Encyclopedia Cost Cost Ndim Curvature Bridge Dot Sharp Dinv Two Sparse
ARTICLE 2 claims 2 theorems
Cost Ndim Curvature Bridge Dot Sharp Dinv Two Sparse
A machine-checked theorem shows that a certain energy-like sum, which naively runs over all dimensions, reduces to just two terms when the system's activity is confined to two coordinates.
The self-energy collapse
In the Recognition Science framework, a central object is a ledger, a discrete record of recognition events, and the cost of recognition is forced, not chosen. The framework works with a potential function whose Hessian, the matrix of second derivatives, defines a metric. The declaration dot_sharp_Dinv_twoSparse is a theorem about a specific sum that appears in this geometry: the self-energy of a vector, which measures how much the vector interacts with itself under the inverse of a diagonal matrix.
The theorem states that if a vector α is two-sparse, meaning it has nonzero components only on two coordinates, say i0 and i1, then the sum dot α (sharp (Dinv t) α) collapses to just two terms: (cosh (t i0))⁻¹ * α i0² + (cosh (t i1))⁻¹ * α i1². In plain language, the self-energy of a two-sparse vector depends only on its two active components and the corresponding diagonal entries of the inverse metric. All other contributions vanish because the vector has no weight there.
This is not a standalone curiosity. It is a key step in a larger proof, the curvature bridge, which shows that the deformed metric h_λ = D + λ g̃ is genuinely non-flat in any dimension n. The theorem dot_sharp_Dinv_twoSparse provides the algebraic simplification that allows the full Riemann curvature tensor, a complicated object with many indices, to be reduced to a single negative component on a two-dimensional slice. This reduction is what lets the framework prove that the metric has curvature, a fact with consequences for the structure of space itself.
It is important to be precise about what this theorem does not claim. It does not say that the self-energy is always positive or negative; it only gives a formula for its value. It does not prove that the metric is non-flat on its own; that requires the additional hypotheses of the capstone theorem RiemannMixedApply_neg, such as t i1 = 0 and α i0 ≠ 0. Finally, it does not apply to vectors that are not two-sparse; the collapse depends on the support being exactly two coordinates.
THEOREM dot_sharp_Dinv_twoSparse · IndisputableMonolith/Cost/Ndim/CurvatureBridge.lean
/-- `S = dot α (D⁻¹α)` restricted to a `TwoSparse` support: only the `i0, i1`
components survive. -/
theorem dot_sharp_Dinv_twoSparse {n : ℕ} (t α : Vec n) (i0 i1 : Fin n) (hne : i0 ≠ i1)
(h2 : TwoSparse α i0 i1) :
dot α (sharp (Dinv t) α)
= (Real.cosh (t i0))⁻¹ * α i0 ^ 2 + (Real.cosh (t i1))⁻¹ * α i1 ^ 2 := by
have hpt : ∀ i : Fin n, α i * sharp (Dinv t) α i = (Real.cosh (t i))⁻¹ * α i ^ 2 := by
intro i; rw [sharp_Dinv_apply]; ring
unfold dot
rw [Finset.sum_congr rfl (fun i _ => hpt i)]
exact sum_twoSparse α i0 i1 hne h2 (fun i => (Real.cosh (t i))⁻¹)
THEOREM RiemannMixedApply_neg · IndisputableMonolith/Cost/Ndim/CurvatureBridge.lean
/-- **Theorem 2, general `n`.** Under the block-diagonal hypotheses plus `b ≠ 0` and
`t i0 ≠ 0`, the mixed Riemann tensor `R^{i0}_{i1,i0,i1}` of the *actual* `n`-dimensional
deformed metric `h_λ` is strictly negative: `h_λ` is genuinely non-flat, for any
ambient dimension `n` and any `α` supported on two coordinates. This is the honest
general-`n` generalization of `R0101Gen_neg` (`ScalarCertificates.lean`), assembled
from the algebraic reduction above plus the already-certified 2-D negativity. -/
theorem RiemannMixedApply_neg {n : ℕ} (α t : Vec n) (lam a b : ℝ) (i0 i1 : Fin n)
(hne01 : i0 ≠ i1) (h2 : TwoSparse α i0 i1)
(ha : α i0 = a) (hb : α i1 = b) (ht1 : t i1 = 0)
(ha0 : a ≠ 0) (hb0 : b ≠ 0) (hlam : 0 < lam) (ht0 : t i0 ≠ 0) :
RiemannMixedApply (hInvFull α t lam) (beta α t lam) i0 i1 i0 i1 < 0 := by
rw [RiemannMixedApply_reduce α t lam a b i0 i1 hne01 h2 ha hb ht1 ha0 hlam]
exact R0101Gen_neg a b lam (t i0) ha0 hb0 hlam ht0
What this page does not claim
The theorem does not prove the metric is non-flat by itself. The theorem does not apply to vectors that are not two-sparse. The theorem does not state the sign of the self-energy.
