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.