The short paper
develops the counterexample and the trinomial argument. Here
Section 2 supplies
the exact tests for the polynomial, while Sections 6 and 9 give
further explicit paths. The area argument in Section 4 and the
isolated-value construction in Section 7 are
ordinary analytic proofs, still requiring formalisation. Their
conclusions appear as remarks. The local notes identify the assumptions
of the existing Lean deductions; Section C collects the
formal and computational references.
The question and the degree-seven counterexample
For a monic polynomial 𝑓, let
Ω𝑓 ={|𝑓| <1}; the notation
𝐸𝑓 used in the segment arguments
denotes the same open set. We write 𝐾𝑡(𝑓) ={|𝑓| ≤𝑡} for a closed
sublevel. Erdős, Herzog and Piranian [4] asked:
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}?
Boundary roots already give an elementary failure of strict
containment. For 𝑓(𝑧) =𝑧2 −1, every
continuous path from −1 to 1 meets the imaginary axis, where |𝑓(𝑖𝑦)| =1 +𝑦2 ≥1. The two endpoints are
therefore unjoinable in {|𝑓| <1}, although the diameter lies
in {|𝑓| ≤1}. This illustrates
the distinction between the open and closed lemniscates.
A repeated zero gives a constant path between two occurrences. Thus
the question concerns distinct zeros. The catalogue of Bloom [3] records the problem and its
discussion. Pendyala [11] proved the degree-four case by chords or
radial segments through the centre of a smallest enclosing disc. The
degree-seven construction of ani
has a different geometry.
Theorem 1.2 (ani’s counterexample).
The monic polynomial in (2) has seven distinct
roots in the open unit disc. Every connected subset of its strict unit
lemniscate containing two roots has one-dimensional Hausdorff measure
greater than 2.
Five components contain one zero each; the remaining component
contains two, and the polynomial has degree two on it. A quadratic
estimate near its critical point counts two inverse images, with
multiplicity, for each value on an outward slit. Since the component has
degree two, these are all its inverse images of that value. Hence the
entire preimage of the slit in the component lies in the small disc
where the local estimate applies.
On each of the two inverse sheets, radial projection gives a lower
bound for the Hausdorff measure of a connected set joining the zeros.
The sheets are disjoint, so the two bounds can be added. Their sum
exceeds 2. Section 2 supplies
the estimates and proof. Applied to a continuous path image, this also
excludes a rectifiable path of total variation less than 2.
The theorem concerns a fixed polynomial. The small-parameter family
reported by ani is not proved here, and independent human
review of correspondence with the 1958 wording is not recorded. The
supplied formal statements and their scope are listed in Section C.
For trinomials the root identity keeps every root-to-origin segment
inside the lemniscate, giving a short broken line between any pair of
zeros. The later analytic remarks seek a pair by following sublevel
components: one argument uses a small least critical-value modulus, and
another uses an isolated simple critical value. Their conclusions have
additional formalisation requirements. A bound on critical-value means
alone makes no choice of a contained path.
The degree-seven construction
The construction has two separate quantitative requirements. The two
roots in the selected component must have combined distance from its
critical point greater than 2, and
the preimage of an outward value slit must be small enough to preserve
that surplus. A narrow neck alone would not suffice: for 𝑝(𝑧) =𝑧2 −𝑟2, 0 <𝑟 <1, the slit ( −1, −𝑟2] has preimage {𝑖𝑦 :|𝑦| <√1−𝑟2}, while the
root segment [ −𝑟,𝑟] still has
length 2𝑟 <2 and lies in {|𝑝| <1}.
We first prove the estimate that separates these requirements. We
then verify root locations, critical values and the membership of the
chosen pair in one component. The final fixed-parameter estimates
compare the root-distance surplus with the neck loss, and distinguish
both from the radial contraction 1 −𝜌 =𝜀8.
A two-sheeted component
The quantity 𝛿 =1 −|𝑝(𝑐)|
measures the remaining length of the slit in the value plane. The local
quadratic coefficient converts it into the spatial scale √𝛿/𝑀. The radius ℎ records where that quadratic comparison
is valid. Degree two will turn the local preimage estimate into a
statement about the whole component.
Lemma 2.1 (a bottleneck estimate). Let 𝑝 be a polynomial and 𝑈 a component of {|𝑝| <1} on which 𝑝 is a proper map of degree two. Suppose
its only critical point 𝑐 is simple
and 𝑣 =𝑝(𝑐) ≠0. Write
𝑝(𝑐+𝑧)−𝑣=𝑧2𝐴(𝑧),𝑀=|𝐴(0)|,𝛿=1−|𝑣|.
Suppose ℎ >0, |𝐴(𝑧)/𝐴(0) −1| ≤1/4 for |𝑧| ≤ℎ, and 𝛿 <𝑀ℎ2/4. If 𝑎,𝑏 are the two zeros in 𝑈, every connected 𝐾 ⊂𝑈 containing 𝑎,𝑏 satisfies
H1(𝐾)≥|𝑎−𝑐|+|𝑏−𝑐|−83√𝛿/𝑀.
Proof. Cut the value disc along 𝐽 ={𝑡𝑣 :1 ≤𝑡 <1/|𝑣|}. Its complement
is simply connected and contains 0.
The restriction of 𝑝 above this
complement is an unramified two-sheeted covering, hence is the disjoint
union of two biholomorphic sheets 𝑈1,𝑈2, containing 𝑎,𝑏 respectively.
Put 𝑟0 =(4/3)√𝛿/𝑀 <2ℎ/3. On
|𝑧| =𝑟0,
|𝑝(𝑐+𝑧)−𝑣|≥34𝑀𝑟20=43𝛿>𝛿.
For each 𝑤 ∈𝐽, Rouché’s theorem
therefore gives two zeros, counted with multiplicity, of 𝑝(𝑐 +𝑧) −𝑤 in |𝑧| <𝑟0. They remain in 𝑈: as 𝑤 moves out from 𝑣 along 𝐽, the zeros continue from 𝑐 and cannot cross |𝑧| =𝑟0. Since the degree on 𝑈 is two, these are all its preimages of
𝑤. Consequently 𝑝−1(𝐽) ∩𝑈 ⊂𝐵(𝑐,𝑟0).
For 𝑟0 <𝑡 <|𝑎 −𝑐|, the set
𝑈1 ∩{|𝑧 −𝑐| >𝑡} has relative
boundary in 𝑈 contained in the
circle |𝑧 −𝑐| =𝑡. If that circle
missed 𝐾 ∩𝑈1, then 𝐾 ∩𝑈1 ∩{|𝑧 −𝑐| >𝑡} would be both
open and closed in 𝐾. It contains
𝑎 and excludes 𝑏, contradicting connectedness. Thus the
radial map 𝑧 ↦|𝑧 −𝑐| sends
𝐾 ∩𝑈1 onto a set containing
(𝑟0,|𝑎 −𝑐|) whenever that interval
is nonempty. This map is 1-Lipschitz, so
H1(𝐾∩𝑈1)≥(|𝑎−𝑐|−𝑟0)+.
The same argument applies to 𝑏 and 𝑈2. Although the two radial intervals
can overlap on the real line, the sets 𝐾 ∩𝑈1 and 𝐾 ∩𝑈2 lie in
disjoint open subsets of the plane. Hausdorff outer measure adds across
that separation, even when 𝐾 is not
assumed measurable. Consequently
H1(𝐾)≥H1(𝐾∩𝑈1)+H1(𝐾∩𝑈2)≥(|𝑎−𝑐|−𝑟0)++(|𝑏−𝑐|−𝑟0)+≥|𝑎−𝑐|+|𝑏−𝑐|−2𝑟0.
Substituting the value of 𝑟0 proves the bound. Connectedness
supplied the intervals; no path or parametrisation of 𝐾 was required. ◻
The diagram
in the short paper distinguishes the value-plane slit from the two
radial projections used above.
Polynomial and roots
The perturbation of 𝑧7 −1 is
small on the unit circle but has a nontrivial shape at 𝑧 =𝜀𝑤: the terms 𝜀4𝑎𝑧3, 𝜀5𝑏𝑧2 and 𝜀6𝑐0𝑧 all become order 𝜀7 there. The paired conjugate
terms give the antisymmetry used to locate the roots. These two features
let us control roots near the unit circle and critical points near the
origin by different tests.
All constants are rational, so both sets of tests can be made without
rounding. Set
𝑠=10−6,𝜀=𝑠2=10−12,𝜌=1−𝑠16=1−10−96,
𝐴0=−3295071600,𝐵0=551827800,𝐶0=−2301381332000,
and define
𝑎=𝐴0−𝑖𝑠,𝑏=𝑖𝐵0+95𝑠,𝑐0=−𝐶0−16225𝑖𝑠.
