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Deceleration parameter q=−1−H˙/H2q = -1 - \dot H/H^2q=−1−H˙/H2, Eq. (31)

Proved
MDOUnifiedCosmology.deceleration_formula

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

cosmologymathematical-physics

Let aaa be a scale factor that is differentiable at ttt with a˙\dot aa˙ also differentiable at ttt, and suppose a(t)≠0a(t)\neq0a(t)=0 and a˙(t)≠0\dot a(t)\neq0a˙(t)=0. With H=a˙/aH=\dot a/aH=a˙/a, the deceleration parameter satisfies

q(t)≡−a¨ aa˙2=−1−H˙H2.q(t)\equiv-\frac{\ddot a\,a}{\dot a^2}=-1-\frac{\dot H}{H^2}.q(t)≡−a˙2a¨a​=−1−H2H˙​.

This is Eq. (31), used to analyse the phantom-like phase at the end of inflation and the reheating epoch.

Preamble
import Mathlib
import Definitions.Def_MDOUnifiedCosmology_model

open MDOUnifiedCosmology Set
Formal statement
namespace MDOUnifiedCosmology

theorem deceleration_formula (a : ℝ → ℝ) (t : ℝ) (ha : DifferentiableAt ℝ a t)
    (ha' : DifferentiableAt ℝ (deriv a) t) (ha0 : a t ≠ 0) (had : deriv a t ≠ 0) :
    decelerationParam a t = -1 - deriv (hubble a) t / hubble a t ^ 2 := by
  sorry

end MDOUnifiedCosmology
Source
S. H. Pereira, M. E. S. Alves, T. M. Guimarães, "An unified cosmological evolution driven by a mass dimension one fermionic field", Eur. Phys. J. C 79 (2019) 543, https://doi.org/10.1140/epjc/s10052-019-7036-5, p. 7, Eq. (31)
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).

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