Answers are grounded in this paper and cite their sources.
This research resolves key problems related to fractal behavior and bifurcations, suggesting implications for chaotic systems.
We resolve all three open problems stated in Bird (2026b) concerning the non-holomorphic fractal family zₙ₊₁ = K z_n exp(Im(z_n)) + c. (OP-A) We compute the cusp-bifurcation locus K_cusp(N) for N = 2,…,7, showing that the locus peaks at N = 4 (K_cusp ≈ 11.047) and ceases to exist at N ≥ 8: the cusp is a finite-depth phenomenon with no N → ∞ limit. (OP-B) We prove that the Class C subleading expansion A(K) sqrt(ln K) = 2R sumₙ₌₀ⁱⁿᶠ D_n / (ln K)^n, with D_n = (2n-1)!! / 2^n, is a Poincaré asymptotic series derived from the erfi expansion (DLMF 7.12.1), with D_1 = 1/2 proved exactly and verified to 0.66% at K = 10^100. (OP-C) We study the one-dimensional imaginary orbit yₙ₊₁ = K exp(y_n) y_n + delta as a parametric map in K and locate its period-doubling bifurcation sequence K_1,…,K_9. The ratio sequence r_n = (K_n - Kₙ₋₁)/(Kₙ₊₁ - K_n) converges to 4.671 at n = 8, within 0.03% of the Feigenbaum constant delta_F = 4.6692…. The cascade accumulates near K_acc ≈ 14.9048, well below the phase-transition threshold K* ≈ 25 of Papers 2 and 3. This two-stage structure identifies K* as a secondary geometric event inside an already-chaotic regime, placing the Aether family within the universality class of one-dimensional maps governed by Feigenbaum renormalisation. An analytically exact non-holomorphic distance estimator is also derived, exploiting the Exact Decoupling Lemma, and produces publication-quality boundary renders at any resolution.
No takes yet. Share an insight, caveat, or question.
Michael Bird (2026) studied this question.
Synapse has enriched 8 closely related papers on similar clinical questions. Consider them for comparative context: