openAI-math-dataset / lean /OAI /Combinatorics /ContingencyTables /Rooted /LargePairEnumeration.lean
Download lean/OAI/Combinatorics/ContingencyTables/Rooted/LargePairEnumeration.lean from roseking/openAI-math-dataset: direct link, hf CLI and curl.
- Browser
- Download file 6.85 kB
-
https://huggingface.co/datasets/roseking/openAI-math-dataset/resolve/main/lean/OAI/Combinatorics/ContingencyTables/Rooted/LargePairEnumeration.lean
- Command line
-
hf download hf://datasets/roseking/openAI-math-dataset/lean/OAI/Combinatorics/ContingencyTables/Rooted/LargePairEnumeration.lean
-
curl -L -o LargePairEnumeration.lean https://huggingface.co/datasets/roseking/openAI-math-dataset/resolve/main/lean/OAI/Combinatorics/ContingencyTables/Rooted/LargePairEnumeration.lean
6.85 kB
| import OAI.Combinatorics.ContingencyTables.Transport.BalancedEnumeration | |
| import Mathlib.Logic.Equiv.Fin.Basic | |
| namespace OAI | |
| /-! | |
| # Physical indexing of all balanced large-cell pairs | |
| The recursively added pairs are identified with the actual finite cells, | |
| and their assignments with the dependent product of the physical finite | |
| intervals. No extra coordinate or assignment multiplicity is introduced. | |
| -/ | |
| namespace ContingencyTables.LargePairEnumeration | |
| open scoped BigOperators Classical | |
| open BalancedFamily BalancedEnumeration IntegerMarginal | |
| universe u | |
| /-- Widths in the explicit order supplied by a finite cell enumeration. -/ | |
| def widths : {n : ℕ} → (Fin n → ℕ) → List ℕ | |
| | 0,_ => [] | |
| | _+1,M => M 0::widths (fun i => M i.succ) | |
| lemma widths_lower {n : ℕ} (M : Fin n → ℕ) (h : ∀ i, 2≤M i) : | |
| ∀ w ∈ widths M, 2≤w := by | |
| induction n with | |
| | zero => intro w hw; exact False.elim (List.not_mem_nil hw) | |
| | succ n ih => | |
| intro w hw | |
| simp only [widths,List.mem_cons] at hw | |
| rcases hw with rfl|hw | |
| · exact h 0 | |
| · exact ih (fun i => M i.succ) (fun i => h i.succ) w hw | |
| private def pairSuccEquiv (n : ℕ) : ((Fin n×Bool)⊕Bool) ≃ Fin (n+1)×Bool where | |
| toFun | |
| | .inl (i,b) => (i.succ,b) | |
| | .inr b => (0,b) | |
| invFun p := Fin.cases (.inr p.2) (fun i => .inl (i,p.2)) p.1 | |
| left_inv p := by cases p with | |
| | inl p => rcases p with ⟨i,b⟩; rfl | |
| | inr b => rfl | |
| right_inv p := by | |
| rcases p with ⟨i,b⟩ | |
| refine Fin.cases ?_ (fun j => ?_) i <;> rfl | |
| /-- The nested coordinate sums contain exactly the retained coordinates | |
| and one doubled coordinate for each physical large cell. -/ | |
| def coordinateEquiv (S : Type u) : {n : ℕ} → (M : Fin n → ℕ) → | |
| Coordinates S (widths M) ≃ S⊕(Fin n×Bool) | |
| | 0,_ => (Equiv.sumEmpty S (Fin 0×Bool)).symm | |
| | n+1,M => | |
| (Equiv.sumCongr (coordinateEquiv S (fun i => M i.succ)) (Equiv.refl Bool)).trans | |
| ((Equiv.sumAssoc S (Fin n×Bool) Bool).trans | |
| (Equiv.sumCongr (Equiv.refl S) (pairSuccEquiv n))) | |
| /-- Balanced choices are the dependent product of the actual intervals. -/ | |
| def assignmentEquiv : {n : ℕ} → (M : Fin n → ℕ) → | |
| Assignments (widths M) ≃ ((i : Fin n) → Fin (M i+1)) | |
| | 0,_ => | |
| { toFun := fun _ i => Fin.elim0 i | |
| invFun := fun _ => PUnit.unit | |
| left_inv := by intro a; cases a; rfl | |
| right_inv := by intro a; funext i; exact Fin.elim0 i } | |
| | n+1,M => | |
| { toFun := fun a => Fin.cases a.2 (assignmentEquiv (fun i => M i.succ) a.1) | |
| invFun := fun a => ((assignmentEquiv (fun i => M i.succ)).symm (fun i => a i.succ),a 0) | |
| left_inv := by intro a; simp only [Fin.cases_zero,Fin.cases_succ,Equiv.symm_apply_apply]; exact Prod.eta a | |
| right_inv := by | |
| intro a | |
| funext i | |
| refine Fin.cases ?_ (fun j => ?_) i | |
| · rfl | |
| · exact congrFun ((assignmentEquiv (fun i => M i.succ)).apply_symm_apply | |
| (fun i => a i.succ)) j } | |
| def joinedProfile {S : Type*} {n : ℕ} (M : Fin n → ℕ) (z : S → ℕ) | |
