Pablo Nogueira Grossi · G6 LLC · Newark, NJ · 2026 · ORCID 0009-0000-6496-2186
Equations (4.1)–(4.3): ṙ = r(1−r²)+2(r−1)e⁻ᶻ, θ̇=1, ż = r²−2(r−1)²e⁻ᶻ. Limit cycle Γ₁₂ = {r=1} shown as dashed gold line. λ(z)=−2(1−e⁻ᶻ): neutral at z=0, attracting for z>0 (Prop. 4.2).
|κ| ↑ κ* ⟺ μ_max < 0 ⟺ τ = √(c/κ_noise) ∈ (0,∞).
κ* is the geometric precursor of τ: curvature accumulation creates the conditions
under which stochastic stability becomes meaningful.
The six dm³ systems are objects in the same category dm³ and are related by explicit contact morphisms f_ij : X_i → X_j satisfying f_ij(Γ_i) = Γ_j. The systems are not analogies — they are exact mathematical identities in the category dm³.
All sorry statements are open proof obligations.
None are hidden. Green badges = closed in Lean 4. Red = open.
λ(0) = 0 — neutral stability at embodiment threshold.
λ(z) < 0 for z > 0 — attracting post-embodiment.
τ = √(4/1) = 2 in closed form.
ε₀ = 2 / (2·(1+2)) = 1/3.
A2, A3 have unique preimages in the singularity correspondence.
λ(z) → μ_max as z → ∞.
H_diss → S(γ) as β→∞ in distributional sense.
|κ|↑κ* ↔ μ_max < 0: requires Floquet theory formalization.
Every τ-stable dm³ system arises from a fold globally on X.
k:m correspondence between higher Ak and higher resonances.
Volume I: C→K→F→U is a piecewise-smooth symplectic map on T*X.
The fold F preserves ω = dγ∧dp (Theorem 11.1 [Vol I]).
Volume II: passes to contact extension M = X×ℝ, α = dz−λ,
dλ = ω. The fold becomes H_diss = −γVe^{−βz} in the regularized limit β→∞.
Liouville's theorem forbids attractors in symplectic systems on compact manifolds. Contact geometry provides: limit cycle attractors, stochastic stability, and variational structure simultaneously. The contact variable z records accumulated dissipation — the orbit earns its stability by accumulating action.