinely smaller component. This is additional geometric information, not a consequence of a small number of roots in the component. The ratio requires μ>0. When μ=0, f has a repeated zero and the constant path already gives the conclusion; there is no capacity ratio to evaluate.

Corollary 4.3 (a criterion using component capacity). Keep the hypotheses of Corollary 4.2 with 0<μ1/2, let C be the component of {|f|<2μ} containing c, and put κ=cap(C)/(2μ)1/n. If κτk0, where

τk=2kAB,A=2833610,B=520299100,

then Erdős #1041 holds for f. In particular κ1/3 suffices for every root count k02, and the rational cutoffs 2/5,12/25,1/2,7/12,16/25,2/3,7/10 suffice at k0=3,,9, rising to 39/40 at k0=16.

Proof. Repeat the averaging proof of Theorem 4.1 with A(σ)=Area(KσC) for σ<2μ. This keeps the chosen paths in the open component C, even if distinct components have touching boundaries at level 2μ. Replace the global area input by the component form Area(C)πcap(C)2=πκ2(2μ)2/n of the area–capacity inequality . Only the high-lift and boundary terms acquire the factor κ; the low-lift term (CF2) is unchanged. Taking λ=2, r=1/20, and the exact bounds above together with log40<12641/3402<(97/50)2, gives length<2/k0(A+Bκ). The definition of τk0 makes the right side at most 2, and for each displayed rational qk integer arithmetic gives (A+Bqk)2<2k. Discarding 2/k01 altogether gives the uniform cutoff κ1/3. ◻

By the component-capacity formula, κ=eΣ/n with Σ the sum of exterior Green function values at the roots excluded from C. Indeed, let Ω be the unbounded component of C^\C, let G be its Green function with pole at infinity, extended by zero off Ω, and let g(,a) be its Green function with pole at aΩ. The function 1nlog|f|2μG+1nag(,a), summed over the roots aΩ with multiplicity, extends harmonically to Ω, is bounded, and vanishes on ΩC, so it vanishes identically; its value at infinity is logκ+1naG(a) by the symmetry g(,a)=G(a). Failure of these component-sensitive criteria alone, in the range μ1/2, forces k016 and exterior Green sum Σ<nlog(40/39) when k0=16. This is a limitation of the area-based criteria. The low-critical theorem already excludes an actual counterexample throughout that range.

The proof of Theorem 4.1 averages over levels in [μ,λμ]. To keep the path at the first critical level instead, one would need a perimeter estimate of the following kind. The regular-level argument (CF1) gives no finite pointwise bound at the critical level: even at a simple critical point, the area derivative diverges logarithmically.

The addendum [26] reports a Runge-approximation construction of monic level-one components with one simple zero and arbitrarily long analytic boundaries. It imposes neither a unit root disc nor a global lower bound on critical-value moduli. That proof was not supplied or available for checking in this revision; the report is not an input to the path estimates here. The question below requires a stronger hypothesis than the existence of one unramified component: the level must lie below every critical-value modulus of the polynomial. A construction without that global condition cannot by itself answer the question.

Problem 4.4 (perimeter below the smallest critical-value modulus). Let f be squarefree and monic of degree n2, and put μ=minf(c)=0|f(c)|. Is there a constant β, independent of n,f and 0<σ<μ, such that every component C of {|f|σ} satisfies

H1(C)βσ1/n?

Equivalently, for each univalent inverse branch defined on D by f(ϕj(w))=σw, is

02π|ϕj(eit)|dtβσ1/n(1jn)?

There is no root-location hypothesis. If such constants exist, write β for their infimum.

All these components contain one zero. The condition σ<μ controls all inverse branches at once; it is stronger than requiring only the selected component to contain one zero. The examples below compare particular constants, not the necessity of this global hypothesis for every possible perimeter bound. For 1<R<μ/σ, the area estimate gives

12π02π|ϕj(eit)|dt(σR)1/nR21.

Indeed, circular means of |ϕj|2 increase, the image of the annulus 1<|w|<R has area at least π(R21) times the mean at 1, and Pólya’s preimage-area bound bounds that area by π(σR)2/n. The loss as R1 belongs to this argument and does not prove an endpoint divergence.

For d>0 and f(z)=z2d2, one has μ=d2 and ρ=d. For σ<d2 the component of {|f|σ} around d contains one root. Its parametrisations d1+(σ/d2)eiθ converge uniformly, as σd2, to one loop of Bernoulli’s lemniscate |z2d2|=d2, of length dΓ(1/4)2/(2π) by the substitution φ(w)=d1+w and Γ(1/4)Γ(3/4)=π2. At σ=d2 the two loops meet at the critical point, and the closed sublevel set is a single component containing both roots. Lower semicontinuity of length under the stated uniform convergence gives βΓ(1/4)2/(2π)=3.70814935; convergence of the lengths themselves is not required. For znrn, polar parametrisation of one limiting loop gives its length divided by r as

21/nnπ/2π/2(cosθ)1/n1dθ=21/nnπΓ(1/(2n))Γ(1/(2n)+1/2).

The evaluation is Euler’s beta integral (5.12.1), in its trigonometric form (5.12.2). To verify the claimed decrease with n, put p=1/n. The expression is 2p+1πΓ(1+p/2)/Γ((1+p)/2); its logarithmic derivative is

log2+12(Γ(1+p/2)Γ(1+p/2)Γ((1+p)/2)Γ((1+p)/2))>0.

Here Γ/Γ is increasing on the positive real axis, by the positive trigamma series (5.15.1). The expression therefore decreases with n and tends to 2.

The comparison with the next example also has an elementary bound, independent of rounded gamma values. One loop of z2d2 has parametrisation

z(s)=2dcoss(1+isins)1+sin2s,π/2sπ/2,

whose speed is 2d/1+sin2s. Convexity puts (1+x)1/2 below its secant on [0,1]. Integrating that secant at x=sin2s bounds the loop length divided by d by (π/2)(1+2), as used below.

The quadratic loop is exceeded in degree eight, even with the global subcritical hypothesis. For p(z)=z8(3/2)z, every critical point c satisfies c7=3/16 and p(c)=(21/16)c. Hence

μ=2116(316)1/7>1,μ7=3217168>1.

Thus σ=1 is below every critical-value modulus, not merely a regular level for the selected component. The component C of {|p|1} containing the origin lies in {|z|<4/5}, because |p(z)|6/5(4/5)8>1 on |z|=4/5, and it contains a neighbourhood of the closed disc of radius 5/8, because |p(z)|(5/8)8+15/16<1 on that disc. The other roots satisfy |z|7=3/2, so C contains exactly one root, and H1(C)>5π/4>(π/2)(1+2)Γ(1/4)2/(2π). Moreover, for fixed a>1 and all sufficiently large N, the one-root component of {|zNaz|1} contains every disc of radius r<1/a, and a circle of radius between 1/a and 1 isolates it by Rouché’s theorem; letting a1 shows that every admissible β is at least 2π. For the latter family all critical values have modulus (11/N)a(a/N)1/(N1)a>1, so it also gives the necessary bound β2π under the corrected global subcritical hypothesis. Kuznetsova–Tkachev [24] establish Laplace-transform and log-convexity properties for regular level-length functions. Those results do not provide a uniform bound at the first critical level. Total lemniscate length and one-branch endpoint length are different extremal quantities.

The preceding examples do not establish a universal perimeter bound. The implication below applies to an individual polynomial; a constant β independent of the polynomial and degree would give a uniform path bound. The construction uses two components meeting at a first critical point and joins each root to that point at a cost of at most half its component’s perimeter. It does not give the constant 2 of the historical question.

Theorem 4.5 (a path from a subcritical perimeter bound). Let f be squarefree and monic of degree n2, and put μ=minf(c)=0|f(c)|>0. Suppose β>0 satisfies

H1(C)βσ1/n

for every 0<σ<μ and every component C of {|f|σ}. Then two distinct roots of f are joined inside Kμ={|f|μ} by a rectifiable path of length at most βμ1/n.

Proof.

Put ρ=μ1/n. On each component of {|f|<μ}, f is a proper unramified covering of the disc {|w|<μ}, hence univalent. Equivalently, exhaust by regular levels below μ and apply the component count . At a critical point c with |f(c)|=μ, the local degree d2 gives d nearby preimages of an inward radial value. Univalence places them in different one-root components. Choose two such components Ua,Ub, containing roots a,b and with c in both closures; simplicity of c is unnecessary. For the boundary passage, take f(ϕ(w))=μw on D. Fix |w0|=1. The finitely many preimages of μw0 have disjoint neighbourhoods. Properness of f and connectedness of a sufficiently small disc cap force ϕ to stay in one of them as ww0. At its preimage c, write

f(z)f(c)=(zc)dh(z),h(c)0.

A local analytic dth root of h makes (zc)h(z)1/d a conformal coordinate. In each inverse sector, ϕ is therefore an analytic function of (ww0)1/d and extends continuously to c. The finitely many critical boundary values are the only exceptional points; at every other boundary value the ordinary inverse function theorem applies. Moreover, near eiθ0=w0 the boundary speed is O(|θθ0|1/d1), which is integrable even when d>2. Thus the extension is continuous on the closed disc and its boundary curve is rectifiable. The identity f(ϕ(eiθ))=μeiθ makes the boundary values injective, so the curve is Jordan.

As r1, the curves ϕ(reiθ) converge uniformly to that boundary and have length at most β(μr)1/n by the hypothesis. Lower semicontinuity of length gives boundary length at most βρ for each component.

A bounded rectifiable Jordan domain U has the following elementary property: any aU can be joined to any cU in U with length at most H1(U)/2. Choose a line through a but not c, and let [u,v] be the closure of the connected interval in its intersection with U containing a. Of the two boundary arcs from u to v, write A for the one containing c and A for the other. The paths from a through u or v and then along A to c have total length

|au|+|av|+length(A)=|uv|+length(A)H1(U),

because |uv|length(A). One path is at most half this sum. The connected interval ensures containment of the straight parts even when U is not convex.

Apply this property in Ua,Ub with common boundary point c. Concatenating the two paths gives length at most 12(H1(Ua)+H1(Ub))βρ, as required. Only these two component perimeters are used; the subcritical hypothesis bounds them by the limiting argument above. Boundary arcs are allowed, so containment is in Kμ, not the open sublevel. ◻

Sources and scope.

Theorem 4.1 is ordinary mathematics with no Lean-checked part. Its inputs are the capacity identity for polynomial preimages [2], Pólya’s area inequality , Cauchy–Schwarz, the Koebe distortion theorem for univalent maps, and averaging over adjacent boundary endpoints. The public source of record is the full area and boundary-length argument, which carries every rational verification quoted above. Its Section 10 gives a weaker conditional bound involving an auxiliary parameter and a logarithm; Theorem 4.5 states the stronger βρ consequence proved here. That section’s proposed numerical perimeter constant is refuted by the degree-eight example above and is not assumed in the theorem. The unconditional construction retains level 2μ and constant 71/10. The scaled low-critical corollary has both a smaller constant and a smaller level. The proof retained here is ordinary, with component-sensitive consequences on their stated regions; its rational cutoffs are exact integer inequalities. The earlier perimeter samples concerned only a selected component. They do not test the stronger condition that the level lie below every critical value. The sharp root-connector conclusion is not established for the unrestricted class by the arguments in this record. The adjacent classical literature on lemniscate length concerns the arclength of the level curve {|p|=1}, which is Erdős #114. Fryntov and Nazarov recall its history : Dolzhenko’s bound 4πn, Pommerenke’s bound 74n2 of 1961, and Borwein’s bound 8πen [13]. Eremenko and Hayman proved 9.173n [14], Fryntov and Nazarov the asymptotically sharp 2n+o(n) , and Tao resolved the problem for large n [16]. These results bound the length of a level curve, not the least internal root-pair path. This distinction identifies the quantity being estimated; no claim of novelty follows from the scope or outcome of a literature search.

Degree three

Theorem 5.1 (the cubic case). Let f(z)=j=13(zzj) with |zj|<1, the roots listed with multiplicity. Then two listed root occurrences are joined inside {|f|<1} by a polygonal path of length strictly below 2. If f is squarefree the two are distinct.

Proof. Multiple roots give a constant path, so assume f squarefree. The Erdős–Herzog–Piranian component lemma [4] gives a component of {|f|<1} containing two roots. Join them by a compact path in that open component, and choose a regular value modulus t<1 larger than max|f| on the path. The component of {|f|<t} containing it has k2 roots and hence k11 critical points, by the component-wise Riemann–Hurwitz count in the proof of . One of these critical points has value of modulus below t<1. This choice of t avoids assuming that the level |f|=1 is regular.

Suppose first that f has two distinct zeros. Choose a critical point c minimising |f(c)|, write the other one as c+δ, and put v=f(c), so 0<|v|<1. Monicity gives the exact expansion f(c+d)=d332δd2+v. Choose α with α3=v and set b=δ/α; dividing by v gives f(c+αw)/v=Pb(w) with

Pb(w)=w332bw2+1.

At the other critical point f(c+δ)=v(1b3/2), so minimality of |v| is exactly the hypothesis |1b3/2|1.

Under that hypothesis Pb has at least two zeros, with multiplicity, in the closed unit disc. In the strict region a unit-circle zero w would give b=23(w+w2). Write w3=e2iu; substitution gives

|1b3/2|2=1+64729cos4u(16cos2u27)1.

Since 16cos2u27<0, equality requires cosu=0, which gives b=0. Thus the strict region has no unit-circle zero. The radial deformation bsb, s1, stays in the strict region, since z=b3/2 and |1z|2>1 give |1s3z|21=s3(s3|z|22z)>0. For large s, Rouché’s theorem on |w|=1 compares Psb with 32sbw2, whose modulus 32s|b| exceeds 2|w3+1|, so Psb has exactly two zeros in the open unit disc; no zero crosses the circle along the deformation. For the equality case with b0, the same radial deformation lies in the strict region for every s>1, and continuity of the root multiset allows s1. If b=0, then Pb(w)=w3+1 and all three roots lie on the unit circle.

If Pb(w)=0 and 0t1, then Pb(tw)=1t2t2(1t)w3, so |w|1 gives |Pb(tw)|(1t2)+t2(1t)|w|31t31. The whole segment from 0 to w therefore lies in the closed unit sublevel set. Selecting two normalized roots w1,w2 with |wi|1, the two segments from c to c+αwi lie in {|f||v|}{|f|<1} and have combined length at most 2|α|=2|v|1/3<2.

If instead f has a double zero c, then f(c+d)=d3+v. With α3=v and ω=e2πi/3, its roots are c+α, c+αω, c+αω2. Averaging their squared moduli gives |c|2+|α|2<1, so |α|<1; any two radial spokes have total length 2|α|<2, and along either spoke the value has modulus |v|(1t3)<1 away from the root endpoint. ◻

The unit level need not be regular, even when all roots lie in the open unit disc. For example, Q(z)=(z1)(z+1)(z+9/10) has Q(1/3)=148/135<1. Its minimum v on [9/10,1] occurs at an interior critical point and satisfies v<1. Set r=|v|1/3<1. The monic cubic r3Q(z/r) has the three distinct roots r,9r/10,r in the open unit disc and a critical value equal to 1. Its unit level is therefore singular, although the cubic path theorem applies.

A formal-source implementation includes the polygonal path, strict variation bound and repeated-root case; its recorded build status is stated below.

Sources and scope.

The source snapshot contains the complete degree-three path implementation and its supporting cubic source. This earlier implementation lies outside the main repository’s recorded checked build. The supplied release snapshot also contains the cubic theorem under monicity, degree three and the open-disc hypothesis and its expanded solution statement. The release proof obtains a root enumeration from monicity and degree; it does not assume an additional analytic path supplier. It constructs a continuous polygonal curve with bounded variation, values strictly below one and length strictly below two. Its endpoints are distinct when the polynomial is squarefree; repeated root occurrences are handled by the enumerated version. The supplied index classifies these release declarations as release_only, not ci_checked. The solution source contains a proof rather than the placeholder in the corresponding challenge file. This identifies the full formal target without claiming a fresh compilation or axiom audit. The proof above remains an ordinary mathematical argument. Pendyala [11] proves the separate quartic case; no historical priority for the cubic theorem is asserted here.

An all-degree critical-value separation theorem

The next theorem applies when one simple critical value is separated from all the others by a disc in the value plane. After a change of variables, the chosen critical point is 0 and its value is 1. The hypothesis below then says that the disc of centre w0 and radius S contains no other critical value. It is a condition to check, not an isolation property guaranteed for every polynomial.

The simplicity assumption means that the chosen critical point is a simple zero of the derivative, so two inverse branches meet there. A multiple chosen critical point is excluded; the other critical points need not be simple. Also, separation of roots in the z-plane is not enough: different critical points can have nearly equal values. An exact quartic example below makes this distinction explicit. For a positive example, take f(z)=z33a2z with 0<a<1/3. Its roots 0,±3a lie in the unit disc. At c=a the critical value is v=2a3, and the other normalised critical value is 1. Thus the disc centred at 1 with radius 4/3 contains 0 and 1 but excludes the other critical value. Radius 2 is allowed as well: the other critical value then lies on the boundary. The proof must therefore allow a nonregular outer level.

