OAI/Dynamics/ThreeTorus/RetainedPackets.lean
86 declarations, 0 contain sorry, 0 declared as axioms
Literal retained passage vectors, spectral identities, regularity, old marginals, and quantitative cutoff losses.
- lemma
OAI.ThreeTorus.integral_passageChartline 15 - lemma
OAI.ThreeTorus.physical_retainedPassage_error_leline 26Source documentation
A complete quantitative form of the physical transport estimate (2.9). The sole right-hand quantity is the actual summed Fourier-mass error.
lemma physical_retainedPassage_error_le {m : ℤ} {H : UnitAddCircle → UnitAddCircle} {A : UnitAddCircle × UnitAddCircle → ℂ} (hH : Continuous H) (hA : Continuous A) (S : Finset ℤ) (χ W : ℤ → UnitAddCircle → ℝ) (hχc : ∀ j, Continuous (χ j)) (ψ : UnitAddCircle → ℝ) (hψc : Continuous ψ) (hψ : ∀ a, 0 ≤ ψ a ∧ ψ a ≤ 1) (hχ : ∀ j a, 0 ≤ χ j a ∧ χ j a ≤ 1) (hW : ∀ j a, W j a ≠ 0 → j ∈ S ∧ χ j a = 1) (hE : ∀ j, Integrable (fun a => |‖exactPassageCoeff m H A j a‖^2-W j a|) AddCircle.haarAddCircle) (hp : ∀ᵐ a ∂AddCircle.haarAddCircle, Summable (fun j => |‖exactPassageCoeff m H A j a‖^2-W j a|)) (hs : Summable (fun j => ∫ a, |‖exactPassageCoeff m H A j a‖^2-W j a| ∂AddCircle.haarAddCircle)) : …Mentions: OAI.ThreeTorus.H, OAI.ThreeTorus.exactPassageCoeff
- lemma
OAI.ThreeTorus.pointwise_array_mass_error_summableline 78 - lemma
OAI.ThreeTorus.physical_retainedPassage_tendstoline 96Source documentation
The actual physical packet cutoff error tends to zero once the unrounded stationary mass theorem is applied. All summability hypotheses are derived.
lemma physical_retainedPassage_tendsto {m : ℤ} {H : ℕ → UnitAddCircle → UnitAddCircle} {A : UnitAddCircle × UnitAddCircle → ℂ} {W : ℝ → UnitAddCircle → ℝ} (hH : ∀ n, Continuous (H n)) (hA : Continuous A) (hWc : Continuous W.uncurry) (hWk : HasCompactSupport W.uncurry) (S : ℕ → Finset ℤ) (χ : ℕ → ℤ → UnitAddCircle → ℝ) (hχc : ∀ n j, Continuous (χ n j)) (hχ : ∀ n j a, 0 ≤ χ n j a ∧ χ n j a ≤ 1) (ψ : UnitAddCircle → ℝ) (hψc : Continuous ψ) (hψ : ∀ a, 0 ≤ ψ a ∧ ψ a ≤ 1) (hW : ∀ (n : ℕ), 0 < n → ∀ (j : ℤ) (a : UnitAddCircle), W ((j:ℝ)/n) a ≠ 0 → j ∈ S n ∧ χ n j a = 1) (ht : Tendsto (fun n : ℕ => ∑' j : ℤ, ∫ a : UnitAddCircle, |‖exactPassageCoeff m (H n) A j a‖^2-(n:ℝ)⁻¹*W ((j:ℝ)/n) a| ∂AddCircle.haarAddCircle) atTop (𝓝 0)) : …Mentions: OAI.ThreeTorus.H, OAI.ThreeTorus.exactPassageCoeff
- lemma
OAI.ThreeTorus.exact_physical_retainedPassage_tendstoline 134Source documentation
Physical transport for the actual signed packet. The summed stationary mass error is proved, not an input to this statement.
lemma exact_physical_retainedPassage_tendsto {A : UnitAddCircle × UnitAddCircle → ℂ} {A₀ : UnitAddCircle → ℝ → ℂ} {P V : ℝ → ℝ} {m : ℤ} {δ : ℕ → ℝ} {H : ℕ → UnitAddCircle → UnitAddCircle} {o l u R : ℝ} (hm : m ≠ 0) (hH : ∀ n (x : ℝ), H n (x : UnitAddCircle) = ((n:ℝ)*(P x+δ n*x) : UnitAddCircle)) (hA : ∀ a x, x ∈ Ioc o (o+1) → A ((x : UnitAddCircle),a) = A₀ a x) (hA₀ : ∀ a, ContDiff ℝ 2 (A₀ a)) (hAc : Continuous A₀.uncurry) (hAd : Continuous (fun p : UnitAddCircle × ℝ => deriv (A₀ p.1) p.2)) (hsupp : ∀ a, Function.support (A₀ a) ⊆ Ioc l u) (hlo : o ≤ l) (huo : u ≤ o+1) (hlu : l ≤ u) (hR : 0 < R) (hP : ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) P) …Mentions: OAI.ThreeTorus.H
- lemma
OAI.ThreeTorus.stationaryWeight_cylinder_supportline 185 - lemma
OAI.ThreeTorus.lifted_amplitude_compactSupportline 200 - lemma
OAI.ThreeTorus.retained_amplitude_disjointline 212Source documentation
The output amplitudes from different colors are exactly disjoint at each shared angular index; asymptotic orthogonality is not used here.
