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f18e7de | 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 61 62 63 64 65 66 67 68 69 70 71 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86 87 88 89 90 91 92 93 94 95 96 97 98 99 100 101 102 103 104 105 106 107 108 109 110 111 112 113 114 115 116 117 118 119 120 121 122 123 124 125 126 127 128 129 130 131 132 133 134 135 136 137 138 139 140 141 142 143 144 145 146 147 148 149 150 151 152 153 154 155 | import Mathlib.Analysis.InnerProductSpace.PiL2
import Mathlib.MeasureTheory.Constructions.HaarToSphere
import Mathlib.MeasureTheory.Group.AddCircle
import Mathlib.MeasureTheory.Measure.Haar.InnerProductSpace
import Mathlib.Tactic.Abel
import Mathlib.Tactic.Ring
namespace OAI
/-!
# Collision model for periodic hard spheres
The normal parametrization and absolute angular kernel here are exactly those of
Sections 1–2 of the paper.
-/
noncomputable section
open MeasureTheory
open scoped RealInnerProductSpace
namespace BoltzmannNonuniqueness
abbrev Velocity := EuclideanSpace ℝ (Fin 3)
abbrev Position := Fin 3 → AddCircle (1 : ℝ)
abbrev Phase := Position × Velocity
abbrev Density := Phase → ℝ
abbrev Sphere := Metric.sphere (0 : Velocity) 1
/-- Ordinary surface area, rather than normalized probability on the sphere. -/
def sphereArea : Measure Sphere := (volume : Measure Velocity).toSphere
def normalComponent (v w ω : Velocity) : ℝ := inner ℝ (v - w) ω
def scatterLeft (v w ω : Velocity) : Velocity := v - normalComponent v w ω • ω
def scatterRight (v w ω : Velocity) : Velocity := w + normalComponent v w ω • ω
def collisionKernel (v w ω : Velocity) : ℝ := |normalComponent v w ω|
def gain (f : Density) (x : Position) (v : Velocity) : ℝ :=
∫ p : Velocity × Sphere,
collisionKernel v p.1 p.2 * f (x, scatterLeft v p.1 p.2) *
f (x, scatterRight v p.1 p.2)
∂((volume : Measure Velocity).prod sphereArea)
def loss (f : Density) (x : Position) (v : Velocity) : ℝ :=
∫ p : Velocity × Sphere,
collisionKernel v p.1 p.2 * f (x, v) * f (x, p.1)
∂((volume : Measure Velocity).prod sphereArea)
def collision (f : Density) (x : Position) (v : Velocity) : ℝ :=
gain f x v - loss f x v
theorem collisionKernel_nonneg (v w ω : Velocity) : 0 ≤ collisionKernel v w ω :=
abs_nonneg _
theorem scatter_momentum (v w ω : Velocity) :
scatterLeft v w ω + scatterRight v w ω = v + w := by
unfold scatterLeft scatterRight
abel
theorem scatter_energy (v w ω : Velocity) (hω : ‖ω‖ = 1) :
‖scatterLeft v w ω‖ ^ 2 + ‖scatterRight v w ω‖ ^ 2 = ‖v‖ ^ 2 + ‖w‖ ^ 2 := by
unfold scatterLeft scatterRight normalComponent
rw [norm_sub_sq_real, norm_add_sq_real]
simp only [inner_smul_right, norm_smul, Real.norm_eq_abs, hω, mul_one, sq_abs,
inner_sub_left]
ring
theorem normalComponent_scatter (v w ω : Velocity) (hω : ‖ω‖ = 1) :
normalComponent (scatterLeft v w ω) (scatterRight v w ω) ω =
-normalComponent v w ω := by
simp only [normalComponent, scatterLeft, scatterRight, inner_sub_left, inner_add_left,
real_inner_smul_left, real_inner_self_eq_norm_sq, hω]
ring
theorem scatterLeft_involutive (v w ω : Velocity) (hω : ‖ω‖ = 1) :
scatterLeft (scatterLeft v w ω) (scatterRight v w ω) ω = v := by
change scatterLeft v w ω -
normalComponent (scatterLeft v w ω) (scatterRight v w ω) ω • ω = v
