OAI/Analysis/LipschitzHilbert/Phase/SourceAngularLongCellMask.lean

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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.

  1. theorem OAI.LipschitzHilbert.SourceLabeledLattice.exists_angular_long_cell_mask line 16
  2. theorem OAI.LipschitzHilbert.SourceLabeledLattice.exists_angular_whitney_masks line 53

    Source 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