The low-degree branch: degrees 2 ≤ n ≤ 5 #
The high-degree argument relaxes the branch point (⋆),
1 ≤ ∫₀¹ ∏ⱼ ‖a + t(1-a²)qⱼ‖ dt,
by AM–GM to the raw polar inequality (1Q), and then needs the origin channel as well. In low
degree none of that is necessary: bounding each factor of (⋆) by the scalar
X(t) = a + (1-a²)t already contradicts itself.
Writing m = n - 1 for the number of non-distinguished zeroes and J_m(a) = ∫₀¹ X(t)^m dt,
the branch point gives 1 ≤ J_m(a) while a direct computation gives J_m(a) < 1 for
0 < a < 1 and 1 ≤ m ≤ 4. The computation is done once, at m = 4:
1 - J₄(a) = ((1-a)³(1+a)/5)(a⁴ - 3a³ + 3a + 4),
whose last factor is 2 + 3a + (1-a)(2 + 2a + a²(2-a)) > 0; the smaller exponents are dominated
by X^m ≤ 1 - m/4 + (m/4)X⁴, four instances of weighted AM–GM that factor as squares.
Note the off-by-one: m ≤ 4 is degree n ≤ 5, so this branch covers degree five as well. All
strictness comes from a < 1; at a = 1 one has J_m(1) = 1, matching the regular-polygon
equality examples.
Main statements #
Sendov.low_degree_contradiction:(⋆)is contradictory for2 ≤ n ≤ 5;Sendov.lowJ_lt_one:J_m(a) < 1for0 < a < 1and1 ≤ m ≤ 4.
The scalar chord and its moments #
X(t) = a + (1-a²)t, the pointwise majorant of ‖a + t(1-a²)qⱼ‖.
Instances For
J_m(a) = ∫₀¹ X(t)^m dt.
Equations
- Sendov.lowJ m a = ∫ (t : ℝ) in 0..1, Sendov.lowX a t ^ m
Instances For
The branch point, bounded factor by factor #
The branch point (⋆), with every factor replaced by the scalar X(t).
The fourth moment #
J₄(a), by the fundamental theorem of calculus against an explicit antiderivative. The
antiderivative is written without dividing by 1 - a², so no side condition on a appears.
Dominating exponents one through four by the fourth #
The contradiction #
The low-degree branch. The branch point (⋆) is already contradictory for
2 ≤ n ≤ 5, with no recourse to the origin channel.