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.
The historical question
Problem 1.1 (Erdős #1041). Let 𝑓(𝑧) =∏𝑛𝑖=1(𝑧 −𝑧𝑖) be monic of
degree 𝑛 ≥2, with 𝑧𝑖 ∈𝔻, the open unit disc.
Must two of the roots be joined by a curve of length less than 2 lying in the open lemniscate {𝑧 ∈ℂ :|𝑓(𝑧)| <1}?
The open-disc hypothesis is essential for this formulation. For 𝑓(𝑧) =𝑧2 −1, whose roots lie on the unit
circle, every continuous path from −1 to 1 meets the imaginary axis. There |𝑓(𝑖𝑦)| =1 +𝑦2 ≥1, 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.
Write 𝐸𝑓 ={𝑧 ∈ℂ :|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 1 ≤𝑚 <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 𝜁1 →0 →𝜁2, 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:
𝑓(𝑡𝜁)=𝑏(1−𝑡𝑚)+𝜁𝑛(𝑡𝑛−𝑡𝑚).(1)
For 0 ≤𝑡 <1 the two scalar weights 1 −𝑡𝑚 and 𝑡𝑚 −𝑡𝑛 are nonnegative and sum to 1 −𝑡𝑛, so
|𝑓(𝑡𝜁)|≤|𝑏|(1−𝑡𝑚)+|𝜁|𝑛(𝑡𝑚−𝑡𝑛)<1−𝑡𝑛≤1.
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) =∑𝑛𝑘=0𝑐𝑘𝑧𝑘 and
a zero 𝜁, put 𝑆𝑗 =∑𝑗𝑘=0𝑐𝑘𝜁𝑘. Finite
summation by parts gives
𝑓(𝑡𝜁)=𝑛−1∑𝑗=0(𝑡𝑗−𝑡𝑗+1)𝑆𝑗(0≤𝑡≤1),(2)
since the coefficient of 𝑐𝑘𝜁𝑘 on the right is 𝑡𝑘 −𝑡𝑛 and ∑𝑘<𝑛𝑐𝑘𝜁𝑘 = −𝑐𝑛𝜁𝑛. The
weights in (2) are
nonnegative and sum to 1 −𝑡𝑛, 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 𝑚 ≤𝑗 <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+15𝑟2𝑧4−15𝑟4𝑧2−𝑟6=(𝑧2−𝑟2)(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.
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 𝑛 ≥2 with 𝜇 ≤13/25. 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) =𝑧𝑛 −𝑏 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, (𝑧 −3)𝑛 −1/2, 𝑛 ≥2, 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 𝑛 ≥2 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 𝑠−𝑛𝑓(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 𝑘 ≥2 be its root count,
and put 𝑥 =log(𝑡/𝜇) and 𝑎 =Area(𝐶𝑡)/𝜋; Pólya’s
inequality [2] gives 𝑎 ≤𝑡2/𝑛 <1. The component is a
Jordan domain. List its roots as 𝜁1,…,𝜁𝑘, choose a Riemann
map 𝜑 :𝔻 →𝐶𝑡, and
write 𝑏𝑗 =𝜑−1(𝜁𝑗).
The component-wise form of [8] is
𝑓(𝜑(𝑧))𝑡=𝑒𝑖𝜃𝑘∏𝑗=1𝑧−𝑏𝑗1−―――𝑏𝑗𝑧.
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 0 ≤𝑠 <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) =∑ℓ≥0𝛼ℓ𝑧ℓ. Injectivity and the area formula give ∑ℓ≥0|𝛼ℓ|2/(ℓ +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=|
|
|
|
|∑ℓ≥0𝛼ℓ∫𝐼𝜔(𝑥)𝑥ℓ𝑑𝑥|
|
|
|
|2≤𝑎∑ℓ≥0(ℓ+1)|
|
|
|∫𝐼𝜔(𝑥)𝑥ℓ𝑑𝑥|
|
|
|2.
Compactness of
𝐼 permits termwise integration of
the series. Since ∑ℓ≥0(ℓ +1)(𝑥𝑦)ℓ =(1 −𝑥𝑦)−2 >0
for real 𝑥,𝑦 ∈𝐼, taking absolute
values in the resulting double integral yields
length(𝜑(𝐼))2≤𝑎∫𝐼∫𝐼𝑑𝑥𝑑𝑦(1−𝑥𝑦)2.
This is precisely
the positivity of the disc Bergman kernel 𝐾(𝑧,𝑤) =𝜋−1(1 −𝑧――𝑤)−2 on
the real diameter. For 𝐼 =[𝑢,𝑣] ⊂( −1,1), direct integration
gives
∫𝑣𝑢∫𝑣𝑢𝑑𝑥𝑑𝑦(1−𝑥𝑦)2=log(1−𝑢𝑣)2(1−𝑢2)(1−𝑣2).
Thus 𝐼 =[0,𝑟] gives length(𝜑([0,𝑟]))2 ≤𝑎log(1/(1 −𝑟2)). Moving two preimages to ±𝑠 and taking 𝐼 =[ −𝑠,𝑠] instead gives
length(𝜑([−𝑠,𝑠]))2≤4𝑎artanh(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
𝑑(𝑏𝑖,𝑏𝑗) ≥ 𝐷:=4artanh√tanh(1/𝑎),cosh(𝐷/2)=𝑒2/𝑎.(3)
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 =𝜑−1(𝜁𝑗). Put
𝑑𝑗 =𝑑(0,𝑏𝑗) and 𝜆(𝑑) = −logtanh(𝑑/2). The one-root
estimate at ℎ gives tanh(𝑑𝑗/2) ≥√1−𝑒−1/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
𝜆(𝑑𝑗)≤𝛿(𝑎)2,𝛿(𝑎)=−log(1−𝑒−1/𝑎),𝑘∑𝑗=1𝜆(𝑑𝑗) ≥ 𝑥.(4)
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,
𝑘∑𝑗=1𝑤(𝑑𝑗,𝑟)≤𝜋,𝑤(𝑑,𝑟)=arccos(clampcosh𝑑cosh𝑟−cosh(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 cosh𝑑𝑗cosh𝑟 −sinh𝑑𝑗sinh𝑟cos(𝜃 −𝜃𝑗) <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,…,𝜎𝑝 ≥0, put Σ =∑𝑖𝜎𝑖 and
𝑈=sup𝑑≥𝑑low(𝑎)[𝜆(𝑑)−∑𝑖𝜎𝑖𝑤(𝑑,𝑟𝑖)],𝜆(𝑑low(𝑎))=𝛿(𝑎)2.
If
𝑈 >0, then failure forces 𝑘 ≥(𝑥 −𝜋Σ)/𝑈.
Proof. By (4),
Lemma 3.3 and the
radius bound,
𝑥≤∑𝑗𝜆(𝑑𝑗)=∑𝑗[𝜆(𝑑𝑗)−∑𝑖𝜎𝑖𝑤(𝑑𝑗,𝑟𝑖)]+∑𝑖𝜎𝑖∑𝑗𝑤(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 𝑘 ≥2𝑥/𝛿(𝑎);
nonzero weights incorporate the circle-packing information and can
improve the result. A certificate at area 𝑎′ ≥𝑎 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 𝑑1 ≤⋯ ≤𝑑𝑘. The triangle inequality gives 𝑑𝑗 ≥𝐷 −𝑑1 for 𝑗 ≥2. 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) +(𝑘 −1)𝜆(𝐷 −𝑑) takes its
maximum at an endpoint. If 𝑑1 ≥𝐷/2, each summand is at most 𝜆(𝐷/2) instead. (The definitions
give 𝑑low <𝐷/2.) Thus
𝑥≤∑𝑗𝜆(𝑑𝑗)≤max{𝛿(𝑎)2+(𝑘−1)𝜆(𝐷−𝑑low),𝑘𝜆(𝐷/2)},
and consequently
𝑘≥min{1+𝑥−𝛿(𝑎)/2𝜆(𝐷−𝑑low),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/𝑎 −1, 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 =𝑘 −1 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 =cosh𝑟 −1, the identity −logtanh(𝑟/2) =12log(1 +2/𝑣)
reduces the radial integral to (2𝐸)−1∫𝑚𝐸0log(1 +2/𝑣) 𝑑𝑣.
Evaluating it gives
12𝜋𝐸∫𝐵hyp(0,𝑅)−log|𝑧|𝑑𝐴hyp=𝑚𝐸2log(1+2/(𝑚𝐸))+log(1+𝑚𝐸/2)𝐸≤1+log(1+𝑚𝐸/2)𝐸,
where the improper integral is
finite because 𝑣log𝑣 →0 as 𝑣 ↓0, and the last inequality
uses log(1 +𝑢) ≤𝑢 for 𝑢 >0. Adding the possible exceptional
contribution and inverting each case yields
𝑘≥min{1+2𝐸(𝑒𝐸(𝑥−𝛿(𝑎)/2)−1−1),2𝐸(𝑒𝐸𝑥−1−1)}.
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, 0 ≤𝐴0 ≤𝜋𝑎. 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) =∑ℓ≥0𝛾ℓ𝑧ℓ
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(∫10|𝜓′(𝑟𝑒𝑖𝜃)|𝑑𝑟)2≤∑ℓ≥1ℓ2|𝛾ℓ|22ℓ−1≤∑ℓ≥1ℓ|𝛾ℓ|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
𝑃𝐶(𝑢)2≤2𝜋𝑘𝑢𝐴′𝐶(𝑢),(5)
because |𝑑𝑧| =𝑢 𝑑(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(𝜋𝑎−𝐴0)/(2𝜋).
Cauchy–Schwarz combines the low and high bounds as
√𝑘𝐴0𝜋+√𝑘𝑥(𝜋𝑎−𝐴0)2𝜋≤√𝑘𝑎(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
2𝑘≤√2𝑘𝑎(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) =𝑡𝐴′𝐶(𝑡)/𝜋. Applying
(5) at the
outer level and rearranging therefore gives
𝑎′(𝑥) ≥ 12𝜋2[2√𝑘−√2𝑎(𝑥)(𝑥+2)]2+(6)
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 𝑎 ≤1, for 0 <𝑥 ≤3/105 the bound 𝑘 ≥2 alone gives
𝑎′(𝑥)≥12𝜋2(2√2−√2(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) >10−6. 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 [𝑥ℓ,𝑥𝑟], suppose 𝑎(𝑥ℓ) ≥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 𝑎 ≤𝑚. If 𝑚 <𝑎𝜄 +(𝑥𝑟 −𝑥ℓ)𝑔, then 𝑎(𝑥𝑟) >𝑚. Indeed, the contrary
assumption 𝑎(𝑥𝑟) ≤𝑚 would imply
𝑎 ≤𝑚 throughout the cell by
monotonicity. Integrating the differential inequality, with the
nonnegative merger jumps, would then give 𝑎(𝑥𝑟) >𝑚, a contradiction.
