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import OAI.MathematicalPhysics.Boltzmann.Approximation.CutoffLossFrequency
import OAI.MathematicalPhysics.Boltzmann.Branching.MixedPhysicalMeasures
import OAI.MathematicalPhysics.Boltzmann.Compactness.PairBoundedTruncation
namespace OAI
section
/-! # Uniform integrability of the actual cutoff equation's right-hand side -/
noncomputable section
open MeasureTheory
open scoped ENNReal
namespace BoltzmannNonuniqueness.CollisionCompactness
variable {X : Type*} [MeasurableSpace X] {μ : Measure X}
def collisionSource (b : ℝ) (f : X × Velocity → ℝ) (p : X × Velocity) : ℝ :=
KineticCollisionNullSets.gain b f p-f p*KineticCollisionNullSets.frequency b f p
theorem collisionSource_measurable {f : X × Velocity → ℝ} (hf : Measurable f) (b : ℝ) :
Measurable (collisionSource b f) :=
(KineticCollisionNullSets.measurable_gain hf b).sub
(hf.mul (KineticCollisionNullSets.measurable_frequency hf b))
private theorem uniformIntegrable_sub {Y : Type*} [MeasurableSpace Y] {ν : Measure Y}
{f g : ℕ → Y → ℝ} (hf : UniformIntegrable f 1 ν) (hg : UniformIntegrable g 1 ν) :
UniformIntegrable (fun n y => f n y-g n y) 1 ν := by
obtain ⟨hu,C,hC⟩ := hf
obtain ⟨hv,D,hD⟩ := hg
refine ⟨hu.sub hv (by norm_num),C+D,fun n => ?_⟩
exact (eLpNorm_sub_le (by norm_num : (1 : ℝ≥0∞) ≤ 1)).trans
(by simpa only [ENNReal.coe_add] using add_le_add (hC n) (hD n))
theorem collisionSource_uniformIntegrable [SFinite μ]
{f : ℕ → X × Velocity → ℝ} (hfm : ∀ n, Measurable (f n)) (hf : ∀ n z, 0 ≤ f n z)
(hpair : UniformIntegrable (fun n => pairDensity (f n)) 1
(μ.prod (volume : Measure (Velocity × Velocity)))) (b : ℕ → ℝ)
(hgain : UniformIntegrable (fun n => KineticCollisionNullSets.gain (b n) (f n)) 1
(μ.prod (volume : Measure Velocity)))
(hloss : UniformIntegrable (fun n => cutoffLossDensity (b n) (f n)) 1
(μ.prod (volume : Measure Velocity))) :
UniformIntegrable (fun n => collisionSource (b n) (f n)) 1
(μ.prod (volume : Measure Velocity)) := by
have he (n) := cutoff_loss_ae_eq_frequency (hfm n) (hf n)
(memLp_one_iff_integrable.mp (hpair.memLp n)) (b n)
exact uniformIntegrable_sub hgain (hloss.ae_eq he)
end BoltzmannNonuniqueness.CollisionCompactness
end
end
section
/-! # Discarding the nonnegative losses in the actual hot source -/
noncomputable section
open MeasureTheory
namespace BoltzmannNonuniqueness.CollisionCompactness
variable {X : Type*}
theorem cutoffFrequency_nonneg (b : ℝ) {f : X × Velocity → ℝ}
(hf : ∀ p, 0 ≤ f p) (p : X × Velocity) :
0 ≤ KineticCollisionNullSets.frequency b f p := by
apply mul_nonneg (by positivity : (0:ℝ) ≤ 2*Real.pi)
exact integral_nonneg (fun w => mul_nonneg (CollisionCutoff.rate_nonneg b p.2 w) (hf _))
theorem collisionSource_le_gain (b : ℝ) {f : X × Velocity → ℝ}
(hf : ∀ p, 0 ≤ f p) (p : X × Velocity) :
collisionSource b f p ≤ KineticCollisionNullSets.gain b f p :=
sub_le_self _ (mul_nonneg (hf _) (cutoffFrequency_nonneg b hf p))
variable [MeasurableSpace X]
theorem hot_source_le_gain (b r e : ℝ) {c h : X × Velocity → ℝ}
(hc : ∀ p, 0 ≤ c p) (hh : ∀ p, 0 ≤ h p) (p : X × Velocity) :
2*mixedGainDensity b c h p-h p*KineticCollisionNullSets.frequency b c p+
r^2*collisionSource b h p+e ≤
2*mixedGainDensity b c h p+r^2*KineticCollisionNullSets.gain b h p+e := by
exact add_le_add (add_le_add (sub_le_self _ (mul_nonneg (hh _) (cutoffFrequency_nonneg b hc p)))
(mul_le_mul_of_nonneg_left (collisionSource_le_gain b hh p) (sq_nonneg r))) le_rfl
end BoltzmannNonuniqueness.CollisionCompactness
end
end
section
/-! # Scaling and base-coordinate identities for physical cutoff collisions -/
noncomputable section
open MeasureTheory
namespace BoltzmannNonuniqueness.CollisionCompactness
variable {X Y : Type*} [MeasurableSpace X] [MeasurableSpace Y]
omit [MeasurableSpace X] in
