roseking's picture
Add lean source and binary files (part 18)
67aee1d verified
Raw History Blame Contribute Delete
4.34 kB
import OAI.Analysis.FiniteFactor.Sampling.Fourier
import OAI.Analysis.FiniteFactor.OrbitSampling.Powers
namespace OAI
namespace FiniteFactor
open MeasureTheory Filter Finset
noncomputable section
theorem sourceBlockSize_monotone : Monotone sourceBlockSize := by
apply monotone_nat_of_le_succ
intro s
have hp := (sourceStage (s+1)).previous_size
have hd : (sourceBlockSize s : ℝ) ≤ (sourceStageState (s+1)).d := by
change (sourceBlockSize s : ℝ) ≤ ((sourceStageState s).d+(sourceStage s).m : ℕ)
change ((sourceStage s).m : ℝ) ≤ ((sourceStageState s).d+(sourceStage s).m : ℕ)
push_cast
exact le_add_of_nonneg_left (Nat.cast_nonneg _)
have hm : (sourceBlockSize s : ℝ) ≤ sourceBlockSize (s+1) := by
change ((sourceStageState (s+1)).d : ℝ) ≤ (sourceBlockSize (s+1) : ℝ)/100 at hp
have := Nat.cast_nonneg (α := ℝ) (sourceBlockSize (s+1))
linarith
exact_mod_cast hm
theorem sourceFrequencyScale_monotone :
Monotone (fun s => sourceBlockSize s * (sourceStageState s).K) := by
have hK : Monotone (fun s => (sourceStageState s).K) := by
apply monotone_nat_of_le_succ
intro s
have := sourceStage_cutoff_growth s
omega
intro s t hst
exact Nat.mul_le_mul (sourceBlockSize_monotone hst) (hK hst)
/-- The full infinite-product angle expectation has the same coordinate
Fourier estimate; no independence between two phases is asserted. -/
theorem sourceAngleLaw_pair_fourier_le (i : SourceCoordinate) (v v' : ℤ) (n n' : ℝ)
(hw : (v : ℝ)*n+(v' : ℝ)*n' ≠ 0) :
‖∫ θ, Complex.exp (2 * Real.pi * Complex.I *
((v : ℂ) * (Int.fract (n*θ i) : ℝ) + (v' : ℂ) * (Int.fract (n'*θ i) : ℝ)))
∂sourceAngleLaw‖ ≤
1/(Real.pi*sourceAngleUnit i*|(v : ℝ)*n+(v' : ℝ)*n'|) := by
have hh := sourceAngle_pair_fourier_le i v v' n n' hw
simp_rw [pair_fourier_fract] at hh ⊢
rw [← sourceAngleLaw_coordinate i,
integral_map (measurable_pi_apply i).aemeasurable (by fun_prop)] at hh
exact hh
theorem sourceSampling_pair_fourier_bound (s : ℕ) (hs : 200000 ≤ sourceBlockSize s)
(i : SourceCoordinate) (hi : i.1 ≤ s) (n n' : ℤ)
(hn : n ∈ sourceSamplingPowers s) (hn' : n' ∈ sourceSamplingPowers s) (hne : n ≠ n')
(v v' : ℤ) (hv : |v| ≤ (samplingH (sourceBlockSize s) : ℤ))
(hv' : |v'| ≤ (samplingH (sourceBlockSize s) : ℤ)) (hvv' : v ≠ 0 ∨ v' ≠ 0) :
‖∫ θ, Complex.exp (2 * Real.pi * Complex.I *
((v : ℂ) * (Int.fract ((n : ℝ)*θ i) : ℝ) +
(v' : ℂ) * (Int.fract ((n' : ℝ)*θ i) : ℝ))) ∂sourceAngleLaw‖ ≤
Real.pi⁻¹*(sourceBlockSize s : ℝ)^(-1000 : ℝ) := by
have hsep := (sourceSamplingPowers_spec s hs).2.2 hn hn' hne
have hfreq : (samplingR (sourceBlockSize s) (sourceStageState s).K : ℤ) < |v*n+v'*n'| := by
by_contra hh
exact hsep ⟨v,mem_Icc.mpr (abs_le.mp hv),v',mem_Icc.mpr (abs_le.mp hv'),hvv',le_of_not_gt hh⟩
let w : ℝ := (v : ℝ)*(n : ℝ)+(v' : ℝ)*(n' : ℝ)
have hwR : (samplingR (sourceBlockSize s) (sourceStageState s).K : ℝ) < |w| := by
dsimp [w]
exact_mod_cast hfreq
have hwpos : 0 < |w| := lt_of_le_of_lt (Nat.cast_nonneg _) hwR
have hw : w ≠ 0 := abs_pos.mp hwpos
apply (sourceAngleLaw_pair_fourier_le i v v' (n : ℝ) (n' : ℝ) hw).trans
have hN : (sourceBlockSize i.1 : ℝ)*(sourceStageState i.1).K ≤
(sourceBlockSize s : ℝ)*(sourceStageState s).K := by
exact_mod_cast sourceFrequencyScale_monotone hi
have hmpos := sourceBlockSize_pos s
have hNpos := mul_pos (sourceBlockSize_pos i.1) (sourceCutoff_pos i.1)
have hscale : (sourceBlockSize s : ℝ)^1000 ≤ sourceAngleUnit i * |w| := by
unfold samplingR at hwR
push_cast at hwR
unfold sourceAngleUnit
rw [one_div, inv_mul_eq_div, le_div_iff₀ hNpos]
have hh := mul_le_mul_of_nonneg_right hN (pow_nonneg hmpos.le 1000)
nlinarith
change 1/(Real.pi*sourceAngleUnit i*|w|) ≤ _
calc
_ = Real.pi⁻¹*(1/(sourceAngleUnit i*|w|)) := by ring
_ ≤ Real.pi⁻¹*(1/(sourceBlockSize s : ℝ)^1000) := by
exact mul_le_mul_of_nonneg_left
(one_div_le_one_div_of_le (pow_pos hmpos 1000) hscale) (inv_nonneg.mpr Real.pi_pos.le)
_ = _ := by rw [Real.rpow_neg, Real.rpow_ofNat, one_div]; positivity
end
end FiniteFactor
end OAI