The notion of locality in (Quantum) Physics should be clearly defined

In summary, the thread about entanglement and Bell tests has been closed prematurely. It has not been clarified what "locality" means. Locality is the property of a relativistic theory that obeys the causality principle of relativistic spacetime. Locality is implemented by construction through the demand that local observables must commute at space-like separated arguments. This means that there cannot be any nonlocal (inter)actions between distant parts of a quantum system. However, in the mostly discussed case of entangled photon pairs you can of course have entangled photon states with the corresponding Bell-inequality violating correlations between the outcomes of measurements on the single photons in the pair at far distant places.
  • #36
Fra said:
So what is it that needs discussion?
Off topic for this thread since this thread is about locality.

We have had plenty of other threads about violations of the Bell inequalities.
 
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  • #37
PeterDonis said:
Off topic for this thread since this thread is about locality.
The central assumption of the thread starter is that there is only one notion of locality that can be clearly defined. But it seems that most of us agree that there is more than one notion of locality. The need to distinguish them is particularly important in order to understand how relativistic QFT can be compatible with the Bell theorem, i.e. how can QFT be both "local" and "nonlocal" at the same time. This idea deeply disturbs the thread starter, but apparently not the rest of us.
 
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  • #38
Demystifier said:
This is a big problem for @vanhees71 because it would imply that there is some notion of locality which is violated, which would contradict his philosophical prejudices, for which he cannot accept that they are philosophical prejudices, because it would ruin his self-picture of a pure scientist who despises philosophy. To preserve his self-picture of a pure scientist, he is forced to use philosophy to argue that it's the others, not himself, who use philosophy. Vicious circle.
No, it's about a clear terminology, not prejudices. It's just a fact that local QFTs are local in the sense that there are no causal connections between space-like separated events. That's mathematics, not philosophy.

To understand the issues about entanglement and Bell tests (which are for sure not off-topic in this thread, because they are at the heart of these questions) one must clearly distinguish between "non-locality" (i.e., theories, which violate the causality constraint of relativistic space-times and allow for some "action at a distance" or at least "faster-than-light signal propagation) and the possibility inseparability, i.e., strong correlations between outcomes of measurements on far-distant parts of a quantum system. All presumed problems go away, as soon as one sticks to the clear probabilistic meaning of the minimal statistical interpretation.

It's really unfortunate that discussion about these interesting issues inevitably end up in a morast of philosophical confusion. I should have known this and not started this thread in the first place :-(.
 
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  • #39
vanhees71 said:
inseparability, i.e., strong correlations between outcomes of measurements on far-distant parts of a quantum system. All presumed problems go away
You can call it inseparability, but it doesn't make the problem go away because the question is what causes the correlation. I know that your answer is that local interactions cause the correlation, but there is no purely scientific paper, without any philosophy, which confirms your thesis that local interactions are enough to cause the correlation. If you claim there is, cite it!
vanhees71 said:
as soon as one sticks to the clear probabilistic meaning of the minimal statistical interpretation.
Does Ballentine stick to clear probabilistic meaning of the minimal statistical interpretation? He concludes that quantum theory is nonlocal.
 
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  • #40
vanhees71 said:
the possibility inseparability, i.e., strong correlations between outcomes of measurements on far-distant parts of a quantum system.
This is what I was thinking about, as the possible question we should be discussing(perhaps not in this THREAD, but as an answer to Peters suggestion that the topic here isn't worth discussing), ie is how can we understand this inseparability?

I wonder if those using different definitions of locality, can even agree to ask this question in principle?

/Fredrik
 
  • #41
vanhees71 said:
It's really unfortunate that discussion about these interesting issues inevitably end up in a morast of philosophical confusion. I should have known this and not started this thread in the first place
Agreed. :smile:
 
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  • #42
vanhees71 said:
No, Bell's "realism" is a clear scientific postulate
I will never understand why there has to be this arbitrary dichotomy between what concept is "philosophy" and what concept is "physics". Physics is in the business of understanding the world. Philosophy is in the business of understanding the world. Obviously there is overlap. Introducing distinctions based on what is "clear" and what is "vague" or "confusing" says more about the aptitude of the one making the distinction towards these concepts than about the concepts themselves. I say this with all due respect and not specifically directed at you, since from your posts you are clearly one of the most knowledgeable and helpful people on this forum. However this attitude in my humble opinion is not only unhelpful and unjustified, but also disrespectful to both the people working at the intersection of physics and philosophy (which includes Bell) as well as philosophers in general.
 