lemma retained_amplitude_disjoint {χ ξ : ℝ × UnitAddCircle → ℝ} (hd : Disjoint (tsupport χ) (tsupport ξ)) (s : ℝ) (F G : UnitAddCircle × UnitAddCircle → ℂ) : Disjoint (tsupport (fun p : UnitAddCircle × UnitAddCircle => (χ (s,p.1):ℂ)*F p)) (tsupport (fun p : UnitAddCircle × UnitAddCircle => (ξ (s,p.1):ℂ)*G p)) := by … - lemma
OAI.ThreeTorus.norm_spare_characterline 225 - lemma
OAI.ThreeTorus.colored_stationary_cutoffsline 231Source documentation
The source's finite stationary-image support selection, including the zero-frequency exclusion and exact disjointness of the cutoffs.
lemma colored_stationary_cutoffs {ι : Type*} [Finite ι] (m : ι → ℤ) (V : ℝ → ℝ) (I : Set ℝ) (K U : ι → Set (ℝ × UnitAddCircle)) (hm : ∀ i, m i ≠ 0) (hV : Continuous V) (hi : InjOn V I) (hK : ∀ i, IsCompact (K i)) (hKI : ∀ i, K i ⊆ I ×ˢ univ) (hzero : ∀ x ∈ I, V x ≠ 0) (hsep : ∀ i j, ∀ x ∈ I, ∀ y ∈ I, (m i:ℝ)*V x = (m j:ℝ)*V y → m i = m j) (hdisj : ∀ i j, i ≠ j → m i = m j → Disjoint (K i) (K j)) (hU : ∀ i, IsOpen (U i)) (hKU : ∀ i, stationaryImage (m i) V (K i) ⊆ U i) : ∃ χ : ι → ℝ × UnitAddCircle → ℝ, (∀ i, CylinderSmooth (χ i) ∧ HasCompactSupport (χ i) ∧ tsupport (χ i) ⊆ U i ∧ (∀ p, 0 ≤ χ i p ∧ χ i p ≤ 1) ∧ (∀ a, χ i (0,a) = 0) ∧ …Mentions: OAI.ThreeTorus.stationaryImage, OAI.ThreeTorus.CylinderSmooth
- lemma
OAI.ThreeTorus.simultaneous_retained_indicesline 270 - theorem
OAI.ThreeTorus.colored_physical_passageline 287Source documentation
Simultaneous physical transport with constructed, disjoint cylinder cutoffs. The limit is a consequence of the signed stationary-phase theorem for the actual Fourier coefficients, not an assumption on an auxiliary array.
theorem colored_physical_passage {ι : Type*} [Finite ι] {A : ι → UnitAddCircle × UnitAddCircle → ℂ} {A₀ : ι → UnitAddCircle → ℝ → ℂ} {P V : ℝ → ℝ} {m : ι → ℤ} {δ : ℕ → ℝ} {H : ℕ → UnitAddCircle → UnitAddCircle} {o l u R : ℝ} (hm : ∀ i, m i ≠ 0) (hH : ∀ n (x : ℝ), H n (x : UnitAddCircle) = ((n:ℝ)*(P x+δ n*x) : UnitAddCircle)) (hA : ∀ i a x, x ∈ Ioc o (o+1) → A i ((x : UnitAddCircle),a) = A₀ i a x) (hA₀ : ∀ i a, ContDiff ℝ 2 (A₀ i a)) (hAc : ∀ i, Continuous (A₀ i).uncurry) (hAd : ∀ i, Continuous (fun p : UnitAddCircle × ℝ => deriv (A₀ i p.1) p.2)) (hsupp : ∀ i a, Function.support (A₀ i a) ⊆ Ioc l u) (hlo : o ≤ l) (huo : u ≤ o+1) (hlu : l ≤ u) (hR : 0 < R) …Mentions: OAI.ThreeTorus.H
- theorem
OAI.ThreeTorus.finite_disjoint_frequency_cutoffsline 355Source documentation
The second support separation in the manuscript uses cutoffs in frequency alone, as opposed to the first passage's frequency/slow-coordinate cutoffs.
theorem finite_disjoint_frequency_cutoffs {ι : Type*} [Finite ι] (K U : ι → Set ℝ) (hK : ∀ i, IsCompact (K i)) (hU : ∀ i, IsOpen (U i)) (hKU : ∀ i, K i ⊆ U i) (hdisj : Pairwise (Disjoint on K)) : ∃ χ : ι → ℝ → ℝ, (∀ i, ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) (χ i) ∧ HasCompactSupport (χ i) ∧ tsupport (χ i) ⊆ U i ∧ (∀ s, 0 ≤ χ i s ∧ χ i s ≤ 1) ∧ ∀ s ∈ K i, χ i =ᶠ[𝓝 s] 1) ∧ Pairwise (fun i j => Disjoint (tsupport (χ i)) (tsupport (χ j))) := by … - lemma
OAI.ThreeTorus.compactSupport_frequency_cylinderline 376 - theorem
OAI.ThreeTorus.disjoint_frequency_indicesline 385Source documentation
Sampling disjoint frequency supports gives exactly disjoint finite index sets. There is no asymptotic assertion in this exact separation conclusion.
