Particles = Lattice Modes
Every particle, coupling, mass hierarchy, and interaction in the Standard Model reduced to wave modes on a 3D discrete lattice. In Planck units (a = k = η = 1), the entire particle zoo follows from d = 3 and π.
§1 — The Standard Model ↔ Lattice Dictionary
Set lattice-Planck units: a = 1, k = 1, η = 1. Then c = 1, ℏ = π/2, G = 1/(4π). Every Standard Model concept maps to a lattice wave concept:
| Standard Model | Lattice Reality | Planck Formula |
|---|---|---|
| Electron | 1D transverse standing wave | me = 2dπd+2αNgauge mP |
| Up quark | Breather n=13, tunneling p=31 | mu = m(13, 31) |
| Down quark | Breather n=5, tunneling p=30 | md = m(5, 30) |
| Proton | j0 spherical standing wave | mp = 2d · πd+2 · me |
| Muon | 2nd-generation axial mode | mμ = [d/(2α) + √(d/2)] me |
| Tau | 3rd-generation axial mode | Koide: (Nc−1)/Nc = 2/d |
| Neutrinos | Extended low-k lattice ripples | Mν = med / (d · mp2) |
| Photon (γ) | Transverse lattice wave (massless) | m = 0, v = c = 1 |
| Gluons (8) | d2−1 = 8 internal bond vibrations | Ng = d2 − 1 |
| W±, Z0 | Massive lattice modes (broken symmetry) | MW = g2v/2 |
| Higgs boson | Amplitude mode of cosine potential | λ = π2g22/2d+2 |
| Color charge | SU(d) rotational symmetry of d bonds | Nc = d |
| Generations (3) | One per spatial axis | Ngen = d |
| Fine structure α | Wyler geometric coupling | d2/[2d+1(d+2)!1/(d+1)π(d2+d−1)/(d+1)] |
| Feynman vertex | Wave scattering at lattice node | Amplitude ∝ αn/2 |
§2 — SU(3) × SU(2) × U(1) from d = 3
The Standard Model gauge group is not an input — it is forced by the lattice geometry. Each factor comes from a different degree of freedom:
Total gauge bosons: (d2−1) + ((d−1)2−1) + 1 = 8 + 3 + 1 = 12
This is purely geometric — any 3D discrete medium with nearest-neighbor restoring forces must have this symmetry group. There is no other option.
Why d−1 for weak isospin?
Each lattice node has d spatial bonds and 2 polarization states. The 2 polarizations form an SU(2) doublet — the “yin-yang” of the medium. But 2 = d − 1 only when d = 3. This is another hint that d = 3 is special: it is the unique dimension where the weak group SU(2) is the “complement” of the color group SU(3).
§3 — The Mass Hierarchy in d and π
In lattice-Planck units, the Planck mass is mP = 1. Every other mass is a fraction of mP, suppressed by powers of α and geometric factors. The “hierarchy problem” dissolves: each power of α is a geometric tunneling step.
| Particle | Planck-Unit Mass | In d, π | Steps from mP |
|---|---|---|---|
| Planck mass | 1 | 1 | 0 steps |
| Higgs VEV v | m(d, d·2d−1) = m(3, 23) | √2 · mt (yt=1) | p = 23 |
| Top quark | m(12, 24) | n=d(d+1), p=d·2d | p = 24 |
| Higgs boson | m(8, 24) | n=2d, p=d·2d | p = 24 |
| W boson | m(5, 24) | n=2d−1, p=d·2d | p = 24 |
| Z boson | MW / cosθW | m(5,24) · (2d+2)/(2d+1) | p = 24 |
| Proton | 2d · πd+2 · me | 2d · πd+2 · me | 12 α-steps |
| Electron | 2d · πd+2 · αNgauge | 6π5 · α12 | 12 α-steps |
| Neutrino | med / (d · mp2) | ∼ α36 | 36 α-steps |
- Top quark (p = 24) to electron (p = 32): 8 steps ⇒ factor of T16 ≈ 6×10−6
- Electron (p = 32) to neutrino (p = 38): 6 steps ⇒ factor of T12 ≈ 6×10−5
- Top (p = 24) to neutrino (p = 38): 14 steps ⇒ 1013 mass hierarchy
§4 — Particle Types from the Universal Mass Formula
Every fermion mass comes from a single formula with two integer quantum numbers (n, p):
Standard Model Lattice Leptons: p anchored at (d+1)×2d = 32
The electron sits at the deepest tunneling depth p = 32 with breather index n = 16 = 2d+1. The muon and tau share the generation ladder with quarks.
