import Mathlib import OAI.Analysis.HardSphere.Allocation.PhysicalCodedMoment import OAI.Analysis.HardSphere.Comparison.PhysicalObservedLaw namespace OAI section noncomputable section open MeasureTheory ProbabilityTheory Set open scoped ENNReal namespace HardSphere.Groups open Wiener Bridge Sampling Comparison GaussianPacking PathCutoff CellOrbital _root_.OAI.HardSphere.Lattice attribute [local instance] Classical.propDecidable variable {K : ℕ} [NeZero K] {x y : DiscreteTorus K} variable {J : Type*} [Fintype J] [DecidableEq J] def physicalCodeTag {N : ℕ} (particle : J↪Fin (N+1)) (hxy : x≠y) (b : Bool) (c : PhysicalRouteCode x y J) : Fin (N+1) := if h : RouteFieldValid c.1 c.2 then particle (fieldRouteLabels hxy c.1 c.2 h (if b then 0 else Fin.last (c.1.val.length-1))) else 0 def taggedPhysicalBathKernel {N M G : ℕ} {L : Length} (particle : J↪Fin (N+1)) (b : Bool) : Kernel (Fin (N+1)×(PhysicalDatum (N+1) K M G L×(Option J→C(Time,Point)))) (Torus L×Torus L×(Fin N→Torus L)) where toFun z := primaryBathKernel b z.1 (physicalFullMidpoint particle z.2) measurable' := measurable_from_prod_countable_right fun i ↦ (primaryBathKernel b i).measurable.comp (physicalFullMidpoint_measurable particle) instance taggedPhysicalBathKernel_markov {N M G : ℕ} {L : Length} (particle : J↪Fin (N+1)) (b : Bool) : IsMarkovKernel (taggedPhysicalBathKernel (K:=K) (M:=M) (G:=G) (L:=L) particle b) := ⟨fun z ↦ inferInstanceAs (IsProbabilityMeasure (primaryBathKernel b z.1 (physicalFullMidpoint particle z.2)))⟩ def physicalCodeObserver {N M G : ℕ} {L : Length} (particle : J↪Fin (N+1)) (hxy : x≠y) (b : Bool) : Kernel (PhysicalDatum (N+1) K M G L×(PhysicalRouteCode x y J×((Option J→C(Time,Point))×(Option J→C(Time,Point))))) (Torus L×Torus L×(Fin N→Torus L)) := (taggedPhysicalBathKernel particle b).comap (fun z ↦ (physicalCodeTag particle hxy b z.2.1,(z.1,if b then z.2.2.1 else z.2.2.2))) (by apply Measurable.prodMk · exact (measurable_of_countable (physicalCodeTag particle hxy b)).comp measurable_snd.fst · cases b <;> simp only [Bool.false_eq_true,ite_false,ite_true] <;> exact measurable_fst.prodMk (by fun_prop)) instance physicalCodeObserver_markov {N M G : ℕ} {L : Length} (particle : J↪Fin (N+1)) (hxy : x≠y) (b : Bool) : IsMarkovKernel (physicalCodeObserver (M:=M) (G:=G) (L:=L) particle hxy b) := by unfold physicalCodeObserver; infer_instance theorem physicalCodedRoute_same_observed {N M G : ℕ} {L : Length} (hL : L.val=(K:ℝ)) (g : Fin G) (m : ℕ) (t r R C S : ℝ) (ht : 0 (funext w simp only [physicalCodeObserver,Kernel.comap_apply,taggedPhysicalBathKernel,Kernel.coe_mk, physicalCodeTag,dite_eq_left hv,ite_true,Bool.false_eq_true,ite_false,physicalBathKernel]) end HardSphere.Groups end end section noncomputable section open MeasureTheory ProbabilityTheory Set open scoped ENNReal namespace HardSphere.Groups open Wiener Bridge Sampling Comparison GaussianPacking PathCutoff CellOrbital _root_.OAI.HardSphere.Lattice attribute [local instance] Classical.propDecidable variable {K : ℕ} [NeZero K] {x y : DiscreteTorus K} variable {J : Type*} [Fintype J] [DecidableEq J] omit [NeZero K] in lemma unitTarget_project {L : Length} (hL : 1≤L.val) (v : Fin 3→Fin K) (z : Point) (hz : z∈unitTarget (anchorPoint v)) : projectPoint L z∈centeredCell L (gridCenter L v) := by rw [centeredCell_image hL] intro j have hj := hz j (mem_univ j) refine ⟨z j-(v j:ℝ),⟨?_,?_⟩,?_⟩ · change (v j:ℝ)-1/2≤z j ∧ z j<(v j:ℝ)+1/2 at hj linarith [hj.1] · change (v j:ℝ)-1/2≤z j ∧ z j<(v j:ℝ)+1/2 at hj linarith [hj.2] · change ((z j-(v j:ℝ):ℝ):AddCircle L.val)=((z j:ℝ):AddCircle L.val)-((v j:ℝ):AddCircle L.val) exact QuotientAddGroup.mk_sub _ _ _ omit [NeZero K] in lemma cellPathReference_support {L : Length} (hL : 1≤L.val) (v : Fin 3→Fin K) : ∀ᵐp ∂cellPathReference v,projectPoint L (p midpointTime)∈centeredCell L (gridCenter L v) := by have hm : Measurable (fun p : C(Time,Point) ↦ projectPoint L (p midpointTime)) := (projectPoint_continuous L).measurable.comp (continuous_eval_const midpointTime).measurable rw [cellPathReference,ae_map_iff pointAsPath_measurable.aemeasurable ((centeredCell_measurable L _).preimage hm)] unfold targetUniform apply Measure.ae_smul_measure filter_upwards [ae_restrict_mem (unitTarget_measurable (anchorPoint v))] with z hz exact unitTarget_project hL v z hz omit [DecidableEq J] in lemma physicalPrimary_extra {N M G : ℕ} {L : Length} (hL : L.val=(K:ℝ)) (g : Fin G) (m : ℕ) (t r R C S : ℝ) (u : Time) (particle : J↪Fin N) (v : Fin 3→Fin K) (d : PhysicalDatum N K M G L) : ∀ᵐw ∂physicalPrimaryReference hL g m t r R C S u particle v d, physicalFullMidpoint particle (d,w) none∈centeredCell L (gridCenter L v) := by have hL1 : 1≤L.val := by rw [hL]; exact_mod_cast NeZero.pos K have hextra := (Measure.quasiMeasurePreserving_eval (fun i ↦ physicalSlotReference hL g m t r R C S u particle v i d) none).ae (cellPathReference_support hL1 v) rw [physicalPrimaryReference_apply,conditionedMeasure] apply Measure.ae_smul_measure filter_upwards [ae_restrict_of_ae hextra] with w hw change fillGroup particle _ _ (optionParticle particle none)∈_ rw [fillGroup_selected] exact hw def physicalTagEvent {N M G : ℕ} {L : Length} (particle : J↪Fin N) (v : Fin 3→Fin K) (i : Fin N) : Set (PhysicalDatum N K M G L×(Option J→C(Time,Point))) := {z | i∈Set.range particle ∧ physicalFullMidpoint particle z (some i)∈centeredCell L (gridCenter L v)} omit [NeZero K] [DecidableEq J] in lemma physicalTagEvent_measurable {N M G : ℕ} {L : Length} (particle : J↪Fin N) (v : Fin 3→Fin K) (i : Fin N) : MeasurableSet (physicalTagEvent (M:=M) (G:=G) (L:=L) particle v i) := .inter (show MeasurableSet {z : PhysicalDatum N K M G L×(Option J→C(Time,Point)) | i∈Set.range particle} from by by_cases h : i∈Set.range particle <;> simp [h]) ((centeredCell_measurable L _).preimage ((measurable_pi_apply (some i)).comp (physicalFullMidpoint_measurable particle))) theorem physicalCodedRoute_tag_support {N M G : ℕ} {L : Length} (hL : L.val=(K:ℝ)) (g : Fin G) (m : ℕ) (t r R C S : ℝ) (ht : 0 simp <;> fun_prop have hm : Measurable (fun w : Option J→C(Time,Point) ↦ physicalFullMidpoint particle (d,w) none) := (measurable_pi_apply none).comp ((physicalFullMidpoint_measurable particle).comp measurable_prodMk_left) have h' := (ae_map_iff hf.aemeasurable ((centeredCell_measurable L _).preimage hm)).mp h cases b <;> simpa using h' have hv := routeFieldValid_of_supported hL g m t r R C S u particle d p z hz ha have hh := fieldRouteLabels_physical hL g m t r R C S u particle d hxy p z hz ha hv have hmid := physicalPairedRoute_midpoint hL g m t r R C S ht u particle (fieldRouteLabels hxy p z hv) (simpleRouteVertices p (p.val.length-1)) (simpleRouteSteps hL p _ (simpleRouteLength_eq hxy p)) (simpleRouteSteps_period hL p _ (simpleRouteLength_eq hxy p)) d (fun i ↦ (hh i).1) (fun i ↦ (hh i).2) have hmid' : ∀ᵐw ∂physicalCodedRoute hL g m t r R C S u particle hxy (p,z) d, ∀i,physicalFullMidpoint particle (d,w.2) i=physicalFullMidpoint particle (d,w.1) (routePermutation ((fieldRouteLabels hxy p z hv).trans particle) i) := by simpa only [physicalCodedRoute,dite_eq_left hv] using hmid filter_upwards [he true,he false,hmid'] with w h1 h2 hm cases b with | true => simp only [physicalTagEvent,mem_ofPred_eq,physicalCodeTag,dite_eq_left hv,ite_true] refine ⟨⟨_,rfl⟩,?_⟩ have H := hm none rw [routePermutation_star] at H simp only [Function.Embedding.trans_apply] at H change physicalFullMidpoint particle (d,w.1) (some (particle (fieldRouteLabels hxy p z hv 0)))∈_ rw [←H] exact h2 | false => simp only [physicalTagEvent,mem_ofPred_eq,physicalCodeTag,dite_eq_left hv,Bool.false_eq_true,ite_false] refine ⟨⟨_,rfl⟩,?_⟩ have H := hm (some (particle (fieldRouteLabels hxy p z hv (Fin.last (p.val.length-1))))) change physicalFullMidpoint particle (d,w.2) (some (((fieldRouteLabels hxy p z hv).trans particle) (Fin.last (p.val.length-1)))) = physicalFullMidpoint particle (d,w.1) (routePermutation ((fieldRouteLabels hxy p z hv).trans particle) (some (((fieldRouteLabels hxy p z hv).trans particle) (Fin.last (p.val.length-1))))) at H rw [routePermutation_lastLabel] at H simp only [Function.Embedding.trans_apply] at H rw [H] exact h1 end HardSphere.Groups end end end OAI