OAI/Geometry/RCD/Heat/GaussianDyadicShells.lean
7 declarations, 0 contain sorry, 0 declared as axioms
Dyadic shell integration and Gaussian summability
- theorem
OAI.RegularPointCoordinates.summable_dyadic_gaussianline 18Source documentation
A geometric volume or normalization loss is summable against the Gaussian decay on dyadic annuli.
theorem summable_dyadic_gaussian {b c d : ℝ} (hb : 0 ≤ b) (hc : 0 < c) (hd : 1 < d) : Summable (fun j : ℕ => b ^ j * Real.exp (-c * d ^ j)) := by … - def
OAI.RegularPointCoordinates.dyadicShellline 47Source documentation
Disjoint dyadic balls, including the initial ball at index zero.
def dyadicShell (p : X) (r : ℝ) (j : ℕ) : Set X := …
- theorem
OAI.RegularPointCoordinates.dyadicShell_subset_ballline 50 - theorem
OAI.RegularPointCoordinates.iUnion_dyadicShellline 54 - theorem
OAI.RegularPointCoordinates.dyadicShell_separationline 62 - theorem
OAI.RegularPointCoordinates.measurableSet_dyadicShellline 75 - theorem
OAI.RegularPointCoordinates.integral_le_dyadic_shell_sum_of_productline 81Source documentation
A weighted integral is bounded by a series of ball error budgets. The kernel bound is only needed on each disjoint shell.
theorem integral_le_dyadic_shell_sum_of_product (μ : Measure X) (p : X) {r : ℝ} (hr : 0 < r) {f w : X → ℝ} {W e : ℕ → ℝ} (hi : Integrable (fun x => w x * f x) μ) (hfi : ∀ j, IntegrableOn f (ball p (2 ^ j * r)) μ) (hf : ∀ᵐ x ∂μ, 0 ≤ f x) (hW : ∀ j, 0 ≤ W j) (hw : ∀ j, ∀ᵐ x ∂μ.restrict (dyadicShell p r j), w x * f x ≤ W j * f x) (he : ∀ j, (∫ x in ball p (2 ^ j * r), f x ∂μ) ≤ e j) (hsum : Summable (fun j => W j * e j)) : (∫ x, w x * f x ∂μ) ≤ ∑' j : ℕ, W j * e j := by …Mentions: OAI.RegularPointCoordinates.dyadicShell