Killtech
- 344
- 35
No, i have reduced the structure i am querying about to the following two states in a similar 4 beam setup but a different source emitting a different initial state instead of two independent Bell pairs.DrChinese said:'ve lost track of your various examples. But if you are talking about the AB + A'B' setup I commented on in #12: There is no difference in observable outcomes regardless of ordering of observations. That is true of all EPR entanglement setups, especially swapping setups.
But you'll need to read a little more about the following discussion to follow the context, specifically to understand my statement about observable outcomes - since you need to know what what observables are being observed. The issue is that within the formalism the observable in question is technically non-local with the way no-signaling theorems use this word (and therefore failing to commute with observables in either part of the space), albeit it remains is a simple measurement.Killtech said:
- a 2-photon 4 beam entanglement with same polarizations:
|ϕ⟩=|HA,HA′⟩+|HB,HB′⟩
So this case is a mirror experimental setup with a mirror photon state - whichever path one photon chose (A or B), his mirror photon had to do the same but mirrored.- a 4-photon 4 beam Bell state
|ψ⟩=|HA,HA′,VB,VB′⟩+|VA,VA′,HB,HB′⟩
Here the distinction is that the HOM interferences will differ when also taking into account polarization depending on the loss of coherence.
The question moved on how physical such state would be since just because the formalism does allow to write them down doesn't make them necessarily realistic.