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import OAI.MathematicalPhysics.Boltzmann.Approximation.CapDilationCompactness
import OAI.MathematicalPhysics.Boltzmann.Approximation.CappedDensitySequence
import OAI.MathematicalPhysics.Boltzmann.Approximation.MildCharacteristics
import OAI.MathematicalPhysics.Boltzmann.Branching.HotWindowInput
import OAI.MathematicalPhysics.Boltzmann.Branching.MarginalUniformIntegrability
import OAI.MathematicalPhysics.Boltzmann.Compactness.WeakL1Operations
import OAI.MathematicalPhysics.Boltzmann.Compactness.WeakTimeSurvival
import OAI.MathematicalPhysics.Boltzmann.Jets.ColdMildRepresentative
import OAI.MathematicalPhysics.Boltzmann.Jets.GeometricColdSource
import OAI.MathematicalPhysics.Boltzmann.Jets.GeometricMesh
import OAI.MathematicalPhysics.Boltzmann.Jets.JetCoreConvergence
import OAI.MathematicalPhysics.Boltzmann.Jets.JetFamilyBounds
import OAI.MathematicalPhysics.Boltzmann.Jets.JetContinuation
namespace OAI
section
/-! # Actual weak hot limits on bounded spacetime windows -/
noncomputable section
open MeasureTheory Filter Set
open scoped Topology
open BoltzmannNonuniqueness.VelocityWeight
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
theorem exists_hot_weak_limit (hDP : Published.DunfordPettis1940HotWindows)
(S : AttainedCapSequence F)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) (κ : ℕ → ℕ)
{A R : ℝ} (hA : 0 ≤ A) (hR : 0 ≤ R) :
∃ (φ : ℕ → ℕ) (g : HotKineticPhase → ℝ), StrictMono φ ∧
Published.WeakL1Converges (hotWindowVolume A R)
(fun n => S.hotDensity (κ (φ n))) g ∧
(∀ᵐ z ∂hotWindowVolume A R, 0 ≤ g z) ∧
(∀ᵐ z ∂hotWindowVolume A R, g z ≤ (A+1)*H q z.2) := by
have hui := S.hotDensity_uniformIntegrable hs₀ hsmax hη hηmax hK hd₀ hq A R
obtain ⟨φ,g,hφ,hg⟩ := hDP A R hA hR (fun n => S.hotDensity (κ n))
(fun n => S.hotDensity_measurable hs₀ hsmax hη hηmax hK hd₀ hq (κ n))
(Compactness.uniformIntegrable_comp hui κ)
((S.hotDensity_unifTight hs₀ hsmax hη hηmax hK hd₀ hq hA R).comp κ)
refine ⟨φ,g,hφ,hg,?_,?_⟩
· exact hg.nonneg (fun n => ae_of_all _
(S.hotDensity_nonneg hs₀ hsmax hη hηmax hK hd₀ hq (κ (φ n))))
· exact hg.le (fun n => memLp_one_iff_integrable.mp (hui.memLp (κ (φ n))))
(((ChartKernel.measurable_H q).comp measurable_snd).const_mul _)
(hot_majorant_integrable hq A R)
(fun n => S.hotDensity_bound hs₀ hsmax hη hηmax hK hd₀ hq (κ (φ n)) A R)
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # The exact affine cap passes to the weak hot limit -/
noncomputable section
open MeasureTheory Filter Set
open scoped Topology
open BoltzmannNonuniqueness.VelocityWeight
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
theorem hotWindow_time_mem (A R : ℝ) :
∀ᵐ z ∂hotWindowVolume A R, z.1.1 ∈ Icc (0:ℝ) A := by
exact Measure.quasiMeasurePreserving_fst.ae
(Measure.quasiMeasurePreserving_fst.ae (ae_restrict_mem measurableSet_Icc))
theorem hotDensity_cap_bound (S : AttainedCapSequence F)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) (n : ℕ) (A R : ℝ) :
∀ᵐ z ∂hotWindowVolume A R, S.hotDensity n z ≤ (z.1.1+S.coldFraction n)*H q z.2 := by
let μt : Measure ℝ := volume.restrict (Icc (0:ℝ) A)
let μx : Measure JetPrototype.Space := volume.restrict (Metric.closedBall 0 R)
have hB : ∀ᵐ u ∂μt.prod (μx.prod volume),
S.extendedHot n u ≤ (u.1+S.coldFraction n)*H q u.2.2 := by
apply (Measure.ae_prod_iff_ae_ae (measurableSet_le
(S.extendedHot_measurable hs₀ hsmax hη hηmax hK hd₀ hq n)
((measurable_fst.add_const _).mul
((ChartKernel.measurable_H q).comp measurable_snd.snd)))).mpr
filter_upwards [ae_restrict_mem measurableSet_Icc] with t ht
have hb := S.extendedHot_bound_at hs₀ hsmax hη hηmax hK hd₀ hq n ht.1
have hab : μx.prod (volume : Measure Velocity) ≤ FlightMeasure.phaseVolume :=
Measure.prod_mono Measure.restrict_le_self le_rfl
exact hb.filter_mono (ae_mono hab)
exact (measurePreserving_prodAssoc μt μx (volume : Measure Velocity)).quasiMeasurePreserving.ae hB
theorem hot_velocity_integrable {q : ℝ} (hq : q < 2) (A R : ℝ) :
Integrable (fun z : HotKineticPhase => H q z.2) (hotWindowVolume A R) := by
unfold hotWindowVolume
have : IsFiniteMeasure ((volume : Measure JetPrototype.Space).restrict
(Metric.closedBall 0 R)) :=
isFiniteMeasure_restrict.mpr (isCompact_closedBall (0 : JetPrototype.Space) R).measure_lt_top.ne
exact (integrable_H hq).comp_snd _
theorem hot_time_majorant_integrable {q : ℝ} (hq : q < 2) (A R : ℝ) :
Integrable (fun z : HotKineticPhase => z.1.1*H q z.2) (hotWindowVolume A R) := by
apply (hot_majorant_integrable hq A R).mono'
(measurable_fst.fst.mul ((ChartKernel.measurable_H q).comp measurable_snd)).aestronglyMeasurable
filter_upwards [hotWindow_time_mem A R] with z hz
change ‖z.1.1*H q z.2‖ ≤ (A+1)*H q z.2
rw [Real.norm_of_nonneg (mul_nonneg hz.1 (H_nonneg q _))]
exact mul_le_mul_of_nonneg_right (hz.2.trans (by linarith)) (H_nonneg q _)
theorem hot_weak_limit_cap (S : AttainedCapSequence F)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) {κ : ℕ → ℕ} {l A R : ℝ}
(hl : Tendsto (fun n => S.coldFraction (κ n)) atTop (𝓝 l))
{g : HotKineticPhase → ℝ}
(hg : Published.WeakL1Converges (hotWindowVolume A R) (fun n => S.hotDensity (κ n)) g) :
∀ᵐ z ∂hotWindowVolume A R, g z ≤ (z.1.1+l)*H q z.2 := by
have hui := S.hotDensity_uniformIntegrable hs₀ hsmax hη hηmax hK hd₀ hq A R
have hb (n) : ∀ᵐ z ∂hotWindowVolume A R,
S.hotDensity (κ n) z ≤ z.1.1*H q z.2+S.coldFraction (κ n)*H q z.2 := by
simpa only [add_mul] using S.hotDensity_cap_bound hs₀ hsmax hη hηmax hK hd₀ hq (κ n) A R
simpa only [Pi.mul_apply,Function.comp_apply,add_mul] using hg.le_affine
(fun n => memLp_one_iff_integrable.mp (hui.memLp (κ n)))
(measurable_fst.fst.mul ((ChartKernel.measurable_H q).comp measurable_snd))
((ChartKernel.measurable_H q).comp measurable_snd)
(hot_time_majorant_integrable hq A R) (hot_velocity_integrable hq A R) hl hb
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # One subsequence for the hot density, mesh phase and limiting horizon -/
noncomputable section
open MeasureTheory Filter Set
open scoped Topology ENNReal
open BoltzmannNonuniqueness.VelocityWeight
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
structure HotLimitExtraction (S : AttainedCapSequence F) where
fraction : ℝ
fraction_mem : fraction ∈ Icc 0 1
phase : ℝ
phase_mem : phase ∈ Icc 1 (Real.exp η)
horizon : ℝ≥0∞
horizon_ge : 1 ≤ horizon
indices : ℕ → ℕ
indices_strict : StrictMono indices
fraction_limit : Tendsto (fun n => S.coldFraction (indices n)) atTop (𝓝 fraction)
phase_limit : Tendsto (fun n => GeometricMesh.phase (s₀/S.radius (indices n)) η)
atTop (𝓝 phase)
horizon_limit : Tendsto (fun n => S.normalizedHorizon (indices n)) atTop (𝓝 horizon)
profile : ℕ → HotKineticPhase → ℝ
weak : ∀ j : ℕ, Published.WeakL1Converges (hotWindowVolume (j+1) (j+1))
(fun n => S.hotDensity (indices n)) (profile j)
nonneg : ∀ j : ℕ, ∀ᵐ z ∂hotWindowVolume (j+1) (j+1), 0 ≤ profile j z
