import QFD.Physics.Postulates import Mathlib.Analysis.SpecialFunctions.Pow.Real import Mathlib.Tactic.Linarith noncomputable section open QFD QFD.Physics namespace QFD.Lepton /-- **Theorem G.5: The Geometric Sign Flip.** This theorem proves that the sign flip in the g-2 anomaly between the electron and muon is a GEOMETRIC NECESSITY. Specifically: 1. For the electron (R_e = 1), V4 is strictly NEGATIVE. 2. For the muon (R_mu ≈ 0.0048), V4 is strictly POSITIVE. This occurs because R_mu < R_vac < R_e, where R_vac = 1/√5. -/ theorem geometric_sign_flip (beta : ℝ) (h_beta_pos : beta > 0) : let R_e := (1 : ℝ) let R_mu := (0.51099895 / 105.6583755 : ℝ) -- Electron V4 is negative V4_geometric R_e beta < 0 ∧ -- Muon V4 is positive V4_geometric R_mu beta > 0 := by -- Preliminaries: Constants are positive have h_phi_pos : phi_qfd > 0 := by unfold phi_qfd have h5 : 0 < Real.sqrt 5 := Real.sqrt_pos.mpr (by norm_num) linarith have h_xi_pos : xi_qfd > 0 := by unfold xi_qfd exact pow_pos h_phi_pos 2 have h_beta_inv_pos : xi_qfd / beta > 0 := div_pos h_xi_pos h_beta_pos -- 1. Prove R_vac < R_e (Electron scale factor is negative) have h_rvac : R_vac_qfd = 1 / Real.sqrt 5 := rfl have h_rvac_lt_1 : R_vac_qfd < 1 := by rw [h_rvac] -- 1/√5 < 1 because √5 > 1 have h5_pos : (0 : ℝ) < Real.sqrt 5 := Real.sqrt_pos.mpr (by norm_num) have h5 : 1 < Real.sqrt 5 := by rw [Real.lt_sqrt (by norm_num : (0 : ℝ) ≤ 1)] norm_num calc (1 : ℝ) / Real.sqrt 5 < 1 / 1 := by apply div_lt_div_of_pos_left (by norm_num) (by norm_num) h5 _ = 1 := by norm_num -- 2. Prove R_mu < R_vac (Muon scale factor is positive) have h_rmu : (0.51099895 / 105.6583755 : ℝ) < R_vac_qfd := by rw [h_rvac] -- 0.004836 < 1/2.236 ≈ 0.447 have h_rmu_val : (0.51099895 / 105.6583755 : ℝ) < 0.005 := by norm_num -- √5 < 3 because √5 < √9 = 3 have h_sqrt5_lt_3 : Real.sqrt 5 < 3 := by have h1 : Real.sqrt 5 < Real.sqrt 9 := by apply Real.sqrt_lt_sqrt (by norm_num : (0 : ℝ) ≤ 5) norm_num have h2 : Real.sqrt 9 = 3 := by have : (9 : ℝ) = 3 ^ 2 := by norm_num rw [this, Real.sqrt_sq (by norm_num : (0 : ℝ) ≤ 3)] linarith have h_rvac_val : (1 : ℝ) / 3 < 1 / Real.sqrt 5 := by apply one_div_lt_one_div_of_lt (Real.sqrt_pos.mpr (by norm_num : (5 : ℝ) > 0)) exact h_sqrt5_lt_3 have h_third : (0.3 : ℝ) < 1 / 3 := by norm_num linarith -- Now evaluate V4_geometric for both cases constructor · -- Case 1: Electron unfold V4_geometric let S_e := (R_vac_qfd - 1) / (R_vac_qfd + 1) have h_se_neg : S_e < 0 := by have h_num : R_vac_qfd - 1 < 0 := by linarith have h_den : R_vac_qfd + 1 > 0 := by have h_rv_pos : R_vac_qfd > 0 := div_pos (by norm_num) (Real.sqrt_pos.mpr (by norm_num)) linarith exact div_neg_of_neg_of_pos h_num h_den -- V4 = S_e * (xi/beta). Since S_e < 0 and xi/beta > 0, V4 < 0. exact mul_neg_of_neg_of_pos h_se_neg h_beta_inv_pos · -- Case 2: Muon unfold V4_geometric have h_smu_pos : (R_vac_qfd - 0.51099895 / 105.6583755) / (R_vac_qfd + 0.51099895 / 105.6583755) > 0 := by have h_num : R_vac_qfd - 0.51099895 / 105.6583755 > 0 := by linarith have h_den : R_vac_qfd + 0.51099895 / 105.6583755 > 0 := by have h_rv_pos : R_vac_qfd > 0 := div_pos (by norm_num) (Real.sqrt_pos.mpr (by norm_num)) have h_rm_pos : (0.51099895 / 105.6583755 : ℝ) > 0 := by norm_num linarith exact div_pos h_num h_den -- V4 = S_mu * (xi/beta). Since S_mu > 0 and xi/beta > 0, V4 > 0. exact mul_pos h_smu_pos h_beta_inv_pos end QFD.Lepton