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import OAI.MathematicalPhysics.Boltzmann.Approximation.RegularizedLogBounds
import OAI.MathematicalPhysics.Boltzmann.Compactness.EntropyDissipationAverage
namespace OAI
section
/-! # Integrable entropy tests for bounded kinetic densities -/
noncomputable section
open MeasureTheory
open BoltzmannNonuniqueness.VelocityWeight
namespace BoltzmannNonuniqueness
variable {X : Type*} [MeasurableSpace X]
theorem kinetic_log_product_integrable {μ : Measure X} [IsFiniteMeasure μ]
{q B C δ : ℝ} (hq₁ : 1 < q) (hq₂ : q < 2) (hB : 0 ≤ B) (hC : 0 ≤ C) (hδ : 0 < δ)
{u a : X × Velocity → ℝ} (hum : Measurable u) (ham : Measurable a)
(hl : ∀ p, δ*Real.exp (-2*‖p.2‖^2) ≤ u p)
(hu : ∀ p, u p ≤ B*H q p.2)
(ha : ∀ᵐ p ∂μ.prod (volume : Measure Velocity), |a p| ≤ C*H q p.2) :
Integrable (fun p => Real.log (u p/maxwellian p.2)*a p) (μ.prod volume) := by
obtain ⟨p,hp,hpi⟩ := exists_integrable_rpow_H hq₁ hq₂
have hmaj := ((logarithmicMajorant_integrable (B := B) (δ := δ) hq₂ hpi).const_mul C).comp_snd μ
have hMm : Measurable (fun p : X × Velocity => maxwellian p.2) := by
unfold maxwellian
fun_prop
apply hmaj.mono' (((hum.div hMm).log).mul ham).aestronglyMeasurable
filter_upwards [ha] with z hz
simp only [Pi.mul_apply]
rw [Real.norm_eq_abs,abs_mul]
calc
_ ≤ |Real.log (u z/maxwellian z.2)| * (C*H q z.2) :=
mul_le_mul_of_nonneg_left hz (abs_nonneg _)
_ = C*(|Real.log (u z/maxwellian z.2)| * H q z.2) := by ring
_ ≤ _ := mul_le_mul_of_nonneg_left (logarithm_weight_bound hB hp hδ z.2 (hl z) (hu z)) hC
end BoltzmannNonuniqueness
end
end
section
/-! # A quantitative integral bound for the kinetic logarithmic test -/
noncomputable section
open MeasureTheory
open BoltzmannNonuniqueness.VelocityWeight
namespace BoltzmannNonuniqueness
variable {X : Type*} [MeasurableSpace X]
theorem kinetic_log_integral_bound {μ : Measure X} [IsFiniteMeasure μ]
{q B C δ p : ℝ} (hq : q < 2) (hB : 0 ≤ B) (hC : 0 ≤ C) (hδ : 0 < δ)
(hp : 1 < p) (hpi : Integrable (fun v : Velocity => H q v^p))
{u a : X × Velocity → ℝ}
(hl : ∀ z, δ*Real.exp (-2*‖z.2‖^2) ≤ u z) (hu : ∀ z, u z ≤ B*H q z.2)
(ha : ∀ᵐ z ∂μ.prod (volume : Measure Velocity), |a z| ≤ C*H q z.2) :
|∫ z, Real.log (u z/maxwellian z.2)*a z ∂μ.prod volume| ≤
C*∫ z : X × Velocity, logarithmicMajorant q B p δ z.2 ∂μ.prod volume := by
have hi := ((logarithmicMajorant_integrable (B := B) (δ := δ) hq hpi).const_mul C).comp_snd μ
have hb : ∀ᵐ z ∂μ.prod (volume : Measure Velocity),
‖Real.log (u z/maxwellian z.2)*a z‖ ≤ C*logarithmicMajorant q B p δ z.2 := by
filter_upwards [ha] with z hz
rw [Real.norm_eq_abs,abs_mul]
calc
_ ≤ |Real.log (u z/maxwellian z.2)| * (C*H q z.2) :=
mul_le_mul_of_nonneg_left hz (abs_nonneg _)
_ = C*(|Real.log (u z/maxwellian z.2)| * H q z.2) := by ring
_ ≤ _ := mul_le_mul_of_nonneg_left (logarithm_weight_bound hB hp hδ z.2 (hl z) (hu z)) hC
have h := norm_integral_le_of_norm_le hi hb
simpa only [Real.norm_eq_abs,integral_const_mul] using h
end BoltzmannNonuniqueness
end
end
section
/-! # The Gaussian entropy error is integrable on a finite kinetic base -/
noncomputable section
open MeasureTheory
open BoltzmannNonuniqueness.VelocityWeight
namespace BoltzmannNonuniqueness
variable {X : Type*} [MeasurableSpace X]
def gaussianRegularizedDensity (δ : ℝ) (f : X × Velocity → ℝ) (p : X × Velocity) : ℝ :=
