OAI/Analysis/LipschitzHilbert/Packets/SourceSelectorConcentrationCenteredFamily.lean

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5 declarations, 0 contain sorry, 0 declared as axioms

The centered main part has one weighted physical exception for all tops and both required jets. Three monotone cutoffs produce only a fixed loss, absorbed in the polynomial threshold.

  1. theorem OAI.LipschitzHilbert.SourceLatticePacket.frozen_centered_rawInterval_eq line 19

    Source documentation

    Exact centered interval identity, including cutoff boundaries.

    theorem frozen_centered_rawInterval_eq
        (P : SourceLatticePacket N κ ι)
        (c : ∀ j, ι j → κ → ℂ) (hc : ∀ j u k, ‖c j u k‖ ≤ 1)
        (alt : ∀ j, ι j → κ → SchwartzMap (ℝ×ℝ) ℂ)
        (hAlt : ∀ j u k, planarProfileConstant (alt j u k) (2*P.order) ≤ P.profileBound)
        (t : ℝ) (d : Fin N → ℝ) (hd : ∀ j, 0 ≤ d j)
        (v : ℝ×ℝ → ℝ) (hv : Measurable v)
        (g : ℝ×ℝ → EuclideanSpace ℂ κ) (hg : Measurable g) (hg1 : ∀ z, ‖g z‖ ≤ 1)
        (i : Fin 3) (lower upper : ℕ) (x y : ℝ) :
        (P.withProfile alt hAlt).rawInterval
            ((P.frozenProfile c hc).physicalCenteredCoefficient t t d v g) i lower upper x y =
          (P.withProfile alt hAlt).rawInterval
    …

    Mentions: OAI.LipschitzHilbert.SourceLatticePacket, OAI.LipschitzHilbert.planarProfileConstant, OAI.LipschitzHilbert.SourceLatticePacket.rawInterval, OAI.LipschitzHilbert.SourceLatticePacket.physicalCenteredCoefficient

  2. theorem OAI.LipschitzHilbert.SourceLatticePacket.frozen_physical_rawInterval_eq_reference line 69

    Source documentation

    Each one-sided physical coefficient is the same original reference integral after the measure-preserving shear.

    theorem frozen_physical_rawInterval_eq_reference
        (P : SourceLatticePacket N κ ι)
        (c : ∀ j, ι j → κ → ℂ) (hc : ∀ j u k, ‖c j u k‖ ≤ 1)
        (alt : ∀ j, ι j → κ → SchwartzMap (ℝ×ℝ) ℂ)
        (hAlt : ∀ j u k, planarProfileConstant (alt j u k) (2*P.order) ≤ P.profileBound)
        (t : ℝ) (d : Fin N → ℝ) (v : ℝ×ℝ → ℝ)
        (g : ℝ×ℝ → EuclideanSpace ℂ κ) (i : Fin 3) (lower upper : ℕ) (x y : ℝ) :
        (P.withProfile alt hAlt).rawInterval
            ((P.frozenProfile c hc).physicalCoefficient t d v g) i lower upper x y =
          (P.withProfile alt hAlt).rawInterval
            ((P.frozenProfile c hc).family.mainCoefficient d
              (fun z => v (sourceReferenceToPhysical t z))
    …

    Mentions: OAI.LipschitzHilbert.SourceLatticePacket, OAI.LipschitzHilbert.planarProfileConstant, OAI.LipschitzHilbert.SourceLatticePacket.rawInterval, OAI.LipschitzHilbert.SourceLatticePacket.physicalCoefficient, OAI.LipschitzHilbert.sourceReferenceToPhysical

  3. def OAI.LipschitzHilbert.SourceLatticePacket.centeredPhaseCutoff line 90

    Also declared: OAI/Analysis/LipschitzHilbert/Packets/SourceSupportedConcentrationCentered.lean:18 (same declaration text).

  4. def OAI.LipschitzHilbert.SourceLatticePacket.centeredPhaseField line 93

    Also declared: OAI/Analysis/LipschitzHilbert/Packets/SourceSupportedConcentrationCentered.lean:21 (same declaration text).

  5. theorem OAI.LipschitzHilbert.SourceLatticePacket.source_frozen_centered_family_concentration line 97