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