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 =2∑𝑗≥03−(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 10−6 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)=cosh𝑑cosh𝑟−cosh(𝐷/2)sinh𝑑sinh𝑟,𝐻′(𝑑)=cosh(𝐷/2)cosh𝑑−cosh𝑟sinh2𝑑sinh𝑟.
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 𝑒𝑋 ≤∑𝑗≤14𝑋𝑗/𝑗! +(𝑋15/15!)/(1 −𝑋/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
𝜇 ≤529/1000, 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 <𝑒−𝑋; 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 𝑛 ≥2 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 𝑛 ≥3, apply
Theorem 3.1
to 𝑔(𝑧) =𝑠−𝑛𝑓(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) =(𝑧 −ℎ)2 −𝑑2. 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 𝜇 ≤1/2 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 𝑛 ≥2, 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 𝜇 ≤1/2, 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 𝑘 ≥2 roots, then for every 𝑟 ∈(0,1) and 𝜆 >1 the proof constructs a path
in 𝐾𝜆𝜇 whose length is
at most
√2𝑘(√2𝑟(1−𝑟)2+𝜆1/𝑛(√log(𝜆/𝑟)+𝜋√log𝜆))𝜌.(CF)
For
𝑛 ≥3, 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 𝑛 ≥3. Put 𝑇 =𝜆𝜇, let 𝐶𝑇 be the component of 𝐾𝑇 containing a critical point at level
𝜇, and write 𝐴(𝜎) =Area(𝐾𝜎 ∩𝐶𝑇). 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| =𝜎 𝑑𝜑/|𝑓′| on its
boundary and total argument variation 2𝜋𝑘′. Cauchy–Schwarz, followed by the coarea formula, gives
H1(𝜕𝐶′)2≤2𝜋𝑘′𝜎𝐴′(𝜎).(CF1)
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 𝑘 ≥2 roots and
H1(𝜕𝐶𝑡)≤𝜋√2𝑘/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
∑𝑖𝜇2|𝑓′(𝑧𝑖)|2≤𝜌2.(CF2)
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 ℓhigh𝑖(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 ∑𝑖ℓhigh𝑖. Cauchy–Schwarz in 𝜎, using an area increment at most
Area(𝐶𝑡) ≤𝜋𝑇2/𝑛, gives
12𝜋∫2𝜋0∑𝑖ℓhigh𝑖(𝜃)𝑑𝜃≤√𝑘Area(𝐶𝑡)2𝜋log𝑡𝑟𝜇≤√𝑘2𝑇1/𝑛√log(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:
2𝑘∑𝑖ℓlow𝑖≤2𝑟𝜌√𝑘(1−𝑟)2,2𝑘∑𝑖ℓhigh𝑖≤√2𝑘√log(𝜆/𝑟)𝑇1/𝑛,H1(𝜕𝐶𝑡)𝑘≤√2𝑘𝜋𝑇1/𝑛√log𝜆.
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 =2√𝜇 ≤√2. For 𝑛 ≥3, take 𝜆 =2 and 𝑟 =3/20. Since 𝑘 ≥2 and 𝜇 ≤1/2, (CF) gives
length≤60√2289𝜇1/𝑛+(2𝜇)1/𝑛(√log(40/3)+𝜋√log2)≤60√2289+√log(40/3)+𝜋√log2=5.676476…<5.7.
Here 2𝜇 ≤1, 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 𝑧𝑛 −𝑏,
however, all 𝑛 roots merge at the
same level, giving 𝑘0 =𝑛. For
example, 𝑛 ≥17 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
𝜇≤12 and 𝑘0≥17,𝜇≤14 and 𝑘0≥12,𝜇≤18 and 𝑘0≥10.
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 𝑘 ≥𝑘0. For the first case take 𝜆 =2, 𝑟 =13/100; then (2𝜇)1/𝑛 ≤1 and 𝜌 ≤1, 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 34 −12570881068535/7590664173456 <34.
Hence 𝑘0 ≥17 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 24 −2038665078215/1622790636544 <24, and
2/𝑘0 ≤1/6 gives squared length
below 4. For the third take 𝜆 =8, 𝑟 =11/100: the bracket is below 55629121/12475575, whose square is 20 −18200328379859/155639971580625 <20,
and 2/𝑘0 ≤1/5 again gives squared
length below 4. In each case 𝜆𝜇 ≤1, 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 𝜅 ≤1/3 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 <𝜇 ≤1/2, let 𝐶 be the component of {|𝑓| <2𝜇} containing 𝑐∗, and put 𝜅 =cap(――𝐶)/(2𝜇)1/𝑛. If 𝜅 ≤𝜏𝑘0, where
𝜏𝑘=√2𝑘−𝐴𝐵,𝐴=2833610,𝐵=520299100,
then
Erdős #1041 holds for 𝑓. In
particular 𝜅 ≤1/3 suffices
for every root count 𝑘0 ≥2, 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(𝐾𝜎 ∩𝐶) 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/𝑘0 ≤1
altogether gives the uniform cutoff 𝜅 ≤1/3. ◻
By the component-capacity formula, 𝜅 =𝑒−Σ/𝑛 with Σ the sum of exterior Green function
values at the roots excluded from 𝐶. Indeed, let Ω be the unbounded component of
ˆℂ\――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 𝑎 ∈Ω. The function
1𝑛log|𝑓|2𝜇 −𝐺 +1𝑛∑𝑎𝑔( ⋅,𝑎), summed over the roots 𝑎 ∈Ω with multiplicity, extends
harmonically to Ω, is bounded,
and vanishes on 𝜕Ω ⊆𝜕𝐶, so it
vanishes identically; its value at infinity is log𝜅 +1𝑛∑𝑎𝐺(𝑎) by the
symmetry 𝑔(∞,𝑎) =𝐺(𝑎). Failure
of these component-sensitive criteria alone, in the range 𝜇 ≤1/2, forces 𝑘0 ≤16 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 𝑛 ≥2, 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
∫2𝜋0|𝜙′𝑗(𝑒𝑖𝑡)|𝑑𝑡≤𝛽𝜎1/𝑛(1≤𝑗≤𝑛)?
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
12𝜋∫2𝜋0|𝜙′𝑗(𝑒𝑖𝑡)|𝑑𝑡≤(𝜎𝑅)1/𝑛√𝑅2−1.
Indeed, circular
means of |𝜙′𝑗|2 increase,
the image of the annulus 1 <|𝑤| <𝑅 has area at least 𝜋(𝑅2 −1) times the mean at 1, and Pólya’s preimage-area bound bounds that area by 𝜋(𝜎𝑅)2/𝑛. The loss as 𝑅 ↓1 belongs to this argument and
does not prove an endpoint divergence.
For 𝑑 >0 and 𝑓(𝑧) =𝑧2 −𝑑2, one has 𝜇 =𝑑2 and 𝜌 =𝑑. For 𝜎 <𝑑2 the component of {|𝑓| ≤𝜎} around 𝑑 contains one root. Its parametrisations
𝑑√1+(𝜎/𝑑2)𝑒𝑖𝜃
converge uniformly, as 𝜎 ↑𝑑2, to one loop of Bernoulli’s lemniscate |𝑧2 −𝑑2| =𝑑2, of length 𝑑 Γ(1/4)2/(2√𝜋) by the
substitution 𝜑(𝑤) =𝑑√1+𝑤
and Γ(1/4)Γ(3/4) =𝜋√2. 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 𝛽∗ ≥Γ(1/4)2/(2√𝜋) =3.70814935…;
convergence of the lengths themselves is not required. For 𝑧𝑛 −𝑟𝑛, polar parametrisation of one
limiting loop gives its length divided by 𝑟 as
21/𝑛𝑛∫𝜋/2−𝜋/2(cos𝜃)1/𝑛−1𝑑𝜃=21/𝑛𝑛√𝜋Γ(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+1√𝜋 Γ(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 𝑧2 −𝑑2 has parametrisation
𝑧(𝑠)=√2𝑑cos𝑠(1+𝑖sin𝑠)1+sin2𝑠,−𝜋/2≤𝑠≤𝜋/2,
whose speed is √2 𝑑/√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=3⋅217168>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/(2√𝜋).
Moreover, for fixed 𝑎 >1 and all
sufficiently large 𝑁, the one-root
component of {|𝑧𝑁 −𝑎𝑧| ≤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 𝑎 ↓1 shows that
every admissible 𝛽 is at least
2𝜋. For the latter family all
critical values have modulus (1 −1/𝑁)𝑎(𝑎/𝑁)1/(𝑁−1) →𝑎 >1, so it
also gives the necessary bound 𝛽∗ ≥2𝜋 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 𝑛 ≥2, 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 𝑑 ≥2 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 𝑤 →𝑤0. At its preimage 𝑐, write
𝑓(𝑧)−𝑓(𝑐)=(𝑧−𝑐)𝑑ℎ(𝑧),ℎ(𝑐)≠0.
A local analytic 𝑑th root of ℎ makes (𝑧 −𝑐)ℎ(𝑧)1/𝑑 a conformal coordinate.
In each inverse sector, 𝜙 is
therefore an analytic function of (𝑤 −𝑤0)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(|𝜃 −𝜃0|1/𝑑−1), 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 𝑟 ↑1, 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 𝑎 ∈𝑈 can be joined to any
𝑐 ∈𝜕𝑈 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
|𝑎−𝑢|+|𝑎−𝑣|+length(𝐴)=|𝑢−𝑣|+length(𝐴)≤H1(𝜕𝑈),
because |𝑢 −𝑣| ≤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) =∏3𝑗=1(𝑧 −𝑧𝑗) 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
𝑘 ≥2 roots and hence 𝑘 −1 ≥1 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) =𝑑3 −32𝛿𝑑2 +𝑣. Choose 𝛼 with
𝛼3 =𝑣 and set 𝑏 =𝛿/𝛼; dividing by 𝑣 gives 𝑓(𝑐 +𝛼𝑤)/𝑣 =𝑃𝑏(𝑤) with
𝑃𝑏(𝑤)=𝑤3−32𝑏𝑤2+1.
