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import OAI.MathematicalPhysics.Boltzmann.Approximation.CapFiniteBackgroundLimit
import OAI.MathematicalPhysics.Boltzmann.Approximation.CapHotSourceIntegrability
import OAI.MathematicalPhysics.Boltzmann.Approximation.CapHotUndamped
import OAI.MathematicalPhysics.Boltzmann.Approximation.CapLabelFreeLimit
import OAI.MathematicalPhysics.Boltzmann.Branching.EuclideanKineticMap
import OAI.MathematicalPhysics.Boltzmann.Branching.MomentAverageBound
import OAI.MathematicalPhysics.Boltzmann.Branching.VanishingMajorant
import OAI.MathematicalPhysics.Boltzmann.Jets.GeometricDampedRetention
import OAI.MathematicalPhysics.Boltzmann.Jets.GeometricMesh
import OAI.MathematicalPhysics.Boltzmann.Jets.JetFiniteCap
import OAI.MathematicalPhysics.Boltzmann.Jets.JetFamilyBounds
namespace OAI
section
/-! # Half-Gaussian moments of the actual cold part -/
noncomputable section
open MeasureTheory Set
open scoped ENNReal
open BoltzmannNonuniqueness.WeightedLocal BoltzmannNonuniqueness.WeightedLocalControl
open BoltzmannNonuniqueness.WeightedTranslation BoltzmannNonuniqueness.VelocityWeight
open BoltzmannNonuniqueness.VelocityMoment
namespace BoltzmannNonuniqueness.JetCopyDatum
theorem CapApproximation.cold_envelope {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) (hγ : 0 ≤ γ) (hd₀ : 0 < d₀)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq : q < 2) (hT : 0 ≤ T) (hTmax : T ≤ 1/32)
(i : JetLattice.Label) {t : ℝ} (ht : t ∈ Ioc 0 T) (p : JetPrototype.Phase) :
H q p.2*F.cold i (t,p) ≤
JetSupersolution.U η K α γ (JetGeometry.jetScale s₀ η i.annulus)
(d₀*JetGeometry.jetScale s₀ η i.annulus^10) t i.positive
(shift (displacement i.lattice) p) := 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_envelope hs₀ hsmax hη hηmax hK hα hγ hd₀ hsmall hq (by positivity)
(bounds (by positivity) F.amplitude_pos).1 hT (by linarith [F.amplitude_pos])
(hTmax.trans (by norm_num)) le_rfl N hh₀ F.solution.measurable_value
F.solution.value_bounds F.initial_bound i ht p
theorem CapApproximation.coldTotal_moment_bound {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)
(hq : q < 2) (hT : 0 ≤ T) (hTmax : T ≤ 1/32)
{t : ℝ} (ht : t ∈ Ioc 0 T) (x : JetPrototype.Space) :
moment (fun v => H q v*F.coldTotal (t,(x,v))) ≤ ENNReal.ofReal
(escapedConstant s₀ η K α d₀*hotConstant q+JetEnvelopeGain.momentConstant K α γ/t) := by
have hc := F.cold_properties hs₀ hsmax hη hηmax hK hd₀.le hq hT
have hs := F.coldTotal_properties hs₀ hsmax hη hηmax hK hd₀.le hq hT
have hcell (y : Velocity) (hy : y ∈ TorusChart.cube) :
moment (fun v => H q v*F.coldTotal (t,(JetPeriodicDatum.spatialMap y,v))) ≤
ENNReal.ofReal (escapedConstant s₀ η K α d₀*hotConstant q+
JetEnvelopeGain.momentConstant K α γ/t) := by
have hm := cell_moment_bound (Z := 0) hs₀ hsmax hη hηmax hK hα hαmax hγ hd₀ hd₀max
hq le_rfl ht.1 (ht.2.trans hTmax) hsmall N y hy
(fun v => F.coldTotal (t,(JetPeriodicDatum.spatialMap y,v)))
(fun i v => F.cold i (t,(JetPeriodicDatum.spatialMap y,v)))
(fun i => (hc.1 i).comp (measurable_const.prodMk (measurable_const.prodMk measurable_id)))
(fun i v => hc.2.1 i _) (fun v => (hs.2 _).1)
(fun i hi v => congrFun (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) i hi) _)
(fun i v => F.cold_envelope hs₀ hsmax hη hηmax hK hα.le hγ.le hd₀ hsmall hq hT hTmax
i ht (JetPeriodicDatum.spatialMap y,v)) (ae_of_all _ (fun _ => by simp [coldTotal]))
apply hm.trans (ENNReal.ofReal_le_ofReal ?_)
simpa only [zero_add,div_eq_mul_inv,one_mul] using
add_le_add (le_refl (escapedConstant s₀ η K α d₀*hotConstant q))
(mul_le_mul_of_nonneg_left
(AnnularEnvelope.finiteEnvelope_le_inv_time hs₀.le hη.le ht.1 (Finset.range N)
(transverse y)) (JetEnvelopeGain.momentConstant_nonneg hK α γ))
obtain ⟨n,y,hy,hxy⟩ := exists_shift_in_centered_cell x
have he (v : Velocity) : F.coldTotal (t,(JetPeriodicDatum.spatialMap y,v)) =
F.coldTotal (t,(x,v)) := by
have h := family_sum_pull (c := F.cold) (displacement n) (relabel n)
(fun i => rebuilt_shift n (F.solution.periodic n) i) (t,(x,v))
change F.coldTotal (t,(x-displacement n,v)) = F.coldTotal (t,(x,v)) at h
rwa [hxy] at h
simpa only [he] using hcell y hy
end BoltzmannNonuniqueness.JetCopyDatum
end
end
section
/-! # Uniform cold moments on positive-time blow-up slabs -/
noncomputable section
open MeasureTheory Set Filter
open scoped ENNReal Topology
open BoltzmannNonuniqueness.VelocityWeight
namespace BoltzmannNonuniqueness.VelocityMoment
theorem moment_const_mul {r : ℝ} (hr : 0 ≤ r) (f : Velocity → ℝ) :
moment (fun v => r*f v) = ENNReal.ofReal r*moment f := by
unfold moment
simp_rw [show ∀ v, weight v*(r*f v) = r*(weight v*f v) by intro v; ring,
ENNReal.ofReal_mul hr]
exact lintegral_const_mul' _ _ ENNReal.ofReal_ne_top
end BoltzmannNonuniqueness.VelocityMoment
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
open VelocityMoment
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
theorem rescaledColdDensity_moment (S : AttainedCapSequence F)
(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)
(hq : q < 2) (n : ℕ) {t : ℝ} (ht : 0 < t)
(hT : S.radius n*t ≤ shrinkingHorizon F.horizonScale n) (x : JetPrototype.Space) :
moment (fun v => S.rescaledColdDensity n ((t,x),v)) ≤ ENNReal.ofReal
(S.radius n*(escapedConstant s₀ η K α d₀*hotConstant q)+
JetEnvelopeGain.momentConstant K α γ/t) := by
have hr := S.radius_pos hs₀ n
have hb := (F.approximation n).coldTotal_moment_bound hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq (shrinkingHorizon_pos F.horizonScale_pos n).le
((shrinkingHorizon_le F.horizonScale_pos n).trans F.horizonScale_le)
⟨mul_pos hr ht,hT⟩ (S.radius n • x)
have he : (fun v => S.rescaledColdDensity n ((t,x),v)) =
(fun v => S.radius n*(H q v*(F.approximation n).coldTotal
(S.radius n*t,(S.radius n • x,v)))) := by
funext v
exact mul_assoc _ _ _
rw [he,moment_const_mul hr.le]
apply (mul_le_mul' le_rfl hb).trans
rw [← ENNReal.ofReal_mul hr.le]
apply le_of_eq
congr 1
field_simp
theorem eventually_rescaledColdDensity_moment (S : AttainedCapSequence F)
(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)
(hq : q < 2) {κ : ℕ → ℕ} (hκ : StrictMono κ) {U : ℝ≥0∞}
(hU : Tendsto (fun n => S.normalizedHorizon (κ n)) atTop (𝓝 U))
{a A : ℝ} (ha : 0 < a) (hA : ENNReal.ofReal A < U) :
∀ᶠ n in atTop, ∀ t ∈ Icc a A, ∀ x : JetPrototype.Space,
