import OAI.Probability.FreeIsing.Cavity.Array import OAI.Probability.FreeIsing.Estimates.ThresholdArithmetic import OAI.Probability.FreeIsing.Posterior.FieldL2Limit namespace OAI noncomputable section open MeasureTheory ProbabilityTheory Filter open scoped Topology NNReal namespace Problem367 open PlantedSymmetry namespace CavityFieldLimit local instance : Nonempty IsingSpin := ⟨.neg⟩ def finiteSiteField {d : ℕ} (beta : ℝ) (D : Finset (TreeVertex d)) (v : D) (y : TreeVertex d → ℝ) : ℝ := Real.artanh (FinitePosterior.fieldMean (finiteIsingEnergy beta D) (fun (eta : D → IsingSpin) w => spinSign (eta w)) (fun eta => spinSign (eta v)) (D.restrict y)) private theorem measurable_artanh : Measurable Real.artanh := by unfold Real.artanh fun_prop theorem measurable_finiteSiteField {d : ℕ} (beta : ℝ) (D : Finset (TreeVertex d)) (v : D) : Measurable (finiteSiteField beta D v) := measurable_artanh.comp ((FinitePosterior.continuous_fieldMean _ _ _).measurable.comp D.measurable_restrict) def finiteCavityField {d : ℕ} {beta : ℝ} (hbeta : 0 ≤ beta) (D : Finset (TreeVertex d)) (v w : D) (y : TreeVertex d → ℝ) : ℝ := (cavityFromSites (tanh_nonneg_of_beta_nonneg hbeta) (Real.tanh_lt_one beta) (finiteSiteField beta D v y, finiteSiteField beta D w y)).1 def infiniteCavityField {d : ℕ} {beta : ℝ} (hbeta : 0 ≤ beta) (v w : TreeVertex d) (y : TreeVertex d → ℝ) : ℝ := CavityArray.field (tanh_nonneg_of_beta_nonneg hbeta) (Real.tanh_lt_one beta) (fun u => Real.artanh (infiniteGibbsSpinMean beta u y)) v w theorem measurable_finiteCavityField {d : ℕ} {beta : ℝ} (hbeta : 0 ≤ beta) (D : Finset (TreeVertex d)) (v w : D) : Measurable (finiteCavityField hbeta D v w) := measurable_fst.comp ((measurable_cavityFromSites _ _).comp ((measurable_finiteSiteField beta D v).prodMk (measurable_finiteSiteField beta D w))) theorem measurable_infiniteCavityField {d : ℕ} {beta : ℝ} (hbeta : 0 ≤ beta) (v w : TreeVertex d) : Measurable (infiniteCavityField hbeta v w) := by exact (CavityArray.measurable_field_apply _ _ v w).comp (Measurable.of_eval (fun u => measurable_artanh.comp (measurable_infiniteGibbsSpinMean beta u))) end CavityFieldLimit open CavityFieldLimit theorem HasFreeIsingLaw.exhaustionSiteField_tendsto_ae {d : ℕ} {beta : ℝ} {μ : Measure (TreeVertex d → IsingSpin)} (hμ : HasFreeIsingLaw (Real.tanh beta) μ) (hbeta : 0 ≤ beta) (D : ℕ → Finset (TreeVertex d)) (hD : Monotone D) (hconn : ∀ n, ConnectedFinset (D n)) (hex : ∀ u, ∃ n, u ∈ D n) (v : TreeVertex d) (hv : ∀ n, v ∈ D n) (t : ℝ≥0) : ∀ᵐ p ∂μ.prod (gaussianNoiseLaw (TreeVertex d) t), Tendsto (fun n => finiteSiteField beta (D n) ⟨v, hv n⟩ (observation t p)) atTop (𝓝 (Real.artanh (infiniteGibbsSpinMean beta v (observation t p)))) := by let : IsProbabilityMeasure μ := hμ.isProbabilityMeasure have hb (n : ℕ) := hμ.finiteObservation_spin_tanh_bounds hbeta (D n) (hconn n) t ⟨v, hv n⟩ have hlim := tendsto_posterior_fields_ae (μ.prod (gaussianNoiseLaw (TreeVertex d) t)) (finiteObservationFiltration D hD t) (fun p => spinSign (p.1 v)) (fun p => observation t p v) ((d : ℝ) * beta) hb rw [finiteObservationFiltration_iSup D hD hex t] at hlim have hce (n : ℕ) := hμ.finiteObservation_condExp (D n) (hconn n) t (fun eta => spinSign (eta ⟨v, hv n⟩)) filter_upwards [hlim, ae_all_iff.mpr hce, hμ.infiniteGibbsSpinMean_eq_posterior t v] with p hp hce hinf convert hp.2.2 using 1 · ext n exact congrArg Real.artanh (hce n).symm · exact congrArg (fun x : ℝ => 𝓝 (Real.artanh x)) hinf theorem HasFreeIsingLaw.exhaustionSiteField_tendsto_meanSquare {d : ℕ} {beta : ℝ} {μ : Measure (TreeVertex d → IsingSpin)} (hμ : HasFreeIsingLaw (Real.tanh beta) μ) (hbeta : 0 ≤ beta) (D : ℕ → Finset (TreeVertex d)) (hD : Monotone D) (hconn : ∀ n, ConnectedFinset (D n)) (hex : ∀ u, ∃ n, u ∈ D n) (v : TreeVertex d) (hv : ∀ n, v ∈ D n) (t : ℝ≥0) : Tendsto (fun n => ∫ p, (finiteSiteField beta (D n) ⟨v, hv n⟩ (observation t p) - Real.artanh (infiniteGibbsSpinMean beta v (observation t p))) ^ 2 ∂μ.prod (gaussianNoiseLaw (TreeVertex d) t)) atTop (𝓝 0) := by let : IsProbabilityMeasure μ := hμ.isProbabilityMeasure have hb (n : ℕ) := hμ.finiteObservation_spin_tanh_bounds hbeta (D n) (hconn n) t ⟨v, hv n⟩ have hlim := tendsto_integral_sq_sub_posterior_fields (μ.prod (gaussianNoiseLaw (TreeVertex d) t)) (finiteObservationFiltration D hD t) (fun p => spinSign (p.1 v)) (fun p => observation t p v) hb rw [finiteObservationFiltration_iSup D hD hex t] at hlim convert hlim using 1 ext n apply integral_congr_ae filter_upwards [hμ.finiteObservation_condExp (D n) (hconn n) t (fun eta => spinSign (eta ⟨v, hv n⟩)), hμ.infiniteGibbsSpinMean_eq_posterior t v] with p hfinite hinf change _ = (Real.artanh (_) - Real.artanh (posteriorMagnetization (μ.prod (gaussianNoiseLaw (TreeVertex d) t)) t v p)) ^ 2 rw [hinf] congr 2 exact congrArg Real.artanh hfinite.symm theorem HasFreeIsingLaw.exhaustionCavityField_tendsto_ae {d : ℕ} {beta : ℝ} {μ : Measure (TreeVertex d → IsingSpin)} (hμ : HasFreeIsingLaw (Real.tanh beta) μ) (hbeta : 0 ≤ beta) (D : ℕ → Finset (TreeVertex d)) (hD : Monotone D) (hconn : ∀ n, ConnectedFinset (D n)) (hex : ∀ u, ∃ n, u ∈ D n) (v w : TreeVertex d) (hv : ∀ n, v ∈ D n) (hw : ∀ n, w ∈ D n) (t : ℝ≥0) : ∀ᵐ p ∂μ.prod (gaussianNoiseLaw (TreeVertex d) t), Tendsto (fun n => finiteCavityField hbeta (D n) ⟨v, hv n⟩ ⟨w, hw n⟩ (observation t p)) atTop (𝓝 (infiniteCavityField hbeta v w (observation t p))) := by filter_upwards [hμ.exhaustionSiteField_tendsto_ae hbeta D hD hconn hex v hv t, hμ.exhaustionSiteField_tendsto_ae hbeta D hD hconn hex w hw t] with p hp hq exact (continuous_fst.comp (continuous_cavityFromSites (tanh_nonneg_of_beta_nonneg hbeta) (Real.tanh_lt_one beta))).continuousAt.tendsto.comp (hp.prodMk_nhds hq) theorem HasFreeIsingLaw.exhaustionCavityField_discrepancy_bound {d : ℕ} {beta : ℝ} {μ : Measure (TreeVertex d → IsingSpin)} (hμ : HasFreeIsingLaw (Real.tanh beta) μ) (hbeta : 0 ≤ beta) (D : Finset (TreeVertex d)) (v w : D) (t : ℝ≥0) : ∀ᵐ p ∂μ.prod (gaussianNoiseLaw (TreeVertex d) t), |finiteCavityField hbeta D v w (observation t p) - infiniteCavityField hbeta v.1 w.1 (observation t p)| ≤ (2 * ((d : ℝ) * beta)) / (1 - Real.tanh beta) := by