cap : ∀ j : ℕ, ∀ᵐ z ∂hotWindowVolume (j+1) (j+1),
profile j z ≤ (z.1.1+fraction)*H q z.2
theorem exists_hot_limit_extraction (hDP : Published.DunfordPettis1940HotWindows)
(S : AttainedCapSequence F)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) : Nonempty (HotLimitExtraction S) := by
obtain ⟨l,hl,θ,hθ,U,hU,a,ha,hla,hθa,hUa⟩ := S.joint_subsequence hs₀ hη
let μ : ℕ → Measure HotKineticPhase := fun j => hotWindowVolume (j+1) (j+1)
have hui (j) : UniformIntegrable (fun n => S.hotDensity (a n)) 1 (μ j) :=
Compactness.uniformIntegrable_comp
(S.hotDensity_uniformIntegrable hs₀ hsmax hη hηmax hK hd₀ hq _ _) a
have htight (j) : UnifTight (fun n => S.hotDensity (a n)) 1 (μ j) :=
(S.hotDensity_unifTight hs₀ hsmax hη hηmax hK hd₀ hq (by positivity) _).comp a
obtain ⟨b,g,hb,hg⟩ := Published.L1WeakCompactnessInput.countable μ
(fun j => hDP (j+1) (j+1) (by positivity) (by positivity))
(fun n => S.hotDensity_measurable hs₀ hsmax hη hηmax hK hd₀ hq (a n)) hui htight
refine ⟨{
fraction := l
fraction_mem := hl
phase := θ
phase_mem := hθ
horizon := U
horizon_ge := hU
indices := a ∘ b
indices_strict := ha.comp hb
fraction_limit := hla.comp hb.tendsto_atTop
phase_limit := hθa.comp hb.tendsto_atTop
horizon_limit := hUa.comp hb.tendsto_atTop
profile := g
weak := hg
nonneg := ?_
cap := ?_ }⟩
· intro j
exact (hg j).nonneg (fun n => ae_of_all _
(S.hotDensity_nonneg hs₀ hsmax hη hηmax hK hd₀ hq (a (b n))))
· intro j
exact S.hot_weak_limit_cap hs₀ hsmax hη hηmax hK hd₀ hq
(hla.comp hb.tendsto_atTop) (hg j)
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Actual cold labels approaching each point of the limiting geometric mesh -/
noncomputable section
open Filter Set
open scoped Topology
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
{S : AttainedCapSequence F}
def HotLimitExtraction.coldLabel (E : HotLimitExtraction S) (k : ℤ) (a : Bool) (n : ℕ) :
JetLattice.Label :=
⟨GeometricMesh.jetIndex s₀ η (fun j => S.radius (E.indices j)) k n,a,0⟩
theorem HotLimitExtraction.coldLabel_scale_limit (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hη : 0 < η) (k : ℤ) (a : Bool) :
Tendsto (fun n => JetGeometry.jetScale s₀ η (E.coldLabel k a n).annulus/S.radius (E.indices n))
atTop (𝓝 (E.phase*Real.exp (η*(k:ℝ)))) :=
GeometricMesh.jet_scale_approximation hs₀ hη (fun n => S.radius_pos hs₀ (E.indices n))
((S.radius_tendsto_zero hs₀).comp E.indices_strict.tendsto_atTop) E.phase_limit k
theorem HotLimitExtraction.coldLabel_retained (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hη : 0 < η) (k : ℤ) (a : Bool)
(hk : E.fraction < E.phase*Real.exp (η*(k:ℝ))) :
∀ᶠ n in atTop, (E.coldLabel k a n).annulus < F.indices (E.indices n) :=
GeometricMesh.jetIndex_eventually_retained hs₀ hη (fun n => S.radius_pos hs₀ (E.indices n))
((S.radius_tendsto_zero hs₀).comp E.indices_strict.tendsto_atTop)
E.phase_limit E.fraction_limit k hk
theorem HotLimitExtraction.coldLabel_scale_tendsto_zero (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hη : 0 < η) (k : ℤ) (a : Bool) :
Tendsto (fun n => JetGeometry.jetScale s₀ η (E.coldLabel k a n).annulus) atTop (𝓝 0) := by
have h := ((S.radius_tendsto_zero hs₀).comp E.indices_strict.tendsto_atTop).mul
(E.coldLabel_scale_limit hs₀ hη k a)
simpa only [Function.comp_def,zero_mul,mul_div_cancel₀ _ (S.radius_pos hs₀ _).ne'] using h
theorem HotLimitExtraction.coldLabel_width_tendsto_zero (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hη : 0 < η) (k : ℤ) (a : Bool) :
Tendsto (fun n => d₀*(JetGeometry.jetScale s₀ η (E.coldLabel k a n).annulus)^10)
atTop (𝓝 0) := by
simpa only [zero_pow (by decide : (10:ℕ) ≠ 0),mul_zero] using
((E.coldLabel_scale_tendsto_zero hs₀ hη k a).pow 10).const_mul d₀
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # The quantitative free-flight error of the constructed cap approximations -/
noncomputable section
open MeasureTheory Set
open BoltzmannNonuniqueness.JetLattice BoltzmannNonuniqueness.JetGeometry
open BoltzmannNonuniqueness.VelocityWeight BoltzmannNonuniqueness.WeightedLocal
open BoltzmannNonuniqueness.WeightedLocalControl BoltzmannNonuniqueness.WeightedTranslation
namespace BoltzmannNonuniqueness.JetCopyDatum
def CapApproximation.cold {s₀ η K α γ d₀ q T : ℝ} {N : ℕ}
(F : CapApproximation s₀ η K α γ d₀ q T N) (i : Label) : ℝ × JetPrototype.Phase → ℝ :=
rebuilt s₀ η K α γ d₀ q (N+1) (damping q (N+1) F.amplitude) T N F.solution.value i
theorem CapApproximation.local_free_error {s₀ η K α γ d₀ q T : ℝ} {N : ℕ}
(F : CapApproximation s₀ η K α γ d₀ q T N)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 ≤ α) (hαmax : α ≤ 1/4) (hγ : 0 ≤ γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1) (hT : 0 ≤ T) (hTmax : T ≤ 1/32)
(hq : q < 2) (hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(m : ℕ) (i : Label) (hi0 : i.lattice = 0) (hi : i.annulus < N)
(hwidth : T*(d₀*jetScale s₀ η i.annulus^10) ≤ enlargementWidth η (jetScale s₀ η i.annulus))
(hdmax : d₀*jetScale s₀ η i.annulus^10 ≤ 1/64)
(Ω : Set JetPrototype.Space) [IsFiniteMeasure (JetPrototype.spaceVolume.restrict Ω)]
{t : ℝ} (ht : t ∈ Ioc 0 T) :
let s := jetScale s₀ η i.annulus
let E := coldOpticalDepth (4*JetBarrierCollision.frequencyConstant*K*d₀*s^9)
(weightFrequencyConstant q 2) (DatumBounds.scale s₀ η (N+1))
(escapedFrequencyConstant s₀ η α K d₀ q m) m t
let ε := JetSupersolution.epsilon K s (d₀*s^10)
let μ := (JetPrototype.spaceVolume.restrict Ω).prod (volume : Measure Velocity)
let error := fun p : JetPrototype.Phase => |H q p.2*F.cold i (t,p)-
JetFreeTransport.free η K α γ s (d₀*s^10) t i.positive (shift (displacement i.lattice) p)|
Integrable error μ ∧ (∫ p, error p ∂μ) ≤
(E+ε)*(JetPrototype.spaceVolume.restrict Ω).real univ*(JetBarrierLocalMass.massConstant*(K/s)) := by
have hδ := DatumBounds.scale_pos (η := η) hs₀ (N+1)
have hδone : DatumBounds.scale s₀ η (N+1) ≤ 1 := by
have h := JetGeometry.scale_antitone hs₀.le hη.le (Nat.zero_le (N+1))
rw [show DatumBounds.scale s₀ η 0 = s₀ by simp [DatumBounds.scale]] at h
linarith
have hh₀ (p) : 0 ≤ F.coefficient*HotSeedProfile.normalized q (DatumBounds.scale s₀ η (N+1)) p :=
mul_nonneg F.coefficient_mem.1 ((HotSeedProfile.normalized_bounds hδ hδone q).choose_spec.2 p).1
exact rebuilt_local_free_error hs₀ hsmax hη hηmax hK hα hαmax hγ hd₀ hd₀max hTmax
hq (by positivity) (bounds (by positivity) F.amplitude_pos).1 hT (by linarith [F.amplitude_pos])
hδ hsmall le_rfl m N i hi0 hwidth hdmax
((HotSeedProfile.normalized_measurable q _).const_mul F.coefficient) hh₀ F.initial_bound
F.solution F.cap.le hi Ω ht
end BoltzmannNonuniqueness.JetCopyDatum
end
end
section
/-! # The positive terminal cap scale is an excluded cold label -/
noncomputable section
open Filter
open scoped Topology
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
{S : AttainedCapSequence F}
