The Eneström–Kakeya theorem #
A polynomial ∑_{k=0}^n a_k z^k with real coefficients a_0 ≥ a_1 ≥ ⋯ ≥ a_n > 0 has no zero in the
open unit disk. On the unit circle a zero z satisfies z^{n+1} = 1, and z^{k+1} = 1 at every
strict descent a_{k+1} < a_k; with strictly decreasing coefficients there is no zero in the closed
disk. The proof multiplies by 1 - z, telescopes, and applies the triangle inequality.
Main results #
Dilog.enestrom_kakeya: no zero in‖z‖ < 1.Dilog.enestrom_kakeya_boundary: the zeros on‖z‖ = 1are roots of unity of the stated orders.Dilog.enestrom_kakeya_strict: strictly decreasing coefficients give no zero in‖z‖ ≤ 1.Dilog.monotoneState_never_orthogonal:∑ p_k e^{-ikt} ≠ 0for every realtwhenp_0 > p_1 > ⋯ > p_n > 0.Dilog.enestrom_kakeya_boundary_series,Dilog.strictAnti_series_ne_zero: the same on the circle for summable non-increasing series (no truncation): zeros sit at roots of unity pinned by the descents, and strictly decreasing positive populations never orthogonalize. The proof takes real parts of the telescoped series instead of the equality case of the triangle inequality.
References #
- A. Hurwitz, Über einen Satz des Herrn Kakeya, Tôhoku Math. J. 4 (1913) 89–93, §2: the zeros on the
unit circle under non-increasing coefficients (roots of unity; coefficients in groups of equal
consecutive values), with the converse.
enestrom_kakeya_boundaryis his argument. - Q. I. Rahman, G. Schmeisser, Analytic Theory of Polynomials, Oxford University Press, 2002.
Boundary refinement and the monotone clock #
The base theorem localises zeros to ‖z‖ ≥ 1. On the circle ‖z‖ = 1 the same
telescoped identity, read through real parts instead of norms, forces a rigid
structure: a boundary zero can only sit at a root of unity. Strict decrease at every step
then rules the circle out entirely.
Boundary Eneström–Kakeya. If the polynomial vanishes at a point of the unit
circle, that point is a root of unity: zⁿ⁺¹ = 1, and zᵏ⁺¹ = 1 at every step where the
coefficients strictly decrease.
The monotone clock that never ticks. A quantum state with strictly decreasing
populations p₀ > p₁ > ⋯ > pₙ > 0 on the equally spaced energy levels 0, 1, …, n never
reaches an orthogonal state: its autocorrelation ∑ pₖ e^{-i k t} is nonzero for every
time t. The finite, coefficient-side companion of zetaState_never_orthogonal.
Eneström–Kakeya on the circle, for series. Let p be summable and non-increasing. If
∑ pₖ zᵏ = 0 at a point ‖z‖ = 1, then z^{k+1} = 1 at every descent p_{k+1} < p_k: the zeros on the
circle are roots of unity, pinned by where the populations drop (Remark 1 of the paper, for series).
Strictly decreasing populations never orthogonalize (series form): for p > 0 summable and strictly
decreasing, ∑ pₖ zᵏ ≠ 0 on the whole unit circle. With p_n = 6/(π² n²) this is Theorem 4 again, read
from the coefficients as Remark 1 says.