Encyclopedia Gravity Gravity Analysis Regge Tthinge Aware Zero Mode Canonical Finite H Zero Momentum
ARTICLE 3 claims 3 theorems
Gravity Analysis Regge Tthinge Aware Zero Mode Canonical Finite H Zero Momentum
In a discrete lattice model of gravity, a machine-checked proof shows that a constant, uniform perturbation of the metric costs no energy at all, for any polarization.
The flat zero mode
In Regge calculus, space is chopped into flat tetrahedra, and gravity is described by the lengths of their edges. The question of whether a perturbation of this discrete geometry carries energy is answered by the second variation of the action, a kind of stiffness matrix. A zero mode, a perturbation with zero stiffness, is a flat direction: the lattice can be deformed along it without changing the action to second order, so it costs no energy.
The declaration canonicalFiniteH_zeroMomentum_eq_zero proves that a constant, uniform perturbation of the metric, one that is the same at every lattice site, is exactly such a zero mode. This holds for every lattice size N and for every polarization matrix, meaning the perturbation can be oriented in any direction and the result still holds. The proof works by showing that the assembled constant block of the stiffness matrix is a perfect square, and that the alternating sum of the edge-class coefficients vanishes for every polarization. This is a theorem in the machine-checked library of formal theorems.
The result is stronger than the specific case that motivated it. The original question concerned transverse-traceless perturbations, a particular class of metric deformations. The proof shows the constant block vanishes for every polarization, not just the transverse-traceless ones. The transverse-traceless case is a special instance, and a separate witness-level theorem exhibits the cancellation between the hinge term and the stencil-only residual on a concrete transverse-traceless example.
What the theorem does not claim is also precise. It does not prove that the full Hessian decomposition, splitting the assembled block into hinge and per-tetrahedron terms, holds everywhere; that split is kernel-checked only at the recorded witness. The theorem concerns the assembled object, not the individual pieces. It also does not claim anything about the physical meaning of this zero mode for the full theory of quantum gravity; it is a statement about the second variation of the classical Regge action on a lattice.
THEOREM zeroMomentum_symbol_is_zero · IndisputableMonolith/Gravity/Analysis/ReggeTTHingeAwareZeroMode.lean
/-- **ZERO-MODE SYMBOL COROLLARY (THEOREM): the fixed-`N` TT Bloch symbol
of the TRUE nonlinear Regge action at ZERO wave vector exists and equals
`0`, for every `N` and every polarization matrix.** This is the lattice
flat zero mode as a statement about the actual second variation, through
the Gate A1 existence chain and the Gate A2 reduction. AXIOM
DISCLOSURE: this corollary (alone in this file) rides the certified
flat-deficit chain and therefore inherits `Lean.ofReduceBool` /
`Lean.trustCompiler` in addition to the standard trio. -/
theorem zeroMomentum_symbol_is_zero (N : ℕ) [NeZero N]
(E : Fin 3 → Fin 3 → ℝ) :
TTBlochSymbolIs N E (fun _ => (0 : ℤ)) 0 := by
have h := ReggeTTFlatSecondVariation.planeWave_TTBlochSymbolIs_reduced
N E (fun _ => (0 : ℤ))
have hval : canonicalFiniteH N E (fun _ => (0 : ℤ)) =
