From the raw origin inequality to its α, β(1) form #
This is (origin-exact) + (beta-bound) ⟹ (1le). The work is in replacing
∫₀¹ t β(t)^((n-2)/2) dt
by a Beta value plus the t³ integral that stat is stated with. Writing β as a sum of
squares, β(t) = (1-axt)² + a²t²(1-x²), the blog post applies the mean value theorem to
s ↦ ((1-axt)² + s)^((n-2)/2). Here that step is Bernoulli's inequality instead: dividing
(P+Q)^p ≤ P^p + p Q (P+Q)^(p-1)
through by (P+Q)^p turns it into 1 ≤ θ^p + p(1-θ) at θ = P/(P+Q), which is exactly
one_add_mul_self_le_rpow_one_add. No derivative and no mean value theorem is needed.
After that, ∫₀¹ t (1-axt)^(n-2) dt is enlarged to [0, 1/ax] — legitimate since ax ≤ 1 and
the integrand stays nonnegative — and evaluated by Sendov.integral_chord_lin, the k = 1
Beta integral of Sendov.Common.Chord. What is left is algebra in α and β(1), using
1 - x² ≤ β(1) (which is (x-a)² ≥ 0) and ax = 1 - β(1)/2 - α/(n-1).
(beta-bound) enters only through β(1) < 1, which is what makes x > a/2 > 0, hence 1/x²
finite and 1/(ax) ≥ 1.
Main statements #
Sendov.rpow_add_le_of_one_le: the Bernoulli form of the mean-value step;Sendov.beta_split: the pointwise consequence forβ;Sendov.one_le_of_origin:(origin-exact) + (beta-bound) ⟹ (1le).
(origin-exact) + (beta-bound) ⟹ (1le). (beta-bound) enters only as β(1) < 1.