How can one event affect another instantly over a distance

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The discussion centers on the challenge of understanding how one event can instantaneously affect another over a distance, particularly in the context of quantum mechanics and relativity. It highlights that while quantum measurements can show correlations, they do not imply a causal relationship as understood in classical physics, complicating the notion of simultaneity. The conversation also addresses the inherent non-locality in quantum theory, which conflicts with the principles of special relativity, suggesting that a new framework may be necessary to reconcile these differences. The role of global variables, such as the angle between polarizers in entangled photon experiments, is debated, with some arguing that they do not necessitate a non-local interpretation. Ultimately, the discussion concludes that the apparent non-locality challenges traditional views of relativity, indicating that our understanding of these fundamental concepts may need to evolve.
  • #61
Sherlock said:
So, I'll repeat my question that you didn't answer. :-)
What happens to these local hidden variables
when we incorporate these individual measurement
events into a correlational context involving other individual
measurement events at spacelike separations from these?
Do the hidden variables just vanish (along with local
reality)? Or is it simply that they aren't determining the
joint results?

If the lhv's simply aren't a factor in determining the joint
results, then isn't it incorrect to say that these setups
show that lhv's don't exist, or that there is no locally
realistic behavior occurring in these setups, or that lhv
descriptions of any setup are therefore ruled out?

And I'll repeat my answer: There are no local hidden variables in QM.

All LHV theories are incompatible with all of the predictions of QM. This has been known for 40 years (per Bell). If you want to postulate a LHV which mimics SOME of the predictions of QM, no one is disputing your ability to do that. But since such a theory makes erroneous predictions about some experiments (such as Aspect), it is not likely to find much acceptance among scientists.

Entangled systems are merely a tool that enables us to realize Bell's Theorem (i.e. that LR is incompatible with QM). It is not a boundary condition, i.e. that the world is local realistic everywhere EXCEPT entangled systems. It is a misreading of the literature to assert otherwise.
 
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  • #62
ttn said:
What is the source of this seemingly irresistable desire people have to associate locality and realism, as if there were only one issue: "local realism" vs everything else? ...

"Reality" is still a damn reasonable assumption. (Really, it's an axiom -- it is necessarily presupposed by any physics at all, and any attempt to deny it refutes itself.) If you mean something narrower, like whether spin-components are real properties (as opposed to "contextual" or "emergent" properties) of particles, well then you should be specific and not imply that somehow anything in QM refutes realism *generally*.

So it is totally misleading to say: "It is wrong to say that any L[ocal] R[ealistic] theories are consistent with QM." The correct statement is: "It is wrong to say that any [Local] theory is consistent with QM."

This is factually incorrect. The reason L and R MUST be mentioned together is because Non-local HV theories are not excluded by Bell's Theorem. But that does not mean that Non-locality is the only solution. You assume by your statement ("Reality is still a damn reasonable assumption"), exactly as EPR did, that there is simultaneous existence of non-commuting observables. Maybe, maybe not!

There is an explicit assumption in Bell's argument: that of reality ("It follows that C is another unit vector [in addition to A and B] ..."). This is the specific narrower context you are asking about. Sure, it is reasonable, but that does not make it true! Please note that Locality is implicitly added into Bell's argument - he mentions it, but basically takes if for granted that if there is some FTL communication between A and B (a la Bohmian Mechanics or similar) then there is no problem reproducing the results of QM.

So the fact is: the Reality and Locality assumptions are both part of Bell. So if you wonder why they are mentioned together so strongly... well, there you are! :)
 
  • #63
DrChinese said:
You assume by your statement ("Reality is still a damn reasonable assumption"), exactly as EPR did, that there is simultaneous existence of non-commuting observables. Maybe, maybe not!

This is exactly why MWI can "weasel out": it takes it (from Alice's point of view) that Bob both did and did not see his detector click. So Alice cannot talk about the "probability that Bob's detector clicked". It did both, each in a separate branch. However, when Alice MEETS Bob, she has to make a choice between the two Bobs and NOW, locally, she assigns a probability to Bob's result. But as this is local, no parameter independence is required anymore (the probability can locally depend as well on Alice's choices of the polarizer as on Bob's, because this information is present locally now).