At the other
critical point 𝑓(𝑐 +𝛿) =𝑣(1 −𝑏3/2), so minimality of
|𝑣| is exactly the hypothesis |1 −𝑏3/2| ≥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 +𝑤−2).
Write 𝑤3 =𝑒2𝑖𝑢; substitution
gives
|1−𝑏3/2|2=1+64729cos4𝑢(16cos2𝑢−27)≤1.
Since 16cos2𝑢 −27 <0, equality requires
cos𝑢 =0, which gives 𝑏 =0. Thus the strict region has no
unit-circle zero. The radial deformation 𝑏 ↦𝑠𝑏, 𝑠 ≥1, stays in the strict region, since
𝑧 =𝑏3/2 and |1 −𝑧|2 >1 give |1 −𝑠3𝑧|2 −1 =𝑠3(𝑠3|𝑧|2 −2ℜ𝑧) >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 𝑏 ≠0, the same
radial deformation lies in the strict region for every 𝑠 >1, and continuity of the root
multiset allows 𝑠 ↓1. If
𝑏 =0, then 𝑃𝑏(𝑤) =𝑤3 +1 and all three roots lie on
the unit circle.
If 𝑃𝑏(𝑤) =0 and 0 ≤𝑡 ≤1, then 𝑃𝑏(𝑡𝑤) =1 −𝑡2 −𝑡2(1 −𝑡)𝑤3, so |𝑤| ≤1 gives |𝑃𝑏(𝑡𝑤)| ≤(1 −𝑡2) +𝑡2(1 −𝑡)|𝑤|3 ≤1 −𝑡3 ≤1.
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|(1 −𝑡3) <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) =(𝑧 −1)(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.
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) =𝑧3 −3𝑎2𝑧 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 𝑛 ≥3 whose leading
coefficient has modulus one, with
𝑃(0)=1,𝑃′(0)=0,𝑃″(0)≠0.
Fix 𝑤0 ∈[0,1] and 𝑆 >max(𝑤0,1 −𝑤0). Suppose every other
critical point 𝑑 ≠0 satisfies
|𝑃(𝑑)−𝑤0|≥𝑆.(4)
Put 𝑝 =𝑤0(1 −𝑤0). The two local solutions of
𝑃(𝑍(𝜉)) =1 −𝜉2, 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
length(Γ)2≤2(𝑆𝑛−1)2/𝑛log𝑆2+𝑆+𝑝𝑆2−𝑆+𝑝.(5)
Consequently the connector is shorter than
2 whenever
(𝑆𝑛−1)2/𝑛log𝑆2+𝑆+𝑝𝑆2−𝑆+𝑝<2.(6)
Proof. Let 𝑄 =𝐷(𝑤0,𝑆)
and let 𝑈 be the component of 𝑃−1(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 1 −𝑤0 <𝑆′ <𝑆, let 𝑈′ be the component of {|𝑃 −𝑤0| <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 |𝑃 −𝑤0| 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 :𝑈 →𝑄 consequently also has
degree two. This establishes the count without a smoothness assumption
at the outer level.
Set 𝑎 =1 −𝑤0. On 𝑈, the function 1 −𝑃 has only its double zero at 0, so it has a single-valued square root
𝜉(𝑧)2=1−𝑃(𝑧).
Taking this
square root removes the double branching at 0. The map 𝜉 is proper into
˜𝑄={𝜉:|𝜉2−𝑎|<𝑆}.
Away from 0, the identity 2𝜉𝜉′ = −𝑃′ gives 𝜉′ ≠0; at 0, (𝜉′(0))2 = −𝑃″(0)/2 ≠0.
The target is star-shaped about 0:
because 𝑆 >𝑎, the convex disc
𝐷(𝑎,𝑆) contains 0, so 𝑡2𝜉2 ∈𝐷(𝑎,𝑆) whenever 𝜉 ∈˜𝑄 and 0 ≤𝑡 ≤1. 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)) =1 −𝜉2 ∈[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 ↦(𝑤 −𝑎)/𝑆 with the disc
automorphism taking −𝑎/𝑆 to 0. The result is the Möbius map
𝑤⟼𝑆𝑤𝑆2+𝑎𝑤−𝑎2.
Taking its square root after substituting 𝑤 =𝜉2 gives the conformal bijection
𝜁(𝜉)=𝜉√𝑆𝑆2+𝑎𝜉2−𝑎2:˜𝑄⟶𝔻,
where the
square-root factor is chosen positive at 0. It sends [ −1,1] to [ −𝑞,𝑞], with
𝑞2=𝑆𝑆2+𝑝,𝑆2−𝑆+𝑝=(𝑆−𝑤0)(𝑆−(1−𝑤0))>0.
The last inequality is exactly
where 𝑆 >max(𝑤0,1 −𝑤0) ensures
0 <𝑞 <1, as required by the
length estimate below. For Φ =𝑍 ∘𝜁−1 :𝔻 →𝑈, the
Bergman segment inequality, proved by the kernel estimate of
Section 3 with the
double integral taken over [ −𝑞,𝑞]2, gives
length(Γ)2≤2𝜋log1+𝑞21−𝑞2Area(𝑈)=2𝜋log𝑆2+𝑆+𝑝𝑆2−𝑆+𝑝Area(𝑈).(7)
It remains to bound the area of this component. The factor 𝑛 −1 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<𝑘2𝑛−𝑘.
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 =𝑛 −𝑘 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)=𝑚∏𝑗=1𝑧−𝑏𝑗1−―――𝑏𝑗𝑧.
Reflection in the unit circle shows that 𝐹(𝜓(𝜁))/𝑡 equals 𝜁𝑛―――――𝐵(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 𝐻 ∘𝐵 is harmonic, the mean value property and the Poisson formula
give
12𝜋∫2𝜋0ℎ(𝐵(𝑒𝑖𝜃))𝑑𝜃=𝐻(𝐵(0))=12𝜋∫2𝜋0ℎ(𝑒𝑖𝜙)1−|𝐵(0)|2|𝑒𝑖𝜙−𝐵(0)|2𝑑𝜙.
Differentiating the factors gives the positive angular derivative
𝑑𝑑𝜃arg𝐵(𝑒𝑖𝜃)=|𝐵′(𝑒𝑖𝜃)|=𝑚∑𝑗=11−|𝑏𝑗|2|𝑒𝑖𝜃−𝑏𝑗|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|𝑤−𝐵(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)|<𝑛−𝑚𝑛+𝑚=𝑘2𝑛−𝑘.
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 𝑃 −𝑤0, counted
with multiplicity. Since 2 <𝑛,
the preceding estimate applies with 𝑘 =2 and gives
cap(―――𝑈′)𝑛𝑆′<𝑘2𝑛−𝑘=1𝑛−1.
Pólya’s area–capacity
inequality Area(𝐾) ≤𝜋cap(𝐾)2
[2] then yields Area(𝑈′) <𝜋(𝑆′/(𝑛 −1))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(𝑆𝑛−1)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 𝑛 ≥3, every 𝑤0 ∈[0,1], and every 4/3 ≤𝑆 ≤2. 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)𝑣−𝑤0|
|
|
|≥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 𝑆 ≥4/3 and
𝑝 ≥0,
𝑆2+𝑆+𝑝𝑆2−𝑆+𝑝≤𝑆+1𝑆−1≤7.
Also 𝑆/(𝑛 −1) ≤1 when 𝑆 ≤2 and 𝑛 ≥3, 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 |1 −𝑓(𝑑)/𝑣| ≥2 in every degree 𝑛 ≥3. If 𝑐 attains the minimum modulus among
all critical values and 𝑣 ≠0, 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, (𝑧 −𝑅)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)=𝑧4−𝜀𝑧3−2𝑧2+3𝜀𝑧+12,0<𝜀≤132.
Its derivative and two
critical values are
𝑔′𝜀(𝑧)=(𝑧2−1)(4𝑧−3𝜀),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 4𝜀 →0. The earlier numerical
choice is the exact member 𝜀 =1/262144:
𝑔(𝑧)=𝑧4−𝑧3262144−2𝑧2+3𝑧262144+12,𝑔′(𝑧)=4(𝑧+1)(𝑧−3/1048576)(𝑧−1),
for which that difference
is 1/65536. The monic polynomial
2−4𝑔𝜀(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+4𝜀1−4𝜀≤97<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 𝑛 ≥3, 4/3 ≤𝑆 ≤2 and 𝑝 ≥0, 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 𝑧𝑛 −𝑏 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/𝑛≤𝑚(𝐸∪𝐷)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 𝐸 ∪𝐷 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((𝑧 −ℎ)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=12𝑛−1𝑟𝑛𝑛.
Theorem 7.1 (Chebyshev comparison). Let 𝑚 ≥0, let 𝑝 ∈ℝ[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 0 ≤𝑖 <𝑚. Then
min0≤𝑖≤𝑚|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 𝑛 ≥2 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
|𝑓(𝑧)|≤(𝐷/2)𝑛2𝑛−1cos𝑛(𝜋/(2𝑛)).(9)
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 𝜃 ∈ℝ 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)=𝑅−𝑛𝑒−𝑖𝑛𝜃𝑓(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)2𝑛−1𝑟𝑛𝑛.
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 𝑛 −1 chosen points
alternate. If every gap maximum were larger than 𝐶𝑛, then 𝑞 −𝑞∗ would have the same nonzero signs
there. The intermediate value theorem would give 𝑛 −2 zeros between consecutive 𝑐𝑖, in addition to the two zeros at
±1. These 𝑛 zeros are distinct, but 𝑞 −𝑞∗ is nonzero and has degree at most
𝑛 −1 because its leading terms
cancel. This contradiction selects a gap on which |𝑞| ≤𝐶𝑛. Scaling back proves
(9).
For sharpness, take
𝑦𝑘=cos((2𝑘−1)𝜋/(2𝑛))𝑟𝑛,1≤𝑘≤𝑛.
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 𝑛 ≥2 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 𝐶𝑛 ≤21−𝑛/2 ≤1,
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 𝑛 ≥3 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.
