import OAI.Probability.InvariantIsing.Fields.FieldTailMgf import OAI.Probability.InvariantIsing.Fields.FieldFiniteDomain import OAI.Probability.InvariantIsing.Magnetic.MagneticFieldInverseConvex namespace OAI /-! The canonical terminal field has a depth-independent second moment, controlled by the initial bias and the final covariance height. -/ noncomputable section open MeasureTheory ProbabilityTheory IsingPerceptron open scoped NNReal BigOperators namespace InvariantIsing lemma fieldTailVariance_total (h : FieldStep) : h.height 0 + fieldTailVariance (scalarFieldIncrements h) = h.height (Fin.last h.depth) := by have hs := fieldIncrement_sum h rw [Fin.sum_univ_succ] at hs have htail : fieldTailVariance (scalarFieldIncrements h) = ∑ i : Fin h.depth, (fieldIncrement h i.succ).2 := by simp only [fieldTailVariance, scalarFieldIncrements, List.map_ofFn, Function.comp_apply, NNReal.coe_mk, List.sum_ofFn] rw [htail] simpa [fieldIncrement] using hs theorem fieldCanonicalEndpointLaw_mgf (h : FieldStep) (b t : ℝ) : Integrable (fun y => Real.exp (t * y)) (fieldCanonicalEndpointLaw h b) ∧ (∫ y, Real.exp (t * y) ∂fieldCanonicalEndpointLaw h b) ≤ Real.exp (t * b + (t ^ 2 / 2 + |t|) * h.height (Fin.last h.depth)) := by let L := scalarFieldIncrements h have hL := scalarFieldIncrements_positive h have hB := scalarFieldIncrements_exponent_le_one h have hreg := fieldScalarValue_regular L hL measurable_logCosh logCosh_linearGrowth let root : ℝ≥0 := ⟨h.height 0, h.nonneg 0⟩ let κ := fieldTransitionKernel 0 root (fieldScalarValue L (fun y => Real.log (Real.cosh y))) hreg.1 have hκ (z : ℝ) := And.intro (fieldTransitionKernel_integrable_exp root z 0 t _ hreg.1 hreg.2) (fieldScalarTransition_mgf L hL root z 0 t le_rfl zero_le_one) have he := kernel_exp_bound_comp κ (fieldTailEndpointKernel L hL) t ((t ^ 2 / 2 + |t|) * root) ((t ^ 2 / 2 + |t|) * fieldTailVariance L) hκ (fieldTailEndpointKernel_mgf L hL hB t) b have hlaw : (fieldTailEndpointKernel L hL ∘ₖ κ) b = fieldCanonicalEndpointLaw h b := by rw [Kernel.comp_apply] dsimp only [κ] rw [fieldTransitionKernel_zero _ _ hreg.1 hreg.2] rfl rw [hlaw] at he refine ⟨he.1, he.2.trans_eq ?_⟩ congr 1 change t * b + (t ^ 2 / 2 + |t|) * h.height 0 + (t ^ 2 / 2 + |t|) * fieldTailVariance (scalarFieldIncrements h) = _ calc _ = t * b + (t ^ 2 / 2 + |t|) * (h.height 0 + fieldTailVariance (scalarFieldIncrements h)) := by ring _ = _ := by rw [fieldTailVariance_total] lemma sq_le_exp_two_add (x : ℝ) : x ^ 2 ≤ Real.exp (2 * x) + Real.exp (-2 * x) := by have ha : |x| ≤ Real.exp |x| := by linarith [Real.add_one_le_exp |x|] have hs := (sq_le_sq₀ (abs_nonneg x) (Real.exp_pos _).le).mpr ha rw [sq_abs] at hs rw [show (Real.exp |x|) ^ 2 = Real.exp (|x| + |x|) by rw [pow_two, Real.exp_add]] at hs by_cases hx : 0 ≤ x · rw [abs_of_nonneg hx, show x + x = 2 * x by ring] at hs linarith [Real.exp_pos (-2 * x)] · rw [abs_of_nonpos (le_of_not_ge hx), show -x + -x = -2 * x by ring] at hs linarith [Real.exp_pos (2 * x)] theorem fieldCanonicalEndpointLaw_second_moment (h : FieldStep) (b : ℝ) : Integrable (fun y : ℝ => y ^ 2) (fieldCanonicalEndpointLaw h b) ∧ (∫ y, y ^ 2 ∂fieldCanonicalEndpointLaw h b) ≤ Real.exp (2 * b + 4 * h.height (Fin.last h.depth)) + Real.exp (-2 * b + 4 * h.height (Fin.last h.depth)) := by have hp := fieldCanonicalEndpointLaw_mgf h b 2 have hn := fieldCanonicalEndpointLaw_mgf h b (-2) have hi : Integrable (fun y : ℝ => y ^ 2) (fieldCanonicalEndpointLaw h b) := by apply (hp.1.add hn.1).mono' (by fun_prop) exact ae_of_all _ (fun y => by rw [Real.norm_eq_abs, abs_of_nonneg (sq_nonneg _)] exact sq_le_exp_two_add y) refine ⟨hi, ?_⟩ have hle := integral_mono hi (hp.1.add hn.1) sq_le_exp_two_add simp only [Pi.add_apply] at hle rw [integral_add hp.1 hn.1] at hle norm_num at hp hn have hn' : (∫ y, Real.exp (-2 * y) ∂fieldCanonicalEndpointLaw h b) ≤ Real.exp (-2 * b + 4 * h.height (Fin.last h.depth)) := by simpa only [neg_mul] using hn.2 exact hle.trans (add_le_add hp.2 hn') end InvariantIsing end end OAI