Again, one can dislike MWI for many reasons, but the very existence of this view means that one cannot say that the observed outcomes of QM mean that the theory is non-local ; in the same way as Bohm's theory means that one cannot say that no hidden variable deterministic theory can make identical predictions as QM. Whether one thinks that Bohm was right or not.

cheers,
Patrick.
 
  • #64
DrChinese said:
This is factually incorrect. The reason L and R MUST be mentioned together is because Non-local HV theories are not excluded by Bell's Theorem. But that does not mean that Non-locality is the only solution.

If you only consider Bell's Theorem, you might fool yourself into thinking that a local theory which dispensed with hv's (e.g., the simultaneously real spin components you were talking about before) could work. But this would be to ignore something that we know thanks to EPR: if you *don't* have those simultaneously real spin components (i.e., if you don't have exactly the kind of hv's Bell assumes in his derivation) you also cannot get the empirically correct predictions without violating locality. Summary: whether you have those extra elements of reality or not, a local theory will conflict with experiment. So... putting *all* the relevant arguments and evidence on the table... non-locality *is* the only solution.

It's interesting that the logic here is the same as the point you made so eloquently to Sherlock. Yes, a LHV theory can explain certain facts. But it can't explain other facts. So LHV theories are excluded. When you put *all* the evidence on the table, it is clear that LHV theories can't account for it. Likewise, when you put all the evidence on the table, it is clear that Bell Locality fails (regardless of what position you want to take on "realism", i.e., hidden variables).


You assume by your statement ("Reality is still a damn reasonable assumption"), exactly as EPR did, that there is simultaneous existence of non-commuting observables. Maybe, maybe not!

No, you're quoting me out of context. There I was using the word "reality" to refer to scientific realism *generally* -- the belief that there is an external physical world independent of my consciousness. (Not *experiments*, mind you, because experiments are part of that physical world -- when I say consciousness I mean it literally.)

If you meant above that, like me, Einstein believed in scientific realism generally, you are absolutely correct. But if you mean by "realism" specifically belief in some particular elements of reality like spin components, then it is absurd to say that EPR *assumed* their existence. They *proved* that they must exist, subject to the assumption of locality. Of course now we know that that assumption isn't true (and Einstein knew all along that it was at least logically *possible* that nature would turn out to violate locality). But that doesn't mean the argument is wrong! Orthodox QM (with the completeness assumption) violates locality, and EPR pointed out that you could perhaps construct an empirically adequate local theory to replace it if you dropped the completeness assumption -- that is, they showed that a LHV theory was the only hope for locality.

But forget all this. Which is more likely? That the EPR paper really is nothing but an emotional ejaculation ("we'd sure would like a hidden variable theory")? Or that you have failed to grasp the *argument* presented in that paper?


There is an explicit assumption in Bell's argument: that of reality ("It follows that C is another unit vector [in addition to A and B] ..."). This is the specific narrower context you are asking about.

Yes, and to avoid any future misunderstanding, we should both refer to Bell's assumption by its standard name ("hidden variables") and not "reality".


Sure, it is reasonable, but that does not make it true!

Bell jumped off from what EPR had proved. They proved that, under the assumption of locality, certain hidden variables had to exist. Bell assumed that those hidden variables existed, imposed the locality condition again, and (by considering more general correlations than EPR had considered) showed that a certain statistical constraint could be derived, the inequality.

Again, your interpretation makes it sound as if Bell just arbitrarily assumed these hidden variables existed. He just woke up one morning and happened to share the emotion that had been previously ejaculated by EPR, so he messed around and found that this contradicted some experiments. So too bad for reality.

But that reading is inexcusably sloppy (not to mention disrespectful to Bell). If you are at all skeptical of my view here, you simply need to read Bell again. He makes it abundantly clear, e.g., here:

"Let me summarize once again the logic that leads to the impasse. The EPRB correlations are such that the result of the experiment on one side immediately foretells that on the other, whenever the analyzers happen to be parallel. If we do not accept the intervention on one side as a causal influence on the other, we seem obliged to admit that the results on both sides are determined in advance anyway, independently of the intervention on the other side, by signals from the source and by the local magnet setting. [*] But this has implications for non-parallel settings which conflict with those of quantum mechanics. So we cannot dismiss intervention on one side as a causal influence on the other."

