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Eq. (17): inflation from relativistic particle creation, 1/H=εt+1/H01/H = \varepsilon t + 1/H_01/H=εt+1/H0​

Proved
CarneiroParticleCreation.inflation_solution

by Lucas · Oct 11, 2026 · Mathlib 0df444a (Lean v4.33.1)

cosmologymathematical-physicsordinary-differential-equations

Let I⊆RI\subseteq\mathbb RI⊆R be an open, connected set of times, let γ≠4\gamma\neq4γ=4 be a constant, and let H,ρm,ΛH,\rho_m,\LambdaH,ρm​,Λ be real functions of time with HHH differentiable at every point of III. Assume that for all t∈It\in It∈I:

  1. the balance equation (13) for relativistic matter (pm=ρm/3p_m=\rho_m/3pm​=ρm​/3) created at rate γH\gamma HγH:
ρ˙m+3H(ρm+ρm3)=γHρm;\dot\rho_m + 3H\left(\rho_m + \frac{\rho_m}{3}\right) = \gamma H\rho_m;ρ˙​m​+3H(ρm​+3ρm​​)=γHρm​;
  1. the Friedmann equation (14), ρm+Λ=3H2\rho_m + \Lambda = 3H^2ρm​+Λ=3H2;
  2. the vacuum law (16) with Λ0=0\Lambda_0 = 0Λ0​=0, Λ=3γ4H2\Lambda = \tfrac{3\gamma}{4}H^2Λ=43γ​H2;
  3. H(t)≠0H(t)\neq 0H(t)=0.

Then there is an integration constant H0H_0H0​ such that

1H(t)=ε t+1H0for all t∈I,ε=4−γ2.\frac{1}{H(t)} = \varepsilon\, t + \frac{1}{H_0}\quad\text{for all } t\in I,\qquad \varepsilon = \frac{4-\gamma}{2}.H(t)1​=εt+H0​1​for all t∈I,ε=24−γ​.

This is the paper's inflationary solution. For γ≈4\gamma\approx4γ≈4 one has ε≪1\varepsilon\ll1ε≪1 and H≈H0H\approx H_0H≈H0​, a quasi-de Sitter phase with constant slow-roll parameter.

Formalization Note III is an interval rather than all of R\mathbb RR because 1/H1/H1/H vanishes at a finite time, so no solution with H≠0H\neq0H=0 exists for all times when ε≠0\varepsilon\neq0ε=0. H0H_0H0​ enters only through 1/H01/H_01/H0​, so (with 1/0=01/0=01/0=0 in Lean) the claim is that 1/H−εt1/H - \varepsilon t1/H−εt is constant on III.

Preamble
import Mathlib
open Filter Topology
Formal statement
namespace CarneiroParticleCreation

theorem inflation_solution (I : Set ℝ) (hI : IsOpen I) (hIc : IsPreconnected I)
    (γ : ℝ) (hγ : γ ≠ 4) (H ρm Λ : ℝ → ℝ)
    (hH : ∀ t ∈ I, DifferentiableAt ℝ H t)
    (h13 : ∀ t ∈ I, deriv ρm t + 3 * H t * (ρm t + ρm t / 3) = γ * H t * ρm t)
    (h14 : ∀ t ∈ I, ρm t + Λ t = 3 * H t ^ 2)
    (h16 : ∀ t ∈ I, Λ t = 3 * γ / 4 * H t ^ 2)
    (hH0 : ∀ t ∈ I, H t ≠ 0) :
    ∃ H₀ : ℝ, ∀ t ∈ I, 1 / H t = (4 - γ) / 2 * t + 1 / H₀ := by sorry

end CarneiroParticleCreation
Source
S. Carneiro, "Inflation driven by particle creation", AIP Conf. Proc. 1471 (2012) 61-65, https://doi.org/10.1063/1.4756813, p. 64, Eq. (17), from Eqs. (13), (14), (16) with Λ₀ = 0
Human review
  • Endorsed by Shuze Chen · Oct 11, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Lucas · Oct 11, 2026

    Confirmed by the mission captain (proposal self-audit).

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