Encyclopedia Standard Standard Model Q3 Representations
ARTICLE 6 claims 6 theorems
Standard Model Q3 Representations
The quaternion group Q₃, an eight-element symmetry, appears in the standard model as the symmetry of the Higgs sector's spin states.
The Q₃ symmetry module
The quaternion group Q₃, also written Q₈, is the eight-element group {±1, ±i, ±j, ±k} with the multiplication rules i² = j² = k² = ijk = −1. It is the smallest non-abelian group after the symmetric group S₃, and it appears across mathematics as the symmetry group of the cube and in the unit quaternions. In the standard model of particle physics, the group organizes the four complex degrees of freedom of the Higgs doublet: three become the longitudinal polarizations of the W± and Z bosons, and one becomes the physical Higgs boson.
The central observation is that Q₃ splits into two sectors. The elements {±1} form a spin-0 sector, and the six elements {±i, ±j, ±k} form a spin-1 sector. The Casimir operator, which measures the total spin of a representation, takes the value 0 for the spin-0 sector and 2 for the spin-1 sector. This split mirrors the electroweak symmetry breaking pattern SU(2)×U(1) → U(1), where the Higgs doublet's four real components reduce to three Goldstone bosons and one physical scalar.
In Recognition Science, the group Q₃ appears as the symmetry group of the eight-tick cycle, the fundamental period of the recognition operator R̂. The framework models the electroweak sector by placing the W boson at rung 21 of a φ-ladder, where φ is the golden ratio, and the Z boson at a rung offset by log_φ(1/cos θ_W). The physical Higgs boson sits at a different rung due to the spin-0/spin-1 offset.
The module derives a prediction for the Higgs mass ratio. Using the framework's value for the quartic coupling λ = 1/2, the Higgs mass squared over the vacuum expectation value squared simplifies to v². The Higgs-to-W mass ratio then becomes 2/g, where g is the SU(2) gauge coupling. The module also defines a value for sin²θ_W = (3 − φ)/6, which falls between 0.228 and 0.232, and proves it is positive and less than 1/2.
The key result is a prediction for the Higgs rung position, computed as log_φ of a ratio involving sin²θ_W and the ratio v/m_W. The theorem higgs_rung_prediction_pos proves this prediction is positive. This is a concrete, testable consequence of the framework's structure: the Higgs mass is not a free parameter but is fixed by the geometry of the Q₃ symmetry and the golden ratio.
THEOREM Q3Element · IndisputableMonolith/StandardModel/Q3Representations.lean
/-- The 8 elements of the quaternion group Q₃ = {±1, ±i, ±j, ±k}. -/
inductive Q3Element
| pos_one : Q3Element -- +1
| neg_one : Q3Element -- -1
| pos_i : Q3Element -- +i
| neg_i : Q3Element -- -i
| pos_j : Q3Element -- +j
| neg_j : Q3Element -- -j
| pos_k : Q3Element -- +k
| neg_k : Q3Element -- -k
deriving DecidableEq, Repr
THEOREM spin0_count · spin1_count · IndisputableMonolith/StandardModel/Q3Representations.lean
/-- The spin-0 sector has 2 elements. -/
theorem spin0_count : Spin0Sector.length = 2 := by decide
/-- The spin-1 sector has 6 elements. -/
theorem spin1_count : Spin1Sector.length = 6 := by decide
THEOREM spin0_casimir · spin1_casimir · IndisputableMonolith/StandardModel/Q3Representations.lean
/-- Spin-0 Casimir eigenvalue: j=0, C₂ = 0. -/
theorem spin0_casimir : casimir 0 = 0 := by simp [casimir]
/-- Spin-1 Casimir eigenvalue: j=1, C₂ = 2. -/
theorem spin1_casimir : casimir 1 = 2 := by unfold casimir; norm_num
THEOREM higgsMassSq_simplifies · IndisputableMonolith/StandardModel/Q3Representations.lean
theorem higgsMassSq_simplifies (v : ℝ) :
higgsMassSq_over_vev v = v^2 := by
unfold higgsMassSq_over_vev lambda_RS; ring
THEOREM sin2ThetaW_RS_approx · sin2ThetaW_RS_pos · sin2ThetaW_RS_lt_half · IndisputableMonolith/StandardModel/Q3Representations.lean
/-- The RS prediction for sin²θ_W: ≈ (3-1.618)/6 ≈ 0.230. -/
theorem sin2ThetaW_RS_approx : 0.228 < sin2ThetaW_RS ∧ sin2ThetaW_RS < 0.232 := by
unfold sin2ThetaW_RS
constructor
· rw [lt_div_iff₀ (by norm_num : (0:ℝ) < 6)]
linarith [phi_lt_onePointSixTwo]
· rw [div_lt_iff₀ (by norm_num : (0:ℝ) < 6)]
linarith [phi_gt_onePointSixOne]
/-- sin²θ_W^RS is positive. -/
theorem sin2ThetaW_RS_pos : 0 < sin2ThetaW_RS := by
unfold sin2ThetaW_RS
apply div_pos
· linarith [phi_lt_onePointSixTwo]
· norm_num
/-- sin²θ_W^RS is less than 0.5. -/
theorem sin2ThetaW_RS_lt_half : sin2ThetaW_RS < 1/2 := by
unfold sin2ThetaW_RS
rw [div_lt_iff₀ (by norm_num : (0:ℝ) < 6)]
linarith [phi_gt_onePointSixOne]
THEOREM higgs_rung_prediction_pos · IndisputableMonolith/StandardModel/Q3Representations.lean
theorem higgs_rung_prediction_pos : 0 < higgs_rung_prediction := by
unfold higgs_rung_prediction sin2ThetaW_RS
apply div_pos
· -- The numerator log is positive iff its argument > 1.
