Encyclopedia Masses Masses Mass Genesis T10 Physical Sigma Zero Selection Current Settled Physical B
ARTICLE 4 claims 4 theorems
Masses Mass Genesis T10 Physical Sigma Zero Selection Current Settled Physical B
A machine-checked theorem shows the current physical model of the photon and matter pattern does not force a key zero-cost condition; the missing piece is an explicit selection law.
The boundary wall
The theorem currentSettledPhysicalBoundary_does_not_force_photonWindowTopologyLoadMatched proves a negative result about the framework's current model of the physical boundary between light and matter. It establishes that the existing physical posting, which includes a photon state and a matter pattern, does not logically force the photon window's load to match the amplitude selected by the matter pattern's topology. In plainer terms, the current model leaves open the possibility that the photon's propagating mode has zero cost while the matter pattern itself carries a nonzero load-recognition cost.
This is not a statement of failure but a precise boundary on what the current model can derive. The theorem shows that the current settled physical boundary class is too weak to select the sigma-zero representative, the pattern with zero load-recognition cost. The proof works by exhibiting a concrete model where the photon's propagating mode has zero cost but the matter pattern does not. This witness separates two notions of zero cost: one belonging to the photon's propagating mode, and the other being the load-recognition cost of the matter pattern itself.
The framework's library also proves that the sigma-zero-enriched physical interface, one where the matter pattern itself is at zero cost, is consistent and inhabited. A positive rescaling of the unit settled gap-one worldline supplies a witness. However, this proves non-vacuity, not selection. The exact open premise is a selection law that would mark the actual settled boundary model as the sigma-zero member of its scale orbit. Existing physical compatibility proves consistency of that choice, not selection.
What this means for the framework's broader project is a clear separation of what is derived from what remains a premise. The theorem does not claim that the physical world fails to satisfy the matching law; it claims that the current model does not force it. The missing piece is a physical selection principle, not a mathematical contradiction. This distinction is the core of the result: it identifies exactly where the framework's derivation chain stops and where a new physical assumption would be needed to proceed.
THEOREM currentSettledPhysicalBoundary_does_not_force_patternSigmaZero · IndisputableMonolith/Masses/MassGenesis/T10PhysicalSigmaZeroSelection.lean
/-- **Physical boundary wall.** The current settled physical boundary class
does not force the matter pattern to be the sigma-zero representative. -/
theorem currentSettledPhysicalBoundary_does_not_force_patternSigmaZero :
¬ ∀ model : SettledCurrentPhysicalBoundaryModel3,
loadRecognitionCost model.base.pattern = 0 := by
intro hall
obtain ⟨model, _hphoton, hpattern⟩ :=
exists_settledCurrentPhysicalBoundary_photonZero_patternNonzero
exact hpattern (hall model)
THEOREM currentSettledPhysicalBoundary_does_not_force_photonWindowTopologyLoadMatched · IndisputableMonolith/Masses/MassGenesis/T10PhysicalSigmaZeroSelection.lean
/-- Equivalent physical-boundary form of the wall: current compatibility does
not force the photon window's load to match the topology-selected matter
amplitude. -/
theorem currentSettledPhysicalBoundary_does_not_force_photonWindowTopologyLoadMatched :
¬ ∀ model : SettledCurrentPhysicalBoundaryModel3,
PhotonWindowTopologyLoadMatched
model.base.photon model.base.pattern := by
intro hall
exact currentSettledPhysicalBoundary_does_not_force_patternSigmaZero
(fun model =>
(model.patternSigmaZero_iff_photonWindowTopologyLoadMatched).2
(hall model))
THEOREM exists_settledCurrentPhysicalBoundary_photonZero_patternNonzero · IndisputableMonolith/Masses/MassGenesis/T10PhysicalSigmaZeroSelection.lean
/-- **Zero-cost mismatch witness.** There is a settled current physical
boundary model whose photon propagating mode has zero cost while its matter
pattern has nonzero load-recognition cost. -/
theorem exists_settledCurrentPhysicalBoundary_photonZero_patternNonzero :
∃ model : SettledCurrentPhysicalBoundaryModel3,
Physics.PhotonAsZeroCostMode.totalModeCost
model.base.photon.zero_cost_carrier = 0 ∧
loadRecognitionCost model.base.pattern ≠ 0 := by
obtain ⟨ψ, a, ha, hcarrier, hwin, _hunique, hne⟩ :=
uniqueGroundStateScale_does_not_force_currentAmplitude
let model :=
settledCurrentPhysicalBoundaryModelOf ha hcarrier hwin
have hpattern : loadRecognitionCost ψ ≠ 0 := by
obtain ⟨E⟩ := hcarrier
intro hzero
exact hne
((settledAnchor_loadRecognitionCost_zero_iff_amplitude
E hwin (le_of_lt ha)).1 hzero)
refine ⟨model, model.base.photon.zero_cost, ?_⟩
exact hpattern
THEOREM physicalSettledSigmaZeroModel_nonempty · IndisputableMonolith/Masses/MassGenesis/T10PhysicalSigmaZeroSelection.lean
/-- The sigma-zero-enriched physical interface is consistent and inhabited.
