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Eq. (2.7): eliminating the torsion from the second Friedmann equation (2.3)

Proved
PereiraGuimaraesElko.raychaudhuri_eq_2_7

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

cosmologymathematical-physicsordinary-differential-equations

Let κ∈R\kappa\in\mathbb Rκ∈R, let I⊆RI\subseteq\mathbb RI⊆R be an open set of times, and let H,h,ΦH,h,\PhiH,h,Φ be real functions with HHH and Φ\PhiΦ differentiable on III. Assume that hhh is given on III by the torsion relation (2.5), h=−18κ2Φ21+κ2Φ2/8Hh=-\frac18\frac{\kappa^2\Phi^2}{1+\kappa^2\Phi^2/8}Hh=−81​1+κ2Φ2/8κ2Φ2​H. Then for every t∈It\in It∈I the second Friedmann equation (2.3),

H˙=−κ22[Φ˙2+34HhΦ2−14ddt[(H+h)Φ2]]−3(1+κ2Φ28)h2,\dot H=-\frac{\kappa^2}{2}\left[\dot\Phi^2+\frac34Hh\Phi^2-\frac14\frac{d}{dt}\big[(H+h)\Phi^2\big]\right]-3\left(1+\frac{\kappa^2\Phi^2}{8}\right)h^2,H˙=−2κ2​[Φ˙2+43​HhΦ2−41​dtd​[(H+h)Φ2]]−3(1+8κ2Φ2​)h2,

holds at ttt if and only if

H˙=−κ22(1+κ2Φ28)[Φ˙2−12 HΦΦ˙(1+κ2Φ2/8)2](2.7)\dot H=-\frac{\kappa^2}{2}\left(1+\frac{\kappa^2\Phi^2}{8}\right)\left[\dot\Phi^2-\frac12\,\frac{H\Phi\dot\Phi}{(1+\kappa^2\Phi^2/8)^2}\right]\qquad(2.7)H˙=−2κ2​(1+8κ2Φ2​)[Φ˙2−21​(1+κ2Φ2/8)2HΦΦ˙​](2.7)

holds at ttt.

Note that (2.3) contains H˙\dot HH˙ on both sides (through ddt[(H+h)Φ2]\frac{d}{dt}[(H+h)\Phi^2]dtd​[(H+h)Φ2]); (2.7) is the explicit form.

Formalization Note The source states the direction (2.3) ⇒\Rightarrow⇒ (2.7); the converse also holds and is included.

Preamble
import Mathlib
Formal statement
namespace PereiraGuimaraesElko

theorem raychaudhuri_eq_2_7 (κ : ℝ) (I : Set ℝ) (hI : IsOpen I) (H h Φ : ℝ → ℝ)
    (hH : ∀ t ∈ I, DifferentiableAt ℝ H t) (hΦ : ∀ t ∈ I, DifferentiableAt ℝ Φ t)
    (h25 : ∀ t ∈ I, h t = -(1 / 8) * (κ ^ 2 * Φ t ^ 2 / (1 + κ ^ 2 * Φ t ^ 2 / 8)) * H t) :
    ∀ t ∈ I,
      (deriv H t = -(κ ^ 2 / 2) * (deriv Φ t ^ 2 + 3 / 4 * H t * h t * Φ t ^ 2
          - 1 / 4 * deriv (fun s => (H s + h s) * Φ s ^ 2) t)
          - 3 * (1 + κ ^ 2 * Φ t ^ 2 / 8) * h t ^ 2 ↔
        deriv H t = -(κ ^ 2 / 2) * (1 + κ ^ 2 * Φ t ^ 2 / 8) *
          (deriv Φ t ^ 2 - 1 / 2 * (H t * Φ t * deriv Φ t) / (1 + κ ^ 2 * Φ t ^ 2 / 8) ^ 2)) := by
  sorry

end PereiraGuimaraesElko
Source
S. H. Pereira and T. M. Guimarães, "From inflation to recent cosmic acceleration: the fermionic Elko field driving the evolution of the universe", JCAP 09 (2017) 038, https://doi.org/10.1088/1475-7516/2017/09/038 (arXiv:1702.07385), p. 5, Eqs. (2.3), (2.5), (2.7)
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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