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  • #43
Physics in the business of describing the world as it is objectively observed and not in the business to say, how the world should behave, according to some vague philosophical assumptions (as the EPR idea about, how a physical theory should look like).

The great achievement by Bell was to find a clear scientific definition of what a "realistic local hidden-variable theory" is, which can be obejctively tested by experiments. The clear result of all the Bell tests is that local (!) Q(F)T is the correct description. For me the case is closed. What philosophers make out of this result, I can't say, because it's again a mess of vague statements. As the history of science and philosophy shows, the best philosophy can do is to use the results of science to a posteriori analyze the consequences for our worldview which goes beyond the objectively observable of the sciences.

The history of science also shows that the greatest breakthrough was the deliberation of science from philosophy in the Renaissance, i.e., a clear distinction between objective (theoretical and experimental) natural sciences and subjective philosophical (and religious!) opinion, is key to that success.
 
  • #44
WernerQH said:
If there were a pair of "magic dice" that show the same face whenever and wherever they are thrown, would you call this an "inseparable" but still "local" system? Would the mystery go away if you explained that the correlations arise because they came from the same factory?
@vanhees71 : At the heart of your local explanation of EPR/B experiments seem to be "magic dice". Don't you find anything mysterious about such dice? Isn't Born's rule relevant in QFT? Have I misunderstood your position?
 
  • #45
There are no "magic dice". There's just relativistic QFT. As in any QT Born's rule, i.e., the probabilistic meaning of the quantum states, is one of the basic postulates and part of the minimal statistical interpretation, which just accepts one of the great objective findings about Nature, i.e., that it is inherently random. There's no magic involved, it's just a fact about Nature, which contradicts the outdated worldview of deterministic classical physics, and that's why many philosophers even today cannot accept it and build up all kinds of presumed paradoxes against this inevitable conclusion.
 
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  • #46
Demystifier said:
Now you are playing with words, like a philosopher
But since when is that what philosophy is?
 
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  • #47
Since when isn't this precisely what philosophy is ;-))?
 
  • #48
Demystifier said:
You can call it inseparability, but it doesn't make the problem go away because the question is what causes the correlation. I know that your answer is that local interactions cause the correlation, but there is no purely scientific paper, without any philosophy, which confirms your thesis that local interactions are enough to cause the correlation. If you claim there is, cite it!
What other interactions? The fundametal ones are: gravitational, electromagnetic weak and strong. All of them are local. Can you cite a paper that discribes those nonlocal one that you suggest are there?

ps Why do you assume that correlation implies causation?
 
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  • #49
Demystifier said:
You can call it inseparability, but it doesn't make the problem go away because the question is what causes the correlation. I know that your answer is that local interactions cause the correlation, but there is no purely scientific paper, without any philosophy, which confirms your thesis that local interactions are enough to cause the correlation. If you claim there is, cite it!
The correlation is caused on the preparation procedure. E.g., you produce an entangled photon pair by using parametric down conversion and selecting the corresponding photon pairs. It's all due to local interactions between the electromagnetic field (laser) and the particles building up the BBO crystal.
Demystifier said:
Does Ballentine stick to clear probabilistic meaning of the minimal statistical interpretation? He concludes that quantum theory is nonlocal.
Where? Ballentine's book is about non-relativistic QM, and there's not even a notion of locality. I'm pretty sure that what he calls "non-local" is just what's described by entanglement, i.e., correlations between far distant parts of a quantum system prepared in an entangled state. As I say, it's unfortunate that physicists are not more strict in the notion of locality, which leads to a great confusion in the literature.
 
  • #50
vanhees71 said:
There are no "magic dice".
Good. At least we agree on something! But I'm still puzzling about how you explain the EPR/B correlations without invoking magic dice. Your account of QED is markedly different from how I think about QED. Perhaps you should explain in a little more detail how QED achieves its "magic", instead of merely pronouncing "There's just relativistic QFT". Or the glib remark "The correlation is caused on the preparation procedure."