Theorem 6.1 (separation of one simple critical value). Let P be a polynomial of degree n3 whose leading coefficient has modulus one, with

P(0)=1,P(0)=0,P(0)0.

Fix w0[0,1] and S>max(w0,1w0). Suppose every other critical point d0 satisfies

(4)|P(d)w0|S.

Put p=w0(1w0). The two local solutions of P(Z(ξ))=1ξ2, Z(0)=0, continue along the real segment to one injective root-to-root connector Γ. Its endpoints are distinct roots, Γ{|P|1}, and

(5)length(Γ)22(Sn1)2/nlogS2+S+pS2S+p.

Consequently the connector is shorter than 2 whenever

(6)(Sn1)2/nlogS2+S+pS2S+p<2.

Proof. Let Q=D(w0,S) and let U be the component of P1(Q) containing 0. Both 0 and 1 lie in Q, and (4) says that 0 is the only critical point in U. A component of a polynomial sublevel set is simply connected: on any Jordan curve in the component, the maximum principle bounds the same polynomial throughout its interior, which must therefore remain in the component. Condition (4) permits critical values on Q, so we must not assume that U is regular. For 1w0<S<S, let U be the component of {|Pw0|<S} containing 0. This level is regular, and 0 contributes its only unit of ramification. The component count in the proof of [8] therefore gives deg(P|U)=2.

These nested components exhaust U. Indeed, a point of U can be joined to 0 by a compact path in U; the maximum of |Pw0| on that path is strictly below S, so the path eventually lies in U. For any fixed regular value in Q, all its finitely many preimages in U therefore lie in one such U once S is sufficiently large. The proper map P:UQ consequently also has degree two. This establishes the count without a smoothness assumption at the outer level.

Set a=1w0. On U, the function 1P has only its double zero at 0, so it has a single-valued square root

ξ(z)2=1P(z).

Taking this square root removes the double branching at 0. The map ξ is proper into

Q~={ξ:|ξ2a|<S}.

Away from 0, the identity 2ξξ=P gives ξ0; at 0, (ξ(0))2=P(0)/20. The target is star-shaped about 0: because S>a, the convex disc D(a,S) contains 0, so t2ξ2D(a,S) whenever ξQ~ and 0t1. It is therefore connected and simply connected. A proper local biholomorphism has open and closed image, hence is a covering of this target. Since U is connected, it is a conformal bijection. Its inverse Z continues both local inverse branches through the critical point. Since [1,1]Q~, the curve Z([1,1]) joins the two distinct points over P=0, and P(Z(ξ))=1ξ2[0,1] gives its containment.

We next map the parameter domain to the unit disc so that the curve becomes a straight interval. This allows its length to be estimated by the area of U, without replacing the domain by a larger disc. Squaring sends Q~ onto D(a,S). To map this disc to D while fixing 0, compose w(wa)/S with the disc automorphism taking a/S to 0. The result is the Möbius map

wSwS2+awa2.

Taking its square root after substituting w=ξ2 gives the conformal bijection

ζ(ξ)=ξSS2+aξ2a2:Q~D,

where the square-root factor is chosen positive at 0. It sends [1,1] to [q,q], with

q2=SS2+p,S2S+p=(Sw0)(S(1w0))>0.

The last inequality is exactly where S>max(w0,1w0) ensures 0<q<1, as required by the length estimate below. For Φ=Zζ1:DU, the Bergman segment inequality, proved by the kernel estimate of Section 3 with the double integral taken over [q,q]2, gives

length(Γ)22πlog1+q21q2Area(U)(7)=2πlogS2+S+pS2S+pArea(U).

It remains to bound the area of this component. The factor n1 comes from the roots outside it, rather than from Pólya’s inequality alone. The auxiliary capacity estimate is as follows: for a monic degree-n polynomial F, a regular value t>0 of |F|, and a component V of {|F|<t} containing k<n zeros counted with multiplicity,

cap(V)nt<k2nk.

Multiplying F by a unimodular constant leaves the estimate unchanged. This is a separate component estimate, not part of the Riemann–Hurwitz statement cited above. We give the harmonic-measure argument behind it, following Theorem 2 and Corollary 3 of the component-capacity proof.

Let m=nk and let ψ map |ζ|>1 conformally onto the exterior of V, with positive leading coefficient cap(V). The m excluded roots have preimages ξj with |ξj|>1. Put bj=1/ξj and form

B(z)=j=1mzbj1bjz.

Reflection in the unit circle shows that F(ψ(ζ))/t equals ζnB(1/ζ) up to a constant of modulus one: their zeros and pole at infinity agree, and both have modulus one on the boundary. Comparing leading coefficients gives

|B(0)|=cap(V)nt.

Regularity of the level permits analytic continuation of ψ across the boundary. On the unit circle,

ddθargF(ψ(eiθ))=n|B(eiθ)|>0.

Positivity follows because a regular polynomial level is mapped locally in the positive boundary direction. Thus |B|<n there.

The boundary-fibre identity used next is Lemma 1 of the same component-capacity proof. Here is its harmonic-measure argument. For a continuous real function h on the unit circle, let H be its harmonic extension to the disc. Since HB is harmonic, the mean value property and the Poisson formula give

12π02πh(B(eiθ))dθ=H(B(0))=12π02πh(eiϕ)1|B(0)|2|eiϕB(0)|2dϕ.

Differentiating the factors gives the positive angular derivative

ddθargB(eiθ)=|B(eiθ)|=j=1m1|bj|2|eiθbj|2>0.

Changing variables through the m boundary inverse branches in the first integral and comparing the continuous densities therefore yields

B(ζ)=w1|B(ζ)|=1|B(0)|2|wB(0)|2(|w|=1).

In particular each boundary fibre consists of m distinct points. Choosing w=B(0)/|B(0)| yields

mn<1|B(0)|1+|B(0)|,|B(0)|<nmn+m=k2nk.

Here B(0)0 because every excluded-root preimage is finite. This proves the component estimate and explains how the excluded roots enter it.

For the regular inner components U above, the degree-two count gives exactly two zeros of Pw0, counted with multiplicity. Since 2<n, the preceding estimate applies with k=2 and gives

cap(U)nS<k2nk=1n1.

Pólya’s area–capacity inequality Area(K)πcap(K)2 [2] then yields Area(U)<π(S/(n1))2/n. The exhaustion proved at the start and continuity of area from below give, without assuming regularity of the limiting boundary,

Area(U)π(Sn1)2/n.

Substitution into (7) proves (5), and (6) makes its right side strictly less than 4. ◻

Corollary 6.2 (uniform radius 4/3). Inequality eq:disk-family-coefficient holds for every n3, every w0[0,1], and every 4/3S2. Thus, if f is monic with roots in the open unit disc, c is a simple critical point with v=f(c)0 and |v|<1, and

|f(d)vw0|43

for every other critical point d, then two roots of f are joined inside {|f|<1} by a curve of length strictly below 2.

Proof. For S4/3 and p0,

S2+S+pS2S+pS+1S17.

Also S/(n1)1 when S2 and n3, while log7<2. This proves eq:disk-family-coefficient. For the unnormalised polynomial, set z=c+|v|1/nw. Then P(w)=f(z)/v has leading coefficient |v|/v, of modulus one. Scaling the connector multiplies its length by |v|1/n<1 and takes {|P|1} to {|f||v|}{|f|<1}. The selected value v need not attain the minimum defining μ. ◻

Taking w0=1 and S=2 gives the earlier criterion |1f(d)/v|2 in every degree n3. If c attains the minimum modulus among all critical values and v0, the Fekete–resultant bound gives |v|Rn<1 when all roots lie in a disc of radius R<1. Deleting zero critical values before taking the minimum would invalidate that inference. For example, (zR)2(z+R) with 0<R<1 has critical values 0 and 32R3/27, so its least nonzero critical-value modulus exceeds R3. The repeated root already gives a constant path, but it does not give this nonzero value the required bound. For a critical point chosen in another way, |v|<1 must remain an explicit hypothesis. In degree three the choice w0=1 already works at S=6/5, since

(35)2/3log11<2.

This sharper cubic constant is part of the numerical Lean kernel cited below.

The separation hypothesis of Theorem 6.1 is a condition on values, not on the positions of roots or critical points. To distinguish these conditions, consider the family

gε(z)=z4εz32z2+3εz+12,0<ε132.

Its derivative and two critical values are

gε(z)=(z21)(4z3ε),gε(±1)=12±2ε.

At the endpoints of each of the intervals (3/2,5/4), (3/4,1/2), (1/2,3/4) and (5/4,3/2), the values of gε have opposite signs throughout this parameter range. Each interval therefore contains exactly one root. Together with the critical points 1,3ε/4,1, these give seven points at pairwise distances greater than 1/4, uniformly in ε. Nevertheless the two displayed critical values differ by 4ε0. The earlier numerical choice is the exact member ε=1/262144:

g(z)=z4z32621442z2+3z262144+12,g(z)=4(z+1)(z3/1048576)(z1),

for which that difference is 1/65536. The monic polynomial 24gε(2z) puts every root inside |z|<3/4 and retains a spatial separation greater than 1/8. For the critical points ±1/2 of the scaled polynomial, the ratio of the two values is unchanged and obeys

gε(1)gε(1)=1+4ε14ε97<43.

The reciprocal ratio lies between 0 and 1. Hence, for any centre w0[0,1], neither selected value satisfies the theorem’s radius-4/3 isolation condition: the other normalised value is less than 4/3 away. This does not exclude a suitable isolated value at a different critical point.

Sources and scope.

The two-sheeted component, its square-root uniformisation, the Bergman segment inequality, the component-capacity estimate, Pólya’s area–capacity inequality and the exhaustion are ordinary arguments. They are collected in the proof using an isolated critical value, whose capacity step is cited separately above. The separate Lean numerical kernel checks the coefficient bound for n3, 4/3S2 and p0, and the implication from the squared length bound to length below 2. It does not formalise the analytic hypotheses producing (5). The adjacent axiom-audit source names those numerical declarations; it is not an axiom audit of the ordinary analytic theorem.

The proof requires both a simple critical point and a disc centred on [0,1] that isolates its normalised value. For example, the trinomial znb with n>2 and 0<|b|<1 has a short path by Theorem 2.1, but its only critical point is not simple, so this method does not apply. The restriction is on the chosen critical point and on the distance of the other critical values from the chosen disc. The other critical points may be multiple, and their values need not be separated from one another. No sharpness is claimed for S=4/3, and no assertion is made that every polynomial has a suitable isolated simple value. In particular, this is not a proof of the unrestricted assertion of Erdős #1041.

A related area comparison is Dubinin’s Theorem 1. The source is , Theorem 1 on printed page 85 of the POMI original. It concerns a holomorphic function that gives a full n-fold covering of an annulus t1<|w|<t2, and, in the notation of that theorem, with E its explicitly defined complementary set, it states

(t2t1)2/nm(ED)m(E).

The full covering and the explicit complementary set are hypotheses of the theorem. Tao cited it on the Erdős Problem #1041 discussion page on 25 March 2026 for the relative scaling factor s2/n between the areas of two nested sublevel sets, which is the reading of the displayed inequality in which E and ED are those two sublevel sets and the covering hypothesis holds. No step of this note uses that relative inequality. The disk-family theorem instead uses Pólya’s absolute area–capacity inequality on a component containing fewer than n roots, after the component-capacity estimate supplies its strict capacity gap. The absolute sublevel inequality Area{|P|<T}πT2/n remains the area input to Theorem 3.1 and to Theorem 4.1. Dubinin’s theorem is a neighbouring result under a full covering hypothesis and supplies no root connector.

Collinear roots and two sparse polynomial families

The following results impose concrete restrictions: roots on one line, a quintic with two missing coefficients, or a polynomial of the form P((zh)q) with P cubic. None covers a general polynomial with roots in the unit disc. We first state the finite inequalities used in their proofs, then explain how the inequalities produce contained paths. The formal links distinguish these two steps.

Collinear roots and Chebyshev comparison

The extreme zeros of Tn are ±cos(π/(2n)). Scaling them to ±1 makes the comparison polynomial have the same endpoint zeros as the polynomial under study; dividing by its leading coefficient makes both polynomials monic. Their difference then has smaller degree. Accordingly, put

rn=cosπ2n,Cn=12n1rnn.

Theorem 7.1 (Chebyshev comparison). Let m0, let pR[X] be monic of degree m+2, and let

1<c0<<cm<1,|ci|1.

Suppose p(1)=p(1)=0 and p(ci)p(ci+1)<0 for 0i<m. Then

min0im|p(ci)|Cm+2.

This is exactly the statement selected as the formal Chebyshev endpoint. It proves the finite alternation inequality; it does not yet construct the segment between two roots.

All real-rooted polynomials, and their images under rotations and translations, satisfy the collinearity hypothesis. Three noncollinear roots already fall outside it. The gain is an explicit sharp bound for the modulus along one adjacent-root segment, not a bound obtained by assuming that segment is contained.

Theorem 7.2 (a sharp bound for collinear roots). Let f be a monic polynomial of degree n2 whose zero occurrences are collinear, and let D be their diameter. Some two adjacent zero occurrences are joined by a segment of length at most D on which

(9)|f(z)|(D/2)n2n1cosn(π/(2n)).

The constant in (9) is best possible in every degree. Equality is attained by affine images of the zeros of Tn whose extreme zeros have distance D.

Proof. A repeated zero gives the constant path, so assume the zero values are distinct. Let m be the midpoint of the two extreme zeros, and choose θR so that their line is m+eiθR. Put R=D/2. Translation by m, rotation by eiθ and scaling by R give the polynomial

q(w)=Rneinθf(m+Reiθw),

which is monic with real zeros 1=y1<<yn=1, and |f(m+Reiθw)|=Rn|q(w)|.

Compare q with the monic endpoint-normalized Chebyshev polynomial

q(x)=Tn(rnx)2n1rnn.

Both q and q vanish at ±1, and |q|Cn on [1,1]. For each gap [yi,yi+1], choose ci at which |q| is maximal. The maximum lies in the interior: q vanishes at the endpoints and nowhere inside the gap. Since every root is simple, the signs at the n1 chosen points alternate. If every gap maximum were larger than Cn, then qq would have the same nonzero signs there. The intermediate value theorem would give n2 zeros between consecutive ci, in addition to the two zeros at ±1. These n zeros are distinct, but qq is nonzero and has degree at most n1 because its leading terms cancel. This contradiction selects a gap on which |q|Cn. Scaling back proves (9).

For sharpness, take

yk=cos((2k1)π/(2n))rn,1kn.

These are the zeros of q, have extremes ±1, and every adjacent gap contains a scaled Chebyshev extremum where |q|=Cn. No smaller universal constant can work. ◻

Corollary 7.3 (collinear Erdős case). If the zero occurrences of a monic polynomial of degree n2 lie on one line in the open unit disc, two of them are joined by a curve of length strictly below 2 inside {|f|<1}.

Proof. A repeated zero gives the constant path, so assume the zeros are distinct. Their diameter satisfies 0<D<2. Since cos(π/(2n))1/2, the defining formula gives Cn21n/21, with equality possible only at n=2. Thus (9) is strictly below one, and the selected segment has length at most D<2. ◻

Corollary 7.3 already follows from a theorem of Erdős, Herzog and Piranian : if the zeros of a monic polynomial of degree n are real, lie in [1,1] and have centroid in [0,1], then {|f|<1}R contains an interval holding at least n/2 of the zeros. Apply it to the normalized polynomial q, replacing it by the monic polynomial (1)nq(w) if its centroid is negative. This reverses the root line without changing modulus bounds. For n3 two consecutive zeros in that interval are joined by a segment of length at most D inside {|f|<(D/2)n}, and for n=2 the segment between the zeros lies in {|f|(D/2)2}. Theorem 7.2 adds the sharp level and its equality configurations.

Critical sequences and the extremal configuration.

For distinct real zeros, each gap between consecutive zeros contains exactly one zero of q, and |q| attains its maximum over the gap only there. The points ci chosen in the proof of Theorem 7.2 are therefore the critical points of q, and the gap maxima are the moduli of its ordered critical sequence (q(c1),,q(cn1)), with c1<<cn1. In this distinct-root setting, the ordered sequence determines the real polynomial up to an increasing real affine change of variable . The proof above uses only the alternation count, not this classification theorem. In this language, (9) says that a real polynomial of degree n with n distinct real zeros, leading coefficient a and zero diameter D has a critical value of modulus at most Cn|a|(D/2)n.

