Encyclopedia Gravity Gravity Analysis Recognition Mesh Exact Jbridge4 D
ARTICLE 4 claims 3 theorems 1 model
Gravity Analysis Recognition Mesh Exact Jbridge4 D
A discrete lattice of points in four dimensions can carry a gravitational action that converges to the continuum theory as the lattice refines.
The mesh bridge
In the Recognition Science framework, gravity analysis recognition mesh exact jbridge4 d is a machine-checked construction that connects a discrete lattice model of spacetime to the smooth continuum of general relativity. The module builds a specific kind of mesh, a periodic Freudenthal 4-torus, which is a regular grid of points on a four-dimensional torus with a particular triangulation. On this mesh it defines an action, a quantity whose variation gives the equations of motion, using a rule called the exact midpoint Bloch symbol. The central result is that as the mesh gets finer, this discrete action approaches the continuum Einstein-Hilbert action, the standard geometric description of gravity.
The construction works in several steps, each checked by the framework's machine-checked library of formal theorems. First, the module defines the mesh and a wave, a fluctuation on the mesh labeled by a momentum mode. It then defines an action at a small amplitude epsilon. The key theorem, recognition (the cost of registering an event in the ledger) is that the second derivative of this action with respect to amplitude, the amplitude Hessian, exists and equals the true Regge Hessian, the discrete gravity action of Regge calculus, by construction. This is a MODEL identification: the action is defined to be the exact midpoint Bloch symbol, not derived from first principles.
The second major theorem concerns the limit as the mesh size N goes to infinity. The module proves that the iterated limit closes at a specific continuum face, the scale-explicit Option-C face, which is the Einstein-Hilbert action with a particular normalization. This is a THEOREM, proved by composing the discrete torus bridge with exact midpoint mass-squared TT and gauge faces. The result is that the discrete action, after normalization by the momentum norm squared, converges to the continuum action. A related theorem proves that pure gauge modes, which represent coordinate choices rather than physical degrees of freedom, converge to zero in this limit, as they should.
The module is explicit about what it does not claim. The elevation of the model action to a literal nonlinear Regge action via the Schläfli formula remains open; the identification is at the level of the Hessian, not the full action. The module also does not flip the gap action recovery flag, meaning it does not recover the action from the gap, and it does not inhabit the statement that the RS action converges to the Einstein-Hilbert action in four dimensions. These are targets, not achievements.
THEOREM exactJEqualsTrueReggeHessian_holds · IndisputableMonolith/Gravity/Analysis/RecognitionMeshExactJBridge4D.lean
/-- **THEOREM:** exact-J amplitude Hessian equals the mesh true-Regge
Hessian by construction (MODEL action identification). -/
theorem exactJEqualsTrueReggeHessian_holds :
ExactJEqualsTrueReggeHessian := by
intro j m E _hm _hTT
refine ⟨meshTrueReggeQuadraticHessian (canonicalRecognitionMesh j) m E,
exactJAmplitudeHessian_eq_mesh _ _ _, rfl⟩
THEOREM recognitionExactJConvergesEH_closed · IndisputableMonolith/Gravity/Analysis/RecognitionMeshExactJBridge4D.lean
/-- The Recognition mesh midpoint sequence closes at the scale-explicit
Option-C EH face. -/
theorem recognitionExactJConvergesEH_closed :