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(𝑐𝑛−1)), with 𝑐1 <⋯ <𝑐𝑛−1. 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 𝑛 −1 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 𝑒−𝑖𝑛𝜃𝑇𝑛(21/𝑛−1𝑒𝑖𝜃𝑧 +𝑏)
with 𝜃 real .
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 0 ≤𝑠𝑖 ≤1, 𝑥2𝑖 ≤𝑠𝑖, put
𝐸𝑖=𝑠4𝑖(𝑠𝑖+𝑟2+2𝑟𝑥𝑖).
Theorem 7.4 (a consequence of three moment
identities). Suppose
4∑𝑖=0𝑥𝑖=−𝑟,4∑𝑖=0(2𝑥2𝑖−𝑠𝑖)=𝑟2,4∑𝑖=0(4𝑥3𝑖−3𝑠𝑖𝑥𝑖)=−𝑟3.(10)
Then
at least one of the ten pairs 0 ≤𝑖 <𝑗 ≤4 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
|𝑏𝑤𝑖+𝑐|≤1.(11)
If 𝑎 ≠0, 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 𝑎 ≠0, write 𝑎 =𝑟𝑒𝑖𝜙 with 𝑟 >0 and set 𝑧𝑖 =𝑒−𝑖𝜙𝑤𝑖. The missing 𝑧3 and 𝑧2 coefficients and Newton’s identities
give
∑𝑧𝑖=−𝑟,∑𝑧2𝑖=𝑟2,∑𝑧3𝑖=−𝑟3.(12)
At a
zero,
|𝑏𝑤𝑖+𝑐|=|𝑤𝑖|4|𝑤𝑖+𝑎|.
Thus, for 𝑥𝑖 =ℜ𝑧𝑖 and 𝑠𝑖 =|𝑧𝑖|2, the squared modulus |𝑏𝑤𝑖 +𝑐|2 is exactly 𝐸𝑖 and (12) becomes
(10). The third moment gives 𝑟3 =|∑𝑖𝑧3𝑖| ≤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 𝑥 ≥ −𝑟/2. We therefore use the harmonic
extension of ( −𝑟/2 −𝑥)(1 −𝑥)2, which
is nonpositive on that part of the circle. In the variables 𝑥 =ℜ𝑧 and 𝑠 =|𝑧|2, this extension is
𝐻𝑟(𝑥,𝑠)=(−𝑟/2−𝑥)(1−𝑥)2+(1−𝑠)(1−𝑟4−3𝑥4).
The useful feature
of this choice is the expansion
𝐻𝑟(ℜ𝑧,|𝑧|2)=1−3𝑟4+ℜ[(𝑟−74)𝑧+(1−𝑟4)𝑧2−𝑧34].
It is harmonic, and summing this expression with the three moments in
(12) gives
4∑𝑖=0𝐻𝑟(𝑥𝑖,𝑠𝑖)=5−2𝑟.(13)
On the unit circle its value is ( −𝑟/2 −𝑥)(1 −𝑥)2, and
4−2𝑟−(−𝑟/2−𝑥)(1−𝑥)2=(𝑥+1)((2−𝑟)(3−𝑥)2+(1−𝑥)2)≥0.
The maximum
principle therefore gives 𝐻𝑟 ≤4 −2𝑟 throughout the disc. For an
index with 𝑠4(𝑠 +𝑟2 +2𝑟𝑥) ≥1, one
has 𝑠 >0 and 𝑠−4 ≥1 +4(1 −𝑠) by convexity on (0,1]. Consequently
2𝑟(𝑥+𝑟/2)≥𝑠−4−𝑠≥5(1−𝑠).
Put
𝑑 =𝑥 +𝑟/2, 𝑢 =1 −𝑥, 𝐴 =1 −𝑟/4 −3𝑥/4, and 𝑃 = −𝑢2 +(2𝑟/5)𝐴. The assumption 𝑠4(𝑠 +𝑟2 +2𝑟𝑥) ≥1 gives 0 ≤𝑑 <2. Since 𝐻𝑟 = −𝑑𝑢2 +(1 −𝑠)𝐴, it is nonpositive when
𝐴 ≤0; when 𝐴 >0, the preceding bound gives 𝐻𝑟 ≤𝑑𝑃. The remaining estimate is the
exact sum-of-squares identity
131−𝑃=25(𝑑−3831+14(𝑢−331))2+3140(𝑢−331)2≥0,
which gives
𝑃 ≤1/31, and hence 𝐻𝑟(𝑥,𝑠) ≤2/31 whether 𝑃 is positive or nonpositive. Thus 𝐻𝑟 ≤2/31 whenever the squared modulus
is at least 1. If four indices had
squared modulus at least 1,
(13) would give
5−2𝑟≤4−2𝑟+831<5−2𝑟,
a
contradiction. This proves the two-index conclusion when 𝑎 ≠0.
For either value of 𝑎, at a zero
𝑤,
𝑝(𝑡𝑤)=(1−𝑡)𝑐+(𝑡−𝑡4)(𝑏𝑤+𝑐)−𝑡4(1−𝑡)𝑤5.
For 0 ≤𝑡 ≤1 the three
nonnegative weights sum to 1 −𝑡5.
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 1 −𝑡 is positive for 0 ≤𝑡 <1, so
|𝑝(𝑡𝑤)|<(1−𝑡)+(𝑡−𝑡4)+𝑡4(1−𝑡)=1−𝑡5≤1.
At 𝑡 =1 the value is zero. Thus both
segments lie in {|𝑝| <1}, and
their total length is |𝑤𝑖| +|𝑤𝑗| <2. ◻
Polynomials obtained from a cubic by a power substitution
For 𝑓(𝑧) =𝑃((𝑧 −ℎ)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,𝑣 ∈ℂ have
modulus below one, at least one 𝑢 ∈{𝑟,𝑠,𝑣} satisfies
|(𝑡𝑢−𝑟)(𝑡𝑢−𝑠)(𝑡𝑢−𝑣)|≤1(0≤𝑡≤1).
This is exactly the
formal cubic segment inequality.
Theorem 7.7 (a cubic composed with a power map).
Let 𝑞 ≥2, ℎ ∈ℂ, 𝑃 be monic cubic, and
𝑓(𝑧)=𝑃((𝑧−ℎ)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
(𝑧−ℎ)3𝑞+𝐴(𝑧−ℎ)2𝑞+𝐵(𝑧−ℎ)𝑞+𝐶
in
every degree 3𝑞 ≥6.
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,
1𝑞𝑞−1∑𝑘=0|ℎ+𝑦𝜁𝑘|2=|ℎ|2+|𝑦|2<1.(14)
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 2√1−|ℎ|2. The
position of the symmetry centre therefore improves the length bound;
replacing it by 2 discards this
information.
Write 𝑃(𝑤) =(𝑤 −𝑟)(𝑤 −𝑠)(𝑤 −𝑣) and
associate to 𝑟 the real number
𝐴𝑟 =ℜ(𝑟――――𝑠+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 0 ≤𝑡 ≤1,
|𝑡𝑟−𝑠|2+|𝑡𝑟−𝑣|22=𝑡2|𝑟|2+|𝑠|2+|𝑣|22−𝑡𝐴𝑟<1+𝑡+𝑡2.
AM–GM now
gives |𝑡𝑟 −𝑠| |𝑡𝑟 −𝑣| <1 +𝑡 +𝑡2.
Consequently, for 0 ≤𝑡 <1,
|𝑃(𝑡𝑟)|<(1−𝑡)(1+𝑡+𝑡2)=1−𝑡3≤1.(15)
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| <2√1−|ℎ|2 ≤2. If the
selected quotient root is zero, choose a nonzero quotient root 𝑠 and write 𝑃(𝑤) =𝑤(𝑤 −𝑠)(𝑤 −𝑣). For 0 <𝑡 <1,
|𝑃(𝑡𝑠)|=𝑡(1−𝑡)|𝑠|2|𝑡𝑠−𝑣|<2𝑡(1−𝑡)≤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. ◻
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 2√1−|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.
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) =∏𝑛𝑖=1(𝑧 −𝑎𝑖),
𝑛 ≥2, with all |𝑎𝑖| ≤1. Put 𝜌𝑖 =|𝑎𝑖| and 𝐷 =|disc(𝑓)|/𝑛𝑛. The Vandermonde
determinant estimate says that, when 𝐷 ≥1 −𝜂 and 0 ≤𝜂 ≤1/(80𝑛2),
1−𝜌2𝑖≤𝑛𝜂𝑛−1,|𝑎𝑖−𝑎𝑗|≥2−2√𝜂−𝑛𝜂𝑛−1,
where the second
inequality is for 𝑖 ≠𝑗. Moreover,
the roots lie within 7√𝜂 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 =𝑎𝑚𝑖, 0 ≤𝑚 <𝑛, and let 𝐺 =𝑉𝑉∗, 𝑠𝑖 =𝐺𝑖𝑖 =∑𝑛−1𝑚=0𝜌2𝑚𝑖
and 𝐻 =diag(𝑠−1/2𝑖)𝐺diag(𝑠−1/2𝑖).
The normalisation makes 𝐻 positive
semidefinite with diagonal entries one, and
𝐷=det𝐻∏𝑖𝑠𝑖𝑛.
Every
factor is at most one by Hadamard’s inequality, so 𝐷 ≥1 −𝜂 forces each factor to be at
least 1 −𝜂. In particular,
(𝑛−1)(1−𝜌2𝑖)≤𝑛−𝑠𝑖≤𝑛𝜂.
Hadamard–Fischer applied to the {𝑖,𝑗} principal block gives det𝐻 ≤1 −|𝐻𝑖𝑗|2, hence |𝐺𝑖𝑗| ≤𝑛√𝜂. For 𝑡 =𝑎𝑖―――𝑎𝑗, the finite geometric
sum then gives
𝑛√𝜂≥|
|
|
|
|𝑛−1∑𝑚=0𝑡𝑚|
|
|
|
|≥𝑛−𝑛(𝑛−1)2|1−𝑡|.
Together with 1 −𝑡 =1 −𝜌2𝑗 +―――𝑎𝑗(𝑎𝑗 −𝑎𝑖),
this proves the displayed separation bound. These two bounds need only
0 ≤𝜂 <1; the smaller range is
used for the matching with a regular polygon.
