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As any QT also QFT is a probabilistic description of Nature.Lynch101 said:Is QFT a statistical interpretation?
As any QT also QFT is a probabilistic description of Nature.Lynch101 said:Is QFT a statistical interpretation?
But Bell indeed DID finally formulate the philosophical quibbles in a clear mathematical way (as described in less than half a page in Weinberg's textbook). That's the great merit of his work: To make sense of some philosophical vaguely formulated quibbles by EPR (the vagueness mostly due to P, as Einstein lamented) such that it could be subject to clear quantitative observational tests.Demystifier said:If one forgets all philosophical quibbles, the idea behind hidden variables is - nothing. Without philosophy, there is no idea at all behind hidden variables. Since you are good in math and natural sciences, you would like if everything that matters could be formulated in terms of math and natural sciences. But unfortunately, many things cannot be formulated so. Since you don't like this fact of life, you try to convince yourself that those things are irrelevant. But they are not. Even you care about some of those things, despite the fact that you would prefer if you didn't care and/or try to convince yourself that you don't care.
No, Bell formulated a part of his philosophical quibbles in a clear mathematical way. But the fact that we still argue about what his proof actually proves (for you it's absence of determinism, for me and Bell and Ballentine it's absence of locality, for some it's absence of observer-independent reality, or absence of statistical independence of apparatus settings, or ...) clearly demonstrates that an important part of his philosophical quibbles is not formulated in a clear mathematical way.vanhees71 said:But Bell indeed DID finally formulate the philosophical quibbles in a clear mathematical way
Do you know why philosophy never makes progress? Because when it does, it's no longer called philosophy.vanhees71 said:The problem is that the disagreement is about philosophy and not about physics.
A word that seems to cause less consternation is the word 'universe' or 'nature'. We can define it as 'that which physics seeks to probe', 'that which physics seeks to describe', 'the subject of investigation of physics', or something along those lines. Even if we strictly define 'physics' as 'reproducible observability' it might be the case that there are limits to how far we can probe nature.vanhees71 said:Well yes. The problem is that the disagreement is about philosophy and not about physics. The indication for that is that obviously we still have not a clear agreement on the meaning of the words, particularly locality. For me locality is simply microcausality. For you obviously it has a different meaning. The same holds for "reality", which is even harder to define. For me reality is objective, reproducible observability, i.e., what can be tested by experiments.
Did it ever occur to you that locality might be a normal word present in nearly all human languages, and that this is an indication that its meaning is actually pretty clear? And that microcausality might simply one way in which a theory can be local?vanhees71 said:we still have not a clear agreement on the meaning of the words, particularly locality. For me locality is simply microcausality. For you obviously it has a different meaning.
I think there is an important distinction to be made here. From my reading of discussions on here and elsewhere, it seems that those you refer to are not necessarily saying that QM is nonlocal rather that nature is nonlocal (or has some form of nonlocal mechanism).gentzen said:the many other people who say that quantum mechanics is nonlocal are not wrong either?
It's clearly an error in thinking. Murray Gell-Mann puts it in “The Quark and the Jaguar” in the following way:gentzen said:And therefore many people say that quantum mechanics is nonlocal.
In science we cannot use everyday language but we have to clearly define what we mean. Microcausality for sure is a meaning of locality nobody has in mind when using the word in everyday language.gentzen said:Did it ever occur to you that locality might be a normal word present in nearly all human languages, and that this is an indication that its meaning is actually pretty clear? And that microcausality might simply one way in which a theory can be local?
As I said, you have to define what's meant by locality, because it has not a well-defined meaning. Microcausality is a clear property of relativistic QFTs and thus has a well-defined meaning, and it seems to me the meaning most physicists and textbook writers interpret the meaning in Bell's HV model, though one cannot always be sure, because all too often the meaning is not explicitly defined by the authors.gentzen said:I guess microcausality actually implies that there is no faster than light signaling, but the absence of faster than light signaling all by itself is also a way in which a theory can be local. And since more people are able to grasp that meaning, it might even be used more often than microcausality.