theorem mixedPostRate_const_mul (b a d : ℝ) (c h : X × Velocity → ℝ)
(z : (X × (Velocity × Velocity)) × Sphere) :
mixedPostRate b (fun p => a*c p) (fun p => d*h p) z =
(a*d)*mixedPostRate b c h z := by
unfold mixedPostRate mixedPreRate
ring
theorem mixedGain_const_mul (b a d : ℝ) (c h : X × Velocity → ℝ) (p : X × Velocity) :
mixedGainDensity b (fun p => a*c p) (fun p => d*h p) p =
(a*d)*mixedGainDensity b c h p := by
unfold mixedGainDensity
simp_rw [mixedPostRate_const_mul]
rw [integral_const_mul,integral_const_mul]
ring
theorem cutoffGain_const_mul (b a : ℝ) (f : X × Velocity → ℝ) (p : X × Velocity) :
KineticCollisionNullSets.gain b (fun p => a*f p) p =
a^2*KineticCollisionNullSets.gain b f p := by
rw [← mixedGainDensity_self, mixedGain_const_mul, mixedGainDensity_self]
ring
omit [MeasurableSpace X] in
theorem cutoffFrequency_const_mul (b a : ℝ) (f : X × Velocity → ℝ) (p : X × Velocity) :
KineticCollisionNullSets.frequency b (fun p => a*f p) p =
a*KineticCollisionNullSets.frequency b f p := by
unfold KineticCollisionNullSets.frequency CollisionCutoff.frequency
simp_rw [show ∀ w, CollisionCutoff.rate b p.2 w*(a*f (p.1,w)) =
a*(CollisionCutoff.rate b p.2 w*f (p.1,w)) by intro w; ring]
rw [integral_const_mul]
ring
omit [MeasurableSpace X] in
theorem cutoffFrequency_add (b : ℝ) (c h : X × Velocity → ℝ) (p : X × Velocity)
(hc : Integrable (fun w => CollisionCutoff.rate b p.2 w*c (p.1,w)))
(hh : Integrable (fun w => CollisionCutoff.rate b p.2 w*h (p.1,w))) :
KineticCollisionNullSets.frequency b (c+h) p =
KineticCollisionNullSets.frequency b c p+KineticCollisionNullSets.frequency b h p := by
unfold KineticCollisionNullSets.frequency CollisionCutoff.frequency
simp only [Pi.add_apply,mul_add]
have he := integral_add hc hh
rw [he]
ring
omit [MeasurableSpace X] [MeasurableSpace Y] in
theorem mixedPostRate_base_comp (b : ℝ) (c h : X × Velocity → ℝ) (τ : Y → X)
(z : (Y × (Velocity × Velocity)) × Sphere) :
mixedPostRate b (fun p => c (τ p.1,p.2)) (fun p => h (τ p.1,p.2)) z =
mixedPostRate b c h ((τ z.1.1,z.1.2),z.2) := rfl
theorem mixedGain_base_comp (b : ℝ) (c h : X × Velocity → ℝ) (τ : Y → X)
(p : Y × Velocity) :
mixedGainDensity b (fun p => c (τ p.1,p.2)) (fun p => h (τ p.1,p.2)) p =
mixedGainDensity b c h (τ p.1,p.2) := rfl
omit [MeasurableSpace X] [MeasurableSpace Y] in
theorem cutoffGain_base_comp (b : ℝ) (f : X × Velocity → ℝ) (τ : Y → X)
(p : Y × Velocity) :
KineticCollisionNullSets.gain b (fun p => f (τ p.1,p.2)) p =
KineticCollisionNullSets.gain b f (τ p.1,p.2) := rfl
omit [MeasurableSpace X] [MeasurableSpace Y] in
theorem cutoffFrequency_base_comp (b : ℝ) (f : X × Velocity → ℝ) (τ : Y → X)
(p : Y × Velocity) :
KineticCollisionNullSets.frequency b (fun p => f (τ p.1,p.2)) p =
KineticCollisionNullSets.frequency b f (τ p.1,p.2) := rfl
end BoltzmannNonuniqueness.CollisionCompactness
end
end
section
/-! # L1 contraction for marginalizing a collision rate -/
noncomputable section
open MeasureTheory
open scoped ENNReal
namespace BoltzmannNonuniqueness.CollisionCompactness
variable {X : Type*} [MeasurableSpace X] {μ : Measure X} [SFinite μ]
local instance : SFinite ((volume : Measure Velocity).prod sphereArea) := Measure.prod.instSFinite
def collisionMarginal (h : (X × (Velocity × Velocity)) × Sphere → ℝ)
(p : X × Velocity) : ℝ :=
∫ q : Velocity × Sphere, h (collisionGrouping.symm (p,q))
∂(volume : Measure Velocity).prod sphereArea
theorem collisionMarginal_integrable {h : (X × (Velocity × Velocity)) × Sphere → ℝ}
(hi : Integrable h ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea)) :
Integrable (collisionMarginal h) (μ.prod volume) :=
((collisionGrouping_measurePreserving μ).symm.integrable_comp_of_integrable hi).integral_prod_left
theorem collisionMarginal_sub_ae {h k : (X × (Velocity × Velocity)) × Sphere → ℝ}