The polynomial is
𝐹(𝑧)=𝑧7−1+𝜀4(𝑎𝑧3−¯𝑎𝑧4)+𝜀5(𝑏𝑧2−¯𝑏𝑧5)+𝜀6(𝑐0𝑧−¯𝑐0𝑧6),𝑓(𝑧)=𝜌7𝐹(𝑧/𝜌).(1)(2)
The identity 𝐹(𝑧) = −𝑧7―――――𝐹(1/¯𝑧) is
useful, but does not by itself place the zeros on the unit circle. For
that purpose put 𝜒(𝑥) =(1 +𝑖𝑥)/(1 −𝑖𝑥). Direct expansion
gives (1 −𝑖𝑥)7𝐹(𝜒(𝑥)) =2𝑖𝐻(𝑥),
where
𝐻(𝑥)=7𝑥−35𝑥3+21𝑥5−𝑥7−𝜀4(1+𝑥2)3(𝑠+𝐴0𝑥)+𝜀5(1+𝑥2)2[𝐵0(1−3𝑥2)+(9𝑠/5)(𝑥3−3𝑥)]+𝜀6(1+𝑥2)[𝐶0(5𝑥−10𝑥3+𝑥5)−(162𝑠/25)(1−10𝑥2+5𝑥4)].
The signs at the following rational endpoints are
obtained by substitution. Both endpoints in each row are divided by
104.
| 𝑗 |
Left endpoint |
Right endpoint |
Left sign |
Right sign |
| 0 |
−1 |
1 |
− |
+ |
| 1 |
4815 |
4816 |
+ |
− |
| 2 |
12539 |
12540 |
− |
+ |
| 3 |
43812 |
43813 |
+ |
− |
| 4 |
−43813 |
−43812 |
+ |
− |
| 5 |
−12540 |
−12539 |
− |
+ |
| 6 |
−4816 |
−4815 |
+ |
− |
The seven intervals give distinct real zeros 𝑥𝑗 of 𝐻, so 𝜁𝑗 =𝜒(𝑥𝑗) are all seven zeros of
𝐹. They have modulus one. Hence the
zeros 𝑏𝑗 =𝜌𝜁𝑗 of 𝑓 are distinct and lie in the open unit
disc.
Critical points and local estimates
The critical points cluster at scale 𝜀. We resolve them by writing
𝐹(𝜀𝑤) = −1 +𝜀7𝑄(𝑤), where
𝑄(𝑤)=𝑐0𝑤+𝑏𝑤2+𝑎𝑤3−𝜀¯𝑎𝑤4−𝜀3¯𝑏𝑤5−𝜀5¯𝑐0𝑤6+𝑤7.
For a centre 𝑣𝑗, let 𝑇𝑘(𝑣𝑗) be the coefficient of 𝑧𝑘 in 𝑄(𝑣𝑗 +𝑧). If 𝑄(𝑤) =∑𝑞𝑘𝑤𝑘, these coefficients are
given by the finite formula
𝑇𝑘(𝑣𝑗)=7∑ℓ=𝑘(ℓ𝑘)𝑞ℓ𝑣ℓ−𝑘𝑗.
Use the following centres, whose displayed
decimals are exact, and radius 𝑟 =10−6:
| 𝑗 |
Re𝑣𝑗 |
Im𝑣𝑗 |
| 0 |
3.1898275786 |
−0.4999999979 |
| 1 |
−3.1898275845 |
−0.5000000021 |
| 2 |
0.0000000039 |
0.8232474662 |
| 3 |
0.0000002274 |
1.8078590858 |
| 4 |
−0.0000002265 |
1.8838591455 |
| 5 |
0.0000000011 |
−3.5149656976 |
These six discs are disjoint. For a Gaussian rational 𝑧 =𝑢 +𝑖𝑣, put 𝑁(𝑧) =|𝑢| +|𝑣| and 𝑚(𝑧) =max(|𝑢|,|𝑣|), so 𝑚(𝑧) ≤|𝑧| ≤𝑁(𝑧). Define
𝐸𝑗=𝑁(𝑇1(𝑣𝑗))+6∑𝑘=2(𝑘+1)𝑁(𝑇𝑘+1(𝑣𝑗))𝑟𝑘,𝐿𝑗=2𝑚(𝑇2(𝑣𝑗))𝑟.
The next table proves 𝐸𝑗 <𝐿𝑗 in every disc. Rouché’s
theorem, applied to the linear term of 𝑄′, gives exactly one critical point
in each.
To determine its critical-value modulus, use
ℋ(𝑤)=1−𝜌142𝜌14𝜀7+Re𝑄(𝑤)−𝜀72|𝑄(𝑤)|2,|𝑓(𝜌𝜀𝑤)|2=1−2𝜌14𝜀7ℋ(𝑤).
For |𝑤 −𝑣𝑗| ≤𝑟, set 𝑉𝑗 =∑7𝑘=1𝑁(𝑇𝑘(𝑣𝑗))𝑟𝑘.
Substituting Re𝑇0(𝑣𝑗) ±𝑉𝑗 for Re𝑄(𝑤) and 𝑁(𝑇0(𝑣𝑗)) +𝑉𝑗 for |𝑄(𝑤)| gives the following rational
bounds. An interval in the last column contains 109ℋ(𝑤) throughout the whole
disc.
| 𝑗 |
109𝐸𝑗 < |
106𝐿𝑗 > |
109ℋ(𝑤) |
| 0 |
423 |
8340 |
[ −502, −486] |
| 1 |
433 |
8340 |
[ −502, −486] |
| 2 |
12 |
378 |
[3556,3558] |
| 3 |
3 |
43 |
[ −75, −74] |
| 4 |
4 |
48 |
[ −864, −863] |
| 5 |
1298 |
16812 |
[ −1566, −1548] |
It follows that 𝑓 has just one
critical point in {|𝑓| <1},
namely 𝑐𝑠 =𝜌𝜀𝑤𝑠 with
|𝑤𝑠 −𝑣2| <𝑟. Its critical value
is nonzero, since the polynomial has simple roots, and no critical point
lies on |𝑓| =1.
Expanding the same Taylor coefficients throughout |𝑤 −𝑣2| ≤𝑟 gives
|𝑇2(𝑤)|>189.1,(|𝑇3(𝑤)|,|𝑇4(𝑤)|,|𝑇5(𝑤)|,|𝑇6(𝑤)|,|𝑇7(𝑤)|)<(190,20,15,6,2).
In the last coordinate the exact value is
|𝑇7| =1. In particular, for ℎ =𝜌𝜀/10 and 𝑓(𝑐𝑠 +𝑧) −𝑓(𝑐𝑠) =𝑧2𝐴𝑠(𝑧),
|𝐴𝑠(0)|>180𝜌5𝜀5,|
|
|
|𝐴𝑠(𝑧)𝐴𝑠(0)−1|
|
|
|<14(|𝑧|≤ℎ).(3)
Indeed the numerator of the relative error is at
most 190/10 +20/100 +15/1000 +6/104 +1/105 <189.1/4
in scaled coordinates. The positive critical-value bound in the table
also gives
0<𝛿=1−|𝑓(𝑐𝑠)|≤1−|𝑓(𝑐𝑠)|2<𝜌7𝜀7365⋅106.
Consequently
√𝛿/|𝐴𝑠(0)|<𝜌𝜀5000,𝛿<|𝐴𝑠(0)|ℎ2/4.(4)
The two roots in the component
The local estimates identify a critical point, but we still have to
find the two roots in its component. The connections from 𝑐𝑠 to 𝑏3,𝑏6 use a small disc and four
segments near the critical point, short segments to the root directions,
and radial segments out to the roots. The following ordinary argument
identifies the component directly; the Lean source uses barriers. Put
Re𝑤𝑞=392265832599170384843469532006471040,Im𝑤𝑞=82324746619448489536729178494728000780831040,𝑥3=𝑤𝑞−6+3𝑖,𝑥6=𝑤𝑞+5−5𝑖,𝑚3=−720775094321935300989+347106991294046496381𝑖1020,𝑚6=498791841486986824420−625465185974423846967𝑖1020.
The elementary inequality 1 −𝜌14 ≥14𝜌14𝜀8
shows that
ℋ0(𝑤)=7𝜀+Re𝑄(𝑤)−𝜀72|𝑄(𝑤)|2≤ℋ(𝑤).
Thus ℋ0 >0 suffices for containment. To check a segment from
𝑢 to 𝑣, expand ℋ0(𝑢 +𝑡(𝑣 −𝑢)) =∑14𝑘=0𝑎𝑘𝑡𝑘. Its Bernstein coefficients
of degree 14 are
𝛽𝑗=𝑗∑𝑘=0𝑎𝑘(𝑗𝑘)(14𝑘),ℋ0(𝑢+𝑡(𝑣−𝑢))=14∑𝑗=0𝛽𝑗(14𝑗)𝑡𝑗(1−𝑡)14−𝑗.
All
weights on the right are nonnegative and sum to one for 0 ≤𝑡 ≤1. Exact substitution gives the
lower bounds
| Segment |
Lower bound for every 𝛽𝑗 |
| [𝑤𝑞,𝑥3] |
3556874/1012 |
| [𝑥3,𝑚3] |
640506 |
| [𝑤𝑞,𝑥6] |
3556874/1012 |
| [𝑥6,𝑚6] |
139485 |
The formula for 𝑇𝑘 above,
followed by the displayed formula for 𝛽𝑗, specifies these checks using
rational arithmetic alone; no sampling between endpoints is involved.
