import OAI.Geometry.EinsteinFour.AngularQuadratic namespace OAI /-! The actual change of normal bases `I_s q` and `J_t q`. Its spherical orthogonality is a consequence of the fourth monomial moment. -/ namespace PositiveEinsteinFour.Angular open Matrix noncomputable section def oppositeMatrix (s : Fin 3) : Mat4 := Geometry.oppositeQuaternion s def mixingCoefficient (r s : Fin 3) : Mat4 := (TraceHessian.quaternionMatrix r)ᵀ * oppositeMatrix s def coefficientTable (r s : Fin 3) : Mat4 := ![![![![-1, 0, 0, 0], ![0, -1, 0, 0], ![0, 0, 1, 0], ![0, 0, 0, 1]], ![![0, 0, 0, 1], ![0, 0, -1, 0], ![0, -1, 0, 0], ![1, 0, 0, 0]], ![![0, 0, -1, 0], ![0, 0, 0, -1], ![-1, 0, 0, 0], ![0, -1, 0, 0]]], ![![![0, 0, 0, -1], ![0, 0, -1, 0], ![0, -1, 0, 0], ![-1, 0, 0, 0]], ![![-1, 0, 0, 0], ![0, 1, 0, 0], ![0, 0, -1, 0], ![0, 0, 0, 1]], ![![0, 1, 0, 0], ![1, 0, 0, 0], ![0, 0, 0, -1], ![0, 0, -1, 0]]], ![![![0, 0, 1, 0], ![0, 0, 0, -1], ![1, 0, 0, 0], ![0, -1, 0, 0]], ![![0, -1, 0, 0], ![-1, 0, 0, 0], ![0, 0, 0, -1], ![0, 0, -1, 0]], ![![-1, 0, 0, 0], ![0, 1, 0, 0], ![0, 0, 1, 0], ![0, 0, 0, -1]]]] r s theorem mixingCoefficient_eq_table (r s : Fin 3) : mixingCoefficient r s = coefficientTable r s := by ext i j simp only [mixingCoefficient, Matrix.mul_apply, Matrix.transpose_apply] fin_cases r <;> fin_cases s <;> fin_cases i <;> fin_cases j <;> norm_num [TraceHessian.quaternionMatrix, oppositeMatrix, Geometry.oppositeQuaternion, coefficientTable, Fin.sum_univ_succ] def mixing (r s : Fin 3) (q : Directions) : ℝ := quadratic (mixingCoefficient r s) q def mixingMatrix (q : Directions) : Geometry.Mat3 := fun r s => mixing r s q theorem mixingCoefficient_symmetric (r s : Fin 3) : (mixingCoefficient r s)ᵀ = mixingCoefficient r s := by rw [mixingCoefficient_eq_table] ext i j change coefficientTable r s j i = coefficientTable r s i j fin_cases r <;> fin_cases s <;> fin_cases i <;> fin_cases j <;> norm_num [coefficientTable] theorem mixingCoefficient_trace (r s : Fin 3) : (mixingCoefficient r s).trace = 0 := by rw [mixingCoefficient_eq_table] fin_cases r <;> fin_cases s <;> norm_num [coefficientTable, Matrix.trace, Matrix.diag, Fin.sum_univ_succ] theorem mixingCoefficient_pairing (r s t u : Fin 3) : (∑ i, ∑ j, mixingCoefficient r s i j * mixingCoefficient t u i j) = if r = t then (if s = u then (4 : ℝ) else 0) else 0 := by simp only [mixingCoefficient_eq_table] fin_cases r <;> fin_cases s <;> fin_cases t <;> fin_cases u <;> norm_num [coefficientTable, Fin.sum_univ_succ] theorem integral_mixing_mul (h : FollandMoments) (r s t u : Fin 3) : (∫ q, mixing r s q * mixing t u q ∂sphereMeasure) = if r = t then (if s = u then (1 / 3 : ℝ) else 0) else 0 := by unfold mixing rw [integral_quadratic_mul_traceFree h _ _ (mixingCoefficient_trace r s) (mixingCoefficient_trace t u) (mixingCoefficient_symmetric t u), mixingCoefficient_pairing] split_ifs <;> norm_num theorem direction_sum_sq (q : Directions) : (∑ i, q.val i ^ 2) = 1 := by have h := congrArg (fun x : ℝ => x ^ 2) q.property simpa only [EuclideanSpace.real_norm_sq_eq, one_pow] using h /-- The two triples give orthonormal normal bases for every unit direction. -/ theorem mixing_orthogonal (q : Directions) : mixingMatrix q * (mixingMatrix q)ᵀ = 1 := by ext i j change (∑ s, mixing i s q * mixing j s q) = if i = j then 1 else 0 calc _ = (∑ a, q.val a ^ 2) ^ 2 * (if i = j then 1 else 0) := by simp only [mixing, quadratic, mixingCoefficient_eq_table] fin_cases i <;> fin_cases j <;> simp [coefficientTable, Fin.sum_univ_succ] all_goals ring _ = _ := by rw [direction_sum_sq]; simp end end PositiveEinsteinFour.Angular end OAI