RecognitionExactJConvergesEH := by
intro m E hm hTT
refine ⟨fun j =>
meshTrueReggeQuadraticHessian (canonicalRecognitionMesh j) m E, ?_, ?_⟩
· intro j
exact exactJAmplitudeHessian_eq_mesh _ _ _
·
set k : Wave4 := fun i => (m i : ℝ)
have hbridge := discrete_torus_family_bridge m E hm
have hk : waveNormSq k ≠ 0 := waveNormSq_intMode_ne_zero m hm
have hRay := exactMidpointBlochM2_eq_neg_eighth_frobenius_tt E k hTT
have hF :
ReggeExactMidpointM2TTIdentity4D.frobeniusNormSq E =
frobeniusNormSq E :=
(frobeniusNormSq_preflight_eq_identity E).symm
have hw :
ReggeExactMidpointM2TTIdentity4D.waveNormSq k = waveNormSq k :=
(waveNormSq_preflight_eq_identity k).symm
have hEq :
exactMidpointBlochM2 E k / waveNormSq k =
continuumEHScaleExplicitFace E := by
calc
exactMidpointBlochM2 E k / waveNormSq k
= ((-(1 / 8) : ℝ) *
ReggeExactMidpointM2TTIdentity4D.frobeniusNormSq E *
ReggeExactMidpointM2TTIdentity4D.waveNormSq k) /
waveNormSq k := by
rw [hRay]
_ = ((-(1 / 8) : ℝ) * frobeniusNormSq E * waveNormSq k) /
waveNormSq k := by
rw [hF, hw]
_ = (-(1 / 8) : ℝ) * frobeniusNormSq E := by
field_simp [hk]
_ = continuumEHScaleExplicitFace E :=
(continuumEHScaleExplicitFace_eq E).symm
simpa [meshTrueReggeQuadraticHessian, meshWave, RecognitionFreudenthalMesh4D.side,
canonicalRecognitionMesh, k, hEq] using hbridge
THEOREM recognitionExactJConvergesGaugeZero_closed · IndisputableMonolith/Gravity/Analysis/RecognitionMeshExactJBridge4D.lean
/-- The Recognition mesh midpoint sequence vanishes on pure-gauge faces. -/
theorem recognitionExactJConvergesGaugeZero_closed :
RecognitionExactJConvergesGaugeZero := by
intro m v hm
set E : Mat4 := pureGaugeFamily (fun i => (m i : ℝ)) v
set k : Wave4 := fun i => (m i : ℝ)
have hbridge := discrete_torus_family_bridge m E hm
have hk : waveNormSq k ≠ 0 := waveNormSq_intMode_ne_zero m hm
have hk' : ReggeExactMidpointM2TTIdentity4D.waveNormSq k ≠ 0 := by
simpa [waveNormSq_preflight_eq_identity] using hk
have hGauge : exactMidpointBlochM2 E k / waveNormSq k = 0 := by
simpa [E, pureGaugeFamily] using exactMidpointBlochM2_gauge_rayleigh_eq_zero k v hk'
simpa [meshTrueReggeQuadraticHessian, meshWave, RecognitionFreudenthalMesh4D.side,
canonicalRecognitionMesh, E, k, hGauge] using hbridge
MODEL exactJActionOnMesh · IndisputableMonolith/Gravity/Analysis/RecognitionMeshExactJBridge4D.lean
/-- Recognition exact-J action on the mesh at amplitude `ε`.
MODEL: identified with the true-weight Regge quadratic Hessian on the
same edge-class perturbation `ε • E` (homogeneous of degree two in the
fold). Not an ArbitraryPullback / TestVariationPullback substitute.
Schläfli elevation remains OPEN. -/
def exactJActionOnMesh (M : RecognitionFreudenthalMesh4D)
(m : IntMode4) (E : Mat4) (ε : ℝ) : ℝ :=
(1 / 2) * ε ^ 2 * meshTrueReggeQuadraticHessian M m E
What this page does not claim
The module does not prove that the discrete action equals the continuum Einstein-Hilbert action for all configurations. The module does not derive the exact midpoint Bloch symbol from the recognition cost function. The module does not claim to recover the action from the spectral gap.
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/Gravity/Analysis/RecognitionMeshExactJBridge4D.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 is the physical interpretation of the recognition mesh in terms of observable spacetime?
- Does the convergence to the continuum action hold for all polarizations or only TT modes?
- What is the status of the Schläfli elevation to a nonlinear Regge action?
- How does this mesh construction relate to the framework's derivation of three spatial dimensions?
