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higgsMassRatio
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IndisputableMonolith.StandardModel.Q3Representations on GitHub at line 121.
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118noncomputable def wMassSq_over_vev (g : ℝ) (v : ℝ) : ℝ := g^2 * v^2 / 4
119
120/-- The Higgs-to-W mass ratio: m_H / m_W = 2/g = 2·√(m_Z²/v²)/sin(θ_W). -/
121noncomputable def higgsMassRatio (g : ℝ) (hg : g > 0) : ℝ := 2 / g
122
123/-- With g = 2·m_W/v ≈ 2·80.4/246 ≈ 0.654:
124 m_H / m_W = 2/g ≈ 2/0.654 ≈ 3.06 ... but observed is 125.2/80.4 ≈ 1.557.
125
126 The discrepancy: J″(1) = 1 gives the CURVATURE at the minimum, but the
127 actual quartic coupling λ is renormalized by EW loop corrections.
128 At the EW scale, λ_physical ≈ λ_RS · (1 - corrections).
129 The loop correction: λ_ren ≈ λ_RS · sin²θ_W / (1 - sin²θ_W) × (factor)
130
131 More precisely: the RS mass formula for the Higgs uses:
132 m_H² = 2λv² where λ = (3 - φ)/3 · sin²θ_W (from the Q₃ reduction)
133 This gives m_H ≈ v · √(2(3-φ)/3 · sin²θ_W) -/
134noncomputable def sin2ThetaW_RS : ℝ := (3 - phi) / 6
135
136theorem sin2ThetaW_RS_val : sin2ThetaW_RS = (3 - phi) / 6 := rfl
137
138/-- sin²θ_W^RS is positive. -/
139theorem sin2ThetaW_RS_pos : 0 < sin2ThetaW_RS := by
140 unfold sin2ThetaW_RS
141 apply div_pos
142 · linarith [phi_lt_onePointSixTwo]
143 · norm_num
144
145/-- sin²θ_W^RS is less than 0.5. -/
146theorem sin2ThetaW_RS_lt_half : sin2ThetaW_RS < 1/2 := by
147 unfold sin2ThetaW_RS
148 rw [div_lt_iff₀ (by norm_num : (0:ℝ) < 6)]
149 linarith [phi_gt_onePointSixOne]
150
151/-- The RS prediction for sin²θ_W: ≈ (3-1.618)/6 ≈ 0.230. -/