Penrose's criterion: is the self-energy of the difference distribution
ProvedPenrose.delta_self_energyFor any real gravitational constant and any two smooth, rapidly decreasing mass distributions on three-dimensional Euclidean space, Penrose's measure of incompatibility
is the gravitational self-energy of the difference of the two mass distributions, up to the explicit constant :
This is the central identification of Section 6 of Penrose (1996, pp. 595–597): the measure of incompatibility of the two superposed space-time geometries — the quantity whose order of magnitude, divided into , gives the lifetime of the superposed state — is basically just the gravitational self-energy of the difference between the two mass distributions. The paper itself notes the constant is loose (apart from the factor it makes no difference which expression is used); here the constant is made fully explicit, and the two sides are defined independently: an norm of a field difference on the left, a double integral of densities on the right.
The statement places no hypothesis on beyond smoothness and rapid decrease, and none on the sign of .
import Mathlib import Definitions.Def_penrose import Definitions.Def_penrose_energy open MeasureTheory
namespace Penrose
theorem delta_self_energy (G : ℝ) (ρ ρ' : SchwartzMap (EuclideanSpace ℝ (Fin 3)) ℝ) :
deltaMeasure G ρ ρ' = -8 * Real.pi * G * gravSelfEnergy G (ρ - ρ') := by sorry
end Penrose
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What the Lean code literally says, in plain math · glm-5-latest-short
The statement asserts the following. Let be an arbitrary real number and arbitrary Schwartz functions from three-dimensional Euclidean space to the reals. Write for their difference in the Schwartz space (a pointwise difference). The claim is the equality of real numbers
where is deltaMeasure G ρ ρ', defined in the preamble as the Bochner integral over of the squared Euclidean norm of the difference of the two field-gradient vectors (each an explicit integral vector), and is gravSelfEnergy G σ, defined in the preamble as times the nested Bochner integral of .
The two sides are defined independently: no definition in the preamble identifies them. No hypotheses appear; the statement quantifies over every real (zero and negative included) and every pair of Schwartz densities (including , where both sides are , and densities taking negative values).
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.