Iterated periodic Fourier integration by parts #
This file iterates the one-step boundary-free identity on [-π, π].
The hypothesis records exactly the endpoint jets used in the iteration:
orders strictly below the number of integrations by parts.
Endpoint periodicity of the jets used in r integrations by parts.
Equations
- Anderson4D.NegPiPiPeriodicJets f r = ∀ j < r, iteratedDeriv j f Real.pi = iteratedDeriv j f (-Real.pi)
Instances For
theorem
Anderson4D.fourierCoeffOn_negPi_pi_eq_inv_I_pow_mul_iteratedDeriv
{f : ℝ → ℂ}
{n : ℤ}
(hn : n ≠ 0)
(r : ℕ)
(hf : ContDiff ℝ (↑r) f)
(hperiod : NegPiPiPeriodicJets f r)
:
Exact r-fold periodic integration by parts on [-π, π].
theorem
Anderson4D.norm_fourierCoeffOn_negPi_pi_le_inv_abs_pow_mul_iteratedDeriv
{f : ℝ → ℂ}
{n : ℤ}
(hn : n ≠ 0)
(r : ℕ)
(hf : ContDiff ℝ (↑r) f)
(hperiod : NegPiPiPeriodicJets f r)
:
Norm consequence of exact r-fold integration by parts.
theorem
Anderson4D.norm_fourierCoeffOn_negPi_pi_le_iteratedDeriv_integral
{f : ℝ → ℂ}
{n : ℤ}
(hn : n ≠ 0)
(r : ℕ)
(hf : ContDiff ℝ (↑r) f)
(hperiod : NegPiPiPeriodicJets f r)
:
The final L¹ estimate after r periodic integrations by parts.
theorem
Anderson4D.norm_fourierCoeffOn_negPi_pi_le_eighthDeriv_integral
{f : ℝ → ℂ}
{n : ℤ}
(hn : n ≠ 0)
(hf : ContDiff ℝ 8 f)
(hperiod : NegPiPiPeriodicJets f 8)
:
Eight-fold periodic integration by parts in the form consumed by the relative-translation argument.