The same Taylor test at 𝑤𝑞, with
radius 10−8, gives one zero of
𝑄′ in that disc and ℋ0 >3556874/1012
throughout it. The disc is contained in |𝑤 −𝑣2| <10−6, so this zero is 𝑤𝑠. For each 𝑗 =3,6, we can therefore follow the
segments from 𝑤𝑠 to 𝑤𝑞, then to 𝑥𝑗 and 𝑚𝑗, staying where ℋ0 >0. It remains to connect
𝑚𝑗 to the corresponding root.
For the remaining segments no large polynomial expansion is needed.
The Cayley intervals give |𝑚𝑗/8 −𝜁𝑗| <1/10 and |𝑚𝑗/8| <101/100, for 𝑗 =3,6. If 𝑥 lies between 𝑚𝑗/8 and 𝜁𝑗, then |𝑥| ≤101/100 and |𝑥 −𝜁𝑗| <1/10. From 𝐹(𝜁𝑗) =0 and |𝜁𝑗| =1 we have |𝜁7𝑗 −1| <10−40. Telescoping
𝑥7 −𝜁7𝑗 therefore gives
Re𝑥7≥1−710(101100)6−10−40>14.
The coefficient bounds
(|𝑞1|,…,|𝑞7|)≤(720,690,206,10−9,10−30,10−55,1)=:(𝑈1,…,𝑈7)
imply
6∑𝑘=1𝑈𝑘(8.08)𝑘<160000,Re𝑄(8𝑥)>350000,|𝑄(8𝑥)|<2500000.
Hence ℋ0(8𝑥) >0. This
connects 𝑚𝑗 to 8𝜁𝑗. Finally, for 8𝜀 ≤𝑡 ≤1, the root equation
gives
𝐹(𝑡𝜁𝑗)=𝑡7−1+6∑𝑘=1𝜀7−𝑘𝑞𝑘𝜁𝑘𝑗(𝑡𝑘−𝑡7),
so
|𝐹(𝑡𝜁𝑗)|≤1−𝑡7+𝑡76∑𝑘=1𝑈𝑘87−𝑘<1,6∑𝑘=1𝑈𝑘87−𝑘<340.
Scaling
by 𝜌 joins 𝜌𝜀 8𝜁𝑗 to 𝑏𝑗 within {|𝑓| <1}. The concatenated segments
connect 𝑐𝑠 to both roots.
Every component of a polynomial lemniscate at a regular level is
simply connected. The component-wise Riemann–Hurwitz formula [8] says that a component
containing 𝑘 zeros has 𝑘 −1 critical points, counted with
multiplicity. The critical point table therefore shows that the
component 𝑈 of 𝑐𝑠 contains exactly 𝑏3,𝑏6, and every other component
contains one root.
The length inequality
It remains to compare the root distances with the loss at the slit.
For a unit complex number 𝜁,
|𝜁 −𝜀𝑤𝑠| ≥1 −𝜀Re(¯𝜁𝑤𝑠). The
Cayley intervals and |𝑤𝑠 −𝑣2| <10−6 give
Re((¯𝜁3+¯𝜁6)𝑤𝑠)<−1431000.
For completeness, this last bound can be
obtained without trigonometric estimates: use the midpoint of each
rational interval and the derivative bound |𝜒′(𝑥)| =2/(1 +𝑥2) to enclose 𝜁𝑗, then substitute the disc for
𝑤𝑠. These enclosures in fact give
an upper bound below −0.28635. Thus
|𝑏3−𝑐𝑠|+|𝑏6−𝑐𝑠|>𝜌(2+1431000𝜀).
Lemma 2.1 and
(4)
now yield
H1(𝐾)>𝜌(2+(1431000−815000)𝜀)>2
for every
connected subset of 𝑈 containing
both roots. The last strict inequality follows by substituting 𝜌 =1 −10−96 and 𝜀 =10−12; its excess over
2 exceeds 1.42 ⋅10−13. A connected set
containing any two roots must lie in one component, so this proves the
assertion for the whole strict lemniscate. In particular it applies to
the image of every continuous root-to-root path. Since the Hausdorff
measure of a rectifiable path image is at most its total variation, both
interpretations of path length are excluded.
The construction above fixes 𝑠 =10−6. It establishes no interval of
parameters for the small-parameter family reported by ani.
The formal files also prove the assertion for arbitrary preconnected
sets; the argument here uses the equivalent connected-subset formulation
and ordinary Rouché and covering arguments. No new Lean build or
independent human review is asserted by this exposition.
Trinomials
At a zero of a trinomial, the root equation eliminates the middle
coefficient. Along the segment from the origin to that zero, the
remaining expression is a nonnegative linear combination of two values
of modulus less than one. The sum of the coefficients is at most one,
which gives the required containment.
Theorem 3.1 (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).(5)
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. ◻
No separate bound on 𝑎 is
needed, since the root equation eliminates it before we take absolute
values. The conclusion concerns segments to zeros and makes no assertion
that 𝐸𝑓 is star-shaped.
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),(6)
since the coefficient of 𝑐𝑘𝜁𝑘 on the right is 𝑡𝑘 −𝑡𝑛 and ∑𝑘<𝑛𝑐𝑘𝜁𝑘 = −𝑐𝑛𝜁𝑛. The
weights in (6) 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 assumption that all zeros lie in the unit disc need
not bound every partial sum by one. The next example shows that a
prescribed radial segment can then escape.
Example 3.2 (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.
A small least critical value
We follow a component from its first merger as the level of |𝑓| increases. Under the assumption that
it contains no path shorter than 2
between distinct roots, conformal length bounds force the roots apart.
Packing then forces area growth beyond Pólya’s upper bound. The
reduction to this comparison is an ordinary analytic argument; the exact
computation at its end does not formalise the reduction. We retain the
resulting criterion as an unformalised remark. Throughout this section
𝜇=min𝑓′(𝑐)=0|𝑓(𝑐)|
is
the least critical-value modulus.
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 connection is required to
stay in |𝑓(𝑧)| <1; the example
places no restriction on its distance from the origin.
Proof. Apply Remark 4.1
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). Their connecting curve
then has length less than 2
whenever artanh(tanh2(𝑑/4)) <1/𝑎.
Under our assumption that no such curve exists, we therefore have
𝑑(𝑏𝑖,𝑏𝑗) ≥ 𝐷:=4artanh√tanh(1/𝑎),cosh(𝐷/2)=𝑒2/𝑎.(7)
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.(8)
A lower bound for the number of roots.
Equation (8) already
gives 𝑘 ≥2𝑥/𝛿(𝑎): the
required sum is at least 𝑥, and
each root contributes at most 𝛿(𝑎)/2. Improving this estimate
requires the pairwise separation, not just the distance of each root
from the origin. 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 4.3 (circle-slice packing). Under (7), 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. ◻
Proof. By (8),
Lemma 4.3 and the
radius bound,
𝑥≤∑𝑗𝜆(𝑑𝑗)=∑𝑗[𝜆(𝑑𝑗)−∑𝑖𝜎𝑖𝑤(𝑑𝑗,𝑟𝑖)]+∑𝑖𝜎𝑖∑𝑗𝑤(𝑑𝑗,𝑟𝑖)≤𝑘𝑈+𝜋Σ.◻
◻
A nonnegative weighted sum of the circle-slice inequalities bounds
every admissible configuration at once. 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),(9)
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
(9) at the
outer level and rearranging therefore gives
𝑎′(𝑥) ≥ 12𝜋2[2√𝑘−√2𝑎(𝑥)(𝑥+2)]2+(10)
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 gives 𝑎 ≤1 until the level reaches 1. Thus an integrated lower bound greater
than 1 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 (10) 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.
Certificate.
The comparison gives an upper bound 𝑋 on the logarithmic time needed for the
forced area to exceed 1. It
therefore gives a contradiction whenever 𝜇𝑒𝑋 <1. The stated constant 13/25 is a convenient rational choice
with room to spare, not an optimality claim. A program
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. Its full run 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 full run certifies
𝑋=6357628895991000000000000<0.6357629,1325𝑒𝑋<1,
which gives Remark 4.1.
The full replay recorded on 29 September 2026 used the immutable program
cited above. It accepted all 126
dual certificates and reproduced this value of 𝑋; no new replay is claimed for the
present editorial revision. The retained certificate data give the exact
radii and nonnegative weights, together with their sums and certified
upper bounds. The program’s Git blob identifier is
e9b4998884575a31ce0d1f6762a210ae2d617103. That replay also
ran the comparison regression and the observer-containing-circle audit.
The comparison check is exact; the geometry audit combines an exact
full-circle boundary test with floating identity checks. No new
per-degree thresholds were computed.
