IndisputableMonolith.Thermodynamics.PhaseTransitions
This module defines the J-cost as a function of order parameter m and temperature T, together with the associated landscape, first-order and second-order transition mechanisms, and critical-point ratios. RS statistical mechanicians cite it when extending the T=0 J-minimization foundation to finite-temperature phase structure. The module consists of a collection of definitions and short lemmas that build directly on the imported Cost and PhiForcing primitives.
claimThe central object is the J-cost landscape $J(m,T)$ for order parameter $m$ and temperature $T$, with a phase transition located at critical temperature $T_c$, first-order transition mechanism, second-order transition mechanism, and critical ratios governing spontaneous symmetry breaking.
background
Recognition Science begins from the absolute minimization of the universal cost functional $J(x) = rac12(x + 1/x) - 1$ at $T=0$. The present module extends this cost to finite temperature by introducing an order parameter $m$ and studies the resulting phase structure. It imports the RS time quantum $ au_0 = 1$ tick from Constants, empirical calibration quarantine from ExternalAnchors, the J-cost definition from Cost, and the self-similar forcing of $\phi$ from PhiForcing.
proof idea
This is a definition module, no proofs. It introduces the J-cost landscape, positivity statements for $T>1$, the location of the transition at $T_c$, the two transition mechanisms, the critical-point object, and example order-parameter constructions, all as direct definitions or one-line wrappers around the imported J and $\phi$ primitives.
why it matters in Recognition Science
The module supplies the finite-temperature phase-transition layer required by the parent Thermodynamics module, which develops the full statistical mechanics of Recognition Science from the T=0 J-minimization foundation. It thereby completes the bridge from the phi-forced discrete ledger to observable thermodynamic behavior.
scope and limits
- Does not derive an explicit closed-form expression for $J(m,T)$ from the RCL.
- Does not identify $m$ with any particular physical order parameter such as magnetization.
- Does not compute numerical values of $T_c$ or critical ratios from external data.
- Does not address dynamical evolution across the transition.
used by (1)
depends on (4)
declarations in this module (20)
-
def
jcostLandscape -
theorem
jcost_at_zero -
theorem
jcost_positive_for_T_gt_1 -
theorem
phase_transition_at_Tc -
structure
FirstOrderTransition -
theorem
first_order_mechanism -
structure
SecondOrderTransition -
theorem
second_order_mechanism -
structure
CriticalPoint -
theorem
critical_ratios -
def
orderParameterExamples -
theorem
spontaneous_symmetry_breaking -
def
ssbMechanism -
structure
MetastableState -
def
nucleationRate -
structure
QuantumPhaseTransition -
def
qptExamples -
structure
TopologicalTransition -
def
summary -
structure
PhaseTransitionFalsifier