Encyclopedia Gravity Gravity Analysis Regge Hinge4 Dstar Kernel12 Hinge4 Dstar Kernel12 Status Flags
ARTICLE 3 claims 3 theorems
Gravity Analysis Regge Hinge4 Dstar Kernel12 Hinge4 Dstar Kernel12 Status Flags
A machine-checked proof shows that one specific four-dimensional lattice hinge has a perfectly flat geometry, a small but concrete step toward a discrete theory of gravity.
A flat hinge in four dimensions
In four-dimensional geometry, a hinge is a two-dimensional triangle where several higher-dimensional shapes meet, much like an edge where several faces of a polyhedron come together. The declaration hinge4DStarKernel12Status_flags concerns one particular hinge in a repeating four-dimensional lattice, and it establishes a precise, machine-checked fact: around this hinge, the surrounding geometry is flat, meaning the angles sum to exactly 360 degrees, the same as in ordinary Euclidean space.
The proof works by examining the four four-dimensional simplices, the simplest building blocks of the lattice, that contain this hinge. For each one, the calculation shows that the dihedral angle, the angle between two faces, is 90 degrees. Since there are four such simplices around the hinge, the total angle is 4 times 90 degrees, or 360 degrees, which is the flatness condition. The declaration also records that this hinge belongs to a particular symmetry class, and that the result is stable under a uniform scaling of the lattice, a check that the flatness is not an accident of a particular size.
This result is part of a larger program to build a discrete theory of gravity, where spacetime is not a smooth continuum but a lattice of discrete pieces. In such a theory, gravity emerges from the curvature of these pieces, and a flat hinge is one where no curvature is concentrated. This declaration proves that one specific type of hinge is flat, which is a necessary but not sufficient step toward showing that the whole lattice approximates Einstein's theory of general relativity.
In Recognition Science, this is a kernel-checked theorem, meaning it has been verified by a machine-checked library of formal theorems. The proof uses no special axioms beyond the standard logical foundations, and it does not rely on any unproven assumptions. It is a small, solid piece of mathematics that can serve as a foundation for further results.
What this declaration does not claim is equally important. It does not prove that the entire lattice is flat, only this one hinge. It does not establish that the full theory of gravity emerges from these lattice pieces, which remains an open target. And it does not attempt to derive the values of physical constants from the geometry, which is a separate and much larger question.
THEOREM star_flat_angle_sum_two_pi · IndisputableMonolith/Gravity/Analysis/ReggeHinge4DStarKernel12.lean
theorem star_flat_angle_sum_two_pi : starFlatAngleSum = 2 * Real.pi := by
simp only [starFlatAngleSum, flatAngleRight_eq]; ring
THEOREM star_cardinality · IndisputableMonolith/Gravity/Analysis/ReggeHinge4DStarKernel12.lean
theorem star_cardinality :
(Finset.univ.filter (fun p : CubeTranslate × Fin 24 =>
containsHinge p.1 p.2 = true)).card = 4 := by
decide
THEOREM fullStar_homothety_stationary · IndisputableMonolith/Gravity/Analysis/ReggeHinge4DStarKernel12.lean
theorem fullStar_homothety_stationary :
fullStarDirectional (fun d => (classWeightNat d : ℝ)) = 0 := by
simp only [fullStarDirectional]
rw [sum15_all]
have hs : Real.sqrt 2 ≠ 0 := Real.sqrt_ne_zero'.mpr (by norm_num)
have w0 : classWeightNat 0 = 1 := by decide
have w1 : classWeightNat 1 = 1 := by decide
have w2 : classWeightNat 2 = 2 := by decide
have w3 : classWeightNat 3 = 1 := by decide
have w4 : classWeightNat 4 = 2 := by decide
have w5 : classWeightNat 5 = 2 := by decide
have w6 : classWeightNat 6 = 3 := by decide
have w7 : classWeightNat 7 = 1 := by decide
have w8 : classWeightNat 8 = 2 := by decide
have w9 : classWeightNat 9 = 2 := by decide
have w10 : classWeightNat 10 = 3 := by decide
have w11 : classWeightNat 11 = 2 := by decide
have w12 : classWeightNat 12 = 3 := by decide
have w13 : classWeightNat 13 = 3 := by decide
have w14 : classWeightNat 14 = 4 := by decide
simp [fullStarClassKernel, w0, w1, w2, w3, w4, w5, w6, w7, w8, w9,
w10, w11, w12, w13, w14]
field_simp
ring
What this page does not claim
This declaration does not prove that the entire four-dimensional lattice is flat. This declaration does not establish that the lattice theory converges to Einstein's general relativity. This declaration does not derive any physical constants from the lattice geometry.
