OAI/MathematicalPhysics/ContinuumCoulomb/Nuclei/MoserEndpoint.lean
3 declarations, 0 contain sorry, 0 declared as axioms
The actual time-one map is a bijection of physical space. This follows from forward uniqueness and trajectories with terminal data, rather than from assuming that the continuity equation already produces a diffeomorphism.
- theorem
OAI.ContinuumCoulomb.moser_trajectory_unique_terminalline 13 - theorem
OAI.ContinuumCoulomb.moser_trajectory_spatial_boundline 37Source documentation
The usual exponential spatial-dependence bound for these actual curves.
theorem moser_trajectory_spatial_bound {rho : ℝ} (hrho : 0 < rho) (V : Position → ℝ) (hV : ContDiff ℝ 6 V) (hc : HasCompactSupport V) (hbound : ∀ x, |manufacturedCharge V x| ≤ rho / 2) : ∃ K : ℝ≥0, ∀ (α β : ℝ → Position), (∀ t ∈ Set.Icc (0 : ℝ) 1, HasDerivWithinAt α (moserVelocity rho V t (α t)) (Set.Icc (0 : ℝ) 1) t) → (∀ t ∈ Set.Icc (0 : ℝ) 1, HasDerivWithinAt β (moserVelocity rho V t (β t)) (Set.Icc (0 : ℝ) 1) t) → ∀ t ∈ Set.Icc (0 : ℝ) 1, dist (α t) (β t) ≤ dist (α 0) (β 0) * Real.exp ((K : ℝ) * t) := by …Mentions: OAI.ContinuumCoulomb.Position, OAI.ContinuumCoulomb.manufacturedCharge, OAI.ContinuumCoulomb.moserVelocity
- theorem
OAI.ContinuumCoulomb.moser_time_one_existsline 66Source documentation
The generated time-one map is globally Lipschitz, bijective, and fixes the complement of the compact well support.
theorem moser_time_one_exists {rho : ℝ} (hrho : 0 < rho) (V : Position → ℝ) (hV : ContDiff ℝ 6 V) (hc : HasCompactSupport V) (hbound : ∀ x, |manufacturedCharge V x| ≤ rho / 2) : ∃ G : Position → ℝ → Position, (∀ x, G x 0 = x) ∧ (∀ x, ∀ t ∈ Set.Icc (0 : ℝ) 1, HasDerivWithinAt (G x) (moserVelocity rho V t (G x t)) (Set.Icc (0 : ℝ) 1) t) ∧ Function.Bijective (fun x => G x 1) ∧ (∃ C : ℝ≥0, LipschitzWith C (fun x => G x 1)) ∧ (∀ x, x ∉ tsupport V → G x 1 = x) := by …Mentions: OAI.ContinuumCoulomb.Position, OAI.ContinuumCoulomb.manufacturedCharge, OAI.ContinuumCoulomb.moserVelocity