A coarser run 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 Remark 4.4. For
orientation, the pairs of the coarser run 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 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 certified stopping time. 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 independent review of this theorem is recorded. 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. A research
note carries the full analytic argument, the table of certified
weighted bounds and the instructions for running 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 existence of a short
curve joining two roots.
Proof. For 𝑛 ≥3, apply
Remark 4.1
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 construction retains the root count and capacity of a chosen
component, at the cost of a larger universal constant.
A path estimate from area and boundary length
We can also average inverse-ray lengths and boundary arcs directly.
This ordinary construction keeps both the number of roots and the
capacity of the selected component in the estimate. Its formal source
assumes the construction in degrees above two, so the resulting path
bounds below are unformalised remarks.
The scaled packing criterion, Remark 4.5, has
smaller constants: 5/2 <71/10 for
length and 25/13 <2 for the
containment level. The advantage of the direct argument is its explicit
dependence on component geometry. Its 𝜇 ≤1/2 specialisations are already
within the range of Remark 4.1.
For a monic degree-𝑛 polynomial put
𝐾𝑡={𝑧:|𝑓(𝑧)|≤𝑡},𝜇=min𝑓′(𝑐)=0|𝑓(𝑐)|,𝜌=𝜇1/𝑛.
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}. ◻
Before replacing the right side of (CF) by the constant 71/10, we can retain its dependence on
the selected component. Its number 𝑘 of roots occurs in the factor √2/𝑘, and its logarithmic capacity
bounds the area used in the estimate. Each gives sufficient conditions
for the length bound to be less than 2.
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 unformalised 13/25 criterion already covers these
three ranges without the additional lower bound on the number of
roots.
Proof. If 𝜇 =0, a
repeated zero gives the constant path. Assume henceforth 𝜇 >0. Every selected component 𝐶𝑡 in the proof of Remark 5.1 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 the
component to have smaller capacity than the full sublevel set. A small
number of roots in the component does not imply this capacity bound. 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.
Proof. Repeat the averaging proof of Remark 5.1 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 [2]. 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 Remark 5.1 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. Its proof is not available, and 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 5.4 (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 [2] 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.
Proposition 5.5 (a counterexample to the proposed
one-root perimeter bound). Let 𝑝(𝑧) =𝑧8 −(3/2)𝑧 and let 𝐶 be the component of {|𝑝| ≤1} containing the origin. Then
𝐶 contains exactly one zero and a
neighbourhood of the closed disc of radius 5/8, so H1(𝜕𝐶) >5𝜋/4. The
constant Γ(1/4)2/(2√𝜋) is at most
(𝜋/2)(1 +√2) <5𝜋/4.
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.
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 [8]. 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.
The inputs of the construction in the proof of Remark 5.1 are the
capacity identity for polynomial preimages [2], Pólya’s area inequality [2], 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; Remark 5.6 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 existence of a root-to-root curve of length less than 2 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 [15]: 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) [15], 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
For a cubic we can estimate the inverse roots directly after
normalising at a critical point of least value modulus. The root-disc
hypothesis makes that modulus less than one, and two radial segments in
the normalised coordinates give a path shorter than 2.
Theorem 6.1 (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 [8]. 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 segments
from 𝑐 to the roots have total
length 2|𝛼| <2, and along
either segment 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.
Sources and scope.
Pendyala [11] proves
the separate quartic case; no historical priority for the cubic theorem
is asserted here.
An isolated simple critical value
A disc containing 0 and one
simple critical value selects a component of degree two. Taking a square
root removes its local branching and gives a coordinate in which the
proposed connecting curve is a real segment. The ordinary argument below
then bounds its length by area and capacity. Lean assumes this combined
analytic construction as DiscSepBergmanArea; it does not
derive it from the polynomial hypotheses. We therefore record the path
criterion and its numerical consequences as unformalised remarks.
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.
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 4 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. The Poisson kernel on the right is smallest at the
boundary point opposite 𝐵(0).
Choosing 𝑤 = −𝐵(0)/|𝐵(0)| therefore
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. ◻
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 (6). 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.
Lean checks this sharper cubic constant.
Remark 7.1
imposes separation in the value plane. Separation of the roots or
critical points alone does not imply its hypothesis. 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 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 3.1, 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 [12], 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 Remark 4.1
and to Remark 5.1. Dubinin’s
theorem is a neighbouring result under a full covering hypothesis and
supplies no curve joining two roots.
Examples separating the geometric hypotheses
The two critical-value hypotheses leave different restrictions on a
polynomial. We first give a cubic satisfying neither of them. A second
cubic shows why the root count at the first merger cannot determine
capacity at a later level.
Proposition 8.1 (failure of two critical-value
criteria to cover all polynomials). Let 𝑓(𝑧) =𝑧3 +(3/100)𝑧 −3/4. Every root lies in
the open unit disc, both critical points are simple, the critical values
lie on distinct positive rays, 𝜇 >13/25, and
|
|
|1−𝑓(𝑐−)/𝑓(𝑐+)|
|
|<2/375<2.
Proof. On |𝑧| =1, |3𝑧/100 −3/4| ≤78/100 <1, so Rouché’s
theorem puts all three roots in the disc. The critical points are 𝑐± = ±𝑖/10, and 𝑓(𝑐±) = −3/4 ±𝑖/500. They are nonzero,
have distinct arguments and modulus greater than 3/4. Moreover
|
|
|
|1−𝑓(𝑐−)𝑓(𝑐+)|
|
|
|=1/250|𝑓(𝑐+)|<2375.
For any 𝑤0 ∈[0,1], the other normalised value
is at distance less than 1 +2/375 <4/3 from 𝑤0, so the radius-4/3 hypothesis fails. ◻
A component with two roots immediately after the first merger may
contain more roots at a later level. Thus its first root count alone
does not give a capacity saving at level 2𝜇.
Proposition 8.2 (root count does not force a capacity
gap). Let 𝑔(𝑧) =𝑧3 −(3/400)𝑧 −3/32. All roots lie in
the open unit disc and 𝜇 =187/2000 ≤1/2. The first merger
joins two root components, so 𝑘0 =2, but the component at level 2𝜇 containing that pair has normalised
capacity 1.
Proof. Rouché’s theorem on the unit circle applies because
3/400 +3/32 <1. The critical
points are ±1/20, with critical
values −187/2000 and −188/2000. The first merger therefore has
one simple critical point and joins two root components. At level 2𝜇 =374/2000, both critical points are
inside the filled lemniscate. The component count 𝑛 −(𝑛 −1) =1 from Riemann–Hurwitz shows that
it is connected. Its capacity is (2𝜇)1/3 [28], so division by that scale gives one.
The use of logarithmic capacity agrees with transfinite diameter by the
Fekete–Szegő theorem [28]. ◻
The degree-eight perimeter example, Proposition 5.5, requires
no root-disc hypothesis. It refutes the proposed Gamma constant, while
the existence of a uniform one-root perimeter bound remains open in
Problem 5.4.
The Runge construction reported in [26] has no supplied proof and is not
used.
Collinear roots and two sparse polynomial families
The next constructions use the roots or coefficients directly. For
collinear roots we compare with a rescaled Chebyshev polynomial. In a
quintic with two missing coefficients, the resulting moment identities
select two radial segments. A cubic composed with a power map provides a
different use of a single contained segment: its rotational copies join
through the centre of a fibre.
Collinear roots and Chebyshev comparison
We scale the extreme zeros of 𝑇𝑛 to ±1 and make the polynomial monic. Its
endpoint zeros then agree with those of the polynomial under study,
while subtraction lowers the degree. This is the comparison needed for
the alternation argument. Put
𝑟𝑛=cos𝜋2𝑛,𝐶𝑛=12𝑛−1𝑟𝑛𝑛.
Theorem 9.1 (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 theorem is the finite alternation inequality; it does not
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 9.2 (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 9.3 (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 9.3 already
follows from a theorem of Erdős, Herzog and Piranian [4]: 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 9.2 adds
the sharp level and its equality configurations.
Critical sequences and the extremal configuration.
For distinct real zeros, each gap between consecutive zeros contains
exactly one zero of 𝑞′, and
|𝑞| attains its maximum over the
gap only there. The points 𝑐𝑖
chosen in the proof of Theorem 9.2 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 [17]. 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 [19].
Quintics with two missing coefficients
The missing cubic and quadratic terms of 𝑧5 +𝑎𝑧4 +𝑏𝑧 +𝑐 give three identities among
the real and radial coordinates of its roots. We first use those
identities to select two indices whose radial segments will be
contained. For 0 <𝑟 <2 and
0 ≤𝑠𝑖 ≤1, 𝑥2𝑖 ≤𝑠𝑖, put
𝐸𝑖=𝑠4𝑖(𝑠𝑖+𝑟2+2𝑟𝑥𝑖).
Theorem 9.4 (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.
The theorem 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 9.5 (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), each
nonzero root of 𝑃 gives a regular
𝑞-gon of roots centred at ℎ. We exploit this symmetry by lifting
one contained segment for the cubic into two segments through ℎ. A generic polynomial of degree 3𝑞 has no such fibre structure. The first
theorem supplies the segment to be lifted.
