OAI/Analysis/LipschitzHilbert/Phase/SourceAngularLongCellMask.lean
2 declarations, 0 contain sorry, 0 declared as axioms
The same parent-witness density masks at an independent angular
width. Spatial strip volumes remain determined by P.width.
- theorem
OAI.LipschitzHilbert.SourceLabeledLattice.exists_angular_long_cell_maskline 16 - theorem
OAI.LipschitzHilbert.SourceLabeledLattice.exists_angular_whitney_masksline 53Source documentation
Choose the density masks on the entire actual Whitney partition. Cells without long packets receive the empty mask.
theorem exists_angular_whitney_masks (b w : ℝ) (cell : ∀ j, P.labels j → ℤ) (grid : ℤ) (tau : ℝ) (htime : P.topLength≤tau) (hY : ∀ a : P.PacketIndex, |P.actualZ a.1 a.2.1 a.2.2-b|≤P.width/2) (hreference : ∀ a : P.PacketIndex, 0∈ scaledAngularCell (w/P.topLength) grid a.1.val (cell a.1 a.2.1)) (E : Set (ℝ×ℝ)) (hE : MeasurableSet E) (u : ℝ×ℝ → ℝ) (hu : Measurable u) (eta : ℝ) (heta : 0≤eta) (hdensity : ∀ a, P.ordinaryDensity 0 cell grid w tau E u a≤eta) : ∃ Omega : P.DensityWhitneyCell → Set ℝ, (∀ i, MeasurableSet (Omega i)) ∧ (∀ i, ¬P.HasLongPacket i → Omega i=∅) ∧ …Mentions: OAI.LipschitzHilbert.scaledAngularCell