Encyclopedia Masses Masses Mass Genesis T10 Pair Kernel Sourced Emission Amplitude Transport Wall Ex
ARTICLE 3 claims 3 theorems
Masses Mass Genesis T10 Pair Kernel Sourced Emission Amplitude Transport Wall Ex
A machine-checked proof shows that the framework's current equations for particle mass cannot pick a single absolute scale, a gap the framework itself names as open.
The transport wall
The Recognition Science framework builds particle masses from a discrete ledger, a record of recognition events with forced costs. A central question is whether the framework's own equations, without any fitted numbers, force the absolute size of the emitted photon amplitude that sets the mass scale. The declaration exists_sharedMagnitudeSignedGreenEmission_amplitude_ne_factor is a theorem in the framework's machine-checked library of formal theorems. It proves that the current strongest candidate equations do not do this: there exists a positive amplitude and a light pattern such that all the tested conditions hold, yet the amplitude differs from the topology-factor value the framework was checking against.
What the theorem actually shows is a transport wall. The framework's signed Green source equation carries a real posting magnitude q, and the scaled sourced-emission construction carries the same q into the photon window. The package joining these two is inhabited for every positive q, including the doubled value 2q. A separate theorem proves the affine Weyl off-shell action is quadratic in field amplitude, so its dilation stationarity is invariant under any nonzero rescaling. Together these mean the present equations transport a chosen scale but do not select one: the doubled witness remains a valid countermodel.
This is not a claim that no future law can select scale. The framework explicitly labels this a transport wall, not a dead end. The missing physical object is an independently derived, inhomogeneous field-to-current transport whose verdict reads field magnitude and rejects the doubled witness. Until such a law exists, the absolute emitted amplitude, and with it the absolute mass scale, remains an open target within the framework. The theorem is a precise statement of what is currently known, not a statement of impossibility.
THEOREM exists_sharedMagnitudeSignedGreenEmission_amplitude_ne_factor · IndisputableMonolith/Masses/MassGenesis/T10PairKernelSourcedEmissionAmplitudeTransportWall.lean
/-- The banked scaled-emission countermodel remains a countermodel after the
canonical signed Green source at the same magnitude is attached. -/
theorem exists_sharedMagnitudeSignedGreenEmission_amplitude_ne_factor
(octave : Q3SettledLedgerOctave) :
∃ (a : ℝ) (ha : 0 < a) (ψ : LightPattern (Fin 8)),
SharedMagnitudeSignedGreenEmissionPackage octave a ha ∧
Q3MatterCarrier ψ ∧
SettledAnchorWindow a ψ ∧
PhotonWindowReadsPatternAnchor
(originEmittedPhotonStateScaled octave a ha).window ψ ∧
a ≠ primitivePositiveStationaryFactorAmplitude ψ := by
obtain ⟨a, ha, ψ, hcarrier, hwin, hread, hne⟩ :=
exists_scaledEmittedRead_amplitude_ne_factor octave
exact
⟨a, ha, ψ,
sharedMagnitudeSignedGreenEmissionPackage_all_positive octave a ha,
hcarrier, hwin, hread, hne⟩
THEOREM sharedMagnitudeSignedGreenEmissionPackage_all_positive · sharedMagnitudeSignedGreenEmissionPackage_accepts_doubling · IndisputableMonolith/Masses/MassGenesis/T10PairKernelSourcedEmissionAmplitudeTransportWall.lean
/-- The package is inhabited at every positive magnitude. The Green source
equation and sourced-emission construction transport a chosen scale but do not
select it. -/
theorem sharedMagnitudeSignedGreenEmissionPackage_all_positive
(octave : Q3SettledLedgerOctave) (q : ℝ) (hq : 0 < q) :
SharedMagnitudeSignedGreenEmissionPackage octave q hq := by