Everything before the "[*]" is a summary of the EPR argument. The subsequent sentence refers to Bell's theorem: the thing that EPR showed to be required by locality has further implications which turn out to conflict with the QM predictions. And the final sentence is admirably (and characteristically) precise. Note in particular that no mention of "realism" or "hidden variables" (or any relevant synonyms) appear in this final conclusion.



Please note that Locality is implicitly added into Bell's argument - he mentions it, but basically takes if for granted that if there is some FTL communication between A and B (a la Bohmian Mechanics or similar) then there is no problem reproducing the results of QM.

Locality is one of the crucial premises of Bell's derivation of the inequality. Are you suggesting this assumption isn't important, or that Bell didn't think it was important? I think the quote above should dissuade you of that. Or see practically anyone of Bell's later papers, where the locality assumption is highlighted more, e.g., "la nouvelle cuisine."
 
  • #65
ttn said:
It's ridiculous to say that EPR *guessed* that QM was incomplete. This makes it sound like the entire content of the EPR argument is to pose a trivial dilemma (either X or not-X) and then to take a wild stab at answering. ("Ummm, I dunno, how about... not-X!??") The fact is, EPR actually had an *argument* for their conclusion. And the *premise* of this argument was: locality. So EPR didn't simply *guess* that maybe OQM was incomplete. They *proved* that OQM *has* to be incomplete if one insists on respecting locality. Or just saying the same thing differently, they proved that anyone who insists on treating OQM as complete has to contend with the fact that the theory is nonlocal.

Not ridiculous. EPR said in its closing sentences [my comments in brackets]:

"This makes the reality of P and Q depend on the process of measurement carried out on the first system, which does not disturb the second in any way." [This is an accurate statement, one which is demonstrated by EPR.]

"No reasonable definition of reality could be expected to permit this." [They just threw out a perfectly logical argument because they deemed it unreasonable.]

"While we have thus shown that the wave function does not provide a complete description of the physical reality, we left open the question of whether or not such a description exists." [The incompleteness conclusion is unwarranted, because they rejected a feasible alternative without rigorous reasoning.]

We believe, however, that such a theory is possible." [This is the guess. A good guess, but wrong. If EPR had known about Bell, they undoubtedly would never have gone out on a limb on this.]
 
  • #66
ttn said:
Bell jumped off from what EPR had proved. They proved that, under the assumption of locality, certain hidden variables had to exist. Bell assumed that those hidden variables existed, imposed the locality condition again, and (by considering more general correlations than EPR had considered) showed that a certain statistical constraint could be derived, the inequality.

Again, your interpretation makes it sound as if Bell just arbitrarily assumed these hidden variables existed. He just woke up one morning and happened to share the emotion that had been previously ejaculated by EPR, so he messed around and found that this contradicted some experiments. So too bad for reality.

But that reading is inexcusably sloppy (not to mention disrespectful to Bell). If you are at all skeptical of my view here, you simply need to read Bell again. He makes it abundantly clear, e.g., here:

"Let me summarize once again the logic that leads to the impasse. The EPRB correlations are such that the result of the experiment on one side immediately foretells that on the other, whenever the analyzers happen to be parallel. If we do not accept the intervention on one side as a causal influence on the other, we seem obliged to admit that the results on both sides are determined in advance anyway, independently of the intervention on the other side, by signals from the source and by the local magnet setting. [*] But this has implications for non-parallel settings which conflict with those of quantum mechanics. So we cannot dismiss intervention on one side as a causal influence on the other."

Bell's paper showed where EPR went wrong. There is really no way to read either and conclude that non-locality is a actual deduction - more like a possibility considered. The stated conclusions in both papers speak for themselves. I already quoted EPR's conclusions in a separate post. Here is Bell's conclusion:

"In a theory in which parameters are added to QM to determine the results of individual measurements, without changing the statistical predictions, there must be a mechanism whereby the setting of one measuring device can influence the reading of another instrument." [I.e. Any hidden variables must be non-local, just as you argue... but he is not saying that hidden variables are a requirement of QM or even that hidden variables exist.]

