miosim said:
I mean the angle between observable photons’ polarization (parallel, antiparallel or anything in between).
I just realized that I made a mistake that causes a major confusion.
While asking about observable polarization of the photon’s pair after one of them passed 90 deg wave plate I thought that antiparallel polarization means 180 degree, while 90 degree represents the middle point between parallel and antiparallel polarization. But I was wrong because 90 degree is difference between parallel and untiparalell polarization so 45 degree is a middle point.
I am sorry for this confusion.
Let me correct my previous question. What happens if one of the entangled photons passed 45 deg wave plate? Would the observable polarization of this photon's pair remain antiparallel or will be shifted by 45 degree?
This question is ill-defined. All that you can talk about are the following experimental parameters:
1) The settings of the detectors at A & B (i.e. the angle at which you set your polarizer).
2) Manipulations of the beams going to A and/or B (i.e. optical elements, including those that may rotate the polarization)
3) Statistics of detection events, either detector-local (i.e. only considering the detection statistics at A or B individually) or coincident (i.e. considering the correlations between time-coincident detections at both detectors).
The language that you use suggests that you think it makes sense to talk about "the polarization of an entangled photon" in between the point where it was generated, and the point where it was detected. In my opinion, such statements have no scientific basis.
So, let's modify your gedanken experiment. Let's talk about a setup where the "detectors" at A & B are actually polarizing beam splitters, each with two detectors that detect the polarization states |H> and |V>. Let us further assume that these are 100% efficient, so that each of the photons coming through is guaranteed to be detected at one of the detectors. Our entangled pairs are being generated by type II parametric down conversion, so that the polarizations of the two photons are anti-correlated in the |H> and |V> basis, corresponding to the entangled wavefunction:
\Psi=(|H_A>\otimes|V_B> + |V_A>\otimes|H_B>)
We start our experiment with both the A & B detectors aligned to detect in the same basis (i.e. |H>=|H
A>=|H
B>, etc.). In this configuration, we will find that each individual detector sees a 50-50 split between |H> and |V> detection events, and there is perfect anti-correlation between the coincidence measurements ... that is, if for a particular entangled pair the |H
A> detector clicks, then the |V
B> detector will also click, and vice-versa.
Now say that we put a 45 degree rotation on the polarization of the A beam. The statistics of the individual detections will not change .. i.e. each detector will still see a 50-50 split between |H> and |V>. However the coincident statistics for pairwise detection will be drastically different. In fact, you will find NO correlation for coincident detections. In other words, when |H
A> is detected, you will have an equal chance of observing |H
B> or |V
B> for that pair. This is in agreement with the predictions of Q.M., and with Malus' Law.
It is important to note that the loss of correlation in the coincidence statistics in the above example is due to the specific choice of 45 degrees as the rotation angle. If you choose a different rotation angle, you will measure coincidence statistics that are somewhere between perfectly anti-correlated and uncorrelated (i.e. random), with the precise coincidence rate given by Malus' law, with theta as the difference between the rotation angle, and the angle of the polarizing beam-splitter.
I suspect that most of this has already been laid out in this thread, but perhaps not in this form, and at the very least not for several pages

. Hopefully this will help clear up some of the confusion.