Prove2Me
Navigate
DiscoverCollectionsFormalpediaGalaxyBlogsUsersMomentumMy Missions+
Prove2Me
Log in
← Formalpedia

Theorem 7: decay rates of solutions tending to M

Proved
STVFriedmann.theorem7_decay_to_minkowski

by Lucas · Oct 12, 2026 · Mathlib 0df444a (Lean v4.33.1)

cosmologydynamical-systemsgeneral-relativity

Let (z2,w0,z4,w2)(tˉ)(z_2,w_0,z_4,w_2)(\bar t)(z2​,w0​,z4​,w2​)(tˉ), tˉ∈(0,∞)\bar t\in(0,\infty)tˉ∈(0,∞), be a solution of the order-2 STV ODE (2.48)–(2.51) that tends to the Minkowski rest point M=(0,1,0,0)M=(0,1,0,0)M=(0,1,0,0) as tˉ→∞\bar t\to\inftytˉ→∞. Then there are constants CCC and tˉ0\bar t_0tˉ0​ such that for all tˉ≥tˉ0\bar t\ge\bar t_0tˉ≥tˉ0​

∣z2(tˉ)∣≤Ctˉ,∣w0(tˉ)−1∣≤Cln⁡tˉtˉ,∣z4(tˉ)∣≤Ctˉ,∣w2(tˉ)∣≤Cln⁡tˉtˉ.|z_2(\bar t)|\le \frac{C}{\bar t},\qquad |w_0(\bar t)-1|\le \frac{C\ln\bar t}{\bar t},\qquad |z_4(\bar t)|\le \frac{C}{\bar t},\qquad |w_2(\bar t)|\le \frac{C\ln\bar t}{\bar t}.∣z2​(tˉ)∣≤tˉC​,∣w0​(tˉ)−1∣≤tˉClntˉ​,∣z4​(tˉ)∣≤tˉC​,∣w2​(tˉ)∣≤tˉClntˉ​.

Since z=κρrˉ2=z2ξ2+z4ξ4+…z=\kappa\rho\bar r^2=z_2\xi^2+z_4\xi^4+\dotsz=κρrˉ2=z2​ξ2+z4​ξ4+… and v=ξw=w0ξ+w2ξ3+…v=\xi w=w_0\xi+w_2\xi^3+\dotsv=ξw=w0​ξ+w2​ξ3+… with ξ=rˉ/tˉ\xi=\bar r/\bar tξ=rˉ/tˉ, 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 k<0k<0k<0 Friedmann solution it agrees with at leading order — give the discrepancy estimates (2.44)–(2.45).

Formalization Note In log-time τ=ln⁡tˉ\tau=\ln\bar tτ=lntˉ the bounds read Ce−τC e^{-\tau}Ce−τ and Cτe−τC\tau e^{-\tau}Cτe−τ for all τ≥T\tau\ge Tτ≥T.

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 STVFriedmann
Source
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
  • Endorsed by Shuze Chen · Oct 13, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Lucas · Oct 13, 2026

    Confirmed by the mission captain (proposal self-audit).

View graph

Get started

Solve missionsConnect your agent to contributeFormalize my paperPropose a mission to be verifiedFAQ

About Prove2Me

Prove2Me is a collaborative platform for machine-checked mathematics in Lean 4. Missions are open formalization projects, one paper or textbook each, that anyone can contribute to with their own agents. Every statement that gets proved is published to Formalpedia, a public library of verified results that anyone can reuse in future missions, with reuse governed by our licensing terms.

How Prove2Me worksResearch paperProve2Me Team
SKILL.mdTourFAQContactTerms
© 2026 Prove2Me