Encyclopedia Condensed Condensed Matter Jcost Phase Transition
ARTICLE 5 claims 4 theorems 1 model
Condensed Matter Jcost Phase Transition
A single mathematical function, born from bookkeeping rules, predicts a narrow window for superconducting transition temperatures.
The cost of recognition
The J-cost function is a specific mathematical formula. It takes any positive number x and returns a non-negative number that measures how far x is from 1. The function reaches its minimum value of zero exactly at x = 1, and it grows as x moves away from 1 in either direction. This function is symmetric: J(x) equals J(1/x), so it treats a number and its reciprocal identically.
The function has a long history in mathematics as a measure of multiplicative distance. The expression (x + x⁻¹)/2 is the arithmetic mean of a number and its reciprocal, and subtracting 1 shifts the minimum to zero. The function is also equal to (x − 1)²/(2x), a form that makes its positivity obvious. This identity appears in the machine-checked library of formal theorems that the Recognition Science framework uses to verify its claims.
In Recognition Science, this cost function is not arbitrary. The framework derives it from five plain conditions on how a ledger, a discrete record of events, must account for recognition. The framework's library proves that any cost function satisfying those conditions must equal J(x). The framework then identifies the golden ratio φ, approximately 1.618, as the unique self-similar scaling. At this special value, the cost function takes a value between 0.09 and 0.12, which the framework treats as a critical energy scale.
The condensed matter module applies this scale to superconductivity. It defines a critical temperature T_critical as this energy scale multiplied by 1000, and it proves that this temperature lies strictly between 80 and 120 Kelvin. The module also defines a superconducting gap scale as the coherence energy times φ². The framework's library proves these bounds as formal theorems, not as empirical observations.
The module makes a falsifiable prediction: superconducting materials with lattices structured by the golden ratio will show critical temperatures around 80 to 120 Kelvin when the coherence energy matches about 0.09 electron volts. It also predicts optimal doping occurs at a carrier density near 1/φ², roughly 0.38 per unit cell. These predictions are testable in the laboratory, which is what separates a hypothesis from a mere definition.
MODEL J_cost · IndisputableMonolith/CondensedMatter/JCostPhaseTransition.lean
/-- The canonical J-cost function: J(x) = (x + x^(-1))/2 - 1 -/
noncomputable def J_cost (x : ℝ) : ℝ := (x + x⁻¹) / 2 - 1
THEOREM J_cost_minimum_at_one · IndisputableMonolith/CondensedMatter/JCostPhaseTransition.lean
theorem J_cost_minimum_at_one : J_cost 1 = 0 := by
unfold J_cost
norm_num
THEOREM J_cost_symmetric · IndisputableMonolith/CondensedMatter/JCostPhaseTransition.lean
theorem J_cost_symmetric (x : ℝ) (hx_pos : 0 < x) : J_cost x = J_cost (x⁻¹) := by
simp only [J_cost, inv_inv]; ring
THEOREM phi_critical_numeric · IndisputableMonolith/CondensedMatter/JCostPhaseTransition.lean
theorem phi_critical_numeric : 0.09 < phi_critical_energy ∧ phi_critical_energy < 0.12 := by
rw [phi_critical_value]
have hphi_inv : phi⁻¹ = phi - 1 := by
have hne : phi ≠ 0 := phi_pos.ne'
have hsq := phi_sq_eq
field_simp at hsq ⊢
nlinarith [phi_pos]
rw [hphi_inv]
have h1 := phi_gt_onePointSixOne
have h2 := phi_lt_onePointSixTwo
constructor <;> linarith
THEOREM sc_prediction · IndisputableMonolith/CondensedMatter/JCostPhaseTransition.lean
/-- **FALSIFIABLE PREDICTION**: Superconducting materials with phi-structured
lattices will show critical temperatures T_c ~ 80-120 K when the coherence
energy E_coh matches phi^(-5) ~ 0.09 eV. This predicts optimal doping
occurs at carrier density n ~ 1/phi^2 ~ 0.38 per unit cell. -/
theorem sc_prediction : 80 < T_critical ∧ T_critical < 120 := by
unfold T_critical
rw [phi_critical_value]
have hphi_inv : phi⁻¹ = phi - 1 := by
have hne : phi ≠ 0 := phi_pos.ne'
have hsq := phi_sq_eq
field_simp at hsq ⊢
nlinarith [phi_pos]
rw [hphi_inv]
have h1 := phi_gt_onePointSixOne
have h2 := phi_lt_onePointSixTwo
constructor <;> nlinarith
What this page does not claim
This module does not prove that any real superconductor exists with a golden-ratio lattice structure. The prediction of 80 to 120 Kelvin does not specify which chemical elements or compounds will exhibit this behavior. The framework's derivation of the cost function does not itself establish the physical bridge between recognition and condensed matter.
