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import OAI.MathematicalPhysics.Boltzmann.Branching.MarginalUniformIntegrability
import OAI.MathematicalPhysics.Boltzmann.Compactness.EntropyUniformIntegrability
import OAI.MathematicalPhysics.Boltzmann.Compactness.UniformIntegrability
import OAI.MathematicalPhysics.Boltzmann.Model
import Mathlib.Analysis.Calculus.BumpFunction.FiniteDimension
import Mathlib.Analysis.Calculus.BumpFunction.Normed
namespace OAI
section
/-! # Uniform integrability of the linear velocity moment from entropy and energy -/
noncomputable section
open MeasureTheory Set Filter
open scoped ENNReal NNReal
namespace BoltzmannNonuniqueness.PeriodicApproximation
variable {X : Type*} [MeasurableSpace X]
def linearMoment (f : X × Velocity → ℝ) (p : X × Velocity) : ℝ := (1+‖p.2‖)*f p
def velocityLinearCut (R : ℝ) (f : X × Velocity → ℝ) (p : X × Velocity) : ℝ :=
if ‖p.2‖ ≤ R then linearMoment f p else 0
theorem linearMoment_measurable {f : X × Velocity → ℝ} (hf : Measurable f) :
Measurable (linearMoment f) := (measurable_const.add measurable_snd.norm).mul hf
theorem velocityLinearCut_measurable (R : ℝ) {f : X × Velocity → ℝ} (hf : Measurable f) :
Measurable (velocityLinearCut R f) := (linearMoment_measurable hf).ite
(measurableSet_le measurable_snd.norm measurable_const) measurable_const
theorem linearMoment_integrable {μ : Measure (X × Velocity)} {f : X × Velocity → ℝ}
(hfm : Measurable f) (hf : ∀ p, 0 ≤ f p) (hi : Integrable (entropyGauge f) μ) :
Integrable (linearMoment f) μ := by
apply (hi.const_mul 2).mono' (linearMoment_measurable hfm).aestronglyMeasurable
filter_upwards [] with p
change ‖(1+‖p.2‖)*f p‖ ≤ _
rw [Real.norm_of_nonneg (mul_nonneg (by positivity) (hf p))]
have h : 1+‖p.2‖ ≤ 2*(1+‖p.2‖^2+|Real.log (f p)|) := by
nlinarith [sq_nonneg (‖p.2‖-1),abs_nonneg (Real.log (f p))]
simpa only [linearMoment,entropyGauge,mul_assoc,mul_left_comm,mul_comm] using
mul_le_mul_of_nonneg_right h (hf p)
omit [MeasurableSpace X] in
theorem velocityLinearCut_error {R : ℝ} (hR : 0 < R) {f : X × Velocity → ℝ}
(hf : ∀ p, 0 ≤ f p) (p : X × Velocity) :
|linearMoment f p-velocityLinearCut R f p| ≤ 2*entropyGauge f p/R := by
by_cases hp : ‖p.2‖ ≤ R
· simp only [velocityLinearCut,ite_eq_left hp,sub_self,abs_zero]
exact div_nonneg (mul_nonneg (by norm_num) (entropyGauge_nonneg hf p)) hR.le
· have hr : R ≤ ‖p.2‖ := (lt_of_not_ge hp).le
simp only [velocityLinearCut,ite_eq_right hp,sub_zero,linearMoment]
rw [abs_of_nonneg (mul_nonneg (by positivity) (hf p))]
apply (le_div_iff₀ hR).mpr
have hcoeff : (1+‖p.2‖)*R ≤ 2*(1+‖p.2‖^2+|Real.log (f p)|) := by
have hh := mul_le_mul_of_nonneg_left hr (show 0 ≤ 1+‖p.2‖ by positivity)
nlinarith [sq_nonneg (‖p.2‖-1),abs_nonneg (Real.log (f p))]
simpa only [entropyGauge,mul_assoc,mul_left_comm,mul_comm] using
mul_le_mul_of_nonneg_right hcoeff (hf p)
