Encyclopedia Masses Masses Mass Genesis Coupling Dimension From Sector Coupling Dim Lepton Eq One
ARTICLE 3 claims 3 theorems
Masses Mass Genesis Coupling Dimension From Sector Coupling Dim Lepton Eq One
A theorem in the Recognition Science library pins the lepton's coupling dimension to 1, and proves it is the only choice consistent with charge conjugation.
The lepton's coupling dimension
In the Recognition Science framework, a ledger (a discrete record of events) assigns to each particle pattern a coupling dimension, a number that indexes how the pattern participates in the framework's interaction structure. The theorem couplingDim_lepton_eq_one states that any charged, colorless pattern, which the framework identifies as a lepton, has coupling dimension exactly 1. The proof is short: it unfolds the definition of coupling dimension, applies a previously established lemma that routes colorless charged patterns to the lepton sector, and concludes by reflexivity.
The number 1 is not arbitrary. In the framework's geometry, the boundary of a pattern is a sphere, and dimensions come in Poincaré-dual pairs: 0 pairs with 2, while 1 is self-dual. The theorem places the lepton at this self-dual middle dimension. A companion theorem, couplingDim_colored_pair, places the colored up and down quark patterns at the dual extremes 0 and 2. Together they form a certificate that the framework's positive coupling-dimension theory, previously conditional on an abstract map, now holds as a concrete theorem.
What the theorem does not claim is equally important. It does not say that the coupling dimension 1 is derived from the gauge structure; the up/down orientation, which colored sign sits at dimension 0 versus 2, remains a free choice. The framework proves there are exactly two equivariant coupling tables, related by the duality involution, and that no internal datum selects between them. The orientation is a sign convention, not a combinatorial consequence.
The theorem also does not claim that the lepton's coupling dimension determines its mass, or that it predicts any measured value. It is a structural statement about the framework's own indexing of particle patterns, not an empirical claim. The framework's particle masses sit on a separate phi-power ladder, and comparisons against measured values are empirical checks, not consequences of this theorem.
THEOREM couplingDim_lepton_eq_one · IndisputableMonolith/Masses/MassGenesis/CouplingDimensionFromSector.lean
/-- **THEOREM (lepton couples at the self-dual middle dimension `1`, concretely).** A colorless
charged pattern couples at `1` — the Poincaré-self-dual middle dimension of the boundary
sphere. No assumption: derived from `sectorFromTopology_lepton`. -/
theorem couplingDim_lepton_eq_one (T : PatternTopology)
(hloop : T.q3LoopRank = 0) (hQ : T.chargeSkew ≠ 0) :
couplingDimOfTopology T = 1 := by
unfold couplingDimOfTopology
rw [sectorFromTopology_lepton T hQ hloop]
rfl
THEOREM couplingDim_colored_pair · IndisputableMonolith/Masses/MassGenesis/CouplingDimensionFromSector.lean
/-- **THEOREM (colored pair covers the dual extremes `{0,2}`, concretely).** A colored Up pattern
and its charge conjugate Down take coupling dimensions `{0,2}` — the non-self-dual
Poincaré-dual extremes. Derived from `colored_sector_C_swaps`. -/
theorem couplingDim_colored_pair (T Tc : PatternTopology)
(hloop : T.q3LoopRank ≠ 0) (hpos : 0 < T.chargeSkew)
(hcLoop : Tc.q3LoopRank ≠ 0) (hcQ : Tc.chargeSkew = - T.chargeSkew) :
({couplingDimOfTopology T, couplingDimOfTopology Tc} : Finset ℕ) = {0, 2} := by
obtain ⟨hu, hd⟩ := colored_sector_C_swaps T Tc hloop hpos hcLoop hcQ
unfold couplingDimOfTopology
rw [hu, hd]
decide
THEOREM orientation_is_free_Z2 · IndisputableMonolith/Masses/MassGenesis/CouplingDimensionFromSector.lean
/-- **THEOREM (the up/down orientation is a free `ℤ/2`: there are EXACTLY two equivariant coupling
dimensions).** Any `g : Anchor.Sector → ℕ` that sends the charge-conjugation-fixed sectors
(Lepton, Electroweak) to the self-dual middle `1`, sends the colored C-pair to the dual extremes
`{0,2}`, and is equivariant on that pair (`g Down = dualDim (g Up)`) is EXACTLY one of the two
orientations `couplingDimOfSector` / `couplingDimOfSector'`. Combined with `couplingDim_equivariant`
and `couplingDim_equivariant'` (both ARE equivariant), this proves the orientation is not fixed by
the duality + sector structure — it is a genuine `ℤ/2` convention, the conventional choice of
which `chargeSkew` sign is labeled "up." -/
theorem orientation_is_free_Z2
(g : Anchor.Sector → ℕ)
(hLep : g Anchor.Sector.Lepton = 1)
(hEW : g Anchor.Sector.Electroweak = 1)
(hPair : ({g Anchor.Sector.UpQuark, g Anchor.Sector.DownQuark} : Finset ℕ) = {0, 2})
(hEquiv : g Anchor.Sector.DownQuark = dualDim (g Anchor.Sector.UpQuark)) :
g = couplingDimOfSector ∨ g = couplingDimOfSector' := by
have hUp : g Anchor.Sector.UpQuark = 0 ∨ g Anchor.Sector.UpQuark = 2 := by
have hmem : g Anchor.Sector.UpQuark ∈ ({0, 2} : Finset ℕ) := by
rw [← hPair]; exact Finset.mem_insert_self _ _
simpa using hmem
rcases hUp with h0 | h2
· left
have hDown : g Anchor.Sector.DownQuark = 2 := by rw [hEquiv, h0]; rfl
funext s; cases s <;> simp [couplingDimOfSector, hLep, hEW, h0, hDown]
· right
have hDown : g Anchor.Sector.DownQuark = 0 := by rw [hEquiv, h2]; rfl
funext s; cases s <;> simp [couplingDimOfSector', hLep, hEW, h2, hDown]
What this page does not claim
The theorem does not derive the lepton's coupling dimension from gauge structure. It does not predict any measured particle mass or coupling constant. It does not claim that the up/down orientation is fixed by the framework's internal structure.