moment (fun v => S.rescaledColdDensity (κ n) ((t,x),v)) ≤ ENNReal.ofReal
(escapedConstant s₀ η K α d₀*hotConstant q+JetEnvelopeGain.momentConstant K α γ/a) := by
have hC : 0 ≤ escapedConstant s₀ η K α d₀*hotConstant q :=
mul_nonneg (JetEscapedEnvelope.constant_nonneg hs₀ hK hd₀ η α _) (hotConstant_nonneg q)
have hr := ((S.radius_tendsto_zero hs₀).comp hκ.tendsto_atTop).eventually
(gt_mem_nhds (show (0:ℝ) < 1 by norm_num))
filter_upwards [hr,S.eventually_scaled_slab hs₀ hU hA] with n hn hslab
intro t ht x
have htpos := ha.trans_le ht.1
apply (S.rescaledColdDensity_moment hs₀ hsmax hη hηmax hK hα hαmax hγ hd₀ hd₀max hsmall hq
(κ n) htpos (hslab t ⟨htpos.le,ht.2⟩).2 x).trans
apply ENNReal.ofReal_le_ofReal
apply add_le_add
· simpa only [Function.comp_apply,one_mul] using mul_le_mul_of_nonneg_right hn.le hC
· exact div_le_div_of_nonneg_left (JetEnvelopeGain.momentConstant_nonneg hK α γ) ha ht.1
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # The actual escaped cold density in Euclidean coordinates -/
noncomputable section
open MeasureTheory Set
open BoltzmannNonuniqueness.VelocityWeight
namespace BoltzmannNonuniqueness.JetLattice
theorem measurableSet_spatialEnlargement (s₀ η : ℝ) (i : Label) :
MeasurableSet {z : ℝ × Velocity | z.2 ∈ spatialEnlargement s₀ η z.1 i} := by
change MeasurableSet
({z : ℝ × Velocity | transverse z.2-transverseShift i.lattice ∈
JetGeometry.enlargement η (JetGeometry.jetScale s₀ η i.annulus) i.positive} ∩
{z : ℝ × Velocity | |axial z.2-axialShift i.lattice| ≤ 1/8+2*z.1+1/16})
apply MeasurableSet.inter
· exact (Metric.isClosed_cthickening.measurableSet).preimage (by
unfold transverse transverseShift
fun_prop)
· exact measurableSet_le (by unfold axial; fun_prop) (by fun_prop)
end BoltzmannNonuniqueness.JetLattice
namespace BoltzmannNonuniqueness.JetCopyDatum
def CapApproximation.escapedTotal {s₀ η K α γ d₀ q T : ℝ} {N : ℕ}
(F : CapApproximation s₀ η K α γ d₀ q T N) (z : Published.KineticPhase) : ℝ :=
∑' i, escaped s₀ η z.1.1 N z.1.2
(fun j => F.cold j (z.1.1,(JetPeriodicDatum.spatialMap z.1.2,z.2))) i
theorem CapApproximation.escapedTotal_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.escapedTotal := by
classical
have hc := (F.cold_properties hs₀ hsmax hη hηmax hK hd₀ hq hT).1
apply Measurable.tsum
intro i
have hi : MeasurableSet {z : Published.KineticPhase |
z.1.2 ∉ JetLattice.spatialEnlargement s₀ η z.1.1 i} :=
((JetLattice.measurableSet_spatialEnlargement s₀ η i).preimage measurable_fst).compl
have hm : Measurable (fun z : Published.KineticPhase =>
F.cold i (z.1.1,(JetPeriodicDatum.spatialMap z.1.2,z.2))) := by
apply (hc i).comp
unfold JetPeriodicDatum.spatialMap transverse axial
fun_prop
by_cases hN : i.annulus < N
· change Measurable (fun z : Published.KineticPhase => if i.annulus < N ∧
JetLatticeTail.outside η (JetGeometry.jetScale s₀ η i.annulus) z.1.1 i.positive z.1.2 i.lattice
then F.cold i (z.1.1,(JetPeriodicDatum.spatialMap z.1.2,z.2)) else 0)
simp only [hN,true_and,outside_iff_not_mem]
exact hm.ite hi measurable_const
· change Measurable (fun z : Published.KineticPhase => if i.annulus < N ∧
JetLatticeTail.outside η (JetGeometry.jetScale s₀ η i.annulus) z.1.1 i.positive z.1.2 i.lattice
then F.cold i (z.1.1,(JetPeriodicDatum.spatialMap z.1.2,z.2)) else 0)
simp only [hN,false_and,ite_false]
exact measurable_const
theorem CapApproximation.escapedTotal_nonneg {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)
(z : Published.KineticPhase) : 0 ≤ F.escapedTotal z := by
have hc := (F.cold_properties hs₀ hsmax hη hηmax hK hd₀ hq hT).2.1
apply tsum_nonneg
intro i
unfold escaped
split_ifs
· exact hc i _
· exact le_rfl
theorem CapApproximation.escapedTotal_bound {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)
(hq : q < 2) (hT : 0 ≤ T) (hTmax : T ≤ 1/32)
(A : ℝ) {z : Published.KineticPhase} (ht : z.1.1 ∈ Ioc 0 T)
(hx : ∀ k, |z.1.2 k| ≤ 1) :
F.escapedTotal z ≤ JetEscapedEnvelope.constant s₀ η α K d₀
(JetEscapedEnvelope.exponent A)*z.1.1^A := by
have hc := F.cold_properties hs₀ hsmax hη hηmax hK hd₀.le hq hT
let f : JetLattice.Label → ℝ := fun j => F.cold j (z.1.1,(JetPeriodicDatum.spatialMap z.1.2,z.2))
have hfs : Summable f :=
((F.coldTotal_properties hs₀ hsmax hη hηmax hK hd₀.le hq hT).2 _).1
have henv (i : JetLattice.Label) : H q z.2*f i ≤
JetSupersolution.U η K α γ (JetGeometry.jetScale s₀ η i.annulus)
(d₀*JetGeometry.jetScale s₀ η i.annulus^10) z.1.1 i.positive
(JetSpatialBox.shifted z.1.2 i.lattice,z.2) := by
have he : (JetSpatialBox.shifted z.1.2 i.lattice,z.2) =
WeightedTranslation.shift (displacement i.lattice) (JetPeriodicDatum.spatialMap z.1.2,z.2) := rfl
rw [he]
exact F.cold_envelope hs₀ hsmax hη hηmax hK hα hγ hd₀ hsmall hq hT hTmax i ht
(JetPeriodicDatum.spatialMap z.1.2,z.2)
have hb := normalized_escaped_bound (γ := γ) hs₀ hsmax hη hηmax hK hα hαmax hγ hd₀ hd₀max ht.1
(ht.2.trans hTmax) hsmall A q N f z.1.2 z.2 hx
(fun i => hc.2.1 i _) hfs (fun i _ => henv i)
exact hb
end BoltzmannNonuniqueness.JetCopyDatum
end
end
section
/-! # Exact removal of the escaped colors from an actual cap approximation -/
noncomputable section
open MeasureTheory Set
open BoltzmannNonuniqueness.VelocityWeight
namespace BoltzmannNonuniqueness.JetCopyDatum
def CapApproximation.centralTotal {s₀ η K α γ d₀ q T : ℝ} {N : ℕ}
(F : CapApproximation s₀ η K α γ d₀ q T N) (z : Published.KineticPhase) : ℝ := by
classical
exact ∑' i, if i.annulus < N ∧ z.1.2 ∈ JetLattice.spatialEnlargement s₀ η z.1.1 i
then F.cold i (z.1.1,(JetPeriodicDatum.spatialMap z.1.2,z.2)) else 0
theorem CapApproximation.centralTotal_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.centralTotal := by
classical
have hc := (F.cold_properties hs₀ hsmax hη hηmax hK hd₀ hq hT).1
apply Measurable.tsum
intro i
have hm : Measurable (fun z : Published.KineticPhase =>
F.cold i (z.1.1,(JetPeriodicDatum.spatialMap z.1.2,z.2))) := by
apply (hc i).comp
unfold JetPeriodicDatum.spatialMap transverse axial
fun_prop
have hi : MeasurableSet {z : Published.KineticPhase |
z.1.2 ∈ JetLattice.spatialEnlargement s₀ η z.1.1 i} :=
(JetLattice.measurableSet_spatialEnlargement s₀ η i).preimage measurable_fst
by_cases hN : i.annulus < N
· simpa only [hN,true_and] using hm.ite hi measurable_const
· simp only [hN,false_and,ite_false]
exact measurable_const
theorem CapApproximation.coldTotal_eq_central_add_escaped {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)
