OAI/Probability/Ising/PinnedMarginal.lean
12 declarations, 0 contain sorry, 0 declared as axioms
- def
OAI.BufferedIsing.contractedPinnedWeightline 12Source documentation
The actual contracted marginal retains arbitrary fields and all effects of the common pins. It is distinct from the zero-field comparison weight.
noncomputable def contractedPinnedWeight {n m : ℕ} (G : FiniteGraph n m) (h : Fin n → ℝ) (I J F : Finset (Fin n)) (τ : Spins n) (σ : KeptVertex F → Bool) : ℝ := …Mentions: OAI.BufferedIsing.FiniteGraph, OAI.BufferedIsing.Spins, OAI.BufferedIsing.KeptVertex
- lemma
OAI.BufferedIsing.respects_terminals_iffline 17 - lemma
OAI.BufferedIsing.contracted_prescription_iffline 37 - lemma
OAI.BufferedIsing.pairTable_contractedPinnedline 67Source documentation
Identifying each terminal set separately is exactly restriction to its constant configurations; no new model comparison enters this identity.
lemma pairTable_contractedPinned {n m : ℕ} (G : FiniteGraph n m) (h : Fin n → ℝ) (I J F : Finset (Fin n)) (hIF : Disjoint I F) (hJF : Disjoint J F) (i j : KeptVertex F) (hi : i.val ∈ I) (hj : j.val ∈ J) (τ : Spins n) (s t : Bool) : pairTable (contractedPinnedWeight G h I J F τ) i j s t = jointWeight G h I J F τ (fun _ => s) (fun _ => t) := by …Mentions: OAI.BufferedIsing.FiniteGraph, OAI.BufferedIsing.KeptVertex, OAI.BufferedIsing.Spins, OAI.BufferedIsing.pairTable, OAI.BufferedIsing.contractedPinnedWeight, OAI.BufferedIsing.jointWeight
- lemma
OAI.BufferedIsing.extremeLogOdds_eq_effectiveline 98 - lemma
OAI.BufferedIsing.sum_pin_incidenceline 111 - def
OAI.BufferedIsing.pinFieldline 144Source documentation
The finite-field contribution induced by the actual prescribed spins. Neither these induced fields nor the original fields survive in
qZero.noncomputable def pinField {n m : ℕ} (G : FiniteGraph n m) (h : Fin n → ℝ) (F : Finset (Fin n)) (τ : Spins n) (v : KeptVertex F) : ℝ := …Mentions: OAI.BufferedIsing.FiniteGraph, OAI.BufferedIsing.Spins, OAI.BufferedIsing.KeptVertex
- def
OAI.BufferedIsing.pinConstantline 153Source documentation
Field and bond terms depending only on fixed sites. They cancel from all normalized laws, but recording them makes the elimination exact.
noncomputable def pinConstant {n m : ℕ} (G : FiniteGraph n m) (h : Fin n → ℝ) (F : Finset (Fin n)) (τ : Spins n) : ℝ := …Mentions: OAI.BufferedIsing.FiniteGraph, OAI.BufferedIsing.Spins
- lemma
OAI.BufferedIsing.energy_pin_expansionline 159 - lemma
OAI.BufferedIsing.sum_keptline 218 - lemma
OAI.BufferedIsing.energy_pinExtensionline 227Source documentation
Exact deletion of fixed sites: their incident bonds become finite real fields, while only bonds with two free endpoints remain as interactions.
lemma energy_pinExtension {n m : ℕ} (G : FiniteGraph n m) (h : Fin n → ℝ) (F : Finset (Fin n)) (τ : Spins n) (σ : KeptVertex F → Bool) : energy G h (pinExtension F τ σ) = pinConstant G h F τ + deletedEnergy G F σ + ∑ v : KeptVertex F, pinField G h F τ v * spin (σ v) := by …Mentions: OAI.BufferedIsing.FiniteGraph, OAI.BufferedIsing.Spins, OAI.BufferedIsing.KeptVertex, OAI.BufferedIsing.energy, OAI.BufferedIsing.pinExtension, OAI.BufferedIsing.pinConstant, OAI.BufferedIsing.deletedEnergy, OAI.BufferedIsing.pinField, OAI.BufferedIsing.spin
- lemma
OAI.BufferedIsing.weight_pinExtensionline 253