Encyclopedia Physics Physics Electroweak Bosons
ARTICLE 5 claims 2 theorems 3 measured
Physics Electroweak Bosons
The W and Z bosons are the heavy particles that carry the weak nuclear force, the force behind radioactive decay.
The weak force carriers
The W and Z bosons are the carriers of the weak nuclear force, the interaction responsible for radioactive beta decay and the fusion reactions that power the Sun. Unlike the massless photon, which carries the electromagnetic force, the W and Z bosons are extremely heavy. The W boson has a measured mass of about 80.37 GeV, and the Z boson is heavier at about 91.19 GeV. Their masses are not arbitrary; in the Standard Model of particle physics, they arise from the Higgs mechanism, in which a field called the Higgs field acquires a nonzero value everywhere in space, breaking the electroweak symmetry and giving mass to these particles.
The relationship between the two masses is set by the weak mixing angle, also called the Weinberg angle θW. The theory predicts that mZ = mW / cos(θW), and the measured masses obey this relation. The sine squared of this angle, sin²θW, is measured to be about 0.231. This angle also connects the electromagnetic and weak couplings, describing how the two forces mix. The Higgs field's vacuum expectation value, the constant background value it takes everywhere, is about 246 GeV, which sets the overall scale for the W and Z masses.
In Recognition Science, the framework models the electroweak sector by placing these known quantities on its phi-ladder, a sequence of powers of the golden ratio φ ≈ 1.618. The framework's library, a machine-checked collection of formal theorems, defines the vacuum expectation value at 246.22 GeV and the measured masses as constants. It proves several basic facts about them: the W boson mass is near 80 GeV, the Z boson mass is near 91 GeV, the Z is heavier than the W, and the ratio of the W mass to the Z mass is close to cos(θW), within 0.005. It also proves that the ratio of the Higgs boson mass to the W mass is within 0.1 of the golden ratio φ itself, a numerical coincidence the framework highlights.
These are not derivations of the masses from first principles. The framework takes the measured values as definitions and then proves approximate relations among them. The theorem that the W-to-Z mass ratio equals cos(θW) is a formal restatement of the Standard Model relation, not a new prediction. The framework's contribution is to show that these numbers sit on its phi-ladder and that some simple ratios among them approximate φ, but it does not explain why the vacuum expectation value takes the value it does. The origin of the electroweak scale remains an open target.
MEASURED wBosonMass_GeV · zBosonMass_GeV · IndisputableMonolith/Physics/ElectroweakBosons.lean
/-- W boson mass in GeV. -/
def wBosonMass_GeV : ℝ := 80.3692
/-- Z boson mass in GeV. -/
def zBosonMass_GeV : ℝ := 91.1876
THEOREM wz_ratio_equals_cos_theta · IndisputableMonolith/Physics/ElectroweakBosons.lean
/-- Predicted W/Z ratio = cos(θW). -/
theorem wz_ratio_equals_cos_theta :
|wz_mass_ratio - cos_theta_W| < 0.005 := by
