Jilang said:
If you have time could you expand on this a bit more. I'm very interested in the Born postulate and would love to have a better understanding of it. As it's defined it looks like a joint probability to me rather than a probability of a single entity. The similarity in its form to probability of transitions between the initial and final states and interactions has an implication that I'm trying to understand.
This is just fooling around with symbols, but...
The probability amplitude to go from state [itex]| A\rangle[/itex] at time [itex]t[/itex] to state [itex]|B\rangle[/itex] at time [itex]t + \delta t[/itex] is given by:
[itex]\langle A | e^{-i H \delta t/\hbar} | B \rangle[/itex]
If we assume that this formula works when [itex]\delta t < 0[/itex], then the probability amplitude for going from state [itex]| B \rangle[/itex] at time [itex]t + \delta t[/itex] to state [itex]|A\rangle[/itex] at time [itex]t[/itex] is given by:
[itex]\langle B | e^{+i H \delta t/\hbar} | A \rangle[/itex]
So the amplitude for going from [itex]| A\rangle[/itex] to [itex]|B\rangle[/itex] and back in time to [itex]| A\rangle[/itex] would be the product:
[itex]\langle A | e^{-i H \delta t/\hbar} | B \rangle\langle B | e^{+i H \delta t/\hbar} | A \rangle = |\langle A | e^{-i H \delta t/\hbar} | B \rangle|^2[/itex]
which is the Born expression for the probability of going from [itex]| A\rangle[/itex] to [itex]|B\rangle[/itex].
So, mathematically, the probability of going from [itex]| A\rangle[/itex] to [itex]|B\rangle[/itex] is the probability
amplitude of making a "round-trip" back to the starting point (and starting time).