import OAI.Probability.FreeIsing.Brownian.DriftMoments import OAI.Probability.FreeIsing.Energy.FiniteIsingFieldEnergy import OAI.Probability.FreeIsing.Stochastic.FiniteIsingBrownianEnergy import OAI.Probability.FreeIsing.Trees.GibbsField namespace OAI noncomputable section open MeasureTheory ProbabilityTheory Filter Set open scoped NNReal ENNReal namespace Problem367 local instance finiteIsingBrownianEntropyNonemptySpin : Nonempty IsingSpin := ⟨.neg⟩ def finiteIsingBrownianEntropy {d : ℕ} {Ω : Type*} (beta : ℝ) (D : Finset (TreeVertex d)) (v : D) (B : TreeVertex d → ℝ≥0 → Ω → ℝ) (t : ℝ) (p : (TreeVertex d → IsingSpin) × (TreeVertex d → Ω)) : ℝ := FinitePosterior.fieldEntropy (finiteIsingEnergy beta D) (fun eta u => spinSign (eta u)) (fun eta => spinSign (eta v)) (finiteIsingBrownianObservation B D t p) def finiteIsingBrownianNormalizedCovariance {d : ℕ} {Ω : Type*} (beta : ℝ) (D : Finset (TreeVertex d)) (v u : D) (B : TreeVertex d → ℝ≥0 → Ω → ℝ) (t : ℝ) (p : (TreeVertex d → IsingSpin) × (TreeVertex d → Ω)) : ℝ := FinitePosterior.normalizedFieldCovariance (finiteIsingEnergy beta D) (fun eta w => spinSign (eta w)) (fun eta => spinSign (eta v)) (finiteIsingBrownianObservation B D t p) u theorem finiteIsingBrownianEntropy_nonneg {d : ℕ} {Ω : Type*} (beta : ℝ) (D : Finset (TreeVertex d)) (v : D) (B : TreeVertex d → ℝ≥0 → Ω → ℝ) (t : ℝ) (p : (TreeVertex d → IsingSpin) × (TreeVertex d → Ω)) : 0 ≤ finiteIsingBrownianEntropy beta D v B t p := by exact FinitePosterior.fieldEntropy_nonneg _ _ _ _ (fun eta => by cases eta v <;> simp [spinSign]) ⟨fun _ => .neg, rfl⟩ ⟨fun _ => .pos, rfl⟩ theorem finiteIsingBrownianEntropy_le_noise {d : ℕ} {Ω : Type*} {beta : ℝ} (hbeta : 0 ≤ beta) (D : Finset (TreeVertex d)) (v : D) (B : TreeVertex d → ℝ≥0 → Ω → ℝ) (t : ℝ≥0) (p : (TreeVertex d → IsingSpin) × (TreeVertex d → Ω)) : finiteIsingBrownianEntropy beta D v B t p ≤ 2 * ((d : ℝ) * beta + (t : ℝ) + |B v t (p.2 v)|) := by let y := finiteIsingBrownianObservation B D t p have he := FinitePosterior.fieldEntropy_le_abs_field (finiteIsingEnergy beta D) (fun (eta : D → IsingSpin) w => spinSign (eta w)) (fun eta => spinSign (eta v)) y (fun eta => by cases eta v <;> simp [spinSign]) ⟨fun _ => .neg, rfl⟩ ⟨fun _ => .pos, rfl⟩ have hb := finite_tree_gibbs_field_uniform_bound D hbeta y v have ho : |y v| ≤ (t : ℝ) + |B v t (p.2 v)| := by change |(t : ℝ) * spinSign (p.1 v) + B v (Real.toNNReal (t : ℝ)) (p.2 v)| ≤ _ rw [Real.toNNReal_coe] calc _ ≤ |(t : ℝ) * spinSign (p.1 v)| + |B v t (p.2 v)| := abs_add_le _ _ _ = _ := by cases p.1 v <;> simp [spinSign, abs_of_nonneg t.coe_nonneg] have hfield : |FinitePosterior.fieldField (finiteIsingEnergy beta D) (fun (eta : D → IsingSpin) w => spinSign (eta w)) (fun eta => spinSign (eta v)) y| ≤ (d : ℝ) * beta + (t : ℝ) + |B v t (p.2 v)| := by have htri := abs_sub_le (FinitePosterior.fieldField (finiteIsingEnergy beta D) (fun (eta : D → IsingSpin) w => spinSign (eta w)) (fun eta => spinSign (eta v)) y) (y v) 0 simp only [sub_zero] at htri change |FinitePosterior.fieldField (finiteIsingEnergy beta D) (fun (eta : D → IsingSpin) w => spinSign (eta w)) (fun eta => spinSign (eta v)) y - y v| ≤ (d : ℝ) * beta at hb linarith exact he.trans (mul_le_mul_of_nonneg_left hfield (by norm_num)) private theorem integral_abs_gaussian_le_sqrt {Ω : Type*} [MeasurableSpace Ω] {P : Measure Ω} [IsProbabilityMeasure P] {X : Ω → ℝ} {t : ℝ≥0} (hX : HasLaw X (gaussianReal 0 t) P) : (∫ ω, |X ω| ∂P) ≤ Real.sqrt (t : ℝ) := by have hX2 : Integrable (fun ω => X ω ^ 2) P := by simpa only [sq_abs] using integrable_abs_pow_of_gaussianLaw hX 2 have htrans := hX.integral_comp (f := fun x : ℝ => x ^ 2) (by fun_prop) have hvar := variance_fun_id_gaussianReal (μ := 0) (v := t) rw [variance_of_integral_eq_zero (μ := gaussianReal 0 t) (X := fun x : ℝ => x) (by fun_prop) (by simp)] at hvar have hsq : (∫ ω, X ω ^ 2 ∂P) = (t : ℝ) := htrans.trans hvar exact (integral_abs_le_sqrt_integral_sq hX.aemeasurable hX2).trans_eq (congrArg Real.sqrt hsq) theorem finiteIsingBrownianEntropy_moment {d : ℕ} {Ω : Type*} [MeasurableSpace Ω] {beta : ℝ} (hbeta : 0 ≤ beta) (μ : Measure (TreeVertex d → IsingSpin)) [IsProbabilityMeasure μ] (ν : TreeVertex d → Measure Ω) {B : TreeVertex d → ℝ≥0 → Ω → ℝ} (hB : ∀ i, IsPreBrownianReal (B i) (ν i)) (hmB : ∀ i t, Measurable (B i t)) (D : Finset (TreeVertex d)) (v : D) (t : ℝ≥0) : Integrable (finiteIsingBrownianEntropy beta D v B t) (μ.prod (Measure.infinitePi ν)) ∧ (∫ p, finiteIsingBrownianEntropy beta D v B t p ∂μ.prod (Measure.infinitePi ν)) ≤ 2 * ((d : ℝ) * beta + (t : ℝ) + Real.sqrt (t : ℝ)) := by have (i : TreeVertex d) : IsProbabilityMeasure (ν i) := (hB i).isGaussianProcess.isProbabilityMeasure let ρ := μ.prod (Measure.infinitePi ν) let X : ((TreeVertex d → IsingSpin) × (TreeVertex d → Ω)) → ℝ := fun p => B v t (p.2 v) have hcoord := (measurePreserving_eval_infinitePi ν (v : TreeVertex d)).comp (measurePreserving_snd (μ := μ) (ν := Measure.infinitePi ν)) have hX : HasLaw X (gaussianReal 0 t) ρ := (hB v).hasLaw_eval t |>.comp ⟨hcoord.measurable.aemeasurable, hcoord.map_eq⟩ have hXi : Integrable (fun p => |X p|) ρ := by simpa only [pow_one] using integrable_abs_pow_of_gaussianLaw hX 1 have hY : Measurable (finiteIsingBrownianObservation B D (t : ℝ)) := by apply Measurable.of_eval intro w exact (((measurable_of_finite spinSign).comp ((measurable_pi_apply (w : TreeVertex d)).comp measurable_fst)).const_mul (t : ℝ)).add ((hmB w (t : ℝ).toNNReal).comp ((measurable_pi_apply (w : TreeVertex d)).comp measurable_snd)) have hF : Measurable (finiteIsingBrownianEntropy beta D v B (t : ℝ)) := (FinitePosterior.continuous_fieldEntropy (finiteIsingEnergy beta D) (fun (eta : D → IsingSpin) w => spinSign (eta w)) (fun eta => spinSign (eta v)) (fun eta => by cases eta v <;> simp [spinSign]) ⟨fun _ => .neg, rfl⟩ ⟨fun _ => .pos, rfl⟩).measurable.comp hY have hdom : Integrable (fun p => 2 * ((d : ℝ) * beta + (t : ℝ) + |X p|)) ρ := ((integrable_const _).add hXi).const_mul 2 have hFi : Integrable (finiteIsingBrownianEntropy beta D v B t) ρ := by apply hdom.mono' hF.aestronglyMeasurable exact Eventually.of_forall fun p => by rw [Real.norm_of_nonneg (finiteIsingBrownianEntropy_nonneg beta D v B t p)] exact finiteIsingBrownianEntropy_le_noise hbeta D v B t p refine ⟨hFi, ?_⟩ calc _ ≤ ∫ p, 2 * ((d : ℝ) * beta + (t : ℝ) + |X p|) ∂ρ := integral_mono hFi hdom (finiteIsingBrownianEntropy_le_noise hbeta D v B t) _ = 2 * ((d : ℝ) * beta + (t : ℝ) + ∫ p, |X p| ∂ρ) := by rw [integral_const_mul, integral_add (integrable_const _) hXi] simp [ρ] _ ≤ _ := mul_le_mul_of_nonneg_left (add_le_add le_rfl (integral_abs_gaussian_le_sqrt hX)) (by norm_num) theorem HasFreeIsingLaw.integral_finiteIsingBrownianNormalizedEnergy_le {d : ℕ} {beta : ℝ} {Ω : Type*} [MeasurableSpace Ω] {μ : Measure (TreeVertex d → IsingSpin)} (hμ : HasFreeIsingLaw (Real.tanh beta) μ) (hbeta : 0 ≤ beta) (ν : TreeVertex d → Measure Ω) {B : TreeVertex d → ℝ≥0 → Ω → ℝ} (hB : ∀ i, IsPreBrownianReal (B i) (ν i)) (hmB : ∀ i t, Measurable (B i t)) (D : Finset (TreeVertex d)) (hD : ConnectedFinset D) (v : D) {T : ℝ} (hT : 0 ≤ T) : let ρ := μ.prod (Measure.infinitePi ν) let E : ℝ → ℝ := fun t => ∫ p, ∑ u : D, finiteIsingBrownianNormalizedCovariance beta D v u B t p ^ 2 ∂ρ IntervalIntegrable E volume 0 T ∧ (∫ t in 0..T, E t) ≤ (∫ p, finiteIsingBrownianEntropy beta D v B T p ∂ρ) ∧ 0 ≤ (∫ t in 0..T, E t) ∧ (∫ t in 0..T, E t) ≤ 2 * ((d : ℝ) * beta + T + Real.sqrt T) := by classical let : IsProbabilityMeasure μ := hμ.isProbabilityMeasure let π := μ.map D.restrict let : IsProbabilityMeasure π := (Measure.isProbabilityMeasure_map_iff D.measurable_restrict.aemeasurable).mpr inferInstance let spin : (D → IsingSpin) → D → ℝ := fun eta u => spinSign (eta u) let q : (D → IsingSpin) → ℝ := fun eta => spinSign (eta v) let F : (D → ℝ) → ℝ := FinitePosterior.fieldEntropy (finiteIsingEnergy beta D) spin q let C : (D → ℝ) → D → ℝ := FinitePosterior.normalizedFieldCovariance (finiteIsingEnergy beta D) spin q let ρ := μ.prod (Measure.infinitePi ν) let ρG := π.prod (Measure.pi fun _ : D => gaussianReal 0 1) let EG : ℝ → ℝ := fun t => ∫ p, ∑ u : D, C (FinitePosterior.finiteStandardObservation spin t p) u ^ 2 ∂ρG let MG : ℝ → ℝ := fun t => ∫ p, F (FinitePosterior.finiteStandardObservation spin t p) ∂ρG let E : ℝ → ℝ := fun t => ∫ p, ∑ u : D, finiteIsingBrownianNormalizedCovariance beta D v u B t p ^ 2 ∂ρ let M : ℝ → ℝ := fun t => ∫ p, finiteIsingBrownianEntropy beta D v B t p ∂ρ have hcoords (eta : D → IsingSpin) (u : D) : spin eta u = -1 ∨ spin eta u = 1 := by dsimp only [spin] cases eta u <;> simp [spinSign] have hneg : ∃ eta, q eta = -1 := ⟨fun _ => .neg, rfl⟩ have hpos : ∃ eta, q eta = 1 := ⟨fun _ => .pos, rfl⟩ have hfm : Measurable F := (FinitePosterior.continuous_fieldEntropy _ _ _ (fun eta => hcoords eta v) hneg hpos).measurable have hcm : Measurable (fun y => ∑ u : D, C y u ^ 2) := (FinitePosterior.continuous_normalizedRowEnergy _ _ _ (fun eta => hcoords eta v) hneg hpos).measurable have hE (t : ℝ) (ht : 0 ≤ t) : E t = EG t := by have h := integral_finiteIsingBrownian_observation_eq_standard μ ν hB hmB D t.toNNReal (fun y => ∑ u : D, C y u ^ 2) hcm unfold E EG finiteIsingBrownianNormalizedCovariance finiteIsingBrownianObservation simpa only [C, spin, q, ρ, ρG, π, Real.coe_toNNReal t ht] using h have hM (t : ℝ) (ht : 0 ≤ t) : M t = MG t := by have h := integral_finiteIsingBrownian_observation_eq_standard μ ν hB hmB D t.toNNReal F hfm unfold M MG finiteIsingBrownianEntropy finiteIsingBrownianObservation simpa only [F, spin, q, ρ, ρG, π, Real.coe_toNNReal t ht] using h have hstd := FinitePosterior.integral_finiteStandardNormalizedEnergy_le π (finiteIsingEnergy beta D) (hμ.restrict_real_eq_normalized_exp D hD) spin q (fun eta => hcoords eta v) hneg hpos hcoords hT change IntervalIntegrable EG volume 0 T ∧ (∫ t in 0..T, EG t) ≤ MG T - F 0 ∧ 0 ≤ (∫ t in 0..T, EG t) at hstd have hzero : F 0 = 0 := finiteIsingEntropy_zero beta D v have hEq : EqOn EG E (uIcc 0 T) := by intro t ht exact (hE t (by simpa only [min_eq_left hT] using ht.1)).symm have hInt : (∫ t in 0..T, EG t) = ∫ t in 0..T, E t := intervalIntegral.integral_congr hEq have hle : (∫ t in 0..T, E t) ≤ M T := by simpa only [hzero, sub_zero, hInt, ← hM T hT] using hstd.2.1 have hterminal : M T ≤ 2 * ((d : ℝ) * beta + T + Real.sqrt T) := by have h := (finiteIsingBrownianEntropy_moment hbeta μ ν hB hmB D v T.toNNReal).2 simpa only [M, ρ, Real.coe_toNNReal T hT] using h change IntervalIntegrable E volume 0 T ∧ (∫ t in 0..T, E t) ≤ M T ∧ 0 ≤ (∫ t in 0..T, E t) ∧ (∫ t in 0..T, E t) ≤ _ exact ⟨hstd.1.congr (fun t ht => hEq (uIoc_subset_uIcc ht)), hle, by simpa only [hInt] using hstd.2.2, hle.trans hterminal⟩ theorem HasFreeIsingLaw.lintegral_finiteIsingBrownianNormalizedEnergy_le {d : ℕ} {beta : ℝ} {Ω : Type*} [MeasurableSpace Ω] {μ : Measure (TreeVertex d → IsingSpin)} (hμ : HasFreeIsingLaw (Real.tanh beta) μ) (hbeta : 0 ≤ beta) (ν : TreeVertex d → Measure