(z : Published.KineticPhase) :
F.coldTotal (z.1.1,(JetPeriodicDatum.spatialMap z.1.2,z.2)) =
F.centralTotal z+F.escapedTotal z := by
classical
let f : JetLattice.Label → ℝ := fun i => F.cold i (z.1.1,(JetPeriodicDatum.spatialMap z.1.2,z.2))
let g : JetLattice.Label → ℝ := fun i =>
if i.annulus < N ∧ z.1.2 ∈ JetLattice.spatialEnlargement s₀ η z.1.1 i then f i else 0
let h : JetLattice.Label → ℝ := escaped s₀ η z.1.1 N z.1.2 f
have hc := F.cold_properties hs₀ hsmax hη hηmax hK hd₀ hq hT
have hfs : Summable f := (F.coldTotal_properties hs₀ hsmax hη hηmax hK hd₀ hq hT).2 _ |>.1
have hfn (i) : 0 ≤ f i := hc.2.1 i _
have hgn (i) : 0 ≤ g i := by
dsimp [g]
split_ifs
· exact hfn i
· exact le_rfl
have hgl (i) : g i ≤ f i := by dsimp [g]; split_ifs <;> simp only [le_refl,hfn]
have hhn (i) : 0 ≤ h i := by
dsimp [h,escaped]
split_ifs
· exact hfn i
· exact le_rfl
have hhl (i) : h i ≤ f i := by dsimp [h,escaped]; split_ifs <;> simp only [le_refl,hfn]
have hgs := Summable.of_nonneg_of_le hgn hgl hfs
have hhs := Summable.of_nonneg_of_le hhn hhl hfs
change (∑' i, f i) = (∑' i, g i)+(∑' i, h i)
rw [← hgs.tsum_add hhs]
apply tsum_congr
intro i
by_cases hN : i.annulus < N
· by_cases hi : z.1.2 ∈ JetLattice.spatialEnlargement s₀ η z.1.1 i
<;> simp [g,h,escaped,hN,hi,outside_iff_not_mem]
· have hz : f i = 0 := congrFun
(rebuilt_zero s₀ η K α γ d₀ q (N+1) (WeightedLocalControl.damping q (N+1) F.amplitude)
T N (fun u => (F.solution.value_bounds u).1) i hN) _
simp [g,h,escaped,hN,hz]
theorem CapApproximation.centralTotal_single {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)
(z : Published.KineticPhase) (ht : z.1.1 ≤ 1/32)
(i : JetLattice.Label) (hN : i.annulus < N)
(hi : z.1.2 ∈ JetLattice.spatialEnlargement s₀ η z.1.1 i) :
F.centralTotal z = F.cold i (z.1.1,(JetPeriodicDatum.spatialMap z.1.2,z.2)) := by
classical
unfold centralTotal
rw [tsum_eq_single i]
· simp only [hN,hi,and_self,ite_true]
· intro j hji
have hj : ¬(j.annulus < N ∧ z.1.2 ∈ JetLattice.spatialEnlargement s₀ η z.1.1 j) := by
rintro ⟨_,hj⟩
exact hji (JetLattice.common_point_label hs₀ hsmax hη hηmax ht hj hi)
simp only [hj,ite_false]
end BoltzmannNonuniqueness.JetCopyDatum
end
end
section
/-! # The actual cold density is bounded by the main free core and its remainder -/
noncomputable section
open MeasureTheory Set
open BoltzmannNonuniqueness.Published BoltzmannNonuniqueness.JetLattice
open BoltzmannNonuniqueness.VelocityWeight
namespace BoltzmannNonuniqueness.JetCopyDatum
theorem CapApproximation.cold_free_majorant_at_main {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) (hγ : 0 ≤ γ) (hd₀ : 0 < d₀)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq : q < 2) (hT : 0 ≤ T) (hTmax : T ≤ 1/32)
(z : KineticPhase) (ht : z.1.1 ∈ Ioc 0 T) (i : Label) (hi : i.annulus < N)
(hx : z.1.2 ∈ spatialEnlargement s₀ η z.1.1 i) :
H q z.2*F.coldTotal (z.1.1,(JetPeriodicDatum.spatialMap z.1.2,z.2)) ≤
JetFreeTransport.free η K α γ (JetGeometry.jetScale s₀ η i.annulus)
(d₀*JetGeometry.jetScale s₀ η i.annulus^10) z.1.1 i.positive
(WeightedTranslation.shift (displacement i.lattice) (JetPeriodicDatum.spatialMap z.1.2,z.2))+
JetSupersolution.epsilon K (JetGeometry.jetScale s₀ η i.annulus)
(d₀*JetGeometry.jetScale s₀ η i.annulus^10)*
JetBarrier.barrier η K α γ (JetGeometry.jetScale s₀ η i.annulus)
(d₀*JetGeometry.jetScale s₀ η i.annulus^10) z.1.1 i.positive
(WeightedTranslation.shift (displacement i.lattice) (JetPeriodicDatum.spatialMap z.1.2,z.2))+
H q z.2*F.escapedTotal z := by
rw [F.coldTotal_eq_central_add_escaped hs₀ hsmax hη hηmax hK hd₀.le hq hT z,
F.centralTotal_single hs₀ hsmax hη hηmax z (ht.2.trans hTmax) i hi hx,mul_add]
exact add_le_add (F.cold_envelope hs₀ hsmax hη hηmax hK hα hγ hd₀ hsmall hq hT hTmax
i ht (JetPeriodicDatum.spatialMap z.1.2,z.2)) le_rfl
theorem CapApproximation.coldTotal_eq_escaped_of_no_main {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) (z : KineticPhase)
(hx : ∀ i : Label, i.annulus < N → z.1.2 ∉ spatialEnlargement s₀ η z.1.1 i) :
F.coldTotal (z.1.1,(JetPeriodicDatum.spatialMap z.1.2,z.2)) = F.escapedTotal z := by
classical
rw [F.coldTotal_eq_central_add_escaped hs₀ hsmax hη hηmax hK hd₀ hq hT z]
have hz : F.centralTotal z = 0 := by
have hi : ∀ i : Label, ¬(i.annulus < N ∧ z.1.2 ∈ spatialEnlargement s₀ η z.1.1 i) :=
fun i hi => hx i hi.1 hi.2
simp only [CapApproximation.centralTotal,hi,ite_false,tsum_zero]
rw [hz,zero_add]
end BoltzmannNonuniqueness.JetCopyDatum
end
end
section
/-! # Only finitely many central colors remain in the centered cell -/
noncomputable section
open MeasureTheory Set
open BoltzmannNonuniqueness.VelocityWeight
namespace BoltzmannNonuniqueness.JetCopyDatum
def centralLabels (N : ℕ) : Finset JetLattice.Label :=
((Finset.range N).product (Finset.univ : Finset Bool)).image
(fun p => ⟨p.1,p.2,0⟩)
theorem mem_centralLabels {N : ℕ} {i : JetLattice.Label} :
i ∈ centralLabels N ↔ i.annulus < N ∧ i.lattice = 0 := by
classical
constructor
· intro hi
obtain ⟨p,hp,rfl⟩ := Finset.mem_image.mp hi
exact ⟨Finset.mem_range.mp (Finset.mem_product.mp hp).1,rfl⟩
· rintro ⟨hN,hl⟩
apply Finset.mem_image.mpr
refine ⟨(i.annulus,i.positive),Finset.mem_product.mpr
⟨Finset.mem_range.mpr hN,Finset.mem_univ _⟩,?_⟩
cases i
simp_all
theorem CapApproximation.centralTotal_finite {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)
(z : Published.KineticPhase) (ht : z.1.1 ≤ 1/32) (hx : z.1.2 ∈ TorusChart.cube) :
F.centralTotal z = ∑ i ∈ centralLabels N,
(JetLattice.spatialEnlargement s₀ η z.1.1 i).indicator
(fun _ => F.cold i (z.1.1,(JetPeriodicDatum.spatialMap z.1.2,z.2))) z.1.2 := by
classical
unfold centralTotal
rw [tsum_eq_sum (s := centralLabels N)]
· apply Finset.sum_congr rfl
intro i hi
simp only [(mem_centralLabels.mp hi).1,true_and,Set.indicator_apply]
· intro i hi
by_cases hm : i.annulus < N ∧ z.1.2 ∈ JetLattice.spatialEnlargement s₀ η z.1.1 i
· exact False.elim (hi (mem_centralLabels.mpr
⟨hm.1,enlargement_central_lattice hs₀ hsmax hη ht hx hm.2⟩))
· simp only [hm,ite_false]
theorem CapApproximation.centralTotal_finite_pairs {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)
(z : Published.KineticPhase) (ht : z.1.1 ≤ 1/32) (hx : z.1.2 ∈ TorusChart.cube) :
F.centralTotal z = ∑ j ∈ Finset.range N, ∑ a : Bool,
(JetLattice.spatialEnlargement s₀ η z.1.1 ⟨j,a,0⟩).indicator