The comparison polynomial q is the monic polynomial of least deviation from zero on [1/rn,1/rn], characterised by the equioscillation conditions recalled in [17]. All n1 of its critical values have modulus Cn, so every critical point of q lies on the level curve {|q|=Cn}. Extremals with this property also occur in the level-curve length problem, where some extremal polynomial has all its critical points on {|p|=1} [14], and in the sharp bound for |f| on a connected sublevel set {|f|1} of a monic polynomial, proved by Eremenko and Lempert [18], whose equality cases are einθTn(21/n1eiθz+b) with θ real .

Formal scope.

Lean checks sign preservation, the alternating root-count mechanism, the scaled Chebyshev endpoint and uniform bound, and Theorem 7.1. It does not check the rigid normalization, the existence of the gap maxima, transport back to the root line, or the equality-node locations used in Theorem 7.2. These are ordinary steps. The sharpness assertion concerns the maximum of |f| on the selected adjacent-root segment, and the displayed configurations attain it; no claim is made that they exhaust the equality cases, and no claim is made that the selected segment is a shortest path in {|f|<1}.

Quintics with two missing coefficients

The next inequality selects two indices from five real pairs. Its three moment identities will come from the missing cubic and quadratic terms of z5+az4+bz+c. For 0<r<2 and 0si1, xi2si, put

Ei=si4(si+r2+2rxi).

Theorem 7.4 (a consequence of three moment identities). Suppose

(10)i=04xi=r,i=04(2xi2si)=r2,i=04(4xi33sixi)=r3.

Then at least one of the ten pairs 0i<j4 satisfies Ei<1 and Ej<1.

This is the exact finite conclusion selected as the formal two-index inequality. It selects two distinct indices. It does not assert that the corresponding complex root values are distinct.

The polynomial must have no z3 or z2 term in the coordinates used here. For example, z5+bz+c is included, but a general quintic with all coefficients nonzero is not. The root-location assumption alone does not imply the three moment identities. Those identities are precisely what lets the finite inequality find two radial segments.

Theorem 7.5 (a quintic with two missing coefficients). Let

p(z)=z5+az4+bz+c

and suppose its five zero occurrences w0,,w4 lie in the closed unit disc. At least two distinct indices satisfy

(11)|bwi+c|1.

If a0, two indices can be chosen with strict inequalities. If a=0, every index satisfies (11), and equality holds exactly when |wi|=1.

For open-disc zeros, two zero occurrences are joined inside {|p|<1} by a curve of length below 2: use the two radial spokes through 0 when their values are distinct, and the constant path when the selected occurrences have the same value.

Proof. If a=0, the root equation gives |bwi+c|=|wi|5 for every index, proving (11) and its equality clause. For a0, write a=reiϕ with r>0 and set zi=eiϕwi. The missing z3 and z2 coefficients and Newton’s identities give

(12)zi=r,zi2=r2,zi3=r3.

At a zero,

|bwi+c|=|wi|4|wi+a|.

Thus, for xi=zi and si=|zi|2, the squared modulus |bwi+c|2 is exactly Ei and (12) becomes (10). The third moment gives r3=|izi3|5<8, so 0<r<2 as required by the finite inequality.

We need to rule out four indices with squared modulus at least 1. The three known power sums determine the sum of any real harmonic polynomial of degree at most three over the roots. On the unit circle, s4(s+r2+2rx)1 reduces to xr/2. We therefore use the harmonic extension of (r/2x)(1x)2, which is nonpositive on that part of the circle. In the variables x=z and s=|z|2, this extension is

Hr(x,s)=(r/2x)(1x)2+(1s)(1r43x4).

The useful feature of this choice is the expansion

Hr(z,|z|2)=13r4+[(r74)z+(1r4)z2z34].

It is harmonic, and summing this expression with the three moments in (12) gives

(13)i=04Hr(xi,si)=52r.

On the unit circle its value is (r/2x)(1x)2, and

42r(r/2x)(1x)2=(x+1)((2r)(3x)2+(1x)2)0.

The maximum principle therefore gives Hr42r throughout the disc. For an index with s4(s+r2+2rx)1, one has s>0 and s41+4(1s) by convexity on (0,1]. Consequently

2r(x+r/2)s4s5(1s).

Put d=x+r/2, u=1x, A=1r/43x/4, and P=u2+(2r/5)A. The assumption s4(s+r2+2rx)1 gives 0d<2. Since Hr=du2+(1s)A, it is nonpositive when A0; when A>0, the preceding bound gives HrdP. The remaining estimate is the exact sum-of-squares identity

131P=25(d3831+14(u331))2+3140(u331)20,

which gives P1/31, and hence Hr(x,s)2/31 whether P is positive or nonpositive. Thus Hr2/31 whenever the squared modulus is at least 1. If four indices had squared modulus at least 1, (13) would give

52r42r+831<52r,

a contradiction. This proves the two-index conclusion when a0.

For either value of a, at a zero w,

p(tw)=(1t)c+(tt4)(bw+c)t4(1t)w5.

For 0t1 the three nonnegative weights sum to 1t5. The tail bound, |w|1, and |c|1 therefore keep each selected radial segment in {|p|1}. Under the open-disc hypothesis, |c|<1. Its coefficient 1t is positive for 0t<1, so

|p(tw)|<(1t)+(tt4)+t4(1t)=1t51.

At t=1 the value is zero. Thus both segments lie in {|p|<1}, and their total length is |wi|+|wj|<2. ◻

Formal scope.

The moment identities and the inequality selecting two indices have formal proofs. The source snapshot additionally contains a complete implementation of the open-disc sparse-quintic path conclusion, including the geometric assembly. The formal-source index places the complete open-disc path conclusion in its checked build. That declaration does not by itself assert every closed-disc equality clause of the longer theorem above. That is supplied build evidence, not a new compilation performed for this prose revision. The ordinary argument above is retained, and the source link remains at its original commit.

Polynomials obtained from a cubic by a power substitution

For f(z)=P((zh)q), the roots associated with a nonzero root of P form a regular q-gon centred at h. This rotational symmetry is a substantial restriction: a generic polynomial of degree 3q does not have it. It lets one contained segment for the cubic give two segments in the original variable. The first theorem supplies that segment.

Theorem 7.6 (a contained radial segment for a cubic). If r,s,vC have modulus below one, at least one u{r,s,v} satisfies

|(tur)(tus)(tuv)|1(0t1).

This is exactly the formal cubic segment inequality.

Theorem 7.7 (a cubic composed with a power map). Let q2, hC, P be monic cubic, and

f(z)=P((zh)q).

If every zero of f lies in the open unit disc and f has at least two distinct zero values, then two zeros are joined through h by a two-segment path of length below 2 inside {|f|<1}. Equivalently this closes the coefficient family

(zh)3q+A(zh)2q+B(zh)q+C

in every degree 3q6.

Proof. Fix a qth root y of a quotient root and a primitive qth root of unity ζ. The full fibre consists of h+yζk. Since every fibre point lies in the open unit disc,

(14)1qk=0q1|h+yζk|2=|h|2+|y|2<1.

Thus |y|<1, and the corresponding quotient root has modulus |y|q<1. This verifies the open-disc hypothesis for all quotient roots before selecting a radial segment for the cubic. The identity retains more information than these separate bounds: |h|<1 and every fibre radius is strictly below 1|h|2. Consequently, any two contained fibre segments constructed below have total length strictly less than 21|h|2. The position of the symmetry centre therefore improves the length bound; replacing it by 2 discards this information.

Write P(w)=(wr)(ws)(wv) and associate to r the real number Ar=(rs+v), cyclically. The exact sum is

Ar+As+Av=|r+s+v|2(|r|2+|s|2+|v|2)>3,

so one of these numbers, say Ar, exceeds 1. For 0t1,

|trs|2+|trv|22=t2|r|2+|s|2+|v|22tAr<1+t+t2.

AM–GM now gives |trs||trv|<1+t+t2. Consequently, for 0t<1,

(15)|P(tr)|<(1t)(1+t+t2)=1t31.

At t=1 the polynomial vanishes. The entire spoke is therefore strictly contained, including its origin endpoint.

For a nonzero quotient root satisfying the segment bound from (15), two distinct fibre points satisfy

f(h+tyζk)=P(tqr),

and their two spokes through h have total length 2|y|<21|h|22. If the selected quotient root is zero, choose a nonzero quotient root s and write P(w)=w(ws)(wv). For 0<t<1,

|P(ts)|=t(1t)|s|2|tsv|<2t(1t)12.

The values at both endpoints are zero, so this nonzero root supplies two distinct fibre points. If no nonzero quotient root exists, f has only one distinct zero value, contrary to the hypothesis. ◻

Formal scope.

Lean checks the identity for these three real numbers, the choice of a contained cubic segment, and the quartic counterexample, and also the complete translated cubic fibre theorem. The latter supplies the finite set of roots in each fibre, root-of-unity average, nonzero-root selection, pullback and explicit rectifiable path through the centre under the hypotheses displayed above. Its exact source occurs in the successfully compiled dependency closure of the source-bound Lean build and axiom-audit record. The theorem gives length below 2; the sharper 21|h|2 reading in the proof is recorded here as an ordinary consequence of the mean-square identity, not as a separately audited endpoint.

Scope of the formal results.

The finite declarations prove the Chebyshev comparison, the two-index quintic inequality and the cubic segment estimate. The formal-source index also records complete path theorems for the sparse quintic and the translated cubic family in its checked build. These are stronger than the finite inequalities alone. The sharper bound 21|h|2 and the quartic lifting arguments below retain the ordinary proof status stated beside them. A formal declaration must still be compared with the exact hypotheses and conclusion of the paper statement; a similar name is not enough.

Further families and counterexamples to proposed proof steps

The following sections collect additional sufficient conditions and counterexamples to particular path constructions. They are not a programme for proving the unrestricted historical assertion. The underlying research notes are retained at commit f214a6b4 and summarised in the dated overview of these arguments. Where a claim is based on a computation rather than a proof, that restriction is stated explicitly.

Roots close to a regular polygon

Let f(z)=i=1n(zai), n2, with all |ai|1. Put ρi=|ai| and D=|disc(f)|/nn. The Vandermonde determinant estimate says that, when D1η and 0η1/(80n2),

1ρi2nηn1,|aiaj|22ηnηn1,

where the second inequality is for ij. Moreover, the roots lie within 7η of a rotated regular n-gon, after a bijection. These estimates come from near equality in Hadamard’s determinant inequality, as follows.

Take the Vandermonde matrix Vim=aim, 0m<n, and let G=VV, si=Gii=m=0n1ρi2m and H=diag(si1/2)Gdiag(si1/2). The normalisation makes H positive semidefinite with diagonal entries one, and

D=detHisin.

Every factor is at most one by Hadamard’s inequality, so D1η forces each factor to be at least 1η. In particular,

(n1)(1ρi2)nsinη.

Hadamard–Fischer applied to the {i,j} principal block gives detH1|Hij|2, hence |Gij|nη. For t=aiaj, the finite geometric sum then gives

nη|m=0n1tm|nn(n1)2|1t|.

Together with 1t=1ρj2+aj(ajai), this proves the displayed separation bound. These two bounds need only 0η<1; the smaller range is used for the matching with a regular polygon.

For that matching, put κ=n2η/(n1)1/80 and ui=ai/ρi. The radial bound gives ρi2n1κ, while (1t)Gij=1tn gives |1ainajn|2nη for ij. Using |1beiθ|2=(1b)2+b|1eiθ|2 with b=ρinρ1n1κ, we obtain

|uinu1n|2nη1κ.

Choose the nearest nth-root phase to ui among u1e2πij/n. The inequality |eiθ1|2|θ|/π for |θ|π shows that its distance from ai is at most

nηn1+πη1κ7η.

The separation bound exceeds 14η in the stated range, so two roots cannot be assigned the same phase. There are n roots and n phases, giving the required bijection. This is an ordinary argument from standard determinant inequalities, not a new Lean declaration or a claim of priority for the stability estimate.

The hypothesis D1η with η1/(80n2) is a strong quantitative assumption, not merely a requirement that roots lie near the unit circle. The regular n-gon has D=1, whereas a configuration with a repeated root has D=0. In particular, radial information alone cannot supply this discriminant bound.

The comparison with unit-modulus roots is pointwise on a specified segment, not an ordering of complex polynomial values. Write ak=ρkuk, with |uk|=1. Under D1η and 0η1/(10n4), the same source proves

|f(sui)|k|suiuk|(0sρi).

The elementary step is

|suiρkuk|2|suiuk|2=(1ρk)(2s(uiuk)1ρk).

Here is where the discriminant hypothesis enters. The two bounds just proved imply

|aiak|>1n1 (ik),1ρknηn1<1(n1)2.

For k=i, the required inequality is 2s1+ρi, which follows from sρi1. For ki, it is immediate if (uiuk)0. Otherwise sρi gives

ρk(2s(uiuk)1ρk)ρi2ρk|aiak|21ρk|aiak|2<0.

Multiplying the factorwise inequalities proves the comparison. This argument uses the two elementary bounds, not the polygon-matching range; it therefore also covers n=2, when 1/(10n4)>1/(80n2). Moving the roots inward reduces this modulus bound, but does not select the angular directions of two contained segments.

For exact regular-polygon directions, write ai=ρiωζi, with |ω|=1 and ζ=e2πi/n. In any degree n2, the sufficient condition

0<ρk1,ρk2cos(2π/n)1for every k

makes the same factorwise comparison hold. Indeed, for ki with positive cosine, s1 gives 2s(ζik)2cos(2π/n)1+ρk; nonpositive cosines and k=i are handled as above. Since k(zωζk)=znωn, we obtain

|f(sωζi)|1sn(0sρi).

Every root-to-origin segment is therefore contained in {|f|1}. If all ρi<1, containment is strict: the displayed bound is below 1 for s>0, and |f(0)|=iρi<1. Any two roots can then be joined through the origin with length ρi+ρj<2. For 2n6 the lower bound on ρk is nonpositive, so every choice of positive radii at most one is allowed. For n7 the argument instead requires each radius to be at least 2cos(2π/n)1. This is a sufficient condition for the factorwise comparison, not a claimed necessary condition for a contained path. The favourable index in the general unit-circle averaging identity may move with s, however; an existence statement at one level does not supply a fixed pair of roots.

The exact binomial chord calculation

For f(z)=znrn, 0<r<1 and n2, the construction in Section 13 of the short note depends on the maximum over an entire chord. The endpoint values alone do not give that maximum. Put ω=e2πi/n and c=cos(π/n). When n3, define r=(1+cn)1/n and ε=(1rn)1/n; in the inner-chord case rr, set t=ε/cr.

Here is the chord estimate, including the smaller radii used in the second construction. For n3, let 0<sr. A point on the chord from s to sω can be written

z=sccosθei(π/n+θ),|θ|π/n.

Concavity of logcosx on [0,π/2) gives cos(nθ/2)cosn/2θ for 0θ<π/n. By symmetry and continuity,

1+cos(nθ)2cosnθ(|θ|π/n).

Set u=cosnθ1. Since zn=(sc)nueinθ, this inequality gives

|znrn|2(rn+(sc)n)2(u1)(sc)n((sc)n(u+1)2rn)0.

The last step uses (sc)nusnrn and (sc)nrn. Equality holds at the midpoint, where θ=0. Consequently the maximum on every such chord is exactly rn+(sc)n. Taking s=r proves the outer threshold; taking s=t=ε/cr proves the inner bound, and taking s=λt<t makes it strict. Every radial leg between s and r has modulus rn|z|n<1. Its two legs and crossing chord have length 2r2s(1sin(π/n))<2r, which proves the stated length formula and shows that contraction preserves the strict length bound.

For n=2, the chord is a diameter and its maximum is r2<1; its length is 2r<2. For n3, the outer chord works exactly when r<r, and its length is 2rsin(π/n). At r=r it reaches level one at its midpoint. If rr, the two radial legs and inner crossing have length

2r2εtan(π4π2n)<2r<2.

Contracting the crossing radius makes the level bound strict, as proved above. The argument compares these constructions, not their lengths with all admissible paths.

A bounded-radius concyclic class

A different argument gives a chord when all roots lie on a circle of sufficiently small radius. Let f be monic of degree n3 with distinct zeros on a circle of radius ρ. If 2ρn1, two adjacent zeros are joined by their straight chord, whose length is at most 2ρsin(π/n)<2, and the chord lies in {|f|<1}. (If a zero is repeated, the short-connection conclusion is immediate; the distinct case is the substantive one.)

For each fixed degree n, the radius condition is ρ21/n. It allows arbitrary spacing on that circle, but does not cover every radius ρ<1. No restriction on the circle’s centre is imposed.

After translating and scaling, let g be the monic polynomial with roots w1,,wn on the unit circle. Such a polynomial is self-inversive: zng(1/z) is a constant multiple of g(z), with the constant of modulus one. Equivalently, einθ/2g(eiθ) is real up to a fixed phase. Choose

c=(1)n+1jwj,q(z)=znc.

