Encyclopedia Physics Physics Heat Capacity Anomaly From Jcost
ARTICLE 3 claims 2 theorems 1 model
Physics Heat Capacity Anomaly From Jcost
A proposed link between a recognition cost function and the critical exponent of heat capacity, where the formal proof stops well short of the physics.
The anomaly and its limits
Near a phase transition, the heat capacity of a material often diverges. The standard way to describe this is a power law: C_p ∝ |T - T_c|^(-α), where T_c is the critical temperature and α is the critical exponent. In the simplest mean-field theory, α equals 0, meaning the heat capacity jumps but does not diverge. In the three-dimensional Ising model, a more accurate description of magnetic transitions, α is about 0.110.
Recognition Science proposes a connection. Its cost function, a measure of the forced price of recognition events, has a unique form J(x) = (x + 1/x)/2 - 1. The framework's research note suggests that the critical exponent might be α = J(φ)/2, where φ is the golden ratio. Since J(φ) ≈ 0.118, this gives α ≈ 0.059, a value between the mean-field prediction of 0 and the Ising value of 0.110.
The machine-checked library of formal theorems proves something much narrower. It defines a cost function on a ratio of two real numbers, m and e, as J(m/e). It then proves three general facts: this cost is zero when m equals e, it is never negative for positive inputs, and the golden-ratio constant φ - 3/2 is positive. These are properties of the cost function itself, not of any physical system.
The gap between the physics and the proof is explicit. The library's own documentation states that it proves nothing specific to heat capacity, because the cost function is defined without reference to any particular physical quantities. To become a theorem about critical exponents, the library would need a definition of m and e in terms of the system's actual parameters, such as temperature and energy. That definition does not exist in the formal library.
What the library does establish is a template. It shows that the cost function has the basic mathematical properties one would want for a physical quantity: it vanishes at equilibrium, stays nonnegative, and has a natural threshold. Whether those properties connect to the measured critical exponent remains an open question, not a proved result.
MODEL domainCost · IndisputableMonolith/Physics/HeatCapacityAnomalyFromJCost.lean
def domainCost (m e : ℝ) : ℝ := Jcost (m / e)
THEOREM domainCost_at_eq · domainCost_nonneg · canonicalThreshold_pos · IndisputableMonolith/Physics/HeatCapacityAnomalyFromJCost.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 (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 : 0 < canonicalThreshold := by
unfold canonicalThreshold; linarith [phi_gt_onePointFive]
THEOREM domainCost · IndisputableMonolith/Physics/HeatCapacityAnomalyFromJCost.lean
def domainCost (m e : ℝ) : ℝ := Jcost (m / e)
What this page does not claim
The library proves that the critical exponent α equals J(φ)/2. The value 0.059 is a measured or derived critical exponent for any real material. The cost function is defined in terms of temperature or 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/Physics/HeatCapacityAnomalyFromJCost.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 definitions of m and e would make the cost function a model of a specific phase transition?
- Does the proposed value α = J(φ)/2 ≈ 0.059 match any measured critical exponent within experimental error?
- What regularity conditions on the cost function select the unique form J(x)?
- How does the framework's cost function relate to the free energy in statistical mechanics?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
MODEL domainCost · IndisputableMonolith/Physics/HeatCapacityAnomalyFromJCost.lean
def domainCost (m e : ℝ) : ℝ := Jcost (m / e)It defines a cost function on a ratio of two real numbers, m and e, as J(m/e). domainCost · IndisputableMonolith/Physics/HeatCapacityAnomalyFromJCost.leanTHEOREM domainCost_at_eq · domainCost_nonneg · canonicalThreshold_pos · IndisputableMonolith/Physics/HeatCapacityAnomalyFromJCost.lean
theorem domainCost_at_eq (r : ℝ) (h : r ≠ 0) : domainCost r r = 0 := by unfold domainCost; rw [div_self h]; exact Jcost_unit0theorem 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 : 0 < canonicalThreshold := by unfold canonicalThreshold; linarith [phi_gt_onePointFive]It then proves three general facts: this cost is zero when m equals e, it is never negative for positive inputs, and the golden-ratio constant φ - 3/2 is positive. domainCost_at_eq · domainCost_nonneg · canonicalThreshold_pos · IndisputableMonolith/Physics/HeatCapacityAnomalyFromJCost.leanTHEOREM domainCost · IndisputableMonolith/Physics/HeatCapacityAnomalyFromJCost.lean
def domainCost (m e : ℝ) : ℝ := Jcost (m / e)The library's own documentation states that it proves nothing specific to heat capacity, because the cost function is defined without reference to any particular physical quantities. domainCost · IndisputableMonolith/Physics/HeatCapacityAnomalyFromJCost.lean