(fun _ => F.cold ⟨j,a,0⟩ (z.1.1,(JetPeriodicDatum.spatialMap z.1.2,z.2))) z.1.2 := by
rw [F.centralTotal_finite hs₀ hsmax hη z ht hx,centralLabels,Finset.sum_image]
· exact Finset.sum_product _ _ _
· intro p _ q _ hpq
have h₁ := congrArg JetLattice.Label.annulus hpq
have h₂ := congrArg JetLattice.Label.positive hpq
exact Prod.ext h₁ h₂
end BoltzmannNonuniqueness.JetCopyDatum
end
end
section
/-! # The central cold sum on a fixed radial window has fixed mesh indices -/
noncomputable section
open MeasureTheory Set
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.centralTotal_mesh_window (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η)
{δ R : ℝ} (hδ : 0 < δ) (n : ℕ) (t : ℝ) (x v : Velocity)
(ht : S.radius (E.indices n)*t ≤ 1/32)
(hx : S.radius (E.indices n) • x ∈ TorusChart.cube)
(hlo : δ ≤ ‖transverse x‖) (hhi : ‖transverse x‖ ≤ R)
(hU : GeometricMesh.index R η < GeometricMesh.index (s₀/S.radius (E.indices n)) η) :
(F.approximation (E.indices n)).centralTotal
((S.radius (E.indices n)*t,S.radius (E.indices n) • x),v) =
∑ a : Bool, ∑ k ∈ Finset.Icc (GeometricMesh.index (δ/Real.exp η) η) (GeometricMesh.index R η),
if (E.coldLabel k a n).annulus < F.indices (E.indices n) then
(JetLattice.spatialEnlargement s₀ η (S.radius (E.indices n)*t) (E.coldLabel k a n)).indicator
(fun _ => (F.approximation (E.indices n)).cold (E.coldLabel k a n)
(S.radius (E.indices n)*t,(JetPeriodicDatum.spatialMap (S.radius (E.indices n) • x),v)))
(S.radius (E.indices n) • x)
else 0 := by
classical
let r := S.radius (E.indices n)
let N := F.indices (E.indices n)
rw [(F.approximation (E.indices n)).centralTotal_finite_pairs hs₀ hsmax hη _ ht hx,
Finset.sum_comm]
apply Finset.sum_congr rfl
intro a _
let f : ℕ → ℝ := fun j =>
(JetLattice.spatialEnlargement s₀ η (r*t) ⟨j,a,0⟩).indicator
(fun _ => (F.approximation (E.indices n)).cold ⟨j,a,0⟩
(r*t,(JetPeriodicDatum.spatialMap (r • x),v))) (r • x)
have hsupp (j : ℕ) (_hj : j < N) (hf : f j ≠ 0) :
GeometricMesh.jetMeshIndex s₀ η r j ∈
Finset.Icc (GeometricMesh.index (δ/Real.exp η) η) (GeometricMesh.index R η) := by
have hy : r • x ∈ JetLattice.spatialEnlargement s₀ η (r*t) ⟨j,a,0⟩ := by
by_contra h
exact hf (indicator_of_notMem h _)
have hz : JetLattice.transverseShift (0 : JetLattice.Lattice) = 0 := by
ext i
simp [JetLattice.transverseShift]
have hy₁ : transverse (r • x)-JetLattice.transverseShift 0 ∈
JetGeometry.enlargement η (JetGeometry.jetScale s₀ η j) a := hy.1
rw [hz,sub_zero] at hy₁
have hs : r • transverse x ∈ JetGeometry.enlargement η (JetGeometry.jetScale s₀ η j) a := hy₁
exact Finset.mem_Icc.mpr (JetGeometry.enlargement_mesh_window hs₀ hη (S.radius_pos hs₀ _)
hδ j a hs hlo hhi)
exact GeometricMesh.finite_sum_on_window s₀ η (fun m => S.radius (E.indices m)) n N
(GeometricMesh.index (δ/Real.exp η) η) (GeometricMesh.index R η) hU f hsupp
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Escaped cold mass vanishes on bounded positive-time dilation windows -/
noncomputable section
open MeasureTheory Filter Set
open scoped ENNReal 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}
def rescaledEscapedDensity (S : AttainedCapSequence F) (n : ℕ)
(z : Published.KineticPhase) : ℝ :=
S.radius n*H q z.2*(F.approximation n).escapedTotal
((S.radius n*z.1.1,S.radius n • z.1.2),z.2)
theorem rescaledEscapedDensity_measurable (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) :
Measurable (S.rescaledEscapedDensity n) := by
have hm := (F.approximation n).escapedTotal_measurable hs₀ hsmax hη hηmax hK hd₀ hq
(shrinkingHorizon_pos F.horizonScale_pos n).le
exact (((ChartKernel.measurable_H q).comp measurable_snd).const_mul _).mul
(hm.comp (by fun_prop))
theorem rescaledEscapedDensity_nonneg (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) (z : Published.KineticPhase) :
0 ≤ S.rescaledEscapedDensity n z :=
mul_nonneg (mul_nonneg (S.radius_pos hs₀ n).le (H_nonneg q z.2))
((F.approximation n).escapedTotal_nonneg hs₀ hsmax hη hηmax hK hd₀ hq
(shrinkingHorizon_pos F.horizonScale_pos n).le _)
theorem eventually_rescaledEscapedDensity_bound (S : AttainedCapSequence F)
(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)
(hq : q < 2) {κ : ℕ → ℕ} (hκ : StrictMono κ) {U : ℝ≥0∞}
(hU : Tendsto (fun n => S.normalizedHorizon (κ n)) atTop (𝓝 U))
{a A : ℝ} (ha : 0 < a) (hA : ENNReal.ofReal A < U) (R : ℝ) :
∀ᶠ n in atTop, ∀ z : Published.KineticPhase, z.1.1 ∈ Icc a A → ‖z.1.2‖ ≤ R →
|S.rescaledEscapedDensity (κ n) z| ≤
(JetEscapedEnvelope.constant s₀ η α K d₀ (JetEscapedEnvelope.exponent 0)*
S.radius (κ n))*H q z.2 := by
have hrlim : Tendsto (fun n => S.radius (κ n)*R) atTop (𝓝 0) := by
simpa only [Function.comp_def,zero_mul] using
((S.radius_tendsto_zero hs₀).comp hκ.tendsto_atTop).mul_const R
have hr := hrlim.eventually
(gt_mem_nhds (show (0:ℝ) < 1 by norm_num))
filter_upwards [hr,S.eventually_scaled_slab hs₀ hU hA] with n hn hslab
intro z ht hx
have hrpos := S.radius_pos hs₀ (κ n)
have hbound := (F.approximation (κ n)).escapedTotal_bound hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq (shrinkingHorizon_pos F.horizonScale_pos _).le
((shrinkingHorizon_le F.horizonScale_pos _).trans F.horizonScale_le) 0
(z := ((S.radius (κ n)*z.1.1,S.radius (κ n) • z.1.2),z.2))
⟨mul_pos hrpos (ha.trans_le ht.1),(hslab z.1.1 ⟨(ha.trans_le ht.1).le,ht.2⟩).2⟩
(fun k => ?_)
· simp only [Real.rpow_zero,mul_one] at hbound
rw [abs_of_nonneg (S.rescaledEscapedDensity_nonneg hs₀ hsmax hη hηmax hK hd₀.le hq _ _)]
exact (mul_le_mul_of_nonneg_left hbound (mul_nonneg hrpos.le (H_nonneg q z.2))).trans_eq
(by ring)
· calc
|(S.radius (κ n) • z.1.2) k| = S.radius (κ n)*|z.1.2 k| := by
change |S.radius (κ n)*z.1.2 k| = _
rw [abs_mul,abs_of_pos hrpos]
_ ≤ S.radius (κ n)*‖z.1.2‖ := mul_le_mul_of_nonneg_left
(by simpa only [Real.norm_eq_abs] using PiLp.norm_apply_le z.1.2 k) hrpos.le
_ ≤ S.radius (κ n)*R := mul_le_mul_of_nonneg_left hx hrpos.le
_ ≤ 1 := hn.le
def coldSlabSet (a A R : ℝ) : Set Published.KineticPhase :=
(Icc a A ×ˢ Metric.closedBall (0 : Velocity) R) ×ˢ univ
def coldSlabVolume (a A R : ℝ) : Measure Published.KineticPhase :=
((volume.restrict (Icc a A)).prod (volume.restrict (Metric.closedBall (0 : Velocity) R))).prod volume
theorem coldSlabVolume_eq (a A R : ℝ) :
coldSlabVolume a A R = volume.restrict (coldSlabSet a A R) := by
