Encyclopedia Masses Masses Electroweak Masses Cos2 Theta Positive
ARTICLE 3 claims 2 theorems 1 model
Masses Electroweak Masses Cos2 Theta Positive
In the standard model, the Weinberg angle mixes the electromagnetic and weak forces; the framework's derivation of its cosine-squared value is a small, fully checked piece of a larger puzzle.
The Weinberg angle in the framework
The Weinberg angle, often written θ_W, is the standard model parameter that describes how the electromagnetic and weak nuclear forces mix. Its sine-squared value is measured to be about 0.231, and it is not predicted by the standard model itself; it is an input. The Recognition Science framework, a machine-checked library of formal theorems, offers a derivation of this number from its own principles. The declaration cos2_theta_positive establishes a simple but necessary fact about that derivation: the cosine-squared of the framework's Weinberg angle is a positive number.
The framework's value for the sine-squared of the Weinberg angle is (3 − φ)/6, where φ is the golden ratio. The declaration cos2_theta_positive proves that the cosine-squared, defined as 1 minus that sine-squared, is greater than zero. This is not a derivation of the angle itself; it is a sanity check on the derived value. The proof is a short argument that uses the fact that the sine-squared value is less than one half, which is itself a proved theorem. The positivity of the cosine-squared ensures that the framework's Weinberg angle is a real, physical angle, not an imaginary one.
In the standard model, the W boson mass is related to the Z boson mass by the cosine of the Weinberg angle: m_W = m_Z cos θ_W. The framework uses this relation to derive the W mass from its Z mass prediction. The positivity of cos²θ_W is a prerequisite for taking the square root to get cos θ_W, which is needed for that mass calculation. The declaration is therefore a small but load-bearing piece of the framework's electroweak sector: it guarantees that the W mass prediction is a real number.
The declaration does not claim that the framework's Weinberg angle matches the measured value. The framework's sine-squared value is approximately 0.236, which is about 2% higher than the measured 0.231. The framework does not claim to derive the standard model's Weinberg angle; it derives its own value from its own principles. The agreement with experiment is not part of the theorem; it is a separate empirical check. The positivity theorem is a purely mathematical statement about the framework's own definitions.
THEOREM cos2_theta_positive · IndisputableMonolith/Masses/ElectroweakMasses.lean
theorem cos2_theta_positive : 0 < cos2_theta_W_rs := by
unfold cos2_theta_W_rs; linarith [sin2_theta_lt_half]
MODEL sin2_theta_W_rs · IndisputableMonolith/Masses/ElectroweakMasses.lean
noncomputable def sin2_theta_W_rs : ℝ := (3 - Constants.phi) / 6
THEOREM sin2_theta_lt_half · IndisputableMonolith/Masses/ElectroweakMasses.lean
theorem sin2_theta_lt_half : sin2_theta_W_rs < 1/2 := by
unfold sin2_theta_W_rs
have hphi : 0 < Constants.phi := phi_pos
linarith
What this page does not claim
The framework's Weinberg angle matches the measured value. The framework derives the standard model's Weinberg angle. The positivity theorem is a derivation of the angle itself.
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Derived articles
This page is generated by a question-recursion engine: the questions its answers raise become the next pages. The current agenda, with open targets marked red:
- How does the framework derive its value for the sine-squared of the Weinberg angle?
- What is the empirical significance of the framework's Weinberg angle being about 2% higher than the measured value?
- What other electroweak parameters does the framework derive from its rung structure?
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THEOREM cos2_theta_positive · IndisputableMonolith/Masses/ElectroweakMasses.lean
theorem cos2_theta_positive : 0 < cos2_theta_W_rs := by unfold cos2_theta_W_rs; linarith [sin2_theta_lt_half]The declaration cos2_theta_positive establishes that the cosine-squared of the framework's Weinberg angle is a positive number. cos2_theta_positive · IndisputableMonolith/Masses/ElectroweakMasses.leanMODEL sin2_theta_W_rs · IndisputableMonolith/Masses/ElectroweakMasses.lean
noncomputable def sin2_theta_W_rs : ℝ := (3 - Constants.phi) / 6The framework's value for the sine-squared of the Weinberg angle is (3 − φ)/6, where φ is the golden ratio. sin2_theta_W_rs · IndisputableMonolith/Masses/ElectroweakMasses.leanTHEOREM sin2_theta_lt_half · IndisputableMonolith/Masses/ElectroweakMasses.lean
theorem sin2_theta_lt_half : sin2_theta_W_rs < 1/2 := by unfold sin2_theta_W_rs have hphi : 0 < Constants.phi := phi_pos linarithThe proof of cos2_theta_positive uses the fact that the sine-squared value is less than one half. sin2_theta_lt_half · IndisputableMonolith/Masses/ElectroweakMasses.lean