Christoph,
I am enjoying your fascinating paper. Nice to see something with some predictions!
I have a few questions about entanglement.

From your book, circa pages 176/177:
"A second example is the entanglement of two photons, the well-known Aspect experiment. Also in this case, entangled spin 0 states, i.e., entangled states of photons of opposite helicity (spin), are most interesting. Again, the strand model helps to visualize the situation.We use the strand model for the photon that we will deduce later on. Figure 32 shows the strand model of the two separable basis states and the strand model of the entangled state. Again, the measurement of the helicity of one photon in the entangled state will lead to one of the two basis states. And as soon as the helicity of one photon is measured, the helicity of its companion collapses to the opposite value, whatever the distance! Experimentally, the effect has been observed for distances of many kilometres. Again, despite the extremely rapid collapse, no energy travels faster than light. And again, the strand model completely reproduces the observations."
OK, I think I follow this. The strands are connected, the basis change instantaneous. Nice. But entanglement has some funny properties, and I would like to extend this example a bit to flesh that out if that is acceptable.
So we have Alice and Bob, several kilometers apart. At any polarizing beam splitter (PBS) angle setting they choose which is identical, their results (in an ideal world) will be perfectly correlated. We are in agreement here, and I will call this the i) case. Time stamps are made of arrivals at Alice and Bob's detectors, and suitable pairs within a suitable coincidence window will be considered only. This technique will be used in all cases discussed here, regardless of how many are seen in any period of time. All we care about is the percentage of correlations, not the absolute number. Alice and Bob hold their angle settings fixed in all cases below.
i) With suitable choice of settings, the correlation is 100%. Bell inequalities are also violated, showing that the photon pair is not only EPR entangled but also violates Bell inequalities (and local realism).
Now, I insert a black box in Alice's path, but not Bob's. I have in fact 2 black boxes which do 2 different things, which I will label cases ii) and iii) below. Again, in all cases, I will make note of time stamps of arrivals at Alice and Bob - considering that the distances traveled may not be equal but we will always calibrate so that proper pairs are matched.
ii) My black box contains a PBS - set 45 degrees offset from Alice - so that one channel is detected there and the other channel is passed on through the black box to Alice. I know which path the photon takes because it either clicks a photodetector or passes through. Obviously, only half the photons make it through to but that will not matter to the final observed number as we are only concerned with correlation percentages. Because we measure 45 degrees offset, we maximally destroy the entanglement and our correlation percentage falls to 50% (coincidences between Alice and Bob). There is no EPR entanglement and no violation of Bell inequalities.
As I understand the strand model, this makes perfect sense. At the time the black box is encountered, the measurement of the helicity via the PBS in the black box causes the normal collapse and the photons are no longer entangled. Because I know which path the photon took to get to Alice, the results of Alice and Bob's measurements are no longer entangled.
iii) Same as case ii) above except: I don't bother to detect which path the photon went through before I send it on to Alice. In fact, I make sure that the 2 paths coming out of the Black Box PBS are exactly equal (but suitably phase matched so the path taken is no longer knowable) but they go in different directions before I finally route them out of the Black Box and on to Alice. In other words, knowledge of the path taken inside the black box PBS is quantum erased. (Of course this is an ideal world, in practice not so easy.)
In such case, I believe Alice and Bob will see full entanglement just as in case i). The correlation will be 100% as before in case i).
As I understand the strand model, the act of having the basis state measured by the PBS in the black box ends the entanglement. There is no further connection between the 2 photons eventually seen by Alice and Bob. So my question is: how does putting Alice's "2 halves back together again" change Bob so that Bob is once again entangled with Alice? Seems to me that Bob is now happily on his merry way. Obviously, you would in practice perform a Bell test to see if the Inequality is violated while also checking to see that perfect EPR correlations are seen.
I don't see how the strand model would yield the correct expected results. How could the Alice and Bob strands get hooked up again? Seems like something would need to move along both paths (half entangled tangles?) so they could merge together later - but that makes no sense to me. Any comments? If my example is not clear, I can put together a diagram to help.