That's cause of a lot of confusion (not only in quantum theory). A statistical correlation does not necessarily imply a causal connection, and that is the case for the correlations of observables on far-distant parts of an entangled quantum system. Einstein introduced the much more precise word "inseparability" for this. Of course, this does not locality (in the sense of microcausality), because it's consistently described by local relativistic QFT. That's why I reserve the word "locality" to mean microcausality and talk about "long-ranged correlations" or "inseparability" rather than (non)locality. Definitions are made to make language as simple and concise as possible and thus one should use different words for different things.gentzen said:And to go further, there appears to be randomness in Bell type experiments, and that randomness seems to include correlations between spatially separated events. And this is one way in which the predictions of quantum mechanics (that have been confirmed in many experiments) seem to not be local. And therefore many people say that quantum mechanics is nonlocal. Can you accept that this meaning does not contradict microcausality, and that therefore both you are right when you point out that quantum theory satisfies locality, but the many other people who say that quantum mechanics is nonlocal are not wrong either?
Obviously it's totally problematic, because I have to repeatedly make clear what I understand using this word as well as you have to make clear what you understand. It would be better not to use the word anymore within physics, but this is of course impossible, because it's all too well established in the literature, including it's fuzzy meaning.gentzen said:But more importantly, did it ever occur to you that this is not the fault of philosophy? Philosophy did not invent the concept of locality, because locality is simply an intuivite concept that has been present in human thinking all along. And it is a totally unproblematic concept, if you ask me!
If you have to tell me personally that you redefined "locality" to mean "microcausality", then this does not seem to be helpful from my perspective. If most introductory textbooks on quantum mechanics would make such a redefinition for some words with good reason, then maybe it could be helpful.vanhees71 said:That's why I reserve the word "locality" to mean microcausality and talk about "long-ranged correlations" or "inseparability" rather than (non)locality.
The negation of the word locality might be problematic, because the negation of a positive property can depend on the context. But trying to forbid the use of a perfectly clear and understandable word is unreasonable, if the only reason for that move is that its negation started to get used in somewhat confusing ways.vanhees71 said:Obviously it's totally problematic, because I have to repeatedly make clear what I understand using this word as well as you have to make clear what you understand.
When talking about “Quantum non-separability” is there the implication that the system is spatially extended?Lord Jestocost said:One should thus avoid the term “quantum non-locality”. “Quantum non-separability” is the correct term in this context. Quantum non-separabilty is indeed rooted in the way the quantum formalism represents systems and sub-systems. Franck Laloë in “Do We Really Understand Quantum Mechanics?”
Franck Laloë in “Do We Really Understand Quantum Mechanics?”:Lynch101 said:When talking about “Quantum non-separability” is there the implication that the system is spatially extended?
Thanks LJ.Lord Jestocost said:Franck Laloë in “Do We Really Understand Quantum Mechanics?”:
“In general, separability is a notion that is conceptually distinct from locality. It is not necessarily related to space: two physical systems could occupy the same region of space and remain distinct with their own physical properties (separable is not the same thing as separate).
What means a "spatially extended quantum systems"?Lynch101 said:Can we infer, from the spatially separated detection events, that the quantum system is also spatially extended? Or do such concepts not apply to the quantum system.
I'm asking if we can infer that the quantum system is spatially extended by virtue of the fact that measurements of it occur in spatially separated locations?Lord Jestocost said:What means a "spatially extended quantum systems"?
Both are certainly nice references, and the quoted parts are relevant to the discussed topic and the points were confusion can arise. I wasn't even aware of Franck Laloë's book, and I am a huge fan of Quantum Mechanics: Volume III: Fermions, Bosons, Photons by Claude Cohen-Tannoudji, Bernard Diu, and Frank Laloë. I was aware of Gell-Mann's book, but I never made any serious effort to read it. I did read (what I believe to be) the last paper coauthored by Gell-Mann, and it has had a huge impact on my thinking about probability. I am quite familiar with the consistent histories framework (from articles and books by Roland Omnès and Robert Griffiths), but less familiar with the related decoherent histories interpretation by Gell-Mann and Hartle.Lord Jestocost said:Murray Gell-Mann puts it in “The Quark and the Jaguar” in the following way:
...
