import Mathlib import OAI.Analysis.CoulombIonization.FieldAnalysis.BarrierObservationTowerBarrier import OAI.Analysis.CoulombIonization.RadialBounds.Error namespace OAI noncomputable section open MeasureTheory Filter open scoped Topology BigOperators ContDiff open MeasureTheory Filter Set Metric ProbabilityTheory open scoped BigOperators Topology namespace CoulombBarrier open CoulombAtom CoulombAnalysis variable {Ω D : Type*} [MeasurableSpace Ω] [StandardBorelSpace Ω] [Nonempty Ω] variable [MeasurableSpace D] (P : Measure Ω) [IsProbabilityMeasure P] variable (X : Ω → D) (hX : Measurable X) lemma conditionalField_nonneg {p : Ω → TFSpace → ℝ} (hn : ∀ sample x, 0 ≤ p sample x) (d : D) (x : TFSpace) : 0 ≤ conditionalField P X p d x := integral_nonneg (fun sample => hn sample x) lemma conditionalField_support {p : Ω → TFSpace → ℝ} {R : ℝ} (hs : ∀ sample x, R < ‖x‖ → p sample x = 0) (d : D) (x : TFSpace) (hx : R < ‖x‖) : conditionalField P X p d x = 0 := by simp only [conditionalField,hs _ x hx,integral_zero] include hX lemma conditionalField_expectation {p : Ω → TFSpace → ℝ} (hm : Measurable (Function.uncurry p)) (hb : DeterministicLocalBound p) (x : TFSpace) : (∫ sample, conditionalField P X p (X sample) x ∂P) = ∫ sample, p sample x ∂P := by rw [←integral_congr_ae (conditionalField_eq_condExp P hX hm hb x)] exact integral_condExp hX.comap_le theorem conditionalField_totalMass {p : Ω → TFSpace → ℝ} (hm : Measurable (Function.uncurry p)) (hb : DeterministicLocalBound p) {R : ℝ} (hs : ∀ sample x, R < ‖x‖ → p sample x = 0) : (∫ sample, (∫ x, conditionalField P X p (X sample) x) ∂P) = ∫ sample, (∫ x, p sample x) ∂P := by have hcm : Measurable (fun z : Ω × TFSpace => conditionalField P X p (X z.1) z.2) := (conditionalField_measurable P X hm).comp ((hX.comp measurable_fst).prodMk measurable_snd) have hcb : DeterministicLocalBound (fun sample x => conditionalField P X p (X sample) x) := by intro K hK obtain ⟨C,hC⟩ := conditionalField_bound P X hb K hK exact ⟨C,fun sample x hx => hC (X sample) x hx⟩ have hcs : ∀ sample x, R < ‖x‖ → conditionalField P X p (X sample) x = 0 := fun sample x hx => conditionalField_support P X hs (X sample) x hx rw [integral_integral_swap (compactBound_integrable_prod hcm hcb hcs), integral_integral_swap (compactBound_integrable_prod hm hb hs)] exact integral_congr_ae (Eventually.of_forall fun x => conditionalField_expectation P X hX hm hb x) theorem conditionalField_spatial_bounds {u : Ω → TFSpace → ℝ} (hm : Measurable (Function.uncurry u)) (hb : DeterministicLocalBound u) (V a b : TFSpace → ℝ) (A : Set TFSpace) (hlo : ∀ᵐ sample ∂P, ∀ x ∈ A, a x ≤ V x+u sample x) (hhi : ∀ᵐ sample ∂P, ∀ x ∈ A, V x+u sample x ≤ b x) : ∀ᵐ d ∂P.map X, ∀ x ∈ A, a x ≤ V x+conditionalField P X u d x ∧ V x+conditionalField P X u d x ≤ b x := by filter_upwards [conditional_all_properties P hX hlo,conditional_all_properties P hX hhi] with d hdlo hdhi intro x hx have hi := (integrable_const (V x) : Integrable (fun _ : Ω => V x) (condDistrib id X P d)).add (deterministicBound_integrable_section hm hb x) have he : (∫ sample, (V x+u sample x) ∂condDistrib id X P d) = V x+conditionalField P X u d x := by rw [integral_add (integrable_const _) (deterministicBound_integrable_section hm hb x)] simp [conditionalField] constructor · rw [←he] simpa only [integral_const,probReal_univ,one_smul,Pi.add_apply] using integral_mono_ae (integrable_const (a x)) hi (hdlo.mono fun sample hω => hω x hx) · rw [←he] simpa only [integral_const,probReal_univ,one_smul,Pi.add_apply] using integral_mono_ae hi (integrable_const (b x)) (hdhi.mono fun sample hω => hω x hx) end CoulombBarrier end end OAI