(hi : Integrable h ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea))
(ki : Integrable k ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea)) :
collisionMarginal (h-k) =ᵐ[μ.prod volume] collisionMarginal h-collisionMarginal k := by
have hhi := (collisionGrouping_measurePreserving μ).symm.integrable_comp_of_integrable hi
have hki := (collisionGrouping_measurePreserving μ).symm.integrable_comp_of_integrable ki
filter_upwards [hhi.prod_right_ae,hki.prod_right_ae] with p hp kp
exact integral_sub hp kp
theorem collisionMarginal_eLpNorm_le {h : (X × (Velocity × Velocity)) × Sphere → ℝ}
(hm : Measurable h) :
eLpNorm (collisionMarginal h) 1 (μ.prod volume) ≤
eLpNorm h 1 ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea) := by
have ht := Compactness.eLpNorm_integral_le (μ := μ.prod volume)
(ν := (volume : Measure Velocity).prod sphereArea) (hm.comp collisionGrouping.symm.measurable)
apply ht.trans_eq
exact eLpNorm_comp_measurePreserving hm.aestronglyMeasurable (collisionGrouping_measurePreserving μ).symm
theorem collisionMarginal_difference_le {h k : (X × (Velocity × Velocity)) × Sphere → ℝ}
(hm : Measurable h) (km : Measurable k)
(hi : Integrable h ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea))
(ki : Integrable k ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea)) :
eLpNorm (collisionMarginal h-collisionMarginal k) 1 (μ.prod volume) ≤
eLpNorm (h-k) 1 ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea) := by
rw [← eLpNorm_congr_ae (collisionMarginal_sub_ae hi ki)]
exact collisionMarginal_eLpNorm_le (hm.sub km)
end BoltzmannNonuniqueness.CollisionCompactness
end
end
section
/-! # Collision operators depend only on the velocity fibre at their base point -/
noncomputable section
open MeasureTheory
namespace BoltzmannNonuniqueness.CollisionCompactness
variable {X : Type*} [MeasurableSpace X]
private theorem mixedPostRate_fiber_congr (b : ℝ) {c d h k : X × Velocity → ℝ} {x : X}
(hc : ∀ v, c (x,v) = d (x,v)) (hh : ∀ v, h (x,v) = k (x,v))
(v : Velocity) (w : Velocity × Sphere) :
mixedPostRate b c h (collisionGrouping.symm ((x,v),w)) =
mixedPostRate b d k (collisionGrouping.symm ((x,v),w)) := by
rw [mixedPostRate_formula,mixedPostRate_formula]
change CollisionCutoff.kernel b v w.1 w.2*c (x,scatterLeft v w.1 w.2)*h (x,scatterRight v w.1 w.2) =
CollisionCutoff.kernel b v w.1 w.2*d (x,scatterLeft v w.1 w.2)*k (x,scatterRight v w.1 w.2)
rw [hc,hh]
theorem mixedGain_fiber_congr (b : ℝ) {c d h k : X × Velocity → ℝ} {x : X}
(hc : ∀ v, c (x,v) = d (x,v)) (hh : ∀ v, h (x,v) = k (x,v)) (v : Velocity) :
mixedGainDensity b c h (x,v) = mixedGainDensity b d k (x,v) := by
unfold mixedGainDensity
simp_rw [mixedPostRate_fiber_congr b hc hh,mixedPostRate_fiber_congr b hh hc]
omit [MeasurableSpace X] in
theorem cutoffGain_fiber_congr (b : ℝ) {f g : X × Velocity → ℝ} {x : X}
(hf : ∀ v, f (x,v) = g (x,v)) (v : Velocity) :
KineticCollisionNullSets.gain b f (x,v) = KineticCollisionNullSets.gain b g (x,v) := by
unfold KineticCollisionNullSets.gain CollisionCutoff.gain CollisionCutoff.integrand
simp_rw [hf]
omit [MeasurableSpace X] in
theorem cutoffFrequency_fiber_congr (b : ℝ) {f g : X × Velocity → ℝ} {x : X}
(hf : ∀ v, f (x,v) = g (x,v)) (v : Velocity) :
KineticCollisionNullSets.frequency b f (x,v) = KineticCollisionNullSets.frequency b g (x,v) := by
unfold KineticCollisionNullSets.frequency CollisionCutoff.frequency
simp_rw [hf]
omit [MeasurableSpace X] in
theorem collisionSource_fiber_congr (b : ℝ) {f g : X × Velocity → ℝ} {x : X}
(hf : ∀ v, f (x,v) = g (x,v)) (v : Velocity) :
collisionSource b f (x,v) = collisionSource b g (x,v) := by
unfold collisionSource
rw [cutoffGain_fiber_congr b hf,cutoffFrequency_fiber_congr b hf,hf]
end BoltzmannNonuniqueness.CollisionCompactness
end
end
end OAI