A positive scale of the unit settled gap-one worldline supplies a witness.
This proves non-vacuity, not selection of that witness by current boundary
data. -/
theorem physicalSettledSigmaZeroModel_nonempty :
Nonempty PhysicalSettledSigmaZeroModel3 := by
obtain ⟨Eseed⟩ := q3MatterCarrier_worldlinePattern_gapOne
obtain ⟨c, hc, hload⟩ :=
exists_scale_loadNormalizedToTopology Eseed
let ψ :=
scalePattern c (worldlinePattern gapOneTwoPhaseMode)
have Eψ : Q3ClosedPatternEvidence ψ :=
scalePattern_q3ClosedEvidence c hc Eseed
have hcarrier : Q3MatterCarrier ψ := ⟨Eψ⟩
have hunit :
SettledAnchorWindow 1 (worldlinePattern gapOneTwoPhaseMode) := by
unfold SettledAnchorWindow
funext t
simp [worldlinePattern, commitSettlementWindow_zero_eq_gapOne]
have hwin : SettledAnchorWindow c ψ := by
simpa [ψ] using scalePattern_settledAnchor c hunit
have hcost : loadRecognitionCost ψ = 0 := by
exact (loadRecognitionCost_eq_zero_iff_loadNormalizedToTopology Eψ).2
hload
exact ⟨
{ boundary :=
settledCurrentPhysicalBoundaryModelOf hc hcarrier hwin
pattern_sigma_zero := hcost }⟩
What this page does not claim
The theorem does not claim that the physical world fails to satisfy the matching law. The theorem does not claim that the sigma-zero-enriched interface is the one realized in nature. The theorem does not claim that the missing selection law can be derived from existing physical compatibility.
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/T10PhysicalSigmaZeroSelection.lean
expected axiom basis: [propext, Classical.choice, Quot.sound] (the Lean kernel's standard three; no RS-specific axioms)
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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 principle could serve as the selection law that marks the actual settled boundary model as the sigma-zero member of its scale orbit?
- How does the missing selection law relate to the framework's derivation of particle masses?
- Does the separation between photon propagating mode cost and pattern load cost appear in other sectors of the framework?
