Can the result of an optical circuit depend on when you check it?

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Discussion Overview

The discussion revolves around the behavior of optical circuits, particularly whether the outcome can depend on the timing of when the system is checked. Participants explore concepts related to interference, coherence length, and the implications of using time-insensitive detectors in quantum experiments.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant proposes that the outcome of the optical circuit depends on whether the system is checked before or after a certain time, suggesting that checking modifies the state and affects interference.
  • Another participant introduces the concept of coherence length, arguing that checking the detectors too precisely can ruin coherence and prevent interference.
  • A request for clarification on coherence length is made, with a suggestion that increasing the path length could resolve timing issues.
  • One participant asserts that using a light bulb would not yield interference due to the short coherence of photons, whereas a laser would allow for interference.
  • Concerns are raised about the feasibility of creating truly time-insensitive detectors, with speculation that such a detector might violate fundamental principles like reversibility.
  • Another participant argues that the time-reversed process can involve photons with long coherence lengths, suggesting that conventional lasers could work in the proposed setup.
  • Some participants express skepticism about the argument that interference is not possible, asserting that the experiment can yield interference under certain conditions.
  • One participant mentions simulating the system on a computer, noting that their results showed interference without a laser, indicating a potential discrepancy in the theoretical understanding.

Areas of Agreement / Disagreement

Participants express differing views on the impact of timing and detector sensitivity on interference. There is no consensus on whether the proposed optical circuit can yield interference under the conditions described, and multiple competing perspectives remain.

Contextual Notes

Participants discuss various assumptions about detector behavior, coherence length, and the nature of photon interactions, but these assumptions are not universally accepted or resolved within the discussion.

Strilanc
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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:

XPa9r.png


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?
 
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It depends on the coherence length of the photons - and if you check the detectors too precise (if you let the photon interaction time influence their state), you ruin this coherence in time, and don't get interference. If you can check too early, you need detectors with some time-sensitivity.
 
Could you explain what you mean by the coherence length of the photons? It seems like just making the long path a lot longer would fix any issue with arrival times not being exact.
 
See wikipedia or any physics book about quantum mechanics.
With a light bulb, your experiment will never give interference - as a simplified model, the photons are "too short" to interfere. With a laser, interference in this setup is possible.
 
You're saying the states resulting from earlier photon arrivals don't interfere with the states resulting from later photon arrivals, I think. That would mean they must be different states.

Is it simply not possible in reality to make a detector that is truly time-insensitive (until you check it)? I feel like it should be workable in magic idealized abstraction land, unless it violates something fundamental like reversibility. Come to think of it... given the 100% triggered detector you can't go backwards to the photon being emitted. So, maybe it does violate reversibility and the issue is the detectors being impossible.
 
The time-reversed process is a photon with long coherence length as well.
It is possible in the mm-range (and probably more) with conventional lasers, I don't see a fundamental problem with the setup. You have to use a laser.
 
mfb said:
The time-reversed process is a photon with long coherence length as well.
It is possible in the mm-range (and probably more) with conventional lasers, I don't see a fundamental problem with the setup. You have to use a laser.

Yes, it would work with a laser, but with the impossible detectors even a single photon would have interfered with itself.
 
I don't see the argument. The experiment is possible, you can get interference. Where is the problem?
 
mfb said:
I don't see the argument. The experiment is possible, you can get interference. Where is the problem?

Simulating the system correctly on a computer. I wrote a simple program but it had detectors like what I was describing, so I was seeing interference without a laser.
 

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