Encyclopedia Gravity Gravity Cubic Regge Convergence Quartic Error Controlled
ARTICLE 2 claims 2 theorems
Gravity Cubic Regge Convergence Quartic Error Controlled
A small inequality about a cost function's error term is the hinge that lets a lattice gravity model converge to the continuum at second order.
The quartic error bound
In numerical analysis, when you approximate a smooth function by a lattice, the error usually falls off as some power of the lattice spacing. The declaration quartic_error_controlled is a theorem about one such error term. It states that for a small positive number ε (less than 1), the quantity ε⁴/24 is strictly less than ε²/2. This is a purely algebraic fact, proved in the machine-checked library of formal theorems.
The inequality matters because ε²/2 is the leading term in the expansion of a certain cost function, and ε⁴/24 bounds the next correction. The theorem guarantees that for weak fields, where ε is small, the quartic correction is genuinely smaller than the quadratic term. This is what allows the lattice action to converge to the continuum action at order a², where a is the lattice spacing, rather than being swamped by higher-order errors.
In Recognition Science, this bound is one piece of a larger convergence argument. The framework models gravity on a cubic lattice with a cost function derived from its core principles. The quartic error bound, combined with other results, shows that in the weak-field regime the lattice action approaches the continuum Einstein-Hilbert action at the expected second-order rate. The bound itself is unconditional: it holds for any ε in (0,1), with no further assumptions.
What the declaration does not claim is just as important. It does not prove that the full lattice gravity theory converges; that requires additional conditions, such as bounded curvature in the strong-field regime. It does not say anything about the physical interpretation of ε or the lattice spacing. And it does not assert that the quartic term vanishes, only that it is dominated by the quadratic term. The theorem is a precise, narrow statement about an inequality, and its role is to support a larger convergence proof, not to stand alone as a physical prediction.
THEOREM quartic_error_controlled · IndisputableMonolith/Gravity/CubicReggeConvergence.lean
/-- In the weak-field regime |ε| < 1, the quartic error in J-cost
is bounded by |ε|⁴/24 at each site.
For N lattice sites, the total error is bounded by:
N · |ε_max|⁴ / 24 ≤ (a⁻³ · V) · a⁴ · const / 24
= V · a · const / 24
where V is the total volume and a is the lattice spacing.
This is O(a) and vanishes in the continuum limit. -/
theorem quartic_error_controlled (ε_max : ℝ) (hε : 0 < ε_max) (hε1 : ε_max < 1) :
ε_max ^ 4 / 24 < ε_max ^ 2 / 2 := by
have h_sq_lt : ε_max * ε_max < 1 := by nlinarith
nlinarith [sq_nonneg ε_max, sq_nonneg (ε_max * ε_max)]
THEOREM weak_field_error_estimate · IndisputableMonolith/Gravity/CubicReggeConvergence.lean
/-- A concrete second-order finite-difference estimate for smooth weak fields.
This upgrades the previous `True` placeholder to an actual analytic bound. -/
theorem weak_field_error_estimate (f : ℝ → ℝ) (x a : ℝ) (ha : a ≠ 0)
(hf : ContDiff ℝ 4 f) :
∃ C : ℝ, 0 ≤ C ∧
|(f (x + a) + f (x - a) - 2 * f x) / a ^ 2 - deriv (deriv f) x| ≤ C * a ^ 2 := by
obtain ⟨C₀, _hC₀_nn, hC₀⟩ :=
Foundation.ContinuumLimit.continuum_limit_second_order f x a ha hf
refine ⟨|C₀|, abs_nonneg _, ?_⟩
calc
|(f (x + a) + f (x - a) - 2 * f x) / a ^ 2 - deriv (deriv f) x|
≤ C₀ * a ^ 2 := hC₀
_ ≤ |C₀| * a ^ 2 := by
exact mul_le_mul_of_nonneg_right (le_abs_self C₀) (sq_nonneg a)
What this page does not claim
The theorem does not prove convergence of the full lattice gravity theory, only the error bound for a single site. It does not assign physical meaning to the lattice spacing or the field ε. It does not claim the quartic term vanishes; it only shows it is smaller than the quadratic term.
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/CubicReggeConvergence.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:
- How does the quartic error bound combine with the other structural advantages of the cubic lattice to prove full convergence?
- What additional conditions are needed for convergence in the strong-field regime where the quartic term is not negligible?
- How does the 8-tick UV cutoff interact with the error bounds to control divergences in the continuum limit?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM quartic_error_controlled · IndisputableMonolith/Gravity/CubicReggeConvergence.lean
/-- In the weak-field regime |ε| < 1, the quartic error in J-cost is bounded by |ε|⁴/24 at each site. For N lattice sites, the total error is bounded by: N · |ε_max|⁴ / 24 ≤ (a⁻³ · V) · a⁴ · const / 24 = V · a · const / 24 where V is the total volume and a is the lattice spacing. This is O(a) and vanishes in the continuum limit. -/ theorem quartic_error_controlled (ε_max : ℝ) (hε : 0 < ε_max) (hε1 : ε_max < 1) : ε_max ^ 4 / 24 < ε_max ^ 2 / 2 := by have h_sq_lt : ε_max * ε_max < 1 := by nlinarith nlinarith [sq_nonneg ε_max, sq_nonneg (ε_max * ε_max)]For any ε in (0,1), the quartic error term ε⁴/24 is strictly less than the quadratic term ε²/2. quartic_error_controlled · IndisputableMonolith/Gravity/CubicReggeConvergence.leanTHEOREM weak_field_error_estimate · IndisputableMonolith/Gravity/CubicReggeConvergence.lean
/-- A concrete second-order finite-difference estimate for smooth weak fields. This upgrades the previous `True` placeholder to an actual analytic bound. -/ theorem weak_field_error_estimate (f : ℝ → ℝ) (x a : ℝ) (ha : a ≠ 0) (hf : ContDiff ℝ 4 f) : ∃ C : ℝ, 0 ≤ C ∧ |(f (x + a) + f (x - a) - 2 * f x) / a ^ 2 - deriv (deriv f) x| ≤ C * a ^ 2 := by obtain ⟨C₀, _hC₀_nn, hC₀⟩ := Foundation.ContinuumLimit.continuum_limit_second_order f x a ha hf refine ⟨|C₀|, abs_nonneg _, ?_⟩ calc |(f (x + a) + f (x - a) - 2 * f x) / a ^ 2 - deriv (deriv f) x| ≤ C₀ * a ^ 2 := hC₀ _ ≤ |C₀| * a ^ 2 := by exact mul_le_mul_of_nonneg_right (le_abs_self C₀) (sq_nonneg a)The bound allows the lattice action to converge to the continuum action at order a² in the weak-field regime. weak_field_error_estimate · IndisputableMonolith/Gravity/CubicReggeConvergence.lean