In a typical EPR/B experiment there are two amplitudes for the two photons to travel from the source to the detectors. (I just had a look at Feynman's discussion of the decay of positronium in his Lectures on Physics.) And following Born's rule you take the squared modulus of the amplitudes to get the probability. Now the amplitude for a photon to go from A to B is just the complex conjugate of the amplitude for going from B to A, so you can read the squared modulus as the product of the amplitudes for a photon travelling from A to B, and another (anti-) photon going from B to A. That's how I understand QED's "magic": the propagators reach also into the backward light cones. It's a local description, but it requires also waves travelling backwards in time. (This is the core of the transactional interpretation.) From a previous discussion I remember that you disagree strongly with that. But how else can you uphold your cherished locality?
 
  • #51
vanhees71 said:
The great achievement by Bell was to find a clear scientific definition of what a "realistic local hidden-variable theory" is, which can be obejctively tested by experiments. The clear result of all the Bell tests is that local (!) Q(F)T is the correct description. For me the case is closed. What philosophers make out of this result, I can't say, because it's again a mess of vague statements. As the history of science and philosophy shows, the best philosophy can do is to use the results of science to a posteriori analyze the consequences for our worldview which goes beyond the objectively observable of the sciences.
As a step towards clarifying Bell's own opinion on the relation of his great achievement to QFT, I carefully checked which articles in "Speakable and Unspeakable in Quantum Mechanics" (second edition, 2004) discuss QFT:
7 The theory of local beables (1975)
19 Beatles for quantum field theory (1984)
23 Against 'measurement' (1989)
24 La nouvelle cuisine (1990)
 
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  • #52
vanhees71 said:
To understand the issues about entanglement and Bell tests (which are for sure not off-topic in this thread, because they are at the heart of these questions) one must clearly distinguish between "non-locality" (i.e., theories, which violate the causality constraint of relativistic space-times and allow for some "action at a distance" or at least "faster-than-light signal propagation) and the possibility inseparability, i.e., strong correlations between outcomes of measurements on far-distant parts of a quantum system. All presumed problems go away, as soon as one sticks to the clear probabilistic meaning of the minimal statistical interpretation.
Also the "minimal statistical interpretation" is an interpretation, with limitations and paradoxical conclusions of its own. As an example for a limitation, I see no way how to apply it without a cut or something similar. As an example of a paradoxical conclusion, my "envisioned proof" that a qubit "in context" contains at most two classical bits of information relies on the minimal statistical interpretation:
vanhees71 said:
I've no clue, how you think you can describe a qubit with two classical bits at all. A qubit can be in a continuity of states, for two classical bits you have only 4 states. So how can there be a one-to-one connection between them?
gentzen said:
Also in this case, what I have to "check" to confirm that two classical bits can describe a single qubit "in context" are statistics of measurement results. ... In the end, this means that I work in the minimal statistical interpretation, and use it as my criterion for "checking" correctness of proposed "protocols".
 
  • #53
vanhees71 said:
Physics in the business of describing the world as it is objectively observed
You can't define what "objective" means without philosophy. You also can't possibly come up with a theory that does that.

On the other hand, what physics does do is... Model how the world SHOULD behave, according to various theories. Which is what you assert philosophy does, with the only difference that you call it "vague". Essentially you define philosophy as "vague". But that says more about your preferences than philosophy itself.

The great success of Bell was that he effectively demolished this supposed "purist" point of view, by pursuing a field that was previously supposedly "philosophy" and "not physics", and extracting results which no one could deny were physics, while also giving more food for thought to philosophy, thus showcasing yet again that there is no arbitrary distinction at all. It also goes completely contrary to your account of the history of science and philosophy, ie that philosophy at best comes after the physics. It didn't come after the physics at the very inception of physics, it didn't come after for Einstein's relativity, and it didn't come after for Bell's investigations. It always came before.

It's also wrong that philosophy and physics separated during the Renaissance. It happened much, much later, during the 19th century. Late/post renaissance "physicists" were, according to themselves, "natural philosophers". Who do you think of when you think of the "great names" of that era for physical science? Galileo, Newton, Leibniz and Descartes. Is it an accident that Leibniz and Descartes were also two of the biggest names in philosophy? What is the full name of Newton's Principia?
 
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  • #54
vanhees71 said:
The clear result of all the Bell tests is that local (!) Q(F)T is the correct description. For me the case is closed.
I also find this statement bizarre. The Bell tests rule out some theories. They can't possibly show "local QFT" is "the correct description", unless you believe they somehow demonstrated local QFT is the final theory of physics. If not you must recognize that the case is not closed, and there are multiple possible descriptions.
 