theorem HotLimitExtraction.coldLabel_at_endpoint (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hη : 0 < η) (hfrac : 0 < E.fraction) (k : ℤ) (a : Bool)
(hk : E.phase*Real.exp (η*(k:ℝ)) = E.fraction) :
∀ᶠ n in atTop, (E.coldLabel k a n).annulus = F.indices (E.indices n) := by
have hm := E.coldLabel_scale_limit hs₀ hη k a
rw [hk] at hm
have he := GeometricMesh.indices_eventually_eq_of_same_positive_limit hs₀.le hη hfrac
(fun n => S.radius_pos hs₀ (E.indices n)) hm E.fraction_limit
filter_upwards [he] with n hn
exact Nat.add_right_cancel hn
theorem HotLimitExtraction.coldLabel_below_endpoint (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hη : 0 < η) (k : ℤ) (a : Bool)
(hk : E.phase*Real.exp (η*(k:ℝ)) < E.fraction) :
∀ᶠ n in atTop, F.indices (E.indices n) < (E.coldLabel k a n).annulus := by
have he := (E.coldLabel_scale_limit hs₀ hη k a).eventually_lt E.fraction_limit hk
filter_upwards [he] with n hn
by_contra h
have hb := JetGeometry.scale_antitone hs₀.le hη.le
(Nat.add_le_add_right (le_of_not_gt h) 1)
exact (not_lt_of_ge hb)
((div_lt_div_iff_of_pos_right (S.radius_pos hs₀ (E.indices n))).mp hn)
theorem HotLimitExtraction.coldLabel_retained_iff (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hη : 0 < η) (k : ℤ) (a : Bool) :
∀ᶠ n in atTop, ((E.coldLabel k a n).annulus < F.indices (E.indices n) ↔
E.fraction < E.phase*Real.exp (η*(k:ℝ))) := by
rcases lt_trichotomy E.fraction (E.phase*Real.exp (η*(k:ℝ))) with h | h | h
· filter_upwards [E.coldLabel_retained hs₀ hη k a h] with n hn
exact iff_of_true hn h
· have hp : 0 < E.fraction := by
rw [h]
exact mul_pos (lt_of_lt_of_le zero_lt_one E.phase_mem.1) (Real.exp_pos _)
filter_upwards [E.coldLabel_at_endpoint hs₀ hη hp k a h.symm] with n hn
rw [hn,h]
simp only [lt_self_iff_false]
· filter_upwards [E.coldLabel_below_endpoint hs₀ hη k a h] with n hn
exact iff_of_false (not_lt_of_ge hn.le) (not_lt_of_ge h.le)
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Actual cold cap colors converge to their free flight on dilation windows -/
noncomputable section
open MeasureTheory Set Filter
open scoped Topology Pointwise
open BoltzmannNonuniqueness.JetLattice BoltzmannNonuniqueness.JetGeometry
open BoltzmannNonuniqueness.VelocityWeight BoltzmannNonuniqueness.WeightedTranslation
namespace BoltzmannNonuniqueness.JetCopyDatum
theorem cap_cold_dilation_free_error {s₀ η K α γ d₀ q T a S U : ℝ}
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 ≤ α) (hαmax : α ≤ 1/4) (hγ : 0 ≤ γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1) (hT : 0 ≤ T) (hTmax : T ≤ 1/32)
(hq : q < 2) (hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(N : ℕ → ℕ) (F : ∀ n, CapApproximation s₀ η K α γ d₀ q T (N n))
(j : ℕ → Label) (hj0 : ∀ n, (j n).lattice = 0) (hj : ∀ n, (j n).annulus < N n)
(r t : ℕ → ℝ) (hr : ∀ n, 0 < r n) (hrlim : Tendsto r atTop (𝓝 0))
(ht : ∀ n, t n ∈ Ioc 0 T) (ha : 0 < a) (hS : 0 ≤ S)
(hlo : ∀ n, a*r n ≤ jetScale s₀ η (j n).annulus)
(hhi : ∀ n, jetScale s₀ η (j n).annulus ≤ S*r n)
(htime : ∀ n, t n ≤ U*r n)
(hδ : ∀ n, DatumBounds.scale s₀ η (N n+1) ≤ r n)
(hwidth : ∀ n, T*(d₀*jetScale s₀ η (j n).annulus^10) ≤
enlargementWidth η (jetScale s₀ η (j n).annulus))
(hdmax : ∀ n, d₀*jetScale s₀ η (j n).annulus^10 ≤ 1/64)
(Ω : Set JetPrototype.Space) (hΩ : IsCompact Ω) :
Tendsto (fun n => ∫ x in Ω, ∫ v : Velocity,
|r n*(H q v*(F n).cold (j n) (t n,(r n • x,v))-
JetFreeTransport.free η K α γ (jetScale s₀ η (j n).annulus)
(d₀*jetScale s₀ η (j n).annulus^10) (t n) (j n).positive
(shift (displacement (j n).lattice) (r n • x,v)))|
∂volume ∂JetPrototype.spaceVolume) atTop (𝓝 0) := by
let s := fun n => jetScale s₀ η (j n).annulus
let δ := fun n => DatumBounds.scale s₀ η (N n+1)
let C := 4*JetBarrierCollision.frequencyConstant*K*d₀
let A := weightFrequencyConstant q 2
let D := escapedFrequencyConstant s₀ η α K d₀ q 0
let E := fun n => coldOpticalDepth (C*s n^9) A (δ n) D 0 (t n)
let ε := fun n => JetSupersolution.epsilon K (s n) (d₀*(s n)^10)
let err := fun n (p : JetPrototype.Phase) =>
H q p.2*(F n).cold (j n) (t n,p)-
JetFreeTransport.free η K α γ (s n) (d₀*(s n)^10) (t n) (j n).positive
(shift (displacement (j n).lattice) p)
let I := fun n => ∫ p : JetPrototype.Phase, |err n p|
∂(JetPrototype.spaceVolume.restrict (r n • Ω)).prod volume
have hs (n) : 0 < s n := DatumBounds.scale_pos (η := η) hs₀ _
have hC : 0 ≤ C := by
dsimp [C]
exact mul_nonneg
(mul_nonneg (mul_nonneg (by norm_num) JetBarrierCollision.frequencyConstant_nonneg) hK) hd₀.le
have hA : 0 ≤ A := weightFrequencyConstant_nonneg q (by norm_num)
have hD : 0 ≤ D := escapedFrequencyConstant_nonneg hs₀ hK hd₀ η α q 0
have hEn (n) : 0 ≤ E n := coldOpticalDepth_nonneg
(mul_nonneg hC (pow_nonneg (hs n).le _)) hA (DatumBounds.scale_pos hs₀ _).le hD (ht n).1.le 0
have hεn (n) : 0 ≤ ε n := JetSupersolution.epsilon_nonneg hK (hs n)
(mul_pos hd₀ (pow_pos (hs n) _))
have hcomp (n) : IsCompact (r n • Ω) := hΩ.image (continuous_const_smul (r n))
have hfin (n) : IsFiniteMeasure (JetPrototype.spaceVolume.restrict (r n • Ω)) :=
isFiniteMeasure_restrict.mpr (hcomp n).measure_lt_top.ne
have hbound (n) : Integrable (fun p => |err n p|)
((JetPrototype.spaceVolume.restrict (r n • Ω)).prod volume) ∧
I n ≤ (E n+ε n)*((r n)^3*JetPrototype.spaceVolume.real Ω)*
(JetBarrierLocalMass.massConstant*(K/s n)) := by
let _ := hfin n
have hb := (F n).local_free_error hs₀ hsmax hη hηmax hK hα hαmax hγ hd₀ hd₀max
hT hTmax hq hsmall 0 (j n) (hj0 n) (hj n) (hwidth n) (hdmax n) (r n • Ω) (ht n)
dsimp only at hb
refine ⟨hb.1,?_⟩
simpa only [I,err,E,ε,C,A,D,s,δ,measureReal_restrict_apply_univ,
ColdDilationMeasure.spaceVolume_real_smul Ω (hr n)] using hb.2
have hElim : Tendsto E atTop (𝓝 0) :=
coldOpticalDepth_tendsto_zero hC hA hD hS (fun n => (hr n).le)
(fun n => (hs n).le) (fun n => (ht n).1.le) (fun n => (DatumBounds.scale_pos hs₀ _).le)
hhi htime hδ hrlim
have hεlim : Tendsto ε atTop (𝓝 0) := jet_epsilon_tendsto_zero hs hhi hrlim K d₀
have hlim : Tendsto (fun n => I n/(r n)^2) atTop (𝓝 0) :=
scaled_local_error_tendsto_zero hEn hεn measureReal_nonneg JetBarrierLocalMass.massConstant_nonneg
hK hr hs ha hlo (fun n => integral_nonneg (fun _ => abs_nonneg _))
(fun n => (hbound n).2) hElim hεlim
convert hlim using 1
funext n
rw [ColdDilationMeasure.dilated_error_integral (err n) Ω (hr n)]
rw [← integral_prod _ (hbound n).1]
end BoltzmannNonuniqueness.JetCopyDatum
end
end
section
/-! # Cold dilation estimates for cap shots with varying horizons -/
noncomputable section
open MeasureTheory Set Filter
open scoped Topology Pointwise
open BoltzmannNonuniqueness.JetLattice BoltzmannNonuniqueness.JetGeometry
open BoltzmannNonuniqueness.VelocityWeight BoltzmannNonuniqueness.WeightedTranslation
namespace BoltzmannNonuniqueness.JetCopyDatum
theorem cap_variable_cold_dilation_free_error {s₀ η K α γ d₀ q a S U : ℝ} {T : ℕ → ℝ}
