- 8,700
- 4,780
Just point to one, if possible in an arXiv version. (You can place it there if it isn't already there.)rkastner said:See my (peer-reviewed) papers
Just point to one, if possible in an arXiv version. (You can place it there if it isn't already there.)rkastner said:See my (peer-reviewed) papers
It may not need one, but given the history of the subject, it obviously has one, as can be seen empirically from the discussions.MarkPercival said:I don't understand why QM needs a subjective side.
MarkPercival said:"Objectivity" usually is taken to mean something like "Any observer stationed *here* will observe *this* under *these* conditions". That is to say, there's something going on that will look the same to anyone who happens to be there looking at it., and it will do so in the same way even if there's nobody there looking at it which must be the case for all possible observers to see the same thing. To put an ever finer point on it, reality is real in and of itself- it doesn't require an audience to be real.
Jilang said:MarkP, QM only has a subjective side. It is totally silent on the objective side.
A. Neumaier said:Just point to one, if possible in an arXiv version. (You can place it there if it isn't already there.)
eltodesukane said:Whether the wavefunction collapses into an (unpredictable) specific state in of the Copenhagen interpretation, or whether the wavefunction branches into an (unpredictable) specific world in the many-worlds interpretation (MWI), it is really the same thing, the same problem. Why the collapse into some state? Why the branch into some world?
Not true.Jilang said:MarkP, QM only has a subjective side. It is totally silent on the objective side.
strangerep said:Not true.
Proof: The half-integral spectrum of quantum angular momentum is independent of the observer, hence objective. But that spectrum arises from representing rotational symmetry on a Hilbert space. Hence the Hilbert space is not subjective. ##\Box##
![]()
That would mean half-integral quantum angular momenta are "unreal". To disprove this, one must derive the half-integral spectrum using purely classical means. (Good luck.)atyy said:The Hilbert space is subjective because the Hilbert space depends on the division of the universe into the unreal quantum part (described by a vector in Hilbert space) and the real classical part (not described by a vector in Hilbert space).

strangerep said:That would mean half-integral quantum angular momenta are "unreal". To disprove this, one must derive the half-integral spectrum using purely classical means. (Good luck.)![]()
That sounds like a very fine drop of port you're enjoying right now.atyy said:Is there anything wrong with half-integral quantum angular momenta being "unreal"?![]()
]strangerep said:That sounds like a very fine drop of port you're enjoying right now.![]()
![]()
[ @Greg Bernhardt : we need another icon in your enhanced list: something portraying a party girl staggering around enjoying herself...]
rkastner said:In my view the big mistake in QM interpretation has been assuming that all QM dynamics must be unitary.
rkastner said:See my (peer-reviewed) papers and books for presentation of the TI alternative. Yes, the direct-action theory has been ignored and marginalized for quite some time, but there is nothing wrong with it. In fact John Wheeler was enthusiastically endorsing it in 2003, see e.g.: http://www.ijqf.org/archives/2004
You are inventing your own rules.vanhees71 said:How is the "collapse of the state" observable? I'm not aware of any example.
vanhees71 said:If this is so, then it should be easy for you to provide an example for a real experiment, where you need the collapse hypothesis to describe its result within quantum theory. I don't know of any. So far, the most simple description is in terms of the minimal interpretation. You just take the Born rule as one more independent assumption, i.e., the quantum mechanical state describes probabilities for the outcome of measurements and nothing more.
vanhees71 said:What's the "generalized Born rule". For me the Born rule is a postulate saying that for any state, represented by a statistical operator ##\hat{R}## the outcome of the measurement of an observable ##A## to be the value ##a##, represented by a self-adjoint operator ##\hat{A}## defining a (generalized) orthonormalized eigenvector basis ##|a,\beta \rangle## is given by
$$P_A(a|\hat{R})=\sum_{\beta} \langle a,\beta|\hat{R}|a,\beta \rangle,$$
where the sum can also be an integral or both a sum and an integral, depending on the specific spectral properties of ##\hat{A}##.
For me that's a postulate and nothing that can be derived. Weinberg has given a thorough analysis of whether the Born rule is derivable from the other postulates (all well hidden above ;-)) coming to the conclusion that it can't be derived. I don't need an assumption about what happens to the state of the system due to the interaction between the measured object and the measure device, and I can't give a general one, because of course it depends on the details of this device. For sure I don't need a collapse for formulate the Born rule. It simply tells me that I have to do the measurement on a large ensemble of equally stochastically independent prepared systems to check whether the prediction of the Born rule concerning the probabilities is correct or not (within a given significance according to standard statistical rules).
Well, that's the Peres and Ballentine claim. Is it correct that with only unitary evolution you can derive collapse? Till this day you have never exhibited a derivation, neither have Peres nor Ballentine. It's a pity that quantum mechanics is still not understood even by experts.vanhees71 said:No having read the complete paper, I think that's just the description of a measurement at time ##t_2## after performing an ideal von Neumann filter measurement at ##t_1<t_2##. Where do you need a collapse here? It's just filtering out subensembles. I just need to block beams, i.e., local interaction of the partial beams with some "beam dumps", not an instantaneous collapse of whatever. One must not loose the foundation of physics in real-world setups of experiments to the abstract formalism! Then all esoterics concerning "interpretation" is usually absent from our description of this real-world experiments.
vanhees71 said:Well, I'm pretty sure I cannot described a "beam dump" in all microscopic detail, but that's not necessary to know that fact that it filters out unwanted beams! Why should I derive something unobservable and unneeded like the collapse from QT?
I prefer just to use the projection operators as given in the text without assuming an instantaneous collapse, which violates fundamental principles of physics like causality.atyy said:The collapse gives the correct prediction of your uncalculatable filtering. Which should I take - collapse which makes the prediction, or filtering which you cannot calculate?
vanhees71 said:I prefer just to use the projection operators as given in the text without assuming an instantaneous collapse, which violates fundamental principles of physics like causality.
vanhees71 said:There is no collapse in this very expression! It's just filtering out unwanted states, which is precisely described by the projection operators (for an idealized filtering). The filtering itself is not due to instantaneous action at a distance but due to local interactions (at least as long as you consider standard relativistic QFT as a correct (effective) description of nature). I'm so strictly against the collapse assumption, because it denies the fundamental property of the locality of interactions in standard relativistic QFT and it assumes dynamics outside of quantum theory.
Maybe he means something like this? http://arxiv.org/abs/hep-th/0205105atyy said:Sorry, this is just wrong.