Ω) {B : TreeVertex d → ℝ≥0 → Ω → ℝ} (hB : ∀ i, IsPreBrownianReal (B i) (ν i)) (hmB : ∀ i t, Measurable (B i t)) (D : Finset (TreeVertex d)) (hD : ConnectedFinset D) (v : D) {T : ℝ} (hT : 0 ≤ T) : (∫⁻ t in Ioc 0 T, ∫⁻ p, ENNReal.ofReal (∑ u : D, finiteIsingBrownianNormalizedCovariance beta D v u B t p ^ 2) ∂μ.prod (Measure.infinitePi ν)) ≤ ENNReal.ofReal (2 * ((d : ℝ) * beta + T + Real.sqrt T)) := by classical let : IsProbabilityMeasure μ := hμ.isProbabilityMeasure have (i : TreeVertex d) : IsProbabilityMeasure (ν i) := (hB i).isGaussianProcess.isProbabilityMeasure let ρ := μ.prod (Measure.infinitePi ν) let R := fun t p => ∑ u : D, finiteIsingBrownianNormalizedCovariance beta D v u B t p ^ 2 let E : ℝ → ℝ := fun t => ∫ p, R t p ∂ρ have hRpos (t : ℝ) (p) : 0 ≤ R t p := Finset.sum_nonneg fun u _ => sq_nonneg _ have hRI (t : ℝ) : Integrable (R t) ρ := by have hY : Measurable (finiteIsingBrownianObservation B D t) := by apply Measurable.of_eval intro w exact (((measurable_of_finite spinSign).comp ((measurable_pi_apply (w : TreeVertex d)).comp measurable_fst)).const_mul t).add ((hmB w t.toNNReal).comp ((measurable_pi_apply (w : TreeVertex d)).comp measurable_snd)) have hs (eta : D → IsingSpin) : spinSign (eta v) = -1 ∨ spinSign (eta v) = 1 := by cases eta v <;> simp [spinSign] have hn : ∃ eta : D → IsingSpin, spinSign (eta v) = -1 := ⟨fun _ => .neg, rfl⟩ have hp : ∃ eta : D → IsingSpin, spinSign (eta v) = 1 := ⟨fun _ => .pos, rfl⟩ apply Integrable.of_bound ((FinitePosterior.continuous_normalizedRowEnergy (finiteIsingEnergy beta D) (fun (eta : D → IsingSpin) w => spinSign (eta w)) (fun eta => spinSign (eta v)) hs hn hp).measurable.comp hY).aestronglyMeasurable (Fintype.card D) exact Eventually.of_forall fun p => by simpa only [Real.norm_eq_abs, Function.comp_def] using FinitePosterior.abs_normalizedRowEnergy_le_card (finiteIsingEnergy beta D) (fun (eta : D → IsingSpin) w => spinSign (eta w)) (fun eta => spinSign (eta v)) (finiteIsingBrownianObservation B D t p) hs hn hp (fun eta w => by cases eta w <;> norm_num [spinSign]) have hinner (t : ℝ) : (∫⁻ p, ENNReal.ofReal (R t p) ∂ρ) = ENNReal.ofReal (E t) := (ofReal_integral_eq_lintegral_ofReal (hRI t) (Eventually.of_forall (hRpos t))).symm have hbound := hμ.integral_finiteIsingBrownianNormalizedEnergy_le hbeta ν hB hmB D hD v hT have hEI : Integrable E (volume.restrict (Ioc 0 T)) := (intervalIntegrable_iff_integrableOn_Ioc_of_le hT).mp hbound.1 change (∫⁻ t in Ioc 0 T, ∫⁻ p, ENNReal.ofReal (R t p) ∂ρ) ≤ _ simp_rw [hinner] rw [← ofReal_integral_eq_lintegral_ofReal hEI (Eventually.of_forall fun t => integral_nonneg (hRpos t))] rw [← intervalIntegral.integral_of_le hT] exact ENNReal.ofReal_le_ofReal hbound.2.2.2 end Problem367 end end OAI