TauLib · API Book I

TauLib.BookI.CF.WindowAlgebra

TauLib.CF.WindowAlgebra

Window algebra on the continued fraction head of ι_τ = 2/(π+e).

Registry Cross-References

  • [CF.01] CF Head — cf_head

  • [CF.05] 17 = a₃+a₄+a₅ — w3_at_3

  • [CF.06] 5/7 symmetric recipe — symmetric_recipe

  • [CF.09] Window Algebra — windowSum, key identities

Mathematical Content

The continued fraction CF[ι_τ] = [0; 2, 1, 13, 3, 1, 1, 1, 42, …] encodes electroweak physics through width-3 sliding window sums W₃(j) = a_j + a_{j+1} + a_{j+2}.

Key values:

  • W₃(3) = 13+3+1 = 17 (g_A NLO denominator: 8/17)

  • W₃(4) = 3+1+1 = 5 (sin²θ_W NLO numerator)

  • W₃(5) = 1+1+1 = 3 (= solenoidal triple )

The symmetric 5/7 identity: 5/7 = W₃(4) / (W₃(3) − 2·W₃(4)) Both numerator and denominator use the same W₃ family.

The 17/5 quotient: M_W/m_n = (17/5)·ι⁻³ = W₃(3)/W₃(4) · ι⁻³

Width 3 = |{π, γ, η}| = cardinality of solenoidal triple = number of generators winding through the fiber T².


Tau.CF.cf_head

source def Tau.CF.cf_head :List Nat

The first 14 partial quotients of CF[ι_τ] = CF[2/(π+e)]. Index 0 = floor part (0), indices 1..13 = partial quotients a₁..a₁₃. Sufficient for all known physics encodings. Equations

  • Tau.CF.cf_head = [0, 2, 1, 13, 3, 1, 1, 1, 42, 1, 2, 1, 5, 5] Instances For

Tau.CF.cf_head_length

source theorem Tau.CF.cf_head_length :cf_head.length = 14


Tau.CF.windowSum

source **def Tau.CF.windowSum (cf : List Nat)

(width start : Nat) :Nat**

Window sum W_k(j): sum of width consecutive CF terms starting at position start. Returns 0 if any index is out of bounds. Equations

  • Tau.CF.windowSum cf width start = List.foldl (fun (acc i : Nat) => acc + cf.getD (start + i) 0) 0 (List.range width) Instances For

Tau.CF.w3_at_3

source theorem Tau.CF.w3_at_3 :windowSum cf_head 3 3 = 17

[CF.05] W₃(3) = a₃ + a₄ + a₅ = 13 + 3 + 1 = 17. The g_A NLO denominator: δ_A = (8/17)·ι².


Tau.CF.w3_at_4

source theorem Tau.CF.w3_at_4 :windowSum cf_head 3 4 = 5

[CF.06] W₃(4) = a₄ + a₅ + a₆ = 3 + 1 + 1 = 5. The sin²θ_W NLO numerator.


Tau.CF.w3_at_5

source theorem Tau.CF.w3_at_5 :windowSum cf_head 3 5 = 3

W₃(5) = a₅ + a₆ + a₇ = 1 + 1 + 1 = 3. Equals the cardinality of the solenoidal triple {π, γ, η}.


Tau.CF.w3_at_1

source theorem Tau.CF.w3_at_1 :windowSum cf_head 3 1 = 16

W₃(1) = a₁ + a₂ + a₃ = 2 + 1 + 13 = 16.


Tau.CF.w3_at_2

source theorem Tau.CF.w3_at_2 :windowSum cf_head 3 2 = 17

W₃(2) = a₂ + a₃ + a₄ = 1 + 13 + 3 = 17.


Tau.CF.symmetric_recipe

source theorem Tau.CF.symmetric_recipe :have w34 := windowSum cf_head 3 4; have denom := windowSum cf_head 3 3 - 2 * windowSum cf_head 3 4; w34 = 5 ∧ denom = 7

[CF.06] The symmetric recipe for 5/7: numerator = W₃(4) = 5, denominator = W₃(3) − 2·W₃(4) = 17 − 10 = 7. Both sides use the same W₃ window family.


Tau.CF.symmetric_product

source theorem Tau.CF.symmetric_product :windowSum cf_head 3 4 * (windowSum cf_head 3 3 - 2 * windowSum cf_head 3 4) = 35

The product 5 × 7 = 35 from the symmetric recipe.


Tau.CF.mw_window_quotient

source theorem Tau.CF.mw_window_quotient :windowSum cf_head 3 3 = 17 ∧ windowSum cf_head 3 4 = 5

[CF.06] The 17/5 quotient: W₃(3)/W₃(4) = 17/5. This is the coefficient in M_W/m_n = (17/5)·ι⁻³.


Tau.CF.window_width_is_solenoidal

source theorem Tau.CF.window_width_is_solenoidal :3 = Kernel.solenoidalGenerators.length

The window width 3 equals the number of solenoidal generators. This is the structural reason WHY width-3 windows encode physics: each W₃ window sum “reads out” one complete fiber period through the three generators {π, γ, η} winding through T².


Tau.CF.w3_at_5_eq_solenoidal

source theorem Tau.CF.w3_at_5_eq_solenoidal :windowSum cf_head 3 5 = Kernel.solenoidalGenerators.length

W₃(5) = 3 = solenoidal : the third window echoes the width itself.

Tau.CF.a3_eq

source theorem Tau.CF.a3_eq :cf_head.getD 3 0 = 13

a₃ = 13 (the CF hub, anomalously large).


Tau.CF.a4_eq

source theorem Tau.CF.a4_eq :cf_head.getD 4 0 = 3

a₄ = 3 = dim(τ³) = window width.


Tau.CF.a8_eq

source theorem Tau.CF.a8_eq :cf_head.getD 8 0 = 42

a₈ = 42 (the “dark number”, highest information content).


Tau.CF.EWCrossWeb

source structure Tau.CF.EWCrossWeb :Type

The electroweak cross-web: all three EW observables (g_A, sin²θ_W, M_W/m_n) are determined by two adjacent W₃ windows at positions 3 and 4.

  • g_A NLO: 8/W₃(3) = 8/17

  • sin²θ_W NLO: W₃(4)/(W₃(3)−2·W₃(4)) = 5/7

  • M_W/m_n: W₃(3)/W₃(4) = 17/5 This structure packages 3 from the 17 that is expressible as a sum of sums from two overlapping W₃ windows.

  • w3_3 : Nat
  • w3_4 : Nat
  • hw3 : self.w3_3 = windowSum cf_head 3 3
  • hw4 : self.w3_4 = windowSum cf_head 3 4 Instances For

Tau.CF.ewCrossWeb

source def Tau.CF.ewCrossWeb :EWCrossWeb

The canonical EW cross-web instance. Equations

  • Tau.CF.ewCrossWeb = { w3_3 := 17, w3_4 := 5, hw3 := Tau.CF.ewCrossWeb._proof_1, hw4 := Tau.CF.ewCrossWeb._proof_2 } Instances For