Eq. (2.6): eliminating the torsion from the first Friedmann equation (2.2)
ProvedPereiraGuimaraesElko.friedmann_eq_2_6cosmologymathematical-physicsordinary-differential-equations
Let be real numbers (the values at one instant of the Hubble rate, the torsion function, the Elko field, its velocity and the potential ). Assume the torsion relation (2.5),
Then the first Friedmann equation (2.2),
holds if and only if
Equation (2.6) shows that, once the torsion is eliminated, the Elko Friedmann equation is the standard scalar-field one multiplied by the factor .
Formalization Note The equation is pointwise in time, so it is stated for real numbers. The source states the direction (2.2) (2.6); the converse also holds and is included.
Preamble
import Mathlib
Formal statement
namespace PereiraGuimaraesElko
theorem friedmann_eq_2_6 (κ H h Φ Φdot V : ℝ)
(h25 : h = -(1 / 8) * (κ ^ 2 * Φ ^ 2 / (1 + κ ^ 2 * Φ ^ 2 / 8)) * H) :
H ^ 2 = κ ^ 2 / 3 * (Φdot ^ 2 / 2 + V + 3 / 8 * H ^ 2 * Φ ^ 2 + 3 / 4 * H * h * Φ ^ 2)
+ (1 + κ ^ 2 * Φ ^ 2 / 8) * h ^ 2 ↔
H ^ 2 = κ ^ 2 / 3 * (1 + κ ^ 2 * Φ ^ 2 / 8) * (Φdot ^ 2 / 2 + V) := 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. (2.2), (2.5), (2.6)
Human review
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.