theorem disjoint_frequency_indices {ι : Type*} (χ : ι → ℝ → ℝ) (hc : ∀ i, HasCompactSupport (χ i)) (hz : ∀ i, χ i 0 = 0) (hd : Pairwise (fun i j => Disjoint (tsupport (χ i)) (tsupport (χ j)))) : ∃ S : ℕ → ι → Finset ℤ, (∀ n i, (0:ℤ) ∉ S n i) ∧ (∀ n, Pairwise (fun i j => Disjoint (S n i) (S n j))) ∧ ∀ n, 0 < n → ∀ i j, j ∈ S n i ↔ χ i ((j:ℝ)/n) ≠ 0 := by … - lemma
OAI.ThreeTorus.frequency_images_disjointline 420Source documentation
Compact slow-coordinate supports at equal old index stay disjoint under strictly monotone stationary maps. Distinct indices use the separated ranges.
lemma frequency_images_disjoint {ι : Type*} (m : ι → ℤ) (V : ℝ → ℝ) (I : Set ℝ) (K : ι → Set ℝ) (hm : ∀ i, m i ≠ 0) (hi : InjOn V I) (hKI : ∀ i, K i ⊆ I) (hsep : ∀ i j, ∀ x ∈ I, ∀ y ∈ I, (m i:ℝ)*V x = (m j:ℝ)*V y → m i = m j) (hdisj : ∀ i j, i ≠ j → m i = m j → Disjoint (K i) (K j)) : Pairwise (fun i j => Disjoint ((fun x => (m i:ℝ)*V x) '' K i) ((fun x => (m j:ℝ)*V x) '' K j)) := by … - theorem
OAI.ThreeTorus.second_separation_cutoffsline 440Source documentation
Full exact producer for the second passage's cutoff and index geometry.
theorem second_separation_cutoffs {ι : Type*} [Finite ι] (m : ι → ℤ) (V : ℝ → ℝ) (I : Set ℝ) (K U : ι → Set ℝ) (hm : ∀ i, m i ≠ 0) (hV : Continuous V) (hi : InjOn V I) (hK : ∀ i, IsCompact (K i)) (hKI : ∀ i, K i ⊆ I) (hzero : ∀ x ∈ I, V x ≠ 0) (hsep : ∀ i j, ∀ x ∈ I, ∀ y ∈ I, (m i:ℝ)*V x = (m j:ℝ)*V y → m i = m j) (hdisj : ∀ i j, i ≠ j → m i = m j → Disjoint (K i) (K j)) (hU : ∀ i, IsOpen (U i)) (hKU : ∀ i, (fun x => (m i:ℝ)*V x) '' K i ⊆ U i) : ∃ (χ : ι → ℝ → ℝ) (S : ℕ → ι → Finset ℤ), (∀ i, ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) (χ i) ∧ HasCompactSupport (χ i) ∧ tsupport (χ i) ⊆ U i ∧ (∀ s, 0 ≤ χ i s ∧ χ i s ≤ 1) ∧ ∀ s ∈ (fun x => (m i:ℝ)*V x) '' K i, χ i =ᶠ[𝓝 s] 1) ∧ … - lemma
OAI.ThreeTorus.CompactParameter.hasFDerivAt_compact_integralline 483Source documentation
Compact-parameter differentiation, used by the exact passage near epsilon=0.
lemma hasFDerivAt_compact_integral {E : Type} {G : Type*} [NormedAddCommGroup E] [NormedSpace ℝ E] [FiniteDimensional ℝ E] [NormedAddCommGroup G] [NormedSpace ℝ G] [CompleteSpace G] {F : E × ℝ → G} (hF : ContDiff ℝ 1 F) (a b : ℝ) (x : E) : HasFDerivAt (fun y => ∫ t in a..b, F (y,t)) (∫ t in a..b, (fderiv ℝ F (x,t)).comp (ContinuousLinearMap.inl ℝ E ℝ)) x := by … - lemma
OAI.ThreeTorus.CompactParameter.contDiff_compact_integralline 508Source documentation
Smooth parameter integration over a fixed compact interval.
lemma contDiff_compact_integral {E : Type} {G : Type*} [NormedAddCommGroup E] [NormedSpace ℝ E] [FiniteDimensional ℝ E] [NormedAddCommGroup G] [NormedSpace ℝ G] [CompleteSpace G] (n : ℕ) {F : E × ℝ → G} (hF : ContDiff ℝ n F) (a b : ℝ) : ContDiff ℝ n (fun y => ∫ t in a..b, F (y,t)) := by … - lemma
OAI.ThreeTorus.CompactParameter.smooth_compact_integralline 533 - lemma
OAI.ThreeTorus.smooth_fourierCoeff_paramline 546Source documentation
Smoothness of a Fourier coefficient in an arbitrary finite-dimensional parameter, obtained from a compact interval integral of the literal lift.
