 |
 |
 |
 |
 |
 |
 |
 |
 |
 |
 |
 |
| • |
The probability
of a global configuration at
|
|
|
thermal
equilibrium is an exponential
function of
|
|
its energy.
|
|
|
|
– |
So
settling to equilibrium makes the log
|
|
|
probability
a linear function of the energy
|
|
|
| • |
The energy is a
linear function of the weights
|
|
|
and states
|
|
|
| • |
The process of
settling to thermal equilibrium
|
|
|
propagates
information about the weights.
|
|