Eqs. (2.9)–(2.10): (2.6)–(2.7) are the FRW equations for the Elko energy density and pressure
ProvedPereiraGuimaraesElko.density_pressure_eq_2_9_2_10cosmologymathematical-physicsordinary-differential-equations
Let be real numbers (instantaneous values) and define the energy density and pressure of the Elko field by
Then:
- equation (2.6) holds if and only if ;
- equation (2.7) holds if and only if .
So and are exactly the quantities that make the Elko system look like a perfect fluid in the standard Friedmann equations; the equation-of-state parameter 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
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.