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  • #55
martinbn said:
Can you cite a paper that discribes those nonlocal one that you suggest are there?
Bohm 1952. Do you need the full reference?

martinbn said:
ps Why do you assume that correlation implies causation?
The Reichenbach common cause principle.
 
  • #56
gentzen said:
As a step towards clarifying Bell's own opinion on the relation of his great achievement to QFT, I carefully checked which articles in "Speakable and Unspeakable in Quantum Mechanics" (second edition, 2004) discuss QFT:
7 The theory of local beables (1975)
19 Beatles for quantum field theory (1984)
23 Against 'measurement' (1989)
24 La nouvelle cuisine (1990)
In this context, I think 24 is the most important one, because it addresses precisely the point that QFT notion of locality is not the adequate one in the context of Bell theorem.
 
  • #57
vanhees71 said:
Where? Ballentine's book is about non-relativistic QM, and there's not even a notion of locality. I'm pretty sure that what he calls "non-local" is just what's described by entanglement, i.e., correlations between far distant parts of a quantum system prepared in an entangled state.
The relevant quotes from Ballentine are here.
https://www.physicsforums.com/threa...be-a-waste-of-time.910190/page-3#post-5734603
 
  • #58
Demystifier said:
Bohm 1952. Do you need the full reference?
Are you saying that he discovered a new interaction, one that is not any of the four known ones?
Demystifier said:
The Reichenbach common cause principle.
How exactly does this apply to the Bell test scenario?
 
  • #59
Indeed QFT is largely a red herring. Bell specifies a concern here when he says:
J.S. Bell said:
What is held sacred is the principle of "local causality" - or "no action at a distance." Of course, mere correlation between distant events does not by itself imply action at a distanct, but only correlation between the signals reaching the two places.[...]Einstein had no difficulty accepting that affairs in different places could be correlated. What he could not accept was that an intervention at one place could influence, immediately, affairs at the other.
QFT will predict the same correlations in EPRB experiments that QM will predict. The question is can we consistently treat these correlations the same way we would correlations in a classical theory: without positing a causal influence between spacelike separated events.
 
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  • #60
martinbn said:
Are you saying that he discovered a new interaction, one that is not any of the four known ones?
You should know by now that I am too smart to be tricked by such a cheap play with words. "Discovered" in an experimental sense does not mean the same as "discovered" in theoretical physics or math. Yes, he made a theoretical discovery, he discovered a mechanism that can describe a "force" which can explain quantum correlations.

martinbn said:
How exactly does this apply to the Bell test scenario?
https://arxiv.org/abs/1311.6852
 
  • #61
Demystifier said:
You should know by now that I am too smart to be tricked by such a cheap play of words. "Discovered" in an experimental sense does not mean the same as "discovered" in theoretical physics or math. Yes, he made a theoretical discovery, he discovered a mechanism that can describe a "force" which can explain quantum correlations.
Of course, I had theoretically discovered in mind. So, you opinion is that there are more than four forces in nature?
Demystifier said:
I meant how specifically it applies. What are the events ##A## and ##B## in the Bell test scenario that are either causally related or have a common cause?
 
  • #62
martinbn said:
Of course, I had theoretically discovered in mind. So, you opinion is that there are more than four forces in nature?
Yes.

martinbn said:
I meant how specifically it applies. What are the events ##A## and ##B## in the Bell test scenario that are either causally related or have a common cause?
A and B are clicks of two spatially separated detectors, I thought it was obvious.
 
  • #63
Morbert said:
Indeed QFT is largely a red herring. Bell specifies a concern here when he says:QFT
He says that they immediately influence each other. That means an infinite speed of influence. But if you change the set up so that one of them measures later, then that would mean that the speed is very big and is just right to reach the second even. And that is the case no matter how much later the second event is. So the speed of this influence somehow depends on the set up. To me this is just like superdeterminism, except that the conspiracy is not in the initial conditions but in the evolution laws.
 
  • #64
vanhees71 said:
There are no "magic dice". There's just relativistic QFT. As in any QT Born's rule, i.e., the probabilistic meaning of the quantum states, is one of the basic postulates and part of the minimal statistical interpretation, which just accepts one of the great objective findings about Nature, i.e., that it is inherently random. There's no magic involved, it's just a fact about Nature, which contradicts the outdated worldview of deterministic classical physics, and that's why many philosophers even today cannot accept it and build up all kinds of presumed paradoxes against this inevitable conclusion.
The heart of all problems people have with quantum theory is their "unwillingness" to simply accept the irreducible randomness of individual events.