Franck Laloë in “Do We Really Understand Quantum Mechanics?”:
...
I assume that you did read carefully what Gell-Mann wrote before quoting him. But I have the impression that you did not read carefully what I have written. Or maybe you cared most about giving a relevant reference, and less about whether it supported your statement.Lord Jestocost said:It's clearly an error in thinking.
Instead of thinking in terms of two separate systems we can think of a single spatially extended system. If the measurement outcomes on either 'end' of the system are not pre-determined but measurement on one 'end' instantly determines the measurement outcome at the other 'end', this would equate to an FTL influence. Wouldn't it?vanhees71 said:Sure, why not?
Maybe, there is some misunderstanding.gentzen said:Both are certainly nice references, and the quoted parts are relevant to the discussed topic and the points were confusion can arise. I wasn't even aware of Franck Laloë's book, and I am a huge fan of Quantum Mechanics: Volume III: Fermions, Bosons, Photons by Claude Cohen-Tannoudji, Bernard Diu, and Frank Laloë. I was aware of Gell-Mann's book, but I never made any serious effort to read it. I did read (what I believe to be) the last paper coauthored by Gell-Mann, and it has had a huge impact on my thinking about probability. I am quite familiar with the consistent histories framework (from articles and books by Roland Omnès and Robert Griffiths), but less familiar with the related decoherent histories interpretation by Gell-Mann and Hartle.I assume that you did read carefully what Gell-Mann wrote before quoting him. But I have the impression that you did not read carefully what I have written. Or maybe you cared most about giving a relevant reference, and less about whether it supported your statement.
The quoted passage from Gell-Mann (and also the wider context in which it appeared in his book) doesn't contradict what I wrote. I highlighted the importance of "the absence of faster than light signaling", and so does Gell-Mann. The "error in thinking" would be to deduce that type of nonlocality from "correlations between spatially separated events". So his complaint about "an abuse of language" for that sort of misconception is fully compatible with my claim that the word "local" is not the problem.
Interesting! Can you substitute them with better words?Lord Jestocost said:To my mind, words like "local" or "non-local" are problematic in conjuction with quantum theory. They can over and over again tirigger people to think about quantum phenomena with classical ideas.
Indeed, two entangled photons are a single system by definition. They are not separable. Nevertheless there are two photons which can be detected at far distant places.Lynch101 said:Instead of thinking in terms of two separate systems we can think of a single spatially extended system. If the measurement outcomes on either 'end' of the system are not pre-determined but measurement on one 'end' instantly determines the measurement outcome at the other 'end', this would equate to an FTL influence. Wouldn't it?
This is assuming we can consider the system spatially extended.
To be honest: I personally try avoid to think about quantum phenomena with classical ideas and concepts. I have the feeling that it merely leads down a rabbit hole.Demystifier said:And can you really talk about quantum phenomena without classical ideas? For example, what about macroscopic measurement outcomes?
Can we therefore conclude that this single system is spatially extended?vanhees71 said:Indeed, two entangled photons are a single system by definition. They are not separable. Nevertheless there are two photons which can be detected at far distant places.
If all our measurements of quantum systems are at the classical level, are are we not then forced to at least consider classical ideas? Surely we have to explain how quantum systems give rise to classical observables?Lord Jestocost said:To be honest: I personally try avoid to think about quantum phenomena with classical ideas and concepts. I have the feeling that it merely leads down a rabbit hole.
It's possible to follow the implications of both scenarios. In general we tend to start with the assumption that there is an 'outer world', but we could equally explore the idea that there isn't. I don't think it would change much however, because ultimately it all boils down to describing our observations.Lord Jestocost said:Regarding observations (measurement outcomes): We can never be certain whether appearances in our mind can be thought "classically" as experiences of an outer world and are not mere imagining. The possibility of thinking of appearances as experiences of “something outer” allows us to talk about measurement outcomes in a conventional classical way.
