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Document 2 of the TFPT 5.4 setCompiler core
TFPT 5.42026-07-231.16 MBSHA-256 40d1142aa301
Paper 2Compiler core

The Standard Model from the Compiler

The φ₀-ladder, flavor from parabolic transport, and the worked closures

The fermion spectrum — masses, Yukawa structure, CKM, the PMNS skeleton and neutrinos — follows from one master formula with one seed φ₀, the carrier base λ_Y = √(φ₀(1−φ₀)), and the residue matrix of the compiler. Plus the flavor block from parabolic transport on ℙ¹∖μ₄, the five worked closures (θ₁₂, quark c, the explicit mass gap, Starobinsky M, the H2 splitting), and gravity/QG as the seam response.

Inputs
  • The two axioms and the E₈ compiler of Document 1.
  • The seed φ₀ = 1/(6π) + 3/(256π⁴) and the carrier base λ_Y = √(φ₀(1−φ₀)).
Contribution
  • One master mass formula for all nine masses, Yukawa, CKM, PMNS and neutrinos, with the word-lengths read off the compiler residue matrix.
  • The residue matrix R with det R = 8 = h(D₅), principal 2-minors (2,3,5), and χ_R = t³ − 9t² + 10t − 8.
  • The solar angle sin²θ₁₂ = 1/3 − φ₀/2 = 0.3067 from the seam misalignment ε = q(A₃)φ₀.
Not claimed here
  • Charged-lepton masses and quark mass ratios are closed; the absolute quark amplitude scale reduces to one overall scale v_geo (Grand Mass Volume + ratios) — the same dimensionful anchor as gravity's 1/G.
  • Dimensionful m_W, m_Z, m_H, sin²θ_W, α_s are RG scheme-layer projections, not compiler outputs.
Falsification surface
  • Fails if the residue invariants (det 8, minors 2,3,5, χ_R) are not respected by a future global CKM/PMNS fit, or if the lepton φ₀-ladder mismatches the observed hierarchy.
Highlights
Masses1 formulaAll nine masses + mixings from one φ₀-ladder
det R8 = h(D₅)Flavor matrix determinant is a compiler number
sin²θ₁₂0.30671/3 − φ₀/2; 0.1% from NuFIT 6.0
Quark ratios55/117, 34/47, 3/26Integer Plücker readouts on the selector stratum
Anchor plane(3x+2)(3x+5)det B(K+xQ): 2/3 (Koide/gap) & 5/3 (D₅/A₃) are its singular points [I/L]
Double coverKoide = branch pty² = det B(K+xQ): Koide −2/3 & carrier −5/3 are the two branch points (deck 2 = |ℤ₂|, disc = N_fam⁴) [I/L]

Key formulas

  • Master mass formula
    m^f,j=vgeo2λYLf,jΛf,j\hat m_{f,j} = \frac{v_{\mathrm{geo}}}{\sqrt2}\,\lambda_Y^{\,L_{f,j}}\,\Lambda_{f,j}
    One seed φ₀, one carrier base, the compiler residue matrix.
  • Flavor invariants
    detR=8,minors=(2,3,5),χR=t39t2+10t8\det R = 8,\quad \mathrm{minors}=(2,3,5),\quad \chi_R = t^3 - 9t^2 + 10t - 8
    Exact compiler signature any future fit must satisfy. [E]
  • Solar angle
    sin2θ12=13φ02=0.3067\sin^2\theta_{12} = \tfrac{1}{3} - \tfrac{\varphi_0}{2} = 0.3067
    Previously open; now conditionally derived (seam ε = (3/4)φ₀). [N/P]
  • Lepton product
    cecμcτ=2gcarNfam2=329c_e c_\mu c_\tau = \frac{2^{g_{\mathrm{car}}}}{N_{\mathrm{fam}}^2} = \frac{32}{9}
    Charged-lepton amplitudes closed in φ₀.

One master formula instead of many Yukawas

Every fermion mass is the same ladder: the geometric VEV times the carrier base raised to a compiler word-length, times an O(1) residue. The word-lengths are the fixed residue matrix of the compiler — not free parameters.

m^f,j=vgeo2λYLf,jΛf,j,λY=φ0(1φ0)\hat m_{f,j} = \frac{v_{\mathrm{geo}}}{\sqrt2}\,\lambda_Y^{\,L_{f,j}}\,\Lambda_{f,j}, \qquad \lambda_Y = \sqrt{\varphi_0(1-\varphi_0)}
φ0=16π+3256π4=0.05317\varphi_0 = \frac{1}{6\pi} + \frac{3}{256\pi^4} = 0.05317\ldots

The flavor residue matrix is the compiler signature

The word-length matrix L = R + 6·(winding) carries only compiler numbers: its trace is N_fam², its determinant is h(D₅) = 8, its principal 2-minors are (2,3,5) with product 30 = h(E₈), and its Frobenius norm is dim E₆ = 78.

