OAI/Analysis/Brenier/NormalizedPaths.lean
5 declarations, 0 contain sorry, 0 declared as axioms
- theorem
OAI.Problem358.exists_normalized_finite_affine_endpoint_potentialsline 18Source documentation
The bounded-energy, normalized interior intercept path itself supplies continuous endpoint potentials with the uniform L² estimate. In particular, no limits or regularity of the original coefficients at times zero and one are assumptions of this theorem.
theorem exists_normalized_finite_affine_endpoint_potentials {d : ℕ} {ι : Type*} [Fintype ι] [Nonempty ι] [MeasurableSpace ι] [MeasurableSingletonClass ι] (K : Set (E d)) [IsFiniteMeasure (uniformMeasure K)] (y v : ι → ℝ → E d) (c r : ι → ℝ → ℝ) (active : ℝ × E d → ι) (m : ι → ℝ) {w κ : ℝ} {R : ℝ≥0} (hw : 0 ≤ w) (hκ : 0 ≤ κ) (hxR : ∀ᵐ x ∂uniformMeasure K, ‖x‖ ≤ R) (hpositive : ∀ i, 0 < m i) (hy : ∀ i, Continuous (y i)) (hv : ∀ i, ContinuousOn (v i) (Ioo 0 1)) (hr : ∀ i, ContinuousOn (r i) (Ioo 0 1)) … - theorem
OAI.Problem358.MaxPotential.supports_of_maximizersline 87Source documentation
An everywhere maximizing affine-slope selection supports its finite maximum at every point, including the tie set.
theorem MaxPotential.supports_of_maximizers {ι V : Type*} [Fintype ι] [Nonempty ι] [NormedAddCommGroup V] [InnerProductSpace ℝ V] (y : ι → V) (c : ι → ℝ) {T : V → V} (hactive : ∀ x, ∃ i, T x = y i ∧ ∀ j, inner ℝ x (y j) + c j ≤ inner ℝ x (y i) + c i) : SupportingMapInterpolation.Supports (MaxPotential.potential y c) T := by …Mentions: OAI.Problem358.SupportingMapInterpolation.Supports, OAI.Problem358.MaxPotential.potential
- theorem
OAI.Problem358.exists_bounded_supporting_finite_affine_endpoint_pairline 103Source documentation
The exact endpoint maps of a continuous finite-affine path have global supporting certificates and inherit the endpoint slope bounds. The interval-law construction is supplied by
exists_unique_optimal_finite_affine_path_endpoints; no injectivity or positive individual mass is needed at the endpoints.theorem exists_bounded_supporting_finite_affine_endpoint_pair {d : ℕ} {ι : Type*} [Fintype ι] [Nonempty ι] {K : Set (E d)} (hK : IsCompact K) (hconv : Convex ℝ K) (hinterior : (interior K).Nonempty) {a b : ℝ} (hab : a < b) {y : ℝ → ι → E d} {c : ℝ → ι → ℝ} {T : ℝ → E d → E d} (w : ι → ℝ≥0∞) (hw : ∑ i, w i = 1) (hy : ∀ i, ContinuousOn (fun t => y t i) (Set.Icc a b)) (hc : ∀ i, ContinuousOn (fun t => c t i) (Set.Icc a b)) (hTm : ∀ t ∈ Set.Ioo a b, Measurable (T t)) (hT : ∀ t ∈ Set.Ioo a b, ∀ᵐ x ∂uniformMeasure K, … - theorem
OAI.Problem358.exists_supporting_pair_of_normalized_affine_pathline 161Source documentation
A normalized positive-mass affine motion gives the actual endpoint supporting potentials and their exact atomic laws, together with the uniform potential estimate. Neither separation nor intercept limits at the endpoints are assumptions.
theorem exists_supporting_pair_of_normalized_affine_path {d : ℕ} {ι : Type*} [Fintype ι] [Nonempty ι] [MeasurableSpace ι] [MeasurableSingletonClass ι] {K : Set (E d)} (hK : IsCompact K) (hKconv : Convex ℝ K) (hKint : (interior K).Nonempty) (y v : ι → ℝ → E d) (c r : ι → ℝ → ℝ) (active : ℝ × E d → ι) (m : ι → ℝ) {w κ : ℝ} {R L : ℝ≥0} (hw : 0 ≤ w) (hκ : 0 ≤ κ) (hxR : ∀ᵐ x ∂uniformMeasure K, ‖x‖ ≤ R) (hpositive : ∀ i, 0 < m i) (hsum : ∑ i, m i = 1) (hy : ∀ i, Continuous (y i)) (hv : ∀ i, ContinuousOn (v i) (Ioo 0 1)) … - theorem
OAI.Problem358.exists_supporting_pair_of_closedCell_pathline 266Source documentation
The geometric closed-cell mass equations suffice for the endpoint potential pair construction. A common measurable maximizing selector and all its mass identities are derived, not supplied as additional path assumptions.
theorem exists_supporting_pair_of_closedCell_path {d : ℕ} {ι : Type*} [Fintype ι] [Nonempty ι] [MeasurableSpace ι] [MeasurableSingletonClass ι] {K : Set (E d)} (hK : IsCompact K) (hKconv : Convex ℝ K) (hKint : (interior K).Nonempty) (y v : ι → ℝ → E d) (c r : ι → ℝ → ℝ) (m : ι → ℝ) {w κ : ℝ} {R L : ℝ≥0} (hw : 0 ≤ w) (hκ : 0 ≤ κ) (hxR : ∀ᵐ x ∂uniformMeasure K, ‖x‖ ≤ R) (hpositive : ∀ i, 0 < m i) (hsum : ∑ i, m i = 1) (hy : ∀ i, Continuous (y i)) (hc : ∀ i, Measurable (c i)) (hv : ∀ i, ContinuousOn (v i) (Ioo 0 1)) (hr : ∀ i, ContinuousOn (r i) (Ioo 0 1)) …