(2 / (N : ℝ) ^ (3 : ℕ)) *
(-∑ τ : PeriodicTet N N N, ∑ f : Fin 6,
ReggeTTFlatSecondVariation.flatSlotSqrtDeriv N E
(commensurateMomentum N (fun _ => (0 : ℤ))) τ f *
ReggeTTFlatSecondVariation.flatSlotAngleDeriv N E
(commensurateMomentum N (fun _ => (0 : ℤ))) τ f) := rfl
rw [← hval, canonicalFiniteH_zeroMomentum_eq_zero N E] at h
exact h
THEOREM zeroMomentum_symbol_is_zero · IndisputableMonolith/Gravity/Analysis/ReggeTTHingeAwareZeroMode.lean
/-- **ZERO-MODE SYMBOL COROLLARY (THEOREM): the fixed-`N` TT Bloch symbol
of the TRUE nonlinear Regge action at ZERO wave vector exists and equals
`0`, for every `N` and every polarization matrix.** This is the lattice
flat zero mode as a statement about the actual second variation, through
the Gate A1 existence chain and the Gate A2 reduction. AXIOM
DISCLOSURE: this corollary (alone in this file) rides the certified
flat-deficit chain and therefore inherits `Lean.ofReduceBool` /
`Lean.trustCompiler` in addition to the standard trio. -/
theorem zeroMomentum_symbol_is_zero (N : ℕ) [NeZero N]
(E : Fin 3 → Fin 3 → ℝ) :
TTBlochSymbolIs N E (fun _ => (0 : ℤ)) 0 := by
have h := ReggeTTFlatSecondVariation.planeWave_TTBlochSymbolIs_reduced
N E (fun _ => (0 : ℤ))
have hval : canonicalFiniteH N E (fun _ => (0 : ℤ)) =
(2 / (N : ℝ) ^ (3 : ℕ)) *
(-∑ τ : PeriodicTet N N N, ∑ f : Fin 6,
ReggeTTFlatSecondVariation.flatSlotSqrtDeriv N E
(commensurateMomentum N (fun _ => (0 : ℤ))) τ f *
ReggeTTFlatSecondVariation.flatSlotAngleDeriv N E
(commensurateMomentum N (fun _ => (0 : ℤ))) τ f) := rfl
rw [← hval, canonicalFiniteH_zeroMomentum_eq_zero N E] at h
exact h
THEOREM ttWitness_isTT · IndisputableMonolith/Gravity/Analysis/ReggeTTHingeAwareZeroMode.lean
/-- The reported witness IS a TT polarization for `k = e_z`: symmetric,
traceless, transverse, Frobenius-normalized. This grounds the phrase
"the reported TT witness" of the recorded residual. -/
theorem ttWitness_isTT :
IsTTPolarization ttWitnessWaveVector ttWitnessPolarization := by
refine ⟨?_, ?_, ?_, ?_⟩
· intro i j
fin_cases i <;> fin_cases j <;> simp only [ttWitnessPolarization]
· simp only [Fin.sum_univ_three, ttWitnessPolarization]
ring
· intro j
fin_cases j <;>
· simp only [Fin.sum_univ_three, ttWitnessPolarization,
ttWitnessWaveVector]
push_cast
ring
· simp only [Fin.sum_univ_three, ttWitnessPolarization]
linear_combination 2 * inv_sqrt2_mul_self
What this page does not claim
The theorem does not prove the full Hessian decomposition assembled = hinge - sum G c c holds everywhere; that split is kernel-checked only at the recorded witness. The theorem does not claim any physical consequence for the full theory of quantum gravity. The theorem does not prove that the stencil-only constant block vanishes; it proves that the assembled block, with the hinge term, vanishes.
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/ReggeTTHingeAwareZeroMode.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 is the physical interpretation of a zero mode in a discrete gravity theory?
- How does this zero mode behave under the full nonlinear Regge action, beyond the second variation?
- What role does the hinge term play in the stability of the lattice in other momentum sectors?
- How does this lattice result connect to the continuum limit of general relativity?
- Does the existence of this zero mode imply a symmetry of the discrete action, and if so, what is its generator?
