OAI/Analysis/Brenier/CellContinuity.lean
22 declarations, 0 contain sorry, 0 declared as axioms
- def
OAI.Problem358.scoreCellline 13Source documentation
The closed cell of an affine score, before restriction to the source set.
def scoreCell {d : ℕ} {ι : Type*} (y : ι → E d) (c : ι → ℝ) (i : ι) : Set (E d) := … - theorem
OAI.Problem358.measurableSet_scoreCellline 16 - theorem
OAI.Problem358.eventually_le_iff_of_tendsto_neline 24Source documentation
A strict limiting comparison has an eventually constant truth value.
theorem eventually_le_iff_of_tendsto_ne {β : Type*} {l : Filter β} {f g : β → ℝ} {a b : ℝ} (hf : Tendsto f l (𝓝 a)) (hg : Tendsto g l (𝓝 b)) (hab : a ≠ b) : ∀ᶠ n in l, f n ≤ g n ↔ a ≤ b := by … - theorem
OAI.Problem358.eventually_mem_scoreCell_iffline 35Source documentation
Away from limiting ties, membership in a finite affine cell stabilizes.
theorem eventually_mem_scoreCell_iff {d : ℕ} {ι β : Type*} [Finite ι] {l : Filter β} {ys : β → ι → E d} {cs : β → ι → ℝ} {y : ι → E d} {c : ι → ℝ} (i : ι) (x : E d) (hy : ∀ j, Tendsto (fun n => ys n j) l (𝓝 (y j))) (hc : ∀ j, Tendsto (fun n => cs n j) l (𝓝 (c j))) (htie : ∀ j, j ≠ i → inner ℝ (y j) x + c j ≠ inner ℝ (y i) x + c i) : ∀ᶠ n in l, x ∈ scoreCell (ys n) (cs n) i ↔ x ∈ scoreCell y c i := by …Mentions: OAI.Problem358.scoreCell
- theorem
OAI.Problem358.ae_eventually_mem_scoreCell_iffline 56Source documentation
Distinct limiting slopes make affine-cell membership stabilize almost everywhere.
theorem ae_eventually_mem_scoreCell_iff {d : ℕ} {ι β : Type*} [Finite ι] (K : Set (E d)) {l : Filter β} {ys : β → ι → E d} {cs : β → ι → ℝ} {y : ι → E d} {c : ι → ℝ} (i : ι) (hinj : Function.Injective y) (hy : ∀ j, Tendsto (fun n => ys n j) l (𝓝 (y j))) (hc : ∀ j, Tendsto (fun n => cs n j) l (𝓝 (c j))) : ∀ᵐ x ∂uniformMeasure K, ∀ᶠ n in l, x ∈ scoreCell (ys n) (cs n) i ↔ x ∈ scoreCell y c i := by …Mentions: OAI.Problem358.scoreCell
- theorem
OAI.Problem358.tendsto_uniformMeasure_scoreCellline 70Source documentation
Cell masses converge under convergence of sites and intercepts, provided only that the limiting sites are distinct and the uniform source is finite.
theorem tendsto_uniformMeasure_scoreCell {d : ℕ} {ι β : Type*} [Finite ι] (K : Set (E d)) {l : Filter β} [l.IsCountablyGenerated] {ys : β → ι → E d} {cs : β → ι → ℝ} {y : ι → E d} {c : ι → ℝ} (i : ι) (hinj : Function.Injective y) (hy : ∀ j, Tendsto (fun n => ys n j) l (𝓝 (y j))) (hc : ∀ j, Tendsto (fun n => cs n j) l (𝓝 (c j))) : Tendsto (fun n => uniformMeasure K (scoreCell (ys n) (cs n) i)) l (𝓝 (uniformMeasure K (scoreCell y c i))) := by …Mentions: OAI.Problem358.scoreCell
- theorem
OAI.Problem358.continuousAt_uniformMeasure_scoreCellline 85Source documentation
Joint continuity in all affine coefficients at configurations with distinct sites.
theorem continuousAt_uniformMeasure_scoreCell {d : ℕ} {ι : Type*} [Finite ι] (K : Set (E d)) (y : ι → E d) (c : ι → ℝ) (i : ι) (hinj : Function.Injective y) : ContinuousAt (fun p : (ι → E d) × (ι → ℝ) => uniformMeasure K (scoreCell p.1 p.2 i)) (y, c) := by …Mentions: OAI.Problem358.scoreCell
- theorem
OAI.Problem358.tendsto_setIntegral_of_ae_eventually_memline 98Source documentation
Dominated convergence for an integrable function over varying measurable sets whose membership stabilizes almost everywhere.