Theorem 9.6 (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).
Theorem 9.7 (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, under the
same hypotheses the conclusion holds for polynomials of the form
(𝑧−ℎ)3𝑞+𝐴(𝑧−ℎ)2𝑞+𝐵(𝑧−ℎ)𝑞+𝐶
in
every degree 3𝑞 ≥6.
Proof. One nonzero root of 𝑃 will supply both endpoints of the path
through ℎ. Before selecting it, we
check that every zero of 𝑃 lies in
the open unit disc. Fix a 𝑞th root
𝑦 of a zero of 𝑃 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.
Hence the entire segment, including the origin, lies in the open unit
lemniscate.
For a nonzero quotient root satisfying the segment bound from
(15), two distinct fibre points satisfy
𝑓(ℎ+𝑡𝑦𝜁𝑘)=𝑃(𝑡𝑞𝑟),
and the two
segments 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. ◻
Further families and counterexamples to proposed proof steps
Some further uses of the radial and conformal arguments are collected
here, together with examples where a prescribed construction fails. The
numbered results retain their linked formal statements. The additional
analytic arguments appear as unformalised remarks, even when an ordinary
proof is supplied in full. These qualifications specify the available
formal evidence without changing the finite calculations.
The underlying research notes are retained at commit f214a6b4
and summarised in the
dated overview of these arguments. Numerical observations are
identified separately. These are restricted questions about polynomial
classes and constructions; they do not supply a programme for proving
the refuted unrestricted assertion.
The exact binomial chord calculation
For 𝑛 ≥2 and 0 <|𝑎| <1, put 𝑟 =|𝑎|1/𝑛 and 𝑟∗ =(1 +cos𝑛(𝜋/𝑛))−1/𝑛. A rotation
reduces 𝑧𝑛 −𝑎 to 𝑧𝑛 −𝑟𝑛 without changing lengths or
moduli. For 𝑛 =2, 𝑟∗ =1 and only the outer-diameter case
occurs.
Theorem 10.1 (complementary binomial chords). Two
adjacent zeros of 𝑧𝑛 −𝑎 can be
joined by an explicit polygonal path inside {|𝑧𝑛 −𝑎| <1} of length strictly below
2. For 𝑟 <𝑟∗ the adjacent-root chord itself
works. For 𝑟 ≥𝑟∗, two radial
legs and an inner adjacent crossing chord work after an arbitrarily
small radial contraction. These two constructions meet at 𝑟 =𝑟∗, where the outer chord attains
|𝑓| =1 at its midpoint and therefore
lies only in the closed lemniscate. Open containment at and above the
switch uses the inner chord after a radial contraction.
For 𝑓(𝑧) =𝑧𝑛 −𝑟𝑛, 0 <𝑟 <1 and 𝑛 ≥2, the two constructions depend 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.
We prove the chord estimate also at the smaller radii needed for 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 comparison concerns these two constructions only; it makes no
claim about shortest paths among all admissible curves.
Power substitutions in trinomials
The segment identity survives a power substitution. We record the
lifting argument as an unformalised remark: the source checks the
segment inequality and finite length calculation, but not selection and
lifting of a suitable quotient root. 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, formalise the selection and
lifting just described, or prove unrestricted Erdős #1041.
The radial-segment identity and strict bound are formalised in cancellation
along a trinomial root segment and containment
of a trinomial root segment.
Unformalised remark: a quartic composed with a
power map
We next examine the ordinary lifting argument based on Pendyala’s
degree-four theorem [11]
and four-point radial lemma [11]. The cited quartic result alone does not
formalise this higher-degree construction. 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.
A mean bound for critical values in every
degree
The Poisson argument first gives a quadratic mean bound, allowing a
disc of any centre and radius and counting all multiplicities. This is
the formally supported theorem below. The subsequent fourth-power
refinement, and the higher exponents obtained from vanishing complex
power sums, are unformalised analytic remarks. A critical-value moment
bound supplies no estimate for the lengths of inverse paths ending at
those 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 [25]. 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 10.2 (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).(11)
Consequently the lower exponents used elsewhere
in the record satisfy
𝑛−1∑𝑗=1|𝑓(𝑐𝑗)|1/(𝑛−1)≤(𝑛−1)𝑅𝑛/(𝑛−1)(12)
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.
Lemma 10.3 (reflected-derivative bound). If 𝑓 is monic of degree 𝑛 ≥2 with roots in the closed unit disk,
and 𝑐1,…,𝑐𝑛−1 list its
critical points with multiplicity, then
|𝑓(𝑐𝑗)|≤𝑛−1∏𝑘=1|1−――𝑐𝑗𝑐𝑘|.(13)
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
(13).
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. ◻
First suppose the zeros of 𝑓 lie
in the closed unit disc, and set 𝑚 =𝑛 −1. Gauss–Lucas puts the critical
points in the same disc. Lemma 10.3 gives
the first inequality below; the weighted Poisson inequality, proved next
and applied with equal weights 1/𝑚,
gives the second:
𝑚∑𝑗=1|𝑓(𝑐𝑗)|2/𝑚≤𝑚∑𝑗=1(𝑚∏𝑘=1|1−――𝑐𝑗𝑐𝑘|)2/𝑚≤𝑚.
Applying
this to 𝑅−𝑛𝑓(ℎ +𝑅𝑧) and scaling
back proves (11)
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 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.
The weighted Poisson inequality and its equality case.
Theorem 10.4 (a weighted inequality for points in a
disc). Let 𝑐1,…,𝑐𝑚 ∈――𝔻 and
let 𝑤𝑗 >0 satisfy ∑𝑗𝑤𝑗 =1. Set
𝐺(𝑧)=∏𝑘|1−―――𝑐𝑘𝑧|𝑤𝑘.
Then
∑𝑗𝑤𝑗𝐺(𝑐𝑗)2≤1,
with equality if and only if every 𝑐𝑗 =0. Equal weights therefore give ∑𝑗(∏𝑘|1 −―――𝑐𝑘𝑐𝑗|)1/𝑚 ≤𝑚 for every 𝑚.
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. Lean checks the
quadratic weighted inequality. 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 10.2 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. Lean does not check this
classification.
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.
Lean checks only the quadratic case; the analytic argument reaches
further. 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 power-parameter
Poisson identity; Lean does not check it.
In particular, equal weights and Lemma 10.3 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. Thus the constant is
sharp. Optimality of the exponent at each fixed degree is not
asserted.
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. The hypotheses require exact
cancellation of the moments; upper bounds for their moduli are
insufficient. Lean does not check the higher-power conclusions in this
paragraph; the Lean proof of Theorem 10.2 has
exponent 2/(𝑛 −1).
Lean proofs of the Poisson and integration steps.
The square-expansion proof above applies whenever 𝑔 is holomorphic on the disc and
continuous on its closure, with |𝑐| <1. The Lean norm-square
majorization uses the Poisson formula for a real part and the
nonnegativity of a square. The weighted
kernel identity identifies the pointwise Poisson mixture.
Separately, absolute
series transport justifies termwise circle integration when the
terms are circle integrable and admit a summable uniform norm bound; its
Taylor double-product form assumes absolute summability of both
coefficient sequences.
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. Equality in this linear form forces equality in the quadratic
inequality, by the variance identity above; Lean proves that
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 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 modulus bounds still require a separate
path selection or metric comparison before they yield an inverse-ray
length estimate.
A sufficient critical-value threshold in degree
five
The reciprocal balance at a critical point bounds the sum of the two
nearest root distances. We begin with this formal geometric statement,
then distinguish distance from containment in the degree-five
argument.
Theorem 10.5 (a geometric-mean bound for distances to
a critical point). Let 𝑛 ≥2,
let 𝑧1,…,𝑧𝑛,𝑐 ∈ℂ
with 𝑐 ≠𝑧𝑘 for every 𝑘, and suppose
𝑛∑𝑘=11𝑐−𝑧𝑘=0.
If 𝑟 >0 is determined by
𝑟𝑛=𝑛∏𝑘=1|𝑐−𝑧𝑘|,
then there are
distinct indices 𝑖,𝑗 such that
|𝑐−𝑧𝑖|+|𝑐−𝑧𝑗|≤2𝑟.
Proof. Relabel the points so that their distances satisfy
𝑑1 ≤𝑑2 ≤⋯ ≤𝑑𝑛. The
reciprocal balance and the triangle inequality give
1𝑑1=|
|
|
|
|𝑛∑𝑗=21𝑐−𝑧𝑗|
|
|
|
|≤𝑛∑𝑗=21𝑑𝑗≤𝑛−1𝑑2.
Thus 𝑑2 ≤(𝑛 −1)𝑑1. Also 𝑑1𝑑𝑛−12 ≤𝑟𝑛, since every
remaining distance is at least 𝑑2.
For 𝑡 =𝑑2/𝑑1 ∈[1,𝑛 −1],
𝑑𝑑𝑡log2𝑡(𝑛−1)/𝑛1+𝑡=𝑛−1−𝑡𝑛𝑡(1+𝑡)≥0.