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 ≤ α) (hαmax : α ≤ 1/4) (hγ : 0 ≤ γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1) (hT : ∀ n, 0 ≤ T n) (hTmax : ∀ n, T n ≤ 1/32)
(hq : q < 2) (hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(N : ℕ → ℕ) (F : ∀ n, CapApproximation s₀ η K α γ d₀ q (T n) (N n))
(j : ℕ → Label) (hj0 : ∀ n, (j n).lattice = 0) (hj : ∀ n, (j n).annulus < N n)
(r t : ℕ → ℝ) (hr : ∀ n, 0 < r n) (hrlim : Tendsto r atTop (𝓝 0))
(ht : ∀ n, t n ∈ Ioc 0 (T n)) (ha : 0 < a) (hS : 0 ≤ S)
(hlo : ∀ n, a*r n ≤ jetScale s₀ η (j n).annulus)
(hhi : ∀ n, jetScale s₀ η (j n).annulus ≤ S*r n)
(htime : ∀ n, t n ≤ U*r n)
(hδ : ∀ n, DatumBounds.scale s₀ η (N n+1) ≤ r n)
(hwidth : ∀ n, T n*(d₀*jetScale s₀ η (j n).annulus^10) ≤
enlargementWidth η (jetScale s₀ η (j n).annulus))
(hdmax : ∀ n, d₀*jetScale s₀ η (j n).annulus^10 ≤ 1/64)
(Ω : Set JetPrototype.Space) (hΩ : IsCompact Ω) :
Tendsto (fun n => ∫ x in Ω, ∫ v : Velocity,
|r n*(H q v*(F n).cold (j n) (t n,(r n • x,v))-
JetFreeTransport.free η K α γ (jetScale s₀ η (j n).annulus)
(d₀*jetScale s₀ η (j n).annulus^10) (t n) (j n).positive
(shift (displacement (j n).lattice) (r n • x,v)))|
∂volume ∂JetPrototype.spaceVolume) atTop (𝓝 0) := by
let s := fun n => jetScale s₀ η (j n).annulus
let δ := fun n => DatumBounds.scale s₀ η (N n+1)
let C := 4*JetBarrierCollision.frequencyConstant*K*d₀
let A := weightFrequencyConstant q 2
let D := escapedFrequencyConstant s₀ η α K d₀ q 0
let E := fun n => coldOpticalDepth (C*s n^9) A (δ n) D 0 (t n)
let ε := fun n => JetSupersolution.epsilon K (s n) (d₀*(s n)^10)
let err := fun n (p : JetPrototype.Phase) =>
H q p.2*(F n).cold (j n) (t n,p)-
JetFreeTransport.free η K α γ (s n) (d₀*(s n)^10) (t n) (j n).positive
(shift (displacement (j n).lattice) p)
let I := fun n => ∫ p : JetPrototype.Phase, |err n p|
∂(JetPrototype.spaceVolume.restrict (r n • Ω)).prod volume
have hs (n) : 0 < s n := DatumBounds.scale_pos (η := η) hs₀ _
have hC : 0 ≤ C := by
dsimp [C]
exact mul_nonneg
(mul_nonneg (mul_nonneg (by norm_num) JetBarrierCollision.frequencyConstant_nonneg) hK) hd₀.le
have hA : 0 ≤ A := weightFrequencyConstant_nonneg q (by norm_num)
have hD : 0 ≤ D := escapedFrequencyConstant_nonneg hs₀ hK hd₀ η α q 0
have hEn (n) : 0 ≤ E n := coldOpticalDepth_nonneg
(mul_nonneg hC (pow_nonneg (hs n).le _)) hA (DatumBounds.scale_pos hs₀ _).le hD (ht n).1.le 0
have hεn (n) : 0 ≤ ε n := JetSupersolution.epsilon_nonneg hK (hs n)
(mul_pos hd₀ (pow_pos (hs n) _))
have hcomp (n) : IsCompact (r n • Ω) := hΩ.image (continuous_const_smul (r n))
have hfin (n) : IsFiniteMeasure (JetPrototype.spaceVolume.restrict (r n • Ω)) :=
isFiniteMeasure_restrict.mpr (hcomp n).measure_lt_top.ne
have hbound (n) : Integrable (fun p => |err n p|)
((JetPrototype.spaceVolume.restrict (r n • Ω)).prod volume) ∧
I n ≤ (E n+ε n)*((r n)^3*JetPrototype.spaceVolume.real Ω)*
(JetBarrierLocalMass.massConstant*(K/s n)) := by
let _ := hfin n
have hb := (F n).local_free_error hs₀ hsmax hη hηmax hK hα hαmax hγ hd₀ hd₀max
(hT n) (hTmax n) hq hsmall 0 (j n) (hj0 n) (hj n) (hwidth n) (hdmax n) (r n • Ω) (ht n)
dsimp only at hb
refine ⟨hb.1,?_⟩
simpa only [I,err,E,ε,C,A,D,s,δ,measureReal_restrict_apply_univ,
ColdDilationMeasure.spaceVolume_real_smul Ω (hr n)] using hb.2
have hElim : Tendsto E atTop (𝓝 0) :=
coldOpticalDepth_tendsto_zero hC hA hD hS (fun n => (hr n).le)
(fun n => (hs n).le) (fun n => (ht n).1.le) (fun n => (DatumBounds.scale_pos hs₀ _).le)
hhi htime hδ hrlim
have hεlim : Tendsto ε atTop (𝓝 0) := jet_epsilon_tendsto_zero hs hhi hrlim K d₀
have hlim : Tendsto (fun n => I n/(r n)^2) atTop (𝓝 0) :=
scaled_local_error_tendsto_zero hEn hεn measureReal_nonneg JetBarrierLocalMass.massConstant_nonneg
hK hr hs ha hlo (fun n => integral_nonneg (fun _ => abs_nonneg _))
(fun n => (hbound n).2) hElim hεlim
convert hlim using 1
funext n
rw [ColdDilationMeasure.dilated_error_integral (err n) Ω (hr n)]
rw [← integral_prod _ (hbound n).1]
end BoltzmannNonuniqueness.JetCopyDatum
end
end
section
/-! # Thermal mask replacement on finite spatial cylinders -/
noncomputable section
open MeasureTheory Filter Set
open scoped Topology
open BoltzmannNonuniqueness.VelocityWeight
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
{S : AttainedCapSequence F}
theorem HotLimitExtraction.coldLabel_mask_average_limit (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hη : 0 < η) (k : ℤ) (a : Bool) (t : ℝ)
(Ω : Set Transverse) (hΩ : volume Ω < ⊤) (ν : Measure ℝ) [IsFiniteMeasure ν] :
let r := fun n => S.radius (E.indices n)
let s := fun n => JetGeometry.jetScale s₀ η (E.coldLabel k a n).annulus
let d := fun n => d₀*(s n)^10
let μ := E.phase*Real.exp (η*(k:ℝ))
Tendsto (fun n => ∫ x : JetPrototype.Space,
|∫ w, JetGeometry.maskError (r n) η (s n) (d n) μ t a (x.1,w)
∂(volume : Measure Transverse).prod volume| ∂(volume.restrict Ω).prod ν)
atTop (𝓝 0) := by
intro r s d μ
have hr (n) : 0 < r n := S.radius_pos hs₀ (E.indices n)
have hrlim : Tendsto r atTop (𝓝 0) :=
(S.radius_tendsto_zero hs₀).comp E.indices_strict.tendsto_atTop
have hb := JetGeometry.maskError_average_L1_tendsto hr hrlim
(E.coldLabel_scale_limit hs₀ hη k a) (E.coldLabel_width_tendsto_zero hs₀ hη k a)
η t a Ω hΩ
change Tendsto (fun n => ∫ y, |∫ w,
JetGeometry.maskError (r n) η (r n*(s n/r n)) (d n) μ t a (y,w)
∂(volume : Measure Transverse).prod volume| ∂volume.restrict Ω) atTop (𝓝 0) at hb
simp only [mul_div_cancel₀ _ (hr _).ne'] at hb
have h := hb.const_mul (ν.real univ)
simp only [mul_zero] at h
apply h.congr'
filter_upwards [] with n
exact (integral_fun_fst (μ := volume.restrict Ω) (ν := ν)
(fun y => |∫ w, JetGeometry.maskError (r n) η (s n) (d n) μ t a (y,w)
∂(volume : Measure Transverse).prod volume|)).symm
theorem HotLimitExtraction.coldLabel_mask_average_integrable (E : HotLimitExtraction S)
(k : ℤ) (a : Bool) (n : ℕ) (t : ℝ)
(Ω : Set Transverse) (hΩ : volume Ω < ⊤) (ν : Measure ℝ) [IsFiniteMeasure ν] :
Integrable (fun x : JetPrototype.Space => ∫ w,
JetGeometry.maskError (S.radius (E.indices n)) η
(JetGeometry.jetScale s₀ η (E.coldLabel k a n).annulus)
(d₀*(JetGeometry.jetScale s₀ η (E.coldLabel k a n).annulus)^10)
(E.phase*Real.exp (η*(k:ℝ))) t a (x.1,w)
∂(volume : Measure Transverse).prod volume) ((volume.restrict Ω).prod ν) := by
let _ : IsFiniteMeasure ((volume : Measure Transverse).restrict Ω) :=
⟨by simpa only [Measure.restrict_apply_univ] using hΩ⟩
exact (JetGeometry.maskError_integrable _ _ _ _ _ _ _
((volume : Measure Transverse).restrict Ω)).integral_prod_left.comp_fst ν
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # The rebuilt cold family of an actual cap shot -/
noncomputable section
open MeasureTheory Set
open BoltzmannNonuniqueness.WeightedLocal BoltzmannNonuniqueness.WeightedLocalControl
namespace BoltzmannNonuniqueness.JetCopyDatum
theorem CapApproximation.cold_properties {s₀ η K α γ d₀ q T : ℝ} {N : ℕ}
