- #736
akhmeteli
- 805
- 38
It is not obvious that b_i is an eigenvalue, not an eigenstate. While b_i was defined earlier in the text, it was defined as an expansion coefficient, not as an eigenvalue. And the narrative suggests that the author is talking about the probability of the eigenstate. But anyway, let’s use your definition.JesseM said:No, I don't think so. If you look at the actual equation they give for the Born rule in section 3.4, the equation is giving a probability of getting a given eigenvalue, not a given eigenstate/eigenvector. The verbal discussion in the paragraph preceding that equation is a bit confusing because they assume the Born rule is always coupled with the collapse postulate, so that the probability of getting a given eigenvalue would be the same as the probability of collapsing to the corresponding eigenstate, but the two assumptions are logically separable, and the article follows every other source I've seen in defining the Born rule in terms of the probability of getting a particular eigenvalue (which is understood as a possible measurement result).
I mean the Born rule is not about “records”, either observable or not, it is about the final results of observation (please advise if you disagree). These are two different things, as, for example, "records” are never final.JesseM said:I don't understand what you mean by "nothing in" them "about" measurement records. Unitary evolution and the Born rule apply the same way to all quantum systems, they don't give specific rules for pointer states so I guess in that sense you could say there is "nothing in" them about pointer states, but nor do they give specific rules for electrons going through a double-slit or for any other particular quantum system, would you say "there is nothing in unitary evolution or in the Born rule about electrons"? The point is that unitary evolution and the Born rule can be applied in exactly the same way to any quantum system you like, so why not apply them to the macroscopic measuring devices and their records/pointer states in just the way you'd apply them to microscopic systems?
As I said, this procedure can be satisfactory for one purpose and unsatisfactory for another one. We are talking about the Born rule as applied to Bell experiments. In this case your procedure should be as follows: you have to take the records of measurements for two spatially separated particles and observe them simultaneously to obtain the input to the correlation. If you observe the records simultaneously (and that means in the same place), you cannot do that fast enough to eliminate the possibility of subluminal signaling (i.e. to close the locality loophole). On the other hand, you cannot be sure the records were the same at the time of the measurement, as the records are not permanent.JesseM said:Who said they had to be permanent? The point is just to pick some time T shortly after all the experiments have been done, and apply the Born rule at T to find the probabilities of observing different measurement records at T. Maybe in the distant future all records of this experiment will be lost and no one will remember what the actual results were, but so what? This is just a procedure for making predictions about empirical results in the here-and-now.
I mean the following. You cannot apply the Born rule in a specific form to an arbitrary measurement. For example, you cannot apply the Born rule defining the probability of the system having certain coordinates to a momentum measurement. In the same way, if you apply the Born rule for spin projections of two spatially separated particles, strictly speaking, the measurement should be designed to measure the two spin projections simultaneously, so perhaps you need some nonlocal measurement arrangement (nightlight said something to this effect). That’s not what happens in Bell experiments, where you measure the spin projections separately, and then combine the results. As I said above, this is something different.JesseM said:Don't know what you mean by that. Any time you use a theoretical model to make predictions about a real-world experiment, the model is always simplified, you couldn't possibly model the precise behavior of every single particle involved in the experiment, so in that sense all models are "abstract", but they are nevertheless highly useful in making predictions about real-world experiments, otherwise we'd just be doing pure math and not physics!
I disagree that “there is no problem” – “at some time T after all measurements have already been performed” you cannot close the locality loophole, as “all the data will be collected in one place”, and you cannot state with certainty that the records have not changed. And that is “what's wrong with waiting until then”.JesseM said:I think you need to review the links I gave you earlier about von Neumann's procedure for calculating probabilities (see post #706 in particular). Again, there is no problem with measurements being made prior to the moment we apply the Born rule, it's just that each measurement is modeled as causing the measuring-device to become entangled with the system being measured exactly as you'd expect from unitary evolution, with no attempt to talk about probabilities at that point. Then at some time T after all measurements have already been performed, the Born ruler is applied to the pointer states of all the measuring devices. Obviously in the a real Bell experiment, at some point all the data will be collected in one place so scientists can review it, what's wrong with waiting until then to apply the Born rule to find the probability that a scientist will see different combinations of results on their computer screen?
