import OAI.Probability.InvariantIsing.Core.PairGibbs namespace OAI /-! Exact two-replica off-diagonal Haar Ward identity. -/ noncomputable section open MeasureTheory IsingPerceptron open scoped BigOperators namespace InvariantIsing lemma abs_crossCoordinateProduct_le {N : ℕ} (i j : Fin N) (U : Orthogonal N) (σ τ : Spin N) : |spinCoordinate U σ i * spinCoordinate U τ j| ≤ N := by have hi := spinCoordinate_sq_le U σ i have hj := spinCoordinate_sq_le U τ j rw [abs_mul] nlinarith [sq_nonneg (|spinCoordinate U σ i| - |spinCoordinate U τ j|), sq_abs (spinCoordinate U σ i), sq_abs (spinCoordinate U τ j)] def offCoordinateProduct {N : ℕ} (i j : Fin N) (F : Spin N → Spin N → ℝ) (U : Orthogonal N) (x : Spin N × Spin N) : ℝ := spinCoordinate U x.1 i * spinCoordinate U x.2 j * F x.1 x.2 def offCoordinateVariation {N : ℕ} (i j : Fin N) (F : Spin N → Spin N → ℝ) (U : Orthogonal N) (x : Spin N × Spin N) : ℝ := (spinCoordinate U x.1 j * spinCoordinate U x.2 j - spinCoordinate U x.1 i * spinCoordinate U x.2 i) * F x.1 x.2 lemma hasDerivAt_offCoordinateProduct {N : ℕ} (i j : Fin N) (hij : i ≠ j) (F : Spin N → Spin N → ℝ) (U : Orthogonal N) (x : Spin N × Spin N) (t : ℝ) : HasDerivAt (fun s => offCoordinateProduct i j F (planeRotation i j s * U) x) (offCoordinateVariation i j F (planeRotation i j t * U) x) t := by have hd := ((hasDerivAt_planeRotation_coordinate i j i U (spinVector x.1) t).mul (hasDerivAt_planeRotation_coordinate i j j U (spinVector x.2) t)).mul_const (F x.1 x.2) convert hd using 1 · rfl · simp only [offCoordinateVariation, spinCoordinate, ite_true, hij, Ne.symm hij, ite_false, sub_zero, zero_sub] ring /-- Exact finite off-diagonal rotation identity. The spin test is fixed during rotation; in the main application it is a function of the rotation-invariant total overlap. Arbitrary deterministic nonzero positive priors are allowed. -/ theorem offDiagonal_coordinate_ward_identity {N : ℕ} (i j : Fin N) (hij : i ≠ j) (μ : Measure (Orthogonal N)) [IsProbabilityMeasure μ] [μ.IsMulLeftInvariant] {w : Spin N → ℝ} (hw : GibbsReference w) (eig c : Fin N → ℝ) (F : Spin N → Spin N → ℝ) (B : ℝ) (hB : 0 ≤ B) (hF : ∀ σ τ, |F σ τ| ≤ B) : (∫ U, gibbsPairAverage w (orbitHamiltonian eig c U) (fun σ τ => (spinCoordinate U σ j * spinCoordinate U τ j - spinCoordinate U σ i * spinCoordinate U τ i) * F σ τ) + (eig i - eig j) * (gibbsPairAverage w (orbitHamiltonian eig c U) (fun σ τ => spinCoordinate U σ i * spinCoordinate U τ j * F σ τ * (coordinateProduct i j U σ + coordinateProduct i j U τ)) - 2 * gibbsPairAverage w (orbitHamiltonian eig c U) (fun σ τ => spinCoordinate U σ i * spinCoordinate U τ j * F σ τ) * gibbsAverage w (orbitHamiltonian eig c U) (coordinateProduct i j U)) ∂μ) = 0 := by let R := planeRotation i j let H : Orthogonal N → Spin N × Spin N → ℝ := fun U x => orbitHamiltonian eig c U x.1 + orbitHamiltonian eig c U x.2 let A := offCoordinateProduct i j F let dH : ℝ → Orthogonal N → Spin N × Spin N → ℝ := fun t U x => (eig i - eig j) * (coordinateProduct i j (R t * U) x.1 + coordinateProduct i j (R t * U) x.2) let dA : ℝ → Orthogonal N → Spin N × Spin N → ℝ := fun t U => offCoordinateVariation i j F (R t * U) have hR : R 0 = 1 := planeRotation_zero i j have hP (σ : Spin N) : Measurable (fun U : Orthogonal N => coordinateProduct i j U σ) := (measurable_spinCoordinate σ i).mul (measurable_spinCoordinate σ j) have hAm (x : Spin N × Spin N) : Measurable (fun U : Orthogonal N => A U x) := ((measurable_spinCoordinate