(F : CapApproximation s₀ η K α γ d₀ q T N)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) (hT : 0 ≤ T) :
(∀ i, Measurable (F.cold i)) ∧ (∀ i u, 0 ≤ F.cold i u) ∧
(∀ s : Finset JetLattice.Label, ∀ u, ∑ i ∈ s, F.cold i u ≤ F.solution.value u) ∧
(∀ i, ColdMildAE q (N+1) (damping q (N+1) F.amplitude) T F.solution.value
(color s₀ η K α γ d₀ q N i) (F.cold i)) := by
have hδ := DatumBounds.scale_pos (η := η) hs₀ (N+1)
have hδone : DatumBounds.scale s₀ η (N+1) ≤ 1 := by
have h := JetGeometry.scale_antitone hs₀.le hη.le (Nat.zero_le (N+1))
rw [show DatumBounds.scale s₀ η 0 = s₀ by simp [DatumBounds.scale]] at h
linarith
have hh₀ (p) : 0 ≤ F.coefficient*HotSeedProfile.normalized q (DatumBounds.scale s₀ η (N+1)) p :=
mul_nonneg F.coefficient_mem.1 ((HotSeedProfile.normalized_bounds hδ hδone q).choose_spec.2 p).1
have hi := initial_color_bounds hs₀ hsmax hη hηmax hK hd₀ α γ q N hh₀
have hc₀ (i) (p) : 0 ≤ color s₀ η K α γ d₀ q N i p ∧
color s₀ η K α γ d₀ q N i p ≤ 2*F.amplitude :=
⟨(hi.1 i p).1,(hi.1 i p).2.trans (F.initial_bound p)⟩
have hL : 0 ≤ damping q (N+1) F.amplitude :=
(bounds (q := q) (by positivity : 0 ≤ (N+1:ℝ)) F.amplitude_pos).1
have hR : 0 ≤ 2*F.amplitude := mul_nonneg (by norm_num) F.amplitude_pos.le
have hp := rebuiltColdFamily_properties hq (by positivity : 0 ≤ (N+1:ℝ)) hL hT hR le_rfl
F.solution.measurable_value (measurable_color s₀ η K α γ d₀ q N)
F.solution.value_bounds hc₀ hi.2 (F.solution.all_mild hT)
exact ⟨hp.1,fun i u => (hp.2.1 i u).1,hp.2.2.1,hp.2.2.2.2⟩
theorem CapApproximation.hotNetSource_measurable {s₀ η K α γ d₀ q T : ℝ} {N : ℕ}
(F : CapApproximation s₀ η K α γ d₀ q T N)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) (hT : 0 ≤ T) :
Measurable F.hotNetSource := by
have hc := F.cold_properties hs₀ hsmax hη hηmax hK hd₀ hq hT
have hh := (F.hot_properties hs₀ hsmax hη hηmax hK hd₀ hq hT).1
exact ((measurable_forcing F.solution.measurable_value q (N+1) _).sub
(Measurable.tsum (fun i => measurable_coldForcing F.solution.measurable_value (hc.1 i) q (N+1) _))).sub
(hh.const_mul _)
end BoltzmannNonuniqueness.JetCopyDatum
end
end
section
/-! # The actual hot remainder satisfies a bounded linear mild equation -/
noncomputable section
open MeasureTheory Set
open BoltzmannNonuniqueness.WeightedLocal BoltzmannNonuniqueness.WeightedLocalControl
namespace BoltzmannNonuniqueness.JetCopyDatum
def CapApproximation.hotInitial {s₀ η K α γ d₀ q T : ℝ} {N : ℕ}
(F : CapApproximation s₀ η K α γ d₀ q T N) (p : JetPrototype.Phase) : ℝ :=
initial s₀ η K α γ d₀ q N
(fun p => F.coefficient*HotSeedProfile.normalized q (DatumBounds.scale s₀ η (N+1)) p) p-
∑' i, color s₀ η K α γ d₀ q N i p
theorem CapApproximation.hot_mild {s₀ η K α γ d₀ q T : ℝ} {N : ℕ}
(F : CapApproximation s₀ η K α γ d₀ q T N)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) (hT : 0 ≤ T) :
∀ t ∈ Icc 0 T, (fun p => F.hot (t,p)) =ᵐ[FlightMeasure.phaseVolume]
(fun p => PositiveIntegral.value T (damping q (N+1) F.amplitude) JetBarrier.flight
F.hotInitial (remainderForcing q (N+1) (damping q (N+1) F.amplitude)
F.solution.value F.cold) (t,p)) := by
have hc := F.cold_properties hs₀ hsmax hη hηmax hK hd₀ hq hT
have hδ := DatumBounds.scale_pos (η := η) hs₀ (N+1)
have hδone : DatumBounds.scale s₀ η (N+1) ≤ 1 := by
have h := JetGeometry.scale_antitone hs₀.le hη.le (Nat.zero_le (N+1))
rw [show DatumBounds.scale s₀ η 0 = s₀ by simp [DatumBounds.scale]] at h
linarith
have hh₀ (p) : 0 ≤ F.coefficient*HotSeedProfile.normalized q (DatumBounds.scale s₀ η (N+1)) p :=
mul_nonneg F.coefficient_mem.1 ((HotSeedProfile.normalized_bounds hδ hδone q).choose_spec.2 p).1
have hi := initial_color_bounds hs₀ hsmax hη hηmax hK hd₀ α γ q N hh₀
exact family_hot_mildAE hq (by positivity : 0 ≤ (N+1:ℝ))
(bounds (by positivity) F.amplitude_pos).1 hT (mul_nonneg (by norm_num) F.amplitude_pos.le) le_rfl
F.solution.measurable_value hc.1 F.solution.value_bounds hc.2.1 hc.2.2.1
(fun i p => (hi.1 i p).1) hi.2 F.solution.mild hc.2.2.2
theorem CapApproximation.hot_localized {s₀ η K α γ d₀ q T : ℝ} {N : ℕ}
(F : CapApproximation s₀ η K α γ d₀ q T N)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) (hT : 0 ≤ T)
(χ χ' : JetPrototype.Phase → ℝ → ℝ)
(hχ : ∀ p, ContinuousOn (χ p) (Icc 0 T))
(hχ' : ∀ p, ContinuousOn (χ' p) (Icc 0 T))
(hdχ : ∀ p t, t ∈ Icc 0 T → HasDerivAt (χ p) (χ' p t) t) :
∀ᵐ p ∂FlightMeasure.phaseVolume,
χ p T*F.hot (T,JetBarrier.flight T p) = Real.exp (-T)*χ p 0*F.hotInitial p+
∫ t in 0..T, Real.exp (-(T-t)) *
(χ p t*F.hotNetSource (t,JetBarrier.flight t p)+
(χ' p t+χ p t)*F.hot (t,JetBarrier.flight t p)) := by
have hc := F.cold_properties hs₀ hsmax hη hηmax hK hd₀ hq hT
have hb := family_hot_bounds hq (by positivity : 0 ≤ (N+1:ℝ)) (mul_nonneg (by norm_num : (0:ℝ) ≤ 2) F.amplitude_pos.le)
le_rfl F.solution.measurable_value hc.1 F.solution.value_bounds hc.2.1 hc.2.2.1
have hm : Measurable F.hotInitial := by
unfold hotInitial initial
exact ((measurable_seed s₀ η K α γ d₀ q N).add
((HotSeedProfile.normalized_measurable q _).const_mul F.coefficient)).sub
(Measurable.tsum (measurable_color s₀ η K α γ d₀ q N))
exact PositiveIntegral.localized_characteristic hT hm hb.1 hb.2.2.1
(fun u => by rw [abs_of_nonneg (hb.2.2.2 u).1]; exact (hb.2.2.2 u).2)
(F.hot_mild hs₀ hsmax hη hηmax hK hd₀ hq hT) χ χ' hχ hχ' hdχ
end BoltzmannNonuniqueness.JetCopyDatum
end
end
section
/-! # The mixed-cold source bound for the actual cap approximations -/
noncomputable section
open MeasureTheory Set
open BoltzmannNonuniqueness.WeightedLocal BoltzmannNonuniqueness.WeightedLocalControl
namespace BoltzmannNonuniqueness.JetCopyDatum
def CapApproximation.coldSource {s₀ η K α γ d₀ q T : ℝ} {N : ℕ}
(F : CapApproximation s₀ η K α γ d₀ q T N) : ℝ × JetPrototype.Phase → ℝ :=
coldFamilySource q (N+1) F.cold
theorem CapApproximation.coldSource_measurable {s₀ η K α γ d₀ q T : ℝ} {N : ℕ}
(F : CapApproximation s₀ η K α γ d₀ q T N)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) (hT : 0 ≤ T) :
Measurable F.coldSource := by
have hc := F.cold_properties hs₀ hsmax hη hηmax hK hd₀ hq hT
have hC : Measurable (fun u => ∑' i, F.cold i u) := Measurable.tsum hc.1
exact (measurable_forcing hC q (N+1) 0).sub
(Measurable.tsum (fun i => measurable_coldForcing hC (hc.1 i) q (N+1) 0))
theorem CapApproximation.cold_source_bound (hcarleman : Published.GPV2009CarlemanInput)
{s₀ η K α γ d₀ q T : ℝ} {N : ℕ} (F : CapApproximation s₀ η K α γ d₀ q T N)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 < α) (hαmax : α ≤ 1) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) (hT : 0 ≤ T) (hTmax : T ≤ 1/32) (m : ℕ)
(htail : JetEscapedEnvelope.constant s₀ η α K d₀
(JetEscapedEnvelope.exponent (m+1 : ℕ))*T^(m+1) ≤ 1) :
∀ᵐ u ∂spacetimeVolume, u.1 ∈ Ioc 0 T → 0 ≤ F.coldSource u ∧
F.coldSource u ≤ (2*JetMainGain.coefficient K α γ q+2*HotApplication.realBound q)*
JetEscapedEnvelope.constant s₀ η α K d₀
(JetEscapedEnvelope.exponent (m+1 : ℕ))*u.1^m := by