lemma smooth_fourierCoeff_param {E : Type} [NormedAddCommGroup E] [NormedSpace ℝ E] [FiniteDimensional ℝ E] {f : E → UnitAddCircle → ℂ} (hf : ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) (fun p : E × ℝ => f p.1 (p.2 : UnitAddCircle))) (j : ℤ) : ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) (fun x => fourierCoeff (f x) j) := by … - lemma
OAI.ThreeTorus.smooth_fourier_liftline 562 - lemma
OAI.ThreeTorus.smooth_exactPassageCoeffline 570Source documentation
Smoothness of the exact old-amplitude coefficients; no stationary-phase approximation replaces these coefficients.
lemma smooth_exactPassageCoeff {m : ℤ} {H : UnitAddCircle → UnitAddCircle} {Hl : ℝ → ℝ} {A : UnitAddCircle × UnitAddCircle → ℂ} (hHl : ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) Hl) (hH : ∀ t : ℝ, H (t : UnitAddCircle) = (Hl t : UnitAddCircle)) (hA : ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) (fun p : ℝ × ℝ => A (p.1,p.2))) (j : ℤ) : ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) (fun a : ℝ => exactPassageCoeff m H A j a) := by …Mentions: OAI.ThreeTorus.H, OAI.ThreeTorus.exactPassageCoeff
- lemma
OAI.ThreeTorus.smooth_retained_amplitudeline 585Source documentation
The new amplitudes retained by the passage lie in the same smooth packet class needed for its next use.
lemma smooth_retained_amplitude {m j : ℤ} {H : UnitAddCircle → UnitAddCircle} {Hl : ℝ → ℝ} {A : UnitAddCircle × UnitAddCircle → ℂ} {χ : ℝ × UnitAddCircle → ℝ} {ψ : UnitAddCircle → ℝ} (s : ℝ) (hHl : ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) Hl) (hH : ∀ t : ℝ, H (t : UnitAddCircle) = (Hl t : UnitAddCircle)) (hA : ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) (fun p : ℝ × ℝ => A (p.1,p.2))) (hχ : CylinderSmooth χ) (hψ : ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) (fun a : ℝ => ψ a)) : ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) (fun p : ℝ × ℝ => (χ (s,p.1):ℂ)*(ψ p.1:ℂ)*exactPassageCoeff m H A j p.1*fourier m (p.2:UnitAddCircle)) := by …Mentions: OAI.ThreeTorus.H, OAI.ThreeTorus.CylinderSmooth, OAI.ThreeTorus.exactPassageCoeff
- lemma
OAI.ThreeTorus.positive_density_map_of_vectorMeasureline 611Source documentation
A nonnegative integrable density identity proved with signed vector measures is the identical ordinary measure identity.
lemma positive_density_map_of_vectorMeasure {X Y : Type*} [MeasurableSpace X] [MeasurableSpace Y] {μ : Measure X} {ν : Measure Y} {f : X → Y} {q : X → ℝ} {p : Y → ℝ} (hf : Measurable f) (hq : Integrable q μ) (hp : Integrable p ν) (hq0 : ∀ x, 0 ≤ q x) (hp0 : ∀ y, 0 ≤ p y) (he : (μ.withDensityᵥ q).map f = ν.withDensityᵥ p) : (μ.withDensity (fun x => ENNReal.ofReal (q x))).map f = ν.withDensity (fun y => ENNReal.ofReal (p y)) := by …Mentions: OAI.ThreeTorus.μ
- lemma
OAI.ThreeTorus.branchDensity_nonnegline 628 - lemma
OAI.ThreeTorus.unfoldedModeDensity_nonnegline 636 - lemma
OAI.ThreeTorus.foldCircleDensity_nonnegline 643 - def
OAI.ThreeTorus.retainedAmplitudeline 649Source documentation
The literal new amplitude at a retained angular mode.
def retainedAmplitude (ψ : UnitAddCircle → ℝ) (χ : ℝ → UnitAddCircle → ℝ) (m : ℤ) (H : ℕ → UnitAddCircle → UnitAddCircle) (A : UnitAddCircle × UnitAddCircle → ℂ) (n : ℕ) (j : ℤ) (p : UnitAddCircle × UnitAddCircle) : ℂ := …Mentions: OAI.ThreeTorus.H
- lemma
OAI.ThreeTorus.retainedPassage_eq_sum_packetsline 655 - lemma
OAI.ThreeTorus.retainedAmplitude_norm_sqline 661 - lemma
OAI.ThreeTorus.retainedAmplitude_modulusline 670 - lemma
OAI.ThreeTorus.map_withDensity_compline 679Source comment
The same elementary identity used in the supplied whitening proof.lemma map_withDensity_comp {X Y : Type*} [MeasurableSpace X] [MeasurableSpace Y] (μ : Measure X) {ζ : X → Y} {w : Y → ℝ≥0∞} (hζ : Measurable ζ) (hw : Measurable w) : (μ.withDensity (w ∘ ζ)).map ζ = (μ.map ζ).withDensity w := by …Mentions: OAI.ThreeTorus.μ
- lemma
OAI.ThreeTorus.packetSpectralMeasure_of_modulusline 693Source documentation
If a coefficient's modulus is independent of its spare coordinate, its literal packet spectral measure is the single-coordinate weighted image.