- What empirical consequences would follow if the selection law were added to the model?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM currentSettledPhysicalBoundary_does_not_force_patternSigmaZero · IndisputableMonolith/Masses/MassGenesis/T10PhysicalSigmaZeroSelection.lean
/-- **Physical boundary wall.** The current settled physical boundary class does not force the matter pattern to be the sigma-zero representative. -/ theorem currentSettledPhysicalBoundary_does_not_force_patternSigmaZero : ¬ ∀ model : SettledCurrentPhysicalBoundaryModel3, loadRecognitionCost model.base.pattern = 0 := by intro hall obtain ⟨model, _hphoton, hpattern⟩ := exists_settledCurrentPhysicalBoundary_photonZero_patternNonzero exact hpattern (hall model)The theorem proves that the current settled physical boundary class does not force the matter pattern to be the sigma-zero representative. currentSettledPhysicalBoundary_does_not_force_patternSigmaZero · IndisputableMonolith/Masses/MassGenesis/T10PhysicalSigmaZeroSelection.leanTHEOREM currentSettledPhysicalBoundary_does_not_force_photonWindowTopologyLoadMatched · IndisputableMonolith/Masses/MassGenesis/T10PhysicalSigmaZeroSelection.lean
/-- Equivalent physical-boundary form of the wall: current compatibility does not force the photon window's load to match the topology-selected matter amplitude. -/ theorem currentSettledPhysicalBoundary_does_not_force_photonWindowTopologyLoadMatched : ¬ ∀ model : SettledCurrentPhysicalBoundaryModel3, PhotonWindowTopologyLoadMatched model.base.photon model.base.pattern := by intro hall exact currentSettledPhysicalBoundary_does_not_force_patternSigmaZero (fun model => (model.patternSigmaZero_iff_photonWindowTopologyLoadMatched).2 (hall model))The theorem shows that the current boundary does not force the photon window's load to match the topology-selected matter amplitude. currentSettledPhysicalBoundary_does_not_force_photonWindowTopologyLoadMatched · IndisputableMonolith/Masses/MassGenesis/T10PhysicalSigmaZeroSelection.leanTHEOREM exists_settledCurrentPhysicalBoundary_photonZero_patternNonzero · IndisputableMonolith/Masses/MassGenesis/T10PhysicalSigmaZeroSelection.lean
/-- **Zero-cost mismatch witness.** There is a settled current physical boundary model whose photon propagating mode has zero cost while its matter pattern has nonzero load-recognition cost. -/ theorem exists_settledCurrentPhysicalBoundary_photonZero_patternNonzero : ∃ model : SettledCurrentPhysicalBoundaryModel3, Physics.PhotonAsZeroCostMode.totalModeCost model.base.photon.zero_cost_carrier = 0 ∧ loadRecognitionCost model.base.pattern ≠ 0 := by obtain ⟨ψ, a, ha, hcarrier, hwin, _hunique, hne⟩ := uniqueGroundStateScale_does_not_force_currentAmplitude let model := settledCurrentPhysicalBoundaryModelOf ha hcarrier hwin have hpattern : loadRecognitionCost ψ ≠ 0 := by obtain ⟨E⟩ := hcarrier intro hzero exact hne ((settledAnchor_loadRecognitionCost_zero_iff_amplitude E hwin (le_of_lt ha)).1 hzero) refine ⟨model, model.base.photon.zero_cost, ?_⟩ exact hpatternThe proof works by exhibiting a concrete model where the photon's propagating mode has zero cost but the matter pattern does not. exists_settledCurrentPhysicalBoundary_photonZero_patternNonzero · IndisputableMonolith/Masses/MassGenesis/T10PhysicalSigmaZeroSelection.leanTHEOREM physicalSettledSigmaZeroModel_nonempty · IndisputableMonolith/Masses/MassGenesis/T10PhysicalSigmaZeroSelection.lean
/-- The sigma-zero-enriched physical interface is consistent and inhabited. A positive scale of the unit settled gap-one worldline supplies a witness. This proves non-vacuity, not selection of that witness by current boundary data. -/ theorem physicalSettledSigmaZeroModel_nonempty : Nonempty PhysicalSettledSigmaZeroModel3 := by obtain ⟨Eseed⟩ := q3MatterCarrier_worldlinePattern_gapOne obtain ⟨c, hc, hload⟩ := exists_scale_loadNormalizedToTopology Eseed let ψ := scalePattern c (worldlinePattern gapOneTwoPhaseMode) have Eψ : Q3ClosedPatternEvidence ψ := scalePattern_q3ClosedEvidence c hc Eseed have hcarrier : Q3MatterCarrier ψ := ⟨Eψ⟩ have hunit : SettledAnchorWindow 1 (worldlinePattern gapOneTwoPhaseMode) := by unfold SettledAnchorWindow funext t simp [worldlinePattern, commitSettlementWindow_zero_eq_gapOne] have hwin : SettledAnchorWindow c ψ := by simpa [ψ] using scalePattern_settledAnchor c hunit have hcost : loadRecognitionCost ψ = 0 := by exact (loadRecognitionCost_eq_zero_iff_loadNormalizedToTopology Eψ).2 hload exact ⟨ { boundary := settledCurrentPhysicalBoundaryModelOf hc hcarrier hwin pattern_sigma_zero := hcost }⟩The sigma-zero-enriched physical interface is consistent and inhabited. physicalSettledSigmaZeroModel_nonempty · IndisputableMonolith/Masses/MassGenesis/T10PhysicalSigmaZeroSelection.lean