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dd14c26 | 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 61 62 63 64 65 66 67 68 69 70 71 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86 87 88 89 90 91 92 93 94 95 96 97 98 99 100 101 102 103 104 105 106 107 108 109 110 111 112 113 114 115 116 117 118 119 120 121 122 123 124 125 126 127 128 129 130 131 132 133 134 135 136 137 138 139 140 141 142 143 144 145 146 147 148 149 150 151 152 153 154 155 156 157 158 159 160 161 162 163 164 165 166 167 168 169 170 171 172 173 174 175 176 177 178 179 180 181 182 183 184 185 186 187 188 189 190 191 192 193 194 195 196 197 198 199 200 201 202 203 204 205 206 207 208 209 210 | import OAI.Probability.Ising.EdwardsSokal
import OAI.Probability.Ising.TwoSpin
namespace OAI
open scoped BigOperators Classical
namespace BufferedIsing
/-- Extension by the actual common pins, in contrast to the deleted zero-field
comparison graph. -/
def pinExtension {n : ℕ} (F : Finset (Fin n)) (τ : Spins n)
(σ : KeptVertex F → Bool) : Spins n :=
fun v => if hv : v ∈ F then τ v else σ ⟨v, hv⟩
lemma pinExtension_agrees {n : ℕ} (F : Finset (Fin n)) (τ : Spins n)
(σ : KeptVertex F → Bool) : AgreesOn F (pinExtension F τ σ) τ := by
intro v hv
simp only [pinExtension, dite_eq_left hv]
lemma pinExtension_apply {n : ℕ} (F : Finset (Fin n)) (τ : Spins n)
(σ : KeptVertex F → Bool) (v : KeptVertex F) :
pinExtension F τ σ v = σ v := by
simp only [pinExtension, dite_eq_right v.property]
/-- Fixing sites is exactly elimination of their spin variables. This finite
bijection does not replace their interactions by deletion. -/
def pinExtensionEquiv {n : ℕ} (F : Finset (Fin n)) (τ : Spins n) :
(KeptVertex F → Bool) ≃ {σ : Spins n // AgreesOn F σ τ} where
toFun σ := ⟨pinExtension F τ σ, pinExtension_agrees F τ σ⟩
invFun σ v := σ.val v
left_inv σ := by ext v; exact pinExtension_apply F τ σ v
right_inv σ := by
apply Subtype.ext
funext v
by_cases hv : v ∈ F
· simpa only [pinExtension, dite_eq_left hv] using (σ.property v hv).symm
· simp only [pinExtension, dite_eq_right hv]
lemma constrainedSum_delete_variables {n m : ℕ} (G : FiniteGraph n m)
(h : Fin n → ℝ) (F : Finset (Fin n)) (τ : Spins n) (P : Spins n → Prop) :
constrainedSum G h (fun σ => AgreesOn F σ τ ∧ P σ) =
∑ σ : KeptVertex F → Bool,
if P (pinExtension F τ σ) then weight G h (pinExtension F τ σ) else 0 := by
classical
calc
_ = ∑ σ : Spins n, if AgreesOn F σ τ then
(if P σ then weight G h σ else 0) else 0 := by
unfold constrainedSum
apply Finset.sum_congr rfl
intro σ _
by_cases hF : AgreesOn F σ τ <;> by_cases hP : P σ <;> simp [hF, hP]
_ = ∑ σ ∈ Finset.univ.filter (fun σ : Spins n => AgreesOn F σ τ),
if P σ then weight G h σ else 0 := (Finset.sum_filter _ _).symm
_ = ∑ σ : {σ : Spins n // AgreesOn F σ τ},
if P σ.val then weight G h σ.val else 0 :=
Finset.sum_subtype _ (by intro σ; simp only [Finset.mem_filter,
Finset.mem_univ, true_and]) _