For example, Bohm and Bub in their paper “A Proposed Solution of the Measurement Problem in Quantum Mechanics by a Hidden Variable Theory“ (Rev. Mod. Phys. 38, 453, 1966):

It is not easy to avoid the feeling that such a sudden break in the theory (i.e., the replacement, unaccounted for in the theory, of one wave function by another when an individual system undergoes a measurement) is rather arbitrary. Of course, this means the renunciation of a deterministic treatment of physical processes, so that the statistics of quantum mechanics becomes irreducible (whereas in classical statistical mechanics it is a simplification – in principle more detailed predictions are possible with more information).
 
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  • #65
Lord Jestocost said:
The heart of all problems people have with quantum theory is their "unwillingness" to simply accept the irreducible randomness of individual events.
I have no problem at all with quantum theory, or the "irreducible randomness of individual events", and I think neither has @vanhees71 . My question was about his explanation of the correlations, according to QFT. It's more subtle than saying that the correlations arise from a common cause (the initial state preparation), because of quantum theory's inherent indeterminism. The future is not fully determined by the initial state.
 
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  • #66
Demystifier said:
Yes.
I think this is the reason for the debates not that there is more than one definition of locality. You, and others, are convinced that there is non-local causality, and @vanhees71 and others make the point that given that there is at least one locally causal model (relativistic QFT) you cannot claim that Bell and all that proves that QM and nature are non-local in the sense that there is non-local causality.
Demystifier said:
A and B are clicks of two spatially separated detectors, I thought it was obvious.
Not to me, and it is still unclear. Assuming we are in the ideal situation there are always clicks at the detectors! So ##A## and ##B## occur with 100% probability.
 
  • #67
WernerQH said:
I have no problem at all with quantum theory, or the "irreducible randomness of individual events", and I think neither has @vanhees71 . My question was about his explanation of the correlations, according to QFT. It's more subtle than saying that the correlations arise from a common cause (the initial state preparation), because of quantum theory's inherent indeterminism. The future is not fully determined by the initial state.
What kind of explanation do you expect? Personally I am not convinced that the common cause principle is applicable when you have a fundamentally probabilistic theory and conservation laws. So, I don't think an explanation is needed. To me it seems that to ask for an explanation requires to assume that there is causality between the space-like events or a common cause.
 
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  • #68
martinbn said:
Personally I am not convinced that the common cause principle is applicable when you have a fundamentally probabilistic theory and conservation laws.
Agreed.

martinbn said:
What kind of explanation do you expect?
I was (and still am) curious about his view how the probabilities/correlations arise in the formalism of QED. My view is that it is essential that the propagators also reach into the backward light cone, i.e. that you have waves travelling backwards in time. But this smacks of retrocausality (at least for some people) and may conflict with another cherished principle of @vanhees71 , causality.
 
  • #69
Demystifier said:
It was you who started talk about Bell's "realism", which is a philosophical concept.
I approached this thread with some excitement. Yet your second entry was an ad hominem attack. Ideas would be better.
 
  • #70
martinbn said:
I think this is the reason for the debates not that there is more than one definition of locality. You, and others, are convinced that there is non-local causality, and @vanhees71 and others make the point that given that there is at least one locally causal model (relativistic QFT) you cannot claim that Bell and all that proves that QM and nature are non-local in the sense that there is non-local causality.
That's a good point. Bell proves what it proves under one additional assumption, which is a notion of mathematical macroscopic realism. This means that macroscopic measurement outcome exists even if nobody observes it, and that it can be analyzed mathematically. Relativistic QFT in its minimal form usually accepts that outcome exists even if nobody observes it, but refuses to analyze it mathematically, which is why it cannot see the Bell theorem. It refuses to analyze it simply because the theory in its minimal form does contain the corresponding mathematical objects, and since the theory makes the right predictions even without them, refuses to consider additional mathematical objects which are not needed for predictions. Minimal QFT is somewhat like naive set theory, which refuses to consider some additional structures which are not needed in practical math, but is then unable to see deeper theorems about set theory, such as those related to the continuity hypothesis.

martinbn said:
Not to me, and it is still unclear. Assuming we are in the ideal situation there are always clicks at the detectors! So ##A## and ##B## occur with 100% probability.
I was sloppy because I was still thinking that I am saying the obvious. By "click", I mean showing a definite state, typically either "up" or "down". The probability that it will be "up" is not 100%.
 

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