On the one hand, the probability of nonzero sum of spin projections is zero, according to the Born rule. On the other hand, according to unitary evolution, the spin projection measurement cannot turn the superposition into a mixture, so the spin projection measurement on the second particle can yield any value, so, according to the Born rule, the probability of nonzero sum of spin projections is not zero.JesseM said:How so?
But Bell experiments involve independent measurements on the two spatially separated particles.JesseM said:But von Neumann's approach doesn't involve multiple successive applications of the Born rule, just a single one after all the experiments have been completed.
See aboveJesseM said:You haven't really explained why you think it contradicts unitary evolution. Many advocates of the many-worlds interpretation have tried to argue that the Born rule would still work for a "typical" observer in that interpretation, despite the fact that in the MWI unitary evolution goes on forever and thus each experiment just results in a superposition of different versions of the same experimenter seeing different results.
I am not trying to say that the Born rule per se contradicts unitary evolution (I am not sure about that), it’s the Born rule as applied for Bell experiments that contradicts unitary evolution (see above).JesseM said:Also, have a look at the paper at http://www.math.ru.nl/~landsman/Born.pdf which I found linked in wikipedia's article on the Born rule, the concluding paragraph says "The conclusion seems to be that no generally accepted derivation of the Born rule has been given to date, but this does not imply that such a derivation is impossible in principle."
My reasoning is as follows: yes, a local realistic theory cannot produce all the predictions of standard quantum mechanics, however, the postulates of standard quantum mechanics are mutually contradictory, so you cannot blame local realistic theories for failing to reproduce all predictions of standard quantum theory. So if you question unitary evolution, you also question standard quantum mechanics, therefore you cannot reasonably blame local realistic theories for failing to reproduce all predictions of standard quantum theory. And I can use unitary evolution with the Born rule for just one observable as an operational rule to get empirical evidence in favor of unitary evolution.JesseM said:Besides, you talk as though "unitary evolution" were a sacred inviolate principle, but in fact all the empirical evidence in favor of QM depends on the fact that we can connect the abstract formalism of wavefunction evolution to actual empirical observations via either the Born rule or the collapse postulate--without them you can't point to a single scrap of empirical evidence in favor of unitary evolution!
See aboveJesseM said:Of course if unitary evolution + collapse/Born rule produces a lot of successful predictions, then on the grounds of elegance there seems to be a good basis for hoping that the same unitary evolution that governs interactions between particles between measurements also governs interactions between particles and measuring devices (since measuring devices are just very large and complex collections of particles)...that's why my hope is that a totally convincing derivation of the Born rule from the MWI will eventually be found. But to just say "the Born rule and the collapse postulate violate the sacred principle of unitary evolution, therefore they must be abandoned", and to not even attempt to show how "unitary evolution" alone can yield a single solitary prediction about any empirical experiment ever performed, seems to be turning unitary evolution into a religious creed rather than a scientific theory.
You see, thermodynamics also “has a perfect track record so far in all experimental tests that have been done”, however, irreversibility is at odds with dynamics, be it classical or quantum dynamicsJesseM said:If the predictions of "quantum mechanics" are understood in von Neumann's way, then we can say that local realism is incompatible with the predictions of "quantum mechanics", and that "quantum mechanics" has a perfect track record so far in all experimental tests that have been done (including Aspect-type experiments, although none so far have done a perfect job of closing all loopholes).
Again, you can use unitary evolution with the Born rule for just one observable, as an operational rule.JesseM said:If on the other hand you choose to define "quantum mechanics" as unitary evolution alone, then unless you have some argument for why the Born rule should still work as MWI advocates do, your version of "quantum mechanics" is a purely abstract mathematical notion that makes no predictions about any real-world empirical experiments whatsoever.