If you want to simulate what a photon does, then at the moment that the "emission" occurs, you need to capture all the information about what that photon can encounter in every possible direction it could be following. So, using that
Mach-Zehnder interferometer experiment I mentioned before, what is important is not whether the block was there at the moment of emission, but whether it would be there when the photon would reach that point in any of its potential trajectories.
It's as if: 1) all of that information is collected at the moment of emission; 2) the interference pattern is calculated; and 3) a random destination is picked weighted by the values in the interference pattern.
But, in all cases, the absorption will occur an amount of time after the emission that is determined by the time it takes light to follow that randomly selected path.
Part of
@Dale response to you (
@spacecadet2563 ) was this:
In light of
@Dale's statement, let's consider the
speed of neutrinos. It was originally thought that neutrinos were massless and that they therefore must travel at the speed of light. But,
about 25 years ago, experiments by Takaaki Kajita and Arthur B. McDonald showed that neutrinos change during flight. They "oscillate" among their three possible neutrino flavors as they cruise through the universe. Well, they can't do that without proper time. Proper time must be defined for them - and holding to the commonly held presumption that they are not interacting with anything in flight, that would mean those neutrinos must have non-zero mass.
So the fact that photons have no proper time is a more significant statement than it might first appear. It means that photons can't change in flight. The end result is as if they follow those superposition of paths and ultimately land on some select destination - but that entire process isn't an evolution of the photon - it is just a single emission/absorption process.
I would guess that if someone said that "time does not move for a photon", they were likely alluding to this characteristic of massless particles. But as you can see, it's really not that simple. And trying to describe it is also not simple because our language is tuned for describing how classical objects move through Newtonian space and time.