| Detailed Balance |
|
|
|
|
|
|
|
| • | When a Boltzmann
machine reaches thermal |
|||||
| equilibrium, the
asymmetric transition |
||||||
| probabilities
between any pair of global |
||||||
| configurations,
A, B, are balanced by the relative |
||||||
| probabilities of
those configurations: |
||||||
| A |
| B |