The logarithm vanishes at
𝑡 =1, so 𝑑1 +𝑑2 ≤2(𝑑1𝑑𝑛−12)1/𝑛 ≤2𝑟. ◻
The distance bound for the two nearest roots.
Corollary 10.6 (two nearest roots). If the roots
lie in the open unit disc and 𝑐 is
a non-root critical point, the two nearest roots to 𝑐 have total distance strictly below
2.
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. A research
note gives the same argument. Lean checks the strict
distance bound from the critical polynomial, including the root-disc
reduction and the choice of the two nearest indices.
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)|.
Two failures of straight segments.
Proposition 10.7 (two counterexamples to straight-path
assertions). There is a monic quintic with all roots in the open
unit disc and a non-root critical point 𝑐 whose unique nearest root has a point
on the straight segment to 𝑐
outside {|𝑓| <1}. There is also
a monic cubic with all roots in the open unit disc such that the
midpoint of every pair of distinct roots lies outside {|𝑓| <1}.
Proof. For the quintic, put 𝑝 =999/1000 and 𝑎 =(901/902)𝑝, and take
𝑄(𝑧)=(𝑧−𝑎)(𝑧2+𝑝2)(𝑧2+902901𝑝𝑧+𝑝2).
Its roots are
𝑎,𝑖𝑝,−𝑖𝑝,𝑝−451+780𝑖901,𝑝−451−780𝑖901.
Since
4512 +7802 =9012, the last four
roots have modulus 𝑝 <1, while
0 <𝑎 <𝑝. Also 𝑄′(0) =0 and 𝑄(0) = −𝑎𝑝4 ≠0. Thus 𝑎 is the uniquely nearest root to the
non-root critical point 0. At one
tenth of that segment, exact rational arithmetic gives
|𝑄(𝑎/10)|=9𝑎10(𝑎2100+𝑝2)(𝑎2100+11𝑝210)>1.
For the
cubic, take 𝑔(𝑧) =𝑧3 −(99/100)3. If
𝑧,𝑤 are distinct roots, then 𝑧 +𝑤 is the negative of the third root, so
𝑔(𝑧+𝑤2)=−98(99100)3,98(99100)3=87326918000000>1.
All three roots have modulus
99/100. ◻
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. Its proof is not available. 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.
Area of a connected sublevel set.
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 [8] 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
We now ask whether a small critical value selects a short pair of
inverse arms. The following records test that selection rule and a
related sum over critical points. 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. A computational
record 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 observations do not yet constitute 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, which establishes
no universal selection rule.
Second, a second
computational 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
suggest failure of the aggregate inequality, but do not certify an
example or an open set of violating polynomials. Its algebraic factor
𝑛−1∑𝑘=1|𝑓(𝑐𝑘)|1/𝑛≤(𝑛−1)𝑅
is proved for every 𝑛 ≥2 in
Theorem 10.2. 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.
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 connecting curve follows from either straight-segment
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 existence of a short curve joining two roots 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 a historical sufficient condition, not an open assertion:
together with the stated compactness and scaling argument it would
contradict Theorem 1.2.
The reduction remains useful on separately specified polynomial
classes.
An integral for successive merger scales
Consider a component containing 𝑘 roots that later joins a larger
component as the level of |𝑓|
increases. If 𝑟 ∈(0,1] is the
ratio of these two merger scales, one logarithmic contribution assigned
to each of its roots is 𝑘−1log(1/𝑟). An earlier length
estimate instead involves the integral
𝐼𝑘(𝑟)=∫1𝑟𝑑𝑞𝑞log((1+𝑞2/𝑘)/(1−𝑞2/𝑘)).
For nearby
merger scales, 𝑟 is close to 1. The integral is then much smaller than
𝑘−1log(1/𝑟). The following
change of variables proves that no fixed positive multiple of this
logarithmic contribution is a uniform lower bound.
Theorem 10.8 (the relation between two merger-scale
integrals). Define
Φ(𝑥)=∫𝑥0𝑑𝑡log(coth𝑡)(𝑥≥0).
At 𝑡 =0
the integrand is understood by its continuous limiting value 0 (equivalently, the integral is improper
at that endpoint). For every integer 𝑘 ≥1 and 0 <𝑟 ≤1, with 𝑥 =𝑘−1log(1/𝑟),
𝐼𝑘(𝑟)=𝑘Φ(𝑥).(O1)
The function Φ is increasing and
strictly convex on (0,∞), and
Φ(𝑥)𝑥⟶0(𝑥↓0).(O2)
Consequently, for every fixed 𝑘 ≥1 and every 𝑐 >0, some 0 <𝑟 <1 satisfies
𝐼𝑘(𝑟)<𝑐1𝑘log1𝑟.(O3)
In particular, no positive universal constant bounds 𝐼𝑘(𝑟) below by that constant times 𝑘−1log(1/𝑟).
Proof. Set 𝑞 =𝑒−𝑘𝑡.
Then 𝑑𝑞/𝑞 = −𝑘 𝑑𝑡, the endpoints
𝑞 =1,𝑟 become 𝑡 =0,𝑥, and
1+𝑒−2𝑡1−𝑒−2𝑡=coth𝑡,
which proves (O1). Since coth𝑡,
and hence log(coth𝑡), is
strictly decreasing, the positive integrand 1/log(coth𝑡) is strictly increasing.
This proves monotonicity and strict convexity. Moreover
0≤Φ(𝑥)𝑥≤1log(coth𝑥)⟶0,
which gives (O2); taking 𝑟 =𝑒−𝑘𝑥 gives (O3). ◻
As 𝑟 approaches 1, two successive merger scales approach
each other. The integral can then be arbitrarily small relative to the
logarithmic contribution, even for fixed 𝑘. Any estimate along a chain of mergers
must retain this nonlinear dependence. Related weighted Jensen estimates
and a lemma selecting two roots with small total logarithmic
contribution are given in a research
note. Those inequalities do not by themselves construct pieces of a
contained path that meet one another.
The Newton value equation
Along a Newton trajectory the polynomial value decays exponentially.
We first derive this scalar equation, then use it to exclude a finite
connection between critical points whose values lie on different rays.
For the classical trajectory and graph statements we follow Kozen and
Stefánsson [7].
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 [7], described
with its endpoint conventions below, is a separate input to the
inverse-sheet discussion in Section 13.
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 [7].
Theorem 11.1 (value equation). For a polynomial
𝑓 and a differentiable curve 𝑧 :𝐼 →ℂ on an interval 𝐼, assume 𝑓′(𝑧(𝑡)) ≠0 and 𝑧′(𝑡) = −𝑓(𝑧(𝑡))/𝑓′(𝑧(𝑡))
throughout 𝐼. Then 𝑤 =𝑓 ∘𝑧 satisfies 𝑤′ = −𝑤, and
𝑓(𝑧(𝑡))=𝑒−(𝑡−𝑡0)𝑓(𝑧(𝑡0))(𝑡,𝑡0∈𝐼).
The computation is one line: 𝑤′ =𝑓′(𝑧) 𝑧′ =𝑓′(𝑧) ⋅( −𝑓(𝑧)/𝑓′(𝑧)) = −𝑓(𝑧) = −𝑤.
Equivalently,
𝑑𝑑𝑡(𝑒𝑡𝑓(𝑧(𝑡)))=0,
and integration on the real interval gives
𝑓(𝑧(𝑡))=𝑒−(𝑡−𝑡0)𝑓(𝑧(𝑡0)),𝑡0≤𝑡,𝑡0,𝑡∈𝐼.
Lean proves the theorem together with this
integrated identity. The separate local complex-parameter calculations
are the value
derivative and the scaled
derivative. They require complex differentiability and do not
themselves integrate a trajectory on a real interval. 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.
Corollary 11.2 (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 corollary constructs no trajectories and supplies no
global monodromy theorem. The Lean ray
exclusion assumes the exponential endpoint identity; it does not
construct or integrate a connecting trajectory. 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 [7].
Separating the rays of critical values
A constant perturbation translates the critical values and leaves the
critical points fixed. We can therefore separate their positive rays by
describing the exceptional translation parameters: two nonzero values
collide in argument exactly when their ratio is positive real.
Along a Newton trajectory the argument of 𝑓 stays constant while its modulus
decreases. By Corollary 11.2, 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 [7]; 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 12.1 (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.
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 15 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.
Local polynomial expansions
For 𝑓(𝑧) =∏𝑗(𝑧 −𝑎𝑗) with
𝑎𝑗 ≠0, put 𝑟 =min𝑗|𝑎𝑗| and 𝑝𝑚 =∑𝑗𝑎−𝑚𝑗. On |𝑧| <𝑟, the exact expansion
log|𝑓(𝑧)|=log|𝑓(0)|−ℜ∑𝑚≥1𝑝𝑚𝑚𝑧𝑚
expresses the local level geometry through the reciprocal power sums. If
𝑞 =|𝑧|/𝑟 <1, the tail after 𝑁 has modulus at most 𝑛𝑞𝑁+1/((𝑁 +1)(1 −𝑞)); differentiated
geometric series give the corresponding first and second derivative
bounds. A research
note gives recurrences for these reciprocal power sums and tests
based on the first two derivatives for a locally contained piecewise
path. The assumption |𝑧| <𝑟 is
essential: this disc contains no zero of 𝑓, so a logarithm exists there. The
expansion does not continue through a root and does not select a pair of
roots to join. A proposed local path must still satisfy the containment
inequalities.
