A large \ scriptstyle { v _ { LZ } } results in a large diabatic transition probability and vice versa.
32.
However, using the other interfaces between the states, one can rewrite the flux in terms of transition probabilities between interfaces
33.
Precise expressions for the transition probability, based on first-order perturbation Hamiltonians, can be found in Thompson and Baker.
34.
The transition probabilities control the way the hidden state at time is chosen given the hidden state at time t-1.
35.
The diabatic transition probability can still be obtained using one of the wide variety of numerical solution algorithms for ordinary differential equations.
36.
Comparison of the initial conditions used with the values of the state amplitudes following the transition can yield the diabatic transition probability.
37.
The RSM decides whether the reaction of the selected molecule proceeds or not by comparing the transition probability with a random number.
38.
A set of rules ( transition probabilities ) are then applied to these units leading to simulated changes in state and behaviour.
39.
The real transition probability is many orders of magnitude higher than the virtual transition one, which is called resonance enhanced effect.
40.
In order to apply the IIT formalism to a system, its full transition probability matrix ( TPM ) must be known.
