- #36
gptejms
- 386
- 2
marlon said:So basically a propagator expresses the probability that a particle with positive energy created in x' on t' will propagate to place x on time t. This is valid for t > t'. If t < t', then the propagator expresses the probability that a particle with negative energy created in x' on t' will propagate BACKWARDS in time to x on some time t. It is the SUM of both these probability-amplitudes that is relativistically invariant !
Can you write down the propagator(math. expression) for Dirac field and then explain each term