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/ReggeHinge4DStarKernel12.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 flatness of this single hinge contribute to the assembly of a flat Hessian over all hinges in the lattice?
- What is the physical significance of the type (2,1) hinge, which remains an open target?
- How does this discrete lattice geometry relate to the smooth geometry of general relativity?
- What is the next kernel-checked increment in the campaign to show that the lattice reproduces Einstein-Hilbert action?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM star_flat_angle_sum_two_pi · IndisputableMonolith/Gravity/Analysis/ReggeHinge4DStarKernel12.lean
theorem star_flat_angle_sum_two_pi : starFlatAngleSum = 2 * Real.pi := by simp only [starFlatAngleSum, flatAngleRight_eq]; ringAround this hinge, the surrounding geometry is flat, meaning the angles sum to exactly 360 degrees. star_flat_angle_sum_two_pi · IndisputableMonolith/Gravity/Analysis/ReggeHinge4DStarKernel12.leanTHEOREM star_cardinality · IndisputableMonolith/Gravity/Analysis/ReggeHinge4DStarKernel12.lean
theorem star_cardinality : (Finset.univ.filter (fun p : CubeTranslate × Fin 24 => containsHinge p.1 p.2 = true)).card = 4 := by decideThe proof works by examining the four four-dimensional simplices, the simplest building blocks of the lattice, that contain this hinge. star_cardinality · IndisputableMonolith/Gravity/Analysis/ReggeHinge4DStarKernel12.leanTHEOREM fullStar_homothety_stationary · IndisputableMonolith/Gravity/Analysis/ReggeHinge4DStarKernel12.lean
theorem fullStar_homothety_stationary : fullStarDirectional (fun d => (classWeightNat d : ℝ)) = 0 := by simp only [fullStarDirectional] rw [sum15_all] have hs : Real.sqrt 2 ≠ 0 := Real.sqrt_ne_zero'.mpr (by norm_num) have w0 : classWeightNat 0 = 1 := by decide have w1 : classWeightNat 1 = 1 := by decide have w2 : classWeightNat 2 = 2 := by decide have w3 : classWeightNat 3 = 1 := by decide have w4 : classWeightNat 4 = 2 := by decide have w5 : classWeightNat 5 = 2 := by decide have w6 : classWeightNat 6 = 3 := by decide have w7 : classWeightNat 7 = 1 := by decide have w8 : classWeightNat 8 = 2 := by decide have w9 : classWeightNat 9 = 2 := by decide have w10 : classWeightNat 10 = 3 := by decide have w11 : classWeightNat 11 = 2 := by decide have w12 : classWeightNat 12 = 3 := by decide have w13 : classWeightNat 13 = 3 := by decide have w14 : classWeightNat 14 = 4 := by decide simp [fullStarClassKernel, w0, w1, w2, w3, w4, w5, w6, w7, w8, w9, w10, w11, w12, w13, w14] field_simp ringThe result is stable under a uniform scaling of the lattice. fullStar_homothety_stationary · IndisputableMonolith/Gravity/Analysis/ReggeHinge4DStarKernel12.lean