theorem tendsto_setIntegral_of_ae_eventually_mem {X V β : Type*} [MeasurableSpace X] [NormedAddCommGroup V] [NormedSpace ℝ V] {μ : Measure X} {l : Filter β} [l.IsCountablyGenerated] {sets : β → Set X} {s : Set X} (hsets : ∀ n, MeasurableSet (sets n)) (hs : MeasurableSet s) {f : X → V} (hf : Integrable f μ) (hmem : ∀ᵐ x ∂μ, ∀ᶠ n in l, x ∈ sets n ↔ x ∈ s) : Tendsto (fun n => ∫ x in sets n, f x ∂μ) l (𝓝 (∫ x in s, f x ∂μ)) := by … - theorem
OAI.Problem358.tendsto_setIntegral_scoreCellline 122Source documentation
Integrals over affine cells, including their first moments, converge jointly in all coefficients whenever the limiting slopes are distinct.
theorem tendsto_setIntegral_scoreCell {d : ℕ} {ι β V : Type*} [Finite ι] [NormedAddCommGroup V] [NormedSpace ℝ V] (K : Set (E d)) {l : Filter β} [l.IsCountablyGenerated] {ys : β → ι → E d} {cs : β → ι → ℝ} {y : ι → E d} {c : ι → ℝ} (i : ι) (hinj : Function.Injective y) (hy : ∀ j, Tendsto (fun n => ys n j) l (𝓝 (y j))) (hc : ∀ j, Tendsto (fun n => cs n j) l (𝓝 (c j))) {f : E d → V} (hf : Integrable f (uniformMeasure K)) : Tendsto (fun n => ∫ x in scoreCell (ys n) (cs n) i, f x ∂uniformMeasure K) l (𝓝 (∫ x in scoreCell y c i, f x ∂uniformMeasure K)) := …Mentions: OAI.Problem358.scoreCell
- theorem
OAI.Problem358.continuousAt_setIntegral_scoreCellline 137Source documentation
Joint continuity of any integrable moment of a finite affine cell.
theorem continuousAt_setIntegral_scoreCell {d : ℕ} {ι V : Type*} [Finite ι] [NormedAddCommGroup V] [NormedSpace ℝ V] (K : Set (E d)) (y : ι → E d) (c : ι → ℝ) (i : ι) (hinj : Function.Injective y) {f : E d → V} (hf : Integrable f (uniformMeasure K)) : ContinuousAt (fun p : (ι → E d) × (ι → ℝ) => ∫ x in scoreCell p.1 p.2 i, f x ∂uniformMeasure K) (y, c) := by …Mentions: OAI.Problem358.scoreCell
- theorem
OAI.Problem358.eventually_injective_sitesline 151Source documentation
Distinctness of a finite family of sites persists locally.
theorem eventually_injective_sites {d : ℕ} {ι : Type*} [Finite ι] (y : ι → E d) (c : ι → ℝ) (hinj : Function.Injective y) : ∀ᶠ p : (ι → E d) × (ι → ℝ) in 𝓝 (y, c), Function.Injective p.1 := by … - theorem
OAI.Problem358.isOpen_distinct_positive_scoreCellline 171Source documentation
The configurations on which the finite-cell differential calculus is used (distinct sites and strictly positive cell masses) form an open set.
theorem isOpen_distinct_positive_scoreCell {d : ℕ} {ι : Type*} [Finite ι] (K : Set (E d)) : IsOpen {p : (ι → E d) × (ι → ℝ) | Function.Injective p.1 ∧ ∀ i, 0 < uniformMeasure K (scoreCell p.1 p.2 i)} := by …Mentions: OAI.Problem358.scoreCell
- theorem
OAI.Problem358.CellGeometry.closedCell_eq_inter_scoreCellline 193Source documentation
The geometric closed cell is the score cell restricted to the source body.
theorem closedCell_eq_inter_scoreCell (K : Set (E d)) (y : ι → E d) (c : ι → ℝ) (i : ι) : closedCell K y c i = K ∩ scoreCell y c i := by …Mentions: OAI.Problem358.CellGeometry.closedCell, OAI.Problem358.scoreCell
- theorem
OAI.Problem358.CellGeometry.closedCell_ae_eq_scoreCellline 201Source documentation
The two cell conventions agree almost everywhere for the uniform source.
theorem closedCell_ae_eq_scoreCell {K : Set (E d)} (hK : MeasurableSet K) (y : ι → E d) (c : ι → ℝ) (i : ι) : closedCell K y c i =ᵐ[uniformMeasure K] scoreCell y c i := by …Mentions: OAI.Problem358.CellGeometry.closedCell, OAI.Problem358.scoreCell
- theorem
OAI.Problem358.CellGeometry.restrict_closedCell_eq_scoreCellline 209Source documentation
Restricting the uniform source is independent of the cell convention.
theorem restrict_closedCell_eq_scoreCell {K : Set (E d)} (hK : MeasurableSet K) (y : ι → E d) (c : ι → ℝ) (i : ι) : (uniformMeasure K).restrict (closedCell K y c i) = (uniformMeasure K).restrict (scoreCell y c i) := …Mentions: OAI.Problem358.CellGeometry.closedCell, OAI.Problem358.scoreCell
- theorem
OAI.Problem358.CellGeometry.uniformMeasure_closedCell_eq_scoreCellline 216Source documentation
Closed-cell masses are exactly the score-cell masses.
