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I'm trying to understand how optical circuits behave. In particular, if they can interfere "across time". Consider this optical circuit:
Suppose that it is completely isolated from the outside world (until we check it), and that the detectors are time-insensitive (they record IF a photon was received, not WHEN it was received [even implicitly]). Call the time it takes for a photon to follow the bottom branch ##t_{1}## and the time it takes for a photon to follow the top branch ##t_{2}##.
Does the outcome of this circuit depend on whether or not we check it (un-isolate it) before or after ##t_{2}##? From what I understand, it does, but this seems counter-intuitive. Let me go through the math.
At ##t_{1}## the state of the system should be this:
##\frac{-1}{2} RightDetector + \frac{-i}{2} BottomDetector + \sqrt{\frac{1}{2}} i^{MirrorsHit} TopPath##
If we don't un-isolate the system at this point, then at ##t_{2}## the system will have reached this state:
##(\frac{-1}{2} RightDetector + \frac{-i}{2} BottomDetector) + (\frac{-i}{2} BottomDetector + \frac{1}{2} RightDetector)##
Since the detectors aren't time-sensitive, the time the photon arrived doesn't matter and the photon-arriving-at-##t_{1}## states interfere with the photon-arriving-at-##t_{2}## states, giving:
##= -i BottomDetector##
So if we only check after ##t_{2}## then we should see that the bottom detector has gone off 100% of the time.
But, going back to the state at ##t_{1}##:
##\frac{-1}{2} RightDetector + \frac{-i}{2} BottomDetector + \sqrt{\frac{1}{2}} i^{MirrorsHit} TopPath##
If we check the system now, we modify its state into the following:
##\frac{-1}{2} InitiallySawRightDetector + \frac{-i}{2} InitiallySawBottomDetector + \sqrt{\frac{1}{2}} i^{MirrorsHit} TopPath##
and it will evolve into the following state at ##t_{2}##:
##\frac{-1}{2} InitiallySawRightDetector + \frac{-i}{2} InitiallySawBottomDetector + \frac{-i}{2} LaterSawBottomDetector + \frac{1}{2} LaterSawRightDetector##
These states are different, because of our meddling, so they don't interfere. In this case we expect the bottom detector to have gone off 50% of the time by the end of the experiment (25% initially, 25% later) and the right detector to have gone off the other 50% of the time (also 25% initially, 25% later).
Is this analysis correct? Do the right detector states actually get erased after the fact, if we haven't checked to make sure they don't?
Suppose that it is completely isolated from the outside world (until we check it), and that the detectors are time-insensitive (they record IF a photon was received, not WHEN it was received [even implicitly]). Call the time it takes for a photon to follow the bottom branch ##t_{1}## and the time it takes for a photon to follow the top branch ##t_{2}##.
Does the outcome of this circuit depend on whether or not we check it (un-isolate it) before or after ##t_{2}##? From what I understand, it does, but this seems counter-intuitive. Let me go through the math.
At ##t_{1}## the state of the system should be this:
##\frac{-1}{2} RightDetector + \frac{-i}{2} BottomDetector + \sqrt{\frac{1}{2}} i^{MirrorsHit} TopPath##
If we don't un-isolate the system at this point, then at ##t_{2}## the system will have reached this state:
##(\frac{-1}{2} RightDetector + \frac{-i}{2} BottomDetector) + (\frac{-i}{2} BottomDetector + \frac{1}{2} RightDetector)##
Since the detectors aren't time-sensitive, the time the photon arrived doesn't matter and the photon-arriving-at-##t_{1}## states interfere with the photon-arriving-at-##t_{2}## states, giving:
##= -i BottomDetector##
So if we only check after ##t_{2}## then we should see that the bottom detector has gone off 100% of the time.
But, going back to the state at ##t_{1}##:
##\frac{-1}{2} RightDetector + \frac{-i}{2} BottomDetector + \sqrt{\frac{1}{2}} i^{MirrorsHit} TopPath##
If we check the system now, we modify its state into the following:
##\frac{-1}{2} InitiallySawRightDetector + \frac{-i}{2} InitiallySawBottomDetector + \sqrt{\frac{1}{2}} i^{MirrorsHit} TopPath##
and it will evolve into the following state at ##t_{2}##:
##\frac{-1}{2} InitiallySawRightDetector + \frac{-i}{2} InitiallySawBottomDetector + \frac{-i}{2} LaterSawBottomDetector + \frac{1}{2} LaterSawRightDetector##
These states are different, because of our meddling, so they don't interfere. In this case we expect the bottom detector to have gone off 50% of the time by the end of the experiment (25% initially, 25% later) and the right detector to have gone off the other 50% of the time (also 25% initially, 25% later).
Is this analysis correct? Do the right detector states actually get erased after the fact, if we haven't checked to make sure they don't?