OAI/Geometry/RCD/Sobolev/PoissonDefectBudget.lean
5 declarations, 0 contain sorry, 0 declared as axioms
The summable defect including the Poisson curvature remainder
- theorem
OAI.RegularPointCoordinates.distanceSourceRadius_sqline 13 - def
OAI.RegularPointCoordinates.normalizedPoissonDefectline 23Source documentation
The second term is the actual curvature remainder in the shifted Poisson mass estimate, in the same normalized units as the full source.
def normalizedPoissonDefect {n : ℕ} {κ r0 : ℝ} {p : X} (S : DyadicDistanceSources μ hQ n κ p r0) (i : ℕ) : ℝ := … - theorem
OAI.RegularPointCoordinates.normalizedPoissonDefect_nonnegline 28 - theorem
OAI.RegularPointCoordinates.normalizedPoissonDefect_unitsline 37Source documentation
Source and curvature masses have exactly the same normalization; the identity uses the actual volume, not a Euclidean replacement.
theorem normalizedPoissonDefect_units {n : ℕ} {κ r0 : ℝ} {p : X} (S : DyadicDistanceSources μ hQ n κ p r0) (i : ℕ) : (distanceSourceRadius r0 i) ^ (n : ℝ) * normalizedPoissonDefect μ hQ S i = (S.source i).real (ball p (distanceSourceRadius r0 i)) + κ * (distanceSourceRadius r0 i) ^ 2 * μ.real (ball p (distanceSourceRadius r0 i)) := by …Mentions: OAI.RegularPointCoordinates.DyadicDistanceSources, OAI.RegularPointCoordinates.distanceSourceRadius, OAI.RegularPointCoordinates.normalizedPoissonDefect
- theorem
OAI.RegularPointCoordinates.DyadicDistanceSources.poisson_defect_budgetline 50Source documentation
The extra curvature remainder costs at most kappa*C*r0²/3 in the total budget. The original positive source measures remain unchanged.
theorem DyadicDistanceSources.poisson_defect_budget {n : ℕ} {κ r0 C : ℝ} {p : X} (S : DyadicDistanceSources μ hQ n κ p r0) (hκ : 0 ≤ κ) (hC : 0 ≤ C) (hsource : Summable (normalizedDistanceSourceMass μ hQ S)) (hvolume : ∀ i, (distanceSourceRadius r0 i) ^ (-(n : ℝ)) * μ.real (ball p (distanceSourceRadius r0 i)) ≤ C) : Summable (normalizedPoissonDefect μ hQ S) ∧ (∑' i, normalizedPoissonDefect μ hQ S i) ≤ (∑' i, normalizedDistanceSourceMass μ hQ S i) + κ * C * r0 ^ 2 / 3 := by …Mentions: OAI.RegularPointCoordinates.DyadicDistanceSources, OAI.RegularPointCoordinates.normalizedDistanceSourceMass, OAI.RegularPointCoordinates.distanceSourceRadius, OAI.RegularPointCoordinates.normalizedPoissonDefect