Encyclopedia Cost Cost Ndim Ricci Scalar Ricci W
ARTICLE 4 claims 3 theorems 1 model
Cost Ndim Ricci Scalar Ricci W
In the geometry of a cost function, one scalar curvature formula takes a single rational shape that unifies two coordinate systems.
The canonical Ricci form
In differential geometry, the Ricci scalar is a number that summarizes how much a space curves at a point, independent of direction. For a two-dimensional surface, it is twice the Gaussian curvature, so it tells whether the surface is locally like a sphere, a saddle, or a flat plane. In the Recognition Science framework, the cost function J(x) = (x + 1/x)/2 - 1 defines a geometry on its positive coordinate space, and that geometry has its own Ricci scalar. The declaration ricciW is the canonical rational form of that scalar.
What ricciW actually establishes is an equivalence, not a new physical law. The same Ricci scalar can be written in two coordinate systems: one using the original positive coordinates (x, y), the other using a hyperbolic coordinate q = a s + b t. The two expressions look very different, one rational in Z = x^{2a} y^{2b}, the other hyperbolic in q. The theorem ricci_scalar_equiv proves that these two forms agree whenever q is nonzero and a denominator condition holds. The proof works by converting both to a common rational form in w = exp q, which is exactly the function ricciW defines. So ricciW is the bridge that shows the two coordinate descriptions are the same geometry.
For a general reader, the point is that coordinate choices should not change the answer. If you measure curvature in one set of coordinates and get a different number than in another, you have made an error or the geometry is not well defined. ricciW is the clean, unified expression that makes the agreement visible. The theorem is machine-checked in the framework's library of formal theorems, meaning the algebraic equivalence is verified step by step without gaps. The conditions, q ≠ 0 and the denominator not vanishing, are the only places where the geometry is singular, so they are exactly where the equivalence could fail.
What ricciW does not claim is any physical interpretation. It does not say the universe has this curvature, nor that the cost function is the actual geometry of spacetime. It only establishes a mathematical identity between two ways of writing the same scalar curvature. The declaration is a definition, and the accompanying theorems are algebraic equivalences. Nothing in the pack connects this Ricci scalar to gravity, particle masses, or the dimensionality of space. Those are separate results, if they exist at all, and this page does not assert them.
MODEL ricciW · IndisputableMonolith/Cost/Ndim/RicciScalar.lean
/-- Canonical rational form of the Ricci scalar in w = exp q. -/
def ricciW (a b w : ℝ) : ℝ :=
4 * (a + b) * w ^ 3 *
((a + b - 2) * w ^ 2 + (a + b + 2)) /
((w ^ 2 - 1) ^ 2 * ((a + b - 1) * w ^ 2 + (a + b + 1)) ^ 2)
THEOREM ricci_scalar_equiv · IndisputableMonolith/Cost/Ndim/RicciScalar.lean
/-- **Main result**: the two coordinate forms of the Ricci scalar agree. -/
theorem ricci_scalar_equiv (a b q : ℝ)
(hq : q ≠ 0)
(hLC : (a + b) * Real.cosh q - Real.sinh q ≠ 0) :
ricciQ a b q = ricciZexp a b q := by
rw [ricciQ_eq_ricciW a b q hq hLC, ricciZexp_eq_ricciW]
THEOREM ricciZexp_eq_ricciW · IndisputableMonolith/Cost/Ndim/RicciScalar.lean
/-- The Z-form is `ricciW` evaluated at w = exp q. -/
theorem ricciZexp_eq_ricciW (a b q : ℝ) :
ricciZexp a b q = ricciW a b (Real.exp q) := by
unfold ricciZexp ricciW; rw [exp_two_mul, exp_three_mul]
THEOREM ricciQ_eq_ricciW · IndisputableMonolith/Cost/Ndim/RicciScalar.lean
/-- The q-form is also `ricciW` at w = exp q. -/
theorem ricciQ_eq_ricciW (a b q : ℝ)
(hq : q ≠ 0)
(hLC : (a + b) * Real.cosh q - Real.sinh q ≠ 0) :
ricciQ a b q = ricciW a b (Real.exp q) := by
set w := Real.exp q with hw_def
have hw_pos : 0 < w := Real.exp_pos q
have hw_ne : w ≠ 0 := hw_pos.ne'
have hsinh_ne : Real.sinh q ≠ 0 := Real.sinh_ne_zero.mpr hq
have hcosh_w : Real.cosh q = (w ^ 2 + 1) / (2 * w) := by
rw [Real.cosh_eq, Real.exp_neg]; field_simp; ring
have hsinh_w : Real.sinh q = (w ^ 2 - 1) / (2 * w) := by
rw [Real.sinh_eq, Real.exp_neg]; field_simp; ring
have hw2m1 : w ^ 2 - 1 ≠ 0 := by
intro h; exact hsinh_ne (by rw [hsinh_w, h, zero_div])
have hLCw : (a + b - 1) * w ^ 2 + (a + b + 1) ≠ 0 := by
intro h; apply hLC; rw [hcosh_w, hsinh_w]; field_simp; linarith
show ricciQ a b q = ricciW a b w
unfold ricciQ ricciW
rw [hcosh_w, hsinh_w]
field_simp [hw_ne, hw2m1, hLCw]
ring
What this page does not claim
The Ricci scalar is not claimed to be the curvature of physical spacetime. The declaration does not derive any particle masses or coupling constants. The equivalence does not hold without the stated conditions on q and the denominator.