- What is the role of the Freudenthal triangulation in the convergence proof?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM exactJEqualsTrueReggeHessian_holds · IndisputableMonolith/Gravity/Analysis/RecognitionMeshExactJBridge4D.lean
/-- **THEOREM:** exact-J amplitude Hessian equals the mesh true-Regge Hessian by construction (MODEL action identification). -/ theorem exactJEqualsTrueReggeHessian_holds : ExactJEqualsTrueReggeHessian := by intro j m E _hm _hTT refine ⟨meshTrueReggeQuadraticHessian (canonicalRecognitionMesh j) m E, exactJAmplitudeHessian_eq_mesh _ _ _, rfl⟩The amplitude Hessian exists and equals the mesh true-Regge Hessian by construction. exactJEqualsTrueReggeHessian_holds · IndisputableMonolith/Gravity/Analysis/RecognitionMeshExactJBridge4D.leanTHEOREM recognitionExactJConvergesEH_closed · IndisputableMonolith/Gravity/Analysis/RecognitionMeshExactJBridge4D.lean
/-- The Recognition mesh midpoint sequence closes at the scale-explicit Option-C EH face. -/ theorem recognitionExactJConvergesEH_closed : RecognitionExactJConvergesEH := by intro m E hm hTT refine ⟨fun j => meshTrueReggeQuadraticHessian (canonicalRecognitionMesh j) m E, ?_, ?_⟩ · intro j exact exactJAmplitudeHessian_eq_mesh _ _ _ · set k : Wave4 := fun i => (m i : ℝ) have hbridge := discrete_torus_family_bridge m E hm have hk : waveNormSq k ≠ 0 := waveNormSq_intMode_ne_zero m hm have hRay := exactMidpointBlochM2_eq_neg_eighth_frobenius_tt E k hTT have hF : ReggeExactMidpointM2TTIdentity4D.frobeniusNormSq E = frobeniusNormSq E := (frobeniusNormSq_preflight_eq_identity E).symm have hw : ReggeExactMidpointM2TTIdentity4D.waveNormSq k = waveNormSq k := (waveNormSq_preflight_eq_identity k).symm have hEq : exactMidpointBlochM2 E k / waveNormSq k = continuumEHScaleExplicitFace E := by calc exactMidpointBlochM2 E k / waveNormSq k = ((-(1 / 8) : ℝ) * ReggeExactMidpointM2TTIdentity4D.frobeniusNormSq E * ReggeExactMidpointM2TTIdentity4D.waveNormSq k) / waveNormSq k := by rw [hRay] _ = ((-(1 / 8) : ℝ) * frobeniusNormSq E * waveNormSq k) / waveNormSq k := by rw [hF, hw] _ = (-(1 / 8) : ℝ) * frobeniusNormSq E := by field_simp [hk] _ = continuumEHScaleExplicitFace E := (continuumEHScaleExplicitFace_eq E).symm simpa [meshTrueReggeQuadraticHessian, meshWave, RecognitionFreudenthalMesh4D.side, canonicalRecognitionMesh, k, hEq] using hbridgeThe iterated N to infinity Tendsto closes at the scale-explicit Option-C face. recognitionExactJConvergesEH_closed · IndisputableMonolith/Gravity/Analysis/RecognitionMeshExactJBridge4D.leanTHEOREM recognitionExactJConvergesGaugeZero_closed · IndisputableMonolith/Gravity/Analysis/RecognitionMeshExactJBridge4D.lean
/-- The Recognition mesh midpoint sequence vanishes on pure-gauge faces. -/ theorem recognitionExactJConvergesGaugeZero_closed : RecognitionExactJConvergesGaugeZero := by intro m v hm set E : Mat4 := pureGaugeFamily (fun i => (m i : ℝ)) v set k : Wave4 := fun i => (m i : ℝ) have hbridge := discrete_torus_family_bridge m E hm have hk : waveNormSq k ≠ 0 := waveNormSq_intMode_ne_zero m hm have hk' : ReggeExactMidpointM2TTIdentity4D.waveNormSq k ≠ 0 := by simpa [waveNormSq_preflight_eq_identity] using hk have hGauge : exactMidpointBlochM2 E k / waveNormSq k = 0 := by simpa [E, pureGaugeFamily] using exactMidpointBlochM2_gauge_rayleigh_eq_zero k v hk' simpa [meshTrueReggeQuadraticHessian, meshWave, RecognitionFreudenthalMesh4D.side, canonicalRecognitionMesh, E, k, hGauge] using hbridgePure gauge modes converge to zero in the large mesh limit. recognitionExactJConvergesGaugeZero_closed · IndisputableMonolith/Gravity/Analysis/RecognitionMeshExactJBridge4D.leanMODEL exactJActionOnMesh · IndisputableMonolith/Gravity/Analysis/RecognitionMeshExactJBridge4D.lean
/-- Recognition exact-J action on the mesh at amplitude `ε`. MODEL: identified with the true-weight Regge quadratic Hessian on the same edge-class perturbation `ε • E` (homogeneous of degree two in the fold). Not an ArbitraryPullback / TestVariationPullback substitute. Schläfli elevation remains OPEN. -/ def exactJActionOnMesh (M : RecognitionFreudenthalMesh4D) (m : IntMode4) (E : Mat4) (ε : ℝ) : ℝ := (1 / 2) * ε ^ 2 * meshTrueReggeQuadraticHessian M m EThe exact J action on the mesh is defined as the exact midpoint Bloch symbol on edge classes at amplitude epsilon. exactJActionOnMesh · IndisputableMonolith/Gravity/Analysis/RecognitionMeshExactJBridge4D.lean