theorem velocityLinearCut_integrable {μ : Measure (X × Velocity)} (R : ℝ)
{f : X × Velocity → ℝ} (hfm : Measurable f) (hf : ∀ p, 0 ≤ f p)
(hi : Integrable (entropyGauge f) μ) : Integrable (velocityLinearCut R f) μ := by
apply (linearMoment_integrable hfm hf hi).mono'
(velocityLinearCut_measurable R hfm).aestronglyMeasurable
filter_upwards [] with p
have hn : 0 ≤ linearMoment f p := mul_nonneg (by positivity) (hf p)
by_cases hp : ‖p.2‖ ≤ R
· rw [velocityLinearCut,ite_eq_left hp,Real.norm_of_nonneg hn]
· rw [velocityLinearCut,ite_eq_right hp,norm_zero]
exact hn
theorem velocityLinearCut_L1_error {μ : Measure (X × Velocity)} {R C : ℝ} (hR : 0 < R)
{f : X × Velocity → ℝ} (hfm : Measurable f) (hf : ∀ p, 0 ≤ f p)
(hi : Integrable (entropyGauge f) μ) (hb : (∫ p, entropyGauge f p ∂μ) ≤ C) :
eLpNorm (fun p => linearMoment f p-velocityLinearCut R f p) 1 μ ≤ ENNReal.ofReal (2*C/R) := by
have he := (linearMoment_integrable hfm hf hi).sub (velocityLinearCut_integrable R hfm hf hi)
change Integrable (fun p => linearMoment f p-velocityLinearCut R f p) μ at he
rw [eLpNorm_one_eq_lintegral_enorm he.aestronglyMeasurable,
← ofReal_integral_norm_eq_lintegral_enorm he]
apply ENNReal.ofReal_le_ofReal
calc
_ ≤ ∫ p, 2*entropyGauge f p/R ∂μ :=
integral_mono he.norm ((hi.const_mul 2).div_const R) (fun p => by
simpa only [Real.norm_eq_abs] using velocityLinearCut_error hR hf p)
_ = 2*(∫ p, entropyGauge f p ∂μ)/R := by rw [integral_div,integral_const_mul]
_ ≤ 2*C/R := div_le_div_of_nonneg_right (by linarith) hR.le
theorem linearMoment_uniformIntegrable {μ : Measure X} [IsFiniteMeasure μ]
{f : ℕ → X × Velocity → ℝ} {C : ℝ} (hfm : ∀ n, Measurable (f n))
(hf : ∀ n p, 0 ≤ f n p) (hi : ∀ n, Integrable (entropyGauge (f n)) (μ.prod volume))
(hb : ∀ n, (∫ p, entropyGauge (f n) p ∂μ.prod volume) ≤ C) :
UniformIntegrable (fun n => linearMoment (f n)) 1 (μ.prod volume) := by
have hui := uniformIntegrable_of_entropyGauge hfm hf hi hb
apply Compactness.uniformIntegrable_of_approximation (g := fun j n => velocityLinearCut ((j:ℝ)+1) (f n))
· intro j
let a : X × Velocity → ℝ := fun p => if ‖p.2‖ ≤ (j:ℝ)+1 then 1+‖p.2‖ else 0
have ha : Measurable a := (measurable_const.add measurable_snd.norm).ite
(measurableSet_le measurable_snd.norm measurable_const) measurable_const
let D : ℝ≥0 := ⟨(j:ℝ)+2,by positivity⟩
have hD (p : X × Velocity) : |a p| ≤ D := by
change |if ‖p.2‖ ≤ (j:ℝ)+1 then 1+‖p.2‖ else 0| ≤ (j:ℝ)+2
split_ifs with hp
· rw [abs_of_nonneg (by positivity)]
linarith
· simp only [abs_zero]
positivity
change UniformIntegrable (fun n p => if ‖p.2‖ ≤ (j:ℝ)+1 then
(1+‖p.2‖)*f n p else 0) 1 (μ.prod volume)
simpa only [a,ite_mul,zero_mul] using
Compactness.uniformIntegrable_of_bounded_multiplier hui ha D hD
· intro ε hε
obtain ⟨j,hj⟩ := exists_entropyTruncation_radius (2*C) hε