lemma packetSpectralMeasure_of_modulus {φ : UnitAddCircle → UnitAddCircle} (hφ : Measurable φ) {j : ℤ} {B : UnitAddCircle × UnitAddCircle → ℂ} {q : UnitAddCircle → ℝ} (hq : Measurable q) (hB : ∀ p, ‖B p‖^2 = q p.1) : packetSpectralMeasure φ j B = (AddCircle.haarAddCircle.withDensity (fun a => ENNReal.ofReal (q a))).map (fun a => j • φ a) := by …Mentions: OAI.ThreeTorus.packetSpectralMeasure
- lemma
OAI.ThreeTorus.retainedCircleWeight_nonnegline 709 - lemma
OAI.ThreeTorus.circleDensityLift_nonnegline 713 - lemma
OAI.ThreeTorus.positive_foldedModeDensity_pushforwardline 723Source documentation
The folded branch is the ordinary (positive) spectral density, not just an identity of signed integrals.
lemma positive_foldedModeDensity_pushforward {q : UnitAddCircle → ℝ} {q₀ J₀ : ℝ → ℝ} {J : UnitAddCircle → ℝ} {o : ℝ} {I : Set ℝ} (hq : Integrable q AddCircle.haarAddCircle) (hqm : Measurable q₀) (hq0 : ∀ a, 0 ≤ q a) (hq00 : ∀ x, 0 ≤ q₀ x) (hq₀ : ∀ x ∈ Ioc o (o+1), q (x : UnitAddCircle) = q₀ x) (hq₀s : support q₀ ⊆ Ioc o (o+1)) (hqs : support q₀ ⊆ I) (hj : Measurable J) (hJ : ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) J₀) (hJe : ∀ x ∈ I, J (x : UnitAddCircle) = J₀ x) (hIo : IsOpen I) (hinj : InjOn J₀ I) (hd : ∀ x ∈ I, deriv J₀ x ≠ 0) {n j : ℝ} (hn : 0 < n) (hjn : j ≠ 0) : (AddCircle.haarAddCircle.withDensity (fun a => ENNReal.ofReal (q a))).map (fun a => (((j+(j/n)*J a)/n : ℝ) : UnitAddCircle)) = … - lemma
OAI.ThreeTorus.passage_speed_modeline 753 - lemma
OAI.ThreeTorus.packetSpectralMeasure_new_speedline 763Source documentation
Any coefficient with the actual retained modulus has the displayed nonnegative folded density under the actual new twist.
lemma packetSpectralMeasure_new_speed {q : UnitAddCircle → ℝ} {q₀ J₀ : ℝ → ℝ} {J : UnitAddCircle → ℝ} {o : ℝ} {I : Set ℝ} {B : UnitAddCircle × UnitAddCircle → ℂ} (hq : Integrable q AddCircle.haarAddCircle) (hqmeas : Measurable q) (hqm : Measurable q₀) (hB : ∀ p, ‖B p‖^2 = q p.1) (hq00 : ∀ x, 0 ≤ q₀ x) (hq₀ : ∀ x ∈ Ioc o (o+1), q (x : UnitAddCircle) = q₀ x) (hq₀s : support q₀ ⊆ Ioc o (o+1)) (hqs : support q₀ ⊆ I) (hj : Measurable J) (hJ : ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) J₀) (hJe : ∀ x ∈ I, J (x : UnitAddCircle) = J₀ x) (hIo : IsOpen I) (hinj : InjOn J₀ I) (hd : ∀ x ∈ I, deriv J₀ x ≠ 0) {n : ℝ} {j : ℤ} (hn : 0 < n) (hjn : j ≠ 0) : packetSpectralMeasure (fun a => (((1+J a/n)/n:ℝ):UnitAddCircle)) j B = …Mentions: OAI.ThreeTorus.packetSpectralMeasure
- lemma
OAI.ThreeTorus.retainedAmplitude_spectralDensityline 788Source documentation
Density identity for the literal retained coefficient used by the passage. The only support hypothesis is that the cutoff lies on the chosen good branch.
lemma retainedAmplitude_spectralDensity {ψ : UnitAddCircle → ℝ} {χ : ℝ → UnitAddCircle → ℝ} {m : ℤ} {H : ℕ → UnitAddCircle → UnitAddCircle} {A : UnitAddCircle × UnitAddCircle → ℂ} {J : UnitAddCircle → ℝ} {J₀ : ℝ → ℝ} {o : ℝ} {I : Set ℝ} (hψ : Continuous ψ) (hχ : Continuous χ.uncurry) (hH : ∀ n, Continuous (H n)) (hA : Continuous A) (hψs : ∀ x ∈ Ioc o (o+1), ψ (x:UnitAddCircle) ≠ 0 → x ∈ I) (hj : Measurable J) (hJ : ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) J₀) (hJe : ∀ x ∈ I, J (x:UnitAddCircle) = J₀ x) (hIo : IsOpen I) (hinj : InjOn J₀ I) (hd : ∀ x ∈ I, deriv J₀ x ≠ 0) {n : ℕ} {j : ℤ} (hn : 0 < n) (hjn : j ≠ 0) : packetSpectralMeasure (fun a => (((1+J a/n)/n:ℝ):UnitAddCircle)) j …Mentions: OAI.ThreeTorus.H, OAI.ThreeTorus.packetSpectralMeasure
- lemma
OAI.ThreeTorus.packet_twisted_pair_zeroline 828 - lemma
OAI.ThreeTorus.disjoint_packet_list_correlationline 856Source documentation
The spectral measure of a smooth disjoint packet list is the sum of the literal packet pushforwards, demonstrated by every bilateral Fourier moment.