Then g and q have the same leading and constant coefficients, and their boundary values have a common real phase. If every root gap contained a point with |g|>|q|, the real boundary function of gq would have alternating signs at these points. Advancing the angle by 2π multiplies that function by (1)n, so the alternation also holds across the final gap. The intermediate value theorem would give n distinct unit-circle zeros of gq. This is impossible: its degree is at most n1, and g=q cannot satisfy the assumed strict inequalities. Thus some adjacent-root arc satisfies |g||q|2. The interior of that arc contains no zero of q, since g is nonzero there. As consecutive zeros of q are separated by angle 2π/n, the selected arc has angular width at most 2π/n. This explains why the same selected pair also has the required short chord. To pass from this arc to its chord [a,b], let ν be the unit normal pointing into the circular segment bounded by them. On the open chord, logarithmic differentiation gives

νlog|g(z)|=wj{a,b}Re(νzwj)|zwj|2>0.

The endpoint terms vanish because their directions are tangent to the chord. Every remaining numerator is positive because the other roots lie strictly on the far side of its line; n3 ensures at least one such term. The harmonic function log|g| has no interior maximum and tends to at a,b. A maximum cannot lie on the open chord either, since moving into the circular segment increases the function. It is therefore attained on the arc, and the maximum on the chord is strictly smaller. Scaling back gives |f|<2ρn1 throughout the chord, with f=0 at its endpoints. These are the arguments of Theorem C and Lemma S, Sections 3–4 of the concyclic note.

The argument is an ordinary proof outside Lean. The exact-rational checker checks finitely many identities used in the proof and configurations, while the numerical checker is regression and stress-test evidence. The arc constant 2 is attained by the regular n-gon. Thus the bound obtained by passing through the arc is ρ21/n, although this cutoff tends to 1 as n. This does not assert optimality of the chord bound or exclude another contained path at a larger radius. Nor does arc sharpness make the pair of radial segments shortest. For example, for g(z)=z31/8 the chord between 1/2 and e2πi/3/2 has length 3/2<1, whereas the two radii have total length 1. The binomial calculation above gives a maximum of 9/64<1 on that chord. The length-2 equality at zn1, proved below, concerns the uncontracted closed-level problem.

Power substitutions in trinomials

The radial-segment identity and strict bound are formalized in cancellation along a trinomial root segment and containment of a trinomial root segment.

The trinomial identity also applies after a power substitution. Fix integers 1r<m and q1, and consider the translated monic polynomial

f(z)=(zh)qm+a(zh)qr+c.

The strict exponent inequality keeps the leading monomial separate. The algebraic identity below also holds when r=m, but then the two leading terms merge and the displayed polynomial need not be monic or have degree qm. Writing w=(zh)q reduces the root equation to wm+awr+c=0. At such a quotient root the middle coefficient can be eliminated exactly: for 0u1,

umwm+aurwr+c=(1ur)c(urum)wm.

This is a nonnegative combination of c and wm, with weights 1ur and urum summing to 1um. The formal radial-segment estimate gives strict containment when |w|<1 and |c|<1.

For q2 and a nonzero quotient root satisfying these bounds, choose two distinct solutions y1,y2 of yq=w. Their common modulus is |w|1/q<1. To lift a quotient radial segment, set u=tq:

|f(h+tyi)|(1tqm)max{|c|,|w|m}<1(0t1).

Thus the two lifted segments join h+y1 to h+y2 through h with length 2|w|1/q<2. The construction uses any quotient root with the stated modulus bound; it does not prove that such a root exists without an additional hypothesis. A zero quotient root instead gives a root of multiplicity at least q at h and hence a constant path between two occurrences. The formal source checks the factorization, radial-segment estimate and finite length inequality. It does not establish the existence of a suitable quotient root or formalise the selection and lifting just described. Thus its scope is the segment inequality and finite length calculation, not the complete path construction or unrestricted Erdős #1041.

A coefficient condition for four-term polynomials

With one additional monomial, Abel summation gives a sufficient condition involving the two lower coefficients. Let

g(w)=wm+awr+bws+c,m>r>s1,

assume all roots of g lie in the open unit disk, and let w1,w2 be roots of the two smallest moduli. If

|c|+|b||w2|s<1,

then the complete radial spokes from w1 and w2 to the origin lie in {|g|<1}, and their broken line has length strictly below 2. The simpler coefficient condition

|b|+|c|1

makes every root-to-origin segment contained; the coefficient a has no additional restriction beyond the assumed root locations. This coefficient condition includes b=0 and |c|1, but is not automatic for all four-term polynomials with roots in the disc.

The mechanism is visible in one identity. At a root w and for 0u1,

g(uw)=(1us)c+(usur)(c+bws)+(urum)(wm).

Here the root equation has eliminated awr before taking absolute values. The three weights are nonnegative and sum to 1um. The controlled terms are c, c+bws and wm; their moduli are strictly below one under the root-dependent condition. The same identity explains why no bound on a is needed. Lean checks the factorization and the resulting strict spoke theorem under the exact weak exponent hypotheses 1srm; it also checks the coefficient-only corollary above. Its weak bound |b|+|c|1 still gives strict containment: the root-disc hypothesis implies |c|<1, and, if b0, |w|s<1 gives |c|+|b||w|s<|c|+|b|1. If b=0, the required bound is simply |c|<1.

An alternative criterion uses a complex power sum to select two indices. Let S index a finite family of roots, N=|S|2, and

M=iSwis.

The squared-modulus identity gives

iS|c+bwis|2=N|c|2+|b|2iS|wis|2+2Re(cbM).

Consequently, if every |wi|<1, |c|<1, and

N(|b|2+|c|2)+2Re(cbM)<N1,

then two distinct indices i,jS satisfy |c+bwis|<1 and |c+bwjs|<1. Indeed, the displayed identity bounds the sum of squared moduli strictly below N1. If at most one index had modulus below one, the other N1 terms would each contribute at least one. This explains both the threshold N1 and why the criterion selects two indices. Applying the resulting contained-segment theorem to these inequalities proves that both root segments lie strictly in {|g|<1}. Retaining the signed cross term permits the inequality to hold for configurations outside the coefficient-only triangle |b|+|c|1. The formal hypotheses do not require iwi to be injective, so distinct indices need not denote distinct root values. For the polynomial consequence, the family must be a submultiset of the zeros, respecting their algebraic multiplicities. A repeated zero then already gives a constant path between two occurrences. Repeating a simple zero in an arbitrary indexed family cannot supply a second occurrence. The two sufficient conditions are not ordered by strength. For example, g(w)=w5+19/20 has all roots in the open unit disc and satisfies the coefficient condition with b=0. For its full five-root list, however, the left side of the power-sum condition is 5(19/20)2=361/80>4=N1, so that condition fails. Its benefit is the use of cancellation in the cross term, not inclusion of every case covered by the coefficient condition. Conversely,

g(w)=(w21/2)(w3+4/5)=w512w3+45w225

has all roots of modulus 1/2 or (4/5)1/3, hence below one, but |b|+|c|=6/5>1. Its full root list has M=iwi2=1: the two quadratic roots contribute 1, and the three cubic roots contribute 0. The power-sum left side is 5(16/25+4/25)16/25=84/25<4. Thus this criterion does cover root-disc polynomials excluded by the coefficient condition.

For q2 and f(z)=g((zh)q), assume also that all roots of f lie in the open unit disc. If yq=w and ω=e2πi/q, the roots h+ωjy satisfy

1qj=0q1|h+ωjy|2=|h|2+|y|2<1.

Thus every quotient root has |w|=|y|q<1, which supplies the root-disc hypothesis used above, and every lifted spoke has length |y|<1. Two selected spokes join through h with total length below 2; repeated root occurrences instead permit the constant path. The Lean theorem assumes the finite root family, its complex power sum M, and the displayed inequality. It neither derives that inequality from arbitrary coefficients nor verifies the family’s polynomial multiplicities, the cyclic lifting, or the final path construction. Completeness of the root list is not required for the selection argument: a submultiset respecting multiplicity suffices. Without one of the power-sum, root-dependent, or coefficient-only inequalities, the tetranomial case is not covered by this argument; this family does not solve unrestricted Erdős #1041.

A quartic composed with a power map

Pendyala’s degree-four theorem [11], with his four-point radial lemma , can also be lifted through every nontrivial cyclic power. Let P be a monic quartic, let q2 be an integer, and set

f(z)=P((zh)q).

Assume that every root of f lies in the open unit disc. A repeated root of f gives the constant path, so suppose f is squarefree. Then the roots of P are distinct and nonzero. For a root w=yq of P, all points h+ζjy, with ζ=e2πi/q, are roots of f. Hence the open-disc hypothesis gives

1qj=0q1|h+ζjy|2=|h|2+|y|2<1.

In particular |w|1/q=|y|<1, which is the bound needed for the lifted length, and also |w|<1. Pendyala’s chord-or-radial argument supplies the quotient geometry in two cases. If two quotient roots satisfy |wiwj|<1, every point w of the chord [wi,wj] lies in the unit disc; the two endpoint factors of |P(w)| have product at most |wiwj|2/4 and the other two factors are below 2, so |P(w)||wiwj|2<1. Otherwise the quotient roots are pairwise at distance at least 1. Choosing R with maxk|wk|<R<1 and applying the four-point radial lemma to the points wk/R gives distinct i,j with |P(twi)|R4 and |P(twj)|R4 for 0t1, so the radial segments [0,wi] and [0,wj] lie in {|P|<1}. The extra issue is metric: a short chord in the w-plane need not lift isometrically through yyq.

Put α=1/q. On a chord avoiding 0, choose a continuous argument and hence a root lift y with yq=w. Differentiation gives |dy|=α|w|α1|dw|, independently of the chosen root. If the supporting line has distance d from 0, and x is distance along that line from the perpendicular foot, then

(d2+x2)α1xα1(x>0).

The negative exponent is why replacing |w| by x gives an upper length bound. Lean checks the integral of the power-map derivative

α0Axα1dx=Aα.

If the foot lies on the chord, split there: the two integrals are bounded by the α-powers of the distances from the foot to the endpoints, hence by |a|α+|b|α. If the foot lies outside the chord, integrate on one side of it; extending the interval to the foot bounds the result by the α-power of the farther endpoint’s modulus. When the chord passes through 0, choose a continuous root on each half and join the lifts at 0; the integral is finite because α>0. This proves the chord-lift estimate

length([a,b]~)|a|1/q+|b|1/q.

The strict endpoint-length estimate also proves that if 0a,b<1, α>0, and a candidate length L is at most aα+bα, then L<2. The close-pair chord therefore has a lift of length below 2. In the other case the quotient arms meet at 0, so their lifts are radial segments meeting at h, with total length |wi|1/q+|wj|1/q<2. In both cases f=P((zh)q) transfers containment from the quotient curve. Distinct quotient endpoints give distinct roots of f. This proves the path assertion in every degree 4q8. The fibre average gives a little more: |h|<1 and |wk|1/q<1|h|2 for every quotient root. Consequently the same constructed path has length

length<21|h|22.

This refinement concerns the translated power-substitution family, not arbitrary degree-4q polynomials.

Pendyala proves the quartic geometric theorem and its four-point radial lemma. The local Lean module checks the antitone density inequality, its integral, the strict powered endpoint-length bound, and the final length estimate. It does not formalize Pendyala’s geometric lemma, the continuous covering-space construction of the root lift, or the ordinary chord/radial case assembly. This is a family defined by a power substitution, not a proof of unrestricted Erdős #1041.

The joining point in the quartic construction.

Pendyala’s proof of [11] uses a smallest enclosing disc and joins the selected roots through its centre. For the power substitution we instead apply [11] to the centred disc |w|R. That lemma requires only the disc and pairwise-distance hypotheses, not minimality of the disc. Keeping the joining point at 0 is what makes the radial lift above valid. The endpoint-length bound for a single chord would not justify lifting an arbitrary broken line through a nonzero quotient vertex.

A mean bound for critical values in every degree

The next theorem gives the quadratic case of a Poisson argument for critical-value moments. It allows a disc of any centre and radius, repeated roots, and repeated critical points. After proving this case, we derive the stronger exponent 4/(n1) and explain how vanishing complex power sums permit still larger exponents. None of these moment bounds controls the lengths of inverse paths ending at the critical points.

Dubinin [21] proves the sharp unit-disc critical-value product inequality using the resultant identity, the maximum-modulus principle and Schur’s Vandermonde inequality. The positive-moment estimate below implies his product bound by AM–GM. When n3, the product estimate alone cannot control a positive moment: a list T,T1,1,,1 has product one, but its sum of pth powers is unbounded as T for every p>0. This compares the information in two inequalities for nonnegative lists; it does not claim that these lists occur as critical values of polynomials in the theorem. In degree two there is just one critical value, and the product and positive-moment bounds are equivalent. For a zero prescribed at the origin, his Theorem 3 (p. 1174) gives

(j|f(cj)|)1/(n1)(n1)(|f(0)|2nn)1/(n1).

Dubinin explicitly identifies Tischler’s earlier contribution . His Theorem 1 uses dissymmetrisation; that is not the proof mechanism of Theorem 2. Schur’s original paper [27] is the historical antecedent cited there, not a separately re-proved source in this record. A sharp marked-zero positive-moment bound remains a separate question. The addendum [26] reports a reduction to boundary-root configurations, without solving the resulting angular optimisation. That unavailable addendum is not a proof dependency of the critical-value theorem below.

Theorem 8.1 (a mean bound for critical values). Let f be monic of degree n2, with roots in a closed disc of radius R0. If c1,,cn1 are its critical points counted with multiplicity, then

(7)j=1n1|f(cj)|2/(n1)(n1)R2n/(n1).

Consequently the lower exponents used elsewhere in the record satisfy

(8)j=1n1|f(cj)|1/(n1)(n1)Rn/(n1)

and

j=1n1|f(cj)|1/n(n1)R.

The constant is attained by f(z)=(zτ)nλ with enclosing disk centred at τ and radius R=|λ|1/n.

The finite inequality behind the theorem concerns arbitrary points of the disk, without asking them to arise as critical points. Its quadratic form is

j=1m(k=1m|1cjck|)2/mm,|cj|1.

The following pointwise bound explains why these finite inequalities control critical values in every degree.

Lemma 8.2 (reflected-derivative bound). If f is monic of degree n2 with roots in the closed unit disk, and c1,,cn1 list its critical points with multiplicity, then

(9)|f(cj)|k=1n1|1cjck|.

The reflected-derivative inequality is checked in Lean, including closed-disc roots and critical-point multiplicities.

Proof. First put all roots ai strictly inside the disk. We want a numerator that equals nf at the critical points and can be compared with f on the circle. Set

N(z)=nf(z)zf(z),G(z)=nk(1ckz).

The numerator is the polar derivative at 0: the conventional polar derivative at α is nf(z)+(αz)f(z); see Rather–Gulzar, Section 1 for this notation. Its leading term cancels, and N(cj)=nf(cj). Reflection gives |G|=|f| on the circle. Gauss–Lucas puts every ck inside the disc, so G has no zero on its closure. Thus N/G is a holomorphic quotient to which the maximum-modulus principle applies. On |ζ|=1,

Reζf(ζ)f(ζ)=i(12+1|ai|22|1aiζ¯|2)n2.

Writing the logarithmic derivative as w, the identity |nw|2|w|2=n22nRew0 gives |N||G| on the circle. The maximum-modulus principle applied to N/G gives the same comparison inside. At cj, N(cj)=nf(cj); dividing by n and conjugating each factor proves eq:critical-reflected-product. For closed-disk roots apply this result to fr(z)=rnf(z/r), 0<r<1, whose critical points are rck:

rn|f(cj)|k|1r2cjck|.

Let r1. This also handles boundary critical points and all multiplicities without selecting local branches. ◻

Set m=n1. The weighted Poisson proof below gives the quadratic finite inequality for every m1. Gauss–Lucas and Lemma 8.2 then give j|f(cj)|2/mm on the unit disc. Applying this to Rnf(h+Rz) and scaling back proves (7) for R>0; if R=0, all critical values vanish.

The two displayed consequences are the lower power means of the same nonnegative m-tuple. Equivalently, after unit-disc normalization, apply the monotonicity of normalized Lp means from exponent 2/m first to 1/m and then to 1/(m+1)=1/n. Scaling back contributes respectively Rn/m and R. These are consequences of the quadratic case; the higher-power argument below strengthens that case without changing these lower-exponent applications.

The quadratic mean and both lower-exponent consequences are recorded as checked in the complete critical-value mean. This includes arbitrary centre, zero radius, and critical points counted with multiplicity. The source version and formal target are identified in the source-bound Lean build and axiom-audit record. The earlier candidate description in the source header predates that run.

The quadratic moment controls the number of large critical values. For R>0, write rj=|f(cj)|1/n. Then

j(rj/R)2n/(n1)n1,#{j:rjtR}n1t2n/(n1)(t>0).