have hδ := DatumBounds.scale_pos (η := η) hs₀ (N+1)
have hδone : DatumBounds.scale s₀ η (N+1) ≤ 1 := by
have h := JetGeometry.scale_antitone hs₀.le hη.le (Nat.zero_le (N+1))
rw [show DatumBounds.scale s₀ η 0 = s₀ by simp [DatumBounds.scale]] at h
linarith
have hh₀ (p) : 0 ≤ F.coefficient*HotSeedProfile.normalized q (DatumBounds.scale s₀ η (N+1)) p :=
mul_nonneg F.coefficient_mem.1 ((HotSeedProfile.normalized_bounds hδ hδone q).choose_spec.2 p).1
have hc := F.cold_properties hs₀ hsmax hη hηmax hK hd₀.le hq₂ hT
have hL : 0 ≤ damping q (N+1) F.amplitude :=
(bounds (q := q) (by positivity : 0 ≤ (N+1:ℝ)) F.amplitude_pos).1
have hR : 0 ≤ 2*F.amplitude := mul_nonneg (by norm_num) F.amplitude_pos.le
have hE := JetEscapedEnvelope.constant_nonneg hs₀ hK hd₀ η α
(JetEscapedEnvelope.exponent (m+1 : ℕ))
have hb := geometric_cold_source (b := (N+1:ℝ)) hcarleman hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq₁ hq₂ hTmax (m+1 : ℕ) N hc.1
(fun u => (F.solution.value_bounds u).2) hc.2.1 hc.2.2.1
(rebuilt_zero s₀ η K α γ d₀ q (N+1) (damping q (N+1) F.amplitude) T N
(fun u => (F.solution.value_bounds u).1))
(fun t ht i x w => rebuilt_envelope hs₀ hsmax hη hηmax hK hα.le hγ.le hd₀ hsmall
hq₂ (by positivity) hL hT hR (hTmax.trans (by norm_num)) le_rfl N hh₀
F.solution.measurable_value F.solution.value_bounds F.initial_bound i ht
(JetPeriodicDatum.spatialMap x,w))
(fun n i => rebuilt_shift n (F.solution.periodic n) i)
(fun t ht => by simpa only [Real.rpow_natCast] using tail_small hE ht.1.le ht.2 htail)
filter_upwards [hb] with u hu hut
refine ⟨(hu hut).1,?_⟩
have h := (hu hut).2
rw [scalarMajorant_eq_source s₀ η K α γ d₀ q N m hut.1 0] at h
simpa only [CapApproximation.coldSource,ZeroProfile.source,mul_zero,zero_pow (by norm_num : (2:ℕ) ≠ 0),
zero_add] using h
end BoltzmannNonuniqueness.JetCopyDatum
end
end
section
/-! # Thermal concentration for the actual mesh labels -/
noncomputable section
open MeasureTheory Filter Set
open scoped Topology
open BoltzmannNonuniqueness.VelocityWeight
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
{S : AttainedCapSequence F}
theorem HotLimitExtraction.coldLabel_thermal_limit (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hη : 0 < η) (hK : 0 ≤ K) (hα : 0 ≤ α) (hγ : 0 ≤ γ) (hd₀ : 0 < d₀)
(k : ℤ) (a : Bool) {t : ℝ} (ht : 0 ≤ t) {B : ℝ} {ψ : Velocity → ℝ}
(hψ : Continuous ψ) (hψB : ∀ v, |ψ v| ≤ B) (x : JetPrototype.Space) :
let r := fun n => S.radius (E.indices n)
let s := fun n => JetGeometry.jetScale s₀ η (E.coldLabel k a n).annulus
let d := fun n => d₀*(s n)^10
let μ := E.phase*Real.exp (η*(k:ℝ))
Tendsto (fun n => (∫ v, r n*JetFreeTransport.free η K α γ (s n) (d n)
(r n*t) a (r n • x,v)*ψ v)-
(JetCoreDensity.compressed K α γ μ t (AxialFlow.foot (JetPrototype.sign a) α γ μ t x.2)*
ψ (PlaneChart.join 0 (AxialFlow.velocity (JetPrototype.sign a) α γ μ t x.2)))*
(∫ w, JetCoreDensity.dilatedMask (r n) η (s n/r n) (d n) t a x w*
JetThermalKernel.J (SheetMeasures.join w)
∂(volume : Measure Transverse).prod volume)) atTop (𝓝 0) := by
intro r s d μ
have hr (n) : 0 < r n := S.radius_pos hs₀ (E.indices n)
have hs (n) : 0 < s n := DatumBounds.scale_pos hs₀ _
have hμ : 0 < μ := mul_pos (zero_lt_one.trans_le E.phase_mem.1) (Real.exp_pos _)
have hrlim : Tendsto r atTop (𝓝 0) :=
(S.radius_tendsto_zero hs₀).comp E.indices_strict.tendsto_atTop
have hslim : Tendsto (fun n => s n/r n) atTop (𝓝 μ) := E.coldLabel_scale_limit hs₀ hη k a
have hdlim : Tendsto d atTop (𝓝 0) := E.coldLabel_width_tendsto_zero hs₀ hη k a
have hclip : Tendsto (fun n => max (μ/2) (s n/r n)) atTop (𝓝 μ) := by
have hm : Tendsto (fun n => max (μ/2) (s n/r n)) atTop (𝓝 (max (μ/2) μ)) :=
tendsto_const_nhds.max hslim
simpa only [max_eq_right (show μ/2 ≤ μ by linarith)] using hm
have hbase := JetCoreDensity.dilated_free_thermal_reduction hr hK hα hγ
(by positivity : 0 < μ/2) (fun n => le_max_left (μ/2) (s n/r n))
(fun n => mul_pos hd₀ (pow_pos (hs n) 10)) hμ ht hrlim hclip hdlim hψ hψB η a x
apply hbase.congr'
filter_upwards [hslim.eventually (lt_mem_nhds (show μ/2 < μ by linarith))] with n hn
rw [max_eq_right hn.le,mul_div_cancel₀ _ (hr n).ne']
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Spatial L1 thermal reduction for the actual retained-scale labels -/
noncomputable section
open MeasureTheory Filter Set
open scoped Topology
open BoltzmannNonuniqueness.VelocityWeight
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
{S : AttainedCapSequence F}
theorem HotLimitExtraction.coldLabel_thermal_L1_limit (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hη : 0 < η) (hK : 0 ≤ K) (hα : 0 < α) (hγ : 0 < γ) (hd₀ : 0 < d₀)
(k : ℤ) (a : Bool) {t : ℝ} (ht : 0 < t) {B : ℝ} {ψ : Velocity → ℝ}
(hψ : Continuous ψ) (hψB : ∀ v, |ψ v| ≤ B)
(ρ : Measure JetPrototype.Space) [IsFiniteMeasure ρ] :
let r := fun n => S.radius (E.indices n)
let s := fun n => JetGeometry.jetScale s₀ η (E.coldLabel k a n).annulus
let d := fun n => d₀*(s n)^10
let μ := E.phase*Real.exp (η*(k:ℝ))
Tendsto (fun n => ∫ x, |(∫ v, r n*JetFreeTransport.free η K α γ (s n) (d n)
(r n*t) a (r n • x,v)*ψ v)-
JetCoreDensity.limitingCoefficient K α γ μ t (JetPrototype.sign a) ψ x*
(∫ w, JetCoreDensity.dilatedMask (r n) η (s n/r n) (d n) t a x w*
JetThermalKernel.J (SheetMeasures.join w)
∂(volume : Measure Transverse).prod volume)| ∂ρ) atTop (𝓝 0) := by
intro r s d μ
let f : ℕ → JetPrototype.Space → ℝ := fun n x =>
(∫ v, r n*JetFreeTransport.free η K α γ (s n) (d n) (r n*t) a (r n • x,v)*ψ v)-
JetCoreDensity.limitingCoefficient K α γ μ t (JetPrototype.sign a) ψ x*
(∫ w, JetCoreDensity.dilatedMask (r n) η (s n/r n) (d n) t a x w*
JetThermalKernel.J (SheetMeasures.join w)
∂(volume : Measure Transverse).prod volume)
have hr (n) : 0 < r n := S.radius_pos hs₀ (E.indices n)
have hs (n) : 0 < s n := DatumBounds.scale_pos hs₀ _
have hd (n) : 0 < d n := mul_pos hd₀ (pow_pos (hs n) 10)
have hμ : 0 < μ := mul_pos (zero_lt_one.trans_le E.phase_mem.1) (Real.exp_pos _)
have hfm (n) : Measurable (f n) :=
(JetCoreDensity.free_average_measurable (r n) η K α γ (s n) (d n) t a hψ.measurable).sub
((JetCoreDensity.limitingCoefficient_measurable hα.le hγ.le hμ ht.le K
(JetPrototype.sign a) hψ).mul
(JetCoreDensity.mask_average_measurable (r n) η (s n/r n) (d n) t a))
have hl (x) : Tendsto (fun n => f n x) atTop (𝓝 0) :=
E.coldLabel_thermal_limit hs₀ hη hK hα.le hγ.le hd₀ k a ht.le hψ hψB x
let C := ((K*max 1 (α*γ)⁻¹)/t)*B
have hb (n x) : |f n x| ≤ 2*C := by
have hfree := JetCoreDensity.dilated_free_average_bound (hr n) hK hα hγ
(hs n) (hd n) ht η a x hψ hψB
have hc := JetCoreDensity.limitingCoefficient_bound hK hα hγ hμ ht hψB
(JetPrototype.sign a) x
have hm := JetCoreDensity.masked_thermal_bound
(JetCoreDensity.dilatedMask_abs_le (r n) η (s n/r n) (d n) t a x)
have hp : |JetCoreDensity.limitingCoefficient K α γ μ t (JetPrototype.sign a) ψ x*