x.1 i).mul (measurable_spinCoordinate x.2 j)).mul_const _ have hHm (x : Spin N × Spin N) : Measurable (fun U => H U x) := (measurable_orbitHamiltonian eig c x.1).add (measurable_orbitHamiltonian eig c x.2) have hdHm (x : Spin N × Spin N) : Measurable (fun U => dH 0 U x) := by simp only [dH, hR, one_mul] exact ((hP x.1).add (hP x.2)).const_mul _ have hdAm (x : Spin N × Spin N) : Measurable (fun U => dA 0 U x) := by simp only [dA, hR, one_mul, offCoordinateVariation] exact (((measurable_spinCoordinate x.1 j).mul (measurable_spinCoordinate x.2 j)).sub ((measurable_spinCoordinate x.1 i).mul (measurable_spinCoordinate x.2 i))).mul_const _ have hHd : ∀ U t, t ∈ Set.Ioo (-1 : ℝ) 1 → ∀ x, HasDerivAt (fun s => H (R s * U) x) (dH t U x) t := by intro U t _ x have h1 := (hasDerivAt_planeRotation_energy i j U eig x.1 t).add_const (fieldEnergy c x.1) have h2 := (hasDerivAt_planeRotation_energy i j U eig x.2 t).add_const (fieldEnergy c x.2) convert h1.add h2 using 1 · rfl · dsimp only [dH, R, coordinateProduct, spinCoordinate] ring have hAd : ∀ U t, t ∈ Set.Ioo (-1 : ℝ) 1 → ∀ x, HasDerivAt (fun s => A (R s * U) x) (dA t U x) t := by intro U t _ x exact hasDerivAt_offCoordinateProduct i j hij F U x t have hAb : ∀ U x, |A U x| ≤ N * B := by intro U x rw [show A U x = spinCoordinate U x.1 i * spinCoordinate U x.2 j * F x.1 x.2 from rfl, abs_mul] exact mul_le_mul (abs_crossCoordinateProduct_le i j U x.1 x.2) (hF x.1 x.2) (abs_nonneg _) (Nat.cast_nonneg _) have hHb : ∀ U t, t ∈ Set.Ioo (-1 : ℝ) 1 → ∀ x, |dH t U x| ≤ |eig i - eig j| * (2 * N) := by intro U t _ x dsimp only [dH] rw [abs_mul] apply mul_le_mul_of_nonneg_left _ (abs_nonneg _) have hs := (abs_add_le _ _).trans (add_le_add (abs_coordinateProduct_le i j (R t * U) x.1) (abs_coordinateProduct_le i j (R t * U) x.2)) linarith have hAdb : ∀ U t, t ∈ Set.Ioo (-1 : ℝ) 1 → ∀ x, |dA t U x| ≤ 2 * N * B := by intro U t _ x dsimp only [dA, offCoordinateVariation] rw [abs_mul] apply mul_le_mul _ (hF x.1 x.2) (abs_nonneg _) (by positivity) have hs := (abs_sub _ _).trans (add_le_add (abs_crossCoordinateProduct_le j j (R t * U) x.1 x.2) (abs_crossCoordinateProduct_le i i (R t * U) x.1 x.2)) linarith have hwrd := integral_gibbs_rotation_identity μ R hR (GibbsReference_pair hw) H A hHm hAm dH dA hdHm hdAm hHd hAd (N * B) (|eig i - eig j| * (2 * N)) (2 * N * B) (by positivity) hAb hHb hAdb simp only [dH, dA, H, A, hR, one_mul, offCoordinateProduct] at hwrd convert hwrd using 1 congr 1 funext U unfold offCoordinateVariation offCoordinateProduct rw [gibbsAverage_pair w (orbitHamiltonian eig c U) (fun σ τ => (spinCoordinate U σ j * spinCoordinate U τ j - spinCoordinate U σ i * spinCoordinate U τ i) * F σ τ)] have hfactor : (fun x : Spin N × Spin N => spinCoordinate U x.1 i * spinCoordinate U x.2 j * F x.1 x.2 * ((eig i - eig j) * (coordinateProduct i j U x.1 + coordinateProduct i j U x.2))) = (fun x => (eig i - eig j) * (spinCoordinate U x.1 i * spinCoordinate U x.2 j * F x.1 x.2 * (coordinateProduct i j U x.1 + coordinateProduct i j U x.2))) := by funext x ring rw [hfactor, gibbsAverage_const_mul, gibbsAverage_const_mul, gibbsAverage_pair_sum hw] rw [gibbsAverage_pair w (orbitHamiltonian eig c U) (fun σ τ => spinCoordinate U σ i * spinCoordinate U τ j * F σ τ * (coordinateProduct i j U σ + coordinateProduct i j U τ)), gibbsAverage_pair w (orbitHamiltonian eig c U) (fun σ τ => spinCoordinate U σ i * spinCoordinate U τ j * F σ τ)] ring end InvariantIsing end end OAI