_ = _ := (Equiv.sum_comp (pinExtensionEquiv F τ)
(fun σ => if P σ.val then weight G h σ.val else 0)).symm
/-- A finite two-spin table extracted from a not necessarily normalized spin weight. -/
noncomputable def pairTable {V : Type*} [Fintype V] [DecidableEq V] (W : (V → Bool) → ℝ)
(i j : V) (s t : Bool) : ℝ :=
∑ σ, if σ i = s ∧ σ j = t then W σ else 0
lemma pairTable_sum {V : Type*} [Fintype V] [DecidableEq V] (W : (V → Bool) → ℝ)
(i j : V) (f : Bool → Bool → ℝ) :
(∑ s, ∑ t, pairTable W i j s t * f s t) =
∑ σ, W σ * f (σ i) (σ j) := by
classical
simp only [pairTable, Finset.sum_mul]
calc
_ = ∑ s, ∑ σ, ∑ t, (if σ i = s ∧ σ j = t then W σ else 0) * f s t := by
apply Finset.sum_congr rfl
intro s _
exact Finset.sum_comm
_ = ∑ σ, ∑ s, ∑ t, (if σ i = s ∧ σ j = t then W σ else 0) * f s t :=
Finset.sum_comm
_ = _ := by
apply Finset.sum_congr rfl
intro σ _
cases σ i <;> cases σ j <;> simp
lemma pairTable_expectation {V : Type*} [Fintype V] [DecidableEq V] (W : (V → Bool) → ℝ)
(i j : V) (f : Bool → Bool → ℝ) :
tableExpectation (pairTable W i j) f =
(∑ σ, W σ * f (σ i) (σ j)) / ∑ σ, W σ := by
unfold tableExpectation
rw [pairTable_sum]
have H := pairTable_sum W i j (fun _ _ => 1)
simp only [mul_one] at H
rw [H]
/-- Global spin reversal is a permutation of configurations. -/
def spinFlipEquiv (V : Type*) : (V → Bool) ≃ (V → Bool) where
toFun σ v := !σ v
invFun σ v := !σ v
left_inv σ := by ext v; simp only [Bool.not_not]
right_inv σ := by ext v; simp only [Bool.not_not]
lemma pairTable_flip {V : Type*} [Fintype V] [DecidableEq V] (W : (V → Bool) → ℝ)
(hW : ∀ σ, W (fun v => !σ v) = W σ) (i j : V) (s t : Bool) :
pairTable W i j (!s) (!t) = pairTable W i j s t := by
classical
unfold pairTable
rw [← Equiv.sum_comp (spinFlipEquiv V)
(fun σ => if σ i = !s ∧ σ j = !t then W σ else 0)]
apply Finset.sum_congr rfl
intro σ _
simp only [spinFlipEquiv, Equiv.coe_fn_mk, Bool.not_inj_iff, hW]
lemma symmetricTable_balanced (w : Bool → Bool → ℝ)
(hw : ∀ s t, w (!s) (!t) = w s t) : balancedTable w = w := by
have h₁ := hw true true
have h₂ := hw true false
simp only [Bool.not_true, Bool.not_false] at h₁ h₂
have hf : tableFieldLeft w = 0 ∧ tableFieldRight w = 0 := by
constructor <;> dsimp only [tableFieldLeft, tableFieldRight] <;> rw [h₁, h₂] <;> ring
funext s t
simp only [balancedTable, hf.1, hf.2, neg_zero, zero_mul, sub_zero,
Real.exp_zero, mul_one]
lemma symmetricTable_correlation (w : Bool → Bool → ℝ) (hw : ∀ s t, 0 < w s t)
(hsym : ∀ s t, w (!s) (!t) = w s t) :
tableExpectation w (fun s t => spin s * spin t) = Real.tanh (tableCoupling w) := by
have H := balancedTable_correlation w hw
rw [symmetricTable_balanced w hsym] at H
exact H
lemma respects_spinFlip {V : Type*} (S : Setoid V) (σ : V → Bool) :
Respects S (fun v => !σ v) ↔ Respects S σ := by
unfold Respects
simp only [Bool.not_inj_iff]
lemma deletedEnergy_spinFlip {n m : ℕ} (G : FiniteGraph n m)
(F : Finset (Fin n)) (σ : KeptVertex F → Bool) :