- What are the implications of a zero mode for the path integral quantization of Regge calculus?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM zeroMomentum_symbol_is_zero · IndisputableMonolith/Gravity/Analysis/ReggeTTHingeAwareZeroMode.lean
/-- **ZERO-MODE SYMBOL COROLLARY (THEOREM): the fixed-`N` TT Bloch symbol of the TRUE nonlinear Regge action at ZERO wave vector exists and equals `0`, for every `N` and every polarization matrix.** This is the lattice flat zero mode as a statement about the actual second variation, through the Gate A1 existence chain and the Gate A2 reduction. AXIOM DISCLOSURE: this corollary (alone in this file) rides the certified flat-deficit chain and therefore inherits `Lean.ofReduceBool` / `Lean.trustCompiler` in addition to the standard trio. -/ theorem zeroMomentum_symbol_is_zero (N : ℕ) [NeZero N] (E : Fin 3 → Fin 3 → ℝ) : TTBlochSymbolIs N E (fun _ => (0 : ℤ)) 0 := by have h := ReggeTTFlatSecondVariation.planeWave_TTBlochSymbolIs_reduced N E (fun _ => (0 : ℤ)) have hval : canonicalFiniteH N E (fun _ => (0 : ℤ)) = (2 / (N : ℝ) ^ (3 : ℕ)) * (-∑ τ : PeriodicTet N N N, ∑ f : Fin 6, ReggeTTFlatSecondVariation.flatSlotSqrtDeriv N E (commensurateMomentum N (fun _ => (0 : ℤ))) τ f * ReggeTTFlatSecondVariation.flatSlotAngleDeriv N E (commensurateMomentum N (fun _ => (0 : ℤ))) τ f) := rfl rw [← hval, canonicalFiniteH_zeroMomentum_eq_zero N E] at h exact hA constant, uniform perturbation of the metric is exactly a zero mode, for every lattice size N and for every polarization matrix. zeroMomentum_symbol_is_zero · IndisputableMonolith/Gravity/Analysis/ReggeTTHingeAwareZeroMode.leanTHEOREM zeroMomentum_symbol_is_zero · IndisputableMonolith/Gravity/Analysis/ReggeTTHingeAwareZeroMode.lean
/-- **ZERO-MODE SYMBOL COROLLARY (THEOREM): the fixed-`N` TT Bloch symbol of the TRUE nonlinear Regge action at ZERO wave vector exists and equals `0`, for every `N` and every polarization matrix.** This is the lattice flat zero mode as a statement about the actual second variation, through the Gate A1 existence chain and the Gate A2 reduction. AXIOM DISCLOSURE: this corollary (alone in this file) rides the certified flat-deficit chain and therefore inherits `Lean.ofReduceBool` / `Lean.trustCompiler` in addition to the standard trio. -/ theorem zeroMomentum_symbol_is_zero (N : ℕ) [NeZero N] (E : Fin 3 → Fin 3 → ℝ) : TTBlochSymbolIs N E (fun _ => (0 : ℤ)) 0 := by have h := ReggeTTFlatSecondVariation.planeWave_TTBlochSymbolIs_reduced N E (fun _ => (0 : ℤ)) have hval : canonicalFiniteH N E (fun _ => (0 : ℤ)) = (2 / (N : ℝ) ^ (3 : ℕ)) * (-∑ τ : PeriodicTet N N N, ∑ f : Fin 6, ReggeTTFlatSecondVariation.flatSlotSqrtDeriv N E (commensurateMomentum N (fun _ => (0 : ℤ))) τ f * ReggeTTFlatSecondVariation.flatSlotAngleDeriv N E (commensurateMomentum N (fun _ => (0 : ℤ))) τ f) := rfl rw [← hval, canonicalFiniteH_zeroMomentum_eq_zero N E] at h exact hThe assembled constant block of the stiffness matrix is a perfect square, and the alternating sum of the edge-class coefficients vanishes for every polarization. zeroMomentum_symbol_is_zero · IndisputableMonolith/Gravity/Analysis/ReggeTTHingeAwareZeroMode.leanTHEOREM ttWitness_isTT · IndisputableMonolith/Gravity/Analysis/ReggeTTHingeAwareZeroMode.lean
/-- The reported witness IS a TT polarization for `k = e_z`: symmetric, traceless, transverse, Frobenius-normalized. This grounds the phrase "the reported TT witness" of the recorded residual. -/ theorem ttWitness_isTT : IsTTPolarization ttWitnessWaveVector ttWitnessPolarization := by refine ⟨?_, ?_, ?_, ?_⟩ · intro i j fin_cases i <;> fin_cases j <;> simp only [ttWitnessPolarization] · simp only [Fin.sum_univ_three, ttWitnessPolarization] ring · intro j fin_cases j <;> · simp only [Fin.sum_univ_three, ttWitnessPolarization, ttWitnessWaveVector] push_cast ring · simp only [Fin.sum_univ_three, ttWitnessPolarization] linear_combination 2 * inv_sqrt2_mul_selfThe transverse-traceless case is a special instance, and a separate witness-level theorem exhibits the cancellation between the hinge term and the stencil-only residual on a concrete transverse-traceless example. ttWitness_isTT · IndisputableMonolith/Gravity/Analysis/ReggeTTHingeAwareZeroMode.lean