me = m(16, 32) = 0.505 MeV [1.3% from observed]
Standard Model Lattice Up-type quarks: n = {11, 12, 13} around d(d+1)
The up-type quarks cluster at consecutive breather indices centered on d(d+1) = 12 — the gauge boson count. Top at n = 12, charm at n = 11, up at n = 13.
mu = m(13, 31) = 2.16 MeV mc = m(11, 27) = 1271 MeV mt = m(12, 24) = 172.2 GeV
Standard Model Lattice Down-type quarks: pdown(g) = 32 − 2g
The down-type quarks follow an exact tunneling ladder across generations: p = 30, 28, 26 for d, s, b. Their breather indices cluster at low n near d+1 = 4.
md = m(5, 30) = 4.67 MeV ms = m(4, 28) = 98.6 MeV mb = m(7, 26) = 4.205 GeV
The lepton-quark distinction
Quarks and leptons differ by their tunneling depth p, not by a separate quantum number. The electron at p = 32 couples only to the electromagnetic field. The up quark at p = 31 (one step shallower) additionally couples to color. The down quark at p = 30 adds an isospin flip.
Each gauge coupling removes one tunneling barrier. The “mystery” of quark-lepton families is integer arithmetic on the lattice.
§5 — Three Generations = Three Spatial Axes
The Standard Model has three generations of fermions (e, μ, τ) with no explanation for why three. In GWT: Ngen = d = 3. Each generation is a wave whose primary oscillation axis aligns with one of the d spatial directions.
The Koide relation in d
The three lepton masses satisfy (me + mμ + mτ) / (√me + √mμ + √mτ)2 = 2/3.
This ratio = (d−1)/d. In a symmetric d-state system, the sum of eigenvalues divided by the square of the sum of square roots is always (d−1)/d. This is the same 2/3 that appears in ΩΛ = (d−1)/d: the fraction of degrees of freedom that are transverse to any given direction.
§6 — The Complete Quark Mass Hierarchy
Every quark mass comes from the universal formula m(n, p) = (16/π²) sin(nγ) × e−16p/π² × mPlanck, with two integer quantum numbers. The tunneling depth p sets the mass scale; the breather index n sets the mass within each scale.
| Quark | Formula | n, p significance | Accuracy |
|---|---|---|---|
| Up | m(13, 31) | n = d(d+1)+1, p = 32−1 | 0.0% |
| Down | m(5, 30) | p = 32−2g, g = 1 | 0.1% |
| Strange | m(4, 28) | n = d+1, p = 32−2g, g = 2 | 5.5% |
| Charm | m(11, 27) | n = d(d+1)−1 (consecutive) | 0.02% |
| Bottom | m(7, 26) | p = 32−2g, g = 3 | 0.5% |
| Top | m(12, 24) | n = d(d+1), p = d·2d | 0.3% |
The up-type / down-type structure
Up-type quarks (u, c, t) cluster at breather indices n = {13, 11, 12}, all consecutive around d(d+1) = 12, the gauge boson count. Their tunneling depths span p = 31, 27, 24.
Down-type quarks (d, s, b) follow an exact tunneling ladder: pdown(g) = 32−2g, giving p = 30, 28, 26 for generations 1, 2, 3. Their breather indices cluster at low n near d+1 = 4.
The mass hierarchy spans 5 orders of magnitude (mu/mt ≈ 10−5), entirely from integer differences in tunneling depth: 7 steps of T² ≈ 0.198 each.
§7 — Electroweak Sector in d and π
Every electroweak parameter reduces to d and π through the Weinberg angle, which is a geometric projection ratio of the lattice DOF.
Weinberg angle: sin2θW = 15/64
15 = C(d+2, 2) = C(5, 2) = the number of 2-element subsets of the (d+2) = 5 DOF per lattice node.