The counting bound follows by retaining just the indicated summands. The fourth-power refinement proved below replaces the exponent 2n/(n1) here by 4n/(n1), improving the count for t>1. For 0<t1 the trivial bound n1 is at least as good. The binomial equality family has every rj=R, but these distributional bounds still leave the geometry of the joining paths to be supplied.

The weighted Poisson inequality and its equality case.

For one point c of weight 1, the quantity to bound is (1|c|2)21; equality holds only at c=0. For two points c,c of equal weight, it is 1|c|41. These examples suggest why a nonzero configuration should lose from equality. Now let wj0, jwj=1, and |cj|1, with repetitions allowed. Write G(z)=k|1ckz|wk, taking a factor of exponent zero to be one. We seek an analytic function with modulus G: its logarithmic derivative will express the weighted Poisson kernel, and its Taylor coefficients will measure the loss from equality. For |c|<1 and |ζ|=1, let Pc(ζ)=(1|c|2)/|ζc|2, and write dm=dt/(2π) on ζ=eit. When every centre is strictly inside the disc, choose analytic logarithms zero at the origin and put

g(z)=expjwjlog(1cjz)=1+ν1aνzν,P=jwjPcj.

On the unit circle P=12(ζg/g), by logarithmic differentiation. The Poisson formula reproduces g(c) from its boundary values and gives Pcdm=1 for |c|<1. Expanding a square therefore yields

|g|2Pcdm|g(c)|2=|gg(c)|2Pcdm0.

This explains why the same kernel bounds the value at each centre. Take c=cj, multiply by wj and sum to obtain

jwjG(cj)2|g|2Pdm=1ν1(2ν1)|aν|2.

To see the last equality, expand |g|2 and ζgg and integrate on the circle. Orthogonality leaves 1+ν1|aν|2 and ν1ν|aν|2, respectively. The analytic function g extends to a neighbourhood of the closed disc in this interior case, which justifies the termwise integrations. For closed-disc centres replace cj by rcj, 0<r<1. The actual coefficient of degree ν becomes rνaν, where the fixed coefficients are defined from the analytic function near zero. Pass to r1 first with an arbitrary finite coefficient sum. Nonnegative finite deficits then give summability and the infinite inequality; no boundary holomorphic logarithm is required. Lean checks the exact radial transport of each Cauchy coefficient, the finite boundary-deficit inequality, and the summable full boundary deficit.

If equality holds, all positive-degree coefficients vanish, so g=1 near zero and jwjcj/(1cjz)=0 there. Group equal centres before clearing denominators. A nonzero centre of positive total weight gives a nonzero pole coefficient, which is impossible. Thus equality is equivalent to cj=0 on positive support. In particular, strictly positive weights force all centres zero. A point of weight zero is unconstrained: weight one at 0 and weight zero at 1 still give equality. Grouping equal centres is necessary: an argument that assumed they were distinct would not prove the stated equality case.

Equal weights in jwjG(cj)21 give the quadratic finite inequality above for every m1, with equality only at the zero configuration. The linear inequality follows separately. For M=jwjG(cj), the variance identity

M2+jwj(G(cj)M)2=jwjG(cj)2

gives M1. Equality in this Cauchy–Schwarz step means that the values G(cj) are constant at all indices of positive weight; equality in the final bound also requires equality in the quadratic inequality. The three-point and four-point specialisations follow with their equality cases. The formal-source index records the complete weighted theorem in its checked build. The hypotheses permit repeated centres and zero weights; the equality condition refers only to centres of positive weight.

This equality condition also identifies all equality cases of Theorem 8.1 for a fixed containing disc D(h,R) with R>0. Equality in the critical-value bound forces equality in the quadratic finite inequality after normalisation, so every critical point is 0. Thus the normalised derivative is nzn1 and the polynomial is znλ, with |λ|=1 forced by equality. Restoring the centre and radius gives exactly f(z)=(zh)nλ with |λ|=Rn. Equality in either lower-power consequence also forces equality in the quadratic bound, so it has the same family. For R=0 the only possible polynomial is (zh)n. This classification follows from the ordinary proof; it is not an additional assertion about the cited Lean endpoints.

The earlier three-point Hölder argument and four-point matching argument are not used here. Their scalar identities do not justify the omitted inequalities; the proof is the weighted Poisson calculation above.

Higher powers and vanishing complex power sums.

The quadratic inequality is the formally recorded case, not the full range of the analytic argument. To estimate Gp for p>0, we need an analytic function whose squared modulus is Gp. Using the same logarithms as above, define

Hp=gp/2=1+ν1bνzν.

For interior centres, logarithmic differentiation and the Poisson majorant give

P=14pζHpHp,jwjG(cj)p|Hp|2Pdm=1ν1(4νp1)|bν|2.

The identity follows from the same two orthogonality calculations used for g; only the coefficient of the derivative term changes. For 0<p4 every displayed coefficient is nonnegative. Hence

jwjG(cj)p1(0<p4).

Boundary centres follow by replacing cj by rcj: the degree-ν coefficient becomes rνbν, and the values on the left are Gr(rcj)=k|1r2ckcj|wk. First retain finitely many nonnegative terms, then let r1. Zero weights can be omitted throughout. This proves the closed-disc inequality without differentiating a boundary logarithm. The argument is the ordinary power-parameter Poisson identity, not an additional conclusion of the cited complete Lean theorem.

In particular, equal weights and Lemma 8.2 give, with m=n1,

1mj|f(cj)|4/m1mjG(cj)41

on the unit disc. For roots in D(h,R) this becomes

j|f(cj)|4/(n1)(n1)R4n/(n1).

As before, R>0 is handled by Rnf(h+Rz), and R=0 by the vanishing of all critical values. The constant is attained by (zh)nλ with |λ|=Rn. This proves sharpness of the constant, not optimality of the exponent for each fixed degree.

At p=4 the coefficient of |b1|2 vanishes, so the previous quadratic equality proof cannot simply be reused. If equality holds, the finite-deficit bounds imply H4=1+b1z. If b10, the rational identity H4/H4=2g/g shows, by comparing poles and their residues, that all nonzero centres coincide at a=b1 and have total weight 1/2. The other half of the weight is at zero. Their fourth-power average is

12(1+(1|a|2)2)=1|a|2+12|a|4<1(0<|a|1),

a contradiction. Thus H4=1, and the pole argument already used for g forces every centre of positive weight to be zero. Conversely that configuration gives equality. It follows that the fourth-power critical-value estimate has the same equality family as the quadratic one for a fixed containing disc.

For p>4, the coefficient 4/p1 is negative, so the nonnegative-deficit argument no longer applies. To extend its range we can force the first Taylor coefficients to vanish. Let s1 be an integer and suppose

jwjcjk=0(1k<s).

The expansion

logHp(z)=p2k1jwjcjkkzk

then has no terms of degree below s, so b1==bs1=0. All remaining coefficient weights are nonnegative for 0<p4s. The same proof therefore gives jwjG(cj)p1 throughout that range. For a monic polynomial with roots in D(h,R), R>0, the resulting endpoint is

j|f(cj)|4s/(n1)(n1)R4sn/(n1),j(cjh)k=0(1k<s).

There is no cancellation hypothesis when s=1. For s=2, the condition says that the critical-point centroid is the disc centre. Comparing the coefficients of f and f shows

1n1jcj=1ni=1nzi,

so this is also the root centroid. Recentring can increase the required radius: for 0<r<1, the roots of (zr)2(z+r) lie in D(0,r), but their centroid is r/3, and a disc centred there needs radius 4r/3 to contain the root r. Thus the exponent-8/(n1) statement cannot be applied at the old centre with the old radius. These are exact cancellations, not merely bounds on the moments. All higher-power conclusions in this paragraph are ordinary analytic results; the linked complete Lean moment endpoint has exponent 2/(n1).

Formal scope of the Poisson and integration steps.

The square-expansion proof above applies whenever g is holomorphic on the disc and continuous on its closure, with |c|<1. The linked norm-square majorization uses the Poisson formula for a real part and the nonnegativity of a square. The weighted kernel identity identifies the pointwise Poisson mixture. Separately, absolute series transport justifies termwise circle integration when the terms are circle integrable and admit a summable uniform norm bound; its Taylor double-product form assumes absolute summability of both coefficient sequences. The complete weighted and critical-value targets are indexed in the recorded checked dependency closure. Their exact statements, dependencies and status are recorded in the accompanying formal-scope map. Historical totals of named axiom prints are not an additional proof of a paper statement; no fresh axiom audit was run for this revision.

A uniform central region in every degree.

For every m1, the inequality for points in a smaller disc proves

|cj|1e2(1jm)j=1m(k=1m|1cjck|)1/mm.

To see the mechanism, set hj=m1klog|1cjck| and Dj=log(1|cj|2). Write Mν=m1kckν for the normalised complex power sums used in this calculation. The absolutely convergent series for log(1z) gives

hj=ν1cjνMνν,1mjhj=ν1|Mν|2ν.

In particular, jhj0. Cauchy–Schwarz applied to the first series, using ν1|cj|2ν/ν=Dj, gives hj2(m1ihi)Dj. The radius bound gives Dj2. Put r=m1ihi. If r=0, every hj vanishes. For r>0, convexity bounds eh by the chord of its graph over [2r,2r]. Averaging and using m1jhj=r2 gives

1mjehjcosh(2r)r2sinh(2r)1.

For the last inequality, the function coshu(u/2)sinhu equals 1 at u=0 and has derivative (sinhuucoshu)/20 for u0. Thus the radius bound supplies the estimates needed for the geometric-mean inequality; no further series hypotheses are imposed. This alternative proof includes the all-zero configuration but requires the smaller radius 1e2. The weighted theorem above covers the whole closed unit disc. The next logarithmic argument imposes a different sufficient radius condition; neither restriction belongs to the weighted theorem.

For m1, let |ci|2a<1, with a0, and put L=log(1a). The uniform-radius theorem gives the geometric-mean inequality

eL1+2Li=1m(j=1m|1cicj|)1/mm.

For a=1/2 the scalar hypothesis holds, since 21+2log2; for a=3/4 it fails, since 4>1+2log4. Thus it supplies a sufficient restriction on the squared radii, not a necessary condition for the geometric-mean inequality.

The proof uses point-dependent logarithmic bounds. Write Hi=m1jlog|1cicj| and Di=log(1|ci|2). The preceding logarithmic calculation gives iHi0 and Hi2(Di/m)jHj. For nonnegative upper bounds MiHi, Taylor’s formula with integral remainder gives

eHi1+Hi+Φ(Mi)Hi2,Φ(t)=01(1s)estds.

Since Φ(Mi)0, summing and using the quadratic bounds yields

ieHim+(11miΦ(Mi)Di)jHjm

whenever iΦ(Mi)Dim. This is the sufficient condition in the formal inequality with individual upper bounds. Taking Mi=L gives Φ(L)L1 as a sufficient condition, since Hi,DiL. For L>0, integration gives Φ(L)=(eL1L)/L2; hence this condition is exactly eL1+2L. At L=0 all centres vanish, so the conclusion is immediate.

Four points without a matching or numerical split.

The preceding weighted proof with m=4 and wj=1/4 gives

j=14(k=14|1ckcj|)1/44,|cj|1,

with equality if and only if all four centres vanish. The checked four-point theorem includes this equality case. In particular, the inequality is strict as soon as one centre is nonzero, even with repeated centres or centres on the unit circle.

This four-point consequence needs neither the former 21/25 split nor a perfect-matching Hölder step. The scalar stationary-point inequalities from that approach are not a proof of its missing steps. The two restricted arguments above remain independent alternatives. The recorded compilation and axiom checks concern the weighted proof and its three- and four-point consequences.

The mean inequality gives μRn. In the unit-disc normalisation R=1, this does not force the smaller quintic threshold μ<1/M5 below. For f(z)=zn1, every critical value has modulus one, so no uniformly smaller bound holds on the closed-disc class. These are bounds for moduli, not inverse-ray lengths; a path selection or a metric comparison is still needed.

A sufficient critical-value threshold in degree five

The distance bound for the two nearest roots.

Let f have degree n2 and all roots in the closed unit disc, and let c be a critical point with f(c)0. List roots with multiplicity. Its two nearest roots have total distance at most 2. The root-disc hypothesis, rather than a bound on |f(c)|, is what gives this estimate.

Rotate so that c=t0, and order the distances as 0<d1d2dn. Logarithmic differentiation gives j(zjc)1=f(c)/f(c)=0. Dividing |zjc|2+2t(zjc)1t2 by dj2, then summing and using the reciprocal balance, gives

n(1t2)jdj2.

Thus t<1 and d11t21. The same reciprocal balance, with the nearest term isolated, gives d2(n1)d1.

Suppose d1+d2>2. Since d21+t, we have d1>1t, and hence

1t2<d1(2d1)<d1d2.

The first strict inequality uses that x(2x) is increasing on [0,1]. It follows that

n(1t2)(d12+(n1)d22)<d2d1+(n1)d1d2n.

For the last step, put x=d2/d1[1,n1] and expand (x1)(x(n1))0. This contradiction proves the closed-disc bound. For roots in the open unit disc, scaling by a containing radius 0<R<1 gives d1+d22R<2. This is the argument in the proof for the two nearest roots; Lean checks its real-inequality core. The root-disc reduction above is an ordinary complex-variable argument.

This argument selects the two nearest roots but does not put their segments inside a polynomial sublevel set. The next calculation supplies that separate containment estimate under a bound on |f(c)|.

Containment of the two selected segments.

Let f be monic of degree n3 with roots in the closed unit disc. The following estimate controls the segments from a critical point to its two nearest roots. To specify the constant, put

Mn2=max0t14nyn(1t)2((1t)2+2ty+n(n2)t2)((1t)2+2t(ny)n2)n2.

Here t parametrises the segment. The product estimates below use f(c)=0 and the ordering of distances, not the root-disc hypothesis; the latter enters when bounding the combined segment length. To explain the other parameter and the coefficient n(n2), suppose f(c)0, order the roots a1,,an by distance from c, and set vj=(a2c)/(ajc). Then v2=1, |vj|1 for j2, and jvj=0 by f(c)=0. With y=1v1, this gives

y=2+j=3nvj[4n,n],|v1|n1.

Consequently

|1tv1|2(1t)2+2ty+n(n2)t2,1n2j=3n|1tvj|2(1t)2+2t(ny)n2.

The factor v2=1 contributes (1t)2. Applying AM–GM to the remaining n2 squared factors in f(c+t(a2c))/f(c)=j(1tvj) gives the defining expression for Mn2. Thus the maximisation is an explicit bound for the second segment, not an additional optimisation hypothesis about the roots.

For the nearer segment, put xj=(a1c)/(ajc). Now x1=1, |xj|1 for every j, and jxj=0. Hence

j=2n|1txj|2(n1)(1+t2)+2t,

so AM–GM gives

|f(c+t(a1c))f(c)|2(1t)2((1t)2+2tnn1)n1.

This bound is at most Mn2 for every n3, not just for numerically tested degrees. Indeed, set y=n/(n1) in the defining maximum. This value is admissible because n/(n1)(4n)=(n2)2/(n1)0. The last factor then has base (1t)2+2tn/(n1), and the preceding factor has this same base plus n(n2)t20. Their product therefore dominates the displayed nearer-segment bound. Thus |f(z)|Mn|f(c)| on both segments, so 0<|f(c)|1/Mn gives containment in {|f|1}; the critical-point distance estimate gives total length at most 2. If f(c)=0, two root occurrences already coincide at c. The quadratic case is the direct root segment treated earlier. For degree five the maximum evaluates to

M5=(1t)(1+t)316t24t+1,t=516+310580,1M5=0.2760461.

The breakpoint comes from the constraint on y, not from a numerical search. For fixed 0<t<1, write the two bases in the definition of M5 as

A=(1t)2+2ty+15t2,B=(1t)2+2t(5y)3.

They are positive for 1y5, and ylog(AB3)=2t(BA)/(AB). Thus the unconstrained maximum occurs at A=B, or y=5/445t/8. This reaches the lower endpoint 1 at t=2/5; thereafter the maximum is at y=1. For 0t2/5 the resulting expression is (1t)(1+t/2+19t2/4)2, whose derivative is

5t(1419t)(19t2+2t+4)160.

For 2/5t1, the square of the resulting expression is (1t)2(1+t)6(16t24t+1), whose derivative is

4t(1t)(1+t)5(40t225t2).

The quadratic changes sign once on this interval, at t, so the second branch increases from the common breakpoint to t and then decreases to zero. Since the first branch increases to that breakpoint, t gives the global maximum. This proves the displayed value without sampling either optimisation variable. As an existence criterion this is weaker than the 13/25 theorem. Its different content is the control of the two straight segments from the specified critical point, rather than a curve selected by area averaging. For z5b it requires |b|1/M5, so it excludes part of a binomial family already covered by the trinomial theorem. No claim is made that every quintic has a critical value below this level.

