101 covered \(G^2\); this course has now defined \(\mu\), \(\eta\), \(\Delta\) on top of \(\pi\), \(\varphi\) — five of the nine named G1–G9 constants. At a fixed point \(x^*\), \(n\) applications of \(G\) contract deviations at rate \(n\mu_{{\max}}\) in the exponent (Week 2): \(\xi(t) \sim \xi_0 e^{{n\mu_{{\max}} t}}\). For \(G^5\) with \(\mu_{{\max}}=-2\): \(\xi(t) \sim \xi_0 e^{{-10t}}\) — a perturbation that took \(t\approx1.15\) to lose 90% of its size under a single \(G\) now loses that same 90% in \(t\approx0.23\), five times faster, exactly as the linear contraction-rate scaling predicts.
AXLE_v6.lean and Weeks 2–4 of this course cited above — no material in this page depends on the external, unverified source removed from earlier drafts of this course.-- dm³ 102 · Week 13 · G⁵ convergence rate
-- Single G: ξ(t) ~ ξ₀·e^{μ_max·t}, μ_max=-2
-- G⁵: ξ(t) ~ ξ₀·e^{5·μ_max·t} = ξ₀·e^{-10t} -- 5x faster in the exponent
-- Two DIFFERENT convergences, both real, not the same object:
-- ladder: ρ_n → τ=2 as n→∞ (sequence of distinct constants φ,η,Δ,...)
-- orbit: G^k(x) → Γ* as k→∞ (single trajectory, rate μ_max=-2)
example : (5:ℝ) * (-2) = -10 := by norm_num