- #36
Varon
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Fredrik said:I'm sure that's how people were thinking at the time of (3) and (4), but it's not implied by the theory we ended up with. I'm not sure if that was already clear at step (8), but it certainly is in many modern textbooks. See e.g. this definition of QM. It certainly leaves the door open for an ensemble interpretation.
Maybe we should blame it on Born. He was the one who proposed that the amplitude square is the probability of A PARTICLE being there. Had Born not been born and you took his place. Maybe the world of QM interpretations would be less chaotic (assuming you are correct).
I don't know how you can say that it didn't make sense, but I can also tell that you read me wrong. You're saying that I said that the CI is QM without the assumption that a wavefunction describes all the properties of a single system. I didn't say that. I've been saying that a) there's no standard definition of the CI, b) everyone seems to include that assumption as a part of their definition of the CI, and c) I would prefer not to, since that assumption is what introduces the measurement problem. If we do include it, the CI is (very likely) logically inconsistent, and I don't see the point of assigning a name to something that's logically inconsistent.
I have to get some sleep, so I won't be answering any more posts for at least 8 hours.
What I should have said was "Now I'm perplexed how you could say CI SHOULD BE just QM without the wave function assumption as this is part of the history of QM". When you wake up. Pls. explain why you said that if we do include the assumptions, the CI is (very likely) logically inconsistent.. are you referring to collapse which conflicts with the deterministic development of the Schroedinger Equation?
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