A near-regular pentagon illustrates why a prescribed joining point is restrictive. For sufficiently small ϵ>0, set

Pϵ(z)=z5+ϵ5z4+ϵ3z3ϵ3z2ϵ5z1,Fϵ(z)=r5Pϵ(z/r),r=1ϵ9.

All five roots of Fϵ lie in the open unit disc, approach a regular pentagon, and have escaping segments from the origin. Here is a proof of that assertion, including the effect of the radial contraction.

The roots of Pϵ are simple perturbations ζϵ=ζ0+O(ϵ3) of the fifth roots of unity. The identity

z5Pϵ(1/z)=Pϵ(z)

makes the roots invariant under conjugate inversion. Uniqueness of the root near each ζ0 therefore forces |ζϵ|=1. The roots rζϵ of Fϵ consequently have modulus r<1. The displacement estimate follows from the implicit function theorem at each simple root of z51, since the first coefficient perturbations have order ϵ3.

For ζ0=1,e4πi/5,e4πi/5, take t=ϵ/4. Substitution into the polynomial gives

|Fϵ(rtζϵ)|2=1+(ζ0281512)ϵ5+O(ϵ6).

The coefficient is positive, since ζ02(51)/4. For the remaining roots, with ζ0=e2πi/5 or e2πi/5, take t=ϵ2/4 instead. Then

|Fϵ(rtζϵ)|2=1+35532ϵ7+O(ϵ9)>1

for sufficiently small ϵ. The two scales are needed because ζ02 is negative for this second pair; its positive linear contribution dominates at the smaller scale. Multiplication by r10=1+O(ϵ9) cannot remove either positive leading term. The remainders are uniform over the five root branches, so one sufficiently small ϵ works for every segment. This is an ordinary asymptotic proof; it gives no numerical upper bound for the permitted ϵ.

The addendum [26] reports the stronger assertion that no critical point of this family supplies two contained straight arms of total length at most 2. That proof is not supplied with this record and was not available for checking in this revision. The origin calculation above does not prove it: Pϵ(0)=ϵ5 shows that the origin is not a critical point. The stronger reported assertion is not used in any theorem here. Neither the proved failure at the origin nor the reported critical-point obstruction excludes curved inverse images of rays or a different joining point.

A different local question allows a freely chosen, noncritical vertex: for some δ>0, does every monic quintic with open-disc roots within δ of a rotated regular pentagon admit two contained straight arms through some hC of total length below 2? Neither the origin nor a critical point is prescribed in this question. The sufficient low-critical threshold preceding this paragraph is unchanged.

Area of a connected sublevel set.

The following calculation applies in every degree n2, independently of the degree-five segment criterion. Let f be monic of degree n and let t>0 with Kt={|f|t} connected. Translate its root centroid to 0, so f(z)=zn+cn2zn2+, and let ψ be the exterior map normalised at infinity with positive leading coefficient. For a regular connected lemniscate, the identity f(ψ(ζ))=tζn is after scaling the value level. The following argument also permits critical boundary points. The exterior Green functions (log|f|logt)/n and log|ψ1| agree: both vanish at the boundary and have a logarithmic pole of coefficient one at infinity. Comparison there gives the leading coefficient t1/n for ψ. The quotient f(ψ(ζ))/(tζn) has constant modulus one and limit one at infinity, proving the polynomial identity. Its ζn1 coefficient forces the constant Laurent coefficient of ψ to vanish. Thus

ψ(ζ)=t1/nζ+k1akζk.

Grönwall’s area identity takes the form

Area(Kt)=π(t2/nk1k|ak|2).

One can obtain it directly without assuming that level t is regular. For r>1, Green’s area formula on the analytic Jordan curve ψ(reiθ) gives the enclosed area π(t2/nr2k1k|ak|2r2k). These enclosed compact sets decrease to Kt as r1; continuity of area from above and monotone convergence of the series give the identity. Comparing the coefficient of ζn2 in the exterior identity now gives

nt(n1)/na1+cn2t(n2)/n=0,a1=cn2nt1/n.

The nonnegative coefficient sum quantifies the loss from Pólya’s upper bound. It does not by itself control an internal path length. No analogous coefficient formula for an individual component of a disconnected sublevel set is established here. The degree-five statements and their evidence classes are recorded in the degree-five estimates and their proofs.

Numerical tests of selection by the smallest critical value

Three examples distinguish critical-value bounds from path-length bounds. For a critical point c whose two inverse arms over [0,f(c)] reach roots, write Lf(c) for their total length. The first computation tests the rule of choosing the critical point with uniquely smallest value modulus. The source gives an unnormalised quintic f0, a selected critical point c0, and the numerical values

Lf0(c0)2.057343275393654508,R1.021393477405696164,

where R is the radius of a smallest disc containing the roots of f0. The first number is not the length after normalisation to the unit disc. If h is the centre of that disc, set

F(z)=R5f0(h+Rz).

This preserves monicity, sends the roots into the closed unit disc, and divides every corresponding curve length by R. The reported normalised values are therefore

LF(c0hR)2.01425143287505,|F(c0hR)|0.899569245.

A further contraction uses Fs(z)=s5F(z/s), with 0<s<1: roots and curve lengths are multiplied by s, and critical values by s5. Thus the reported excess would persist for s sufficiently close to 1, with roots in the open unit disc.

These are numerical observations, not a certified counterexample. A small residual at a computed fibre root does not enclose that root or establish its membership in the tracked inverse branch. The inscribed-polyline comparison needs both facts before it gives a rigorous lower bound for the intended arms. Another critical point supplies a shorter pair in the reported computation; this is evidence at that configuration, not a universal selection theorem.

Second, the linked record reports numerical violations of cLf(c)2(n1)R in degrees four and five. Here R is the radius of a smallest disc containing the roots. The quartic computation gives cLf(c)=6.006352157 against the proposed bound 6. Several differential-equation solvers agree, and an inscribed-polyline calculation using numerically computed fibre roots gives a similar excess. These checks do not provide rigorous enclosures for those roots, their branch assignment or the resulting length lower bound. They are evidence against the aggregate inequality, not a certified refutation or a proof that an open set of polynomials violates it. Its algebraic factor

k=1n1|f(ck)|1/n(n1)R

is proved for every n2 in Theorem 8.1. The value estimate alone supplies no bound for the associated path-length sum. The algebraic theorem therefore remains useful independently of how the numerical aggregate examples are resolved. The two computational records, to be read with the evidence limitations just stated, are the numerical test of selection by the smallest critical value and the comparison between sums of critical values and path lengths.

Third, all five origin segments can escape even when the roots are arbitrarily close to a regular pentagon. The two-scale calculation above proves this for the family Fϵ attributed to the earlier note [26]; an isolated numerical example would not prove the assertion for arbitrarily small defects. Failure for every critical joining point is a different, stronger claim, reported in the addendum but not established by the origin calculation. No conclusion about curved inverse-ray paths or an arbitrary connector follows from either straight-segment assertion.

Limits of contained paths at fixed degree

The compactness argument used in Section 17 of the short note is given here in full. It concerns arbitrary contained curves, not a prescribed pair of inverse rays.

Fix n2, and let Kn be the compact coefficient class of monic degree-n polynomials with roots in the closed unit disc. Define

Λ(f)=infγlength(γ),

where γ{|f|1} joins two different listed root occurrences. A repeated root permits a constant curve; an empty set of competitors has infimum +.

Passing a length bound to a limit.

Let fjf in Kn. If the lower limit of Λ(fj) is finite, pass to a subsequence on which these infima converge to it and choose rectifiable curves γj with lengths at most Λ(fj)+1/j. Every closed unit sublevel lies in |z|2: for |z|>2, the root factorization gives |fj(z)|(|z|1)n>1. Constant-speed parametrisation on [0,1] therefore gives uniformly bounded images and Lipschitz constants. Arzelà–Ascoli supplies a uniformly convergent subsequence.

To retain the endpoints with their multiplicities, list the two chosen occurrences first among the roots of fj, and list the remaining roots arbitrarily. Compactness of the product of n closed unit discs gives a further subsequence on which this entire list converges. The limiting factorization is f, so its first two entries remain two occurrences, even if their locations coincide. Uniform convergence of the curves and of the polynomials on |z|2 gives |f|1 on the limiting curve γ. For any partition 0=t0<<tM=1,

=1M|γ(t)γ(t1)|=limj=1M|γj(t)γj(t1)|lim infjlength(γj).

Taking the supremum over partitions proves the required lower semicontinuity of length and hence Λ(f)lim infjΛ(fj). An infinite lower limit needs no argument. With f fixed, the same compactness proof shows that a finite infimum is attained. Thus a bound Λ2 on a dense class gives an actual path of length at most 2 throughout Kn. For an open-disc polynomial, choose a containing disc of radius 0<R<1 and scale: the resulting path has length at most 2R<2 and lies in {|f|Rn}{|f|<1}.

For f(z)=zn1, the inequality |zn1|1 implies 2(zn)|z|2n>0 whenever z0. Thus the punctured sublevel lies in n disjoint angular sectors, one per root. A path between different roots must pass through zero and has length at least 2 by the triangle inequality. The two radial segments attain that length. The corresponding historical assertion on the closed class is

Λ(f)Λ(zn1)=2(fKn).

The lower-semicontinuity argument is proved in the compactness proof.

The displayed universal inequality is recorded to explain the earlier reduction, not proposed here as a remaining open assertion. A counterexample to the original problem would also refute this inequality and, by the same compactness argument, any dense-class estimate implying it. The reduction can still be used for separately specified polynomial classes.

Blaschke-product examples and limits in varying degree

The following family separates the limitations of the sufficient conditions from bounds for the actual shortest contained path.

The ordinary note on powers of Blaschke products uses the degree-2N polynomials

FN(z)=[z(z+b)]N(1+bz)N,N1,0<b<1,

and their radial contractions. Its finite rational certificates and its asymptotic proofs have different roles. The degree-eight certificate excludes an unconditional critical-value exponent 8/7. It does not contradict the ordinary exponent 4/7 proved by the Poisson argument above, or the smaller exponent 2/7 in the cited Lean theorem. For N2, the root centroid of FN is b/2, as its z2N1 coefficient is Nb. A radial contraction by r>0 changes this to rb/2, not zero. Thus the degree-eight example does not satisfy the additional centroid condition that permits numerator 8 above. The degree-twenty-four certificate gives critical values in |v+1|<1/12, so μ>11/12 while every radius-4/3 separation test fails. These fixed-degree examples do not establish optimality uniformly in degree. That conclusion uses the limiting measures in Sections 2–3 of the linked full proof.

For b=λ/N with fixed 0<λ1, Section 4 constructs connectors of length at most [log(2/λ)+π+o(1)]/N. The two radial pieces reduce the oscillatory term; a short circular arc then joins them in a sector where the remaining factor has modulus below one. The unspecified starting degree depends on λ. For b=eαN/N with fixed α>0, the same section instead proves Λ(FN)2(1eα/2) for the uncontracted polynomials FN displayed above and the closed-level functional defined earlier. The second assertion is a separate argument, not a substitution of a varying parameter into the first. Both are ordinary asymptotic arguments, not consequences of the finite certificates or formally checked analytic theorems. They concern varying degree and do not contradict fixed-degree compactness or prove the unrestricted assertion.

What the earlier inverse-ray approach would have required

The earlier proposed sufficient condition concerned curved inverse images of rays, not straight segments. On a generic ray-separated class let Lf(c) be the length of the two-root descent arc at an admissible critical point, where |f(c)|1. Then

minc admissibleLf(c)2

would imply the root-connector conclusion by the stated compactness argument. The unrestricted infimum over all contained curves can be smaller; equality of these two optimisation problems is not assumed. The obstruction to two straight segments through a critical point does not by itself prove or disprove this curved-arc estimate. Examples in which another critical point gives a shorter curve do not prove the estimate universally. The critical value bound, containment and length bound must hold for the same curve. The displayed universal inequality is recorded as a historical sufficient condition, not proposed as an open assertion: a counterexample to the original question would refute it as well. The reduction remains useful on separately specified polynomial classes.

The Newton value equation

Sutherland uses the term Newton flow for z˙=f(z)/f(z) and notes that its solution curves map under f to radial lines [6]. The value equation [7] determines their orientation and time parametrisation. The global Newtonian graph , described with its endpoint conventions below, is a separate input to the inverse-sheet discussion in Section 11.

A Newton trajectory is a differentiable curve satisfying

z(t)=f(z(t))f(z(t))

where f(z(t))0. Let IR be an interval on which these assumptions hold; put w(t)=f(z(t)). Kozen and Stefánsson record the following identity as a lemma of Shub, Tischler and Williams .

Theorem 9.1 (value equation). Let f be a polynomial and z:IC a differentiable curve on an interval I, with f(z(t))0 and z(t)=f(z(t))/f(z(t)) throughout I. For w=fz, one has w(t)=w(t) on I.

The computation is one line: w=f(z)z=f(z)(f(z)/f(z))=f(z)=w. The kernel checks the local complex-parameter chain rule as the derivative of the polynomial value along a Newton trajectory, together with the differential form of the first integral, the derivative of the exponentially rescaled value:

ddt(etf(z(t)))=0.

Equivalently,

f(z(t))=e(tt0)f(z(t0)),t0t,t0,tI.

Integration on the real interval gives the last identity as an ordinary consequence of the differential equation. For an existing trajectory with nonzero initial value, its value moves inward on one positive ray; a zero value has no argument and remains zero. Thus |f|<1 is preserved for later times in that trajectory’s existing interval. No global existence or description of a whole ray preimage follows from this scalar equation. The real-time candidate endpoint is the real-time value equation in the real-time trajectory source.

Corollary 9.2 (ray separation). Let a<b and let the value trajectory tf(z(t)) be continuous on [a,b]. Assume the Newton equation and f(z(t))0 on (a,b) only. Then

f(z(b))=eabf(z(a)).

If these endpoint values are nonzero, they lie on one positive ray. Therefore critical points with values on distinct positive rays cannot be endpoints of such a finite connection. The trajectory in the z plane need not be radial.

The interior identity passes to the endpoints by continuity, not by evaluating f/f at a critical endpoint. The candidate declarations value decay at continuous endpoints and no finite connection of distinct value rays in the trajectory endpoint source make these premises explicit. Their compilation and axiom checks are not reported here. They construct no trajectories and supply no global monodromy theorem. Kozen and Stefánsson draw the same ray consequence for the Newtonian graph: under f, every edge maps onto a segment of a ray through the origin whose endpoints are 0 or critical values .

Arguments, not moduli

It is tempting to arrange a generic perturbation so that the critical values are pairwise distinct, or that their moduli are pairwise distinct, and to conclude that saddle connections are excluded. Neither is enough.

Along a Newton trajectory the argument of f stays constant while its modulus decreases. By Corollary 9.2, arranging pairwise distinct arguments of the nonzero critical values is therefore a sufficient way to exclude finite connections between critical points. It is not asserted to be necessary. This condition imposes no lower bound on the distances between critical values and no upper bound on their moduli.

The weaker conditions really can coexist with a connection, even when all roots lie in the open unit disc. Take

f(z)=z3316z+364.

On |z|=1, the lower terms have total modulus at most 15/64<1, so Rouché’s theorem places all three roots inside. The critical points are 1/4 and 1/4, with distinct positive values 5/64 and 1/64. On the intervening real interval f is positive and strictly decreasing. The equation

f(x(t))=564et,0<t<log5,

therefore defines a differentiable path with x(t)=f(x(t))/f(x(t)). Its endpoint limits are 1/4 and 1/4. It is an actual critical-to-critical Newton trajectory, not merely a pair of values on one ray. The time convention is that of the value equation ; the singular field is not evaluated at the endpoints.

A common translation of distinct values can separate their arguments. The next calculation describes the translations to avoid.

Theorem 10.1 (ray-collision locus). Let ab be complex. Every common translation β for which a+β and b+β lie on the same positive ray has the form

β=rab1r,rR>0, r1.

Indeed, write b+β=r(a+β) with r>0. Since ab, one has r1, and solving for β gives the displayed formula. Equivalently, β=a+(ab)/(1r), so the forbidden translations lie on the real affine line through a and b.

The formula is checked as translations that put two values on one ray. A finite union of these loci has empty interior. Adding a constant to f translates all critical values by that constant and leaves the critical points unchanged. Section 13 records the formal avoidance and root-retention estimates. A constant cannot separate equal critical values; coefficient perturbation and control of the remaining geometric margins are separate requirements.

