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I agree.martinbn said:If you mean this then I agree. But for this is von Neuman's reduction postulate not the Born's rule.
Mixing collapse and probability is not a good idea; I should have been more careful.
I agree.martinbn said:If you mean this then I agree. But for this is von Neuman's reduction postulate not the Born's rule.
atyy said:I replied to this above, but let me just add: when I say there is no uncnotroversial derivation of the Born rule from unitary time evolution in the context of Everett, I do not mean there can never ever be such a derivation, I mean there is none at present. As I stated, David Wallace, building on Deutsch, has given a strong argument for such a derivation. Earlier in the thread, I was responding to tom.stoer, with whom we have discussed Wallace's work in other threads in these forums, so he would have understood my meaning.
I think that you put meaning into my words which contradict exactly what I'm saying, and this is for me a typical sign that one leaves the realm of the natural sciences and enters the discussion culture of philosophy which is not helping understanding each other but confusing the subject. This thread is imho at this point.tom.stoer said:Strange reflex.
Discussing interpretations of quantum mechanics is always about philosophy; in this thread that begins with the headline and the very first post.
But b/c many physicists contributed to these questions (Einstein, Bohr, Weizsäcker, ...), b/c interpretations are developed and discussed by physicists ( ..., Bohm, ..., Everett, Carroll, Tegmark et al. re "many-worlds", ... GRW, ... Rovelli, ...) this seems to be relevant to many physicists.
So why closing this thread? Think about it!
Again, with this latter point I strongly disagree, and so far I've not heard any convincing (physics!) argument against the view that the classical behavior of macroscopic systems, and that's what I think you mean by "macro/micro distinction", is understood within quantum theory as an approximation valid for sufficiently coarse-grained ("macrcosopic") observables. The application of QT to many-body systems from condensed-matter to relativistic heavy-ion collisions and astrophysics (to put it in order of increasing energy) is pretty convincing evidence for this point of view. So what's "consistently wrong" with just observing this success of quantum statistical methods to explain the macroscopic systems and its "classical" behavior?atyy said:That the pure state represent complete knowledge of a single system is, of course, standard Copenhagen. Additionally, the full knowledge is probabilistic and specified by the Born rule. Under a frequentist interpretation of probability, we get a statistical interpretation of quantum mechanics, in which we only get predictions about ensembles of systems. As you point out, the standard interpretation requires a macroscopic/microscopic distinction - so yes, vanhees71 is consistently wrong on this issue.
I've no clue. For me, Born's rule is among the basic postulates that cannot be derived from the other postulates, which are more or less just providing the framework to formulate Born's rule, which is the key of the (minimal!) interpretation of QT necessary to apply the formalism to real-world experiments/observations. As any fundamental natural law it has been "derived" from a subtle interplay between empirical findings and theoretical/mathematical developments. Now it appears on half a page in any good QM 1 textbook, but it has developed within an amazingly short time of about 26 (from 1900 when Planck introduced the naive "old quantum mechanics" to Heisenberg/Born/Jordan (matrix mechanics), Schrödinger (wave mechanics), and Dirac (representation free approach, then called "transformation theory") and now forms "modern quantum theory".akvadrako said:I would like to point out that the many derivations of the Born rule require some additional assumptions and those are the controversial aspect. They either assume ##\psi## can be interpreted as probability in some general sense or that it represents the density of worlds/reality. I can't image how it would ever be possible to derive it without some way to connect a mathematical object to the physical world.
So I would like to ask, what could an uncontroversial derivation of Born's rule in EQM even look like?
Sorry if I misinterpreted your post, but ...vanhees71 said:I think that you put meaning into my words which contradict exactly what I'm saying
If you like it if not - I know that you don't like it - interpretation of science is not pure science but - at least partially - philosophy. So yes, the thread is in the realm of philosophy from the very beginning.vanhees71 said:... and this is for me a typical sign that one leaves the realm of the natural sciences and enters the discussion culture of philosophy ... This thread is imho at this point.
Yes, for you. Others may have a different opinion.vanhees71 said:For me, Born's rule is among the basic postulates that cannot be derived from the other postulates, ...
I think everybody will agree that the minimal interpretation does work in that restricted sense. But that does not automatically mean that everybody is happy with this minimal interpretation. Some of us are not, therefore we are discussing these questions.vanhees71 said:... which are more or less just providing the framework to formulate Born's rule, which is the key of the (minimal!) interpretation of QT necessary to apply the formalism to real-world experiments/observations.
That's why Born's rule is (and will always be) important. But that does by no means support the statement that it must be fundamental.vanhees71 said:As any fundamental natural law it has been "derived" from a subtle interplay between empirical findings and theoretical/mathematical developments. Now it appears on half a page in any good QM 1 textbook, but it has developed within an amazingly short time of about 26 (from 1900 when Planck introduced the naive "old quantum mechanics" to Heisenberg/Born/Jordan (matrix mechanics), Schrödinger (wave mechanics), and Dirac (representation free approach, then called "transformation theory") and now forms "modern quantum theory".
I agree.akvadrako said:I would like to point out that the many derivations of the Born rule require some additional assumptions and those are the controversial aspect.
I don't have any clue.akvadrako said:So I would like to ask, what could an uncontroversial derivation of Born's rule in EQM even look like?
tom.stoer said:I don't have any clue.
I don't think that will work.akvadrako said:... just assuming the wave-function has some kind of probabilistic interpretation is already pretty weak.
tom.stoer said:Even the Hartle frequency operator or Gleason's theorem do not derive Born's rule. The conclusion of these approaches is not "Born's rule" but that "if one wants to introduce a probabilistic interpretation then it must comply with the probability measure given by Born's rule".
tom.stoer said:I don't think that will work.
The fundamental problem we have to solve is the emergence of probabilities p and 1-p for two (infinite dimensional) subspaces. Given these two subspaces, why should a pre-factor have any probabilistic meaning in a fully deterministic theory? We should at least have a frequentist approach in the sense of "counting subspaces".
As I said the problem is not to derive which probability measure has to be used (this is unique) but why we should interpret some mathematical structure as probability at all.