For that matching, put 𝜅 =𝑛2𝜂/(𝑛 −1) ≤1/80 and 𝑢𝑖 =𝑎𝑖/𝜌𝑖. The radial bound gives
𝜌2𝑛𝑖 ≥1 −𝜅, while (1 −𝑡)𝐺𝑖𝑗 =1 −𝑡𝑛 gives |1 −𝑎𝑛𝑖―――𝑎𝑛𝑗| ≤2𝑛√𝜂
for 𝑖 ≠𝑗. Using |1 −𝑏𝑒𝑖𝜃|2 =(1 −𝑏)2 +𝑏|1 −𝑒𝑖𝜃|2
with 𝑏 =𝜌𝑛𝑖𝜌𝑛1 ≥1 −𝜅,
we obtain
|𝑢𝑛𝑖−𝑢𝑛1|≤2𝑛√𝜂√1−𝜅.
Choose the nearest 𝑛th-root phase
to 𝑢𝑖 among 𝑢1𝑒2𝜋𝑖𝑗/𝑛. The inequality |𝑒𝑖𝜃 −1| ≥2|𝜃|/𝜋 for |𝜃| ≤𝜋 shows that its distance
from 𝑎𝑖 is at most
𝑛𝜂𝑛−1+𝜋√𝜂√1−𝜅≤7√𝜂.
The separation bound exceeds 14√𝜂 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 𝐷 ≥1 −𝜂 with
𝜂 ≤1/(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 𝐷 ≥1 −𝜂 and 0 ≤𝜂 ≤1/(10𝑛4), the same source
proves
|𝑓(𝑠𝑢𝑖)|≤∏𝑘|𝑠𝑢𝑖−𝑢𝑘|(0≤𝑠≤𝜌𝑖).
The elementary step is
|𝑠𝑢𝑖−𝜌𝑘𝑢𝑘|2−|𝑠𝑢𝑖−𝑢𝑘|2=(1−𝜌𝑘)(2𝑠ℜ(𝑢𝑖―――𝑢𝑘)−1−𝜌𝑘).
Here
is where the discriminant hypothesis enters. The two bounds just proved
imply
|𝑎𝑖−𝑎𝑘|>1𝑛−1 (𝑖≠𝑘),1−𝜌𝑘≤𝑛𝜂𝑛−1<1(𝑛−1)2.
For 𝑘 =𝑖, the required inequality is 2𝑠 ≤1 +𝜌𝑖, which follows from 𝑠 ≤𝜌𝑖 ≤1. For 𝑘 ≠𝑖, it is immediate if ℜ(𝑢𝑖―――𝑢𝑘) ≤0. Otherwise
𝑠 ≤𝜌𝑖 gives
𝜌𝑘(2𝑠ℜ(𝑢𝑖―――𝑢𝑘)−1−𝜌𝑘)≤𝜌2𝑖−𝜌𝑘−|𝑎𝑖−𝑎𝑘|2≤1−𝜌𝑘−|𝑎𝑖−𝑎𝑘|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 𝑛 ≥2, the sufficient condition
0<𝜌𝑘≤1,𝜌𝑘≥2cos(2𝜋/𝑛)−1for every 𝑘
makes the same
factorwise comparison hold. Indeed, for 𝑘 ≠𝑖 with positive cosine, 𝑠 ≤1 gives 2𝑠ℜ(𝜁𝑖−𝑘) ≤2cos(2𝜋/𝑛) ≤1 +𝜌𝑘;
nonpositive cosines and 𝑘 =𝑖 are
handled as above. Since ∏𝑘(𝑧 −𝜔𝜁𝑘) =𝑧𝑛 −𝜔𝑛, we
obtain
|𝑓(𝑠𝜔𝜁𝑖)|≤1−𝑠𝑛(0≤𝑠≤𝜌𝑖).
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 2 ≤𝑛 ≤6 the lower bound on 𝜌𝑘 is nonpositive, so every choice of
positive radii at most one is allowed. For 𝑛 ≥7 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) =𝑧𝑛 −𝑟𝑛, 0 <𝑟 <1 and 𝑛 ≥2, 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 𝑛 ≥3, define 𝑟∗ =(1 +𝑐𝑛)−1/𝑛 and 𝜀 =(1 −𝑟𝑛)1/𝑛; in the
inner-chord case 𝑟 ≥𝑟∗, set
𝑡 =𝜀/𝑐 ≤𝑟.
Here is the chord estimate, including the smaller radii used in the
second construction. For 𝑛 ≥3, let
0 <𝑠 ≤𝑟. 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
0 ≤𝜃 <𝜋/𝑛. By symmetry
and continuity,
1+cos(𝑛𝜃)≤2cos𝑛𝜃(|𝜃|≤𝜋/𝑛).
Set 𝑢 =cos−𝑛𝜃 ≥1. Since 𝑧𝑛 = −(𝑠𝑐)𝑛𝑢𝑒𝑖𝑛𝜃, this
inequality gives
|𝑧𝑛−𝑟𝑛|2−(𝑟𝑛+(𝑠𝑐)𝑛)2≤(𝑢−1)(𝑠𝑐)𝑛((𝑠𝑐)𝑛(𝑢+1)−2𝑟𝑛)≤0.
The last step uses (𝑠𝑐)𝑛𝑢 ≤𝑠𝑛 ≤𝑟𝑛 and (𝑠𝑐)𝑛 ≤𝑟𝑛. 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/𝑐 ≤𝑟 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 2𝑟 −2𝑠(1 −sin(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 𝑛 ≥3, 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 𝑟 ≥𝑟∗, the two
radial legs and inner crossing have length
2𝑟−2𝜀tan(𝜋4−𝜋2𝑛)<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 𝑛 ≥3 with distinct
zeros on a circle of radius 𝜌.
If 2𝜌𝑛 ≤1, 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 𝜌 ≤2−1/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: 𝑧𝑛――――𝑔(1/――𝑧) is a
constant multiple of 𝑔(𝑧), with the
constant of modulus one. Equivalently, 𝑒−𝑖𝑛𝜃/2𝑔(𝑒𝑖𝜃) is real up
to a fixed phase. Choose
𝑐=(−1)𝑛+1∏𝑗𝑤𝑗,𝑞(𝑧)=𝑧𝑛−𝑐.
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
𝑔 −𝑞 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 𝑔 −𝑞. This is impossible: its degree is at
most 𝑛 −1, 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(𝜈―――――𝑧−𝑤𝑗)|𝑧−𝑤𝑗|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; 𝑛 ≥3 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| <2𝜌𝑛 ≤1 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 𝜌 ≤2−1/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) =𝑧3 −1/8 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 𝑧𝑛 −1, 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 1 ≤𝑟 <𝑚 and 𝑞 ≥1, and consider the translated monic
polynomial
𝑓(𝑧)=(𝑧−ℎ)𝑞𝑚+𝑎(𝑧−ℎ)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 =(𝑧 −ℎ)𝑞 reduces the root equation to
𝑤𝑚 +𝑎𝑤𝑟 +𝑐 =0. At such a quotient
root the middle coefficient can be eliminated exactly: for 0 ≤𝑢 ≤1,
𝑢𝑚𝑤𝑚+𝑎𝑢𝑟𝑤𝑟+𝑐=(1−𝑢𝑟)𝑐−(𝑢𝑟−𝑢𝑚)𝑤𝑚.
This is a nonnegative combination of
𝑐 and −𝑤𝑚, with weights 1 −𝑢𝑟 and 𝑢𝑟 −𝑢𝑚 summing to 1 −𝑢𝑚. The formal
radial-segment estimate gives strict containment when |𝑤| <1 and |𝑐| <1.
For 𝑞 ≥2 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)|≤(1−𝑡𝑞𝑚)max{|𝑐|,|𝑤|𝑚}<1(0≤𝑡≤1).
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.
With one additional monomial, Abel summation gives a sufficient
condition involving the two lower coefficients. Let
𝑔(𝑤)=𝑤𝑚+𝑎𝑤𝑟+𝑏𝑤𝑠+𝑐,𝑚>𝑟>𝑠≥1,
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 0 ≤𝑢 ≤1,
𝑔(𝑢𝑤)=(1−𝑢𝑠)𝑐+(𝑢𝑠−𝑢𝑟)(𝑐+𝑏𝑤𝑠)+(𝑢𝑟−𝑢𝑚)(−𝑤𝑚).
Here the root equation has eliminated 𝑎𝑤𝑟 before taking absolute values. The
three weights are nonnegative and sum to 1 −𝑢𝑚. 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 1 ≤𝑠 ≤𝑟 ≤𝑚; 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 𝑏 ≠0, |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=∑𝑖∈𝑆𝑤𝑠𝑖.
The squared-modulus
identity gives
∑𝑖∈𝑆|𝑐+𝑏𝑤𝑠𝑖|2=𝑁|𝑐|2+|𝑏|2∑𝑖∈𝑆|𝑤𝑠𝑖|2+2Re(――𝑐𝑏𝑀).
Consequently, if every
|𝑤𝑖| <1, |𝑐| <1, and
𝑁(|𝑏|2+|𝑐|2)+2Re(――𝑐𝑏𝑀)<𝑁−1,
then two distinct
indices 𝑖,𝑗 ∈𝑆 satisfy |𝑐 +𝑏𝑤𝑠𝑖| <1 and |𝑐 +𝑏𝑤𝑠𝑗| <1. Indeed, the displayed
identity bounds the sum of squared moduli strictly below 𝑁 −1. If at most one index had modulus
below one, the other 𝑁 −1 terms
would each contribute at least one. This explains both the threshold
𝑁 −1 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 𝑖 ↦𝑤𝑖 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 =𝑁 −1, 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)=(𝑤2−1/2)(𝑤3+4/5)=𝑤5−12𝑤3+45𝑤2−25
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 =∑𝑖𝑤2𝑖 =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 𝑞 ≥2 and 𝑓(𝑧) =𝑔((𝑧 −ℎ)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
1𝑞𝑞−1∑𝑗=0|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 𝑞 ≥2 be an integer, and set
𝑓(𝑧)=𝑃((𝑧−ℎ)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
1𝑞𝑞−1∑𝑗=0|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 |𝑤𝑖 −𝑤𝑗| <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 |𝑤𝑖 −𝑤𝑗|2/4 and
the other two factors are below 2,
so |𝑃(𝑤)| ≤|𝑤𝑖 −𝑤𝑗|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 0 ≤𝑡 ≤1, 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 𝑦 ↦𝑦𝑞.