"Moreover, the signal involved must propagate instantaneously, so that such a theory could not be Lorentz invariant." [He is saying clearly: If you think there are hidden variables, you must throw out Einstein's special relativity. Bell knows this will be difficult for many, making the price too high for retaining hidden variables.]

Regardless of how you read the above, Bell's paper does not prove that QM is non-local. If you are unsure of that, simply re-read the proof in which the hidden variable assumption is included: ("It follows that C is another unit vector [in addition to A and B] ..."). It is certainly a logical possibility that this assumption is invalid, how can you deny this? Everything Bell does after depends on this crucial assumption, which he makes knowing fully where it leads.

P.S. I would appreciate it if you would not accuse me of disrespect to Bell. Anyone who is familiar with my work knows that is far off the mark (you can google EPR Bell and see where I am). I suspect we agree far more than we disagree.
 
  • #67
This discussion is, more or less, repeated here monthly, so, as usual, here's my take on the issue:

Really, what EPR, Bell, Aspect, and a whole host of other brilliant people have demonstrated is that there is no 'nice' QM. It is possible to construct particle models that correspond to the experimental results, but all have some strange qualities. Choosing one over the other is currently more of a choice of interpretation or taste than one of science.

By not nice, I mean to say that the model must be non-local (e.g. bohmian mechanics), non-realistic (e.g. plug and chug), mathematically monstrous (involving non-measurable sets), or some other similarly strange notion (such as many worlds, or mini-wormholes).

As a fan of locality and realism, I personally like the notion of 'monstrous' particles, but recognize that such an interpretation has some philosophical issues associated with it (google Banach Tarski paradox for more information.)
 
  • #68
NateTG said:
This discussion is, more or less, repeated here monthly, so, as usual, here's my take on the issue:

Really, what EPR, Bell, Aspect, and a whole host of other brilliant people have demonstrated is that there is no 'nice' QM. It is possible to construct particle models that correspond to the experimental results, but all have some strange qualities. Choosing one over the other is currently more of a choice of interpretation or taste than one of science.

By not nice, I mean to say that the model must be non-local (e.g. bohmian mechanics), non-realistic (e.g. plug and chug), mathematically monstrous (involving non-measurable sets), or some other similarly strange notion (such as many worlds, or mini-wormholes).

LOL, You nailed it in a lot fewer words...
 
  • #69
DrChinese said:
P.S. I would appreciate it if you would not accuse me of disrespect to Bell. Anyone who is familiar with my work knows that is far off the mark (you can google EPR Bell and see where I am). I suspect we agree far more than we disagree.

I don't know how much we agree, really. But I've made my views (including my disagreement with at least some of your views) as clear as I can make them. I think it's a waste of everybody's time to continue this back and forth about what Bell did and didn't prove. I've provided a quote from one of his later papers that, I think, completely undermines your position. If you don't agree, we'll have to just agree to disagree because nothing I say will convince you if Bell can't. And it's the same with Einstein/EPR. I've had my say elsewhere (e.g., 0404016) and if I haven't convinced you yet that you don't understand their argument, I don't think I ever will.
 
  • #70
ttn said:
Yes, a LHV theory can explain certain facts. But it can't explain other facts.
So LHV theories are excluded.

I'd put it this way. Lhv theories apply to some setups but not to
others. What class of setups are lhv descriptions compatible with?
According to Bell, individual measurements where, eg., you're recording
random/spontaneous output of a single detector.

What class of setups are lhv descriptions incompatible with?
Composite (A,B) measurements of the sort that characterize
typical Bell tests.

Now I'll ask you the question that I asked DrChinese.
What happens to the lhv's in the composite systems?
Do we conclude that they don't exist in either individual
or composite systems? Or that they exist in one but not
the other?

My thinking on this is that they exist in both sorts
of setups. However, while they're factors in determining
the outcomes of individual measurements, they're not
factors (at least their variability isn't) in determining the
outcomes of composite setups.

Nobody has yet addressed this: what if the hidden
property in the (A,B) setup isn't varying from pair to pair?
 