Why the proposed spanning-tree estimate fails
The spanning-tree estimate in [10] fails already for a quadratic Cassini
lemniscate. That manuscript, posted by shtuka on 24 March
2026, claims the unrestricted statement [10]. 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 is incorrect.
We give the explicit numerical contradiction first. We then examine the
saddle model and give an unformalised decomposition into inverse sheets,
including the arcs that join them.
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 [20]. 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 (5.1). Thus neither a
different local saddle neighbourhood nor a perfect topological
decomposition can recover the printed coefficient 1/(2𝜋). The exact numerical inequality
and the resulting contradiction for a tree-length bound also have a Lean
proof, in the repository’s research corpus, a library the checked
build does not compile. The level-length majorant is an explicit
analytic input.
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 [20]. A
global component argument cannot delete one local sector from a disc
already contained in 𝑉.
The four-sector calculation identifies an error in the proof, while
the Cassini example above disproves the printed metric inequality
itself. Possible alternative constructions include cutting an adjoining
regular annulus along a separatrix or regular flow arc, retaining a
four-pronged saddle neighbourhood, or using the inverse-sheet
decomposition below. None can restore (5.1). A revised
estimate would have to include the length needed to join the pieces,
seek only one short pair instead of a tree spanning all roots, or use a
different global metric inequality. The shorter descriptions of the same
three-ended block do not repair the four-sector topology.
The following ordinary topological argument assumes that the critical
values have pairwise distinct arguments and moduli and that 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 [21] 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 remark 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.
Inverse-branch prerequisites.
For a nonconstant complex polynomial, each component of {|𝑓| <1} contains
a root. The restriction to that component is onto
the unit disc and has finite
fibres. Over values avoiding the critical values attained in that
component, it is a covering
map. Choose finitely many nonzero slit starts that include every
critical value attained in the component, and remove the outward rays
beginning at those starts from the value disc. On the remaining domain,
each root in the component determines a unique
continuous inverse branch, taking 0 to that root. The archived Lean source
states these prerequisites and supplies proof scripts; a kernel-check
receipt for this module is not supplied here. The full conformal sheet
decomposition, sheet count, monodromy and embedded-tree assertions
remain ordinary arguments here; the prerequisites give no length
estimate.
Proof of Remark 13.1. 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 argument is also written out in the
proof of the decomposition into inverse sheets. This remark supplies
a topological construction with no useful bound on the sum of lengths:
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 11.2 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 15.5 satisfies its
hypotheses but has a non-Hausdorff orbit quotient. Boundary tangencies
and quantitative estimates for joining the strips remain separate
questions. The embedded tree supplies no length bound for the historical
question.
Numerical path searches
The earlier searches discretised root configurations and tested
candidate connections. Their finite scope is recorded here so that a
negative search is not mistaken for a general path theorem.
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 in these
trials. The reported grid distances are below 2, but they do not certify lengths of
curves in the lemniscate. A polygon whose vertices satisfy |𝑓| <1 can cross the boundary along an
edge. Joining an approximate root to its grid vertex introduces another
edge requiring the same check. 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 do not test ani’s degree-seven counterexample.
Numerical tests of a particular path construction should also examine
near-degenerate saddles, thin necks, boundary-critical configurations
and almost-connected separatrices. Any paths found on a grid still
require verification along their entire edges.
Further questions about topology, length and perturbation
The degree-seven example refutes the unrestricted formulation. The
questions below concern the topology and quantitative estimates needed
on restricted classes. They preserve the distinction between a valid
inverse-sheet decomposition, bounds for its pieces, and a bound for a
contained curve assembled from those pieces.
1. Local saddle geometry and the refuted tree
estimate
Problem 15.1 (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 upper bound
strictly smaller than the distance between its roots. Any later argument
must include the positive length needed to join the pieces, 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 (5.1).
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 15.2 (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 15.5 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 (5.1).
Cassini already excludes the printed coefficient 1/(2𝜋) for any embedded tree that
contains all 𝑚 roots: Problem 15.1 records that no
later gluing argument can retain that estimate.
Problem 15.3 (strip gluing after the printed
coefficient). Assuming Problem 15.2, 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 (5.1).
The printed coefficient 1/(2𝜋) is not an open target. Better
additive control of saddle, annular-cut and root-cap cost cannot
recover (5.1).
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 error term assigned to the collar in the printed argument
𝑞=12𝜋∫2𝛼𝛼𝑃𝑉(𝑡)𝑑𝑡>0
uses the same excluded coefficient. It cannot be treated as an unused
error allowance in an otherwise complete spanning-tree estimate.
Shortest trajectories chosen independently in different strips may have
endpoints that do not meet; the lengths needed to join them must also be
bounded. Even such a bound would not restore the printed 1/(2𝜋) tree estimate.
4. Coefficient perturbation and stability
Once a finite critical-value family is injective, Lean proves
that an arbitrarily small translation makes every value nonzero and
pairwise positive-ray separated. Lean 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.
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 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 15.4 (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 [7].
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 15.5 (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.
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.
The unrestricted assertion in Erdős #1041 is false by Theorem 1.2.
The positive results do not give a classification of the polynomials
that admit a short connection. Their hypotheses and containment levels
differ: low critical value, separated simple critical value, and the
individually proved polynomial families treat separate sufficient
conditions. 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. The degree-seven counterexample
above rules 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.
Numerical estimates for the packing inequality
The circle-slice inequality can be relaxed to finitely many radii.
The numerical values below compare that relaxation with specific
configurations. They are historical optimisation measurements; only the
directed rational bounds used in Section 4 enter its
certificate.
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 4; the
hyperbolic packing bound used for the earlier threshold 2/5; the linear-programming value 𝑀circ of the relaxation of
Lemma 4.3; 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 bound 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 main constructions have different hypotheses. The table locates
their conclusions and distinguishes the formal results from the
additional analytic remarks. The detailed evidence associations are in
the evidence record.
| Family or mechanism |
Conclusion and qualification |
| Degree seven |
The fixed polynomial has no connected
two-root subset of Hausdorff measure at most 2 in its strict lemniscate. |
| Trinomials |
Every root-to-origin segment is contained;
any two roots are joined with length below 2. |
| Low critical values |
Unformalised area-growth criterion with
cutoff 13/25 and scaled level (25/13)𝜇. Its recorded rational
comparison also covers 𝜇 ≤529/1000; the analytic reduction
remains required. |
| Separated simple value |
Unformalised square-root, Bergman and
capacity construction. The chosen critical point must be simple and its
value isolated as stated. |
| Collinear and sparse families |
Formal segment constructions for the
specified root geometry or coefficient patterns. The stronger 2√1−|ℎ|2 cyclic-fibre estimate
remains an ordinary argument. |
| Critical-value means |
Formal exponent 2/(𝑛 −1). The sharp 4/(𝑛 −1) refinement and higher exponents
under complex power-sum cancellations remain unformalised. No path
selection follows. |
| Perimeter and prescribed paths |
The Cassini example refutes the stated
spanning-tree coefficient. The degree-eight example refutes the proposed
Gamma-function constant, while a uniform perimeter bound is still open.
The implication from 𝛽𝜎1/𝑛 to a path of length at
most 𝛽𝜌 in 𝐾𝜇 needs the unformalised
first-critical-level split. Several prescribed straight-segment rules
fail. |
The inverse-ray estimate in the earlier note is retained only as a
historical sufficient condition. It does not follow from these value,
segment or perimeter calculations.
Formal statements and computational checks
The formal sources supplied with these manuscripts have not been
rebuilt for this revision. Their recorded statements include the fixed
counterexample for preconnected
sets, the negation
of the Formal Conjectures statement, its answer(False)
form, and the total-variation
formulation. The independent ordinary reconstruction in
Section 2 uses
Rouché’s theorem, the component degree and Hausdorff measure. Its Cayley
signs, critical-disc estimates and all four Bernstein tests were
recomputed with rational arithmetic in an earlier revision; the present
edit retains those finite calculations. Independent human review of the
construction and its correspondence with the 1958 wording is not
recorded.
The 13/25 calculation has the
recorded full replay described in Section 4. Its
analytic reduction is an ordinary proof and remains unformalised. The
same distinction applies to the fourth-power mean estimate and the
longer analytic family arguments. The numbered statements without a
complete formal proof have therefore been retained as remarks, with
their original mathematical content and local input notes. The following
list records exactly what the existing formal deductions assume.
- 4.1.
