import Mathlib import OAI.Probability.LogConcave.Numerics.CompositeAngle import OAI.Probability.LogConcave.Complexity.HarmonicCorrectionBudget namespace OAI section section noncomputable section namespace LogConcaveSampling open Set MeasureTheory open scoped Classical BigOperators NNReal RealInnerProductSpace open TensorEnergy Quadrature local instance : DecidableEq Unit := Classical.decEq _ def angleNodes (n : ℕ) (i : Fin (n+1)) : ℝ := (i:ℝ) lemma angleNodes_injective (n : ℕ) : Function.Injective (angleNodes n) := by intro i j h apply Fin.ext change (i:ℝ)=(j:ℝ) at h exact_mod_cast h lemma liePathJet_measurable {S : Type} [Fintype S] {d : ℕ} {H : Point d → ℝ} (hH : PolySmooth H) (A : (Unit ⊕ Unit → Fin d) → Point d → ℝ) (F : (S → Fin d) → Point d → ℝ) (hA : ∀c,PolySmooth (A c)) (hF : ∀c,PolySmooth (F c)) (Ξ : Point d → ℝ → Point d) (hm : Measurable (fun p : ℝ × Point d => Ξ p.2 p.1)) (k : ℕ) (v : ℝ) : Measurable (fun y => tensorVector (iterTensorLie H A F k) (Ξ y v)) := (tensorVector_contDiff _ (fun c => (iterTensorLie_polySmooth hH A F hA hF k c).smooth)).continuous.measurable.comp (hm.comp (measurable_const.prodMk measurable_id)) lemma chainTaylor_measurable {Ω E : Type*} [MeasurableSpace Ω] [NormedAddCommGroup E] [NormedSpace ℝ E] [MeasurableSpace E] [BorelSpace E] [SecondCountableTopology E] (J : ℕ → ℝ → Ω → E) (hm : ∀k t,Measurable (J k t)) (n : ℕ) (a b : ℝ) : Measurable (fun y => chainTaylor (fun k t => J k t y) n a b) := by unfold chainTaylor exact Finset.measurable_sum _ (fun k _ => (hm k a).const_smul _) theorem harmonic_correction_stencil_rms {d : ℕ} {F : Point d → ℝ} {lam : ℝ≥0} (hF : Primitive F lam) (x : Point d) {r R T : ℝ} (hr : 0 Ξ p.2 p.1)) (hlaw : ∀v∈Icc (0:ℝ) 1,(gibbs (centeringPotential F x r u)).map (fun y => Ξ y v)= gibbs (centeringPotential F x r u)) : let A := jointCorrectionArray (fun z => probabilityTransport hF x hr.le hl hT0 hT1 s t z-z) let J := fun k v y => tensorVector (iterTensorLie (centeringPotential F x r u) (harmonicSkew d) A k) (Ξ y v) ∀n : ℕ,1≤n → ∀ψ : ℝ,0<ψ → ψ*n≤1 → Integrable (fun y => ‖derivativeStencil (angleNodes n) ψ (fun i => J 0 (ψ*angleNodes n i) y)-J 1 0 y‖^2) (gibbs (centeringPotential F x r u)) ∧ (∫y,‖derivativeStencil (angleNodes n) ψ (fun i => J 0 (ψ*angleNodes n i) y)-J 1 0 y‖^2 ∂gibbs (centeringPotential F x r u))≤ ((∑i,|derivativeWeight (angleNodes n) i|)/ψ)^2* (((ψ*n)^(n+1)/(n.factorial:ℝ))^2* ((d*((lam:ℝ)*r^2)^2)*(R⁻¹)^(4*(n+1))*harmonicCorrectionBudget (n+1))) := by intro A J n hn ψ hψ hψn have hu1 := u.2.2.trans_lt hT1 have hH : PolySmooth (centeringPotential F x r u) := productPotential_polySmooth (interpolationPotential_polySmooth hF x hr hlam hl u.2.1 hu1) (gaussianPotential_polySmooth d) have hJ (k : ℕ) (v : ℝ) : Measurable (J k v) := liePathJet_measurable hH (harmonicSkew d) A (harmonicSkew_polySmooth d) (jointCorrectionArray_polySmooth hF x hr hlam hl hR hRT hT0 hT1 s t) Ξ hm k v have hnode (i : Fin (n+1)) : 0≤ψ*angleNodes n i ∧ ψ*angleNodes n i≤ψ*n := by constructor · exact mul_nonneg hψ.le (Nat.cast_nonneg _) · apply mul_le_mul_of_nonneg_left _ hψ.le change (i:ℝ)≤(n:ℝ) exact_mod_cast Nat.le_of_lt_succ i.2 have htay (i : Fin (n+1)) := harmonic_correction_taylor_rms hF x hr hlam hl hR hRT hT0 hT1 s t u Ξ hder hm hlaw n 0 (ψ*angleNodes n i) le_rfl (hnode i).1 ((hnode i).2.trans hψn) apply derivative_stencil_error_rms (angleNodes n) (angleNodes_injective n) n hn (by simp) hψ J · intro i exact ((hJ 0 _).sub (chainTaylor_measurable J hJ n 0 _)).aestronglyMeasurable · intro i simpa only [J,iterTensorLie,sub_zero] using (htay i).1 · intro i have hh := (htay i).2 change (∫y,‖J 0 (ψ*angleNodes n i) y-chainTaylor (fun k v => J k v y) n 0 (ψ*angleNodes n i)‖^2 ∂gibbs (centeringPotential F x r u))≤_ at hh apply hh.trans simp only [sub_zero] apply mul_le_mul_of_nonneg_right _ (by positivity [harmonicCorrectionBudget_nonneg (n+1)]) apply pow_le_pow_left₀ (div_nonneg (pow_nonneg (hnode i).1 _) (Nat.cast_nonneg _)) apply div_le_div_of_nonneg_right _ (Nat.cast_nonneg _) exact pow_le_pow_left₀ (hnode i).1 (hnode i).2 _ end LogConcaveSampling end end end end OAI