piezas said:
BTW, looking at the extensions of the Dopfer experiment I couldn't see why observing the photon on 'the short arm' wouldn't break down the entanglement of the photon on the long arm before it is observed. It seems that if the lens position is shifted to a length longer than that of the short arm to the screen, the difference is explainable by the entanglement breaking on the short arm. I may be reading it wrong.
I think that observing one of two entangled photons does not break the entanglement. It just causes collapse of the wavefunction for that photon. The only way you may ever verify that there is such a thing as entanglement between two photons is by making measurements on each and after comparing the results finding that there is a correlation. You can visualize this easily with an EPR-type setup that involves two spin-1/2 particles. If you always find that when you measure the second particle, it's spin is the opposite than that of the first, then there is entanglement. You can measure the spins with a Stern-Gerlach apparatus on each end. The Stern-Gerlach apparatus does not force the spin to be up or down, it just picks one of the two possible values from the superposition.
I think you are confusing destruction of entanglement with collapse of the wave function.
In the combined Hilbert space of the two particles, you get a collapse to one of the two possible spin combinations. But these combination still complies with the correlation determined by the entanglement. Now, going back to Dopfer's experiment. Measurement at D2 is done in such a way that you don't know by which slit the photon passed. So we could say that (ignoring whatever happens to the other photon) you have a superposition of states, each corresponding to the photon going through each slit. If, on the other hand you set D2 in such a way that you can detect which slit the photon went through, then you are
collapsing the superposition. If that is the case, then the other photon will also be collapsed to having gone through one of the two slits but not both. But this is not the way the Dopfer's experiment is constructed, in that experiment, you don't detect which-way information on D2.
The function of the lens in arm 1, is a little tricky. Paul Friedlander explains quite well how that works. So if you position detector D1 in the correct place, you can find out which slit the first photon went through. So this apears as a contradiction, and it is here where different people explain it differently.
Cramer says that if arm 1 is very long, then you can effectively choose after the fact, which slit the first photon went through. So this would be "retrocausality". According to him, if you position D1 in such a way that you don't detect which-way information, then you'll see an interference pattern in D2. (Of course interference patterns appear only after a few photons have been detected). I personaly doubt it that retrocausality could be the cause for this behavior.
Zeilinger on the other hand, says that because it is possible to eventually determine which-way information using the photon on arm 1, then you'll never see an interference pattern in D2. I don't find this argument very convincing either.
Those who say that you would never see an interference pattern in D2 explain the fact that you do in fact see it in Dopfer's experiment, by saying that the coincidence counter is what makes the pattern appear. I haven't see any convincing evidence that this is the case.
I do think that in Dopfer's experiment the difference in length between the arms is not enough and that could be a loophole, as signals traveling at the speed of light could travell from one detector to the other before each measurement is finished. (it takes a finite time for each detector to "click")