Encyclopedia Masses Masses Mass Genesis Coupling Dimension From Sector Coupling Dim Colored Pair
ARTICLE 2 claims 2 theorems
Masses Mass Genesis Coupling Dimension From Sector Coupling Dim Colored Pair
A theorem about quarks assigns them to the two non-middle dimensions of a boundary, and proves the assignment survives charge conjugation.
The colored pair's dimensions
In the Recognition Science framework, a ledger (a discrete record of events) carries a cost, and from that cost the framework derives a chain of physical structure. One branch of that chain concerns coupling dimensions, which are whole numbers attached to particle sectors. The theorem couplingDim_colored_pair states that a colored Up pattern and its charge conjugate Down pattern take the coupling dimensions {0, 2}.
This is a concrete result. The framework's library of formal theorems proves that a colorless Lepton couples at dimension 1, the self-dual middle dimension of the boundary sphere. The colored pair, by contrast, covers the two dual extremes, 0 and 2. The theorem is proved for any pattern with nonzero charge skew and nonzero loop rank, and it relies on the earlier result that charge conjugation swaps the colored Up and Down sectors.
The significance is that the equivariance hypothesis, which the positive coupling-dimension theory previously assumed as an abstract input, is now derived as a theorem. The library shows that the coupling dimension of a charge conjugate equals the dual of the original. This is not a definitional choice; it is a proved consequence of the sector structure.
What the theorem does not claim is also sharp. It does not fix which colored sign sits at dimension 0 versus dimension 2. The opposite orientation, Up at 2 and Down at 0, is equally equivariant. The library proves there are exactly two equivariant coupling tables, related by the duality involution, and that no internal datum selects between them. The up/down orientation remains a free choice, a sign convention, not a combinatorial consequence.
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 specify which colored sign is up. The theorem does not derive the up/down orientation from the gauge structure. The theorem does not assign a numerical mass value to any particle.
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:
- What physical prediction follows from the colored pair sitting at dimensions 0 and 2?
- How does the free up/down orientation affect the mass ladder?
- What is the dual of a coupling dimension in physical terms?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
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] decideThe theorem couplingDim_colored_pair states that a colored Up pattern and its charge conjugate Down pattern take the coupling dimensions {0, 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]The library proves there are exactly two equivariant coupling tables, related by the duality involution, and that no internal datum selects between them. orientation_is_free_Z2 · IndisputableMonolith/Masses/MassGenesis/CouplingDimensionFromSector.lean