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/Cost/Ndim/RicciScalar.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 physical meaning, if any, does the Ricci scalar of the cost Hessian metric carry for the framework's claims about spacetime?
- How does the Ricci scalar behave at the singular points where q = 0 or the denominator vanishes?
- Does the equivalence extend to higher-dimensional cost geometries beyond the two-coordinate case?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
MODEL ricciW · IndisputableMonolith/Cost/Ndim/RicciScalar.lean
/-- Canonical rational form of the Ricci scalar in w = exp q. -/ def ricciW (a b w : ℝ) : ℝ := 4 * (a + b) * w ^ 3 * ((a + b - 2) * w ^ 2 + (a + b + 2)) / ((w ^ 2 - 1) ^ 2 * ((a + b - 1) * w ^ 2 + (a + b + 1)) ^ 2)The declaration ricciW is the canonical rational form of the Ricci scalar for the cost Hessian metric. ricciW · IndisputableMonolith/Cost/Ndim/RicciScalar.leanTHEOREM ricci_scalar_equiv · IndisputableMonolith/Cost/Ndim/RicciScalar.lean
/-- **Main result**: the two coordinate forms of the Ricci scalar agree. -/ theorem ricci_scalar_equiv (a b q : ℝ) (hq : q ≠ 0) (hLC : (a + b) * Real.cosh q - Real.sinh q ≠ 0) : ricciQ a b q = ricciZexp a b q := by rw [ricciQ_eq_ricciW a b q hq hLC, ricciZexp_eq_ricciW]The two coordinate forms of the Ricci scalar agree whenever q is nonzero and a denominator condition holds. ricci_scalar_equiv · IndisputableMonolith/Cost/Ndim/RicciScalar.leanTHEOREM ricciZexp_eq_ricciW · IndisputableMonolith/Cost/Ndim/RicciScalar.lean
/-- The Z-form is `ricciW` evaluated at w = exp q. -/ theorem ricciZexp_eq_ricciW (a b q : ℝ) : ricciZexp a b q = ricciW a b (Real.exp q) := by unfold ricciZexp ricciW; rw [exp_two_mul, exp_three_mul]The Z-form of the Ricci scalar is ricciW evaluated at w = exp q. ricciZexp_eq_ricciW · IndisputableMonolith/Cost/Ndim/RicciScalar.leanTHEOREM ricciQ_eq_ricciW · IndisputableMonolith/Cost/Ndim/RicciScalar.lean
/-- The q-form is also `ricciW` at w = exp q. -/ theorem ricciQ_eq_ricciW (a b q : ℝ) (hq : q ≠ 0) (hLC : (a + b) * Real.cosh q - Real.sinh q ≠ 0) : ricciQ a b q = ricciW a b (Real.exp q) := by set w := Real.exp q with hw_def have hw_pos : 0 < w := Real.exp_pos q have hw_ne : w ≠ 0 := hw_pos.ne' have hsinh_ne : Real.sinh q ≠ 0 := Real.sinh_ne_zero.mpr hq have hcosh_w : Real.cosh q = (w ^ 2 + 1) / (2 * w) := by rw [Real.cosh_eq, Real.exp_neg]; field_simp; ring have hsinh_w : Real.sinh q = (w ^ 2 - 1) / (2 * w) := by rw [Real.sinh_eq, Real.exp_neg]; field_simp; ring have hw2m1 : w ^ 2 - 1 ≠ 0 := by intro h; exact hsinh_ne (by rw [hsinh_w, h, zero_div]) have hLCw : (a + b - 1) * w ^ 2 + (a + b + 1) ≠ 0 := by intro h; apply hLC; rw [hcosh_w, hsinh_w]; field_simp; linarith show ricciQ a b q = ricciW a b w unfold ricciQ ricciW rw [hcosh_w, hsinh_w] field_simp [hw_ne, hw2m1, hLCw] ringThe q-form of the Ricci scalar is also ricciW at w = exp q. ricciQ_eq_ricciW · IndisputableMonolith/Cost/Ndim/RicciScalar.lean