OAI/Geometry/RCD/Heat/ActualHeatEnvelope.lean
4 declarations, 0 contain sorry, 0 declared as axioms
The Gaussian upper decrement in terms of the actual Bochner envelope
- def
OAI.RegularPointCoordinates.dyadicHeatEnvelopeConstantline 20Source documentation
A single constant for the shell convolution, exterior finite mass and scalar regularizer, independent of the dyadic index and vector.
def dyadicHeatEnvelopeConstant (M : PositiveBilinearMeasure X E) (m : ℕ) (A D R lambda η : ℝ) : ℝ := …Mentions: OAI.RegularPointCoordinates.PositiveBilinearMeasure
- theorem
OAI.RegularPointCoordinates.dyadicHeatEnvelopeConstant_nonnegline 28 - theorem
OAI.RegularPointCoordinates.gaussian_mass_budget_le_envelopeline 37Source documentation
Reindexing the Gaussian shell bound and using the finite total source gives the desired actual positive operator envelope.
theorem gaussian_mass_budget_le_envelope (M : PositiveBilinearMeasure X E) (m N : ℕ) (p : X) {s R A D lambda η : ℝ} (hs : 0 < s) (hR : (2 : ℝ) ^ N * s = R) (hA : 0 ≤ A) (hD : 0 < D) (hreg_nonneg : 0 ≤ lambda + η) (v : E) : (3 / 2 : ℝ) * (A * gaussianMassConvolutionConstant m D⁻¹ * (∑ j ∈ Finset.range (N + 1), (3 / 4 : ℝ) ^ j * (((2 ^ j * s) ^ 2 / (2 ^ j * s) ^ (m + 2)) * (M.measure v).real (ball p (2 ^ j * s)))) + s ^ 2 * ((A / s ^ (m + 2)) * Real.exp (-(4 : ℝ) ^ N / D)) * (M.measure v).real univ) + (3 / 4 : ℝ) * s ^ 2 * (lambda + η) * ‖v‖ ^ 2 ≤ dyadicHeatEnvelopeConstant M m A D R lambda η * …Mentions: OAI.RegularPointCoordinates.PositiveBilinearMeasure, OAI.RegularPointCoordinates.gaussianMassConvolutionConstant, OAI.RegularPointCoordinates.dyadicHeatEnvelopeConstant
- theorem
OAI.RegularPointCoordinates.gaussian_dyadic_heat_increment_envelopeline 99Source documentation
The actual cutoff heat Gram satisfies the upper envelope required by the cumulative comparison, with the actual scaled Bochner mass operators.
theorem gaussian_dyadic_heat_increment_envelope (m : ℕ) (hρ : 0 < ρ) (hρr : ρ < r) (hκ : 0 ≤ κ) {s R A D η lambda : ℝ} (hs : 0 < s) (hA : 0 ≤ A) (hD : 0 < D) (hη : 0 ≤ η) (hlambda0 : 0 ≤ lambda) (hlambda : 2 * κ * (L : ℝ) ^ 2 + η ≤ lambda) (herror : ∀ t ∈ Icc (s ^ 2 / 4) (s ^ 2), ‖harmonicHeatError μ hQ (k := ker) G χ t p‖ ≤ η) …