  • #71
Sherlock said:
So, I'll repeat my question that you didn't answer. :-)
What happens to these local hidden variables
when we incorporate these individual measurement
events into a correlational context involving other individual
measurement events at spacelike separations from these?
Do the hidden variables just vanish (along with local
reality)? Or is it simply that they aren't determining the
joint results?

If the lhv's simply aren't a factor in determining the joint
results, then isn't it incorrect to say that these setups
show that lhv's don't exist, or that there is no locally
realistic behavior occurring in these setups, or that lhv
descriptions of any setup are therefore ruled out?
DrChinese said:
And I'll repeat my answer: There are no local hidden variables in QM.
This isn't what I asked.

DrChinese said:
All LHV theories are incompatible with all of the predictions of QM.
No, some qm formulations can be supplemented with
lhv info, and some can't. What's the difference between
those that can and those that can't?

DrChinese said:
If you want to postulate a LHV which mimics SOME of the predictions of QM, no one is disputing your ability to do that. But since such a theory makes erroneous predictions about some experiments (such as Aspect), it is not likely to find much acceptance among scientists.
It's a matter of supplementing qm formulations with lhv
info. In some cases this would improve qm predictions
(eg. individual results), and in some cases (composite
setups) including lhv's as determining parameters
reduces the accuracy of predictions. Why?

DrChinese said:
Entangled systems are merely a tool that enables us to realize Bell's Theorem (i.e. that LR is incompatible with QM). It is not a boundary condition, i.e. that the world is local realistic everywhere EXCEPT
entangled systems.
We see that lhv's apply (determine outcomes) in some setups
and not in others. Am I to suppose that there are no
lhv's existing in the composite setups simply because they
don't determine the outcomes, or is there more to it than
that?
 
  • #72
Sherlock said:
...We see that lhv's apply (determine outcomes) in some setups and not in others.

There are no known such situations within the realm of QM - there couldn't be, because such would violate the HUP.

You are free to contradict that with an actual example. An example would be something which displays the actual local hidden variables for us to see, not something which is a hypothetical abstraction.
 
  • #73
DrChinese said:
There are no known such situations within the realm of QM - there couldn't be, because such would violate the HUP.

You are free to contradict that with an actual example. An example would be something which displays the actual local hidden variables for us to see, not something which is a hypothetical abstraction.

If we could see them they wouldn't be hidden variables,
would they? :-)

So, the whole discussion is about hypothetical abstractions ...
ie., what would happen if we supplemented some formulation
or other with hidden variable information?

And, we see that wrt some formulations it would help, and
wrt other formulations it wouldn't.

The HUP has nothing to do with more accurately predicting
detection patterns given some inferred additional information
about submicroscopic processes that's otherwise hidden from us.

This is what's happening when random individual
detections are combined to produce predictable joint
results.
 
  • #74
Sherlock said:
If we could see them they wouldn't be hidden variables,
would they? :-)

So, the whole discussion is about hypothetical abstractions ...
ie., what would happen if we supplemented some formulation
or other with hidden variable information?

And, we see that wrt some formulations it would help, and
wrt other formulations it wouldn't.

The HUP has nothing to do with more accurately predicting
detection patterns given some inferred additional information
about submicroscopic processes that's otherwise hidden from us.

This is what's happening when random individual
detections are combined to produce predictable joint
results.

Well, I can't allot weight much to a theory that explains nothing new, predicts nothing new, is not falsifiable (even when experiments such as Aspect DO falsify it), applies only in occasional spots and appears to do nothing other than satisfy perceived dissatisfactions with QM. This is why Bell's Theorem is so useful. I don't even need to consider the idea of this theory further because the entire class of LHV theories are ruled out.

If I was really smart, I'd get you and ttn talking to each other... You advocating Local HV theories as being "proven", and ttn advocating Non-local HV theories as being "proven". Then I would just side-step outta here. :smile:
 
  • #75
DrChinese said:
Well, I can't allot weight much to a theory that explains nothing new, predicts nothing new, is not falsifiable (even when experiments such as Aspect DO falsify it), applies only in occasional spots and appears to do nothing other than satisfy perceived dissatisfactions with QM. This is why Bell's Theorem is so useful. I don't even need to consider the idea of this theory further because the entire class of LHV theories are ruled out.