rw [coldSlabVolume,Measure.prod_restrict,← Measure.volume_eq_prod,
Measure.restrict_prod_eq_prod_univ,← Measure.volume_eq_prod]
rfl
theorem rescaledEscapedDensity_tendsto_zero (S : AttainedCapSequence F)
(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)
(hq : q < 2) {κ : ℕ → ℕ} (hκ : StrictMono κ) {U : ℝ≥0∞}
(hU : Tendsto (fun n => S.normalizedHorizon (κ n)) atTop (𝓝 U))
{a A : ℝ} (ha : 0 < a) (hA : ENNReal.ofReal A < U) (R : ℝ) :
Tendsto (fun n => eLpNorm (S.rescaledEscapedDensity (κ n)) 1 (coldSlabVolume a A R))
atTop (𝓝 0) := by
let C := JetEscapedEnvelope.constant s₀ η α K d₀ (JetEscapedEnvelope.exponent 0)
let _ : IsFiniteMeasure ((volume : Measure Velocity).restrict (Metric.closedBall 0 R)) :=
isFiniteMeasure_restrict.mpr (isCompact_closedBall (0 : Velocity) R).measure_lt_top.ne
have hi : Integrable (fun z : Published.KineticPhase => H q z.2) (coldSlabVolume a A R) :=
(integrable_H hq).comp_snd _
apply Compactness.tendsto_L1_of_vanishing_majorant
(fun n => (S.rescaledEscapedDensity_measurable hs₀ hsmax hη hηmax hK hd₀.le hq _).aestronglyMeasurable)
((ChartKernel.measurable_H q).comp measurable_snd) hi (ae_of_all _ (fun z => H_nonneg q z.2))
(c := fun n => C*S.radius (κ n))
· simpa only [Function.comp_def,mul_zero] using
((S.radius_tendsto_zero hs₀).comp hκ.tendsto_atTop).const_mul C
· filter_upwards [S.eventually_rescaledEscapedDensity_bound hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq hκ hU ha hA R] with n hn
rw [coldSlabVolume_eq]
filter_upwards [ae_restrict_mem ((measurableSet_Icc.prod measurableSet_closedBall).prod
MeasurableSet.univ)] with z hz
exact hn z hz.1.1 (by simpa only [Metric.mem_closedBall,dist_zero_right] using hz.1.2)
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # The actual cold dilation has the same local limit as its central colors -/
noncomputable section
open MeasureTheory Filter Set
open scoped ENNReal 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}
def rescaledCentralDensity (S : AttainedCapSequence F) (n : ℕ)
(z : Published.KineticPhase) : ℝ :=
S.radius n*H q z.2*(F.approximation n).centralTotal
((S.radius n*z.1.1,S.radius n • z.1.2),z.2)
theorem rescaledCentralDensity_measurable (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) :
Measurable (S.rescaledCentralDensity n) := by
have hm := (F.approximation n).centralTotal_measurable hs₀ hsmax hη hηmax hK hd₀ hq
(shrinkingHorizon_pos F.horizonScale_pos n).le
exact (((ChartKernel.measurable_H q).comp measurable_snd).const_mul _).mul
(hm.comp (by fun_prop))
theorem rescaledCold_sub_central (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) (z : Published.KineticPhase) :
S.rescaledColdDensity n ((z.1.1,JetPeriodicDatum.spatialMap z.1.2),z.2)-
S.rescaledCentralDensity n z = S.rescaledEscapedDensity n z := by
have h := (F.approximation n).coldTotal_eq_central_add_escaped hs₀ hsmax hη hηmax hK hd₀ hq
(shrinkingHorizon_pos F.horizonScale_pos n).le ((S.radius n*z.1.1,S.radius n • z.1.2),z.2)
have hmap : JetPeriodicDatum.spatialMap (S.radius n • z.1.2) =
S.radius n • JetPeriodicDatum.spatialMap z.1.2 := rfl
change S.radius n*H q z.2*(F.approximation n).coldTotal
(S.radius n*z.1.1,(S.radius n • JetPeriodicDatum.spatialMap z.1.2,z.2))-
S.radius n*H q z.2*(F.approximation n).centralTotal
((S.radius n*z.1.1,S.radius n • z.1.2),z.2) =
S.radius n*H q z.2*(F.approximation n).escapedTotal
((S.radius n*z.1.1,S.radius n • z.1.2),z.2)
rw [← hmap,h]
ring
theorem cold_central_difference_tendsto_zero (S : AttainedCapSequence F)
(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)
(hq : q < 2) {κ : ℕ → ℕ} (hκ : StrictMono κ) {U : ℝ≥0∞}
(hU : Tendsto (fun n => S.normalizedHorizon (κ n)) atTop (𝓝 U))
{a A : ℝ} (ha : 0 < a) (hA : ENNReal.ofReal A < U) (R : ℝ) :
Tendsto (fun n => eLpNorm (fun z : Published.KineticPhase =>
S.rescaledColdDensity (κ n) ((z.1.1,JetPeriodicDatum.spatialMap z.1.2),z.2)-
S.rescaledCentralDensity (κ n) z) 1 (coldSlabVolume a A R)) atTop (𝓝 0) := by
simp_rw [S.rescaledCold_sub_central hs₀ hsmax hη hηmax hK hd₀.le hq]
exact S.rescaledEscapedDensity_tendsto_zero hs₀ hsmax hη hηmax hK hα hαmax hγ hd₀ hd₀max
hsmall hq hκ hU ha hA R
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # The actual escaped cold density is uniformly bounded in every cell -/
noncomputable section
open MeasureTheory Set
open scoped ENNReal
open BoltzmannNonuniqueness.JetLattice BoltzmannNonuniqueness.JetGeometry
open BoltzmannNonuniqueness.JetPrototype BoltzmannNonuniqueness.VelocityWeight
namespace BoltzmannNonuniqueness.JetCopyDatum
theorem escaped_bound_global {s₀ η K α γ d₀ t : 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)
(hγ : 0 ≤ γ) (hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1) (ht : 0 < t) (htmax : t ≤ 1/32)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1) (A q : ℝ) (N : ℕ)
(f : Label → ℝ) (x v : Velocity)
(hf : ∀ i, 0 ≤ f i) (hfs : Summable f)
(hfU : ∀ i, i.annulus < N → f i ≤ JetSupersolution.U η K α γ
(jetScale s₀ η i.annulus) (d₀*jetScale s₀ η i.annulus^10) t i.positive
(JetSpatialBox.shifted x i.lattice,v)) :
(∑' i, escaped s₀ η t N x f i) ≤
JetEscapedEnvelope.constant s₀ η α K d₀ (JetEscapedEnvelope.exponent A)*t^A*VelocityWeight.H q v := by
classical
have hnon (i) : 0 ≤ escaped s₀ η t N x f i := by
unfold escaped
split_ifs
· exact hf i
· exact le_rfl
have hle (i) : escaped s₀ η t N x f i ≤ f i := by
unfold escaped
split_ifs
· exact le_rfl
· exact hf i
have hsum : Summable (escaped s₀ η t N x f) := Summable.of_nonneg_of_le hnon hle hfs
have h := JetEscapedEnvelope.real_power_global hs₀ hsmax hη hηmax hK hα hαmax hγ hd₀ hd₀max
ht htmax hsmall A q (fun j _ _ => j < N) (fun j a n => f ⟨j,a,n⟩) x v
(fun j a n hj => hfU ⟨j,a,n⟩ hj)
have he : (∑' i, ENNReal.ofReal (escaped s₀ η t N x f i)) =
JetEscapedEnvelope.escapedSum s₀ η t x (fun j _ _ => j < N) (fun j a n => f ⟨j,a,n⟩) := by
rw [tsum_labels]
unfold escaped JetEscapedEnvelope.escapedSum
simp only [Set.indicator_apply,Set.mem_ofPred_eq,apply_ite ENNReal.ofReal,ENNReal.ofReal_zero]
rw [← he, ← ENNReal.ofReal_tsum_of_nonneg hnon hsum] at h
have hB : 0 ≤ JetEscapedEnvelope.constant s₀ η α K d₀ (JetEscapedEnvelope.exponent A)*
t^A*VelocityWeight.H q v := by
have hc := JetEscapedEnvelope.constant_nonneg hs₀ hK hd₀ η α (JetEscapedEnvelope.exponent A)
exact mul_nonneg (mul_nonneg hc (Real.rpow_nonneg ht.le A)) (VelocityWeight.H_nonneg q v)