Sure, why not? All there is are, however, the probabilities or probability distributions for the outcome of measurements.Lynch101 said:Can we therefore conclude that this single system is spatially extended?
It's more to do with the use of the term 'quantum non-separability' instead of 'quantum non-locality' (FTL-nonlocality).vanhees71 said:Sure, why not? All there is are, however, the probabilities or probability distributions for the outcome of measurements.
If we can infer the spatial extension of the quantum system then it isn't necessarily a classical interpretation in terms of hidden variables that indicates FTL-nonlocality. If the measurement on one 'end' of the system immediately determines the outcome at the other, spatially separated 'end' of the system, this too would imply FTL-nonlocality.Lord Jestocost said:It's clearly an error in thinking. Murray Gell-Mann puts it in “The Quark and the Jaguar” in the following way:
“The label ‘nonlocal’ applied by some physicists to quantum-mechanical phenomena like the EPRB effect is thus an abuse of language. What they mean is that if interpreted classically in terms of hidden variables, the result would indicate nonlocality, but of course such a classical interpretation is wrong.” [bold by LJ]
But measurements are macroscopic. So on the microscopic level, where measurements don't exist, there are no even probabilities. In a theoretical universe containing only one hydrogen atom there would be nothing at all, not even probabilities. Is it what you are saying?vanhees71 said:All there is are, however, the probabilities or probability distributions for the outcome of measurements.
So probabilities of measurement outcomes are only relevant when there are no measurement outcomes?vanhees71 said:If there were only a single hydrogen atom there'd be nobody to bother about its state and the meaning of this state.
Of course the probabilities are there when nobody measures. If the measurement is done you don't need any probabilities anymore.
I see. I never had to teach students, so the problem that my words would trigger ideas that make it harder for them to learn quantum theory never happened to me. For me personally, it was rather the absence of the concept of density matrix that initially prevented me from understanding quantum mechanics (in my QM course at university).Lord Jestocost said:Maybe, there is some misunderstanding.
To my mind, words like "local" or "non-local" are problematic in conjuction with quantum theory. They can over and over again trigger people to think about quantum phenomena with classical ideas (this I meant with "error in thinking").
vanhees71 said:The same holds for "reality", which is even harder to define. For me reality is objective, reproducible observability, i.e., what can be tested by experiments.
Lynch101 said:if the measurement on one 'end' of the system immediately determines the outcome at the other, spatially separated 'end' of the system, this too would imply FTL-nonlocality.
Sure, in "bread-and-butter physics" dealing with the description of observable phenomena, there's only one meaning of "locality", namely the impossibility to transmit information with any "faster-than-light signal" within any theory which is consistent with any theory within the (special-)relativistic (!) spacetime model. In relativistic QFT this is implemented from the very beginning by the microcausality principle for local observables, from which all the fundamental properties derivable from the so realized local relativsitic QFTs follow: unitarity and Poincare invariance of the S-matrix/optical theorem/dispersion relations, relation between spin and statistics (half-integer spin=fermions; integer spin=bosons), CPT symmetry.gentzen said:I see. I never had to teach students, so the problem that my words would trigger ideas that make it harder for them to learn quantum theory never happened to me. For me personally, it was rather the absence of the concept of density matrix that initially prevented me from understanding quantum mechanics (in my QM course at university).
After I learned a similar concept in statistical optics later in my job, I guessed that it was this concept that had been missing for me before. Much later a new job forced me to really learn and understand QM. Today I have the impression that most of classical physics remains valid, and the tricky part is rather to convince others that taking quantum corrections (like exchange effects, quantum surface transmission, channeling contrast, quantum moment conservation) into account is both possible and required for reproducing certain effects seen in experimental data, despite the fact that Monte Carlo simulations seem to be based entirely on classical concepts. A correction for exchange effects or for channeling contrast can feel badly non-local. To convince others, it helps to dig a bit into where the non-locality came from. Typically two or more electrons became indistinguishable for some specific reason. I don't think that the word "non-local" itself ever played a role is such discussions, neither positive nor negative.