Encyclopedia Condensed Condensed Matter Spin Glass Freezing Ratio Freezing Ratio3 D Band
ARTICLE 4 claims 1 theorem 1 measured
Condensed Matter Spin Glass Freezing Ratio Freezing Ratio3 D Band
In a spin glass, the temperature where magnetic moments freeze is set by the golden ratio relative to the ferromagnetic ordering temperature, a claim now pinned to a precise numerical band.
The 3D freezing band
A spin glass is a magnetic alloy, such as copper with a sprinkle of manganese atoms, where the magnetic moments of the impurity atoms point in random directions and become locked into a disordered pattern when cooled. The freezing temperature Tg is where that locking happens. In a ferromagnet, the Curie temperature Tc marks where moments align. The Recognition Science declaration freezingRatio3D_band proves a narrow numerical statement: for a canonical three-dimensional Heisenberg spin glass, the ratio Tg/Tc lies strictly between 0.617 and 0.622.
That band is not pulled from a fit. It is a theorem in the framework's machine-checked library of formal theorems, derived from the definition that sets the ratio to 1/φ, where φ is the golden ratio, approximately 1.618. The proof uses only the known bounds on φ to show 1/φ falls inside the stated interval. The framework's account treats the spin glass as realizing a frustrated sector of its recognition lattice, while a ferromagnet realizes an unfrustrated sector; the ratio of their characteristic energy scales is the golden ratio's reciprocal.
The empirical baseline comes from CuMn with 1% manganese: Tg ≈ 10 K and a theoretical pure-manganese ferromagnetic Tc ≈ 16 K, giving a ratio near 0.625. Gold-iron data spans 0.60 to 0.65 depending on composition. The framework's provable band of (0.617, 0.622) sits inside this observed window, but the structural claim is that the cluster center is 1/φ, not that variance is zero.
In Recognition Science, this is a recognition event, a discrete record of a system settling into a state, and the ratio is forced by the framework's cost structure rather than chosen. The declaration does not claim that every spin glass obeys this ratio, nor that the empirical data prove the framework. It establishes a precise mathematical bound on a defined quantity, and offers a falsifiable prediction: a survey of at least ten spin glasses with calibrated Tc references should find the median ratio inside (0.61, 0.62) at the 2σ level.
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
MODEL freezingRatio3D · IndisputableMonolith/CondensedMatter/SpinGlassFreezingRatio.lean
/-- The freezing-to-Curie ratio for canonical 3D Heisenberg spin
glasses: `1 / φ`. -/
def freezingRatio3D : ℝ := 1 / phi
MEASURED 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
HYPOTHESIS 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
What this page does not claim
This does not claim that all spin glasses obey the golden ratio, only a canonical 3D Heisenberg class. This does not claim the empirical data prove the framework; the data are a consistency check, not a theorem. This does not claim the framework derives the freezing temperature itself, only the ratio to the Curie temperature.
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 physical mechanism sets the freezing temperature in a spin glass?
- How does the framework derive the golden ratio from its cost function?
- What distinguishes a canonical 3D Heisenberg spin glass from other spin glass models?
- How is the ferromagnetic Curie temperature calibrated for a pure manganese reference?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
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] nlinarithfor a canonical three-dimensional Heisenberg spin glass, the ratio T_g/T_c lies strictly between 0.617 and 0.622. freezingRatio3D_band · IndisputableMonolith/CondensedMatter/SpinGlassFreezingRatio.leanMODEL freezingRatio3D · IndisputableMonolith/CondensedMatter/SpinGlassFreezingRatio.lean
/-- The freezing-to-Curie ratio for canonical 3D Heisenberg spin glasses: `1 / φ`. -/ def freezingRatio3D : ℝ := 1 / phiThe framework's account treats the spin glass as realizing a frustrated sector of its recognition lattice, while a ferromagnet realizes an unfrustrated sector. freezingRatio3D · IndisputableMonolith/CondensedMatter/SpinGlassFreezingRatio.leanMEASURED 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] nlinarithThe empirical baseline comes from CuMn with 1% manganese: T_g ≈ 10 K and a theoretical pure-manganese ferromagnetic T_c ≈ 16 K, giving a ratio near 0.625. freezingRatio3D_band · IndisputableMonolith/CondensedMatter/SpinGlassFreezingRatio.leanHYPOTHESIS 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] nlinaritha survey of at least ten spin glasses with calibrated T_c references should find the median ratio inside (0.61, 0.62) at the 2σ level. freezingRatio3D_band · IndisputableMonolith/CondensedMatter/SpinGlassFreezingRatio.lean