(∫ w, JetCoreDensity.dilatedMask (r n) η (s n/r n) (d n) t a x w*
JetThermalKernel.J (SheetMeasures.join w)
∂(volume : Measure Transverse).prod volume)| ≤ C := by
rw [abs_mul]
exact (mul_le_of_le_one_right (abs_nonneg _) hm).trans hc
exact (abs_sub _ _).trans ((add_le_add hfree hp).trans_eq (by dsimp [C]; ring))
have h := tendsto_integral_of_dominated_convergence (μ := ρ)
(F := fun n x => |f n x|) (f := fun _ => (0:ℝ)) (fun _ => 2*C)
(fun n => (hfm n).abs.aestronglyMeasurable) (integrable_const _)
(fun n => ae_of_all _ (fun x => by
rw [Real.norm_of_nonneg (abs_nonneg _)]
exact hb n x)) (ae_of_all _ (fun x => by simpa only [abs_zero] using (hl x).abs))
simpa only [integral_zero] using h
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # The actual free-core average reduces to its limiting shell and fine stripes -/
noncomputable section
open MeasureTheory Filter Set
open scoped Topology
open BoltzmannNonuniqueness.VelocityWeight
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
{S : AttainedCapSequence F}
def HotLimitExtraction.coldLabelFreeAverage (E : HotLimitExtraction S) (k : ℤ) (a : Bool)
(n : ℕ) (t : ℝ) (ψ : Velocity → ℝ) (x : JetPrototype.Space) : ℝ :=
let r := S.radius (E.indices n)
let s := JetGeometry.jetScale s₀ η (E.coldLabel k a n).annulus
∫ v, r*JetFreeTransport.free η K α γ s (d₀*s^10) (r*t) a (r • x,v)*ψ v
def HotLimitExtraction.coldLabelStripeAverage (E : HotLimitExtraction S) (k : ℤ) (a : Bool)
(n : ℕ) (t : ℝ) (y : Transverse) : ℝ :=
let r := S.radius (E.indices n)
let s := JetGeometry.jetScale s₀ η (E.coldLabel k a n).annulus
∫ w, (JetGeometry.stripe s a).indicator (fun _ => (1:ℝ))
(r • (y-t • ((d₀*s^10) • w.1)))*JetThermalKernel.J (SheetMeasures.join w)
∂(volume : Measure Transverse).prod volume
def HotLimitExtraction.coldLabelStripedProfile (E : HotLimitExtraction S) (k : ℤ) (a : Bool)
(n : ℕ) (t : ℝ) (ψ : Velocity → ℝ) (x : JetPrototype.Space) : ℝ :=
let μ := E.phase*Real.exp (η*(k:ℝ))
JetCoreDensity.limitingCoefficient K α γ μ t (JetPrototype.sign a) ψ x*
((JetGeometry.scaleShell η μ).indicator (fun _ => (1:ℝ)) x.1*
E.coldLabelStripeAverage k a n t x.1)
theorem HotLimitExtraction.coldLabel_free_striped_L1_limit (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hη : 0 < η) (hK : 0 ≤ K) (hα : 0 < α) (hγ : 0 < γ) (hd₀ : 0 < d₀)
(k : ℤ) (a : Bool) {t : ℝ} (ht : 0 < t) {B : ℝ} {ψ : Velocity → ℝ}
(hψ : Continuous ψ) (hψB : ∀ v, |ψ v| ≤ B)
(Ω : Set Transverse) (hΩ : volume Ω < ⊤) (ν : Measure ℝ) [IsFiniteMeasure ν] :
Tendsto (fun n => ∫ x, |E.coldLabelFreeAverage k a n t ψ x-
E.coldLabelStripedProfile k a n t ψ x| ∂(volume.restrict Ω).prod ν) atTop (𝓝 0) := by
let _ : IsFiniteMeasure ((volume : Measure Transverse).restrict Ω) :=
⟨by simpa only [Measure.restrict_apply_univ] using hΩ⟩
let ρ := (volume.restrict Ω).prod ν
let r := fun n => S.radius (E.indices n)
let s := fun n => JetGeometry.jetScale s₀ η (E.coldLabel k a n).annulus
let d := fun n => d₀*(s n)^10
let μ := E.phase*Real.exp (η*(k:ℝ))
let c := JetCoreDensity.limitingCoefficient K α γ μ t (JetPrototype.sign a) ψ
let m := fun n x => ∫ w, JetCoreDensity.dilatedMask (r n) η (s n/r n) (d n) t a x w*
JetThermalKernel.J (SheetMeasures.join w) ∂(volume : Measure Transverse).prod volume
let e := fun n (x : JetPrototype.Space) => ∫ w,
JetGeometry.maskError (r n) η (s n) (d n) μ t a (x.1,w)
∂(volume : Measure Transverse).prod volume
let f := E.coldLabelFreeAverage k a
let C := ((K*max 1 (α*γ)⁻¹)/t)*B
have hr (n) : 0 < r n := S.radius_pos hs₀ (E.indices n)
have hs (n) : 0 < s n := DatumBounds.scale_pos hs₀ _
have hd (n) : 0 < d n := mul_pos hd₀ (pow_pos (hs n) 10)
have hμ : 0 < μ := mul_pos (zero_lt_one.trans_le E.phase_mem.1) (Real.exp_pos _)
have htlim := E.coldLabel_thermal_L1_limit hs₀ hη hK hα hγ hd₀ k a ht hψ hψB ρ
have hmlim := E.coldLabel_mask_average_limit hs₀ hη k a t Ω hΩ ν
change Tendsto (fun n => ∫ x, |f n t ψ x-c x*m n x| ∂ρ) atTop (𝓝 0) at htlim
change Tendsto (fun n => ∫ x, |e n x| ∂ρ) atTop (𝓝 0) at hmlim
have hlim := htlim.add (hmlim.const_mul C)
simp only [mul_zero,zero_add] at hlim
apply squeeze_zero (fun _ => integral_nonneg (fun _ => abs_nonneg _)) _ hlim
intro n
have hi₁ : Integrable (fun x => f n t ψ x-c x*m n x) ρ :=
JetCoreDensity.thermal_error_integrable (hr n) hK hα hγ (hs n) (hd n) hμ ht η a hψ hψB ρ
have hi₂ : Integrable (e n) ρ := E.coldLabel_mask_average_integrable k a n t Ω hΩ ν
rw [← integral_const_mul,← integral_add hi₁.abs (hi₂.abs.const_mul C)]
apply integral_mono_of_nonneg (ae_of_all _ (fun _ => abs_nonneg _))
(hi₁.abs.add (hi₂.abs.const_mul C))
filter_upwards [] with x
have he : e n x = m n x-(JetGeometry.scaleShell η μ).indicator (fun _ => (1:ℝ)) x.1*
E.coldLabelStripeAverage k a n t x.1 := by
have hb := JetGeometry.maskError_average_eq (r n) η (s n/r n) (d n) μ t a x
simp only [mul_div_cancel₀ _ (hr n).ne'] at hb
simpa only [e,m,r,s,d,coldLabelStripeAverage] using hb
have hid : f n t ψ x-E.coldLabelStripedProfile k a n t ψ x =
(f n t ψ x-c x*m n x)+c x*e n x := by
rw [he]
change f n t ψ x-c x*((JetGeometry.scaleShell η μ).indicator (fun _ => (1:ℝ)) x.1*
E.coldLabelStripeAverage k a n t x.1) = _
ring
rw [hid]
apply (abs_add_le _ _).trans
apply add_le_add le_rfl
rw [abs_mul]
exact mul_le_mul_of_nonneg_right
(JetCoreDensity.limitingCoefficient_bound hK hα hγ hμ ht hψB (JetPrototype.sign a) x)
(abs_nonneg _)
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Cold free-flight convergence on varying cap horizons -/
noncomputable section
open MeasureTheory Set Filter
open scoped Topology Pointwise
open BoltzmannNonuniqueness.JetLattice BoltzmannNonuniqueness.JetGeometry
open BoltzmannNonuniqueness.VelocityWeight BoltzmannNonuniqueness.WeightedTranslation
namespace BoltzmannNonuniqueness.JetCopyDatum
theorem cap_variable_cold_dilation_limit {s₀ η K α γ d₀ q a S U : ℝ} {T : ℕ → ℝ}
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 ≤ α) (hαmax : α ≤ 1/4) (hγ : 0 ≤ γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1) (hT : ∀ n, 0 ≤ T n) (hTmax : ∀ n, T n ≤ 1/32)
(hq : q < 2) (hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(N : ℕ → ℕ) (F : ∀ n, CapApproximation s₀ η K α γ d₀ q (T n) (N n))
(j : ℕ → Label) (hj0 : ∀ n, (j n).lattice = 0) (hj : ∀ n, (j n).annulus < N n)
(r t : ℕ → ℝ) (hr : ∀ n, 0 < r n) (hrlim : Tendsto r atTop (𝓝 0))
(ht : ∀ n, t n ∈ Ioc 0 (T n)) (ha : 0 < a) (hS : 0 ≤ S)
(hlo : ∀ n, a*r n ≤ jetScale s₀ η (j n).annulus)
(hhi : ∀ n, jetScale s₀ η (j n).annulus ≤ S*r n)
(htime : ∀ n, t n ≤ U*r n)
(hδ : ∀ n, DatumBounds.scale s₀ η (N n+1) ≤ r n)
(Ω : Set JetPrototype.Space) (hΩ : IsCompact Ω) :
Tendsto (fun n => ∫ x in Ω, ∫ v : Velocity,
|r n*(H q v*(F n).cold (j n) (t n,(r n • x,v))-
JetFreeTransport.free η K α γ (jetScale s₀ η (j n).annulus)
(d₀*jetScale s₀ η (j n).annulus^10) (t n) (j n).positive
(shift (displacement (j n).lattice) (r n • x,v)))|