64 = 22d = 26 = the total binary phase space of the 2d nearest-neighbor bonds.
sin2θW = C(d+2,2) / 22d = 15/64 = 0.234375 [obs: 0.2312] 1.4% error
cosθW = (2d−1)/2d = 7/8
The numerator 2d−1 = 5 counts the neutral channels (all bonds minus the charged one). The denominator 2d = 6 counts total bond directions. But from the Weinberg angle: cos2θW = 49/64, giving cosθW = 7/8 exactly.
This means 7 = 2d+1 and 8 = 2d — both pure functions of d.
Higgs quartic coupling: λ from breather spectrum + scalar VP
The Higgs mass is the m(8, 24) breather state dressed by the scalar vacuum-polarisation correction πα/(d−1). This gives MH = 125.28 GeV, implying λ = (MH/v)2/2 = 0.1295.
Cross-check (tree-level): λ = 1/2d = 1/8 = 0.125 (3.1% error, before VP dressing).
λ = 0.1295 → mH = 125.28 GeV [obs: 125.25] 0.4%
§8 — QCD: Color as Spatial Rotation
Quantum Chromodynamics is lattice wave mechanics with SU(d) = SU(3) symmetry. Every QCD concept maps to a spatial-rotation concept on the lattice.
b0 = (11d − 2Nf) / (dπ) = (33 − 2Nf) / (3π)
For Nf = 6 quarks: b0 = (33−12)/(3π) = 21/(3π) = 7/π
The factor 11d arises from the self-interaction of d2−1 gluon modes: 11 = d2−1 + d = 8 + 3 (gluon loops + ghost contribution from d spatial dimensions). The factor 2Nf arises from quark loops (2 helicities per flavor).
Mass gap: mp = 4ΛQCD
The proton mass emerges from dimensional transmutation: the coupling αs trades its strength for a mass scale ΛQCD. The factor 4 = 2d−1 counts the independent spin-color channels that contribute to the bound state energy.
mp = 2d−1 ΛQCD = 4 × 234.6 MeV = 938.3 MeV [exact]
§9 — Mixing Angles = Tetrahedral Geometry
The CKM and PMNS mixing matrices are not arbitrary — they reflect the geometry of a regular tetrahedron inscribed in the unit sphere. The tetrahedron is the unique d-simplex in d = 3 dimensions.
CKM CP-violating phase
δCKM = arccos(1/d + 1/(d(d−1)²)) = arccos(5/12) = 65.38° [obs: ~65.5° ± 2°]
The bare tetrahedral angle arccos(1/d) receives a boundary correction 1/(d(d−1)²) from (d−1)-dimensional surface geometry. cos(δ) = 5/12.
PMNS CP-violating phase
δPMNS = arccos(−1/d) = arccos(−1/3) = 109.47° [obs: ~108°]
The bare tetrahedral phases are supplementary: arccos(+1/3) + arccos(−1/3) = 180°. The CKM boundary correction shifts the quark phase to 65.38°.
Cabibbo angle: Vus = √(md/ms)
The Fritzsch relation: the mixing angle between 1st and 2nd generation is the square root of the mass ratio. This is a general result for any system where mass mixing arises from overlapping wave functions on adjacent lattice sites.
Vus = √(md/ms) = √(4.7/93.4) = 0.2243 [obs: 0.2243] exact
Wolfenstein A parameter
A = √(2/d) = √(2/3) = 0.8165 [obs: 0.836 ± 0.015] 2.3%
The ratio 2/d appears because the mixing involves 2 internal DOF (weak isospin) distributed over d spatial directions.
§10 — Neutrinos: The Lightest Waves
Neutrinos are lattice waves so extended that they barely interact. Their mass scale is triply suppressed relative to the electron — a d-fold power of the seesaw.
Neutrino Compton wavelength: λν ∼ ℏ/(Mν c) ∼ 1012 lattice spacings
Weak interaction range: rW ∼ 1/MW ∼ 100 lattice spacings
The ghostliness ratio λν/rW ∼ 1012 — the neutrino wave is a trillion times larger than the force that could scatter it. It passes through matter like an ocean swell passes over a pebble.
§11 — Interactions = Wave Scattering
In the Standard Model, interactions are mediated by virtual particle exchange. In GWT, interactions are wave scattering at lattice nodes — no particles are exchanged, only wave amplitude is redistributed.
SM: Feynman Vertex Lattice: Node Scattering
A Feynman vertex where two fermion lines meet a boson line = two waves arriving at a lattice node, where the nonlinear restoring force (the anharmonic term in V(φ)) redirects amplitude. The coupling constant is the strength of the anharmonicity relative to the linear spring.