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/CurvatureBridge.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 geometric meaning of the self-energy term in the context of the deformed metric?
- How does the two-sparse condition relate to the physical interpretation of the recognition framework?
- What are the implications of the curvature being negative for the structure of space in the framework?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM dot_sharp_Dinv_twoSparse · IndisputableMonolith/Cost/Ndim/CurvatureBridge.lean
/-- `S = dot α (D⁻¹α)` restricted to a `TwoSparse` support: only the `i0, i1` components survive. -/ theorem dot_sharp_Dinv_twoSparse {n : ℕ} (t α : Vec n) (i0 i1 : Fin n) (hne : i0 ≠ i1) (h2 : TwoSparse α i0 i1) : dot α (sharp (Dinv t) α) = (Real.cosh (t i0))⁻¹ * α i0 ^ 2 + (Real.cosh (t i1))⁻¹ * α i1 ^ 2 := by have hpt : ∀ i : Fin n, α i * sharp (Dinv t) α i = (Real.cosh (t i))⁻¹ * α i ^ 2 := by intro i; rw [sharp_Dinv_apply]; ring unfold dot rw [Finset.sum_congr rfl (fun i _ => hpt i)] exact sum_twoSparse α i0 i1 hne h2 (fun i => (Real.cosh (t i))⁻¹)The theorem states that if a vector α is two-sparse, meaning it has nonzero components only on two coordinates, say i0 and i1, then the sum dot α (sharp (Dinv t) α) collapses to just two terms: (cosh (t i0))⁻¹ * α i0² + (cosh (t i1))⁻¹ * α i1². dot_sharp_Dinv_twoSparse · IndisputableMonolith/Cost/Ndim/CurvatureBridge.leanTHEOREM RiemannMixedApply_neg · IndisputableMonolith/Cost/Ndim/CurvatureBridge.lean
/-- **Theorem 2, general `n`.** Under the block-diagonal hypotheses plus `b ≠ 0` and `t i0 ≠ 0`, the mixed Riemann tensor `R^{i0}_{i1,i0,i1}` of the *actual* `n`-dimensional deformed metric `h_λ` is strictly negative: `h_λ` is genuinely non-flat, for any ambient dimension `n` and any `α` supported on two coordinates. This is the honest general-`n` generalization of `R0101Gen_neg` (`ScalarCertificates.lean`), assembled from the algebraic reduction above plus the already-certified 2-D negativity. -/ theorem RiemannMixedApply_neg {n : ℕ} (α t : Vec n) (lam a b : ℝ) (i0 i1 : Fin n) (hne01 : i0 ≠ i1) (h2 : TwoSparse α i0 i1) (ha : α i0 = a) (hb : α i1 = b) (ht1 : t i1 = 0) (ha0 : a ≠ 0) (hb0 : b ≠ 0) (hlam : 0 < lam) (ht0 : t i0 ≠ 0) : RiemannMixedApply (hInvFull α t lam) (beta α t lam) i0 i1 i0 i1 < 0 := by rw [RiemannMixedApply_reduce α t lam a b i0 i1 hne01 h2 ha hb ht1 ha0 hlam] exact R0101Gen_neg a b lam (t i0) ha0 hb0 hlam ht0It is a key step in a larger proof, the curvature bridge, which shows that the deformed metric h_λ = D + λ g̃ is genuinely non-flat in any dimension n. RiemannMixedApply_neg · IndisputableMonolith/Cost/Ndim/CurvatureBridge.lean