import OAI.Geometry.RCD.Coordinates.CoordinateHeatInput import OAI.Geometry.RCD.Coordinates.LongBoundedSource import OAI.Geometry.RCD.Harmonic.AveragedLpPairing import OAI.Geometry.RCD.Heat.DyadicTimeIntegral namespace OAI /-! # Integrating the bounded curvature and endpoint source estimates -/ open Set Metric MeasureTheory open scoped BigOperators ENNReal noncomputable section namespace RegularPointCoordinates variable {X : Type*} [MetricSpace X] [MeasurableSpace X] [BorelSpace X] [ProperSpace X] (μ : Measure X) [μ.Regular] [IsLocallyFiniteMeasure μ] (hQ : QuadraticCheegerEnergy μ) {ker : ℝ → X → X → ℝ} (hk : IsContinuousHeatKernel μ hQ ker) include hk in /-- The complete short-time bounded-source contribution has the square of the averaging radius. -/ theorem exists_short_bounded_source_integral_bound (hg : HasCoordinateHeatBounds μ ker) (n : ℕ) {A V W : ℝ} (hA : 0 ≤ A) (hV : 0 < V) (hW : 0 ≤ W) : ∃ C : ℝ, 0 < C ∧ ∀ (R : ℝ), 0 < R → R ≤ 1 → ∀ (i : ℕ) (x q : X), μ (ball q (R / 2 ^ i)) ≠ ∞ → V * (R / 2 ^ i) ^ n ≤ μ.real (ball q (R / 2 ^ i)) → dist x q ≤ A * (R / 2 ^ i) → (∀ j ≤ i, μ.real (ball x (2 ^ j * (R / 2 ^ i))) ≤ W * (2 ^ j * (R / 2 ^ i)) ^ n) → (∀ t, 0 < t → t ≤ R ^ 2 → ∀ z ∈ ball x R, V * (Real.sqrt t) ^ n ≤ μ.real (ball z (Real.sqrt t))) → ∀ (f : Lp ℝ 2 μ) (B : ℝ), 0 ≤ B → (∀ᵐ z ∂μ, |f z| ≤ B) → (∀ᵐ z ∂μ, z ∉ ball x R → f z = 0) → |∫ t in (0 : ℝ)..(R / 2 ^ i) ^ 2, ∫ z, kernelAverage μ ker t (ball q (R / 2 ^ i)) z * f z ∂μ| ≤ C * B * (R / 2 ^ i) ^ 2 := by obtain ⟨C, hC, hb⟩ := exists_short_bounded_source_bound μ hQ hk hg n hA hV hW refine ⟨C, hC, ?_⟩ intro R hR hR1 i x q hfinite hvol hcenter hupper hsource f B hB hfb hfzero have hs : 0 < R / (2 : ℝ) ^ i := div_pos hR (by positivity) have hsR : (R / (2 : ℝ) ^ i) ^ 2 ≤ R ^ 2 := by apply pow_le_pow_left₀ hs.le exact div_le_self hR.le (one_le_pow₀ (by norm_num)) apply short_time_integral_norm_le hs (by positivity) intro t ht htime have he := hb R hR hR1 i x q hfinite hvol hcenter hupper t ht htime (hsource t ht (htime.trans hsR)) f B hB hfb hfzero nlinarith only [mul_le_mul_of_nonneg_left he (sq_nonneg (R / (2 : ℝ) ^ i))] include hk in /-- All long-time bounded-source blocks sum to r times the working radius. This is the gain needed for the curvature contribution. -/ theorem exists_long_bounded_source_integral_bound (hg : HasCoordinateHeatBounds μ ker) (hdiff : HasGaussianHeatDifferenceBounds μ ker) (n : ℕ) {A V W : ℝ} (hA : 0 ≤ A) (hV : 0 < V) (hW : 0 ≤ W) : ∃ C : ℝ, 0 < C ∧ ∀ (R : ℝ), 0 < R → R ≤ 1 → ∀ (i : ℕ) (x q : X), μ (ball q (R / 2 ^ i)) ≠ ∞ → 0 < μ.real (ball q (R / 2 ^ i)) → dist x q ≤ A * (R / 2 ^ i) → (∀ j, μ.real (ball x (R / 2 ^ j)) ≤ W * (R / 2 ^ j) ^ n) → (∀ t, 0 < t → t ≤ R ^ 2 → ∀ z ∈ ball x R, V * (Real.sqrt t) ^ n ≤ μ.real (ball z (Real.sqrt t))) → ∀ (f : Lp ℝ 2 μ) (B : ℝ), 0 ≤ B → (∀ᵐ z ∂μ, |f z| ≤ B) → (∀ᵐ z ∂μ, z ∉ ball x R → f z = 0) → |∫ t in (R / 2 ^ i) ^ 2..R ^ 2, ∫ z, (kernelAverage μ ker t (ball q (R / 2 ^ i)) z - ker t x z) * f z ∂μ| ≤ C * B * (R / 2 ^ i) * R := by obtain ⟨C, hC, hb⟩ := exists_long_bounded_source_bound μ hQ hk hg hdiff n hA hV hW refine ⟨2 * C, by positivity, ?_⟩ intro R hR hR1 i x q hfinite hvol hcenter hupper hsource f B hB hfb hfzero let F := fun t => ∫ z, (kernelAverage μ ker t (ball q (R / 2 ^ i)) z - ker t x z) * f z ∂μ have hs : 0 < R / (2 : ℝ) ^ i := div_pos hR (by positivity) have hsR : (R / (2 : ℝ) ^ i) ^ 2 ≤ R ^ 2 := by apply pow_le_pow_left₀ hs.le exact div_le_self hR.le (one_le_pow₀ (by norm_num)) have hi := kernelAverage_difference_lp_intervalIntegrable μ hQ hk (ball q (R / (2 : ℝ) ^ i)) measurableSet_ball hfinite x f (sq_pos_of_pos hs) hsR have hblock : ∀ j < i, |∫ t in (R / (2 : ℝ) ^ j) ^ 2 / 4..(R / (2 : ℝ) ^ j) ^ 2, F t| ≤ C * B * (R / (2 : ℝ) ^ i) * (R / (2 : ℝ) ^ j) := by intro j hji have hj : 0 < R / (2 : ℝ) ^ j := div_pos hR (by positivity) have hrj : R / (2 : ℝ) ^ i ≤ (R / (2 : ℝ) ^ j) / 2 := by rw [div_div, ← pow_succ] exact div_le_div_of_nonneg_left hR.le (by positivity) (pow_le_pow_right₀ (by norm_num) hji) have hjR : (R / (2 : ℝ) ^ j) ^ 2 ≤ R ^ 2 := by apply pow_le_pow_left₀ hj.le exact div_le_self hR.le (one_le_pow₀ (by norm_num)) apply dyadic_time_integral_norm_le hj (by positivity) intro t htime have ht : 0 < t := (div_pos (sq_pos_of_pos hj) (by norm_num : (0 : ℝ) < 4)).trans_le htime.1 have hroot : (2 : ℝ) ^ j * (R / (2 : ℝ) ^ j) = R := by field_simp have he := hb R hR hR1 j (R / (2 : ℝ) ^ i) x q hs hrj hfinite hvol hcenter (fun k hk => by have he := outward_radius_eq_ancestor hroot (Nat.sub_le j k) simp only [Nat.sub_sub_self hk] at he rw [he] exact hupper (j - k)) t ht htime (hsource t ht (htime.2.trans hjR)) f B hB hfb hfzero have hm := mul_le_mul_of_nonneg_left he (sq_nonneg (R / (2 : ℝ) ^ j)) apply hm.trans_eq field_simp have he := dyadic_time_integral_abs_le F hR i hi _ hblock have hsum : (∑ j ∈ Finset.range i, C * B * (R / (2 : ℝ) ^ i) * (R / (2 : ℝ) ^ j)) = C * B * (R / (2 : ℝ) ^ i) * R * ∑ j ∈ Finset.range i, (1 / 2 : ℝ) ^ j := by rw [Finset.mul_sum] apply Finset.sum_congr rfl intro j _ rw [div_eq_mul_inv, one_div_pow] ring rw [hsum] at he have hbound := mul_le_mul_of_nonneg_left (sum_geometric_two_le i) (by positivity : 0 ≤ C * B * (R / (2 : ℝ) ^ i) * R) nlinarith only [he, hbound] end RegularPointCoordinates end end OAI