lemma disjoint_packet_list_correlation {ι : Type*} [Fintype ι] (m : ι → ℤ) (A : ι → UnitAddCircle × UnitAddCircle → ℂ) (hA : ∀ i, Continuous (A i)) {φ : UnitAddCircle → UnitAddCircle} (hφ : Continuous φ) (hd : ∀ i j, i ≠ j → m i = m j → Disjoint (support (A i)) (support (A j))) (n : ℤ) : (∫ x : TripleTorus, starRingEnd ℂ (∑ i, packet (m i) (A i) x)* (∑ i, packet (m i) (A i) (twistIter φ n x)) ∂tripleVolume) = ∑ i, ∫ z, fourier n z ∂packetSpectralMeasure φ (m i) (A i) := by …Mentions: OAI.ThreeTorus.TripleTorus, OAI.ThreeTorus.packet, OAI.ThreeTorus.twistIter, OAI.ThreeTorus.tripleVolume, OAI.ThreeTorus.packetSpectralMeasure
- lemma
OAI.ThreeTorus.foldCircleDensity_add_aeline 904 - lemma
OAI.ThreeTorus.foldCircleDensity_finsetSum_aeline 919 - lemma
OAI.ThreeTorus.moment_withDensity_realline 939 - lemma
OAI.ThreeTorus.continuous_retainedAmplitudeline 949 - theorem
OAI.ThreeTorus.retainedPassage_spectral_momentline 963Source documentation
All bilateral Koopman moments of the actual finite retained vector are exactly those of its explicit nonnegative folded coefficient density.
theorem retainedPassage_spectral_moment {ψ : UnitAddCircle → ℝ} {χ : ℝ → UnitAddCircle → ℝ} {m : ℤ} {H : ℕ → UnitAddCircle → UnitAddCircle} {A : UnitAddCircle × UnitAddCircle → ℂ} {J : UnitAddCircle → ℝ} {J₀ : ℝ → ℝ} {I : Set ℝ} (hψ : Continuous ψ) (hχ : Continuous χ.uncurry) (hH : ∀ n, Continuous (H n)) (hA : Continuous A) (hψs : ∀ x ∈ Ioc (0:ℝ) 1, ψ (x:UnitAddCircle) ≠ 0 → x ∈ I) (hj : Continuous J) (hJ : ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) J₀) (hJe : ∀ x ∈ I, J (x:UnitAddCircle) = J₀ x) (hIo : IsOpen I) (hinj : InjOn J₀ I) (hd : ∀ x ∈ I, deriv J₀ x ≠ 0) {n : ℕ} {S : Finset ℤ} (hn : 0 < n) (hS : ∀ j ∈ S, j ≠ 0) (k : ℤ) : let φ := fun a => (((1+J a/n)/n:ℝ):UnitAddCircle) …Mentions: OAI.ThreeTorus.H
- lemma
OAI.ThreeTorus.support_branchDensity_subsetline 1049 - lemma
OAI.ThreeTorus.branchDensity_compactline 1060 - lemma
OAI.ThreeTorus.branchDensity_smoothline 1067 - lemma
OAI.ThreeTorus.unfoldedModeDensity_smoothline 1101 - lemma
OAI.ThreeTorus.unfoldedModeDensity_compactline 1115 - lemma
OAI.ThreeTorus.periodizedReal_eq_periodizeline 1134 - lemma
OAI.ThreeTorus.foldCircleDensity_smooth_liftline 1153 - def
OAI.ThreeTorus.realRetainedWeightline 1166Source documentation
The literal real lift of a retained coefficient weight. The smooth cutoff is taken before the final passage integer, as in the source.
def realRetainedWeight (ψ₀ : ℝ → ℝ) (χ : ℝ → UnitAddCircle → ℝ) (m : ℤ) (H : ℕ → UnitAddCircle → UnitAddCircle) (A : UnitAddCircle × UnitAddCircle → ℂ) (n : ℕ) (j : ℤ) (x : ℝ) : ℝ := …Mentions: OAI.ThreeTorus.H
- lemma
OAI.ThreeTorus.realRetainedWeight_supportline 1171 - lemma
OAI.ThreeTorus.realRetainedWeight_compactline 1179 - lemma
OAI.ThreeTorus.realRetainedWeight_smoothline 1185 - lemma
OAI.ThreeTorus.retainedWeight_lift_eqline 1200 - theorem
OAI.ThreeTorus.exactRetainedPacketDensity_smooth_liftline 1216Source documentation
Actual retained densities are smooth at all branch edges, including their zero set. This supplies the next passage's regularity; it is not an assumption that the density is already smooth.