filter_upwards [hμ.gaussian_posterior_field_bound hbeta t v.1, hμ.gaussian_posterior_field_bound hbeta t w.1, hμ.infiniteGibbsSpinMean_eq_posterior t v.1, hμ.infiniteGibbsSpinMean_eq_posterior t w.1] with p hbv hbw hev hew let y := observation t p have hb (u : D) (hu : |Real.artanh (infiniteGibbsSpinMean beta u.1 y) - y u.1| ≤ (d : ℝ) * beta) : |finiteSiteField beta D u y - Real.artanh (infiniteGibbsSpinMean beta u.1 y)| ≤ 2 * ((d : ℝ) * beta) := by have hf := finite_tree_gibbs_field_uniform_bound D hbeta (D.restrict y) u change |finiteSiteField beta D u y - y u.1| ≤ (d : ℝ) * beta at hf calc _ = |(finiteSiteField beta D u y - y u.1) - (Real.artanh (infiniteGibbsSpinMean beta u.1 y) - y u.1)| := by congr 1; ring _ ≤ |finiteSiteField beta D u y - y u.1| + |Real.artanh (infiniteGibbsSpinMean beta u.1 y) - y u.1| := abs_sub _ _ _ ≤ _ := by linarith have hv := hb v (by simpa only [y, hev] using hbv.2) have hw := hb w (by simpa only [y, hew] using hbw.2) have h0 := tanh_nonneg_of_beta_nonneg hbeta have h1 := Real.tanh_lt_one beta have hs := cavityFromSites_spec h0 h1 (finiteSiteField beta D v y, finiteSiteField beta D w y) have hs' := cavityFromSites_spec h0 h1 (Real.artanh (infiniteGibbsSpinMean beta v.1 y), Real.artanh (infiniteGibbsSpinMean beta w.1 y)) exact cavity_pair_sub_abs_le h0 h1 hs.1 hs.2 hs'.1 hs'.2 hv hw theorem HasFreeIsingLaw.exhaustionCavityField_tendsto_meanSquare {d : ℕ} {beta : ℝ} {μ : Measure (TreeVertex d → IsingSpin)} (hμ : HasFreeIsingLaw (Real.tanh beta) μ) (hbeta : 0 ≤ beta) (D : ℕ → Finset (TreeVertex d)) (hD : Monotone D) (hconn : ∀ n, ConnectedFinset (D n)) (hex : ∀ u, ∃ n, u ∈ D n) (v w : TreeVertex d) (hv : ∀ n, v ∈ D n) (hw : ∀ n, w ∈ D n) (t : ℝ≥0) : Tendsto (fun n => ∫ p, (finiteCavityField hbeta (D n) ⟨v, hv n⟩ ⟨w, hw n⟩ (observation t p) - infiniteCavityField hbeta v w (observation t p)) ^ 2 ∂μ.prod (gaussianNoiseLaw (TreeVertex d) t)) atTop (𝓝 0) := by let : IsProbabilityMeasure μ := hμ.isProbabilityMeasure have hm (n : ℕ) := ((measurable_finiteCavityField hbeta (D n) ⟨v, hv n⟩ ⟨w, hw n⟩).comp (measurable_observation t)).sub ((measurable_infiniteCavityField hbeta v w).comp (measurable_observation t)) have hbound (n : ℕ) : ∀ᵐ p ∂μ.prod (gaussianNoiseLaw (TreeVertex d) t), ‖(finiteCavityField hbeta (D n) ⟨v, hv n⟩ ⟨w, hw n⟩ (observation t p) - infiniteCavityField hbeta v w (observation t p)) ^ 2‖ ≤ ((2 * ((d : ℝ) * beta)) / (1 - Real.tanh beta)) ^ 2 := by filter_upwards [hμ.exhaustionCavityField_discrepancy_bound hbeta (D n) ⟨v, hv n⟩ ⟨w, hw n⟩ t] with p hp rw [Real.norm_of_nonneg (sq_nonneg _)] simpa only [sq_abs] using pow_le_pow_left₀ (abs_nonneg _) hp 2 have hzero := hμ.exhaustionCavityField_tendsto_ae hbeta D hD hconn hex v w hv hw t have hlim := tendsto_integral_of_dominated_convergence (fun _ => ((2 * ((d : ℝ) * beta)) / (1 - Real.tanh beta)) ^ 2) (fun n => (hm n).aestronglyMeasurable.pow 2) (integrable_const _) hbound (hzero.mono (fun p hp => by simpa using (hp.sub_const (infiniteCavityField hbeta v w (observation t p))).pow 2)) simpa using hlim end Problem367 end end OAI