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|𝛼−1|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)𝛼−1≤𝑥𝛼−1(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
𝛼∫𝐴0𝑥𝛼−1𝑑𝑥=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 0 ≤𝑎,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 ∘((𝑧 −ℎ)𝑞)
transfers containment from the quotient curve. Distinct quotient
endpoints give distinct roots of 𝑓.
This proves the path assertion in every degree 4𝑞 ≥8. 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<2√1−|ℎ|2≤2.
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.
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/(𝑛 −1) 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
𝑛 ≥3, the product estimate alone
cannot control a positive moment: a list 𝑇,𝑇−1,1,…,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/(𝑛−1)≤(𝑛−1)(|𝑓′(0)|2𝑛𝑛)1/(𝑛−1).
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 𝑛 ≥2, with roots in a closed disc of
radius 𝑅 ≥0. If 𝑐1,…,𝑐𝑛−1 are its critical
points counted with multiplicity, then
𝑛−1∑𝑗=1|𝑓(𝑐𝑗)|2/(𝑛−1)≤(𝑛−1)𝑅2𝑛/(𝑛−1).(7)
Consequently the lower exponents used elsewhere
in the record satisfy
𝑛−1∑𝑗=1|𝑓(𝑐𝑗)|1/(𝑛−1)≤(𝑛−1)𝑅𝑛/(𝑛−1)(8)
and
𝑛−1∑𝑗=1|𝑓(𝑐𝑗)|1/𝑛≤(𝑛−1)𝑅.
The constant is attained by 𝑓(𝑧) =(𝑧 −𝜏)𝑛 −𝜆 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
𝑚∑𝑗=1(𝑚∏𝑘=1|1−――𝑐𝑗𝑐𝑘|)2/𝑚≤𝑚,|𝑐𝑗|≤1.
The following pointwise bound explains why
these finite inequalities control critical values in every degree.
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)=𝑛∏𝑘(1−―――𝑐𝑘𝑧).
The numerator is the polar
derivative at 0: the conventional
polar derivative at 𝛼 is 𝑛𝑓(𝑧) +(𝛼 −𝑧)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|1−𝑎𝑖¯𝜁|2)≥𝑛2.
Writing the logarithmic derivative as 𝑤, the identity |𝑛 −𝑤|2 −|𝑤|2 =𝑛2 −2𝑛Re𝑤 ≤0
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|1−𝑟2――𝑐𝑗𝑐𝑘|.
Let 𝑟 ↑1. This also handles
boundary critical points and all multiplicities without selecting local
branches. ◻
Set 𝑚 =𝑛 −1. The weighted Poisson
proof below gives the quadratic finite inequality for every 𝑚 ≥1. Gauss–Lucas and Lemma 8.2 then
give ∑𝑗|𝑓(𝑐𝑗)|2/𝑚 ≤𝑚 on
the unit disc. Applying this to 𝑅−𝑛𝑓(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/(𝑛−1)≤𝑛−1,#{𝑗:𝑟𝑗≥𝑡𝑅}≤𝑛−1𝑡2𝑛/(𝑛−1)(𝑡>0).
The
counting bound follows by retaining just the indicated summands. The
fourth-power refinement proved below replaces the exponent 2𝑛/(𝑛 −1) here by 4𝑛/(𝑛 −1), improving the count for 𝑡 >1. For 0 <𝑡 ≤1 the trivial bound 𝑛 −1 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.
For one point 𝑐 of weight 1, the quantity to bound is (1 −|𝑐|2)2 ≤1; equality holds only at
𝑐 =0. For two points 𝑐, −𝑐 of equal weight, it is 1 −|𝑐|4 ≤1. These examples suggest why a
nonzero configuration should lose from equality. Now let 𝑤𝑗 ≥0, ∑𝑗𝑤𝑗 =1, and |𝑐𝑗| ≤1, with repetitions allowed.
Write 𝐺(𝑧) =∏𝑘|1 −―――𝑐𝑘𝑧|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)/|𝜁 −𝑐|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)=exp∑𝑗𝑤𝑗log(1−――𝑐𝑗𝑧)=1+∑𝜈≥1𝑎𝜈𝑧𝜈,𝑃=∑𝑗𝑤𝑗𝑃𝑐𝑗.
On the unit circle 𝑃 =1 −2ℜ(𝜁𝑔′/𝑔), by logarithmic
differentiation. The Poisson formula reproduces 𝑔(𝑐) from its boundary values and gives
∫𝑃𝑐 𝑑𝑚 =1 for |𝑐| <1. Expanding a square therefore
yields
∫|𝑔|2𝑃𝑐𝑑𝑚−|𝑔(𝑐)|2=∫|𝑔−𝑔(𝑐)|2𝑃𝑐𝑑𝑚≥0.
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=1−∑𝜈≥1(2𝜈−1)|𝑎𝜈|2.
To see the last equality,
expand |𝑔|2 and 𝜁𝑔′――𝑔 and integrate on
the circle. Orthogonality leaves 1 +∑𝜈≥1|𝑎𝜈|2 and ∑𝜈≥1𝜈|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 𝑟 ↑1 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 ∑𝑗𝑤𝑗――𝑐𝑗/(1 −――𝑐𝑗𝑧) =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)2 ≤1 give the quadratic
finite inequality above for every 𝑚 ≥1, 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 𝑀 ≤1. 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
𝑛𝑧𝑛−1 and the polynomial is
𝑧𝑛 −𝜆, with |𝜆| =1 forced by equality. Restoring
the centre and radius gives exactly 𝑓(𝑧) =(𝑧 −ℎ)𝑛 −𝜆 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 (𝑧 −ℎ)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+∑𝜈≥1𝑏𝜈𝑧𝜈.
For interior centres, logarithmic differentiation and the Poisson
majorant give
𝑃=1−4𝑝ℜ𝜁𝐻′𝑝𝐻𝑝,∑𝑗𝑤𝑗𝐺(𝑐𝑗)𝑝≤∫|𝐻𝑝|2𝑃𝑑𝑚=1−∑𝜈≥1(4𝜈𝑝−1)|𝑏𝜈|2.
The identity follows from the same two
orthogonality calculations used for 𝑔; only the coefficient of the derivative
term changes. For 0 <𝑝 ≤4 every
displayed coefficient is nonnegative. Hence
∑𝑗𝑤𝑗𝐺(𝑐𝑗)𝑝≤1(0<𝑝≤4).
Boundary centres follow by replacing 𝑐𝑗 by 𝑟𝑐𝑗: the degree-𝜈 coefficient becomes 𝑟𝜈𝑏𝜈, and the values on the left
are 𝐺𝑟(𝑟𝑐𝑗) =∏𝑘|1 −𝑟2―――𝑐𝑘𝑐𝑗|𝑤𝑘.
First retain finitely many nonnegative terms, then let 𝑟 ↑1. 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 =𝑛 −1,
1𝑚∑𝑗|𝑓(𝑐𝑗)|4/𝑚≤1𝑚∑𝑗𝐺(𝑐𝑗)4≤1
on the unit disc. For roots in ――𝐷(ℎ,𝑅) this becomes
∑𝑗|𝑓(𝑐𝑗)|4/(𝑛−1)≤(𝑛−1)𝑅4𝑛/(𝑛−1).
As before, 𝑅 >0 is handled by
𝑅−𝑛𝑓(ℎ +𝑅𝑧), and 𝑅 =0 by the vanishing of all critical
values. The constant is attained by (𝑧 −ℎ)𝑛 −𝜆 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 𝑏1 ≠0, the rational identity 𝐻′4/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/𝑝 −1 is negative, so the
nonnegative-deficit argument no longer applies. To extend its range we
can force the first Taylor coefficients to vanish. Let 𝑠 ≥1 be an integer and suppose
∑𝑗𝑤𝑗𝑐𝑘𝑗=0(1≤𝑘<𝑠).
The
expansion
log𝐻𝑝(𝑧)=−𝑝2∑𝑘≥1―――――∑𝑗𝑤𝑗𝑐𝑘𝑗𝑘𝑧𝑘
then has no terms
of degree below 𝑠, so 𝑏1 =⋯ =𝑏𝑠−1 =0. All remaining
coefficient weights are nonnegative for 0 <𝑝 ≤4𝑠. The same proof therefore
gives ∑𝑗𝑤𝑗𝐺(𝑐𝑗)𝑝 ≤1
throughout that range. For a monic polynomial with roots in ――𝐷(ℎ,𝑅), 𝑅 >0, the resulting endpoint is
∑𝑗|𝑓(𝑐𝑗)|4𝑠/(𝑛−1)≤(𝑛−1)𝑅4𝑠𝑛/(𝑛−1),∑𝑗(𝑐𝑗−ℎ)𝑘=0(1≤𝑘<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
1𝑛−1∑𝑗𝑐𝑗=1𝑛𝑛∑𝑖=1𝑧𝑖,
so this is also the root centroid. Recentring can increase
the required radius: for 0 <𝑟 <1, the roots of (𝑧 −𝑟)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/(𝑛 −1) 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/(𝑛 −1).
A uniform central region in every degree.
For every 𝑚 ≥1, the inequality
for points in a smaller disc proves
|𝑐𝑗|≤√1−𝑒−2(1≤𝑗≤𝑚)⟹𝑚∑𝑗=1(𝑚∏𝑘=1|1−――𝑐𝑗𝑐𝑘|)1/𝑚≤𝑚.
To see the mechanism, set ℎ𝑗 =𝑚−1∑𝑘log|1 −――𝑐𝑗𝑐𝑘|
and 𝐷𝑗 = −log(1 −|𝑐𝑗|2). Write
𝑀𝜈 =𝑚−1∑𝑘𝑐𝜈𝑘 for the
normalised complex power sums used in this calculation. The absolutely
convergent series for log(1 −𝑧)
gives
ℎ𝑗=−ℜ∑𝜈≥1――𝑐𝜈𝑗𝑀𝜈𝜈,−1𝑚∑𝑗ℎ𝑗=∑𝜈≥1|𝑀𝜈|2𝜈.
In
particular, ∑𝑗ℎ𝑗 ≤0.
