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Eqs. (2.9)–(2.10): (2.6)–(2.7) are the FRW equations for the Elko energy density and pressure

Proved
PereiraGuimaraesElko.density_pressure_eq_2_9_2_10

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

cosmologymathematical-physicsordinary-differential-equations

Let κ,H,H˙,Φ,Φ˙,V\kappa,H,\dot H,\Phi,\dot\Phi,Vκ,H,H˙,Φ,Φ˙,V be real numbers (instantaneous values) and define the energy density and pressure of the Elko field by

ρ=Φ˙22+V+38 H2Φ21+κ2Φ2/8,(2.9)\rho=\frac{\dot\Phi^2}{2}+V+\frac38\,\frac{H^2\Phi^2}{1+\kappa^2\Phi^2/8},\qquad(2.9)ρ=2Φ˙2​+V+83​1+κ2Φ2/8H2Φ2​,(2.9) p=Φ˙22−V−38 H2Φ21+κ2Φ2/8−14 H˙Φ21+κ2Φ2/8−12 HΦΦ˙(1+κ2Φ2/8)2.(2.10)p=\frac{\dot\Phi^2}{2}-V-\frac38\,\frac{H^2\Phi^2}{1+\kappa^2\Phi^2/8}-\frac14\,\frac{\dot H\Phi^2}{1+\kappa^2\Phi^2/8}-\frac12\,\frac{H\Phi\dot\Phi}{(1+\kappa^2\Phi^2/8)^2}.\qquad(2.10)p=2Φ˙2​−V−83​1+κ2Φ2/8H2Φ2​−41​1+κ2Φ2/8H˙Φ2​−21​(1+κ2Φ2/8)2HΦΦ˙​.(2.10)

Then:

  1. equation (2.6) holds if and only if H2=κ23ρH^2=\dfrac{\kappa^2}{3}\rhoH2=3κ2​ρ;
  2. equation (2.7) holds if and only if H˙=−κ22(ρ+p)\dot H=-\dfrac{\kappa^2}{2}(\rho+p)H˙=−2κ2​(ρ+p).

So ρ\rhoρ and ppp are exactly the quantities that make the Elko system look like a perfect fluid in the standard Friedmann equations; the equation-of-state parameter ω=p/ρ\omega=p/\rhoω=p/ρ of Section 3.2 is built from them.

Formalization Note The source lists (2.9)–(2.10) alongside (2.6)–(2.8) and identifies them, in Appendix A, as the energy density and pressure; this item records the precise sense in which that is true.

Preamble
import Mathlib
Formal statement
namespace PereiraGuimaraesElko

theorem density_pressure_eq_2_9_2_10 (κ H Hdot Φ Φdot V ρ p : ℝ)
    (h29 : ρ = Φdot ^ 2 / 2 + V + 3 / 8 * (H ^ 2 * Φ ^ 2) / (1 + κ ^ 2 * Φ ^ 2 / 8))
    (h210 : p = Φdot ^ 2 / 2 - V - 3 / 8 * (H ^ 2 * Φ ^ 2) / (1 + κ ^ 2 * Φ ^ 2 / 8)
        - 1 / 4 * (Hdot * Φ ^ 2) / (1 + κ ^ 2 * Φ ^ 2 / 8)
        - 1 / 2 * (H * Φ * Φdot) / (1 + κ ^ 2 * Φ ^ 2 / 8) ^ 2) :
    (H ^ 2 = κ ^ 2 / 3 * (1 + κ ^ 2 * Φ ^ 2 / 8) * (Φdot ^ 2 / 2 + V) ↔
        H ^ 2 = κ ^ 2 / 3 * ρ) ∧
      (Hdot = -(κ ^ 2 / 2) * (1 + κ ^ 2 * Φ ^ 2 / 8) *
          (Φdot ^ 2 - 1 / 2 * (H * Φ * Φdot) / (1 + κ ^ 2 * Φ ^ 2 / 8) ^ 2) ↔
        Hdot = -(κ ^ 2 / 2) * (ρ + p)) := 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. (2.6), (2.7), (2.9), (2.10); p. 14, remark after (A.17) that the right sides of (A.14), (A.15) are energy density and pressure
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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