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import OAI.MeasureTheory.Falconer.Recursion.ProfileEnvelopes
import OAI.MeasureTheory.Falconer.Estimates.RegularizationSelection
import Mathlib.Analysis.SpecialFunctions.Pow.Asymptotics
namespace OAI
/-!
# Frostman lower envelopes for the constructed all-dimensional profiles
The enclosing-ball constant is 2*sqrt d, and the numerical choice of block
length is independent of dimension.
-/
namespace Falconer.Regularization
open Set MeasureTheory Metric
open scoped ENNReal
variable {d : ℕ}
theorem dyadic_rpow_scale {N : ℕ} (hN : 0 < N) (j : ℕ) (s : ℝ) :
((2:ℝ)^N)^(-s*(j:ℝ)/(N:ℝ)) = (((2:ℝ)^j)^s)⁻¹ := by
rw [← Real.rpow_natCast_mul (by norm_num : (0:ℝ) ≤ 2)]
have hN' : (N:ℝ) ≠ 0 := by exact_mod_cast hN.ne'
have he : (N:ℝ)*(-s*(j:ℝ)/(N:ℝ)) = -((j:ℝ)*s) := by field_simp
rw [he,Real.rpow_neg (by norm_num : (0:ℝ) ≤ 2),Real.rpow_natCast_mul (by norm_num : (0:ℝ) ≤ 2)]
theorem dyadic_cell_frostman_bound (hd : 0 < d) (Q : DyadicCube d) (hQ : 0 < Q.side)
(μ : Measure (Space d)) {s C : ℝ}
(hball : ∀ x : Space d, ∀ r > 0, μ (ball x r) ≤ ENNReal.ofReal (C*r^s))
(p : CellPath d) :
μ (Q.descendant p).carrier ≤ ENNReal.ofReal (C*(2*Real.sqrt d*(Q.descendant p).side)^s) := by
have hside := Q.descendant_side_pos hQ p
have hsqrt : 0 < Real.sqrt (d : ℝ) := Real.sqrt_pos.mpr (by exact_mod_cast hd)
apply (measure_mono (show (Q.descendant p).carrier ⊆
ball (Q.descendant p).center (2*Real.sqrt d*(Q.descendant p).side) from ?_)).trans
(hball _ _ (by positivity))
intro x hx
have hh := (Q.descendant p).dist_le hside.le hx ((Q.descendant p).center_mem hside)
exact mem_ball.mpr (by nlinarith [mul_pos hsqrt hside])
theorem dyadic_cell_frostman_profile_bound (hd : 0 < d) (Q : DyadicCube d) (hQ : 0 < Q.side)
(μ : Measure (Space d)) [IsFiniteMeasure μ] {s C : ℝ} (hC : 0 ≤ C)
(hball : ∀ x : Space d, ∀ r > 0, μ (ball x r) ≤ ENNReal.ofReal (C*r^s))
{N : ℕ} (hN : 0 < N) (p : CellPath d) :
(μ (Q.descendant p).carrier).toReal ≤
(C*(2*Real.sqrt d*Q.side)^s)*((2:ℝ)^N)^(-s*(p.length:ℝ)/(N:ℝ)) := by
have hh := ENNReal.toReal_mono ENNReal.ofReal_ne_top (dyadic_cell_frostman_bound hd Q hQ μ hball p)
have hside := Q.descendant_side_pos hQ p
rw [ENNReal.toReal_ofReal (by positivity : 0 ≤ C*(2*Real.sqrt d*(Q.descendant p).side)^s)] at hh
apply hh.trans_eq
rw [Q.descendant_side,dyadic_rpow_scale hN]
rw [show 2*Real.sqrt d*(Q.side/(2:ℝ)^p.length) =
(2*Real.sqrt d*Q.side)/(2:ℝ)^p.length by ring,
Real.div_rpow (by positivity) (by positivity)]
ring
theorem fixed_constant_absorbed {lam : ℝ} (hlam : 0 < lam) (C : ℝ) :
∃ N₀ : ℕ, ∀ N ≥ N₀, C ≤ ((2:ℝ)^N)^lam := by
have ht : Filter.Tendsto (fun N : ℕ => ((2:ℝ)^N)^lam) Filter.atTop Filter.atTop :=
(tendsto_rpow_atTop hlam).comp (tendsto_pow_atTop_atTop_of_one_lt (by norm_num))
exact Filter.eventually_atTop.mp (ht.eventually (Filter.eventually_ge_atTop C))
theorem retained_label_real_mass_lower (Q : DyadicCube d) (μ : Measure (Space d))
[IsFiniteMeasure μ] {N B : ℕ} {p : CellPath d} {lam : ℝ}
(hp : regularizationLabel Q μ N B p ∈ regularizationIndex Q μ N B
(ENNReal.ofReal (((2:ℝ)^N)^(-lam)))) :
((2:ℝ)^N)^(-lam) ≤ (classMeasure Q μ (regularizationLeaves Q μ N)
(regularizationLabel Q μ N B) (regularizationLabel Q μ N B p) univ).toReal := by
have hm := regularizationSet_mass Q μ N B _ hp
have hh := ENNReal.toReal_mono (measure_ne_top μ _) hm
simpa only [classMeasure,Measure.restrict_apply_univ,regularizationSet,
ENNReal.toReal_ofReal (by positivity : 0 ≤ ((2:ℝ)^N)^(-lam))] using hh
theorem sourceProfile_frostman_envelope (hd : 0 < d) (Q : DyadicCube d) (hQ : 0 < Q.side)
(μ : Measure (Space d)) [IsProbabilityMeasure μ] {s C lam : ℝ} (hC : 0 ≤ C)
(hlam : 0 < lam) (hball : ∀ x : Space d, ∀ r > 0,
μ (ball x r) ≤ ENNReal.ofReal (C*r^s)) :
∃ H N₀ : ℕ, 0 < H ∧ ∀ N ≥ N₀, ∀ p ∈ regularizationLeaves Q μ N,
regularizationLabel Q μ N (N/H) p ∈ regularizationIndex Q μ N (N/H)
(ENNReal.ofReal (((2:ℝ)^N)^(-lam))) →
∀ j ≤ N, s*(j:ℝ)/(N:ℝ)-((d:ℝ)+3)*lam ≤ sourceProfile Q μ N (N/H) p j := by
obtain ⟨H,N₁,hH,hscales⟩ := PlanarFalconer.exists_regularization_block_control hlam
obtain ⟨N₂,hconst⟩ := fixed_constant_absorbed hlam (C*(2*Real.sqrt d*Q.side)^s)
refine ⟨H,max N₁ N₂,hH,?_⟩
intro N hN p hp hret j hj
have hs := hscales N ((le_max_left _ _).trans hN)
apply sourceProfile_frostman_lower Q hQ μ hs.1 hs.2.1 hs.2.2.2.1 hs.2.2.2.2 hp
(retained_label_real_mass_lower Q μ hret) _ hj
intro k hk P hP
have hh := dyadic_cell_frostman_profile_bound hd Q hQ μ hC hball hs.1 P
rw [hP] at hh
exact hh.trans (mul_le_mul_of_nonneg_right (hconst N ((le_max_right _ _).trans hN)) (by positivity))
end Falconer.Regularization
end OAI