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Add lean source and binary files (part 20)
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import OAI.Analysis.IrrationalRotation.Rotation.FieldDiagonal
import OAI.Analysis.IrrationalRotation.Spectral.WeightedShiftPolar
import OAI.Analysis.IrrationalRotation.Spectral.PolarFactor
namespace OAI
noncomputable section
open MeasureTheory Filter
open scoped ENNReal InnerProductSpace ComplexOrder
namespace Invariant233.WeightedShift
variable {X : Type*} [MeasurableSpace X] {μ : Measure X}
theorem fieldDiagonal_nonneg (a : X → Weight) (C : ℝ) (hC : 0 ≤ C)
(ha : ∀ x, ‖a x‖ ≤ C)
(hm : ∀ k, AEStronglyMeasurable (fun x => a x k) μ)
(hpos : ∀ᵐ x ∂μ, ∀ k, 0 ≤ a x k) :
0 ≤ fieldDiagonal a C hC ha hm := by
apply ContinuousLinearMap.nonneg_iff_isPositive.mpr
apply ContinuousLinearMap.isPositive_def.mpr
constructor
· intro f g
simp only [L2.inner_def]
apply integral_congr_ae
filter_upwards [fieldDiagonal_ae a C hC ha hm f,
fieldDiagonal_ae a C hC ha hm g, hpos] with x hf hg hx
change inner ℂ ((fieldDiagonal a C hC ha hm f) x) (g x) =
inner ℂ (f x) ((fieldDiagonal a C hC ha hm g) x)
rw [hf, hg]
exact ContinuousLinearMap.nonneg_iff_isPositive.mp
(PolarSupport.diagonal_nonneg (a x) hx) |>.isSymmetric (f x) (g x)
· intro f
change 0 ≤ (inner ℂ (fieldDiagonal a C hC ha hm f) f).re
rw [L2.inner_def]
change 0 ≤ RCLike.re (∫ x, inner ℂ ((fieldDiagonal a C hC ha hm f) x) (f x) ∂μ)
rw [← integral_re (L2.integrable_inner (𝕜 := ℂ) (fieldDiagonal a C hC ha hm f) f)]
apply integral_nonneg_of_ae
filter_upwards [fieldDiagonal_ae a C hC ha hm f, hpos] with x hf hx
rw [hf]
exact (ContinuousLinearMap.nonneg_iff_isPositive.mp
(PolarSupport.diagonal_nonneg (a x) hx)).re_inner_nonneg_left (f x)
theorem star_global_shift (n : ℤ) :
star ((shift n).toLinearIsometry.toContinuousLinearMap.compLpL 2 μ) =
(shift (-n)).toLinearIsometry.toContinuousLinearMap.compLpL 2 μ := by
symm
rw [ContinuousLinearMap.star_eq_adjoint]
apply (ContinuousLinearMap.eq_adjoint_iff _ _).2
intro f g
simp only [L2.inner_def]
apply integral_congr_ae
filter_upwards [fieldShift_ae (-n) f, fieldShift_ae n g] with x hf hg
rw [hf, hg]
have hinv : shift (-n) (f x) = (shift n).symm (f x) := by
apply (shift n).injective
ext k
simp [shift_apply]
rw [hinv]
have h := (shift n).inner_map_map ((shift n).symm (f x)) (g x)
simpa only [(shift n).apply_symm_apply] using h.symm
theorem global_shift_mem_unitary (n : ℤ) :
(shift n).toLinearIsometry.toContinuousLinearMap.compLpL 2 μ ∈
unitary (Lp Hilbert 2 μ →L[ℂ] Lp Hilbert 2 μ) := by
apply Unitary.mem_iff.mpr
rw [star_global_shift, ← fieldShift_add, ← fieldShift_add]
simpa using And.intro (fieldShift_zero (μ := μ)) (fieldShift_zero (μ := μ))
local instance fieldDiagonalPolarRealModule : Module ℝ
(Lp Hilbert 2 μ →L[ℂ] Lp Hilbert 2 μ) :=
Module.complexToReal (Lp Hilbert 2 μ →L[ℂ] Lp Hilbert 2 μ)
local instance fieldDiagonalPolarFunctionalCalculus : NonUnitalContinuousFunctionalCalculus ℝ
(Lp Hilbert 2 μ →L[ℂ] Lp Hilbert 2 μ) IsSelfAdjoint := by
infer_instance
theorem abs_global_shift_mul_fieldDiagonal (n : ℤ) (a : X → Weight)
(C : ℝ) (hC : 0 ≤ C) (ha : ∀ x, ‖a x‖ ≤ C)
(hm : ∀ k, AEStronglyMeasurable (fun x => a x k) μ)
(hpos : ∀ᵐ x ∂μ, ∀ k, 0 ≤ a x k) :
CFC.abs ((shift n).toLinearIsometry.toContinuousLinearMap.compLpL 2 μ *
fieldDiagonal a C hC ha hm) = fieldDiagonal a C hC ha hm :=
PolarFactor.abs_unitary_mul_of_nonneg
⟨_, global_shift_mem_unitary n⟩ _ (fieldDiagonal_nonneg a C hC ha hm hpos)
end Invariant233.WeightedShift
end
end OAI