If I was really smart, I'd get you and ttn talking to each other... You advocating Local HV theories as being "proven", and ttn advocating Non-local HV theories as being "proven". Then I would just side-step outta here. :smile:

I'm not advocating lhv theories as being proven. I just think that
some important points are being overlooked. Lhv's (not lhv theories,
just lhv's) can exist and still not be relevant in some setups. So,
where they're not relevant you just don't use them. That's all.
This doesn't rule out lhv theories in general. It doesn't mean
that lhv's don't exist. There's still some real stuff happening
between emitters and detectors and we use what we can
infer about it to develop better, more complete, descriptions
of physical reality.
 
  • #76
Sherlock said:
Now I'll ask you the question that I asked DrChinese.
What happens to the lhv's in the composite systems?
Do we conclude that they don't exist in either individual
or composite systems? Or that they exist in one but not
the other?

The problem with 'nice' LHV theories for explaining composite systems is that they don't provide a mechanism for the HUP. Since I'm not particularly interested in the QM nuts and bolts I can't be certain of this, but Bells theorem looks like it rules out any 'hidden local realistic' theory that assigns a value to the chance of correlating non-commuting measurements, for example, measuring spin direction along a couple of different axes.

Before discussing them, I will warn you that this type of model is not AFAIK well received in mainstream physics. However, there are hidden variable theories that do not assign values to the correlations of non-commuting measurements, and hence are not invalidated by Bell's theorem + Aspect et al., but that involves unmeasurable sets. Moreover, it's clear that models of this type that make identical predictions to the 'wave equation' model can be constructed.
 
  • #77
DrChinese said:
You are free to contradict that with an actual example. An example would be something which displays the actual local hidden variables for us to see, not something which is a hypothetical abstraction.

Ah, but Science works by falsification, not by demonstration, and I can suggest an experiment that could falsify the notion that spin state can be completely explained by LHV theories:

This is only a thought experiment, but consider the following:
Let's say we have an entangled positron source, and an entangled electron source, separated by two light seconds, covered so that only pairs that send one member towards the other source are emitted. So the set up might look something like
Code:
   ______         ______
     E+             E-
   ______         ______

So, we have the source on the left emitting positrons, and the source on the right emitting electrons, and sending them into the middle where they anihillate pairwise.

We can time the anihillation, and measure the spin orientations (along the up-down axis only) of the particles that are sent out the outside ends of the apparatus.

If the anihillation occurs readily for all of the particle-antiparticle pairings, and the spins correlate then we have correlating measurements that cannot be drawn back to a single (non-hidden) event since they are (or at least could be) separated from the creation of the other particle by more than ct. This cannot be explained by any local hidden variable theory.
 
  • #78
I suppose at this point I should add that there is an obscenly comprehensive review of hidden variable theories written by Marco Genovese[1]. It is a 78-page review of the theories and experiments on the EPR-type issues, and contains 504 references! It took me a week to actually finish reading the damn thing, and I need to go over it again. It covers the historical development of the field along with practically all the important theoretical and experimental results in this field, except for the 3 that I have mentioned that was recently published (see PF Blog).

There are some strange sentences in the article (a more accurate proof-reading might have made it better), but I still highly recommend this for anyone wishing to understand this area of physics. I think other than Special Relativity, this is one area of physics that has a lot of misunderstanding.

Zz.

[1] M. Genovese, Phys. Rep. v.413, p.319 (2005).
 
  • #79
It may be true that this argument is repeated once a month, as NateTG noted, but I learn something new each time.
 
  • #80
NateTG said:
Ah, but Science works by falsification, not by demonstration, and I can suggest an experiment that could falsify the notion that spin state can be completely explained by LHV theories:

This is only a thought experiment, but consider the following:
Let's say we have an entangled positron source, and an entangled electron source, separated by two light seconds, covered so that only pairs that send one member towards the other source are emitted. So the set up might look something like
Code:
   ______         ______
     E+             E-
   ______         ______

So, we have the source on the left emitting positrons, and the source on the right emitting electrons, and sending them into the middle where they anihillate pairwise.

