Theorem 9 (n = 2): non-self-similar blow-up at the Big Bang
ProvedSTVFriedmann.theorem9_non_self_similar_blowupcosmologydynamical-systemsgeneral-relativity
Fix . There is a solution , , of the order-2 STV ODE (2.48)–(2.51) such that
- it agrees exactly with the Friedmann spacetime at leading order: whenever , (notation of (2.41));
- it tends to the Minkowski rest point as ;
- it blows up at the Big Bang: as .
So, with time since the Big Bang imposed, solutions in have a self-similar Big Bang at order (they tend to , Theorem 5) but need not at order : such a solution misses in backward time.
Formalization Note Solutions are functions of log-time ; is the sup norm on .
Preamble
import Mathlib import Definitions.Def_STVFriedmann_basic open Filter Topology Real
Formal statement
namespace STVFriedmann
/-- Theorem 9 at order 2: there are solutions of the order-2 STV ODE that agree exactly with
the `k = -1` Friedmann spacetime at leading order and decay to `M` as `t̄ → ∞`, but blow up
(instead of tending to `SM`) as `t̄ → 0⁺`. -/
theorem theorem9_non_self_similar_blowup (Δ₀ : ℝ) (hΔ₀ : 0 < Δ₀) :
∃ U : ℝ → Fin 4 → ℝ, IsSTVSolution stvField2 U ∧
(∀ θ : ℝ, 0 < θ → U (Real.log (Δ₀ * bigBangTime θ)) 0 = friedmannZ2 θ ∧
U (Real.log (Δ₀ * bigBangTime θ)) 1 = friedmannW0 θ) ∧
Tendsto U atTop (𝓝 restM2) ∧
Tendsto (fun τ => ‖U τ‖) atBot atTop := 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. 20, Theorem 9; p. 18 (solutions in F not in the unstable manifold of SM); p. 19, Section 2.8
Human review
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.