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Corollary 2 — Λ>0\Lambda>0Λ>0 implies a unique vacuum solution of FFR

Proved
FlatlyFoliated.corollary2_unique_vacuum

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

elliptic-pdegeneral-relativitymathematical-physics

Let Λ>0\Lambda>0Λ>0.

  1. (Existence) ω0(x)=Λ/3 x\omega_0(x)=\sqrt{\Lambda/3}\,xω0​(x)=Λ/3​x (i.e. ω0=Λ/3 r dr\omega_0=\sqrt{\Lambda/3}\,r\,drω0​=Λ/3​rdr) and η0=1\eta_0=1η0​=1 form a smooth vacuum solution of the FFR equations (34)–(35) (with μ=0\mu=0μ=0, J=0J=0J=0) that satisfies (∇⋅ω0)/η0>0(\nabla\cdot\omega_0)/\eta_0>0(∇⋅ω0​)/η0​>0 and is spherically symmetric at infinity.
  2. (Uniqueness) If smooth (ω,η)(\omega,\eta)(ω,η) with η>0\eta>0η>0 and (∇⋅ω)/η>0(\nabla\cdot\omega)/\eta>0(∇⋅ω)/η>0 solve the vacuum FFR equations and are spherically symmetric at infinity, then for some constant c>0c>0c>0
η≡c,ω(x)=cΛ/3  x.\eta\equiv c,\qquad \omega(x)=c\sqrt{\Lambda/3}\;x .η≡c,ω(x)=cΛ/3​x.

So the vacuum solution is unique up to an overall positive constant, i.e. a rescaling of the time coordinate.

Formalization Note The arrow-of-time convention (∇⋅ω)/η>0(\nabla\cdot\omega)/\eta>0(∇⋅ω)/η>0 (Convention 1, in force for Λ>0\Lambda>0Λ>0) is an explicit hypothesis; without it the time-reversed solution −ω0-\omega_0−ω0​ also exists.

Preamble
import Mathlib
import Definitions.Def_FlatlyFoliatedRelativity_basic

open scoped ContDiff
Formal statement
namespace FlatlyFoliated

/-- **Goal — Corollary 2**: for `Λ > 0` there is a unique (up to an overall positive
constant, i.e. rescaling of `t`) smooth vacuum solution of (34)–(35) with `η > 0` that is
spherically symmetric at infinity (with the arrow-of-time convention `(∇·w)/η > 0`), namely
`w = √(Λ/3) r ∂ᵣ`, `η = 1`. -/
theorem corollary2_unique_vacuum (Λ : ℝ) (hΛ : 0 < Λ) :
    (ContDiff ℝ ∞ (fun x : R3 => Real.sqrt (Λ / 3) • x) ∧
      (∀ x, 0 < divg (fun x : R3 => Real.sqrt (Λ / 3) • x) x / 1) ∧
      FFREquations Λ 0 0 (fun x : R3 => Real.sqrt (Λ / 3) • x) (fun _ => 1) ∧
      SphSymmAtInfty (fun x : R3 => Real.sqrt (Λ / 3) • x) (fun _ => 1)) ∧
    ∀ (w : R3 → R3) (η : R3 → ℝ),
      ContDiff ℝ ∞ w → ContDiff ℝ ∞ η → (∀ x, 0 < η x) → (∀ x, 0 < divg w x / η x) →
      FFREquations Λ 0 0 w η → SphSymmAtInfty w η →
      ∃ c : ℝ, 0 < c ∧ η = (fun _ => c) ∧ w = fun x => (c * Real.sqrt (Λ / 3)) • x := by sorry

end FlatlyFoliated
Source
Bray, Hamm, Hirsch, Wheeler, Zhang, Flatly Foliated Relativity, arXiv:1911.00967v2, https://arxiv.org/abs/1911.00967, p. 19, Corollary 2 (Section 5; uniqueness up to positive constant and smoothness with η > 0 as defined on p. 15; Convention 1, eq. (54); explicit solution p. 20, ω = √(Λ/3) r dr)
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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