OAI/Geometry/RCD/Heat/DyadicTimeIntegral.lean
2 declarations, 0 contain sorry, 0 declared as axioms
Finite dyadic time decomposition for actual integrable sources
- theorem
OAI.RegularPointCoordinates.dyadic_time_integral_eq_sumline 17Source documentation
Consecutive dyadic time blocks telescope exactly. Integrability is explicit, so no use is made of the undefined-integral zero convention.
theorem dyadic_time_integral_eq_sum (f : ℝ → ℝ) {R : ℝ} (hR : 0 < R) (i : ℕ) (hf : IntervalIntegrable f volume ((R / (2 : ℝ) ^ i) ^ 2) (R ^ 2)) : (∫ t in (R / (2 : ℝ) ^ i) ^ 2..R ^ 2, f t) = ∑ j ∈ Finset.range i, ∫ t in (R / (2 : ℝ) ^ j) ^ 2 / 4..(R / (2 : ℝ) ^ j) ^ 2, f t := by … - theorem
OAI.RegularPointCoordinates.dyadic_time_integral_abs_leline 43Source documentation
A bound on each actual block gives the corresponding finite weighted sum on the entire long-time interval.
theorem dyadic_time_integral_abs_le (f : ℝ → ℝ) {R : ℝ} (hR : 0 < R) (i : ℕ) (hf : IntervalIntegrable f volume ((R / (2 : ℝ) ^ i) ^ 2) (R ^ 2)) (B : ℕ → ℝ) (hb : ∀ j < i, |∫ t in (R / (2 : ℝ) ^ j) ^ 2 / 4..(R / (2 : ℝ) ^ j) ^ 2, f t| ≤ B j) : |∫ t in (R / (2 : ℝ) ^ i) ^ 2..R ^ 2, f t| ≤ ∑ j ∈ Finset.range i, B j := by …