R=(130152253),detR=8,RF2=78R = \begin{pmatrix} 1 & 3 & 0 \\ 1 & 5 & 2 \\ 2 & 5 & 3 \end{pmatrix}, \qquad \det R = 8, \quad \|R\|_F^2 = 78
χR(t)=t39Nfam2t2+10(52)t8h(D5)\chi_R(t) = t^3 - \underbrace{9}_{N_{\mathrm{fam}}^2}t^2 + \underbrace{10}_{\binom{5}{2}}t - \underbrace{8}_{h(D_5)}

Charged leptons: completely closed in φ₀

The lepton amplitudes are the rationals (16/7, 4/3, 7/6) with product 2⁵/N_fam² = 32/9, and the masses are exact φ₀-powers. Applied to the down sector the lepton law provably fails — the quark c's live on the parabolic wall.

(m^e,m^μ,m^τ)=vgeoπ2(167(φ0)5, 43(φ0)3, 76(φ0)2)(\hat m_e, \hat m_\mu, \hat m_\tau) = \frac{v_{\mathrm{geo}}\pi}{\sqrt2}\Big(\tfrac{16}{7}(\varphi_0)^5,\ \tfrac{4}{3}(\varphi_0)^3,\ \tfrac{7}{6}(\varphi_0)^2\Big)
cecμcτ=2gcarNfam2=329c_e\,c_\mu\,c_\tau = \frac{2^{g_{\mathrm{car}}}}{N_{\mathrm{fam}}^2} = \frac{32}{9}

Quark ratios from the same word-lengths

The quark mass ratios are pure integer Plücker readouts on the derived selector stratum — no transcendental solve. The absolute amplitude reduces to one overall scale v_geo (ratios + Grand Mass Volume), the same dimensionful anchor as gravity's 1/G. The remaining ℤ₃ deck choice is since derived: the integer deck pairs the Q₊=1 line with the self-conjugate character 2, so the geometric boundary deck is the sheet-twisted class and the cusp exponential is excluded (v141) — GATE.QGEO keeps only its realisation premise, with no discrete freedom left — and that premise sits at its floor: the full Möbius D₄ of the seam curve matches the integer model parity by parity (ι = T_A exactly, δι = Σ; v146). The finite rigidity is now proven exactly [E]: μ₄ has cross-ratio 2 and a faithful Möbius D₄ stabiliser, H¹(ℙ¹∖μ₄) has rank N_fam = 3, and the eigenforms ω_k carry the μ₄ characters of weights (1,2,3) = the A₃ exponents = Spec(Q₊) — so only the seam-collar realisation stays open (v168). The Sheet Diamond carrying these operators is a discrete geometry with two axes (v218): the determinant is linear along the winding axis (A₃-driven, slope 6 = |R⁺(A₃)|) and quadratic along the sheet axis with curvatures (8, 6) = (rank E₈, |R⁺(A₃)|); the anchor-Plücker coordinates lift K→C→F in two exact steps (1,8,10) then (1,8,16) — the decuple A_Λ then the full spinor generation dim S⁺; and the characteristic-polynomial discriminants of Q,K,C,F factor as q(r)²·Disc(q) with squares (1,3,4,6) = (N_Φ,N_fam,|μ₄|,|R⁺(A₃)|) and kernels (13,48,65,105). No new numbers — it organises the existing operators more strictly. Sharper still (v410): the sheet axis V = Q·diag(0,1,1) is a binary internal compiler — its powers print the carrier spine Vⁿ·1 = (2ⁿ⁻¹, 2ⁿ, 2ⁿ⁺¹−1) = (1,2,3),(2,4,7),(4,8,15),(8,16,31), and four exact bilinear families collapse the recurring integers (6,7,9,11; 13 = Δ_Q, 27 = 1ᵀRa, 55, 56 = dim 56_E₇) into one operator's iteration. The quark ratio is then a pure V-power readout c_u/c_d = (1ᵀV⁴1)/((aᵀV1)(1ᵀV²1)) = 55/117 (v411, an exact re-encoding); the unnamed Z₂-wall corner J = M(1,−2) carries χ_J = (6,3,2), aᵀJa = 30 = h(E₈), det(I+J) = 12, det(2I+J) = 40 (v412); the sheet axis encodes the atoms as difference orders Δe₁ = 3, Δ²e₂ = 4, Δ²e₃ = 8 with anchor energy 52+11t (v413); and the center C is a resolvent portal det C = 14 = dim G₂, det(I+C) = 52 = dim F₄, det(2I+C) = 120 = |R⁺(E₈)| (v414). All [E] algebra; the binary spine is forced by Spec(V) = {0,1,2}, so the Lie-dimension readings stay [C], audit-typed.

