OAI/Analysis/SignedDisk/LocalCancellation2.lean
33 declarations, 0 contain sorry, 0 declared as axioms
- lemma
OAI.SignedDisk.LocalCancellation.integrable_bounded_pairingline 21 - lemma
OAI.SignedDisk.LocalCancellation.position_boundline 30 - lemma
OAI.SignedDisk.LocalCancellation.corrected_increment_boundline 43Source documentation
The decisive corrected active increment, prior to substitution of the dyadic powers. The zero moment is the exact one furnished by two balanced kernels, not a bound.
lemma corrected_increment_bound {Cs α δ ρ : ℝ} (b : ι → ErrorPiece Cs) (hCs : 0 ≤ Cs) (hα : α ≤ 1) (hδ : 0 ≤ δ) (hδ1 : δ ≤ 1) (hρ : 0 ≤ ρ) {L : ℝ≥0} {F : ℂ → ℂ} (hF : LipschitzWith L F) {D : Set ℂ} (hD : MeasurableSet D) (hFb : ∀ y, ‖F y‖ ≤ 1) (hFD : ∀ y, F y ≠ 0 → y ∈ D) (x z : ℂ) (hz : (1 : ℝ)/2 ≤ ‖z-x‖) (hD3 : ∀ y ∈ D, ‖y-x‖ ≤ 3) (hzero : ∑ d, ∫ y, star (y-x)*F y*(b d).density y = 0) : ‖∑ d, ∫ y, F y*(b d).density y‖ ≤ 2*ρ*coarseMass b δ univ+7*coarseMass b δ (D \ Metric.ball z ρ)+ ((L : ℝ)+2*(3*(L : ℝ)+1))*Cs*δ^(2*(1-α))*errorPrice b α := by …Mentions: OAI.SignedDisk.LocalCancellation.ErrorPiece, OAI.SignedDisk.LocalCancellation.coarseMass, OAI.SignedDisk.LocalCancellation.errorPrice
- lemma
OAI.SignedDisk.DiskKernels.kernel_nonnegline 102 - lemma
OAI.SignedDisk.DiskKernels.kernel_le_oneline 105 - lemma
OAI.SignedDisk.DiskKernels.complex_kernel_lipschitzline 108 - lemma
OAI.SignedDisk.DiskKernels.complex_kernel_boundline 112 - lemma
OAI.SignedDisk.DiskKernels.difference_boundline 116 - lemma
OAI.SignedDisk.DiskKernels.difference_supportline 122 - lemma
OAI.SignedDisk.DiskKernels.tendsto_kernelline 144Source documentation
At every point away from the boundary circle, all such mixtures tend to the actual sharp disk. No convergence of the chosen radius densities is assumed.
lemma tendsto_kernel {r : ℝ} {δ : ℕ → ℝ} {M : ℕ → ℝ≥0} (k : ∀ n, RadiusDensity (r-δ n) (r+δ n) (M n)) (hδ : Tendsto δ atTop (𝓝 0)) (x y : ℂ) (hy : ‖y-x‖ ≠ r) : Tendsto (fun n => kernel (k n) x y) atTop (𝓝 ((Metric.ball x r).indicator (fun _ => (1 : ℝ)) y)) := by …Mentions: OAI.SignedDisk.DiskKernels.RadiusDensity, OAI.SignedDisk.DiskKernels.kernel
- lemma
OAI.SignedDisk.DiskKernels.tendsto_kernel_pairingline 170Source documentation
Dominated convergence of an arbitrary sequence of mixtures against each actual absolutely continuous finite vector measure.
lemma tendsto_kernel_pairing {r : ℝ} {δ : ℕ → ℝ} {M : ℕ → ℝ≥0} (k : ∀ n, RadiusDensity (r-δ n) (r+δ n) (M n)) (hδ : Tendsto δ atTop (𝓝 0)) (x : ℂ) {b : ℂ → ℂ} (hb : Integrable b) : Tendsto (fun n => ∫ y, (kernel (k n) x y : ℂ)*b y) atTop (𝓝 (∫ y in Metric.ball x r, b y)) := by …Mentions: OAI.SignedDisk.DiskKernels.RadiusDensity, OAI.SignedDisk.DiskKernels.kernel
- theorem
OAI.SignedDisk.LocalCancellation.size_stepline 202 - lemma
OAI.SignedDisk.DiskGeometry.thinShell_eq_diffline 258 - lemma
OAI.SignedDisk.DiskGeometry.volume_thinShellline 266Source documentation
Exact area of an annulus, including the inner and outer circles.
lemma volume_thinShell (x : ℂ) {r δ : ℝ} (hδ : 0 ≤ δ) (hr : δ ≤ r) : volume (thinShell x r δ) = ENNReal.ofReal (4*Real.pi*r*δ) := by …Mentions: OAI.SignedDisk.DiskGeometry.thinShell
- lemma
OAI.SignedDisk.DiskGeometry.measurableSet_shellPairsline 282 - def
OAI.SignedDisk.DiskGeometry.shellMassline 286 - lemma
OAI.SignedDisk.DiskGeometry.measurable_shellMassline 288 - lemma
OAI.SignedDisk.DiskGeometry.shell_symmline 292 - lemma
OAI.SignedDisk.DiskGeometry.lintegral_shellMassline 296Source documentation
The integrated shell mass is its exact area times the total input mass.
lemma lintegral_shellMass (ν : Measure ℂ) [IsFiniteMeasure ν] {r δ : ℝ} (hδ : 0 ≤ δ) (hr : δ ≤ r) : (∫⁻ x, shellMass ν r δ x) = ENNReal.ofReal (4*Real.pi*r*δ)*ν univ := by …Mentions: OAI.SignedDisk.DiskGeometry.shellMass
- lemma
OAI.SignedDisk.DiskGeometry.shellMass_exceptionline 318 - lemma
OAI.SignedDisk.DiskGeometry.thinShell_subset_endpointline 330Source documentation
A shell whose radius is sufficiently close to an endpoint is contained in the endpoint annulus; this covers forced endpoint radii as well.
lemma thinShell_subset_endpoint {x : ℂ} {r a δ : ℝ} (hra : |r-a| ≤ δ) : thinShell x r δ ⊆ thinShell x a (2*δ) := by …Mentions: OAI.SignedDisk.DiskGeometry.thinShell
- def
OAI.SignedDisk.DiskScales.widthline 344 - lemma
OAI.SignedDisk.DiskScales.width_posline 346 - lemma
OAI.SignedDisk.DiskScales.width_leline 350 - lemma
OAI.SignedDisk.DiskScales.width_succline 354 - lemma
OAI.SignedDisk.DiskScales.width_antitoneline 358 - lemma
OAI.SignedDisk.DiskScales.tendsto_widthline 365 - lemma
OAI.SignedDisk.DiskScales.width_rpowline 371 - lemma
OAI.SignedDisk.DiskScales.ratio_norm_ltline 378 - lemma
OAI.SignedDisk.DiskScales.summable_width_rpowline 382 - lemma
OAI.SignedDisk.DiskScales.tsum_width_rpowline 387 - lemma
OAI.SignedDisk.DiskScales.scaled_incrementline 393 - lemma
OAI.SignedDisk.DiskScales.exists_admissible_widthline 431Source documentation
A single small width works for both shell geometry and every smaller width.
lemma exists_admissible_width : ∃ δ₀ : ℝ, 0 < δ₀ ∧ δ₀ ≤ 1/4 ∧ ∀ δ : ℝ, 0 < δ → δ ≤ δ₀ → δ ≤ (δ^(1/5 : ℝ))^2/1600 := by …