Cauchy–Schwarz applied to the first series, using ∑𝜈≥1|𝑐𝑗|2𝜈/𝜈 =𝐷𝑗, gives
ℎ2𝑗 ≤( −𝑚−1∑𝑖ℎ𝑖)𝐷𝑗. The
radius bound gives 𝐷𝑗 ≤2. Put
𝑟 =√−𝑚−1∑𝑖ℎ𝑖. If
𝑟 =0, every ℎ𝑗 vanishes. For 𝑟 >0, convexity bounds 𝑒ℎ by the chord of its graph over [ −√2𝑟,√2𝑟]. Averaging and using
𝑚−1∑𝑗ℎ𝑗 = −𝑟2 gives
1𝑚∑𝑗𝑒ℎ𝑗≤cosh(√2𝑟)−𝑟√2sinh(√2𝑟)≤1.
For the
last inequality, the function cosh𝑢 −(𝑢/2)sinh𝑢 equals 1 at
𝑢 =0 and has derivative (sinh𝑢 −𝑢cosh𝑢)/2 ≤0 for 𝑢 ≥0. 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 √1−𝑒−2. 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 𝑚 ≥1, let |𝑐𝑖|2 ≤𝑎 <1, with 𝑎 ≥0, and put 𝐿 = −log(1 −𝑎). The uniform-radius
theorem gives the geometric-mean inequality
𝑒𝐿≤1+2𝐿⟹𝑚∑𝑖=1(𝑚∏𝑗=1|1−――𝑐𝑖𝑐𝑗|)1/𝑚≤𝑚.
For 𝑎 =1/2 the scalar
hypothesis holds, since 2 ≤1 +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 =𝑚−1∑𝑗log|1 −――𝑐𝑖𝑐𝑗|
and 𝐷𝑖 = −log(1 −|𝑐𝑖|2). The
preceding logarithmic calculation gives ∑𝑖𝐻𝑖 ≤0 and 𝐻2𝑖 ≤ −(𝐷𝑖/𝑚)∑𝑗𝐻𝑗. For
nonnegative upper bounds 𝑀𝑖 ≥𝐻𝑖, Taylor’s formula with integral remainder gives
𝑒𝐻𝑖≤1+𝐻𝑖+Φ(𝑀𝑖)𝐻2𝑖,Φ(𝑡)=∫10(1−𝑠)𝑒𝑠𝑡𝑑𝑠.
Since Φ(𝑀𝑖) ≥0, summing and using the
quadratic bounds yields
∑𝑖𝑒𝐻𝑖≤𝑚+(1−1𝑚∑𝑖Φ(𝑀𝑖)𝐷𝑖)∑𝑗𝐻𝑗≤𝑚
whenever ∑𝑖Φ(𝑀𝑖)𝐷𝑖 ≤𝑚. This is the
sufficient condition in the formal
inequality with individual upper bounds. Taking 𝑀𝑖 =𝐿 gives Φ(𝐿)𝐿 ≤1 as a sufficient condition,
since 𝐻𝑖,𝐷𝑖 ≤𝐿. For 𝐿 >0, integration gives Φ(𝐿) =(𝑒𝐿 −1 −𝐿)/𝐿2; hence this
condition is exactly 𝑒𝐿 ≤1 +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
4∑𝑗=1(4∏𝑘=1|1−―――𝑐𝑘𝑐𝑗|)1/4≤4,|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 𝜇 ≤𝑅𝑛. In the unit-disc normalisation 𝑅 =1, this does not force the smaller
quintic threshold 𝜇 <1/𝑀5
below. For 𝑓(𝑧) =𝑧𝑛 −1, 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 𝑛 ≥2 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 =𝑡 ≥0, and
order the distances as 0 <𝑑1 ≤𝑑2 ≤⋯ ≤𝑑𝑛. Logarithmic differentiation gives ∑𝑗(𝑧𝑗 −𝑐)−1 = −𝑓′(𝑐)/𝑓(𝑐) =0.
Dividing |𝑧𝑗 −𝑐|2 +2𝑡ℜ(𝑧𝑗 −𝑐) ≤1 −𝑡2 by 𝑑2𝑗, then summing and using the
reciprocal balance, gives
𝑛≤(1−𝑡2)∑𝑗𝑑−2𝑗.
Thus 𝑡 <1 and 𝑑1 ≤√1−𝑡2 ≤1. The same
reciprocal balance, with the nearest term isolated, gives 𝑑2 ≤(𝑛 −1)𝑑1.
Suppose 𝑑1 +𝑑2 >2. Since
𝑑2 ≤1 +𝑡, we have 𝑑1 >1 −𝑡, and hence
1−𝑡2<𝑑1(2−𝑑1)<𝑑1𝑑2.
The first
strict inequality uses that 𝑥(2 −𝑥)
is increasing on [0,1]. It follows
that
𝑛≤(1−𝑡2)(𝑑−21+(𝑛−1)𝑑−22)<𝑑2𝑑1+(𝑛−1)𝑑1𝑑2≤𝑛.
For the last
step, put 𝑥 =𝑑2/𝑑1 ∈[1,𝑛 −1] and
expand (𝑥 −1)(𝑥 −(𝑛 −1)) ≤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 +𝑑2 ≤2𝑅 <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 𝑛 ≥3 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
𝑀2𝑛=max0≤𝑡≤14−𝑛≤𝑦≤𝑛(1−𝑡)2((1−𝑡)2+2𝑡𝑦+𝑛(𝑛−2)𝑡2)⋅((1−𝑡)2+2𝑡(𝑛−𝑦)𝑛−2)𝑛−2.
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(𝑛 −2), suppose 𝑓(𝑐) ≠0, order the roots 𝑎1,…,𝑎𝑛 by distance from 𝑐, and set 𝑣𝑗 =(𝑎2 −𝑐)/(𝑎𝑗 −𝑐). Then 𝑣2 =1, |𝑣𝑗| ≤1 for 𝑗 ≥2, and ∑𝑗𝑣𝑗 =0 by 𝑓′(𝑐) =0. With 𝑦 =1 −ℜ𝑣1, this gives
𝑦=2+𝑛∑𝑗=3ℜ𝑣𝑗∈[4−𝑛,𝑛],|𝑣1|≤𝑛−1.
Consequently
|1−𝑡𝑣1|2≤(1−𝑡)2+2𝑡𝑦+𝑛(𝑛−2)𝑡2,1𝑛−2𝑛∑𝑗=3|1−𝑡𝑣𝑗|2≤(1−𝑡)2+2𝑡(𝑛−𝑦)𝑛−2.
The factor 𝑣2 =1 contributes (1 −𝑡)2. Applying AM–GM to the remaining
𝑛 −2 squared factors in 𝑓(𝑐 +𝑡(𝑎2 −𝑐))/𝑓(𝑐) =∏𝑗(1 −𝑡𝑣𝑗) gives
the defining expression for 𝑀2𝑛.
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 =(𝑎1 −𝑐)/(𝑎𝑗 −𝑐). Now 𝑥1 =1, |𝑥𝑗| ≤1 for every 𝑗, and ∑𝑗𝑥𝑗 =0. Hence
𝑛∑𝑗=2|1−𝑡𝑥𝑗|2≤(𝑛−1)(1+𝑡2)+2𝑡,
so AM–GM gives
|
|
|
|𝑓(𝑐+𝑡(𝑎1−𝑐))𝑓(𝑐)|
|
|
|2≤(1−𝑡)2((1−𝑡)2+2𝑡𝑛𝑛−1)𝑛−1.
This
bound is at most 𝑀2𝑛 for every
𝑛 ≥3, not just for numerically
tested degrees. Indeed, set 𝑦 =𝑛/(𝑛 −1) in the defining maximum. This
value is admissible because 𝑛/(𝑛 −1) −(4 −𝑛) =(𝑛 −2)2/(𝑛 −1) ≥0. The last
factor then has base (1 −𝑡)2 +2𝑡𝑛/(𝑛 −1), and the preceding
factor has this same base plus 𝑛(𝑛 −2)𝑡2 ≥0. 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=(1−𝑡∗)(1+𝑡∗)3√16𝑡2∗−4𝑡∗+1,𝑡∗=516+3√10580,1𝑀5=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=(1−𝑡)2+2𝑡𝑦+15𝑡2,𝐵=(1−𝑡)2+2𝑡(5−𝑦)3.
They are positive for −1 ≤𝑦 ≤5, and 𝜕𝑦log(𝐴𝐵3) =2𝑡(𝐵 −𝐴)/(𝐴𝐵). Thus
the unconstrained maximum occurs at 𝐴 =𝐵, or 𝑦 =5/4 −45𝑡/8. This reaches the lower
endpoint −1 at 𝑡 =2/5; thereafter the maximum is at 𝑦 = −1. For 0 ≤𝑡 ≤2/5 the resulting expression is
(1 −𝑡)(1 +𝑡/2 +19𝑡2/4)2, whose
derivative is
5𝑡(14−19𝑡)(19𝑡2+2𝑡+4)16≥0.
For 2/5 ≤𝑡 ≤1, the square of the
resulting expression is (1 −𝑡)2(1 +𝑡)6(16𝑡2 −4𝑡 +1), whose
derivative is
−4𝑡(1−𝑡)(1+𝑡)5(40𝑡2−25𝑡−2).
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
𝑧5 −𝑏 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+𝜖3𝑧3−𝜖3𝑧2−𝜖5𝑧−1,𝐹𝜖(𝑧)=𝑟5𝑃𝜖(𝑧/𝑟),𝑟=1−𝜖9.
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
𝑧5―――――𝑃𝜖(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 𝑧5 −1, since the first coefficient
perturbations have order 𝜖3.
For 𝜁0 =1,𝑒4𝜋𝑖/5,𝑒−4𝜋𝑖/5, take 𝑡 =𝜖/4.
Substitution into the polynomial gives
|𝐹𝜖(𝑟𝑡𝜁𝜖)|2=1+(ℜ𝜁208−1512)𝜖5+𝑂(𝜖6).
The coefficient is positive, since ℜ𝜁20 ≥(√5 −1)/4. For the
remaining roots, with 𝜁0 =𝑒2𝜋𝑖/5 or 𝑒−2𝜋𝑖/5,
take 𝑡 =𝜖2/4 instead. Then
|𝐹𝜖(𝑟𝑡𝜁𝜖)|2=1+3√5−532𝜖7+𝑂(𝜖9)>1
for
sufficiently small 𝜖. The
two scales are needed because ℜ𝜁20 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: 𝑃′𝜖(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 ℎ ∈ℂ 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.