theorem uniformMeasure_closedCell_eq_scoreCell {K : Set (E d)} (hK : MeasurableSet K) (y : ι → E d) (c : ι → ℝ) (i : ι) : uniformMeasure K (closedCell K y c i) = uniformMeasure K (scoreCell y c i) := …Mentions: OAI.Problem358.CellGeometry.closedCell, OAI.Problem358.scoreCell
- theorem
OAI.Problem358.CellGeometry.continuousAt_uniformMeasure_closedCellline 222Source documentation
Joint continuity of the actual geometric closed-cell mass at distinct sites.
theorem continuousAt_uniformMeasure_closedCell [Finite ι] {K : Set (E d)} (hK : MeasurableSet K) (y : ι → E d) (c : ι → ℝ) (i : ι) (hinj : Function.Injective y) : ContinuousAt (fun p : (ι → E d) × (ι → ℝ) => uniformMeasure K (closedCell K p.1 p.2 i)) (y, c) := by …Mentions: OAI.Problem358.CellGeometry.closedCell
- theorem
OAI.Problem358.CellGeometry.continuousAt_real_closedCellline 231Source documentation
Real-valued closed-cell masses are jointly continuous at distinct sites.
theorem continuousAt_real_closedCell [Finite ι] {K : Set (E d)} (hK : MeasurableSet K) (y : ι → E d) (c : ι → ℝ) (i : ι) (hinj : Function.Injective y) : ContinuousAt (fun p : (ι → E d) × (ι → ℝ) => (uniformMeasure K).real (closedCell K p.1 p.2 i)) (y, c) := by …Mentions: OAI.Problem358.CellGeometry.closedCell
- theorem
OAI.Problem358.CellGeometry.continuousAt_setIntegral_closedCellline 244Source documentation
Cell integral continuity transfers to the geometric closed-cell convention.
theorem continuousAt_setIntegral_closedCell [Finite ι] {V : Type*} [NormedAddCommGroup V] [NormedSpace ℝ V] {K : Set (E d)} (hK : MeasurableSet K) (y : ι → E d) (c : ι → ℝ) (i : ι) (hinj : Function.Injective y) {f : E d → V} (hf : Integrable f (uniformMeasure K)) : ContinuousAt (fun p : (ι → E d) × (ι → ℝ) => ∫ x in closedCell K p.1 p.2 i, f x ∂uniformMeasure K) (y, c) := by …Mentions: OAI.Problem358.CellGeometry.closedCell
- theorem
OAI.Problem358.CellGeometry.continuousAt_firstMoment_closedCellline 255Source documentation
The actual first moment of a closed cell is jointly continuous.
theorem continuousAt_firstMoment_closedCell [Finite ι] {K : Set (E d)} (hK : IsCompact K) (y : ι → E d) (c : ι → ℝ) (i : ι) (hinj : Function.Injective y) : ContinuousAt (fun p : (ι → E d) × (ι → ℝ) => ∫ x in closedCell K p.1 p.2 i, x ∂uniformMeasure K) (y, c) := …Mentions: OAI.Problem358.CellGeometry.closedCell
- theorem
OAI.Problem358.CellGeometry.isOpen_distinct_positive_real_closedCellline 265Source documentation
The admissible locus used by geometric cell calculus is open, in the real-mass convention of the normalized implicit-function construction.
theorem isOpen_distinct_positive_real_closedCell [Finite ι] {K : Set (E d)} (hK : MeasurableSet K) : IsOpen {p : (ι → E d) × (ι → ℝ) | Function.Injective p.1 ∧ ∀ i, 0 < (uniformMeasure K).real (closedCell K p.1 p.2 i)} := by …Mentions: OAI.Problem358.CellGeometry.closedCell
- theorem
OAI.Problem358.CellGeometry.eventually_real_closedCell_comparableline 282Source documentation
All positive cell masses simultaneously stay between half and twice their original masses in a neighborhood of a distinct-site configuration.
theorem eventually_real_closedCell_comparable [Finite ι] {K : Set (E d)} (hK : MeasurableSet K) (y : ι → E d) (c : ι → ℝ) (hinj : Function.Injective y) (hpos : ∀ i, 0 < (uniformMeasure K).real (closedCell K y c i)) : ∀ᶠ p : (ι → E d) × (ι → ℝ) in 𝓝 (y, c), ∀ i, (uniformMeasure K).real (closedCell K y c i) / 2 < (uniformMeasure K).real (closedCell K p.1 p.2 i) ∧ (uniformMeasure K).real (closedCell K p.1 p.2 i) < 2 * (uniformMeasure K).real (closedCell K y c i) := by …Mentions: OAI.Problem358.CellGeometry.closedCell