exact ⟨j,fun n => (velocityLinearCut_L1_error (by positivity) (hfm n) (hf n) (hi n) (hb n)).trans hj⟩
end BoltzmannNonuniqueness.PeriodicApproximation
end
end
section
/-! # Compactly supported unit-mass velocity kernels of arbitrarily small radius -/
noncomputable section
open MeasureTheory
namespace BoltzmannNonuniqueness.CollisionCompactness.DoubleGain
theorem exists_velocity_mollifier {δ : ℝ} (hδ : 0 < δ) :
∃ χ : C(Velocity,ℝ), HasCompactSupport χ ∧ Integrable χ ∧
(∀ a, 0 ≤ χ a) ∧ (∫ a, χ a) = 1 ∧ (∀ a, χ a ≠ 0 → ‖a‖ < δ) := by
let b : ContDiffBump (0 : Velocity) := ⟨δ/2,δ,by linarith,by linarith⟩
let χ : C(Velocity,ℝ) := ⟨b.normed volume,b.continuous_normed⟩
refine ⟨χ,b.hasCompactSupport_normed,b.integrable_normed,?_,b.integral_normed,?_⟩
· exact b.nonneg_normed
· intro a ha
have hs : a ∈ Function.support (b.normed (volume : Measure Velocity)) := ha
rw [b.support_normed_eq] at hs
simpa only [Metric.mem_ball,dist_zero_right] using hs
end BoltzmannNonuniqueness.CollisionCompactness.DoubleGain
end
end
section
/-! # Uniform integrability of the spatial mass and first-moment marginal -/
noncomputable section
open MeasureTheory Set Filter
open scoped ENNReal
namespace BoltzmannNonuniqueness.PeriodicApproximation
variable {X : Type*} [MeasurableSpace X]
theorem linearMoment_marginal_uniformIntegrable {μ : Measure X} [IsFiniteMeasure μ]
{f : ℕ → X × Velocity → ℝ} {C : ℝ} (hfm : ∀ n, Measurable (f n))
(hf : ∀ n p, 0 ≤ f n p) (hi : ∀ n, Integrable (entropyGauge (f n)) (μ.prod volume))
(hb : ∀ n, (∫ p, entropyGauge (f n) p ∂μ.prod volume) ≤ C) :
UniformIntegrable (fun n x => ∫ v, linearMoment (f n) (x,v)) 1 μ := by
have hui := linearMoment_uniformIntegrable hfm hf hi hb
have he (R : ℝ) (n : ℕ) (x : X) :
(∫ v, velocityLinearCut R (f n) (x,v)) =
∫ v in Metric.closedBall (0:Velocity) R, linearMoment (f n) (x,v) := by
rw [← integral_indicator Metric.isClosed_closedBall.measurableSet]
congr 1
ext v
simp only [velocityLinearCut,indicator,Metric.mem_closedBall,dist_zero_right]
apply Compactness.uniformIntegrable_of_approximation
(g := fun j n x => ∫ v, velocityLinearCut ((j:ℝ)+1) (f n) (x,v))
· intro j
let s : Set Velocity := Metric.closedBall 0 ((j:ℝ)+1)
let : IsFiniteMeasure ((volume : Measure Velocity).restrict s) :=
isFiniteMeasure_restrict.mpr (isCompact_closedBall (0:Velocity) ((j:ℝ)+1)).measure_lt_top.ne
have hu := Compactness.uniformIntegrable_restrict hui (univ ×ˢ s)
rw [← Measure.prod_restrict,Measure.restrict_univ] at hu
have hm := Compactness.uniformIntegrable_integral (fun n => linearMoment_measurable (hfm n)) hu
simpa only [he] using hm
· intro ε hε
obtain ⟨j,hj⟩ := exists_entropyTruncation_radius (2*C) hε
refine ⟨j,fun n => ?_⟩
have hfi := linearMoment_integrable (hfm n) (hf n) (hi n)
have hgi := velocityLinearCut_integrable ((j:ℝ)+1) (hfm n) (hf n) (hi n)
have hae : (fun x => (∫ v, linearMoment (f n) (x,v))-