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/JCostPhaseTransition.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 supports the prediction of critical temperatures near 100 Kelvin?
- How does the coherence energy E_coh relate to measurable properties of a material?
- What does the golden ratio structure of a lattice look like in real materials?
- Can the framework's derivation of J from ledger conditions be extended to other physical systems?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
MODEL J_cost · IndisputableMonolith/CondensedMatter/JCostPhaseTransition.lean
/-- The canonical J-cost function: J(x) = (x + x^(-1))/2 - 1 -/ noncomputable def J_cost (x : ℝ) : ℝ := (x + x⁻¹) / 2 - 1The J-cost function is J(x) = (x + x⁻¹)/2 − 1. J_cost · IndisputableMonolith/CondensedMatter/JCostPhaseTransition.leanTHEOREM J_cost_minimum_at_one · IndisputableMonolith/CondensedMatter/JCostPhaseTransition.lean
theorem J_cost_minimum_at_one : J_cost 1 = 0 := by unfold J_cost norm_numThe function reaches its minimum value of zero exactly at x = 1. J_cost_minimum_at_one · IndisputableMonolith/CondensedMatter/JCostPhaseTransition.leanTHEOREM J_cost_symmetric · IndisputableMonolith/CondensedMatter/JCostPhaseTransition.lean
theorem J_cost_symmetric (x : ℝ) (hx_pos : 0 < x) : J_cost x = J_cost (x⁻¹) := by simp only [J_cost, inv_inv]; ringThe function is symmetric: J(x) equals J(1/x). J_cost_symmetric · IndisputableMonolith/CondensedMatter/JCostPhaseTransition.leanTHEOREM phi_critical_numeric · IndisputableMonolith/CondensedMatter/JCostPhaseTransition.lean
theorem phi_critical_numeric : 0.09 < phi_critical_energy ∧ phi_critical_energy < 0.12 := by rw [phi_critical_value] have hphi_inv : phi⁻¹ = phi - 1 := by have hne : phi ≠ 0 := phi_pos.ne' have hsq := phi_sq_eq field_simp at hsq ⊢ nlinarith [phi_pos] rw [hphi_inv] have h1 := phi_gt_onePointSixOne have h2 := phi_lt_onePointSixTwo constructor <;> linarithAt the golden ratio, the cost function takes a value between 0.09 and 0.12. phi_critical_numeric · IndisputableMonolith/CondensedMatter/JCostPhaseTransition.leanTHEOREM sc_prediction · IndisputableMonolith/CondensedMatter/JCostPhaseTransition.lean
/-- **FALSIFIABLE PREDICTION**: Superconducting materials with phi-structured lattices will show critical temperatures T_c ~ 80-120 K when the coherence energy E_coh matches phi^(-5) ~ 0.09 eV. This predicts optimal doping occurs at carrier density n ~ 1/phi^2 ~ 0.38 per unit cell. -/ theorem sc_prediction : 80 < T_critical ∧ T_critical < 120 := by unfold T_critical rw [phi_critical_value] have hphi_inv : phi⁻¹ = phi - 1 := by have hne : phi ≠ 0 := phi_pos.ne' have hsq := phi_sq_eq field_simp at hsq ⊢ nlinarith [phi_pos] rw [hphi_inv] have h1 := phi_gt_onePointSixOne have h2 := phi_lt_onePointSixTwo constructor <;> nlinarithThe critical temperature lies strictly between 80 and 120 Kelvin. sc_prediction · IndisputableMonolith/CondensedMatter/JCostPhaseTransition.lean