Encyclopedia Materials Materials Lattice Parameter Fcc Rs
ARTICLE 5 claims 3 theorems 1 measured
Materials Lattice Parameter Fcc Rs
A research note in Recognition Science links copper's lattice spacing to the golden ratio and the Bohr radius, but the machine-checked proof stops short of that claim.
The lattice parameter note
The lattice parameter of a face-centered cubic (FCC) crystal is the edge length of its unit cell, the repeating cube that defines the crystal's geometry. For copper, the measured value is 3.615 angstroms (Å), where one angstrom is 10⁻¹⁰ meters. The research note in the Recognition Science (RS) framework proposes a striking correspondence: this length equals the fourth power of the golden ratio φ ≈ 1.618 multiplied by the Bohr radius a₀ ≈ 0.529 Å, the classical radius of a hydrogen atom's ground-state orbit. Since φ⁴ ≈ 6.854 and 6.854 × 0.529 ≈ 3.62 Å, the match with copper's 3.615 Å is close, within about 0.1 percent.
The golden ratio itself is the number satisfying φ² = φ + 1, approximately 1.618. Its connection to crystal structure is not new in mathematics; the ratio appears in quasicrystals and certain packing problems. But the RS note extends this to a specific claim about a fundamental constant: that the lattice parameter of FCC copper is φ⁴ times the Bohr radius. The Bohr radius, named after Niels Bohr, is a standard unit in atomic physics, so the proposal ties a macroscopic material property to a microscopic quantum scale.
What the machine-checked library actually proves is much narrower. The module domainCost defines a cost function J(m/e) that measures the recognition cost between two quantities m and e. Three theorems are verified: the cost is zero when m equals e, it is nonnegative for positive inputs, and the threshold φ − 3/2 is positive. These are general properties of the cost function, universally quantified, with no reference to copper, lattices, or the Bohr radius. The library states this explicitly: the module proves nothing specific to its subject because the cost is defined without connecting m and e to any physical quantity.
In Recognition Science, the ledger (a discrete record of recognition events) and its forced cost function J(x) = (x + 1/x)/2 − 1 form the framework's foundation. The lattice parameter note is a research direction, not a derived result. To turn it into a theorem, one would need to define m and e in terms of the FCC lattice and the Bohr radius, then prove the equality holds. That definition is absent, so the numerical agreement remains an observation, not a proof.
The distinction matters for anyone reading the framework's claims. The machine-checked theorems are real and axiom-clean, but they establish only the cost function's basic properties. The copper correspondence is a hypothesis waiting for a definition that would make it testable. Until then, it is a suggestive numerical coincidence recorded in the research notes, not a result the framework's library endorses.
MEASURED LatticeParamCert · IndisputableMonolith/Materials/Lattice_Parameter_FCC_RS.lean
structure LatticeParamCert where
cost_at_eq : ∀ r : ℝ, r ≠ 0 → domainCost r r = 0
cost_nonneg : ∀ m e : ℝ, 0 < m → 0 < e → 0 ≤ domainCost m e
threshold_pos : 0 < canonicalThreshold
HYPOTHESIS domainCost · IndisputableMonolith/Materials/Lattice_Parameter_FCC_RS.lean
def domainCost (m e : ℝ) : ℝ := Jcost (m / e)
THEOREM domainCost_at_eq · IndisputableMonolith/Materials/Lattice_Parameter_FCC_RS.lean
theorem domainCost_at_eq (r : ℝ) (h : r ≠ 0) : domainCost r r = 0 := by
unfold domainCost; rw [div_self h]; exact Jcost_unit0
THEOREM domainCost_nonneg · IndisputableMonolith/Materials/Lattice_Parameter_FCC_RS.lean
theorem domainCost_nonneg (m e : ℝ) (hm : 0 < m) (he : 0 < e) : 0 ≤ domainCost m e := by
unfold domainCost; exact Jcost_nonneg (div_pos hm he)
THEOREM canonicalThreshold_pos · IndisputableMonolith/Materials/Lattice_Parameter_FCC_RS.lean
theorem canonicalThreshold_pos : 0 < canonicalThreshold := by
unfold canonicalThreshold; linarith [phi_gt_onePointFive]
What this page does not claim
The copper lattice parameter equals φ⁴ times the Bohr radius is not a proved theorem. The module does not establish any property specific to FCC lattices or copper. The numerical agreement is not a measurement or a derived result from the framework.
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/Materials/Lattice_Parameter_FCC_RS.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 definition of m and e in terms of the FCC lattice would make the copper correspondence a theorem?
- Does the φ⁴ scaling hold for other FCC metals beyond copper?
- What is the physical interpretation of the recognition cost between a lattice parameter and the Bohr radius?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
MEASURED LatticeParamCert · IndisputableMonolith/Materials/Lattice_Parameter_FCC_RS.lean
structure LatticeParamCert where cost_at_eq : ∀ r : ℝ, r ≠ 0 → domainCost r r = 0 cost_nonneg : ∀ m e : ℝ, 0 < m → 0 < e → 0 ≤ domainCost m e threshold_pos : 0 < canonicalThresholdThe measured lattice parameter of copper is 3.615 angstroms. LatticeParamCert · IndisputableMonolith/Materials/Lattice_Parameter_FCC_RS.leanHYPOTHESIS domainCost · IndisputableMonolith/Materials/Lattice_Parameter_FCC_RS.lean
def domainCost (m e : ℝ) : ℝ := Jcost (m / e)The research note proposes that copper's lattice parameter equals φ⁴ times the Bohr radius. domainCost · IndisputableMonolith/Materials/Lattice_Parameter_FCC_RS.leanTHEOREM domainCost_at_eq · IndisputableMonolith/Materials/Lattice_Parameter_FCC_RS.lean
theorem domainCost_at_eq (r : ℝ) (h : r ≠ 0) : domainCost r r = 0 := by unfold domainCost; rw [div_self h]; exact Jcost_unit0The module proves that the cost function vanishes when m equals e. domainCost_at_eq · IndisputableMonolith/Materials/Lattice_Parameter_FCC_RS.leanTHEOREM domainCost_nonneg · IndisputableMonolith/Materials/Lattice_Parameter_FCC_RS.lean
theorem domainCost_nonneg (m e : ℝ) (hm : 0 < m) (he : 0 < e) : 0 ≤ domainCost m e := by unfold domainCost; exact Jcost_nonneg (div_pos hm he)The module proves the cost is nonnegative for positive inputs. domainCost_nonneg · IndisputableMonolith/Materials/Lattice_Parameter_FCC_RS.leanTHEOREM canonicalThreshold_pos · IndisputableMonolith/Materials/Lattice_Parameter_FCC_RS.lean
theorem canonicalThreshold_pos : 0 < canonicalThreshold := by unfold canonicalThreshold; linarith [phi_gt_onePointFive]The module proves the threshold φ − 3/2 is positive. canonicalThreshold_pos · IndisputableMonolith/Materials/Lattice_Parameter_FCC_RS.lean