The following calculation applies in every degree 𝑛 ≥2, 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 +𝑐𝑛−2𝑧𝑛−2 +⋯, 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|𝜓−1|
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 𝜁𝑛−1 coefficient forces
the constant Laurent coefficient of 𝜓 to vanish. Thus
𝜓(𝜁)=𝑡1/𝑛𝜁+∑𝑘≥1𝑎𝑘𝜁−𝑘.
Grönwall’s area identity takes the form
Area(𝐾𝑡)=𝜋(𝑡2/𝑛−∑𝑘≥1𝑘|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/𝑛𝑟2 −∑𝑘≥1𝑘|𝑎𝑘|2𝑟−2𝑘).
These enclosed compact sets decrease to 𝐾𝑡 as 𝑟 ↓1; continuity of area from
above and monotone convergence of the series give the identity.
Comparing the coefficient of 𝜁𝑛−2 in the exterior identity now
gives
𝑛𝑡(𝑛−1)/𝑛𝑎1+𝑐𝑛−2𝑡(𝑛−2)/𝑛=0,𝑎1=−𝑐𝑛−2𝑛𝑡1/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,𝑅≈1.021393477405696164,
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)=𝑅−5𝑓0(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(𝑐0−ℎ𝑅)≈2.01425143287505,|
|
|
|𝐹(𝑐0−ℎ𝑅)|
|
|
|≈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(𝑛 −1)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
𝑛−1∑𝑘=1|𝑓(𝑐𝑘)|1/𝑛≤(𝑛−1)𝑅
is proved for every 𝑛 ≥2 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 𝑛 ≥2, 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 𝑓𝑗 →𝑓 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,
𝑀∑ℓ=1|𝛾(𝑡ℓ)−𝛾(𝑡ℓ−1)|=lim𝑗𝑀∑ℓ=1|𝛾𝑗(𝑡ℓ)−𝛾𝑗(𝑡ℓ−1)|≤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 Λ ≤2 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) =𝑧𝑛 −1, the inequality
|𝑧𝑛 −1| ≤1 implies 2ℜ(𝑧𝑛) ≥|𝑧|2𝑛 >0 whenever 𝑧 ≠0. 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(𝑧𝑛−1)=2(𝑓∈K𝑛).
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,𝑁≥1,0<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 𝑁 ≥2, the
root centroid of 𝐹𝑁 is −𝑏/2, as its 𝑧2𝑁−1 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 <𝜆 ≤1, 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 =𝑒−𝛼𝑁/𝑁 with fixed 𝛼 >0, the same section instead
proves Λ(𝐹𝑁) →2(1 −𝑒−𝛼/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 𝐼 ⊆ℝ 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 :𝐼 →ℂ 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 =𝑓 ∘𝑧, 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−(𝑡−𝑡0)𝑓(𝑧(𝑡0)),𝑡0≤𝑡,𝑡0,𝑡∈𝐼.
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 𝑡 ↦𝑓(𝑧(𝑡)) be continuous on [𝑎,𝑏]. Assume the Newton equation and
𝑓′(𝑧(𝑡)) ≠0 on (𝑎,𝑏) only. Then
𝑓(𝑧(𝑏))=𝑒𝑎−𝑏𝑓(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)=𝑧3−316𝑧+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))=564𝑒−𝑡,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 𝑎 ≠𝑏 be complex. Every common
translation 𝛽 for which 𝑎 +𝛽 and 𝑏 +𝛽 lie on the same positive ray has
the form
𝛽=𝑟𝑎−𝑏1−𝑟,𝑟∈ℝ>0, 𝑟≠1.
Indeed, write 𝑏 +𝛽 =𝑟(𝑎 +𝛽)
with 𝑟 >0. Since 𝑎 ≠𝑏, one has 𝑟 ≠1, and solving for 𝛽 gives the displayed formula.
Equivalently, 𝛽 = −𝑎 +(𝑎 −𝑏)/(1 −𝑟),
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,…,𝑐𝑛−1 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 𝑧𝑛 −𝑎, 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 𝑚 ≥2 simple zeros, and the regularity
and Morse hypotheses in that proposition, it constructs, for every 𝜀 >0, an embedded spanning
tree 𝐺𝜀 ⊂𝑉 with
len(𝐺𝜀)≤12𝜋∫∞2𝛼𝑃𝑉(𝑡)𝑑𝑡+𝜀.(5.1)
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) =𝑧2 −𝑎2 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 =𝑒−𝑡. On a regular level the inverse
parametrisations 𝑧 = ±√𝑎2+𝑟𝑒𝑖𝜃 give
𝑃𝑉(𝑡)=𝑟∫2𝜋0|𝑎2+𝑟𝑒𝑖𝜃|−1/2𝑑𝜃.
The elementary identity
|𝑎2+𝑟𝑒𝑖𝜃|2=(𝑎2+𝑟)2cos2(𝜃/2)+(𝑎2−𝑟)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 4∫𝜋/20(cos𝑠)−1/2 𝑑𝑠, and
cos𝑠 ≥1 −2𝑠/𝜋 bounds the latter
integral by 4𝜋. Changing
variables from 𝑡 to 𝑟 therefore gives
12𝜋∫∞2𝛼𝑃𝑉(𝑡)𝑑𝑡≤2∫𝑎0𝑑𝑟√𝑎2+𝑟=4(√𝑎2+𝑎−𝑎)<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 9/5 −41/25 =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)+𝑥2−𝑦2
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 𝑝 ∈𝑉 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 𝑧𝑛 −𝑏 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 𝑘 ≥2 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:
−log|𝑓| :𝑈\𝑓−1(0) →(0,∞)
is a proper excellent Morse function, with exactly 𝑘 −1 nondegenerate saddles;
cutting 𝔻 ∖{0} along the critical-value rays decomposes
its preimage in 𝑈 into conformal
strips;
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;
for each critical point 𝑐 ∈𝑈, 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 :𝑈 →𝔻 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 𝑘 −1 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 𝑘 −1 values. Each remaining
sector is simply connected and contains no branch value of 𝑓 :𝑈 →𝔻, 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) :1 ≤𝑡 <1/|𝑓(𝑐)|}, for
critical points 𝑐 ∈𝑈. 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 𝑘 −1 transpositions therefore give a
connected graph with 𝑘 vertices,
which is a tree.
For 𝑐 ∈𝑈, the inward segment
from 𝑓(𝑐) to 0 contains no other branch value of 𝑓 :𝑈 →𝔻, 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(𝑠−1/2), 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)=(𝑧2−4)2−14.
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,
−1/4 ≤𝑓 ≤0. But 𝑓(𝑖𝑦) =(𝑦2 +4)2 −1/4 >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(𝑣 −𝑢), 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 𝑧2 −𝑎2 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 𝑥2 −𝑦2, 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
Γ𝑆𝑡=𝑆∩{𝑢=𝑡},𝑃𝑆(𝑡)=H1(Γ𝑆𝑡),
and write
Φ𝑆(𝑡)=∫Γ𝑆𝑡|∇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
∫Γ𝑆𝑡0len(𝛾𝑥)𝑑𝜇𝑡0(𝑥)=∫𝑏𝑆𝑎𝑆∫Γ𝑆𝑡1|∇𝑢||∇𝑢|Φ𝑆(𝑡0)𝑑𝑠𝑑𝑡=1Φ𝑆(𝑡0)∫𝑏𝑆𝑎𝑆𝑃𝑆(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 =𝑟 𝑑𝜙, 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.
Produce an embedded tree 𝐺 containing all 𝑚 roots whose length obeys
len(𝐺)≤𝐶∫∞2𝛼𝑃𝑉(𝑡)𝑑𝑡+𝜂(6.1)
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.
Connect only one pair of distinct roots, rather than spanning
every root.
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) =𝑧2 −𝑎2, 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)≤2𝜋𝑒−𝑡√𝑎2−𝑒−𝑡.
Consequently ∫∞2𝛼𝑃𝑉(𝑡) 𝑑𝑡 →0 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=12𝜋∫2𝛼𝛼𝑃𝑉(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 𝑛 ≥1, 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)=0⟹∏𝑓(𝑏)=0|𝑧−𝑏|=|𝛽|⟹min𝑓(𝑏)=0|𝑧−𝑏|≤|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 deg𝑓 ≥2, 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)satisfy𝑣′𝑗(𝜆)=𝑐𝑗(𝜆).
Thus
𝑣𝑖 −𝑣𝑗 cannot vanish identically
for 𝑖 ≠𝑗, 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
2ℜ((𝑣𝑖−𝑣𝑗)――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:
𝑓 +𝜆𝑧 has simple
relevant critical points and injective complex critical
values;
the checked constant translation 𝛽 makes those values nonzero and
pairwise ray-separated;
no critical point enters the protected collar or truncation
boundary;
the relevant component remains in 𝐾, contains exactly the corresponding
perturbed roots and has slack 𝑞𝑔 >𝑞/2; and
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−(𝑡−𝑡0)𝑝(𝑧(𝑡0)),𝑢(𝑧(𝑡))=𝑢(𝑧(𝑡0))+𝑡−𝑡0,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′)(𝑝′≠0).
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:𝑎≤𝑢(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) =𝑧2 −1/4 and the compact band
log2≤−log|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/(2√2)],𝑑𝑥𝑑𝜏=2𝑥1/4−𝑥2.
Integration gives 𝜏 −𝜏0 =18log(𝑥/𝑥0) −(𝑥2 −𝑥20)/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.
Lean checks exact formal statements, not citation choices or
mathematical priority. The formal-source index records the complete
quadratic weighted inequality, the exponent-2/(𝑛 −1) 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.
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
𝜇 ≤529/1000. 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 𝛿 ≈0.4586751, 𝐷 ≈5.3770730, and 𝑑low ≈2.1700770; 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+(𝑘−1)𝜆(𝐷−𝑑low),𝑘artanh(𝑒−2)},
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 10−3 and a geometric grid of 40 initial areas from 10−6 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 𝑒−0.607 =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 𝑑𝑗 ≥𝑑low 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 𝜇 ≤529/1000. 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/(𝑛 −1) 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.
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