-- wz_mass_ratio = 80.3692 / 91.1876 ≈ 0.88136
-- cos_theta_W = sqrt(1 - 0.23122) = sqrt(0.76878) ≈ 0.87683
-- |0.88136 - 0.87683| = 0.00453 < 0.005
simp only [wz_mass_ratio, wBosonMass_GeV, zBosonMass_GeV, cos_theta_W, sin2_theta_W]
-- Need: |80.3692/91.1876 - sqrt(0.76878)| < 0.005
-- Bounds on ratio: 0.8813 < ratio < 0.8814
have h_ratio_lo : (80.3692 : ℝ) / 91.1876 > 0.8813 := by norm_num
have h_ratio_hi : (80.3692 : ℝ) / 91.1876 < 0.8814 := by norm_num
-- Bounds on sqrt: 0.8768 < sqrt(0.76878) < 0.8769
-- 0.8768^2 = 0.76877824, 0.8769^2 = 0.76895361
have h_sqrt_lo : sqrt 0.76878 > 0.8768 := by
have h_sq : (0.8768 : ℝ)^2 < 0.76878 := by norm_num
exact (Real.lt_sqrt (by norm_num : (0 : ℝ) ≤ 0.8768)).mpr h_sq
have h_sqrt_hi : sqrt 0.76878 < 0.8769 := by
have h_sq : 0.76878 < (0.8769 : ℝ)^2 := by norm_num
have h_pos : (0 : ℝ) ≤ 0.76878 := by norm_num
have h := Real.sqrt_lt_sqrt h_pos h_sq
simp only [Real.sqrt_sq (by norm_num : (0 : ℝ) ≤ 0.8769)] at h
exact h
-- Difference: (0.8813, 0.8814) - (0.8768, 0.8769) = (0.0044, 0.0046)
rw [abs_lt]
constructor <;> linarith
MEASURED sin2_theta_W · IndisputableMonolith/Physics/ElectroweakBosons.lean
/-- Weak mixing angle sin²θW (on-shell scheme). -/
def sin2_theta_W : ℝ := 0.23122
MEASURED vev_GeV · IndisputableMonolith/Physics/ElectroweakBosons.lean
/-- Higgs VEV in GeV. -/
def vev_GeV : ℝ := 246.22
THEOREM higgs_w_near_phi · IndisputableMonolith/Physics/ElectroweakBosons.lean
/-- Higgs to W ratio ≈ 1.56 ≈ φ. -/
theorem higgs_w_near_phi : |higgs_w_ratio - phi| < 0.1 := by
-- 125.25 / 80.3692 ≈ 1.5585, φ ∈ (1.61, 1.62)
-- |1.5585 - 1.618| ≈ 0.06 < 0.1
simp only [higgs_w_ratio, higgsMass_GeV, wBosonMass_GeV]
have hphi_lo : phi > 1.61 := phi_gt_onePointSixOne
have hphi_hi : phi < 1.62 := phi_lt_onePointSixTwo
have h1 : (125.25 : ℝ) / 80.3692 > 1.55 := by norm_num
have h2 : (125.25 : ℝ) / 80.3692 < 1.56 := by norm_num
rw [abs_lt]
constructor <;> linarith
What this page does not claim
No derivation of the W and Z masses from the framework's cost function is claimed. No explanation for the value of the weak mixing angle is claimed. No claim that the electroweak scale is uniquely forced by the framework is made.
Verify this page
Every tagged claim above names its theorem. To check one yourself rather than trust this page, elaborate the source module with Lean 4 and audit its axiom basis:
$ lake env lean IndisputableMonolith/Physics/ElectroweakBosons.lean
expected axiom basis: [propext, Classical.choice, Quot.sound] (the Lean kernel's standard three; no RS-specific axioms)
A page whose claims cannot be reproduced this way does not ship. In production, every anchor links to the exact declaration in the public source release, and this block carries the build receipt for the page itself.
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:
- Why does the vacuum expectation value of the Higgs field take the value 246 GeV?
- What physical mechanism, if any, places the electroweak scale on the phi-ladder?
- Does the framework derive the weak mixing angle from its geometric structure, or only fit it?
- What is the significance of the Higgs-to-W mass ratio being close to the golden ratio?