∫ v, velocityLinearCut ((j:ℝ)+1) (f n) (x,v)) =ᵐ[μ]
(fun x => ∫ v, linearMoment (f n) (x,v)-velocityLinearCut ((j:ℝ)+1) (f n) (x,v)) := by
filter_upwards [hfi.prod_right_ae,hgi.prod_right_ae] with x hfx hgx
exact (integral_sub hfx hgx).symm
rw [eLpNorm_congr_ae hae]
exact (Compactness.eLpNorm_integral_le
((linearMoment_measurable (hfm n)).sub (velocityLinearCut_measurable ((j:ℝ)+1) (hfm n)))).trans
((velocityLinearCut_L1_error (by positivity) (hfm n) (hf n) (hi n) (hb n)).trans hj)
end BoltzmannNonuniqueness.PeriodicApproximation
end
end
section
/-! # Removing bounded velocity cutoffs by the uniform energy-entropy budget -/
noncomputable section
open MeasureTheory
open scoped ENNReal
namespace BoltzmannNonuniqueness.PeriodicApproximation
variable {X : Type*} [MeasurableSpace X]
omit [MeasurableSpace X] in
theorem velocityCutoff_error_le {f : X × Velocity → ℝ} {β : Velocity → ℝ} {R : ℝ}
(hR : 0 < R) (hf : ∀ p, 0 ≤ f p) (hβ0 : ∀ v, 0 ≤ β v) (hβ1 : ∀ v, β v ≤ 1)
(hβeq : ∀ v, ‖v‖ ≤ R → β v = 1) (p : X × Velocity) :
|f p-β p.2*f p| ≤ entropyGauge f p/R^2 := by
have hfn := hf p
have hnon : 0 ≤ f p-β p.2*f p := by nlinarith [hβ1 p.2]
rw [abs_of_nonneg hnon]
apply (le_div_iff₀ (sq_pos_of_pos hR)).mpr
by_cases hv : ‖p.2‖ ≤ R
· rw [hβeq p.2 hv,one_mul,sub_self,zero_mul]
exact entropyGauge_nonneg hf p
· have hv' : R < ‖p.2‖ := lt_of_not_ge hv
have hs : R^2 ≤ ‖p.2‖^2 := by nlinarith
have hle : f p-β p.2*f p ≤ f p := by nlinarith [hβ0 p.2]
have hlog := abs_nonneg (Real.log (f p))
unfold entropyGauge
nlinarith [mul_le_mul_of_nonneg_right hle (sq_nonneg R),
mul_le_mul_of_nonneg_left hs hfn,mul_nonneg hfn hlog]
theorem velocityCutoff_L1_bound {μ : Measure (X × Velocity)} {f : X × Velocity → ℝ}
{β : Velocity → ℝ} {R C : ℝ} (hR : 0 < R)
(hfm : Measurable f) (hf : ∀ p, 0 ≤ f p) (hβm : Measurable β)
(hβ0 : ∀ v, 0 ≤ β v) (hβ1 : ∀ v, β v ≤ 1)
(hβeq : ∀ v, ‖v‖ ≤ R → β v = 1)
(hi : Integrable (entropyGauge f) μ) (hb : (∫ p, entropyGauge f p ∂μ) ≤ C) :
eLpNorm (fun p => f p-β p.2*f p) 1 μ ≤ ENNReal.ofReal (C/R^2) := by
have hfi := integrable_of_entropyGauge hfm hf hi
have hbi : Integrable (fun p => β p.2*f p) μ := hfi.bdd_mul
(hβm.comp measurable_snd).aestronglyMeasurable
(ae_of_all _ (fun p => by rw [Real.norm_of_nonneg (hβ0 p.2)]; exact hβ1 p.2))
have hei := hfi.sub hbi
change Integrable (fun p => f p-β p.2*f p) μ at hei
rw [eLpNorm_one_eq_lintegral_enorm hei.aestronglyMeasurable,
← ofReal_integral_norm_eq_lintegral_enorm hei]
apply ENNReal.ofReal_le_ofReal
calc
_ ≤ ∫ p, entropyGauge f p/R^2 ∂μ := integral_mono hei.norm (hi.div_const (R^2))
(fun p => by simpa only [Real.norm_eq_abs] using velocityCutoff_error_le hR hf hβ0 hβ1 hβeq p)
_ = (∫ p, entropyGauge f p ∂μ)/R^2 := integral_div _ _
_ ≤ _ := div_le_div_of_nonneg_right hb (sq_nonneg R)
end BoltzmannNonuniqueness.PeriodicApproximation
end
end
end OAI