refine ⟨?_, ?_⟩
· exact signedPostingSourceAttachment3_realGreen
(N := 3) (by norm_num) q
(phaseBearingPostingEvent3 0).1
(phaseBearingPostingEvent3_is_S8 0)
(Equiv.refl (Fin 3))
· exact
EmittedPhotonStateScaled.window_eq_scaledCommit
(originEmittedPhotonStateScaled octave q hq)
/-- The same lower-level package holds at a positive magnitude and its doubled
copy. -/
theorem sharedMagnitudeSignedGreenEmissionPackage_accepts_doubling
(octave : Q3SettledLedgerOctave) (q : ℝ) (hq : 0 < q) :
SharedMagnitudeSignedGreenEmissionPackage octave q hq ∧
SharedMagnitudeSignedGreenEmissionPackage octave (2 * q)
(mul_pos (by norm_num) hq) :=
⟨sharedMagnitudeSignedGreenEmissionPackage_all_positive octave q hq,
sharedMagnitudeSignedGreenEmissionPackage_all_positive
octave (2 * q) (mul_pos (by norm_num) hq)⟩
THEOREM affineWeylEventAction27_mul_const · affineWeylDilationCritical27_mul_const_iff · IndisputableMonolith/Masses/MassGenesis/T10PairKernelSourcedEmissionAmplitudeTransportWall.lean
/-- The full affine action is quadratic in field amplitude at every
dilation. -/
theorem affineWeylEventAction27_mul_const
(event : RealizedPostingEvent3 3)
(dilation c : ℝ) (ψ : WeylEventAmplitude27) :
affineWeylEventAction27 event dilation (fun s => c * ψ s) =
c ^ 2 * affineWeylEventAction27 event dilation ψ := by
unfold affineWeylEventAction27
rw [finiteWeylShiftOccupationCost27_mul_const,
finiteWeylClockOccupationCost27_mul_const]
ring
/-- For a nonzero field rescaling, affine-Weyl dilation stationarity is
unchanged. It can select a shift/clock balance but not absolute field
amplitude. -/
theorem affineWeylDilationCritical27_mul_const_iff
(event : RealizedPostingEvent3 3)
(dilation : EventDilationCoord)
(c : ℝ) (hc : c ≠ 0)
(ψ : WeylEventAmplitude27) :
AffineWeylDilationCritical27 event (fun s => c * ψ s) dilation ↔
AffineWeylDilationCritical27 event ψ dilation := by
unfold AffineWeylDilationCritical27
rw [affineWeylDilationResponse27_mul_const]
exact mul_eq_zero.trans (or_iff_right (pow_ne_zero 2 hc))
What this page does not claim
The theorem does not prove that no future law can select scale; it only proves the current candidate equations cannot. The theorem does not derive the absolute value of any particle mass from first principles. The theorem does not claim the framework's mass scale is wrong, only that it is not yet forced by the tested equations.
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/T10PairKernelSourcedEmissionAmplitudeTransportWall.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 would an independently derived field-to-current transport look like, and what property would let it reject the doubled witness?
- Does the framework contain any other lower-level law that could select an absolute amplitude without being fitted?
- How does the transport wall relate to the framework's phi-power ladder for particle masses, which is an empirical check rather than a theorem?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM exists_sharedMagnitudeSignedGreenEmission_amplitude_ne_factor · IndisputableMonolith/Masses/MassGenesis/T10PairKernelSourcedEmissionAmplitudeTransportWall.lean
/-- The banked scaled-emission countermodel remains a countermodel after the canonical signed Green source at the same magnitude is attached. -/ theorem exists_sharedMagnitudeSignedGreenEmission_amplitude_ne_factor (octave : Q3SettledLedgerOctave) : ∃ (a : ℝ) (ha : 0 < a) (ψ : LightPattern (Fin 8)), SharedMagnitudeSignedGreenEmissionPackage octave a ha ∧ Q3MatterCarrier ψ ∧ SettledAnchorWindow a ψ ∧ PhotonWindowReadsPatternAnchor (originEmittedPhotonStateScaled octave a ha).window ψ ∧ a ≠ primitivePositiveStationaryFactorAmplitude ψ := by obtain ⟨a, ha, ψ, hcarrier, hwin, hread, hne⟩ := exists_scaledEmittedRead_amplitude_ne_factor octave exact ⟨a, ha, ψ, sharedMagnitudeSignedGreenEmissionPackage_all_positive octave a ha, hcarrier, hwin, hread, hne⟩It proves that the current strongest candidate equations do not force the absolute size of the emitted photon amplitude that sets the mass scale. exists_sharedMagnitudeSignedGreenEmission_amplitude_ne_factor · IndisputableMonolith/Masses/MassGenesis/T10PairKernelSourcedEmissionAmplitudeTransportWall.leanTHEOREM sharedMagnitudeSignedGreenEmissionPackage_all_positive · sharedMagnitudeSignedGreenEmissionPackage_accepts_doubling · IndisputableMonolith/Masses/MassGenesis/T10PairKernelSourcedEmissionAmplitudeTransportWall.lean
/-- The package is inhabited at every positive magnitude. The Green source equation and sourced-emission construction transport a chosen scale but do not select it. -/ theorem sharedMagnitudeSignedGreenEmissionPackage_all_positive (octave : Q3SettledLedgerOctave) (q : ℝ) (hq : 0 < q) : SharedMagnitudeSignedGreenEmissionPackage octave q hq := by refine ⟨?_, ?_⟩ · exact signedPostingSourceAttachment3_realGreen (N := 3) (by norm_num) q (phaseBearingPostingEvent3 0).1 (phaseBearingPostingEvent3_is_S8 0) (Equiv.refl (Fin 3)) · exact EmittedPhotonStateScaled.window_eq_scaledCommit (originEmittedPhotonStateScaled octave q hq)/-- The same lower-level package holds at a positive magnitude and its doubled copy. -/ theorem sharedMagnitudeSignedGreenEmissionPackage_accepts_doubling (octave : Q3SettledLedgerOctave) (q : ℝ) (hq : 0 < q) : SharedMagnitudeSignedGreenEmissionPackage octave q hq ∧ SharedMagnitudeSignedGreenEmissionPackage octave (2 * q) (mul_pos (by norm_num) hq) := ⟨sharedMagnitudeSignedGreenEmissionPackage_all_positive octave q hq, sharedMagnitudeSignedGreenEmissionPackage_all_positive octave (2 * q) (mul_pos (by norm_num) hq)⟩The package joining the signed Green source equation and the scaled sourced-emission construction is inhabited for every positive q, including the doubled value 2q. sharedMagnitudeSignedGreenEmissionPackage_all_positive · sharedMagnitudeSignedGreenEmissionPackage_accepts_doubling · IndisputableMonolith/Masses/MassGenesis/T10PairKernelSourcedEmissionAmplitudeTransportWall.leanTHEOREM affineWeylEventAction27_mul_const · affineWeylDilationCritical27_mul_const_iff · IndisputableMonolith/Masses/MassGenesis/T10PairKernelSourcedEmissionAmplitudeTransportWall.lean
/-- The full affine action is quadratic in field amplitude at every dilation. -/ theorem affineWeylEventAction27_mul_const (event : RealizedPostingEvent3 3) (dilation c : ℝ) (ψ : WeylEventAmplitude27) : affineWeylEventAction27 event dilation (fun s => c * ψ s) = c ^ 2 * affineWeylEventAction27 event dilation ψ := by unfold affineWeylEventAction27 rw [finiteWeylShiftOccupationCost27_mul_const, finiteWeylClockOccupationCost27_mul_const] ring/-- For a nonzero field rescaling, affine-Weyl dilation stationarity is unchanged. It can select a shift/clock balance but not absolute field amplitude. -/ theorem affineWeylDilationCritical27_mul_const_iff (event : RealizedPostingEvent3 3) (dilation : EventDilationCoord) (c : ℝ) (hc : c ≠ 0) (ψ : WeylEventAmplitude27) : AffineWeylDilationCritical27 event (fun s => c * ψ s) dilation ↔ AffineWeylDilationCritical27 event ψ dilation := by unfold AffineWeylDilationCritical27 rw [affineWeylDilationResponse27_mul_const] exact mul_eq_zero.trans (or_iff_right (pow_ne_zero 2 hc))A separate theorem proves the affine Weyl off-shell action is quadratic in field amplitude, so its dilation stationarity is invariant under any nonzero rescaling. affineWeylEventAction27_mul_const · affineWeylDilationCritical27_mul_const_iff · IndisputableMonolith/Masses/MassGenesis/T10PairKernelSourcedEmissionAmplitudeTransportWall.lean