Originally posted by subtillioN
What do you mean when you say "forced"? Do you actually see something different happen to the other meson?
It is not something you can "see" directly, especially because we are talking about the effect on the unmeasured side. However, the behavior you find is just as predicted by QM, with its "collapse" and all.
This is somewhat difficult to explain without the math (Fourier analysis in particular). I don't have much time now, but I'll try to come back with some illustration of it.
Or do you mean that its flavor was indeterminate until the moment of the collapse?
The moment you measure the flavor of one, the other collapses into the opposite flavor. It is not just a matter of our knowledge.
If the latter then how do we know it wasn't already this flavor before its partner was measured?
Because QM says so :)
No, really. Because if we decided to measure something else, then the other side would show a different behavior, which is incompatible with that of a different measurement selection[/color].
Remember I mentioned the article by Mermin? I wrote to him and got the reference:
``Hidden Variables and the Two Theorems of John Bell'', Revs. Mod. Phys. 65, 803-815 (1993).
I'll try to summarize the main idea here later.
How does one measure "flavor"?
It basically means determining if the particle was a B0 or an anti-B0. The difficulty arises from two factors: 1. both are neutral states (hence no trace left, and it decays in the same number of positive and negative particles), and 2. They oscillate into each other!
Can you give me a time breakdown of this experimental procedure?
Here's a link to a http://hep.ph.liv.ac.uk/babar/talks/Durham.pdf. I know it is a bit technical and sketchy, but it may be helpful (also, it includes something about the detectors and analysis). Look at page 13 (21 has a sketch also).