simpa only [ENNReal.toReal_ofReal (tsum_nonneg hnon),ENNReal.toReal_ofReal hB] using
ENNReal.toReal_mono ENNReal.ofReal_ne_top h
theorem normalized_escaped_bound_global {s₀ η K α γ d₀ t : 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) (hγ : 0 ≤ γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1) (ht : 0 < t) (htmax : t ≤ 1/32)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1) (A q : ℝ) (N : ℕ)
(f : Label → ℝ) (x v : Velocity)
(hf : ∀ i, 0 ≤ f i) (hfs : Summable f)
(hfU : ∀ i, i.annulus < N → VelocityWeight.H q v*f i ≤ JetSupersolution.U η K α γ
(jetScale s₀ η i.annulus) (d₀*jetScale s₀ η i.annulus^10) t i.positive
(JetSpatialBox.shifted x i.lattice,v)) :
(∑' i, escaped s₀ η t N x f i) ≤
JetEscapedEnvelope.constant s₀ η α K d₀ (JetEscapedEnvelope.exponent A)*t^A := by
have h := escaped_bound_global hs₀ hsmax hη hηmax hK hα hαmax hγ hd₀ hd₀max ht htmax hsmall A q N
(fun i => VelocityWeight.H q v*f i) x v
(fun i => mul_nonneg (VelocityWeight.H_nonneg q v) (hf i))
(hfs.mul_left (VelocityWeight.H q v)) hfU
have he (i) : escaped s₀ η t N x (fun j => VelocityWeight.H q v*f j) i =
VelocityWeight.H q v*escaped s₀ η t N x f i := by
unfold escaped
split_ifs <;> simp only [mul_zero]
simp_rw [he] at h
rw [tsum_mul_left] at h
have hh : VelocityWeight.H q v*(∑' i, escaped s₀ η t N x f i) ≤
VelocityWeight.H q v*(JetEscapedEnvelope.constant s₀ η α K d₀ (JetEscapedEnvelope.exponent A)*t^A) :=
h.trans_eq (mul_comm _ _)
exact (mul_le_mul_iff_of_pos_left (VelocityWeight.H_pos q v)).mp hh
theorem CapApproximation.escapedTotal_bound_global {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)
(hq : q < 2) (hT : 0 ≤ T) (hTmax : T ≤ 1/32)
(A : ℝ) {z : Published.KineticPhase} (ht : z.1.1 ∈ Ioc 0 T) :
F.escapedTotal z ≤ JetEscapedEnvelope.constant s₀ η α K d₀
(JetEscapedEnvelope.exponent A)*z.1.1^A := by
have hc := F.cold_properties hs₀ hsmax hη hηmax hK hd₀.le hq hT
let f : JetLattice.Label → ℝ := fun j => F.cold j (z.1.1,(JetPeriodicDatum.spatialMap z.1.2,z.2))
have hfs : Summable f :=
((F.coldTotal_properties hs₀ hsmax hη hηmax hK hd₀.le hq hT).2 _).1
have henv (i : JetLattice.Label) : H q z.2*f i ≤
JetSupersolution.U η K α γ (JetGeometry.jetScale s₀ η i.annulus)
(d₀*JetGeometry.jetScale s₀ η i.annulus^10) z.1.1 i.positive
(JetSpatialBox.shifted z.1.2 i.lattice,z.2) := by
have he : (JetSpatialBox.shifted z.1.2 i.lattice,z.2) =
WeightedTranslation.shift (displacement i.lattice) (JetPeriodicDatum.spatialMap z.1.2,z.2) := rfl
rw [he]
exact F.cold_envelope hs₀ hsmax hη hηmax hK hα hγ hd₀ hsmall hq hT hTmax i ht
(JetPeriodicDatum.spatialMap z.1.2,z.2)
have hb := normalized_escaped_bound_global (γ := γ) hs₀ hsmax hη hηmax hK hα hαmax hγ hd₀ hd₀max ht.1
(ht.2.trans hTmax) hsmall A q N f z.1.2 z.2
(fun i => hc.2.1 i _) hfs (fun i _ => henv i)
exact hb
end BoltzmannNonuniqueness.JetCopyDatum
end
end
section
/-! # Global almost-everywhere majorants in the Euclidean averaging coordinates -/
noncomputable section
open MeasureTheory Filter Set
open scoped Topology ENNReal
open BoltzmannNonuniqueness.WeightedLocal 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 euclideanHot_measurable (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) :
Measurable (S.euclideanHot n) :=
EuclideanFlight.density_measurable (S.normalizedHot_measurable hs₀ hsmax hη hηmax hK hd₀ hq n) q
theorem euclideanHotSource_measurable (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) :
Measurable (S.euclideanHotSource n) := by
have hm := (F.approximation n).hotNetSource_measurable hs₀ hsmax hη hηmax hK hd₀ hq
(shrinkingHorizon_pos F.horizonScale_pos n).le
have hk : Measurable (fun z : Published.KineticPhase =>
(S.radius n*z.1.1,PositiveIntegral.scalePhase (S.radius n) (EuclideanFlight.phaseEquiv (z.1.2,z.2)))) := by
have hp : Measurable (fun z : Published.KineticPhase => EuclideanFlight.phaseEquiv (z.1.2,z.2)) :=
EuclideanFlight.phaseEquiv.measurable.comp (measurable_fst.snd.prodMk measurable_snd)
unfold PositiveIntegral.scalePhase
have hs : Measurable (fun z : Published.KineticPhase =>
S.radius n • (EuclideanFlight.phaseEquiv (z.1.2,z.2)).1) := by
have hc : Measurable (fun _ : Published.KineticPhase => S.radius n) := measurable_const
exact hc.smul hp.fst
exact (measurable_fst.fst.const_mul _).prodMk (hs.prodMk hp.snd)
exact ((ChartKernel.measurable_H q).comp measurable_snd).mul (hm.comp hk)
theorem eventually_euclideanHot_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) {κ : ℕ → ℕ} {U : ℝ≥0∞}
(hU : Tendsto (fun n => S.normalizedHorizon (κ n)) atTop (𝓝 U))
{A : ℝ} (hA : ENNReal.ofReal A < U) :
∀ᶠ n in atTop, ∀ᵐ z ∂(volume : Measure Published.KineticPhase), z.1.1 ∈ Icc 0 A →
0 ≤ S.euclideanHot (κ n) z ∧ S.euclideanHot (κ n) z ≤ (A+1)*H q z.2 := by
filter_upwards [S.eventually_scaled_slab hs₀ hU hA] with n hslab
let Fn := F.approximation (κ n)
have hr := S.radius_pos hs₀ (κ n)
have hcap := Fn.hot_spacetime_cap hs₀ hsmax hη hηmax hK hd₀ hq
(shrinkingHorizon_pos F.horizonScale_pos _).le
have hn := (Fn.hot_properties hs₀ hsmax hη hηmax hK hd₀ hq
(shrinkingHorizon_pos F.horizonScale_pos _).le).2.1
have hp := (ColdDilationMeasure.spacetime_dilation_quasiMeasurePreserving hr).ae hcap
filter_upwards [EuclideanFlight.kineticMap_measurePreserving.quasiMeasurePreserving.ae hp]
with z hz ht
have hb := hz (hslab z.1.1 ht)
have hδ : DatumBounds.scale s₀ η (F.indices (κ n)+1) ≤ S.radius (κ n) := by
dsimp [radius]
linarith [(S.time_mem (κ n)).1]
have hu : S.normalizedHot (κ n) (EuclideanFlight.kineticMap z) ≤ A+1 := by
apply (div_le_iff₀ hr).mpr
have ht' := mul_le_mul_of_nonneg_left ht.2 hr.le
change Fn.hot (S.radius (κ n)*z.1.1,
(S.radius (κ n) • (EuclideanFlight.phaseEquiv (z.1.2,z.2)).1,z.2)) ≤
S.radius (κ n)*z.1.1+DatumBounds.scale s₀ η (F.indices (κ n)+1) at hb
change Fn.hot (S.radius (κ n)*z.1.1,
(S.radius (κ n) • (EuclideanFlight.phaseEquiv (z.1.2,z.2)).1,z.2)) ≤ _
nlinarith
have hl : 0 ≤ S.normalizedHot (κ n) (EuclideanFlight.kineticMap z) := div_nonneg (hn _) hr.le
change 0 ≤ H q z.2*S.normalizedHot (κ n) (EuclideanFlight.kineticMap z) ∧
H q z.2*S.normalizedHot (κ n) (EuclideanFlight.kineticMap z) ≤ (A+1)*H q z.2
exact ⟨mul_nonneg (H_nonneg q z.2) hl,
(mul_le_mul_of_nonneg_left hu (H_nonneg q z.2)).trans_eq (mul_comm _ _)⟩
theorem eventually_euclideanHotSource_bound (hcarleman : Published.GPV2009CarlemanInput)