rw [normalComponent_scatter v w ω hω]
simp [scatterLeft, neg_smul]
theorem scatterRight_involutive (v w ω : Velocity) (hω : ‖ω‖ = 1) :
scatterRight (scatterLeft v w ω) (scatterRight v w ω) ω = w := by
change scatterRight v w ω +
normalComponent (scatterLeft v w ω) (scatterRight v w ω) ω • ω = w
rw [normalComponent_scatter v w ω hω]
simp [scatterRight, neg_smul]
theorem collisionKernel_scatter (v w ω : Velocity) (hω : ‖ω‖ = 1) :
collisionKernel (scatterLeft v w ω) (scatterRight v w ω) ω =
collisionKernel v w ω := by
simp only [collisionKernel, normalComponent_scatter v w ω hω, abs_neg]
theorem scatterLeft_translate (v w u ω : Velocity) :
scatterLeft (v - u) (w - u) ω = scatterLeft v w ω - u := by
have h : v - u - (w - u) = v - w := by abel
simp only [scatterLeft, normalComponent, h]
abel
theorem scatterRight_translate (v w u ω : Velocity) :
scatterRight (v - u) (w - u) ω = scatterRight v w ω - u := by
have h : v - u - (w - u) = v - w := by abel
simp only [scatterRight, normalComponent, h]
abel
/-- The center may vary with space and time: this identity is pointwise in the center. -/
theorem scatter_centered_energy (v w u ω : Velocity) (hω : ‖ω‖ = 1) :
‖scatterLeft v w ω - u‖ ^ 2 + ‖scatterRight v w ω - u‖ ^ 2 =
‖v - u‖ ^ 2 + ‖w - u‖ ^ 2 := by
simpa only [scatterLeft_translate, scatterRight_translate] using
scatter_energy (v - u) (w - u) ω hω
/-- A Gaussian with arbitrary amplitude, exponent, and center. -/
def gaussian (A β : ℝ) (u v : Velocity) : ℝ := A * Real.exp (-β * ‖v - u‖ ^ 2)
/-- Detailed balance, used for the transported Maxwellian barrier in Section 4. -/
theorem gaussian_detailed_balance (A β : ℝ) (u v w ω : Velocity) (hω : ‖ω‖ = 1) :
gaussian A β u (scatterLeft v w ω) * gaussian A β u (scatterRight v w ω) =
gaussian A β u v * gaussian A β u w := by
have h := scatter_centered_energy v w u ω hω
unfold gaussian
calc
A * Real.exp (-β * ‖scatterLeft v w ω - u‖ ^ 2) *
(A * Real.exp (-β * ‖scatterRight v w ω - u‖ ^ 2)) =
A ^ 2 * Real.exp (-β * (‖scatterLeft v w ω - u‖ ^ 2 +
‖scatterRight v w ω - u‖ ^ 2)) := by rw [mul_add, Real.exp_add]; ring
_ = A ^ 2 * Real.exp (-β * (‖v - u‖ ^ 2 + ‖w - u‖ ^ 2)) := by rw [h]
_ = A * Real.exp (-β * ‖v - u‖ ^ 2) * (A * Real.exp (-β * ‖w - u‖ ^ 2)) := by
rw [mul_add, Real.exp_add]
ring
/-- Pointwise detailed balance proves equality of the gain and loss integrands. -/
theorem gaussian_gain_eq_loss (A β : ℝ) (u : Velocity) (x : Position) (v : Velocity) :
gain (fun z => gaussian A β u z.2) x v =
loss (fun z => gaussian A β u z.2) x v := by
apply integral_congr_ae
filter_upwards [] with p
have hω : ‖(p.2 : Velocity)‖ = 1 := mem_sphere_zero_iff_norm.mp p.2.property
rw [mul_assoc, gaussian_detailed_balance A β u v p.1 p.2 hω, ← mul_assoc]
/-- This algebraic identity alone does not assert collision integrability for arbitrary `β`.
The admissibility interface separately requires genuine finite collision integrals. -/
theorem gaussian_collision_eq_zero (A β : ℝ) (u : Velocity) (x : Position)
(v : Velocity) : collision (fun z => gaussian A β u z.2) x v = 0 := by
exact sub_eq_zero.mpr (gaussian_gain_eq_loss A β u x v)
end BoltzmannNonuniqueness
end
end OAI
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