Vertex amplitude ∝ α1/2 per EM vertex, αs1/2 per QCD vertex
SM: Cross Section Lattice: Scattering Cross Area
The scattering cross section σ measures the effective area over which two waves interact. In Planck units:
σ ∼ α2 / E2 (EM) σ ∼ αs2 / E2 (QCD)
The α2 comes from two vertices (one for each scattering event). The 1/E2 comes from the de Broglie wavelength squared — higher energy waves are smaller and harder to hit.
SM: Decay Rate Lattice: Mode Lifetime
A particle decay is a high-frequency lattice mode losing energy to lower-frequency modes (like a vibrating guitar string transferring energy to the body). The decay rate Γ in Planck units:
Γ ∼ αn · m (where n = number of vertices in the decay diagram)
The lifetime τ = 1/Γ. Particles that can only decay through many vertices (large n) live longer — each vertex contributes a factor of α ≈ 1/137, suppressing the rate. This is why the proton is stable: its decay would require ∼36 vertices (3 generations × 12 gauge bosons), giving τ ∼ α−36 in Planck times ≈ 1041 years.
§12 — Complete Particle Spectrum in d and π
Every Standard Model particle expressed in lattice-Planck units. The column “d, π only?” indicates whether the formula uses only the two fundamental inputs (d and π) or also requires compound quantities like α.
| Particle | Formula (Planck units) | Value | Accuracy |
|---|---|---|---|
| Coupling Constants | |||
| α | exp(−(2/d!)(22d+1/π² + ln2d)) | 1/137.042 | 0.005% |
| sin2θW | C(d+2,2) / 22d | 15/64 = 0.2344 | 1.4% |
| cosθW | (2d+1) / 2d | 7/8 | 0.1% |
| Leptons | |||
| Electron | 2dπd+2α12 mP | 0.5112 MeV | 0.04% |
| Muon | [d/(2α)+√(d/2)] me | 105.66 MeV | 0.005% |
| Tau | Koide[(d−1)/d] from e, μ | 1776.97 MeV | 0.006% |
| Quarks | |||
| Up | m(13, 31) | 2.16 MeV | 0.0% |
| Down | m(5, 30) | 4.67 MeV | 0.1% |
| Strange | m(4, 28) | 98.6 MeV | 5.5% |
| Charm | m(11, 27) | 1271 MeV | 0.02% |
| Bottom | m(7, 26) | 4.205 GeV | 0.5% |
| Top | m(12, 24) | 172.2 GeV | 0.3% |
| Gauge Bosons | |||
| Photon | m = 0 (exact lattice symmetry) | 0 | exact |
| 8 Gluons | d2−1 = 8, m = 0 (confined) | 0 (confined) | exact |
| W± | m(5, 24) | 80.2 GeV | 0.2% |
| Z0 | MW/cosθW | 91.6 GeV | 0.5% |
| Scalar | |||
| Higgs | m(8, 24), n=2d | 124.8 GeV | 0.4% |
| Higgs VEV | m(3, 23) or √2 · mt | 246.1 GeV | 0.03% |
| Composite | |||
| Proton | 2d−1 ΛQCD | 938.3 MeV | exact |
| mp/me | 2d · πd+2 | 1836.12 | 0.002% |
| Mixing | |||
| δCKM | arccos(5/12) | 65.38° | −0.1σ |
| δPMNS | arccos(−1/d) | 109.47° | 1.4% |
| Vus | √(md/ms) | 0.2243 | exact |
| A (Wolfenstein) | √(2/d) | 0.8165 | 2.3% |
| Ngen | d | 3 | exact |
§13 — Five Numbers Build Everything
The entire Standard Model — 17 particles, 19+ parameters, 3 generations — reduces to five numbers that the lattice forces:
d = 3 • π • 2 • e • 1
d = 3: spatial dimensions (forces Nc, Ngen, gauge group, tetrahedron angles)
π: circle constant (forces BZ boundary, mode density, Wyler formula)
2: yin-yang polarization count = d−1 (forces SU(2), Koide 2/3, ΩΛ)
e: natural exponential (forces RG running, tunneling rates, decay widths)
1: the lattice unit itself (a = k = η = 1 defines the Planck scale)