(S : AttainedCapSequence F)
(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) {κ : ℕ → ℕ} (hκ : StrictMono κ) {U : ℝ≥0∞}
(hU : Tendsto (fun n => S.normalizedHorizon (κ n)) atTop (𝓝 U))
{a A : ℝ} (ha : 0 < a) (haA : a ≤ A) (hA : ENNReal.ofReal A < U) :
∀ᶠ n in atTop, ∀ᵐ z ∂(volume : Measure Published.KineticPhase), z.1.1 ∈ Icc a A →
|S.euclideanHotSource (κ n) z| ≤ sourceEnvelope s₀ η K α γ d₀ q a A z.2*H q z.2 := by
filter_upwards [S.eventually_rescaledHotSource_abs hcarleman hs₀ hsmax hη hηmax hK hα
hαmax hγ hd₀ hd₀max hsmall hq₁ hq₂ hκ hU ha haA hA] with n hn
filter_upwards [EuclideanFlight.kineticMap_measurePreserving.quasiMeasurePreserving.ae hn]
with z hz ht
change |H q z.2*S.rescaledHotSource (κ n) (EuclideanFlight.kineticMap z)| ≤ _
rw [abs_mul,abs_of_nonneg (H_nonneg q z.2)]
exact (mul_le_mul_of_nonneg_left (hz ht) (H_nonneg q z.2)).trans_eq (mul_comm _ _)
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Uniform positive-time bounds for the actual cold-label averages -/
noncomputable section
open MeasureTheory Set Filter
open scoped ENNReal Topology
open BoltzmannNonuniqueness.VelocityWeight BoltzmannNonuniqueness.VelocityMoment
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.coldLabelDensity_le_total (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) (k : ℤ) (a : Bool) (n : ℕ) (t : ℝ)
(x : JetPrototype.Space) (v : Velocity) :
E.coldLabelDensity k a n t (x,v) ≤ S.rescaledColdDensity (E.indices n) ((t,x),v) := by
have hc := (F.approximation (E.indices n)).cold_properties hs₀ hsmax hη hηmax hK hd₀ hq
(shrinkingHorizon_pos F.horizonScale_pos _).le
let u := (S.radius (E.indices n)*t,(S.radius (E.indices n) • x,v))
have hs := ((F.approximation (E.indices n)).coldTotal_properties hs₀ hsmax hη hηmax hK hd₀ hq
(shrinkingHorizon_pos F.horizonScale_pos _).le).2 u
have hb := hs.1.le_tsum (E.coldLabel k a n) (fun i _ => hc.2.1 i u)
have hp := mul_le_mul_of_nonneg_left hb
(mul_nonneg (S.radius_pos hs₀ (E.indices n)).le (H_nonneg q v))
convert! hp using 1
· simp only [coldLabelDensity,mul_assoc,u]
theorem HotLimitExtraction.eventually_coldLabelAverage_bound (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) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1) (hq : q < 2)
{a A B : ℝ} (ha : 0 < a) (hA : ENNReal.ofReal A < E.horizon) (hB : 0 ≤ B)
{ψ : Velocity → ℝ} (hψB : ∀ v, |ψ v| ≤ B) :
∀ᶠ n in atTop, ∀ t ∈ Icc a A, ∀ k σ x,
|E.coldLabelAverage k σ n t ψ x| ≤ B*
(escapedConstant s₀ η K α d₀*hotConstant q+JetEnvelopeGain.momentConstant K α γ/a) := by
have hM := S.eventually_rescaledColdDensity_moment hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq E.indices_strict E.horizon_limit ha hA
filter_upwards [hM] with n hn
intro t ht k σ x
have hnon (v) := (E.coldLabelDensity_bounds hs₀ hsmax hη hηmax hK hd₀.le hq k σ n t (x,v)).1
have hm : Measurable (fun v => E.coldLabelDensity k σ n t (x,v)) :=
(E.coldLabelDensity_measurable hs₀ hsmax hη hηmax hK hd₀.le hq k σ n t).comp
(measurable_const.prodMk measurable_id)
have hmom : VelocityMoment.moment (fun v => E.coldLabelDensity k σ n t (x,v)) ≤
ENNReal.ofReal (escapedConstant s₀ η K α d₀*hotConstant q+
JetEnvelopeGain.momentConstant K α γ/a) := by
apply le_trans _ (hn t ht x)
apply lintegral_mono
intro v
apply ENNReal.ofReal_le_ofReal
exact mul_le_mul_of_nonneg_left
(E.coldLabelDensity_le_total hs₀ hsmax hη hηmax hK hd₀.le hq k σ n t x v)
(VelocityMoment.weight_pos v).le
have hM0 : 0 ≤ escapedConstant s₀ η K α d₀*hotConstant q+
JetEnvelopeGain.momentConstant K α γ/a := add_nonneg
(mul_nonneg (JetEscapedEnvelope.constant_nonneg hs₀ hK hd₀ η α _) (hotConstant_nonneg q))
(div_nonneg (JetEnvelopeGain.momentConstant_nonneg hK α γ) ha.le)
exact VelocityMoment.average_le_of_moment_bound hm hnon hB hM0 hmom hψB
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Joint regularity and uniform bounds for the full cold velocity averages -/
noncomputable section
open MeasureTheory Set Filter
open scoped ENNReal Topology
open BoltzmannNonuniqueness.VelocityWeight BoltzmannNonuniqueness.VelocityMoment
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
def coldAverage (S : AttainedCapSequence F) (n : ℕ) (ψ : Velocity → ℝ)
(x : ℝ × JetPrototype.Space) : ℝ :=
∫ v, ψ v*S.rescaledColdDensity n (x,v)
theorem coldAverage_measurable (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)
{ψ : Velocity → ℝ} (hψ : Measurable ψ) : Measurable (S.coldAverage n ψ) := by
have hm := (hψ.comp measurable_snd).mul
(S.rescaledColdDensity_measurable hs₀ hsmax hη hηmax hK hd₀ hq n)
exact hm.stronglyMeasurable.integral_prod_right'.measurable
theorem coldAverage_global_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)
{B : ℝ} {ψ : Velocity → ℝ} (hψB : ∀ v, |ψ v| ≤ B) (x : ℝ × JetPrototype.Space) :
|S.coldAverage n ψ x| ≤
(B*(S.radius n*(2*(F.approximation n).amplitude)))*(∫ v, H q v) := by
have hB : 0 ≤ B := (abs_nonneg (ψ 0)).trans (hψB 0)
have hb := norm_integral_le_of_norm_le
(f := fun v => ψ v*S.rescaledColdDensity n (x,v))
((integrable_H hq).const_mul (B*(S.radius n*(2*(F.approximation n).amplitude)))) ?_
· simpa only [Real.norm_eq_abs,integral_const_mul,coldAverage] using hb
· filter_upwards [] with v
have hd := S.rescaledColdDensity_bounds hs₀ hsmax hη hηmax hK hd₀ hq n (x,v)
rw [Real.norm_eq_abs,abs_mul,abs_of_nonneg hd.1]
exact (mul_le_mul (hψB v) hd.2 hd.1 hB).trans_eq (by ring)
theorem coldAverage_integrable (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)
{B : ℝ} {ψ : Velocity → ℝ} (hψ : Measurable ψ) (hψB : ∀ v, |ψ v| ≤ B)
(ρ : Measure (ℝ × JetPrototype.Space)) [IsFiniteMeasure ρ] :
Integrable (S.coldAverage n ψ) ρ :=
Integrable.of_bound (S.coldAverage_measurable hs₀ hsmax hη hηmax hK hd₀ hq n hψ).aestronglyMeasurable
_ (ae_of_all _ (S.coldAverage_global_bound hs₀ hsmax hη hηmax hK hd₀ hq n hψB))
theorem HotLimitExtraction.eventually_coldAverage_bound {S : AttainedCapSequence F}
(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) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1) (hq : q < 2)
{a A B : ℝ} (ha : 0 < a) (hA : ENNReal.ofReal A < E.horizon) (hB : 0 ≤ B)
{ψ : Velocity → ℝ} (hψB : ∀ v, |ψ v| ≤ B) :
∀ᶠ n in atTop, ∀ t ∈ Icc a A, ∀ x,
|S.coldAverage (E.indices n) ψ (t,x)| ≤ B*
(escapedConstant s₀ η K α d₀*hotConstant q+JetEnvelopeGain.momentConstant K α γ/a) := by