Why the proposed spanning-tree estimate fails

Recent work on polynomial lemniscates separates component counts from metric path questions. Ghosh and Ramachandran record that the open set {|f|<1} has 1+#{j:|f(cj)|1} components, where c1,,cn1 are the critical points listed with multiplicity [5]; the underlying component-wise Riemann–Hurwitz count appears in the proof of [8]. For the binomial family zna, the condition |a|<1 therefore puts the filled unit lemniscate in the connected regime. Connectedness alone gives no path-length bound. Bishop, Eremenko and Lazebnik describe the possible shapes: every rational lemniscate is a lemniscate graph whose vertices are the critical points on the level set, each of even degree at least four [20], and a lemniscate graph is realised by a polynomial lemniscate up to a homeomorphism of the plane exactly when it is the boundary of its unbounded face . This topological description also gives no path-length bound.

The March manuscript’s Proposition 12 claims the following estimate. For u=log|f|, a connected component V of {u>c} carrying m2 simple zeros, and the regularity and Morse hypotheses in that proposition, it constructs, for every ε>0, an embedded spanning tree GεV with

(5.1)len(Gε)12π2αPV(t)dt+ε.

Here PV(t)=H1(V{u=t}) is the length of the level set in V, and α>0 is the truncation parameter in the proposed estimate. The final theorem depends on this bound.

The estimate itself is false. Take fa(z)=z2a2 with a=9/10 and choose 2α=loga. For 0<c<α/2, the component V of {log|fa|>c} contains {|fa|a} and both roots. The only critical point is a nondegenerate saddle at 0; distinctness of critical values is vacuous.

Here the level-length integral can be bounded directly. Put r=et. On a regular level the inverse parametrisations z=±a2+reiθ give

PV(t)=r02π|a2+reiθ|1/2dθ.

The elementary identity

|a2+reiθ|2=(a2+r)2cos2(θ/2)+(a2r)2sin2(θ/2)

implies

|a2+reiθ|1/2(a2+r)1/2|cos(θ/2)|1/2.

The angular factor has mean at most 2. Indeed, symmetry reduces its integral to 40π/2(coss)1/2ds, and coss12s/π bounds the latter integral by 4π. Changing variables from t to r therefore gives

12π2αPV(t)dt20adra2+r=4(a2+aa)<4125.

The isolated critical level is handled by the corresponding improper integral. Every connected set containing both roots has length at least 2a=9/5. Since 9/541/25=4/25, any 0<ε<4/25 contradicts eq:prop12-bound. Thus neither a different local saddle neighbourhood nor a perfect topological decomposition can recover the printed coefficient 1/(2π). Lean checks the exact numerical inequality and the resulting contradiction for a tree-length bound. The level-length majorant remains an explicit analytic input; the integral evaluation is not checked by that formal proof.

At an interior index-one critical point p, the proof invokes a Morse chart

u=u(p)+x2y2

and replaces the saddle by a three-ended neighbourhood having one connected lower cross-section and two connected upper cross-sections. That local model is false as written. Because pV and V is open, a sufficiently small closed disc around p lies entirely in V. In that disc the full Morse chart has four sectors: two components of u>u(p) and two components of u<u(p). The level set {u=u(p)} is a lemniscate graph with a vertex of degree four at p . A global component argument cannot delete one local sector from a disc already contained in V.

This independently diagnoses a proof step, but the Cassini witness above also refutes the proposition’s printed metric statement. A different route might cut an adjoining regular annulus along a separatrix or regular flow arc before forming the block, retain a four-pronged saddle neighbourhood and change the assembly, or replace the local construction by the ray-cut decomposition proposed below. But no repair can retain eq:prop12-bound; it must pay a positive attachment cost, select only one short pair instead of spanning every root, or use a different global metric inequality. The shorter descriptions of the same three-ended block do not repair the four-sector topology.

There is an ordinary topological theorem when the critical values have pairwise distinct arguments and moduli, and the critical points are simple. Its ingredients are classical: the Newtonian graph of Shub, Tischler and Williams [7], the component-wise Riemann–Hurwitz count in the proof of [8], and the division of the Riemann surface of the inverse function into sheets by outward critical-value slits. Dubinin describes the sheet adjacency tree directly in and uses a related network for capacity in [9]. The latter paper assumes bounded critical values and controls capacity; it does not supply a Euclidean tree-length bound. The theorem below specifies the sheets, critical transpositions and descent arcs for the stated component.

The assumptions exclude a component containing a multiple critical point or two critical values on the same ray. For znb with n>2 and 0<|b|<1, the component containing the origin fails the first condition. They hold, for example, for f(z)=z3(3/25)z+1/500: its critical points are ±1/5 and its critical values are 7/500 and 9/500. On the unit circle the two lower terms have total modulus at most 61/500<1, so all three roots lie in the open unit disc by Rouché’s theorem. In the statement, “excellent” means that the critical levels of the Morse function are pairwise distinct. This regularity permits a decomposition into sheets; it does not bound the total length of the resulting tree.

Theorem 11.1 (inverse sheets with distinct critical-value arguments). Let f be monic, and let U be a component of {|f|<1} containing k2 roots, counted with multiplicity. Suppose every critical point of f in U is simple, its critical value is nonzero, and these critical values have pairwise distinct arguments and pairwise distinct moduli. All preimages and sheets below are taken inside U, and only critical points in U determine the cuts. Then:

  1. log|f|:U\f1(0)(0,) is a proper excellent Morse function, with exactly k1 nondegenerate saddles;

  2. cutting D{0} along the critical-value rays decomposes its preimage in U into conformal strips;

  3. cutting each ray only from its critical value to the unit circle gives k conformal sheets, one per root, whose critical transpositions form a tree;

  4. for each critical point cU, the two inverse lifts of [0,f(c)] join two roots through c inside U{|f||f(c)|}, and the union of these arcs is an embedded geometric realisation of that tree.

Small neighbourhoods of the saddles can be chosen with diameter O(δ) at value radius δ.

Proof. The map f:UD is proper of degree k, and U is simply connected. To apply the count from the proof of [8] only at a regular level, join all roots and critical points in U by finitely many compact paths in U. Choose a regular t<1 above the maximum of |f| on their union. One component of {|f|<t} then contains exactly the roots and critical points of U; Riemann–Hurwitz there gives k1 simple critical points. No regularity of the level-one boundary is needed. The holomorphic Morse lemma makes these points nondegenerate saddles of log|f|, and their distinct moduli separate the critical levels. A compact range in (0,) stays away from both the level-one boundary and the deleted roots, proving properness of the Morse function.

Remove 0 and the rays determined by these k1 values. Each remaining sector is simply connected and contains no branch value of f:UD, even if it contains critical values coming from outside U. Each component of its preimage in U maps biholomorphically to the sector. If the sector has angular range (θ1,θ2), the holomorphic coordinate logf maps this component onto the semi-infinite strip

{x+iy:x>0, θ2<y<θ1}.

Thus its real coordinate is log|f|, while its imaginary coordinate is argf. The minus sign in both coordinates is needed for a holomorphic map; keeping +argf would reverse orientation.

For the sheet tree, remove only the outward slits {tf(c):1t<1/|f(c)|}, for critical points cU. The remaining value domain is star-shaped about 0, hence simply connected, and its preimage in U splits into k sheets labelled by the roots. Local monodromy at each slit endpoint is a transposition of two of these sheets. Deleting the finitely many fibres over the branch values from U leaves a connected domain, so the monodromy action is transitive. The k1 transpositions therefore give a connected graph with k vertices, which is a tree.

For cU, the inward segment from f(c) to 0 contains no other branch value of f:UD, by the distinct-argument hypothesis. Distinct moduli were needed only to separate the Morse levels. Its two inverse lifts converge to c by the holomorphic Morse coordinate and start at the two root labels exchanged by its transposition. These labels are distinct, as are the roots, because a root in U cannot also be a critical point under the nonzero-critical-value hypothesis. Lifts belonging to different critical points cannot cross away from roots, since an intersection would give one nonzero value on two critical rays. Their union is therefore an embedded tree. Each edge is rectifiable: at a simple critical endpoint, parametrising the value segment by its distance s from the critical value gives speed O(s1/2), which is integrable. The root endpoint is regular, and the derivative is bounded on compact subsegments between the endpoints. This proves finiteness of each length, not a uniform bound for it. The same local Morse coordinate identifies a value disc of radius δ with a spatial neighbourhood of diameter O(δ). The constant and the permitted range of δ depend on f and the chosen saddle. Indeed, in the coordinate f(z)f(c)=u2, the inverse map has derivative of modulus 2/|f(c)| at u=0. No bound uniform over degenerating critical points is asserted. For a fixed polynomial there are finitely many saddles, so their individual constants have a finite maximum. ◻

The complete ordinary argument is recorded in the proof of the decomposition into inverse sheets. Its Lean companion checks the ray-distance, averaging and finite-tree kernels; it explicitly does not formalise Riemann–Hurwitz, monodromy, the strip diffeomorphisms or the geometric assembly. The theorem supplies topology, not a useful length sum: the canonical inverse-ray tree can already have the Cassini deficit discussed above.

The component restriction cannot be dropped. For example, take

f(z)=(z24)214.

Its critical points are 0,±2, with values 63/4,1/4,1/4. The positive roots 7/2 and 9/2 lie in one component U: on the intervening real interval, 1/4f0. But f(iy)=(y2+4)21/4>1 for real y, so this component cannot contain the negative roots or 2. Its only critical point is the simple point 2. Thus the theorem applies in U, although the other component has the same critical value. This example concerns component topology; no root-unit-disc hypothesis is imposed here.

Corollary 9.2 also excludes finite saddle-to-saddle Newton connections inside U. The theorem does not treat coincident arguments, simultaneous critical levels or multiple saddles in that component. Nor does it identify a slit domain with the quotient by all trajectories: the quadratic example following Problem 13.5 satisfies its hypotheses but has a non-Hausdorff orbit quotient. Boundary tangencies and quantitative strip attachment remain separate questions. The embedded tree supplies no length bound for the historical question.

Numerical path searches

A search was run over random monic polynomials with roots in the unit disc. For each sample the region {|f|<1} was rasterised and shortest grid paths were computed between every pair of roots. The reported grid distances were

degree 5,500 trials:1.1052648928degree 6,1500 trials:0.8450414343degree 8,1500 trials:0.6203916714degree 10,1500 trials:0.4303640486.

No counterexample candidate was found, and the measured values sit well below the threshold 2. These are numerical candidate connectors. A polygon whose vertices satisfy |f|<1 need not lie in the open lemniscate, since an edge can cross the boundary between two safe vertices, and root snapping adds further edges of the same kind. Turning a candidate into a proof needs a continuous certificate on every edge, for instance strict positivity of the real polynomial 1|f(z(t))|2 on [0,1] for each straight edge z(t)=u+t(vu), established by exact coefficients or outward-rounded interval arithmetic with subdivision, together with exact root enclosures. No such certificate is attached to the numbers above. They are grid distances for the sampled configurations, and the apparent decrease with degree is a property of the sample, from which we draw no conjecture. Even a finite collection of proved instances would not establish the universal statement. These searches also cannot adjudicate a counterexample reported elsewhere. Useful stress tests for particular path constructions include near-degenerate saddles, thin necks, boundary-critical configurations, and almost-connected separatrices. They should report those diagnostics. Raster paths remain candidate finders, never continuous certificates.

Further questions about topology, length and perturbation

The questions below separate topological, metric and perturbative steps of earlier arguments. They are retained for their own content, not as a claim that completing them must prove the unrestricted historical assertion. A counterexample or a necessary additional hypothesis can be as informative as a positive theorem.

1. Local saddle geometry and the refuted tree estimate

Problem 13.1 (corrected local saddle assembly). The printed 1/(2π) spanning-tree estimate of Proposition 12 is false: the Cassini polynomial z2a2 at a=9/10 makes the proposed tree budget strictly shorter than the distance between its roots. Any later argument must pay a positive attachment cost, select only one short pair instead of spanning every root, or use a different global metric inequality. A four-pronged or cut-annulus local model may still be useful for another estimate, but it cannot recover eq:prop12-bound.

The full-disc model x2y2, an annulus in which lower branches rejoin, two saddles joined by a separatrix and simultaneous saddle levels are mandatory tests. Repeating the one-lower/two-upper assertion does not answer the problem.

2. Cutting a compact region into flow strips

Let p be a polynomial with simple roots and simple critical points, and set u=log|p| away from the roots. Simplicity of the roots makes every critical value nonzero; critical points themselves may lie at 0. For regular values c<T, let V be a component of {u>c} and assume that V{c<u<T} is a compact genus-zero surface, its lower boundary is one smooth Jordan curve, its upper boundary consists of m smooth level curves each enclosing one root, all interior critical points are nondegenerate index-one saddles, the normalised gradient field, defined away from the saddles,

X=u|u|2=pp,

is transverse to the level boundaries, and no maximal X-trajectory has two saddle endpoints. The equality uses the identification of a planar vector with a complex number: u=p/p. In particular, du(X)=1 wherever X is defined.

Problem 13.2 (finite strip decomposition after ray cuts). For every η>0, construct disjoint Morse neighbourhoods Nj with jdiamNj<η and a finite set of complete separatrix or regular-flow cuts so that the closure of each remaining component in the cut-open surface is flow-diffeomorphic to a rectangle

[aS,bS]×[0,1],u=t,

with connected level sections and no uncut annular component. Give an explicit finite bound for the number of strips in terms of the number s of saddles and the number m of upper boundary curves, or exhibit the minimal missing hypothesis or a counterexample.

No particular formula such as 2s+1 is presumed. Boundary tangencies, simultaneous levels and branch reunion through an annulus require explicit cuts. The closure is taken in the cut-open surface, with its separate boundary copies, not after regluing them in the plane. The quadratic example following Problem 13.5 explains why replacing this construction by the ordinary orbit quotient would fail.

3. Length estimates for joining flow strips

For a strip S, write

ΓtS=S{u=t},PS(t)=H1(ΓtS),

and write

ΦS(t)=ΓtS|u|ds

for its transverse flux. On a regular sub-band, u is harmonic and the side boundaries are flow lines. The divergence theorem therefore makes ΦS(t) independent of t. Normalise the transverse measure by

dμt0(x)=|u(x)|ΦS(t0)ds(x).

The choice of measure is determined by the length calculation. Since u=t along the normalised flow, its Euclidean speed is 1/|u|. Transporting the flux measure to level t therefore gives

Γt0Slen(γx)dμt0(x)=aSbSΓtS1|u||u|ΦS(t0)dsdt=1ΦS(t0)aSbSPS(t)dt.

Here 0<ΦS(t0)< for a nonempty regular strip. Tonelli’s theorem applies to the nonnegative integrand. At a critical endpoint level, exhaustion through regular sub-bands gives the same identity, allowing the common value to be infinite. A finite right side gives a trajectory of length at most that mean; an identity with both sides infinite gives no length estimate. A strip flux need not be an integer multiple of 2π. For f(z)=z and u=log|z|, take an annular sector of angular width θ. On a circular level arc, |u|=1/r and ds=rdϕ, so its flux is ΦS=θ. For f(z)=zn, the same calculation gives ΦS=nθ. A closed regular level curve enclosing k roots has flux 2πk by the argument principle. Restricting it to a strip replaces that full winding by the strip’s share of the flux. The averaging measure therefore depends on the width of the strip. Summing separate strip estimates cannot replace those widths by the winding number of a closed level curve. They do not reopen eq:prop12-bound. Cassini already excludes the printed coefficient 1/(2π) for any embedded tree that contains all m roots: Problem 13.1 records that no later gluing argument can retain that estimate.

Problem 13.3 (strip gluing after the printed coefficient). Assuming Problem 13.2, do one of the following, for every η>0.

  1. Produce an embedded tree G containing all m roots whose length obeys

    (6.1)len(G)C2αPV(t)dt+η

    for an explicit constant C>1/(2π), uniform over a stated class of polynomials and an explicitly restricted range of truncations α. The restrictions must account for attachment cost and for a valid allocation of the strip fluxes ΦS.

  2. Connect only one pair of distinct roots, rather than spanning every root.

  3. Give a different global metric inequality that is not eq:prop12-bound.

The printed coefficient 1/(2π) is not an open target. Better additive control of saddle, annular-cut and root-cap cost cannot recover eq:prop12-bound.

The restriction on α is essential in the first alternative. For a fixed f(z)=z2a2, with 0<a<1, choose 0<c<2loga and let V be the component of {log|f|>c} containing both roots. At sufficiently deep levels, the Cassini parametrisation used above gives

PV(t)2πeta2et.

Consequently 2αPV(t)dt0 as α, whereas every spanning tree has length at least 2a. No fixed C can cover arbitrary truncations. This is a limitation of the unrestricted formulation of (6.1), separate from the earlier counterexample to the particular coefficient 1/(2π).

The printed collar slack

q=12πα2αPV(t)dt>0

used the same excluded coefficient. It is not an unused error allowance in an otherwise complete spanning-tree estimate. Independently choosing a shortest trajectory in each strip is not enough unless the attachment mismatch is controlled, and controlling that mismatch does not restore the printed 1/(2π) tree bound.

