Eq. (3.8): matter domination gives
ProvedHackCosmologicalAQFT.scale_factor_matterLet and let be an open, connected set of cosmological times. Let be twice continuously differentiable on with and there (an expanding universe), and suppose the first Friedmann equation holds on for a matter-dominated energy density
with a constant . Then there are constants and such that for every , and
This is the matter-dominated solution in eq. (3.8) of Hack (2016). The constant is the time at which the scale factor of this solution would vanish.
Formalization Note "" is encoded as equality with a strictly positive constant factor. The power is the real power of the positive number .
import Mathlib import Definitions.Def_hack_flrw_friedmann
namespace HackCosmologicalAQFT
/-- Hack 2016, Sect. 3.1, eq. (3.8): matter domination gives `a(t) ∝ (t - t₀)^{2/3}`. -/
theorem scale_factor_matter (G : ℝ) (hG : 0 < G) (a ρ : ℝ → ℝ) (I : Set ℝ)
(hI : IsOpen I) (hIc : IsPreconnected I)
(ha : ContDiffOn ℝ 2 a I) (hpos : ∀ t ∈ I, 0 < a t) (hexp : ∀ t ∈ I, 0 < deriv a t)
(hF1 : FirstFriedmannEq G a ρ I)
(K : ℝ) (hK : 0 < K) (hρ : ∀ t ∈ I, ρ t = K / a t ^ 3) :
∃ C > 0, ∃ t₀ : ℝ, ∀ t ∈ I, t₀ < t ∧ a t = C * (t - t₀) ^ (2 / 3 : ℝ) := by sorry
end HackCosmologicalAQFTRead-back
What the Lean code literally says, in plain math · Aristotle (Harmonic) — non-blind, same agent as drafter
NON-BLIND READ-BACK — not independent testimony. This read-back was written by the same agent (Aristotle, by Harmonic) that drafted the Lean statement, with full knowledge of the source text and of the intended meaning. It was not produced by a blind, independent auditor, so it may silently read the intended meaning into the code. Reviewers must not mistake it for independent testimony; compare the Lean code against the source directly.
Fix with , functions , a set , and a real constant . Assume:
- is open and preconnected;
- is twice continuously differentiable on ; and for all ;
- for all : ;
- , and for all .
Conclusion. There exist a real number and a real number such that for every both and
where the power is the real power of the positive base . The constants do not depend on . If is empty the statement holds trivially (any , work).