From the last part of 4.2
> Here's how it works. We send a pair of EPR photons through a pair of two-slit
apparati each of which has a polarization rotator on one of the slits. On one side
of the apparatus (side A) we install a polarization filter which filters out
interference on that side and makes it visible. We can filter out interference on
the other side (side B) of the apparatus as follows: on side A we keep a record of
which photons passed through the filter and which were reflected. On side B we
keep a record of where each photon landed on the screen. We then take these
two records and combine them: for each photon that was passed through the
filter on side A, we take the corresponding photon on side B and note where it
landed on the screen. The end result is a (visible) interference pattern. It was
there all along, but the only way we can filter it out so we can see it is to combine
information from both sides of the experiment. And that is the last nail in the
coffin of superluminal communication via entangled photons.
Let's suppose you are in lab B and measure where the photons hit the screen. There are no visible interference patters. But just before you call to lab A, it's is nuked from orbit.
Now, you are unsure if the people that was generating the photons were sending pairs of entangled photons to A and B, or they were just sending pairs of normal photons.
Can you look at the data you collected in B and discover what the people in the generator were doing?
Now imagine the same experiment with a rebuild lab A', but you remove the polarization rotator. Now you see the interference pattern. And A' gets nuked again. Can you look at the data you collected in B and discover what the people in the generator were doing?
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I understand that you can take a plane and collect all the pieces of A and A' are reconstruct them, after all Classic Mechanics and Quantum Mechanics without the measurement rule are reversible, so it's theoretically possible, but very impractical.
I think this discussed in section 5. For the measurement problem, I prefer the something-something-decoherence solution. I call it something-something-decoherence because there are still a lot of work to be done before it's clear if it's the correct solution.
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About the experiment in 4.2:
I'm 99% sure after adding the polarizer at 45° there will not be interference. You can split the polarizer into two smaller polarizers with the same angle, one for each slit. The exchange the order of the rotator+polarizer in one slit to polarizer+rotator. Note that after the exchange, the new polarizer must be rotated 90°, so it's polarizer at "-45°". Now the first thing in one slit is a polarizer at "+45°" and the other is at "-45°", so they will select orthogonal states and not get interference even after rotating one of them.
I think this can be fixed using a quarter-wave plate, but the calculation is slightly more complicated.
[Sorry for the delay.]