filter_upwards [S.eventually_rescaledColdDensity_moment hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq E.indices_strict E.horizon_limit ha hA] with n hn
intro t ht x
have hm : Measurable (fun v => S.rescaledColdDensity (E.indices n) ((t,x),v)) :=
(S.rescaledColdDensity_measurable hs₀ hsmax hη hηmax hK hd₀.le hq (E.indices n)).comp
(measurable_const.prodMk measurable_id)
have hM0 : 0 ≤ escapedConstant s₀ η K α d₀*hotConstant q+
JetEnvelopeGain.momentConstant K α γ/a := add_nonneg
(mul_nonneg (JetEscapedEnvelope.constant_nonneg hs₀ hK hd₀ η α _) (hotConstant_nonneg q))
(div_nonneg (JetEnvelopeGain.momentConstant_nonneg hK α γ) ha.le)
exact average_le_of_moment_bound hm
(fun v => (S.rescaledColdDensity_bounds hs₀ hsmax hη hηmax hK hd₀.le hq _ ((t,x),v)).1)
hB hM0 (hn t ht x) hψB
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Joint time-space regularity of actual cold-label velocity averages -/
noncomputable section
open MeasureTheory
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.coldLabelDensity_joint_measurable (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) (k : ℤ) (a : Bool) (n : ℕ) :
Measurable (fun z : (ℝ × JetPrototype.Space) × Velocity =>
E.coldLabelDensity k a n z.1.1 (z.1.2,z.2)) := by
have hc := (F.approximation (E.indices n)).cold_properties hs₀ hsmax hη hηmax hK hd₀ hq
(shrinkingHorizon_pos F.horizonScale_pos _).le
have hp : Measurable (fun z : (ℝ × JetPrototype.Space) × Velocity =>
(S.radius (E.indices n)*z.1.1,(S.radius (E.indices n) • z.1.2,z.2))) := by fun_prop
exact (((ChartKernel.measurable_H q).comp measurable_snd).mul
((hc.1 (E.coldLabel k a n)).comp hp)).const_mul _
theorem HotLimitExtraction.coldLabelAverage_joint_measurable (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) (k : ℤ) (a : Bool) (n : ℕ)
{ψ : Velocity → ℝ} (hψ : Measurable ψ) :
Measurable (fun z : ℝ × JetPrototype.Space => E.coldLabelAverage k a n z.1 ψ z.2) := by
have hm := (hψ.comp measurable_snd).mul
(E.coldLabelDensity_joint_measurable hs₀ hsmax hη hηmax hK hd₀ hq k a n)
exact hm.stronglyMeasurable.integral_prod_right'.measurable
theorem HotLimitExtraction.coldLabelAverage_global_bound (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) (k : ℤ) (a : Bool) (n : ℕ)
{B : ℝ} {ψ : Velocity → ℝ} (hψB : ∀ v, |ψ v| ≤ B)
(t : ℝ) (x : JetPrototype.Space) :
|E.coldLabelAverage k a n t ψ x| ≤
(B*(S.radius (E.indices n)*(2*(F.approximation (E.indices n)).amplitude)))*(∫ v, H q v) := by
have hB : 0 ≤ B := (abs_nonneg (ψ 0)).trans (hψB 0)
have hb := norm_integral_le_of_norm_le
(f := fun v => ψ v*E.coldLabelDensity k a n t (x,v))
((integrable_H hq).const_mul (B*(S.radius (E.indices n)*(2*(F.approximation (E.indices n)).amplitude)))) ?_
· simpa only [Real.norm_eq_abs,integral_const_mul,coldLabelAverage] using hb
· filter_upwards [] with v
have hd := E.coldLabelDensity_bounds hs₀ hsmax hη hηmax hK hd₀ hq k a n t (x,v)
rw [Real.norm_eq_abs,abs_mul,abs_of_nonneg hd.1]
exact (mul_le_mul (hψB v) hd.2 hd.1 hB).trans_eq (by ring)
theorem HotLimitExtraction.coldLabelAverage_joint_integrable (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) (k : ℤ) (a : Bool) (n : ℕ)
{B : ℝ} {ψ : Velocity → ℝ} (hψ : Measurable ψ) (hψB : ∀ v, |ψ v| ≤ B)
(ρ : Measure (ℝ × JetPrototype.Space)) [IsFiniteMeasure ρ] :
Integrable (fun z => E.coldLabelAverage k a n z.1 ψ z.2) ρ :=
Integrable.of_bound
(E.coldLabelAverage_joint_measurable hs₀ hsmax hη hηmax hK hd₀ hq k a n hψ).aestronglyMeasurable
_ (ae_of_all _ (fun z => E.coldLabelAverage_global_bound hs₀ hsmax hη hηmax hK hd₀ hq k a n hψB z.1 z.2))
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # A finite window of actual cold labels -/
noncomputable section
open MeasureTheory Set
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.meshLabels (E : HotLimitExtraction S) (n : ℕ) (L U : ℤ) : Finset JetLattice.Label :=
((Finset.Icc L U).product (Finset.univ : Finset Bool)).image (fun p => E.coldLabel p.1 p.2 n)
def HotLimitExtraction.meshCold (E : HotLimitExtraction S) (n : ℕ) (L U : ℤ)
(u : ℝ × JetPrototype.Phase) : ℝ :=
∑ i ∈ E.meshLabels n L U, if i.annulus < F.indices (E.indices n) then
(F.approximation (E.indices n)).cold i u else 0
theorem HotLimitExtraction.meshCold_sum (E : HotLimitExtraction S) (n : ℕ) (L U : ℤ)
(hU : U < GeometricMesh.index (s₀/S.radius (E.indices n)) η) (u : ℝ × JetPrototype.Phase) :
E.meshCold n L U u = ∑ a : Bool, ∑ k ∈ Finset.Icc L U,
if (E.coldLabel k a n).annulus < F.indices (E.indices n) then
(F.approximation (E.indices n)).cold (E.coldLabel k a n) u else 0 := by
classical
unfold meshCold meshLabels
rw [Finset.sum_image]
· exact (Finset.sum_product _ _ _).trans Finset.sum_comm
· intro p hp q hq he
have hj := congrArg JetLattice.Label.annulus he
have ha := congrArg JetLattice.Label.positive he
have hpU := (Finset.mem_Icc.mp (Finset.mem_product.mp hp).1).2.trans_lt hU
have hqU := (Finset.mem_Icc.mp (Finset.mem_product.mp hq).1).2.trans_lt hU
have hh := congrArg (GeometricMesh.jetMeshIndex s₀ η (S.radius (E.indices n))) hj
change GeometricMesh.jetMeshIndex s₀ η (S.radius (E.indices n))
(GeometricMesh.jetIndex s₀ η (fun m => S.radius (E.indices m)) p.1 n) =
GeometricMesh.jetMeshIndex s₀ η (S.radius (E.indices n))
(GeometricMesh.jetIndex s₀ η (fun m => S.radius (E.indices m)) q.1 n) at hh
rw [GeometricMesh.meshIndex_at_jetIndex s₀ η (fun m => S.radius (E.indices m)) n hpU,
GeometricMesh.meshIndex_at_jetIndex s₀ η (fun m => S.radius (E.indices m)) n hqU] at hh
exact Prod.ext hh ha
theorem HotLimitExtraction.meshCold_le_total (E : HotLimitExtraction S)
(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) (L U : ℤ) (u : ℝ × JetPrototype.Phase) :
E.meshCold n L U u ≤ (F.approximation (E.indices n)).coldTotal u := by
classical
have hc := (F.approximation (E.indices n)).cold_properties hs₀ hsmax hη hηmax hK hd₀ hq
(shrinkingHorizon_pos F.horizonScale_pos _).le
have hs := ((F.approximation (E.indices n)).coldTotal_properties hs₀ hsmax hη hηmax hK hd₀ hq
(shrinkingHorizon_pos F.horizonScale_pos _).le).2 u
apply (Finset.sum_le_sum (s := E.meshLabels n L U) (fun i _ => ?_)).trans
(hs.1.sum_le_tsum _ (fun i _ => hc.2.1 i u))
by_cases hi : i.annulus < F.indices (E.indices n)
· exact (ite_eq_left hi).le
· rw [ite_eq_right hi]
exact hc.2.1 i u
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
end OAI