cucd=gcar11Nfam2ΔQ=55117,cccs=3447,ctcb=326\frac{c_u}{c_d} = \frac{g_{\mathrm{car}}\cdot 11}{N_{\mathrm{fam}}^2\,\Delta_Q} = \frac{55}{117}, \quad \frac{c_c}{c_s} = \frac{34}{47}, \quad \frac{c_t}{c_b} = \frac{3}{26}
m^t/m^b=326(φ0)2=40.81\hat m_t/\hat m_b = \tfrac{3}{26}(\varphi_0)^{-2} = 40.81

The absolute neutrino scale: one parameter under the carrier normalisation

The absolute ν-mass scale is one seesaw ratio m₃ = (y_ν v)²/(2M_R) — honestly typed as one open UV input (v272), with the NO floor Σm_ν = 0.0586 eV as the cosmological kill test. New (v481, FLAV.NUSCALE.02, CANDIDATE class like v467/v468): the y_ν = 1 probe was not the carrier normalisation — one SO(10) 16 per family with the minimal Yukawa sector (10_H / PS (1,2,2)) forces y_ν = y_t at the matching scale, collapsing the (y_ν, M_R) trade-off to M_R alone. With explicit 1-loop RG (gauge/y_t/λ up, ADKLR Weinberg-operator running down) the observed m₃ = 0.0503 eV demands M_R = 9.3×10¹³ GeV — inside the compiler's own PS window [4.2×10¹³, 2.4×10¹⁵] GeV (v249) at log_c₃(M̄/M_R) = 3.15 (y_ν = 1 gives the structureless 2.58). Honesty gate: the integer rung M_R = c₃³M̄ predicts m₃ = 0.030 eV, 40% low at 1-loop, so the ladder pin is DECLINED per the anti-numerology rule — and the named decision computation is meanwhile EXECUTED in bracketed form (v482, FLAV.NUSCALE.03): the rung needs a rescue factor ×1.670 while >3σ-generous input envelopes (m_t ±3 GeV, α_s, κ-run ±10%, PS-leg β ×[0.5,1.5]) reach at most ×1.165 combined, so the unstructured rung is EXCLUDED (not an RG artifact); the only escape, a third-generation Majorana structure factor r ≈ 1.67 sitting 0.18% from g_car/N_fam = 5/3, is recorded post-hoc and declined (no forcing mechanism). That escape is now DECIDED dead (v488, FLAV.NUSCALE.04): since the 126bar is not in the E₈ hull (v247), M_R can only come from the d=5 operator (16·16bar_H)²/Λ with singlet/45 insertion channels; every ν^c channel weight {1, 1/4, 1, −1/2, 3/8} is a {2,3}-smooth rational, so no channel combination can produce 5/3 — and the unique natural 5 of the embedding, k_Y = 5/3 (Ginsparg), is a full-multiplet trace whose direction has Y(ν^c) = 0 exactly, structurally decoupled from the Majorana operator; Clebsches are generation-blind (family-space scalars), so diag(1,1,3/5) cannot arise from group theory at all. A clean negative: the rung+5/3 rescue is a numerical coincidence without mechanism, and the one-parameter window candidate stands as the honest endpoint. The candidate band m₃ ∈ [0.002, 0.115] eV brackets the observation and DESI cuts the window from below; nothing closes and the frozen record is untouched.

yν=yt  (161610)    MR=9.3×1013GeV[MPS,MGUT]y_\nu = y_t \;(\mathbf{16}\cdot\mathbf{16}\cdot\mathbf{10}) \;\Rightarrow\; M_R = 9.3\times10^{13}\,\mathrm{GeV} \in [M_{\mathrm{PS}}, M_{\mathrm{GUT}}]
logc3(MˉPl/MR)=3.15  (integer rung c33MˉPl declined at 1-loop)\log_{c_3}(\bar M_{\mathrm{Pl}}/M_R) = 3.15 \;(\text{integer rung } c_3^3\bar M_{\mathrm{Pl}} \text{ declined at 1-loop})

The solar angle θ₁₂ from the seam

Tri-bimaximal gives 1/3; the charged-lepton 1–2 misalignment is the seam ε = q(A₃)φ₀ = (3/4)φ₀, and TBM geometry gives the only previously open SM angle as a conditional derivation — 0.1% from NuFIT 6.0.

