Theorem 7: decay rates of solutions tending to M
ProvedSTVFriedmann.theorem7_decay_to_minkowskicosmologydynamical-systemsgeneral-relativity
Let , , be a solution of the order-2 STV ODE (2.48)–(2.51) that tends to the Minkowski rest point as . Then there are constants and such that for all
Since and with , the order-1 estimates are the STV ODE form of the decay to Minkowski spacetime (2.46)–(2.47), and the order-2 estimates — applied to a solution and to the Friedmann solution it agrees with at leading order — give the discrepancy estimates (2.44)–(2.45).
Formalization Note In log-time the bounds read and for all .
Preamble
import Mathlib import Definitions.Def_STVFriedmann_basic open Filter Topology Real
Formal statement
namespace STVFriedmann
/-- Theorem 7, (2.44)–(2.47), at the level of the order-2 STV ODE: every solution tending to
`M` satisfies `z₂, z₄ = O(1/t̄)` and `w₀ - 1, w₂ = O(ln t̄ / t̄)` as `t̄ → ∞`
(here `τ = ln t̄`). -/
theorem theorem7_decay_to_minkowski (U : ℝ → Fin 4 → ℝ) (hU : IsSTVSolution stvField2 U)
(hM : Tendsto U atTop (𝓝 restM2)) :
∃ C T : ℝ, ∀ τ : ℝ, T ≤ τ →
|U τ 0| ≤ C * Real.exp (-τ) ∧ |U τ 1 - 1| ≤ C * τ * Real.exp (-τ) ∧
|U τ 2| ≤ C * Real.exp (-τ) ∧ |U τ 3| ≤ C * τ * Real.exp (-τ) := by sorry
end STVFriedmannSource
C. Alexander, B. Temple, Z. Vogler, The Instability of the Critical Friedmann Spacetime at the Big Bang as an Alternative to Dark Energy, arXiv:2510.14228v1 (2025), https://arxiv.org/abs/2510.14228, p. 16, Theorem 7 eqs. (2.44)-(2.47) and the preceding paragraph (z_2 and w_0 decay to M like O(t^-1) and O(t^-1 ln t))
Human review
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.