∂volume ∂JetPrototype.spaceVolume) atTop (𝓝 0) := by
have hslim : Tendsto (fun n => jetScale s₀ η (j n).annulus) atTop (𝓝 0) := by
apply squeeze_zero (fun n => (DatumBounds.scale_pos (η := η) hs₀ _).le) hhi
simpa only [mul_zero] using hrlim.const_mul S
obtain ⟨n₀,hn₀⟩ := eventually_atTop.mp (eventually_cold_survival_geometry (T := (1/32:ℝ)) (d₀ := d₀) hη hslim)
apply (tendsto_add_atTop_iff_nat n₀).mp
exact cap_variable_cold_dilation_free_error hs₀ hsmax hη hηmax hK hα hαmax hγ hd₀ hd₀max (fun n => hT (n+n₀)) (fun n => hTmax (n+n₀)) hq hsmall
(fun n => N (n+n₀)) (fun n => F (n+n₀)) (fun n => j (n+n₀))
(fun n => hj0 (n+n₀)) (fun n => hj (n+n₀)) (fun n => r (n+n₀)) (fun n => t (n+n₀))
(fun n => hr (n+n₀)) (hrlim.comp (tendsto_add_atTop_nat n₀))
(fun n => ht (n+n₀)) ha hS (fun n => hlo (n+n₀)) (fun n => hhi (n+n₀))
(fun n => htime (n+n₀)) (fun n => hδ (n+n₀))
(fun n => (mul_le_mul_of_nonneg_right (hTmax (n+n₀)) (by positivity)).trans
(hn₀ (n+n₀) (by omega)).1) (fun n => (hn₀ (n+n₀) (by omega)).2) Ω hΩ
end BoltzmannNonuniqueness.JetCopyDatum
end
end
section
/-! # Product-space cold dilation with varying cap horizons -/
noncomputable section
open MeasureTheory Set Filter
open scoped Topology Pointwise
open BoltzmannNonuniqueness.JetLattice BoltzmannNonuniqueness.JetGeometry
open BoltzmannNonuniqueness.VelocityWeight BoltzmannNonuniqueness.WeightedTranslation
namespace BoltzmannNonuniqueness.JetCopyDatum
theorem cap_variable_cold_L1_dilation_limit {s₀ η K α γ d₀ q a S U : ℝ} {T : ℕ → ℝ}
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 ≤ α) (hαmax : α ≤ 1/4) (hγ : 0 ≤ γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1) (hT : ∀ n, 0 ≤ T n) (hTmax : ∀ n, T n ≤ 1/32)
(hq : q < 2) (hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(N : ℕ → ℕ) (F : ∀ n, CapApproximation s₀ η K α γ d₀ q (T n) (N n))
(j : ℕ → Label) (hj0 : ∀ n, (j n).lattice = 0) (hj : ∀ n, (j n).annulus < N n)
(r t : ℕ → ℝ) (hr : ∀ n, 0 < r n) (hrlim : Tendsto r atTop (𝓝 0))
(ht : ∀ n, t n ∈ Ioc 0 (T n)) (ha : 0 < a) (hS : 0 ≤ S)
(hlo : ∀ n, a*r n ≤ jetScale s₀ η (j n).annulus)
(hhi : ∀ n, jetScale s₀ η (j n).annulus ≤ S*r n)
(htime : ∀ n, t n ≤ U*r n)
(hδ : ∀ n, DatumBounds.scale s₀ η (N n+1) ≤ r n)
(Ω : Set JetPrototype.Space) (hΩ : IsCompact Ω) :
Tendsto (fun n => ∫ p : JetPrototype.Phase,
|r n*(H q p.2*(F n).cold (j n) (t n,(r n • p.1,p.2))-
JetFreeTransport.free η K α γ (jetScale s₀ η (j n).annulus)
(d₀*jetScale s₀ η (j n).annulus^10) (t n) (j n).positive
(shift (displacement (j n).lattice) (r n • p.1,p.2)))|
∂(JetPrototype.spaceVolume.restrict Ω).prod volume) atTop (𝓝 0) := by
have hbase := cap_variable_cold_dilation_limit hs₀ hsmax hη hηmax hK hα hαmax hγ hd₀ hd₀max
hT hTmax hq hsmall N F j hj0 hj r t hr hrlim ht ha hS hlo hhi htime hδ Ω hΩ
apply hbase.congr'
have hslim : Tendsto (fun n => jetScale s₀ η (j n).annulus) atTop (𝓝 0) := by
apply squeeze_zero (fun n => (DatumBounds.scale_pos (η := η) hs₀ _).le) hhi
simpa only [mul_zero] using hrlim.const_mul S
filter_upwards [eventually_cold_survival_geometry (T := (1/32:ℝ)) (d₀ := d₀) hη hslim] with n hn
have hcomp : IsCompact (r n • Ω) := hΩ.image (continuous_const_smul (r n))
let _ : IsFiniteMeasure (JetPrototype.spaceVolume.restrict (r n • Ω)) :=
isFiniteMeasure_restrict.mpr hcomp.measure_lt_top.ne
have hb := (F n).local_free_error hs₀ hsmax hη hηmax hK hα hαmax hγ hd₀ hd₀max
(hT n) (hTmax n) hq hsmall 0 (j n) (hj0 n) (hj n)
((mul_le_mul_of_nonneg_right (hTmax n) (by positivity)).trans hn.1) hn.2 (r n • Ω) (ht n)
dsimp only at hb
exact (integral_prod _ (ColdDilationMeasure.integrable_dilated_error (hr n) Ω hb.1)).symm
end BoltzmannNonuniqueness.JetCopyDatum
end
end
section
/-! # Cold/free convergence for the actual retained mesh labels -/
noncomputable section
open MeasureTheory Filter Set
open scoped Topology ENNReal
open BoltzmannNonuniqueness.VelocityWeight BoltzmannNonuniqueness.WeightedTranslation
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
{S : AttainedCapSequence F}
theorem HotLimitExtraction.coldLabel_free_limit (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 ≤ α) (hαmax : α ≤ 1/4) (hγ : 0 ≤ γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq : q < 2) (k : ℤ) (a : Bool)
(hk : E.fraction < E.phase*Real.exp (η*(k:ℝ)))
{t : ℝ} (ht : 0 < t) (htU : ENNReal.ofReal t < E.horizon)
(Ω : Set JetPrototype.Space) (hΩ : IsCompact Ω) :
let j := E.coldLabel k a
let r := fun n => S.radius (E.indices n)
Tendsto (fun n => ∫ p : JetPrototype.Phase,
|r n*(H q p.2*(F.approximation (E.indices n)).cold (j n) (r n*t,(r n • p.1,p.2))-
JetFreeTransport.free η K α γ (JetGeometry.jetScale s₀ η (j n).annulus)
(d₀*(JetGeometry.jetScale s₀ η (j n).annulus)^10) (r n*t) (j n).positive
(shift (displacement (j n).lattice) (r n • p.1,p.2)))|
∂(JetPrototype.spaceVolume.restrict Ω).prod volume) atTop (𝓝 0) := by
intro j r
let μ := E.phase*Real.exp (η*(k:ℝ))
have hμ : 0 < μ := mul_pos (zero_lt_one.trans_le E.phase_mem.1) (Real.exp_pos _)
have hrlim : Tendsto r atTop (𝓝 0) :=
(S.radius_tendsto_zero hs₀).comp E.indices_strict.tendsto_atTop
have hr (n) : 0 < r n := S.radius_pos hs₀ (E.indices n)
have hs : Tendsto (fun n => JetGeometry.jetScale s₀ η (j n).annulus/r n) atTop (𝓝 μ) :=
E.coldLabel_scale_limit hs₀ hη k a
have hlo := hs.eventually (lt_mem_nhds (show μ/2 < μ by linarith))
have hhi := hs.eventually (gt_mem_nhds (show μ < 2*μ by linarith))
have hgood : ∀ᶠ n in atTop,
(j n).annulus < F.indices (E.indices n) ∧
r n*t ∈ Ioc 0 (shrinkingHorizon F.horizonScale (E.indices n)) ∧
(μ/2)*r n ≤ JetGeometry.jetScale s₀ η (j n).annulus ∧
JetGeometry.jetScale s₀ η (j n).annulus ≤ (2*μ)*r n := by
filter_upwards [E.coldLabel_retained hs₀ hη k a hk,
S.eventually_scaled_slab hs₀ E.horizon_limit htU,hlo,hhi] with n hj htime hl hu
exact ⟨hj,⟨mul_pos (hr n) ht,(htime t ⟨ht.le,le_rfl⟩).2⟩,
((lt_div_iff₀ (hr n)).mp hl).le,((div_lt_iff₀ (hr n)).mp hu).le⟩
obtain ⟨n₀,hn₀⟩ := eventually_atTop.mp hgood
apply (tendsto_add_atTop_iff_nat n₀).mp
exact cap_variable_cold_L1_dilation_limit hs₀ hsmax hη hηmax hK hα hαmax hγ hd₀ hd₀max
(fun n => (shrinkingHorizon_pos F.horizonScale_pos (E.indices (n+n₀))).le)
(fun n => (shrinkingHorizon_le F.horizonScale_pos _).trans F.horizonScale_le)
hq hsmall (fun n => F.indices (E.indices (n+n₀)))
(fun n => F.approximation (E.indices (n+n₀))) (fun n => j (n+n₀)) (fun _ => rfl)
(fun n => (hn₀ (n+n₀) (by omega)).1) (fun n => r (n+n₀)) (fun n => r (n+n₀)*t)
(fun n => hr (n+n₀)) (hrlim.comp (tendsto_add_atTop_nat n₀))
(fun n => (hn₀ (n+n₀) (by omega)).2.1) (by positivity : 0 < μ/2)
(by positivity : 0 ≤ 2*μ) (fun n => (hn₀ (n+n₀) (by omega)).2.2.1)
(fun n => (hn₀ (n+n₀) (by omega)).2.2.2)
(U := t) (fun n => (mul_comm (r (n+n₀)) t).le)
(fun n => (div_le_one (hr (n+n₀))).mp (S.coldFraction_mem hs₀ (E.indices (n+n₀))).2)
Ω hΩ
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
end OAI