OAI/Geometry/RCD/Sobolev/LocalPoissonDimensionalDensity.lean
2 declarations, 0 contain sorry, 0 declared as axioms
Finite-dimensional density bound for the actual Poisson measure
This is a consequence of the scalar weak Bochner inequality of Han, Theorem 3.3. Countable compact exhaustion retains the prescribed full measure and proves the density bound on the whole interior ball.
- theorem
OAI.RegularPointCoordinates.NoncollapsedRCD.local_poisson_dimensional_densityline 21 - theorem
OAI.RegularPointCoordinates.NoncollapsedRCD.local_poisson_shifted_densityline 47Source documentation
Completing the one-dimensional square supplies every scalar shift, without a separate assertion about the local dimension.
theorem NoncollapsedRCD.local_poisson_shifted_density {K : ℝ} {n : ℕ} (hX : NoncollapsedRCD K n X) [(hausdorff n X).Regular] (hn : 2≤n) (hscalar : ScalarDimensionalBochner (hausdorff n X) hX.quadratic K n) (f : SobolevSpace (hausdorff n X) hX.quadratic) (c κ : ℝ) (hK : -κ≤K) {p : X} {r : ℝ} (hr : 0<r) (hf : IsConstantLaplacianOn (hausdorff n X) hX.quadratic (ball p (8*r)) f c) (L : ℝ≥0) (hL : ∀ᵐ x ∂(hausdorff n X).restrict (ball p (8*r)), localGamma (hausdorff n X) hX.quadratic f f x≤(L:ℝ)^2) (F₀ : SobolevSpace (hausdorff n X) hX.quadratic) (σ : Measure X) [IsFiniteMeasure σ] (hF₀ : SobolevSpace.toLp (hausdorff n X) hX.quadratic F₀ =ᵐ[(hausdorff n X).restrict (ball p (2*r))] localGamma (hausdorff n X) hX.quadratic f f) …Mentions: OAI.RegularPointCoordinates.NoncollapsedRCD, OAI.RegularPointCoordinates.hausdorff, OAI.RegularPointCoordinates.ScalarDimensionalBochner, OAI.RegularPointCoordinates.SobolevSpace, OAI.RegularPointCoordinates.IsConstantLaplacianOn, OAI.RegularPointCoordinates.localGamma, OAI.RegularPointCoordinates.SobolevSpace.toLp