4. Coefficient perturbation and stability

The constant-translation stage is no longer open. Once a finite critical-value family is injective, Lean proves an arbitrarily small translation making every value nonzero and pairwise positive-ray separated (a small translation separating the arguments). It also proves the explicit root-retention estimate: for a monic polynomial f of degree n1, a constant shift of modulus below ε>0 keeps all roots in the unit disc provided

((n+1)ε)1/n+maxf(b)=0|b|<1

(the root-retention estimate for the unit disc). Adding a constant leaves the difference of two critical values unchanged, so it cannot separate values that were equal to begin with.

For a constant shift alone, factorisation gives the sharper elementary bound

(f+β)(z)=0f(b)=0|zb|=|β|minf(b)=0|zb||β|1/n,

where the product counts roots with multiplicity. Hence maxf(b)=0|b|+|β|1/n<1 already ensures retention in the open unit disc. The factor n+1 in the recorded Lean estimate is not needed for this ordinary constant-shift argument. The coefficient one in the displacement bound is optimal, as f(z)=zn shows. The estimate does not match labelled root lists or bound the cost of transporting an existing curve.

Qualitatively, a small linear perturbation also supplies distinct critical values as well as simple critical points. For degf2, a multiple critical point of f+λz must satisfy f(c)=0 and λ=f(c); only finitely many parameters are excluded. Near any other parameter, label the distinct critical points by holomorphic functions cj(λ). Their values

vj(λ)=f(cj(λ))+λcj(λ)satisfyvj(λ)=cj(λ).

Thus vivj cannot vanish identically for ij, and its zeros are isolated. Avoiding the finitely many pairs in a sufficiently small parameter neighbourhood gives simple critical points with distinct values. The neighbourhood can be chosen inside any prescribed disc about λ=0, proving the required arbitrarily small choice.

If distinct moduli are also needed for the excellent Morse function, the translation β can avoid them at the same time as the ray collisions. For each distinct pair vi,vj, the equality |vi+β|=|vj+β| is the real affine line

2((vivj)β)=|vj|2|vi|2.

For ray separation it is enough to avoid, for each pair, the real line through vi and vj: the ray-collision formula puts every forbidden translation on that line. Avoid also the finitely many points vj to keep the translated values nonzero. Thus the full excluded set is contained in two real affine lines per pair of critical values, together with finitely many points. Its complement meets every open disc, so imposing distinct moduli costs no lower bound on the size of the perturbation. Root retention is also qualitative: choose a circle |z|=R<1 enclosing the original open-disc roots. If |λ|R+|β|<min|z|=R|f(z)|, Rouché’s theorem keeps all roots of f+λz+β inside that circle. These ordinary arguments establish genericity and root retention; they do not estimate the collar or the cost of transferring a selected curve. The first two requirements below therefore have qualitative proofs, while their simultaneous quantitative use is the remaining task.

For the next problem, fix a specified valid replacement for the refuted metric inequality. Its slack is the difference between the permitted length and the bound supplied by that replacement. The symbols q and qg refer to this same specified quantity for f and g, respectively; they are not the historical collar integral with coefficient 1/(2π). Without a choice of replacement inequality, the requirement qg>q/2 has no defined geometric content.

Problem 13.4 (two-stage generic perturbation with slack). For fixed root discs, compact collar K, regular levels α/2,α,2α,5α/2, and a specified valid replacement metric inequality with slack q>0 at f, prove that an arbitrarily small

gλ,β(z)=f(z)+λz+β

can be chosen so that:

  1. f+λz has simple relevant critical points and injective complex critical values;

  2. the checked constant translation β makes those values nonzero and pairwise ray-separated;

  3. no critical point enters the protected collar or truncation boundary;

  4. the relevant component remains in K, contains exactly the corresponding perturbed roots and has slack qg>q/2; and

  5. root displacement and straight-line transfer back to the original roots consume less than a prescribed fraction of q/m.

If the one-coefficient perturbation λz cannot ensure all five properties, give the smallest additional lower-coefficient direction that can, or an explicit obstruction.

The cited declarations supply finite planar avoidance and the constant translation. The ordinary argument above additionally supplies a linear perturbation with simple critical points and distinct critical values. What remains for the stated problem is simultaneous control of the protected collar, the component, the quantitative slack and the root-to-root transfer cost. No formalisation of the new genericity argument or solution of those stability requirements is claimed.

5. Newton flow on a compact region between regular levels

Classical Newton-flow theory describes maximal trajectories and the graph they form. Away from the roots and critical points, every orbit satisfies

p(z(t))=e(tt0)p(z(t0)),u(z(t))=u(z(t0))+tt0,u=log|p|,

by the lemma of Shub, Tischler and Williams [7]. For an initial point that is neither a root nor a critical point, the maximal Newton trajectory has one of four endpoint patterns: each finite-time end is a critical point, an infinite forward end is a root, and an infinite backward end is the point at infinity [7]. Stationary trajectories at simple roots are not part of this classification. The maximal nonconstant trajectories with endpoints among the roots and critical points form a connected Newtonian graph with finitely many edges . Critical-to-critical edges are included; pairwise distinct arguments exclude them by the value equation, not by the definition of the graph.

The smooth field needed for Morse theory is not p/p, which is undefined at a critical point with nonzero value. On the root-free band the Euclidean gradient satisfies

u=p/p=|p|2|p|2(pp)(p0).

It has the same oriented nonstationary trajectories as the Newton field, with a different time parameter. At a simple critical point c, its derivative is the real Hessian of u, whose eigenvalues are ±|p(c)/p(c)|. Thus it extends as a hyperbolic saddle there. A finite critical endpoint in Newton time is not a finite arrival at an equilibrium of the smooth field. These two parametrisations must be distinguished in a statement about a Morse–Smale flow.

Problem 13.5 (relative global Newton-flow theorem). Let p be a nonconstant polynomial, let a<b be finite regular values of u=log|p|, and suppose every critical point in the compact band

{z:au(z)b}

is simple, with the critical values in the band on pairwise distinct positive rays. Describe the maximal trajectories of the smooth gradient field u relative to the lower and upper level boundaries, each of which may have several components. Construct a cut-open model by regular flow strips, specifying the separate copies of cut boundaries and the equivalence relation used for its trajectory parameter space. Prove that this parameter space is Hausdorff, or identify the obstruction to the proposed identifications. The ordinary orbit quotient of the uncut band is not required to be Hausdorff. State the boundary convention and the comparison with Newton trajectories through the positive change of time above, without evaluating p/p at its singular points.

The endpoint classification on this band follows from the cited Newton classification and the time change. Each nonconstant trajectory runs from the lower boundary to the upper boundary, from the lower boundary to a saddle, or from a saddle to the upper boundary. Indeed, Newton time equals the change in u, so the part of a Newton trajectory in the band has bounded Newton-time interval. At either end it must meet a regular boundary or tend to a critical point. Ray separation excludes two different critical endpoints, and strict increase of u excludes two ends at the same critical point. In smooth-gradient time, regular boundary crossings occur in finite time, whereas convergence to a saddle takes infinite time by uniqueness for the smooth differential equation. The remaining trajectories are the stationary saddles. This is an ordinary consequence of the classical classification, not an additional checked Lean theorem.

The planar transversality condition also follows from the hypotheses. Along a nonstationary gradient trajectory, the value of p has constant argument, so a trajectory between two different saddles would contradict ray separation. A homoclinic trajectory is excluded by the strict increase of u. The stable-manifold theorem gives local stable and unstable curves tangent to the Hessian eigenspaces. Their global branches for different saddles therefore do not meet; at one saddle they meet transversely, since their tangent lines are the two distinct Hessian eigenspaces. The regular lower boundary is an entrance and the regular upper boundary an exit. With this boundary convention, the gradient satisfies the Morse–Smale transversality condition. This does not make the quotient by entire trajectories Hausdorff.

For an explicit obstruction, take p(z)=z21/4 and the compact band

log2log|p(z)|log8.

Its only critical point is the simple saddle at 0, whose value is 1/4; both boundary levels are regular and ray separation is vacuous. The positive real separatrix, including its upper-boundary endpoint, is

(0,1/(22)],dxdτ=2x1/4x2.

Integration gives ττ0=18log(x/x0)(x2x02)/4, so this trajectory tends to 0 as smooth-gradient time τ. Thus this orbit is not closed in the band: its closure also contains the stationary orbit {0}. In the quotient topology its image is a nonclosed singleton, so the orbit quotient is not even T1, hence not Hausdorff. Reparametrising the nonstationary trajectories leaves this quotient unchanged.

On an actual cut-open flow rectangle, by contrast, collapsing the trajectories gives the transverse interval. Identifying boundary copies is a further quotient and requires a separate separation argument. The Reeb graph uses yet another equivalence relation: it identifies connected components of level sets, not complete trajectories. Neither that graph nor the embedded Newtonian graph can be substituted for the orbit quotient without specifying a new equivalence relation.

The recorded checked algebra gives the pointwise value equation and excludes distinct endpoint rays once the exponential endpoint relation is assumed. The ordinary value-equation proof derives that relation for an existing real-time trajectory, using continuity at critical endpoints; the separate endpoint candidate has no reported compilation here. Global solution theory and the finite graph are the classical results cited above. The relative endpoint classification and transversality are proved above. They do not construct the required finite cut-open space, justify its boundary identifications or control the length needed to join the pieces. The quadratic example settles the uncut-orbit-space question negatively; it does not obstruct a construction that retains the required separate boundary copies.

This record does not establish the unrestricted conclusion of Erdős #1041. Its sufficient conditions have different hypotheses and containment levels: low critical value, separated simple critical value, and the individually proved polynomial families are not a cover of the remaining class. In particular, the scaled (5/2)μ1/n bound is at level (25/13)μ, which is smaller than 2μ; it therefore improves both the constant and the level of the 71/10 construction. The latter is retained for its independent proof and component-sensitive estimates. The critical-value moment does not choose a contained pair. The ordinary generic slit-sheet topology has classical antecedents; the earlier proposed sufficient estimate concerned the lengths of particular inverse-ray curves. Their minimum need not equal the infimum over all contained curves. A reported counterexample to the unrestricted assertion would rule out the corresponding universal estimate for these particular curves too, without invalidating conditional estimates on smaller classes.

Adjacent inverse-map methods.

Crane [22] uses inverse-branch hyperbolic geometry, Dubinin’s radial-slit input and capacity for a derivative-normalised Smale ratio. Dubinin’s four-point result [23] assumes bounded critical values and estimates distortion. These are relevant methods, not direct sources of the present positive moment or connector constant, and their normalisations are not interchangeable with a root-disc hypothesis.

Statements and declarations

Lean checks exact formal statements, not citation choices or mathematical priority. The formal-source index records the complete quadratic weighted inequality, the exponent-2/(n1) critical-value mean, the translated cubic family and the open-disc sparse-quintic path conclusion in its checked build. The fourth-power and higher-moment refinements proved here remain ordinary analytic results. The complete degree-three path also has a release-source proof under monicity, degree three and the open-disc root hypothesis, distinct from the earlier implementation outside that build; its release status is explained above. Finite inequalities do not replace a comparison of the full geometric statements. The analytic path arguments and the research addendum retain the ordinary proof status stated locally. No fresh Lean build or independent mathematical review was performed for this revision.

Acknowledgements

I thank Wouter van Doorn for advice on mathematical exposition, in particular on explaining restrictive hypotheses, avoiding private terminology and introducing notation only when it helps the reader. His remarks concerned another note; this acknowledgement does not imply that he reviewed or endorsed the mathematics of the present paper.

Guide to the formal sources

The formal-source index describes sources at snapshot 6b78209ab63a. The links below retain their earlier commits and line numbers. The index distinguishes complete statements in its recorded checked build from implementations present outside that build.

No source-link reachability check or fresh kernel build is implied by these snapshot links. The original paper-wide commit macro is retained for legacy links; newer target links name their own snapshot explicitly.

Numerical estimates for the packing inequality

This appendix records numerical estimates for the packing argument in Theorem 3.1. The short paper does not depend on the floating-point comparisons below. Those comparisons are not certified upper bounds; the separate table of certified lower root counts is identified as such. The computations indicate where particular relaxations lose strength in the displayed range 13/25<μ<1. This is not an uncovered interval: the rigorous comparison above also covers μ529/1000. The floating-point comparisons neither enlarge that certified range nor assert the historical path bound throughout the rest of the interval.

At a=1 the constants of the failure inequalities have the rounded values δ0.4586751, D5.3770730, and dlow2.1700770; the identity cosh(D/2)=e2 is exact. The quantity being estimated is jλ(dj) for k roots at this fixed area, not a Euclidean path length. The four columns compare the earlier bound

max{δ2+(k1)λ(Ddlow),kartanh(e2)},

where λ(d)=logtanh(d/2) as in Section 3; the hyperbolic packing bound used for the earlier threshold 2/5; the linear-programming value Mcirc of the relaxation of Lemma 3.3; and the largest reported objective value at a numerically constructed configuration. The last column is a search result, not a certified feasible value or a proved optimum.

k earlier bound packing Mcirc search
2 0.3103 0.5899 0.3102 0.3103
3 0.4085 0.6878 0.3893 0.3784
4 0.5447 0.7475 0.4450 0.4306
5 0.6809 0.7906 0.4846 0.4694
6 0.8170 0.8244 0.5155 0.4986
7 0.9532 0.8521 0.5408 0.5208
8 1.0894 0.8757 0.5622 0.5413
10 1.3617 0.9142 0.5972 0.5759
14 1.9064 0.9710 0.6487 0.6228
20 2.7234 1.0298 0.7022 0.6717
30 4.0851 1.0955 0.7624 0.7283
100 13.617 1.2871 0.9428 n/a

Both right-hand columns come from floating-point searches. In addition, Mcirc uses a 2600-point d-grid and a 1400-point r-grid. Restricting the allowed d values and checking only finitely many circle constraints have opposite effects on the feasible set. Without a separate continuous feasibility or dual certificate, the computed value is not a proved lower or upper bound for the continuous relaxation. At k=2, the grid value 0.31018 differs from the analytic value, approximately 0.310338. Their proximity supplies no rigorous bracket.

The certified lower bounds for k, rounded up to integers, are as follows at a=1.

x 0.40 0.45 0.50 0.55 0.60 0.63 0.65 0.70
earlier bound 3 4 4 5 5 5 5 6
packing bound 2 2 2 2 2 3 3 4
circle-slice bound 3 4 6 8 10 12 14 18

In one explicit-Euler floating replica with step 103 and a geometric grid of 40 initial areas from 106 to 1, the largest computed time to reach the area cap falls from 0.89703 with the earlier packing lower bound for k to 0.65503 with the certified circle-slice bounds, and to 0.63003 if the relaxation’s linear-programming value replaces those bounds. Shrinking the relaxation by the worst measured slack factor 1.045 moves it only to 0.60703. These computations suggest that this particular relaxation may stop near e0.607=0.545; they do not prove that it does, and they exclude neither a stronger lower bound on the root count nor a larger certified range.

The search uses only ten or fourteen radii in its two settings and a coarse a-grid with upward rounding. The reported loss from the first restriction at a=1, k=8 is about one per cent; the reported rounding loss is comparable. These are empirical estimates, not certified error bounds relative to the unrestricted continuous optimum.

The continuous optimisation remains unevaluated: maximise jλ(dj) subject to djdlow and jw(dj,r)π for every r>0, allowing the relaxed radial distributions used in the computation. The numerical optimiser spreads mass over several radii and suggests logarithmic growth in k. Neither that growth law nor its coefficient is proved. Evaluating the relaxation would clarify this packing argument; its effect on the final path threshold would still need to be established.

Guide to the results

The table distinguishes the main conclusions and their limitations. Each theorem retains its own hypotheses; the scope of formal verification is recorded separately.

Family or mechanism Conclusion and limitations
Trinomials The root equation controls every root-to-origin segment.
Low critical values Area growth and a finite certificate give the stated cutoff 13/25; the recorded certificate also covers μ529/1000. The scaled consequence uses level (25/13)μ.
Separated simple value A square root removes local branching; Bergman and capacity estimates bound length. The chosen critical point must be simple and its value isolated.
Collinear and sparse families Segment constructions for roots on a line or specified coefficients, not for arbitrary sparse polynomials.
Critical-value means An unconditional exponent 4/(n1) with sharp constant; higher exponents require specified complex power-sum cancellations. No choice of a short contained path follows.
Counterexamples and conditional reductions The Cassini example refutes the stated spanning-tree coefficient. The degree-eight example refutes the proposed Gamma-function perimeter constant, not every uniform perimeter bound. An assumed uniform subcritical perimeter bound βσ1/n gives length at most βρ in Kμ. Prescribed straight-segment rules also fail; the inverse-ray bound remains a historical sufficient condition.

A critical-value mean, a contained segment and a formally checked finite inequality do not supply the same conclusion.

References

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