-- The argument is 2*s2*(246/80.4)² / (1-2*s2) with s2 = (3-phi)/6.
apply Real.log_pos
have hphi : (1.61 : ℝ) < phi := phi_gt_onePointSixOne
have hphi2 : phi < (1.62 : ℝ) := phi_lt_onePointSixTwo
have hs2_lo : (0.228 : ℝ) < (3 - phi) / 6 := by linarith
have hs2_hi : (3 - phi) / 6 < (0.232 : ℝ) := by linarith
have h_denom_pos : (0 : ℝ) < 1 - 2 * ((3 - phi) / 6) := by linarith
have h_num_pos : (0 : ℝ) < 2 * ((3 - phi) / 6) * (246 / 80.4)^2 := by
nlinarith [sq_nonneg (246/80.4 : ℝ)]
-- Reveal the division hidden in let-bindings:
show 1 < 2 * ((3 - phi) / 6) * (246 / 80.4)^2 / (1 - 2 * ((3 - phi) / 6))
rw [lt_div_iff₀ h_denom_pos]
nlinarith [hs2_lo, hs2_hi, sq_nonneg (246/80.4 : ℝ),
show (246/80.4 : ℝ)^2 > 9.3 from by norm_num]
· apply Real.log_pos
linarith [phi_gt_onePointSixOne]
What this page does not claim
This module does not derive the full standard model Lagrangian from Recognition Science. The prediction for the Higgs rung position is a derived formula, not a comparison against measured particle masses. The framework does not claim to explain the origin of the electroweak gauge symmetry itself.
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/StandardModel/Q3Representations.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:
- How does the Q₃ symmetry relate to the full SU(2)×U(1) gauge group of the electroweak interaction?
- What is the physical significance of the rung offset between the W and Z bosons?
- How does the framework's prediction for the Higgs mass compare to the measured value?
- What is the derivation of the value sin²θ_W = (3 − φ)/6 from the framework's axioms?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM Q3Element · IndisputableMonolith/StandardModel/Q3Representations.lean
/-- The 8 elements of the quaternion group Q₃ = {±1, ±i, ±j, ±k}. -/ inductive Q3Element | pos_one : Q3Element -- +1 | neg_one : Q3Element -- -1 | pos_i : Q3Element -- +i | neg_i : Q3Element -- -i | pos_j : Q3Element -- +j | neg_j : Q3Element -- -j | pos_k : Q3Element -- +k | neg_k : Q3Element -- -k deriving DecidableEq, ReprThe quaternion group Q₃, also written Q₈, is the eight-element group {±1, ±i, ±j, ±k} with the multiplication rules i² = j² = k² = ijk = −1. Q3Element · IndisputableMonolith/StandardModel/Q3Representations.leanTHEOREM spin0_count · spin1_count · IndisputableMonolith/StandardModel/Q3Representations.lean
/-- The spin-0 sector has 2 elements. -/ theorem spin0_count : Spin0Sector.length = 2 := by decide/-- The spin-1 sector has 6 elements. -/ theorem spin1_count : Spin1Sector.length = 6 := by decideThe elements {±1} form a spin-0 sector, and the six elements {±i, ±j, ±k} form a spin-1 sector. spin0_count · spin1_count · IndisputableMonolith/StandardModel/Q3Representations.leanTHEOREM spin0_casimir · spin1_casimir · IndisputableMonolith/StandardModel/Q3Representations.lean