f p+δ*Real.exp (-2*‖p.2‖^2)
theorem gaussianRegularizedDensity_measurable (δ : ℝ) {f : X × Velocity → ℝ}
(hfm : Measurable f) : Measurable (gaussianRegularizedDensity δ f) := by
unfold gaussianRegularizedDensity
fun_prop
theorem kinetic_regularization_error_bound (hcarleman : Published.GPV2009CarlemanInput)
{μ : Measure X} [SFinite μ] {δ A q b : ℝ}
(hδ : 0 ≤ δ) (hδone : δ ≤ 1) (hA : 0 ≤ A)
(hq₁ : 1 < q) (hq₂ : q < 2) (hb : 0 ≤ b)
{f : X × Velocity → ℝ} (hfm : Measurable f) (hfn : ∀ p, 0 ≤ f p)
(hfb : ∀ p, f p ≤ A*H q p.2) :
∀ᵐ p ∂μ.prod (volume : Measure Velocity),
|CollisionCompactness.collisionSource b (gaussianRegularizedDensity δ f) p-
CollisionCompactness.collisionSource b f p| ≤
(δ*entropyErrorCoefficient q A b)*H q p.2 := by
have hgm := gaussianRegularizedDensity_measurable δ hfm
have hsm := (CollisionCompactness.collisionSource_measurable hgm b).sub
(CollisionCompactness.collisionSource_measurable hfm b)
have hH : Measurable (fun p : X × Velocity => (δ*entropyErrorCoefficient q A b)*H q p.2) := by
unfold H singularity transverse
fun_prop
apply (Measure.ae_prod_iff_ae_ae (measurableSet_le hsm.abs hH)).mpr
filter_upwards [] with x
have hx := gaussianRegularization_collision_error hcarleman hδ hδone hA hq₁ hq₂ hb
(hfm.comp (measurable_const.prodMk measurable_id)) (fun v => hfn (x,v)) (fun v => hfb (x,v))
exact hx
theorem kinetic_regularization_entropy_integrable (hcarleman : Published.GPV2009CarlemanInput)
{μ : Measure X} [IsFiniteMeasure μ] {δ A q b : ℝ}
(hδ : 0 < δ) (hδone : δ ≤ 1) (hA : 0 ≤ A)
(hq₁ : 1 < q) (hq₂ : q < 2) (hb : 0 ≤ b)
{f : X × Velocity → ℝ} (hfm : Measurable f) (hfn : ∀ p, 0 ≤ f p)
(hfb : ∀ p, f p ≤ A*H q p.2) :
Integrable (fun p => Real.log (gaussianRegularizedDensity δ f p/maxwellian p.2)*
(CollisionCompactness.collisionSource b (gaussianRegularizedDensity δ f) p-
CollisionCompactness.collisionSource b f p)) (μ.prod volume) := by
have hgm := gaussianRegularizedDensity_measurable δ hfm
apply kinetic_log_product_integrable hq₁ hq₂ (add_nonneg hA tiltConstant_pos.le)
(mul_nonneg hδ.le (entropyErrorCoefficient_nonneg hA hb q)) hδ hgm
((CollisionCompactness.collisionSource_measurable hgm b).sub
(CollisionCompactness.collisionSource_measurable hfm b))
· intro p
dsimp [gaussianRegularizedDensity]
linarith [hfn p]
· intro p
exact gaussianRegularization_bound hδ.le hδone (fun v => hfb (p.1,v)) p.2
· exact kinetic_regularization_error_bound hcarleman hδ.le hδone hA hq₁ hq₂ hb hfm hfn hfb
end BoltzmannNonuniqueness
end
end
section
/-! # Vanishing of the entropy-error majorant after integrating the finite base -/
noncomputable section
open MeasureTheory Filter
open scoped Topology
open BoltzmannNonuniqueness.VelocityWeight
namespace BoltzmannNonuniqueness
variable {X : Type*} [MeasurableSpace X]
theorem kinetic_entropy_error_tendsto (μ : Measure X) [SFinite μ]
{q B p : ℝ} (C : ℝ) (hq : q < 2)
(hp : Integrable (fun v : Velocity => H q v^p)) :
Tendsto (fun δ : ℝ => δ*C*(∫ z : X × Velocity,
logarithmicMajorant q B p δ z.2 ∂μ.prod volume)) (𝓝 0) (𝓝 0) := by
have h := (tendsto_integrated_entropy_error (B := B) C hq hp).mul_const (μ.real Set.univ)
convert h using 1
· funext δ
rw [integral_fun_snd,smul_eq_mul]
ring
· ring_nf
end BoltzmannNonuniqueness
end
end
end OAI