import Mathlib import OAI.Geometry.CAT0Fillings.Currents.GeneralPush import OAI.Geometry.CAT0Fillings.Radial.MassComparison import OAI.Geometry.CAT0Fillings.Slicing.IntegralBoundary import OAI.Geometry.CAT0Fillings.Swept.WholeMass namespace OAI section open Set Filter MeasureTheory Matrix open scoped Topology NNReal BigOperators namespace CAT0Fillings open CurrentOperations variable {X : Type*} [MetricSpace X] [MeasurableSpace X] [BorelSpace X] [CompactSpace X] [Nonempty X] {k : ℕ} structure ChartGeometry {T : Functional X k} (hT : IsMetricCurrent T) where chart : ℕ → IntegerChart X k field : ℕ → Euc k → Seminorm ℝ (Euc k) disjoint : Pairwise (fun i j => Disjoint (chart i).image (chart j).image) summable : Summable (fun i => mass (chart i).action) action : ∀ b π, T b π = ∑' i, (chart i).action b π measurable : ∀ i v, Measurable (fun z => field i z v) differential : ∀ i, ∀ᵐ z ∂volume.restrict (chart i).domain, (∀ hz : z ∈ (chart i).domain, MetricDifferentiation.HasCenteredMetricDifferentialWithin (chart i).domain (chart i).param (field i z) ⟨z,hz⟩) ∧ (∀ u v, field i z (u+v)^2+field i z (u-v)^2 = 2*field i z u^2+2*field i z v^2) ∧ (∀ v, field i z v = 0 ↔ v = 0) integrable : ∀ i, Integrable (fun z => |((chart i).multiplicity z : ℝ)| *Real.sqrt (polarizationMatrix (field i z) (EuclideanSpace.basisFun (Fin k) ℝ).toBasis).det) (volume.restrict (chart i).domain) chart_mass : ∀ i, mass (chart i).action = ∫ z, |((chart i).multiplicity z : ℝ)| *Real.sqrt (polarizationMatrix (field i z) (EuclideanSpace.basisFun (Fin k) ℝ).toBasis).det ∂volume.restrict (chart i).domain measure_eq : MassMeasure.currentMassMeasure hT = Measure.sum (fun i => (chart i).majorantMeasure (fun z => Real.sqrt (polarizationMatrix (field i z) (EuclideanSpace.basisFun (Fin k) ℝ).toBasis).det)) total_mass : mass T = ∑' i, mass (chart i).action current : ∀ i, IsMetricCurrent (chart i).action control : ∀ i, Controls (chart i).action ((chart i).majorantMeasure (fun z => Real.sqrt (polarizationMatrix (field i z) (EuclideanSpace.basisFun (Fin k) ℝ).toBasis).det)) theorem exists_chartGeometry {T : Functional X k} (hX : IsCAT0 X) (hT : IsMetricCurrent T) (hr : IntegerRectifiable T) : Nonempty (ChartGeometry hT) := by classical obtain ⟨C,hdis,hC,hsum,heq⟩ := hr choose P hPm hP hρ hfin hcontrol hmin hfield using fun i => (C i).exists_exact_quadratic_mass hX (hC i) choose p hPeq hpm hp using hfield simp only [hPeq] at hρ hfin hcontrol hmin let J (i : ℕ) (z : Euc k) := Real.sqrt (polarizationMatrix (p i z) (EuclideanSpace.basisFun (Fin k) ℝ).toBasis).det have hmass (i : ℕ) : mass (C i).action = ∫ z, |((C i).multiplicity z : ℝ)| *J i z ∂volume.restrict (C i).domain := (C i).mass_eq_integral_majorant (hC i) (hρ i) (Eventually.of_forall fun _ => Real.sqrt_nonneg _) (hcontrol i) (hmin i) let μ (i : ℕ) : Measure X := (C i).majorantMeasure (J i) have hμfin : ∀ i, IsFiniteMeasure (μ i) := hfin let := hμfin have htot (i : ℕ) : (μ i).real univ = mass (C i).action := by have heqm : MassMeasure.currentMassMeasure (hC i) = μ i := by apply le_antisymm (MassMeasure.currentMassMeasure_le (hC i) (hcontrol i)) exact hmin i _ inferInstance (MassMeasure.currentMassMeasure_controls (hC i)) rw [←heqm] exact MassMeasure.currentMassMeasure_total _ have hμsum : Summable (fun i => (μ i).real univ) := by simpa only [htot] using hsum let := finite_sum_measure_of_summable_total μ hμsum have hmeasure : MassMeasure.currentMassMeasure hT = Measure.sum μ := by apply le_antisymm · exact