ε=q(A3)φ0=34φ0=c3+36c34,q(A3)=Nfamμ4\varepsilon = q(A_3)\,\varphi_0 = \tfrac{3}{4}\varphi_0 = c_3 + 36\,c_3^4, \qquad q(A_3) = \frac{N_{\mathrm{fam}}}{|\mu_4|}
sin2θ12seed=1323ε=13φ02=0.306747\sin^2\theta_{12}^{\mathrm{seed}} = \tfrac{1}{3} - \tfrac{2}{3}\varepsilon = \tfrac{1}{3} - \tfrac{\varphi_0}{2} = 0.306747

Branch kernels select the sectors (the sheet question, closed modulo one gate)

At the two branch points of the anchor-block double cover the block is rank 1, with integer kernels — at the carrier point the kernel is the democratic vector itself. Rank 1 forces the kernel image onto the antisymmetric direction (−1,1,0): up and down are the deck-odd pair, and the lepton pairing vanishes — the leptons sit on the ramification (Koide is leptonic). The anchor-forced cusp conjugation T_A (with a = e₂+e₃, the conjugation-symmetric vector) realises the same deck action, and the dictionary 'Q₊ grading = A₃ discriminant grading' is now derived (G = T_A·Σ acts integrally as the B₁⊕E decomposition on the cusp basis): the sheet question carries no separate [C] — its residual coincides with the one existing Q-geometry gate.

P(23)w=203(1,1,0),P(53)w=23(1,1,0)P(-\tfrac23)\,w = \tfrac{20}{3}(1,-1,0), \qquad P(-\tfrac53)\,w = \tfrac{2}{3}(-1,1,0)
TA=(010100221),a=e2+e3,detTA=1T_A = \begin{pmatrix} 0 & 1 & 0 \\ 1 & 0 & 0 \\ 2 & -2 & 1 \end{pmatrix}, \qquad a = e_2 + e_3, \qquad \det T_A = -1

Key formulas at a glance

  • Master mass formula
    m^f,j=vgeo2λYLf,jΛf,j\hat m_{f,j} = \frac{v_{\mathrm{geo}}}{\sqrt2}\,\lambda_Y^{\,L_{f,j}}\,\Lambda_{f,j}

    One seed φ₀, one carrier base, the compiler residue matrix.

  • Flavor invariants
    detR=8,minors=(2,3,5),χR=t39t2+10t8\det R = 8,\quad \mathrm{minors}=(2,3,5),\quad \chi_R = t^3 - 9t^2 + 10t - 8

    Exact compiler signature any future fit must satisfy. [E]

  • Solar angle
    sin2θ12=13φ02=0.3067\sin^2\theta_{12} = \tfrac{1}{3} - \tfrac{\varphi_0}{2} = 0.3067

    Previously open; now conditionally derived (seam ε = (3/4)φ₀). [N/P]

  • Lepton product
    cecμcτ=2gcarNfam2=329c_e c_\mu c_\tau = \frac{2^{g_{\mathrm{car}}}}{N_{\mathrm{fam}}^2} = \frac{32}{9}

    Charged-lepton amplitudes closed in φ₀.

Cite this document

A reproducible citation pack: the BibTeX entry plus the verifiable release facts. The PDF SHA-256 pins the exact bytes; the source and ledger are public.

BibTeX
@misc{tfpt_standard_model_2026,
  title        = {The Standard Model from the Compiler},
  author       = {Hamann, Stefan and Rizzo, Alessandro},
  year         = {2026},
  howpublished = {\url{https://www.fixpoint-theory.com/papers/standard-model}},
  url          = {https://www.fixpoint-theory.com/papers/tfpt_2_standard_model.pdf},
  note         = {TFPT 5.4, 2026-07-23, PDF SHA-256 40d1142a6cbac3e75f4326a7de4e03528cba2b8408bd12c7d189e3e87504a301}
}
Authors
Stefan Hamann, Alessandro Rizzo
Version
TFPT 5.4
Date
2026-07-23
Claim status
Compiler core
PDF SHA-256
40d1142a6cbac3e75f4326a7de4e03528cba2b8408bd12c7d189e3e87504a301