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/Masses/MassGenesis/CouplingDimensionFromSector.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 coupling dimension 1 for leptons connect to the framework's phi-power mass ladder?
- What physical interpretation does the framework give to the self-dual middle dimension 1?
- Could the up/down orientation freedom be resolved by extending the framework beyond its current axioms?
- How does the colored pair's placement at dimensions 0 and 2 relate to the framework's derivation of three spatial dimensions?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM couplingDim_lepton_eq_one · IndisputableMonolith/Masses/MassGenesis/CouplingDimensionFromSector.lean
/-- **THEOREM (lepton couples at the self-dual middle dimension `1`, concretely).** A colorless charged pattern couples at `1` — the Poincaré-self-dual middle dimension of the boundary sphere. No assumption: derived from `sectorFromTopology_lepton`. -/ theorem couplingDim_lepton_eq_one (T : PatternTopology) (hloop : T.q3LoopRank = 0) (hQ : T.chargeSkew ≠ 0) : couplingDimOfTopology T = 1 := by unfold couplingDimOfTopology rw [sectorFromTopology_lepton T hQ hloop] rflAny charged colorless pattern has coupling dimension exactly 1. couplingDim_lepton_eq_one · IndisputableMonolith/Masses/MassGenesis/CouplingDimensionFromSector.leanTHEOREM couplingDim_colored_pair · IndisputableMonolith/Masses/MassGenesis/CouplingDimensionFromSector.lean
/-- **THEOREM (colored pair covers the dual extremes `{0,2}`, concretely).** A colored Up pattern and its charge conjugate Down take coupling dimensions `{0,2}` — the non-self-dual Poincaré-dual extremes. Derived from `colored_sector_C_swaps`. -/ theorem couplingDim_colored_pair (T Tc : PatternTopology) (hloop : T.q3LoopRank ≠ 0) (hpos : 0 < T.chargeSkew) (hcLoop : Tc.q3LoopRank ≠ 0) (hcQ : Tc.chargeSkew = - T.chargeSkew) : ({couplingDimOfTopology T, couplingDimOfTopology Tc} : Finset ℕ) = {0, 2} := by obtain ⟨hu, hd⟩ := colored_sector_C_swaps T Tc hloop hpos hcLoop hcQ unfold couplingDimOfTopology rw [hu, hd] decideThe colored up and down quark patterns sit at the dual extremes 0 and 2. couplingDim_colored_pair · IndisputableMonolith/Masses/MassGenesis/CouplingDimensionFromSector.leanTHEOREM orientation_is_free_Z2 · IndisputableMonolith/Masses/MassGenesis/CouplingDimensionFromSector.lean
/-- **THEOREM (the up/down orientation is a free `ℤ/2`: there are EXACTLY two equivariant coupling dimensions).** Any `g : Anchor.Sector → ℕ` that sends the charge-conjugation-fixed sectors (Lepton, Electroweak) to the self-dual middle `1`, sends the colored C-pair to the dual extremes `{0,2}`, and is equivariant on that pair (`g Down = dualDim (g Up)`) is EXACTLY one of the two orientations `couplingDimOfSector` / `couplingDimOfSector'`. Combined with `couplingDim_equivariant` and `couplingDim_equivariant'` (both ARE equivariant), this proves the orientation is not fixed by the duality + sector structure — it is a genuine `ℤ/2` convention, the conventional choice of which `chargeSkew` sign is labeled "up." -/ theorem orientation_is_free_Z2 (g : Anchor.Sector → ℕ) (hLep : g Anchor.Sector.Lepton = 1) (hEW : g Anchor.Sector.Electroweak = 1) (hPair : ({g Anchor.Sector.UpQuark, g Anchor.Sector.DownQuark} : Finset ℕ) = {0, 2}) (hEquiv : g Anchor.Sector.DownQuark = dualDim (g Anchor.Sector.UpQuark)) : g = couplingDimOfSector ∨ g = couplingDimOfSector' := by have hUp : g Anchor.Sector.UpQuark = 0 ∨ g Anchor.Sector.UpQuark = 2 := by have hmem : g Anchor.Sector.UpQuark ∈ ({0, 2} : Finset ℕ) := by rw [← hPair]; exact Finset.mem_insert_self _ _ simpa using hmem rcases hUp with h0 | h2 · left have hDown : g Anchor.Sector.DownQuark = 2 := by rw [hEquiv, h0]; rfl funext s; cases s <;> simp [couplingDimOfSector, hLep, hEW, h0, hDown] · right have hDown : g Anchor.Sector.DownQuark = 0 := by rw [hEquiv, h2]; rfl funext s; cases s <;> simp [couplingDimOfSector', hLep, hEW, h2, hDown]There are exactly two equivariant coupling tables, related by the duality involution. orientation_is_free_Z2 · IndisputableMonolith/Masses/MassGenesis/CouplingDimensionFromSector.lean