openAI-math-dataset / lean /OAI /Probability /InvariantIsing /Cavity /CavityCanonicalSynchronization.lean
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import OAI.Probability.InvariantIsing.Cavity.CavityCanonicalLabels
import OAI.Probability.InvariantIsing.Spectral.SpectralCanonicalIdentification
namespace OAI
/-! The limiting Ward equations give the canonical monotone spectral
labels on every off-diagonal entry, not only along quantile parameters. -/
noncomputable section
open MeasureTheory ProbabilityTheory IsingPerceptron Set Filter
open scoped BigOperators Topology
namespace InvariantIsing
theorem cavity_canonical_group_synchronization {m : ℕ}
{Q : ProbabilityMeasure (SpectralArray (m + 1))}
(hgg : HasEntryGhirlandaGuerra (fun x i j => x (i,j)) (Q : Measure (SpectralArray (m + 1))))
(hG : ∀ᵐ x ∂(Q : Measure (SpectralArray (m + 1))), SpectralGram x)
(q : Fin (m + 1) → ℝ) (hq : ∀ a, 0 ≤ q a)
(hd : ∀ᵐ x ∂(Q : Measure (SpectralArray (m + 1))), ∀ i a, (x (i,i) a : ℝ) = q a)
(hE : ∀ e : ℕ → ℕ, Function.Injective e →
(Q : Measure (SpectralArray (m + 1))).map (permuteSpectralArray e) = Q)
(hP : ∀ᵐ x ∂(Q : Measure (SpectralArray (m + 1))), SpectralPartitionGeometry m x)
(hn : ∀ᵐ x ∂(Q : Measure (SpectralArray (m + 1))), ∀ a, 0 ≤ (x (0,1) a : ℝ))
(ρ eig : Fin m → ℝ) (hρ : ∀ a, 0 < ρ a) (hρsum : ∑ a, ρ a = 1)
(hoff : ∀ a b, ∀ Φ : ℝ → ℝ, Continuous Φ → ∀ C : ℝ, 0 ≤ C → (∀ r, |Φ r| ≤ C) →
spectralOffWardResidual Q ρ eig a b Φ = 0)
(hdiag : ∀ a b, spectralDiagonalWardResidual Q ρ eig a b = 0) :
let p := spectralSpinQuantilePath Q hP hn
(∀ a, q a.castSucc = spectralGroupDiagonal ρ eig hρ hρsum p a) ∧
∀ᵐ x ∂(Q : Measure (SpectralArray (m + 1))), ∀ i j, i ≠ j → ∀ a : Fin m,
(x (i,j) a.castSucc : ℝ) =
cavityCanonicalCoordinate ρ eig hρ hρsum p a (spectralSpinArray x i j) := by
intro p
obtain ⟨hdq, hc⟩ := spectralCanonical_identification hgg hG q hq hd hE hP hn
ρ eig hρ hρsum hoff hdiag
refine ⟨hdq, ?_⟩
have hall (a : Fin m) : ∀ᵐ x ∂(Q : Measure (SpectralArray (m + 1))), ∀ i j, i ≠ j →
(x (i,j) a.castSucc : ℝ) =
cavityCanonicalCoordinate ρ eig hρ hρsum p a (spectralSpinArray x i j) := by
apply spectral_factor_all_off_diagonal hE a _
(continuous_cavityCanonicalCoordinate ρ eig hρ hρsum p a)
have hsingle : ∀ b, 0 ≤ (Pi.single a.castSucc 1 : Fin (m + 1) → ℝ) b := by
intro b
simp only [Pi.single_apply]
split_ifs <;> norm_num
have hp : ∀ᵐ x ∂(Q : Measure (SpectralArray (m + 1))),
spectralLinearArray (spectralSpinWeight m) x 0 1 ∈ Icc (0 : ℝ) 1 := by
simpa only [spectralLinearArray_spinWeight] using spectralPartition_spin_unit hP hn
have he := factor_of_pair_law pathMeasure (Q : Measure (SpectralArray (m + 1)))
p (spectralGroupQuantilePath Q hn a)
(fun x => spectralLinearArray (spectralSpinWeight m) x 0 1)
(fun x => spectralLinearArray (Pi.single a.castSucc 1) x 0 1)
p.measurable (spectralGroupQuantilePath Q hn a).measurable
(by unfold spectralLinearArray spectralLinearEntry; fun_prop)
(by unfold spectralLinearArray spectralLinearEntry; fun_prop)
(spectralQuantilePath_pair_law hgg hG q hq hd (fun e => hE e e.injective)
(spectralSpinWeight m) (Pi.single a.castSucc 1) (spectralSpinWeight_nonneg m)
hsingle hp (spectralCoordinate_unit hn a.castSucc))
(cavityCanonicalCoordinate ρ eig hρ hρsum p a)
(continuous_cavityCanonicalCoordinate ρ eig hρ hρsum p a)
(by
filter_upwards [hc] with s hs
exact (hs a).trans (cavityCanonicalCoordinate_at_path ρ eig hρ hρsum p a s).symm)
simpa only [spectralLinearArray_spinWeight, spectralLinearArray_single,
spectralCoordinateArray] using he
filter_upwards [ae_all_iff.mpr hall] with x hx
intro i j hij a
exact hx a i j hij
end InvariantIsing
end
end OAI