Rigid System (Low Temperature)
Ω = 0.05
Position
0.250
C / Ω
0%
Ruptures
0
Changes
0
Fluid System (High Temperature)
Ω = 0.80
Position
0.250
C / Ω
0%
Ruptures
0
Changes
0
Low Ω: Rigid Dynamics
With low temperature, the exp(C/Ω) weighting becomes sharply peaked. Only the highest-coherence moments dominate regeneration.
The system ruptures frequently but most ruptures reconstitute the same patterns—many ruptures, low success rate per rupture.
exp(C/Ω) with small Ω → peaked weighting
Only recent/strongest memories count
Only recent/strongest memories count
High Ω: Fluid Dynamics
With high temperature, the exp(C/Ω) weighting becomes flat. The full breadth of accumulated history informs regeneration.
Ruptures are rare, but when they occur, genuine transformation is far more likely—fewer ruptures, high success rate per rupture.
exp(C/Ω) with large Ω → flat weighting
Entire history contributes equally
Entire history contributes equally