MassMeasure.currentMassMeasure_le hT (controls_sum_general hcontrol heq) · exact sum_measure_le_of_component_minimal hC hcontrol hmin heq (fun i => (C i).measurableSet_image) hdis (fun i => (C i).majorantMeasure_ae_image _) (MassMeasure.currentMassMeasure_controls hT) have htotal : mass T = ∑' i, mass (C i).action := by rw [←MassMeasure.currentMassMeasure_total hT,hmeasure] rw [measureReal_def,Measure.sum_apply _ MeasurableSet.univ, ENNReal.tsum_toReal_eq (fun i => measure_ne_top (μ i) univ)] exact tsum_congr htot exact ⟨⟨C,p,hdis,hsum,heq,hpm,hp,hρ,hmass,hmeasure,htotal,hC,hcontrol⟩⟩ namespace ChartGeometry variable {T : Functional X k} {hT : IsMetricCurrent T} (q : ChartGeometry hT) noncomputable def gram (i : ℕ) (z : Euc k) : Matrix (Fin k) (Fin k) ℝ := polarizationMatrix (q.field i z) (EuclideanSpace.basisFun (Fin k) ℝ).toBasis noncomputable def density (i : ℕ) (z : Euc k) : ℝ := |((q.chart i).multiplicity z : ℝ)| *Real.sqrt (q.gram i z).det lemma density_integrable (i : ℕ) : Integrable (q.density i) (volume.restrict (q.chart i).domain) := q.integrable i lemma density_summable : Summable (fun i => ∫ z, q.density i z ∂volume.restrict (q.chart i).domain) := by simpa only [density,gram,q.chart_mass] using q.summable lemma density_mass : mass T = ∑' i, ∫ z, q.density i z ∂volume.restrict (q.chart i).domain := by simpa only [density,gram,q.chart_mass] using q.total_mass end ChartGeometry end CAT0Fillings end section open Set Filter MeasureTheory open scoped Topology NNReal BigOperators namespace CAT0Fillings open CurrentOperations variable {X : Type*} [MetricSpace X] [MeasurableSpace X] [BorelSpace X] [CompactSpace X] [Nonempty X] {k : ℕ} omit [MeasurableSpace X] [BorelSpace X] [CompactSpace X] [Nonempty X] in lemma endpoint_lipschitz [MeasurableSpace X] [BorelSpace X] [CompactSpace X] [Nonempty X] (t : Icc (0:ℝ) 1) : LipschitzWith 1 (fun y : X => (t,y) : X → ClosedCylinder X) := by simpa using (LipschitzWith.const t).prodMk (LipschitzWith.id : LipschitzWith 1 (id : X → X)) theorem swept_boundary_integral {T : Functional X (k+1)} (hT : IsIntegral (k+1) T) (hz : boundarySucc T = 0) (C : ℕ → IntegerChart X (k+1)) (hd : Pairwise (fun i j => Disjoint (C i).image (C j).image)) (hs : Summable (fun i => mass (C i).action)) (heq : ∀ b π, T b π = ∑' i, (C i).action b π) (F : ClosedCylinder X → X) {K : ℝ≥0} (hF : LipschitzWith K F) (hF0 : ∀ y, F (⟨0,by constructor <;> norm_num⟩,y) = y) : IsIntegral (k+2) (pushCurrent F (closedPrismFamily C)) ∧ boundarySucc (pushCurrent F (closedPrismFamily C)) = pushCurrent (fun y => F (⟨1,by constructor <;> norm_num⟩,y)) T - T := by let f : X → X := fun y => F (⟨1,by constructor <;> norm_num⟩,y) have hf : LipschitzWith K f := by simpa only [mul_one,Function.comp_def,f] using hF.comp (endpoint_lipschitz (X := X) ⟨1,by constructor <;> norm_num⟩) let : Nonempty (ClosedCylinder X) := ⟨(⟨0,by constructor <;> norm_num⟩,Classical.choice inferInstance)⟩ have hb : boundarySucc (pushCurrent F (closedPrismFamily C)) = pushCurrent f T - T := by funext b π by_cases hab : Admissible b π · rw [pushCurrent_boundarySucc _ hF,pushCurrent_apply _ _ hab, closedPrismFamily_boundary_cycle hT.1 hT.2.1 hz C hs heq _ _ (admissible_comp hab hF)] simp only [Pi.sub_apply,pushCurrent_apply _ _ hab,Function.comp_apply,hF0,f] rfl · simp only [boundarySucc,Pi.sub_apply,pushCurrent,ite_eq_right hab, hT.1.offDomain b π hab,sub_self] have hbi := (integral_push hT hf).sub hT refine ⟨⟨pushCurrent_isMetricCurrent (closedPrismFamily_current C hs) hF, integerRectifiable_push (closedPrismFamily_rectifiable C hd hs) hF,?