theorem exactRetainedPacketDensity_smooth_lift {I : Set ℝ} {J : ℝ → ℝ} {ψ : UnitAddCircle → ℝ} {ψ₀ : ℝ → ℝ} {χ : ℝ → UnitAddCircle → ℝ} {m : ℤ} {H : ℕ → UnitAddCircle → UnitAddCircle} {Hl : ℕ → ℝ → ℝ} {A : UnitAddCircle × UnitAddCircle → ℂ} {S : Finset ℤ} {n : ℕ} (hJ : ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) J) (hIo : IsOpen I) (hinj : InjOn J I) (hd : ∀ x ∈ I, deriv J x ≠ 0) (hψ : ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) ψ₀) (hc : HasCompactSupport ψ₀) (he : ∀ x ∈ Ioc (0:ℝ) (0+1), ψ (x:UnitAddCircle) = ψ₀ x) (hs : tsupport ψ₀ ⊆ Ioc (0:ℝ) (0+1) ∩ I) (hχ : CylinderSmooth χ.uncurry) (hHl : ∀ n, ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) (Hl n)) …Mentions: OAI.ThreeTorus.H, OAI.ThreeTorus.CylinderSmooth
- lemma
OAI.ThreeTorus.continuous_of_continuous_liftline 1251 - lemma
OAI.ThreeTorus.positive_circle_branch_foldline 1269 - lemma
OAI.ThreeTorus.stationaryWeight_change_branchline 1301 - theorem
OAI.ThreeTorus.oldPacket_spectralDensity_of_modulusline 1311Source documentation
The density of a literal old angular packet, not an abstract probability model. The integer speed carrier vanishes on the temporal circle.
theorem oldPacket_spectralDensity_of_modulus {A : UnitAddCircle × UnitAddCircle → ℂ} {A₀ : ℝ → ℂ} {v : UnitAddCircle → ℝ} {V : ℝ → ℝ} {m c : ℤ} {o : ℝ} {C I : Set ℝ} (hA : Continuous A) (hA₀ : Continuous A₀) (hmod : ∀ u a, ‖A (u,a)‖ = ‖A (u,0)‖) (hAe : ∀ x ∈ Ioc o (o+1), A ((x:UnitAddCircle),0) = A₀ x) (has : support A₀ ⊆ Ioc o (o+1)) (hAs : support A₀ ⊆ I) (hv : Measurable v) (hV : ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) V) (hVe : ∀ x ∈ I, v (x:UnitAddCircle) = V x) (hIo : IsOpen I) (hIC : I ⊆ C) (hinj : InjOn (fun x => (m:ℝ)*V x) C) (hd : ∀ x ∈ I, deriv (fun x => (m:ℝ)*V x) x ≠ 0) : packetSpectralMeasure (fun a => ((v a-c:ℝ):UnitAddCircle)) m A = …Mentions: OAI.ThreeTorus.packetSpectralMeasure
- lemma
OAI.ThreeTorus.map_fst_withDensity_marginalline 1364 - lemma
OAI.ThreeTorus.continuous_slowMarginalline 1386 - lemma
OAI.ThreeTorus.packetSpectralMeasure_marginalline 1394 - lemma
OAI.ThreeTorus.branchDensity_integralline 1411 - theorem
OAI.ThreeTorus.oldPacket_spectralDensityline 1423Source documentation
An arbitrary smooth/continuous old packet has the stationary marginal as its temporal density. Spare-coordinate independence is not required.
theorem oldPacket_spectralDensity {A : UnitAddCircle × UnitAddCircle → ℂ} {A₀ : UnitAddCircle → ℝ → ℂ} {v : UnitAddCircle → ℝ} {V : ℝ → ℝ} {m c : ℤ} {o : ℝ} {C I : Set ℝ} (hA : Continuous A) (hA₀ : Continuous A₀.uncurry) (hAe : ∀ a x, x ∈ Ioc o (o+1) → A ((x:UnitAddCircle),a) = A₀ a x) (has : ∀ a, support (A₀ a) ⊆ Ioc o (o+1)) (hAs : ∀ a, support (A₀ a) ⊆ I) (hv : Measurable v) (hV : ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) V) (hVe : ∀ x ∈ I, v (x:UnitAddCircle) = V x) (hIo : IsOpen I) (hIC : I ⊆ C) (hinj : InjOn (fun x => (m:ℝ)*V x) C) (hd : ∀ x ∈ I, deriv (fun x => (m:ℝ)*V x) x ≠ 0) : packetSpectralMeasure (fun a => ((v a-c:ℝ):UnitAddCircle)) m A = AddCircle.haarAddCircle.withDensity (fun z => ENNReal.ofReal …Mentions: OAI.ThreeTorus.packetSpectralMeasure
- lemma
OAI.ThreeTorus.signed_circle_branch_foldline 1500 - theorem
OAI.ThreeTorus.oldStationaryMarginal_mapline 1530 - lemma
OAI.ThreeTorus.cutoff_slowMarginal_l1line 1595 - theorem
OAI.ThreeTorus.oldStationaryMarginal_cutoff_l1line 1642Source documentation
The reference in the neutral Riemann estimate is genuinely the cutoff old spectrum. Its loss is bounded independently of slope, residue modulus or passage integer.