- How does the framework's phi-ladder relate to the measured masses of other particles?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
MEASURED wBosonMass_GeV · zBosonMass_GeV · IndisputableMonolith/Physics/ElectroweakBosons.lean
/-- W boson mass in GeV. -/ def wBosonMass_GeV : ℝ := 80.3692/-- Z boson mass in GeV. -/ def zBosonMass_GeV : ℝ := 91.1876The W boson has a measured mass of about 80.37 GeV, and the Z boson is heavier at about 91.19 GeV. wBosonMass_GeV · zBosonMass_GeV · IndisputableMonolith/Physics/ElectroweakBosons.leanTHEOREM wz_ratio_equals_cos_theta · IndisputableMonolith/Physics/ElectroweakBosons.lean
/-- Predicted W/Z ratio = cos(θW). -/ theorem wz_ratio_equals_cos_theta : |wz_mass_ratio - cos_theta_W| < 0.005 := by -- wz_mass_ratio = 80.3692 / 91.1876 ≈ 0.88136 -- cos_theta_W = sqrt(1 - 0.23122) = sqrt(0.76878) ≈ 0.87683 -- |0.88136 - 0.87683| = 0.00453 < 0.005 simp only [wz_mass_ratio, wBosonMass_GeV, zBosonMass_GeV, cos_theta_W, sin2_theta_W] -- Need: |80.3692/91.1876 - sqrt(0.76878)| < 0.005 -- Bounds on ratio: 0.8813 < ratio < 0.8814 have h_ratio_lo : (80.3692 : ℝ) / 91.1876 > 0.8813 := by norm_num have h_ratio_hi : (80.3692 : ℝ) / 91.1876 < 0.8814 := by norm_num -- Bounds on sqrt: 0.8768 < sqrt(0.76878) < 0.8769 -- 0.8768^2 = 0.76877824, 0.8769^2 = 0.76895361 have h_sqrt_lo : sqrt 0.76878 > 0.8768 := by have h_sq : (0.8768 : ℝ)^2 < 0.76878 := by norm_num exact (Real.lt_sqrt (by norm_num : (0 : ℝ) ≤ 0.8768)).mpr h_sq have h_sqrt_hi : sqrt 0.76878 < 0.8769 := by have h_sq : 0.76878 < (0.8769 : ℝ)^2 := by norm_num have h_pos : (0 : ℝ) ≤ 0.76878 := by norm_num have h := Real.sqrt_lt_sqrt h_pos h_sq simp only [Real.sqrt_sq (by norm_num : (0 : ℝ) ≤ 0.8769)] at h exact h -- Difference: (0.8813, 0.8814) - (0.8768, 0.8769) = (0.0044, 0.0046) rw [abs_lt] constructor <;> linarithThe theory predicts that m<sub>Z</sub> = m<sub>W</sub> / cos(θ<sub>W</sub>), and the measured masses obey this relation. wz_ratio_equals_cos_theta · IndisputableMonolith/Physics/ElectroweakBosons.leanMEASURED sin2_theta_W · IndisputableMonolith/Physics/ElectroweakBosons.lean
/-- Weak mixing angle sin²θW (on-shell scheme). -/ def sin2_theta_W : ℝ := 0.23122The sine squared of this angle, sin²θ<sub>W</sub>, is measured to be about 0.231. sin2_theta_W · IndisputableMonolith/Physics/ElectroweakBosons.leanMEASURED vev_GeV · IndisputableMonolith/Physics/ElectroweakBosons.lean
/-- Higgs VEV in GeV. -/ def vev_GeV : ℝ := 246.22The Higgs field's vacuum expectation value, the constant background value it takes everywhere, is about 246 GeV, which sets the overall scale for the W and Z masses. vev_GeV · IndisputableMonolith/Physics/ElectroweakBosons.leanTHEOREM higgs_w_near_phi · IndisputableMonolith/Physics/ElectroweakBosons.lean
/-- Higgs to W ratio ≈ 1.56 ≈ φ. -/ theorem higgs_w_near_phi : |higgs_w_ratio - phi| < 0.1 := by -- 125.25 / 80.3692 ≈ 1.5585, φ ∈ (1.61, 1.62) -- |1.5585 - 1.618| ≈ 0.06 < 0.1 simp only [higgs_w_ratio, higgsMass_GeV, wBosonMass_GeV] have hphi_lo : phi > 1.61 := phi_gt_onePointSixOne have hphi_hi : phi < 1.62 := phi_lt_onePointSixTwo have h1 : (125.25 : ℝ) / 80.3692 > 1.55 := by norm_num have h2 : (125.25 : ℝ) / 80.3692 < 1.56 := by norm_num rw [abs_lt] constructor <;> linarithIt also proves that the ratio of the Higgs boson mass to the W mass is within 0.1 of the golden ratio φ itself, a numerical coincidence the framework highlights. higgs_w_near_phi · IndisputableMonolith/Physics/ElectroweakBosons.lean