-
No Lean proof covers the whole assertion. Lean checks the degree-two
case, and the closing inequality (13/25)𝑒𝑋 <1 at the stopping time
𝑋 certified in the proof. The
computation that certifies 𝑋, done
by an exact-arithmetic program, and the analytic argument in degrees
three and higher are not checked in Lean.
- 4.2.
-
The Lean proof assumes Remark 4.1.
- 4.4.
-
The Lean proof takes the separation bound (7) and the
individual and summed bounds (8) as
hypotheses; their derivation from the failure assumption, given in that
section, is not checked in Lean.
- 4.5.
-
The Lean proof assumes Remark 4.1
in degrees above two; the degree-two case is checked without it.
- 5.1.
-
The Lean proof assumes the two-parameter bound (CF) in degrees 𝑛 ≥3, which the proof obtains by
averaging over levels and value directions. The degenerate case, degree
two and the numerical constants are checked without that input.
- 5.2.
-
The Lean proof assumes the bound (CF) from the proof of Remark 5.1, for a
component containing at least 𝑘0
roots; the rational inequalities are checked.
- 5.3.
-
The Lean proof assumes the averaging construction in the proof of
Remark 5.1, rerun
with the area–capacity inequality for the area of 𝐶; the rational cutoffs are checked.
- 5.6.
-
The Lean proof assumes the two-component split at the first critical
level constructed in the ordinary argument: two one-root components
whose closures meet at a critical point, each with boundary length at
most 𝛽𝜌 and each joining its
root to that point within half its perimeter.
- 7.1.
-
The Lean proof assumes the ordinary analytic construction: the
connector obtained through the square-root map, its Bergman length bound
(7), and the capacity bound for the area of the two-sheeted
component.
- 7.2.
-
The Lean proof assumes the same construction as Remark 7.1 for
the second assertion. Inequality (6) and
every numerical step are checked without it.
- 13.1.
-
No Lean proof covers the whole assertion. Lean checks the
ray-disjointness, level-separation and saddle-scale steps of the proof;
the Morse, monodromy and strip statements are not checked.
- 8.2.
-
The formal capacity conclusion takes as input the classical
transfinite-diameter formula for a filled monic lemniscate. The root
count at the first merger does not require that input.
No supplied proof establishes the reported Runge construction of
unbounded one-root perimeters or the stronger assertion that every
critical joining point fails in the near-pentagon example. Neither is
used in the positive theorems. The fixed value of the degree-seven
parameter is not a proof of the reported parameter family.
References
G. Pólya, Beitrag zur Verallgemeinerung des Verzerrungssatzes
auf mehrfach zusammenhängende Gebiete, Sitzungsberichte der
Preussischen Akademie der Wissenschaften, Physikalisch-Mathematische
Klasse (1928), printed pp. 228–232 and 280–282. https://archive.org/details/sitzungsbericht1928preu.
E. Crane, The areas of polynomial images and pre-images,
Bull. London Math. Soc. 36 (2004), no. 6, 786–792,
doi:10.1112/S0024609304003509;
preprint arXiv:math/0302189v1, whose
statement numbers are cited.
T. F. Bloom, Erdős Problems, problem 1041. https://www.erdosproblems.com/1041
P. Erdős, F. Herzog, and G. Piranian, Metric properties of
polynomials, J. Analyse Math. 6 (1958), 125–148,
doi:10.1007/BF02790232.
S. Ghosh and K. Ramachandran, Number of Components of
Polynomial Lemniscates: A Problem of Erdős, Herzog, and Piranian,
J. Math. Anal. Appl. 540 (2024), no. 1, 128571, doi:10.1016/j.jmaa.2024.128571;
preprint arXiv:2312.13673v1, whose
statement numbers are cited.
S. Sutherland, Bad Polynomials for Newton’s Method, in
B. Bielefeld and M. Lyubich (eds.), Conformal Dynamics Problem
List, Stony Brook IMS preprint (1992), 42–44. https://www.math.stonybrook.edu/preprints/ims92-7.pdf
D. Kozen and K. Stefánsson, Computing the Newtonian
graph, J. Symbolic Comput. 24 (1997), no. 2,
125–136, doi:10.1006/jsco.1997.0118;
authors’ copy https://www.cs.cornell.edu/kozen/Papers/newton.pdf.
P. Ebenfelt, D. Khavinson, and H. S. Shapiro, Two-dimensional
shapes and lemniscates, in Complex Analysis and Dynamical
Systems IV, Part 1, Contemp. Math. 553, Amer.
Math. Soc., Providence, RI, 2011, 45–59, doi:10.1090/conm/553/10931;
preprint arXiv:1003.4567v1, whose
statement numbers are cited.
V. N. Dubinin, Lemniscates and inequalities for the
logarithmic capacities of continua, Mat. Zametki
80 (2006), no. 1, 33–37, doi:10.4213/mzm2777; English
translation, Math. Notes 80 (2006), no. 1, 31–35,
doi:10.1007/s11006-006-0105-8.
shtuka, A Short Path Joining Two Zeros Inside a
Polynomial Lemniscate, manuscript posted 24 March 2026, 48 pp. https://shtuka123.github.io/1041/main.pdf. The file at
this URL has since been replaced by a shorter partial version that no
longer contains Proposition 12; the durable public record of the March
version, its defect, and the author’s 26 March 2026 concession is the
discussion thread at https://www.erdosproblems.com/forum/thread/1041.
V. S. Pendyala, A Degree-Four Lemniscate Path Theorem,
arXiv:2606.24875v1
(2026), doi:10.48550/arXiv.2606.24875.
V. N. Dubinin, Some inequalities for polynomials and rational
functions associated with lemniscates, Zap. Nauchn. Sem. POMI
404 (2012), 83–99; English translation, J. Math. Sci.
193 (2013), no. 1, 45–54, doi:10.1007/s10958-013-1432-4.
P. Borwein, The arc length of the lemniscate {|𝑝(𝑧)| =1}, Proc. Amer. Math. Soc.
123 (1995), no. 3, 797–799, doi:10.1090/S0002-9939-1995-1223265-3.
A. Eremenko and W. Hayman, On the length of lemniscates,
Michigan Math. J. 46 (1999), no. 2, 409–415, doi:10.1307/mmj/1030132418;
preprint arXiv:0805.2295.
A. Fryntov and F. Nazarov, New estimates for the length of
the Erdős–Herzog–Piranian lemniscate, in Linear and Complex
Analysis, Amer. Math. Soc. Transl. Ser. 2 226,
Amer. Math. Soc., Providence, RI, 2009, 49–60, doi:10.1090/trans2/226/05;
preprint arXiv:0808.0717v1.
T. Tao, The maximal length of the Erdős–Herzog–Piranian
lemniscate in high degree, arXiv:2512.12455v1
(2025).
A. Eremenko and P. Yuditskii, Comb functions, Contemp.
Math. 578 (2012), 99–118, doi:10.1090/conm/578/11472;
preprint arXiv:1109.1464v1.
A. Eremenko and L. Lempert, An extremal problem for
polynomials, Proc. Amer. Math. Soc. 122 (1994),
no. 1, 191–193, doi:10.1090/S0002-9939-1994-1207536-1.
A. Eremenko, A Markov-type inequality for arbitrary plane
continua, Proc. Amer. Math. Soc. 135 (2007),
no. 5, 1505–1510, doi:10.1090/S0002-9939-06-08640-0;
preprint arXiv:math/0606745v1.
C. J. Bishop, A. Eremenko, and K. Lazebnik, On the shapes of
rational lemniscates, Geom. Funct. Anal. 35
(2025), no. 2, 359–407, doi:10.1007/s00039-025-00704-2;
preprint arXiv:2407.14610v1.
V. N. Dubinin, Inequalities for critical values of
polynomials, Sb. Math. 197 (2006), no. 8,
1167–1176, doi:10.1070/SM2006v197n08ABEH003793.
E. Crane, A bound for Smale’s mean value conjecture for
complex polynomials, Bull. London Math. Soc. 39
(2007), no. 5, 781–791, doi:10.1112/blms/bdm063;
author preprint https://people.maths.bris.ac.uk/~maetc/SMVCbound.pdf.
V. N. Dubinin, Four-point distortion theorem for complex
polynomials, arXiv:1301.3985v1
(2013).
O. S. Kuznetsova and V. G. Tkachev, Length functions of
lemniscates, Manuscripta Math. 112 (2003),
519–538, doi:10.1007/s00229-003-0411-3;
preprint arXiv:math/0306327.
D. Tischler, Critical points and values of complex
polynomials, J. Complexity 5 (1989), no. 4,
438–456.
W. Cook / Plectis, Three refinements for the lemniscate-path
programme, 16 September 2026, unreviewed research note,
Sections 1–3, together with the earlier note Structural
obstructions.
I. Schur, Über die Verteilung der Wurzeln bei gewissen
algebraischen Gleichungen mit ganzzahligen Koeffizienten, Math. Z.
1 (1918), no. 4, 377–402.
T. Ransford, Potential Theory in the Complex Plane,
London Mathematical Society Student Texts 28, Cambridge University
Press, Cambridge, 1995, doi:10.1017/CBO9780511623776.