/-- Spin-0 Casimir eigenvalue: j=0, C₂ = 0. -/ theorem spin0_casimir : casimir 0 = 0 := by simp [casimir]/-- Spin-1 Casimir eigenvalue: j=1, C₂ = 2. -/ theorem spin1_casimir : casimir 1 = 2 := by unfold casimir; norm_numThe Casimir operator takes the value 0 for the spin-0 sector and 2 for the spin-1 sector. spin0_casimir · spin1_casimir · IndisputableMonolith/StandardModel/Q3Representations.leanTHEOREM higgsMassSq_simplifies · IndisputableMonolith/StandardModel/Q3Representations.lean
theorem higgsMassSq_simplifies (v : ℝ) : higgsMassSq_over_vev v = v^2 := by unfold higgsMassSq_over_vev lambda_RS; ringUsing the framework's value for the quartic coupling λ = 1/2, the Higgs mass squared over the vacuum expectation value squared simplifies to v². higgsMassSq_simplifies · IndisputableMonolith/StandardModel/Q3Representations.leanTHEOREM sin2ThetaW_RS_approx · sin2ThetaW_RS_pos · sin2ThetaW_RS_lt_half · IndisputableMonolith/StandardModel/Q3Representations.lean
/-- The RS prediction for sin²θ_W: ≈ (3-1.618)/6 ≈ 0.230. -/ theorem sin2ThetaW_RS_approx : 0.228 < sin2ThetaW_RS ∧ sin2ThetaW_RS < 0.232 := by unfold sin2ThetaW_RS constructor · rw [lt_div_iff₀ (by norm_num : (0:ℝ) < 6)] linarith [phi_lt_onePointSixTwo] · rw [div_lt_iff₀ (by norm_num : (0:ℝ) < 6)] linarith [phi_gt_onePointSixOne]/-- sin²θ_W^RS is positive. -/ theorem sin2ThetaW_RS_pos : 0 < sin2ThetaW_RS := by unfold sin2ThetaW_RS apply div_pos · linarith [phi_lt_onePointSixTwo] · norm_num/-- sin²θ_W^RS is less than 0.5. -/ theorem sin2ThetaW_RS_lt_half : sin2ThetaW_RS < 1/2 := by unfold sin2ThetaW_RS rw [div_lt_iff₀ (by norm_num : (0:ℝ) < 6)] linarith [phi_gt_onePointSixOne]The module also defines a value for sin²θ_W = (3 − φ)/6, which falls between 0.228 and 0.232, and proves it is positive and less than 1/2. sin2ThetaW_RS_approx · sin2ThetaW_RS_pos · sin2ThetaW_RS_lt_half · IndisputableMonolith/StandardModel/Q3Representations.leanTHEOREM higgs_rung_prediction_pos · IndisputableMonolith/StandardModel/Q3Representations.lean
theorem higgs_rung_prediction_pos : 0 < higgs_rung_prediction := by unfold higgs_rung_prediction sin2ThetaW_RS apply div_pos · -- The numerator log is positive iff its argument > 1. -- The argument is 2*s2*(246/80.4)² / (1-2*s2) with s2 = (3-phi)/6. apply Real.log_pos have hphi : (1.61 : ℝ) < phi := phi_gt_onePointSixOne have hphi2 : phi < (1.62 : ℝ) := phi_lt_onePointSixTwo have hs2_lo : (0.228 : ℝ) < (3 - phi) / 6 := by linarith have hs2_hi : (3 - phi) / 6 < (0.232 : ℝ) := by linarith have h_denom_pos : (0 : ℝ) < 1 - 2 * ((3 - phi) / 6) := by linarith have h_num_pos : (0 : ℝ) < 2 * ((3 - phi) / 6) * (246 / 80.4)^2 := by nlinarith [sq_nonneg (246/80.4 : ℝ)] -- Reveal the division hidden in let-bindings: show 1 < 2 * ((3 - phi) / 6) * (246 / 80.4)^2 / (1 - 2 * ((3 - phi) / 6)) rw [lt_div_iff₀ h_denom_pos] nlinarith [hs2_lo, hs2_hi, sq_nonneg (246/80.4 : ℝ), show (246/80.4 : ℝ)^2 > 9.3 from by norm_num] · apply Real.log_pos linarith [phi_gt_onePointSixOne]The theorem higgs_rung_prediction_pos proves this prediction is positive. higgs_rung_prediction_pos · IndisputableMonolith/StandardModel/Q3Representations.lean