theorem oldStationaryMarginal_cutoff_l1 {A : UnitAddCircle × UnitAddCircle → ℂ} {A₀ : UnitAddCircle → ℝ → ℂ} {v : UnitAddCircle → ℝ} {V : ℝ → ℝ} {m : ℤ} {o : ℝ} {C I : Set ℝ} (hA : Continuous A) (hA₀ : Continuous A₀.uncurry) (hAe : ∀ a x, x ∈ Ioc o (o+1) → A ((x:UnitAddCircle),a) = A₀ a x) (has : ∀ a, support (A₀ a) ⊆ Ioc o (o+1)) (hAs : ∀ a, support (A₀ a) ⊆ I) (hv : Measurable v) (hV : ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) V) (hVe : ∀ x ∈ I, v (x:UnitAddCircle) = V x) (hIo : IsOpen I) (hIC : I ⊆ C) (hinj : InjOn (fun x => (m:ℝ)*V x) C) (hd : ∀ x ∈ I, deriv (fun x => (m:ℝ)*V x) x ≠ 0) {ψ : UnitAddCircle → ℝ} (hψc : Continuous ψ) (hψ : ∀ a, 0 ≤ ψ a ∧ ψ a ≤ 1) {B : ℝ} (hB : 0 ≤ B) (hAb : ∀ p, ‖A p‖^2 ≤ B) : … - lemma
OAI.ThreeTorus.sq_norm_sub_le_twoline 1699 - lemma
OAI.ThreeTorus.continuous_passageChartline 1710 - lemma
OAI.ThreeTorus.continuous_retainedPassageline 1716 - lemma
OAI.ThreeTorus.cutoff_packet_error_eqline 1726 - lemma
OAI.ThreeTorus.cutoff_packet_error_leline 1748 - lemma
OAI.ThreeTorus.uncut_retainedPassage_error_leline 1770Source documentation
Removing the good-arc cutoff adds no assumed physical approximation. Its missing mass is explicitly paid.
lemma uncut_retainedPassage_error_le {A : UnitAddCircle × UnitAddCircle → ℂ} {m : ℤ} {H : ℕ → UnitAddCircle → UnitAddCircle} {χ : ℝ → UnitAddCircle → ℝ} (hA : Continuous A) (hH : ∀ n, Continuous (H n)) (hχ : Continuous χ.uncurry) (hmod : ∀ u a, ‖A (u,a)‖ = ‖A (u,0)‖) {δ : ℝ} (c : LawCutoffs δ) (hδ : 0 < δ) (hδ' : δ < 1/8) (n : ℕ) (S : Finset ℤ) : (∫ x : TripleTorus, ‖packet m A x-retainedPassage m (H n) A S (fun j => χ ((j:ℝ)/n)) (neutralCircleCutoff c) (passageChart (H n) x)‖^2 ∂tripleVolume) ≤ 8*δ*(∫ u, ‖A (u,0)‖^2 ∂AddCircle.haarAddCircle)+ 2*(∫ x : TripleTorus, ‖(neutralCircleCutoff c x.2.2:ℂ)*packet m A x- …Mentions: OAI.ThreeTorus.H, OAI.ThreeTorus.LawCutoffs, OAI.ThreeTorus.TripleTorus, OAI.ThreeTorus.packet, OAI.ThreeTorus.retainedPassage, OAI.ThreeTorus.neutralCircleCutoff, OAI.ThreeTorus.passageChart, OAI.ThreeTorus.tripleVolume
- theorem
OAI.ThreeTorus.exact_quantile_passageline 1815Source documentation
A single actual quantile passage simultaneously satisfies the physical, spectral, smoothness and all bilateral-moment conclusions. The passage integer remains arbitrarily large after the law, cutoffs and amplitudes are fixed.
theorem exact_quantile_passage {A : UnitAddCircle × UnitAddCircle → ℂ} {A₀ : UnitAddCircle → ℝ → ℂ} {Pr V : ℝ → ℝ} {m : ℤ} {Δ : ℕ → ℝ} {H : ℕ → UnitAddCircle → UnitAddCircle} {o l u R : ℝ} (hm : m ≠ 0) (hH : ∀ n (x : ℝ), H n (x : UnitAddCircle) = ((n:ℝ)*(Pr x+Δ n*x) : UnitAddCircle)) (hA : ∀ a x, x ∈ Ioc o (o+1) → A ((x : UnitAddCircle),a) = A₀ a x) (hA₀ : ∀ a, ContDiff ℝ 2 (A₀ a)) (hAc : Continuous A₀.uncurry) (hAd : Continuous (fun p : UnitAddCircle × ℝ => deriv (A₀ p.1) p.2)) (hAr : ContDiff ℝ ((⊤ : ℕ∞) : WithTop ℕ∞) (fun p : ℝ × ℝ => A₀ (p.2 : UnitAddCircle) p.1)) (hsupp : ∀ a, support (A₀ a) ⊆ Ioc l u) …Mentions: OAI.ThreeTorus.H
- lemma
OAI.ThreeTorus.continuous_stationaryWeight_parameterline 1926 - lemma
OAI.ThreeTorus.stationaryCutoffLift_marginalline 1937 - lemma
OAI.ThreeTorus.packet_cutoff_error_uniformline 1960 - lemma
OAI.ThreeTorus.packet_neutral_cutoff_errorline 1998 - lemma
OAI.ThreeTorus.uncut_retainedPassage_uniform_errorline 2007 - theorem
OAI.ThreeTorus.exact_neutral_passageline 2062