| (a : (i : Fin n) → Fin (M i+1)) : S⊕(Fin n×Bool) → ℕ | |
| | .inl s => z s | |
| | .inr (i,b) => if b then M i-(a i).val else (a i).val | |
| lemma embedding_coordinate {S : Type*} {n : ℕ} (M : Fin n → ℕ) (z : S → ℕ) | |
| (a : (i : Fin n) → Fin (M i+1)) (c : Coordinates S (widths M)) : | |
| embedding (widths M) z ((assignmentEquiv M).symm a) c= | |
| joinedProfile M z a (coordinateEquiv S M c) := by | |
| induction n with | |
| | zero => rfl | |
| | succ n ih => | |
| cases c with | |
| | inl c => | |
| change embedding (widths (fun i => M i.succ)) z | |
| ((assignmentEquiv (fun i => M i.succ)).symm (fun i => a i.succ)) c=_ | |
| rw [ih] | |
| change joinedProfile (fun i => M i.succ) z (fun i => a i.succ) | |
| (coordinateEquiv S (fun i => M i.succ) c)= | |
| joinedProfile M z a (((Equiv.sumAssoc S (Fin n×Bool) Bool).trans | |
| (Equiv.sumCongr (Equiv.refl S) (pairSuccEquiv n))) | |
| (.inl (coordinateEquiv S (fun i => M i.succ) c))) | |
| generalize hc : coordinateEquiv S (fun i => M i.succ) c=q | |
| cases q with | |
| | inl s => rfl | |
| | inr p => rcases p with ⟨i,b⟩; rfl | |
| | inr b => cases b <;> rfl | |
| /-- The recursively proved marginal is the direct finite sum over the | |
| actual physical intervals. -/ | |
| theorem eliminate_eq_physical_sum {S : Type*} {n : ℕ} (M : Fin n → ℕ) | |
| (F : (S⊕(Fin n×Bool) → ℕ) → ℝ) (z : S → ℕ) : | |
| eliminate (widths M) (fun q => F (q ∘ (coordinateEquiv S M).symm)) z= | |
| ∑ a : ((i : Fin n) → Fin (M i+1)), F (joinedProfile M z a) := by | |
| rw [eliminate_eq_sum] | |
| apply Fintype.sum_equiv (assignmentEquiv M) | |
| intro a | |
| congr 1 | |
| funext c | |
| have h := embedding_coordinate M z ((assignmentEquiv M) a) ((coordinateEquiv S M).symm c) | |
| simpa only [Equiv.symm_apply_apply,Equiv.apply_symm_apply,Function.comp_apply] using h | |
| variable {C : Type*} | |
| @[reducible] def SmallView (small : C → Bool) := {c : C // small c=true}×Bool | |
| @[reducible] def LargeCell (small : C → Bool) := {c : C // small c=false} | |
| /-- This is the actual partition of doubled cells into small views and | |
| large pairs. -/ | |
| noncomputable def partitionEquiv (small : C → Bool) : | |
| SmallView small⊕(LargeCell small×Bool) ≃ C×Bool where | |
| toFun | |
| | .inl p => (p.1.val,p.2) | |
| | .inr p => (p.1.val,p.2) | |
| invFun p := if h : small p.1=true then .inl (⟨p.1,h⟩,p.2) | |
| else .inr (⟨p.1,Bool.eq_false_iff.mpr h⟩,p.2) | |
| left_inv p := by | |
| cases p with | |
| | inl p => simp only [p.1.property,dite_eq_left] | |
| | inr p => simp only [p.1.property,Bool.false_eq_true,dite_false] | |
| right_inv p := by | |
| dsimp only | |
| split_ifs <;> rfl | |
| noncomputable def physicalJoinEquiv (small : C → Bool) {n : ℕ} | |
| (e : Fin n ≃ LargeCell small) : SmallView small⊕(Fin n×Bool) ≃ C×Bool := | |
| (Equiv.sumCongr (Equiv.refl _) (Equiv.prodCongr e (Equiv.refl Bool))).trans | |
| (partitionEquiv small) | |
| /-- Every finite enumeration of the large cells gives the same physical | |
| coordinate space, with each original doubled cell appearing once. -/ | |
| noncomputable def physicalCoordinateEquiv (small : C → Bool) {n : ℕ} | |
| (e : Fin n ≃ LargeCell small) (M : Fin n → ℕ) : | |
| Coordinates (SmallView small) (widths M) ≃ C×Bool := | |
| (coordinateEquiv (SmallView small) M).trans (physicalJoinEquiv small e) | |
| theorem eliminate_eq_actual_cells (small : C → Bool) {n : ℕ} | |
| (e : Fin n ≃ LargeCell small) (M : Fin n → ℕ) | |
| (F : (C×Bool → ℕ) → ℝ) (z : SmallView small → ℕ) : | |
| eliminate (widths M) (fun q => F (q ∘ (physicalCoordinateEquiv small e M).symm)) z= | |
| ∑ a : ((i : Fin n) → Fin (M i+1)), | |
| F (joinedProfile M z a ∘ (physicalJoinEquiv small e).symm) := by | |
| exact eliminate_eq_physical_sum M (fun q => F (q ∘ (physicalJoinEquiv small e).symm)) z | |
| end ContingencyTables.LargePairEnumeration | |
| end OAI | |