import Mathlib import OAI.MathematicalPhysics.PEPSFilters.LocalOperators import OAI.MathematicalPhysics.PEPSSubvolume.SquareRecurrence namespace OAI /-! Residue-grid partitions and all-scale square estimates. -/ noncomputable section open scoped BigOperators ComplexOrder open scoped BigOperators ComplexOrder Matrix.Norms.L2Operator open scoped BigOperators open scoped Topology open Filter open scoped MatrixOrder open scoped BigOperators Matrix.Norms.L2Operator open scoped ComplexOrder BigOperators Matrix.Norms.L2Operator open Matrix open Filter Topology open Set Filter Complex Complex.HadamardThreeLines open scoped BigOperators Matrix.Norms.L2Operator MatrixOrder ComplexOrder open PolynomialPEPS.PinnedEntropy namespace PolynomialPEPS.Subvolume.RectangleTiling open scoped BigOperators open RectangleContours variable {L : ℕ} def rect (lo₁ lo₂ : ℤ) (w h : ℕ) : Finset (Vertex L) := rectangle lo₁ (lo₁+w-1) lo₂ (lo₂+h-1) 0 lemma mem_rect (lo₁ lo₂ : ℤ) (w h : ℕ) (v : Vertex L) : v∈rect lo₁ lo₂ w h ↔ (0≤(v.1.val:ℤ)-lo₁ ∧ (v.1.val:ℤ)-lo₁ (⟨((v.val.1.val:ℤ)-lo₁).toNat,by have hh := (mem_rect lo₁ lo₂ w h v.val).mp v.property omega⟩, ⟨((v.val.2.val:ℤ)-lo₂).toNat,by have hh := (mem_rect lo₁ lo₂ w h v.val).mp v.property omega⟩) have hf : Function.Injective f := by intro v u he have hv := (mem_rect lo₁ lo₂ w h v.val).mp v.property have hu := (mem_rect lo₁ lo₂ w h u.val).mp u.property have h1 := congrArg (fun z : Fin w × Fin h => z.1.val) he have h2 := congrArg (fun z : Fin w × Fin h => z.2.val) he dsimp only [f] at h1 h2 apply Subtype.ext apply Prod.ext <;> apply Fin.ext <;> omega have hh := Fintype.card_le_of_injective f hf simpa only [Fintype.card_coe,Fintype.card_prod,Fintype.card_fin] using hh lemma box_eq_rect (lo₁ lo₂ : ℤ) (M r : ℕ) : box (L:=L) lo₁ lo₂ M r=rect lo₁ lo₂ (M*r) (M*r) := by simp only [box,rect,Nat.cast_mul] lemma box_mono (lo₁ lo₂ : ℤ) {n m : ℕ} (hnm : n ≤ m) : box (L:=L) lo₁ lo₂ 1 n ⊆ box lo₁ lo₂ 1 m := by intro v hv rw [mem_box] at hv ⊢ have hh : (n:ℤ)≤ m := by exact_mod_cast hnm simpa only [Nat.cast_one,one_mul] using And.intro (And.intro hv.1.1 (lt_of_lt_of_le (by simpa using hv.1.2) hh)) (And.intro hv.2.1 (lt_of_lt_of_le (by simpa using hv.2.2) hh)) lemma box_remainder_card (lo₁ lo₂ : ℤ) (n r : ℕ) (hr : 0 h.2 hv⟩ have hsub := RegionSSA.conditional_entropy_antitone hq Ω (E\B) (E\B) E (Finset.Subset.refl _) Finset.sdiff_subset rw [hdiff,Finset.sdiff_self,vonNeumannEntropy_empty Ω hΩ,sub_zero] at hsub have hparts := PolynomialPEPS.SubvolumeTiling.tiles_subadditive (vonNeumannEntropy Ω) (vonNeumannEntropy_empty Ω hΩ) (RegionSSA.conditional_entropy_antitone hq Ω) (tile (L:=L) (M:=n/r) lo₁ lo₂ r) Finset.univ (fun i _ j _ hij => tiles_disjoint lo₁ lo₂ r hr i j hij) dsimp only [PolynomialPEPS.SubvolumeTiling.unionTiles] at hparts rw [tiles_cover lo₁ lo₂ r hr] at hparts have hsum := Finset.sum_le_sum (fun (i : Index (n/r)) (_ : i∈Finset.univ) => hF i) simp only [Finset.sum_const,Finset.card_univ,Index,Fintype.card_prod, Fintype.card_fin,nsmul_eq_mul,Nat.cast_mul] at hsum have hfull : vonNeumannEntropy Ω B≤((n/r:ℕ):ℝ)^2*F := by simpa only [pow_two] using hparts.trans hsum have hrem := vonNeumannEntropy_le_card_log hq Ω hΩ (E\B) have hc : ((E\B).card:ℝ)≤2*(n:ℝ)*(r:ℝ) := by dsimp only [E,B] exact_mod_cast box_remainder_card (L:=L) lo₁ lo₂ n r hr have hQ : 0≤Real.log q := Real.log_nonneg (by exact_mod_cast hq) have herr := hrem.trans (mul_le_mul_of_nonneg_right hc hQ) change vonNeumannEntropy Ω E≤_ linarith only [hsub,hfull,herr] theorem square_entropy_below_scale (hq : 0