- #1
San K
- 911
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Do we need a coincidence counter (for correlation) in delayed erasure?...in case of repeating the same experiment many times (with one photon at a time) the same way
In the DCQE experiment such as the one listed below
http://grad.physics.sunysb.edu/~amarch/
Notice the polarizer placed before detector Dp. This is used to erase which way information.
Now let's perform the delayed erasure as per the following (same as performed in the link above):
1. We detect S before P
2. Once we have detected S, we place a polarized (eraser) before Dp
3. We repeat this experiment many many times
4. We get an interference pattern, as expected
Now in this case (part of the experiment), do we need the coincidence counter? (for correlating s and p)
I argue we don’t need the coincidence counter because
1. We don’t need to co-relate s and p photons i.e. we don’t’ need to detect the quantum state of the P or S because we are repeating the same sequence of events (i.e. delayed erasure) every time we send a photon pair in a “erased” manner (although delayed)
2. We can remove the “noise” without use of co-incidence counter because we can tell when photon p is expected to arrive at Ds via velocity of light calculations i.e.simply correlate with emission time, however we don’t need to correlated with photon P.
Is the above argument valid? I will then proceed to the next idea/point.
In the DCQE experiment such as the one listed below
http://grad.physics.sunysb.edu/~amarch/
Notice the polarizer placed before detector Dp. This is used to erase which way information.
Now let's perform the delayed erasure as per the following (same as performed in the link above):
1. We detect S before P
2. Once we have detected S, we place a polarized (eraser) before Dp
3. We repeat this experiment many many times
4. We get an interference pattern, as expected
Now in this case (part of the experiment), do we need the coincidence counter? (for correlating s and p)
I argue we don’t need the coincidence counter because
1. We don’t need to co-relate s and p photons i.e. we don’t’ need to detect the quantum state of the P or S because we are repeating the same sequence of events (i.e. delayed erasure) every time we send a photon pair in a “erased” manner (although delayed)
2. We can remove the “noise” without use of co-incidence counter because we can tell when photon p is expected to arrive at Ds via velocity of light calculations i.e.simply correlate with emission time, however we don’t need to correlated with photon P.
Is the above argument valid? I will then proceed to the next idea/point.
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