_,?_⟩,hb⟩ · rw [hb]; exact hbi.1 · rw [hb]; exact hbi.2.1 end CAT0Fillings end section open Set Filter MeasureTheory Matrix open scoped Topology NNReal BigOperators namespace CAT0Fillings open CurrentOperations variable {X : Type*} [MetricSpace X] [MeasurableSpace X] [BorelSpace X] [CompactSpace X] [Nonempty X] {k : ℕ} namespace ChartGeometry variable {T : Functional X k} {hT : IsMetricCurrent T} (q : ChartGeometry hT) noncomputable def sweptMass (o : X) (g : X → ℝ) : ℝ := ∑' i, ∫ z, |((q.chart i).multiplicity z : ℝ)| *(q.chart i).sweptWeight (q.field i) o g z ∂volume.restrict (q.chart i).domain lemma swept_integrable_summable (o : X) {g : X → ℝ} {K : ℝ≥0} (hg : LipschitzWith K g) (hg0 : ∀ y, 0 ≤ g y) : (∀ i, Integrable (fun z => |((q.chart i).multiplicity z : ℝ)| * (q.chart i).sweptWeight (q.field i) o g z) (volume.restrict (q.chart i).domain)) ∧ Summable (fun i => ∫ z, |((q.chart i).multiplicity z : ℝ)| * (q.chart i).sweptWeight (q.field i) o g z ∂volume.restrict (q.chart i).domain) := by obtain ⟨B,hB⟩ := isCompact_univ.exists_bound_of_continuousOn ((continuous_const.dist continuous_id).mul hg.continuous).continuousOn apply summable_swept_integrals q.chart q.field q.measurable q.differential q.integrable q.density_summable o hg hg0 intro y exact (le_abs_self _).trans (by simpa only [Real.norm_eq_abs,Pi.mul_apply,id_eq] using hB y (mem_univ y)) lemma sweptMass_nonneg (o : X) {g : X → ℝ} (hg0 : ∀ y, 0 ≤ g y) : 0 ≤ q.sweptMass o g := by apply tsum_nonneg intro i apply integral_nonneg_of_ae filter_upwards [(q.chart i).ae_sweptWeight_nonneg (q.field i) o hg0] with z hz exact mul_nonneg (abs_nonneg _) hz lemma sweptMass_const_mul (o : X) (g : X → ℝ) (h : ℝ) : q.sweptMass o (fun y => h*g y) = h*q.sweptMass o g := by have hs (C : IntegerChart X k) : C.scalar (fun y => h*g y) = fun z => h*C.scalar g z := by funext z by_cases hz : z ∈ C.domain <;> simp [IntegerChart.scalar,hz] simp only [sweptMass,IntegerChart.sweptWeight,hs] simp_rw [show ∀ (a b c d e : ℝ), a*(b*(h*c)*d*e) = h*(a*(b*c*d*e)) by intros; ring] simp only [integral_const_mul,tsum_mul_left] end ChartGeometry theorem exists_swept_current {T : Functional X (k+1)} (hT : IsIntegral (k+1) T) (hz : boundarySucc T = 0) (q : ChartGeometry hT.1) (seg : X → X → ℝ → X) (hseg : ∀ o x a b, a ∈ Icc (0:ℝ) 1 → b ∈ Icc (0:ℝ) 1 → dist (seg o x a) (seg o x b) = |a-b| *dist o x) (hcomp : ∀ o x y a b, a ∈ Icc (0:ℝ) 1 → b ∈ Icc (0:ℝ) 1 → dist (seg o x a) (seg o y b)^2 ≤ (a*dist o x-b*dist o y)^2+ a*b*(dist x y^2-(dist o x-dist o y)^2)) (hseg1 : ∀ o x, seg o x 1 = x) (o : X) {g : X → ℝ} {K : ℝ≥0} (hg : LipschitzWith K g) (hg0 : ∀ y, 0 ≤ g y) (hg1 : ∀ y, g y ≤ 1) : ∃ S : Functional X (k+2), IsIntegral (k+2) S ∧ boundarySucc S = pushCurrent (fun y => seg o y (1-g y)) T - T ∧ mass S ≤ q.sweptMass o g := by obtain ⟨F,⟨L,hF⟩,hFeq,hFcl⟩ := exists_swept_radial_map seg hseg hcomp o hg hg0 hg1 have hF0 : ∀ y, F (⟨0,by constructor <;> norm_num⟩,y) = y := by intro y rw [hFeq] simp only [zero_mul,sub_zero,hseg1] obtain ⟨hS,hb⟩ := swept_boundary_integral hT hz q.chart q.disjoint q.summable q.action F hF hF0 obtain ⟨hI,hIs⟩ := q.swept_integrable_summable o hg hg0 refine ⟨pushCurrent F (closedPrismFamily q.chart),hS,?_,?_⟩ · simpa only [hFeq,one_mul] using hb · exact whole_swept_mass_le q.chart q.summable seg hcomp o g hg hg0 hg1 F hF hFcl q.field hI hIs q.differential end CAT0Fillings end end OAI