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Eq. (3.8): a cosmological constant gives a(t)∝eΛ/3 ta(t)\propto e^{\sqrt{\Lambda/3}\,t}a(t)∝eΛ/3​t

Proved
HackCosmologicalAQFT.scale_factor_cosmological_constant

by Lucas · Oct 9, 2026 · Mathlib 0df444a (Lean v4.33.1)

cosmologymathematical-physicsode

Let G>0G>0G>0 and let I⊆RI\subseteq\mathbb RI⊆R be an open, connected set of cosmological times. Let aaa be twice continuously differentiable on III with a>0a>0a>0 and a˙>0\dot a>0a˙>0 there, and suppose the first Friedmann equation H2=8πG3ρH^2=\frac{8\pi G}{3}\rhoH2=38πG​ρ holds on III with the energy density of a cosmological constant Λ>0\Lambda>0Λ>0,

ρ(t)=ρΛ=Λ8πG(t∈I).\rho(t)=\rho_\Lambda=\frac{\Lambda}{8\pi G}\qquad(t\in I).ρ(t)=ρΛ​=8πGΛ​(t∈I).

Then there is a constant C>0C>0C>0 such that

a(t)=C eΛ/3 tfor all t∈I.a(t)=C\,e^{\sqrt{\Lambda/3}\,t}\qquad\text{for all }t\in I.a(t)=CeΛ/3​tfor all t∈I.

This is the Λ\LambdaΛ-dominated (de Sitter) solution in eq. (3.8) of Hack (2016).

Formalization Note The source leaves the relation between ρΛ\rho_\LambdaρΛ​ and Λ\LambdaΛ implicit. The standard convention ρΛ=Λ/(8πG)\rho_\Lambda=\Lambda/(8\pi G)ρΛ​=Λ/(8πG) is the one under which eq. (3.8) has exponent Λ/3\sqrt{\Lambda/3}Λ/3​.

Preamble
import Mathlib
import Definitions.Def_hack_flrw_friedmann
Formal statement
namespace HackCosmologicalAQFT

/-- Hack 2016, Sect. 3.1, eq. (3.8): domination by a cosmological constant `Λ > 0`
(energy density `ρ_Λ = Λ / (8πG)`) gives `a(t) ∝ exp(√(Λ/3) t)`. -/
theorem scale_factor_cosmological_constant (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)
    (Λ : ℝ) (hΛ : 0 < Λ) (hρ : ∀ t ∈ I, ρ t = Λ / (8 * Real.pi * G)) :
    ∃ C > 0, ∀ t ∈ I, a t = C * Real.exp (Real.sqrt (Λ / 3) * t) := by sorry

end HackCosmologicalAQFT
Source
T.-P. Hack, *Cosmological Applications of Algebraic Quantum Field Theory in Curved Spacetimes*, SpringerBriefs in Mathematical Physics 6, Springer, 2016, DOI 10.1007/978-3-319-21894-6 (https://doi.org/10.1007/978-3-319-21894-6), Sect. 3.1, p. 80, eq. (3.8) (with eq. (3.7))
Read-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 G∈RG\in\mathbb RG∈R with G>0G>0G>0, functions a,ρ:R→Ra,\rho:\mathbb R\to\mathbb Ra,ρ:R→R, a set I⊆RI\subseteq\mathbb RI⊆R, and a real number Λ\LambdaΛ. Assume:

  1. III is open and preconnected;
  2. aaa is twice continuously differentiable on III; a(t)>0a(t)>0a(t)>0 and a′(t)>0a'(t)>0a′(t)>0 for all t∈It\in It∈I;
  3. for all t∈It\in It∈I: (a′(t)/a(t))2=8πG3ρ(t)\left(a'(t)/a(t)\right)^2=\frac{8\pi G}{3}\rho(t)(a′(t)/a(t))2=38πG​ρ(t);
  4. Λ>0\Lambda>0Λ>0, and ρ(t)=Λ8πG\rho(t)=\dfrac{\Lambda}{8\pi G}ρ(t)=8πGΛ​ for all t∈It\in It∈I.

Conclusion. There exists a real number C>0C>0C>0 such that for every t∈It\in It∈I

a(t)=C exp⁡ ⁣(Λ/3  t),a(t)=C\,\exp\!\Big(\sqrt{\Lambda/3}\;t\Big),a(t)=Cexp(Λ/3​t),

where ⋅\sqrt{\cdot}⋅​ is the real square root (here of a positive number). The constant CCC does not depend on ttt. If III is empty the statement holds trivially.

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