Larry Pendarvis
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DrChinese said:It is true that an individual particle in a superposition (per A) does not appear different to an observer than a single one from a group of mixed H> and V> (per B). But I am not so sure that a group of such particles cannot be differentiated, assuming they are all from either a stream of A's or a stream of B's. Not sure if that is what you are talking about, but if it is, I think I would disagree.
I am thinking specifically of photon polarization tests and things that you can do with entangled pairs. Specifically: you can provide a light source of indefinite H/V polarization as input to a PDC crystal, and you WILL get some pairs of polarization entangled photons out. If you provide a light source of DEFINITE H/V polarization as input to a PDC crystal, you do NOT get any pairs of polarization entangled photons out. Entangled pairs produce different statistics than ones in a product state. The difference in statistics may not be much though, and might not be enough to measure reliably. Not sure. But that's the concept.
That is intriguing, but my description of (B) did not involve any H>, only V>:
"(B) The scientist knows for a fact that someone has already measured his particles on the vertical axis."
So (B) involves only up and down, no left no right.
Still, it would be interesting to prepare two such ensembles as you describe and see if a PDC crystal can be used to distinguish between an ensemble of definite H/V polarization and an ensemble of indefinite H/V polarization... creating entanglement where there was none, in order to make a measurement. If you can physically distinguish between the two ensembles in this way, it might demonstrate nonlocality without relying on Bell's Theorem, closing all loopholes.
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