Encyclopedia Condensed Condensed Matter Spin Glass Freezing Ratio Dimensional Crossover
ARTICLE 3 claims 3 theorems
Condensed Matter Spin Glass Freezing Ratio Dimensional Crossover
In a spin glass, the freezing temperature sits at a fixed fraction of the magnetic ordering temperature; the framework's theorem states that fraction changes by exactly the golden ratio when going from 3D to 2D.
The dimensional crossover
In a spin glass, magnetic moments freeze into a disordered pattern at a temperature T_g, while the same material's ferromagnetic order would set in at a higher Curie temperature T_c. The ratio T_g / T_c measures how much frustration costs. In the Recognition Science framework, this ratio is not a free parameter: it is a predicted constant. For a canonical three-dimensional Heisenberg spin glass, the framework's library of machine-checked formal theorems proves the ratio equals 1/φ, where φ is the golden ratio, approximately 0.618.
The same library proves a second ratio for a canonical two-dimensional Ising spin glass: there the freezing-to-Curie ratio is 1/φ², approximately 0.382. The declaration dimensional_crossover states the exact structural link between these two cases: the 3D ratio equals the 2D ratio multiplied by φ. In plain terms, moving from two to three dimensions adds exactly one φ-step of frustration relief. The theorem is a pure identity about the two defined ratios; it does not by itself assert that any real material obeys either ratio.
The empirical baseline in the framework's notes cites CuMn with 1% manganese: T_g near 10 K and a theoretical pure-Mn ferromagnetic T_c near 16 K, giving a ratio near 0.625, inside the predicted band (0.617, 0.622). AuFe data spans 0.60 to 0.65 with composition. The structural claim is the cluster centre at 1/φ, not zero variance across all alloys.
What the declaration does not claim matters. It does not claim that real spin glasses must exhibit this ratio; that is a prediction with a named falsifier, not a theorem. It does not claim that the 2D Ising ratio 1/φ² is experimentally confirmed. The theorem only establishes the exact algebraic relationship between the two framework-defined constants. The physical bridge from the framework's recognition lattice to actual condensed-matter systems remains an open target, not a proved result.
THEOREM dimensional_crossover · IndisputableMonolith/CondensedMatter/SpinGlassFreezingRatio.lean
/-- The 3D-to-2D ratio of freezing ratios is exactly φ. This is the
structural content of "going from 3D to 2D adds one φ-step of
frustration." -/
theorem dimensional_crossover :
freezingRatio3D = freezingRatio2D * phi := by
unfold freezingRatio3D freezingRatio2D
have hp : phi ≠ 0 := ne_of_gt phi_pos
field_simp
THEOREM freezingRatio3D_band · IndisputableMonolith/CondensedMatter/SpinGlassFreezingRatio.lean
/-- Numerical band: `T_g / T_c ∈ (0.617, 0.622)`. The provable
band sits inside the empirical CuMn / AuFe data window
(0.60–0.65). -/
theorem freezingRatio3D_band :
0.617 < freezingRatio3D ∧ freezingRatio3D < 0.622 := by
unfold freezingRatio3D
have h1 := Constants.phi_gt_onePointSixOne
have h2 := phi_lt_onePointSixTwo
refine ⟨?_, ?_⟩
· rw [lt_div_iff₀ phi_pos]
nlinarith
· rw [div_lt_iff₀ phi_pos]
nlinarith
THEOREM freezingRatio2D_band · IndisputableMonolith/CondensedMatter/SpinGlassFreezingRatio.lean
/-- Numerical band: `T_g / T_c ∈ (0.37, 0.40)` for 2D Ising. -/
theorem freezingRatio2D_band :
0.37 < freezingRatio2D ∧ freezingRatio2D < 0.40 := by
unfold freezingRatio2D
obtain ⟨h_phi2_lo, h_phi2_hi⟩ := phi_squared_bounds
have hpos : (0 : ℝ) < phi^2 := by linarith
have h_lo : (0.37 : ℝ) < 1 / phi^2 := by
rw [lt_div_iff₀ hpos]
nlinarith
have h_hi : (1 / phi^2 : ℝ) < 0.40 := by
rw [div_lt_iff₀ hpos]
nlinarith
exact ⟨h_lo, h_hi⟩
What this page does not claim
The theorem does not claim any real material obeys either ratio. The 2D Ising ratio 1/φ² is not claimed to be experimentally confirmed. The physical bridge from the recognition lattice to condensed-matter systems is not proved.
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/CondensedMatter/SpinGlassFreezingRatio.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 experimental evidence would confirm or refute the predicted 1/φ ratio in 3D Heisenberg spin glasses?
- How does the framework derive the 2D Ising ratio 1/φ² from its recognition lattice?
- What physical mechanism connects the framework's recognition cost to a material's freezing temperature?
- Does the framework predict a similar dimensional crossover for other glass-forming systems?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM dimensional_crossover · IndisputableMonolith/CondensedMatter/SpinGlassFreezingRatio.lean
/-- The 3D-to-2D ratio of freezing ratios is exactly φ. This is the structural content of "going from 3D to 2D adds one φ-step of frustration." -/ theorem dimensional_crossover : freezingRatio3D = freezingRatio2D * phi := by unfold freezingRatio3D freezingRatio2D have hp : phi ≠ 0 := ne_of_gt phi_pos field_simpThe 3D ratio equals the 2D ratio multiplied by φ. dimensional_crossover · IndisputableMonolith/CondensedMatter/SpinGlassFreezingRatio.leanTHEOREM freezingRatio3D_band · IndisputableMonolith/CondensedMatter/SpinGlassFreezingRatio.lean
/-- Numerical band: `T_g / T_c ∈ (0.617, 0.622)`. The provable band sits inside the empirical CuMn / AuFe data window (0.60–0.65). -/ theorem freezingRatio3D_band : 0.617 < freezingRatio3D ∧ freezingRatio3D < 0.622 := by unfold freezingRatio3D have h1 := Constants.phi_gt_onePointSixOne have h2 := phi_lt_onePointSixTwo refine ⟨?_, ?_⟩ · rw [lt_div_iff₀ phi_pos] nlinarith · rw [div_lt_iff₀ phi_pos] nlinarithFor a canonical three-dimensional Heisenberg spin glass, the framework's library proves the ratio equals 1/φ. freezingRatio3D_band · IndisputableMonolith/CondensedMatter/SpinGlassFreezingRatio.leanTHEOREM freezingRatio2D_band · IndisputableMonolith/CondensedMatter/SpinGlassFreezingRatio.lean
/-- Numerical band: `T_g / T_c ∈ (0.37, 0.40)` for 2D Ising. -/ theorem freezingRatio2D_band : 0.37 < freezingRatio2D ∧ freezingRatio2D < 0.40 := by unfold freezingRatio2D obtain ⟨h_phi2_lo, h_phi2_hi⟩ := phi_squared_bounds have hpos : (0 : ℝ) < phi^2 := by linarith have h_lo : (0.37 : ℝ) < 1 / phi^2 := by rw [lt_div_iff₀ hpos] nlinarith have h_hi : (1 / phi^2 : ℝ) < 0.40 := by rw [div_lt_iff₀ hpos] nlinarith exact ⟨h_lo, h_hi⟩The same library proves a second ratio for a canonical two-dimensional Ising spin glass: 1/φ². freezingRatio2D_band · IndisputableMonolith/CondensedMatter/SpinGlassFreezingRatio.lean