deletedEnergy G F (fun v => !σ v) = deletedEnergy G F σ := by
unfold deletedEnergy
apply Finset.sum_congr rfl
intro e he
obtain ⟨hl, hr⟩ := (Finset.mem_filter.mp he).2
have hleft (σ : KeptVertex F → Bool) :
extendKept F σ (G.left e) = σ ⟨G.left e, hl⟩ := by
exact extendKept_apply F σ ⟨G.left e, hl⟩
have hright (σ : KeptVertex F → Bool) :
extendKept F σ (G.right e) = σ ⟨G.right e, hr⟩ := by
exact extendKept_apply F σ ⟨G.right e, hr⟩
rw [hleft, hright, hleft, hright, spin_not, spin_not]
ring
lemma contractedZeroWeight_spinFlip {n m : ℕ} (G : FiniteGraph n m)
(I J F : Finset (Fin n)) (σ : KeptVertex F → Bool) :
contractedZeroWeight G I J F (fun v => !σ v) = contractedZeroWeight G I J F σ := by
unfold contractedZeroWeight
rw [respects_spinFlip, deletedEnergy_spinFlip]
lemma contractedZeroWeight_nonneg {n m : ℕ} (G : FiniteGraph n m)
(I J F : Finset (Fin n)) (σ : KeptVertex F → Bool) :
0 ≤ contractedZeroWeight G I J F σ := by
unfold contractedZeroWeight
split_ifs
· exact (Real.exp_pos _).le
· exact le_rfl
lemma contractedZero_pairTable_pos {n m : ℕ} (G : FiniteGraph n m)
(I J F : Finset (Fin n)) (hIJ : Disjoint I J)
(i j : KeptVertex F) (hi : i.val ∈ I) (hj : j.val ∈ J) (s t : Bool) :
0 < pairTable (contractedZeroWeight G I J F) i j s t := by
classical
let σ : KeptVertex F → Bool := fun v => if v.val ∈ I then s else t
have hjI : j.val ∉ I := fun hjI => Finset.disjoint_left.mp hIJ hjI hj
have hσi : σ i = s := by simp only [σ, ite_eq_left hi]
have hσj : σ j = t := by simp only [σ, ite_eq_right hjI]
have hresp : Respects (comparisonSetoid G I J F ∅) σ := by
intro x y hxy
have hI := comparison_empty_preserves_I G I J F hIJ x y hxy
simp only [σ, hI]
unfold pairTable
apply Finset.sum_pos'
· intro τ _
split_ifs
· exact contractedZeroWeight_nonneg G I J F τ
· exact le_rfl
· refine ⟨σ, Finset.mem_univ _, ?_⟩
rw [ite_eq_left ⟨hσi, hσj⟩, contractedZeroWeight, ite_eq_left hresp]
exact Real.exp_pos _
/-- The FK terminal connection probability is the hyperbolic tangent of the zero-field effective coupling. -/
lemma qZero_eq_tanh_effective {n m : ℕ} (G : FiniteGraph n m)
(I J F : Finset (Fin n)) (hIJ : Disjoint I J)
(i j : KeptVertex F) (hi : i.val ∈ I) (hj : j.val ∈ J) :
qZero G I J F i j =
Real.tanh (tableCoupling (pairTable (contractedZeroWeight G I J F) i j)) := by
rw [← symmetricTable_correlation _ (contractedZero_pairTable_pos G I J F hIJ i j hi hj)
(pairTable_flip _ (contractedZeroWeight_spinFlip G I J F) i j)]
rw [pairTable_expectation, qZero_eq_zero_field_correlation]
simp only [mul_assoc]
lemma artanh_qZero_eq_effective {n m : ℕ} (G : FiniteGraph n m)
(I J F : Finset (Fin n)) (hIJ : Disjoint I J)
(i j : KeptVertex F) (hi : i.val ∈ I) (hj : j.val ∈ J) :
Real.artanh (qZero G I J F i j) =
tableCoupling (pairTable (contractedZeroWeight G I J F) i j) := by
rw [qZero_eq_tanh_effective G I J F hIJ i j hi hj, Real.artanh_tanh]
end BufferedIsing
end OAI
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