We can time the anihillation, and measure the spin orientations (along the up-down axis only) of the particles that are sent out the outside ends of the apparatus.

If the anihillation occurs readily for all of the particle-antiparticle pairings, and the spins correlate then we have correlating measurements that cannot be drawn back to a single (non-hidden) event since they are (or at least could be) separated from the creation of the other particle by more than ct. This cannot be explained by any local hidden variable theory.

The simpler, optical Bell tests can't be explained by lhv
theory either -- unless you don't assign a value to the
hidden parameter. Then it's not an lhv theory, but a
local hidden whatever (some mysterious constant
relationship between members of each pair?) theory. :-)

Anyway, I'm curious. Regarding your thought experiment,
how would you correlate anihilations to coincidences? Or,
would you just compare the counts per unit of time, or what?
 
  • #81
NateTG said:
The problem with 'nice' LHV theories for explaining composite systems is that they don't provide a mechanism for the HUP. Since I'm not particularly interested in the QM nuts and bolts I can't be certain of this, but Bells theorem looks like it rules out any 'hidden local realistic' theory that assigns a value to the chance of correlating non-commuting measurements, for example, measuring spin direction along a couple of different axes.

Before discussing them, I will warn you that this type of model is not AFAIK well received in mainstream physics. However, there are hidden variable theories that do not assign values to the correlations of non-commuting measurements, and hence are not invalidated by Bell's theorem + Aspect et al., but that involves unmeasurable sets. Moreover, it's clear that models of this type that make identical predictions to the 'wave equation' model can be constructed.

This sounds like the way I've been thinking about it. Do you
happen to have any references handy?
 
  • #82
Sherlock said:
The simpler, optical Bell tests can't be explained by lhv
theory either -- unless you don't assign a value to the
hidden parameter. Then it's not an lhv theory, but a
local hidden whatever (some mysterious constant
relationship between members of each pair?) theory. :-)

Actually, Bell's theorem only eliminates 'nice' lhv theories. To avoid confusion, I will refer to the local hidden theories that it does not eliminate as local hiden monster theories (lhm). The experiment I described may be able to falsify these lhm theories because it has a larger separation between the measurements than a traditional EPR experiment.

Sherlock said:
Anyway, I'm curious. Regarding your thought experiment,
how would you correlate anihilations to coincidences? Or,
would you just compare the counts per unit of time, or what?

I was thinking that you control the emitters so that the events are sparse. Then count per unit time should work. I expect that a macroscopic count per unit time would be theoretically nice. However, the net spin of a bunch of particles is going to be about the square root of the number of particles or less, which means that if you deal with large numbers of particles and anihillations there should be more 'noise'.

From my perspective the experiment has the bigger problem that I have absolutely no idea what sort of prediction conventional models make for the experimental results - so it may be a non-experiment in that the predictions made by the theories do not differ.
 
  • #83
NateTG said:
From my perspective the experiment has the bigger problem that I have absolutely no idea what sort of prediction conventional models make for the experimental results - so it may be a non-experiment in that the predictions made by the theories do not differ.

A more detailed diagram of what you have in mind
is necessary (at least for me).

My intuitive prediction is that local hidden monster
(I prefer local hidden constant) formulations won't be
falsified. :-)

If I get time, I'll do some homework about how your
proposed setup might work.
 
  • #84
Let me look at QM v. Special Relativity from a slightly different perspective.

The basic deal in entanglement is that when you locally learn facts about half of a set of entangled particles, you know something about the other half of the set of engtangled particles, regardless of their distance.

In advance, you can't know what data will be found when you collapse the wave function on either set of particles. And, viewed alone, each set of particles will comply with QM predictions.

To use the Copenhagen interpretation (or as it has been called in this thread) OQM, the reason that you can't know in advance what data will be found when you collapse the wave function on either set of particles is that this data doesn't exist yet. Until there collapse happens, any result is possible. A set of particles does not have a deterministic pre-ordained state upon collapse.

OK, so enough of OQM for a moment. We'll come back to that.

Now, one of the most basic elements of SR is that light in a vacuum travels at speed c. It has been assumed that one can infer from SR the stricter condition that information also does not travel in excess of speed c.

It seems to me that one way to reconcile SR and OCM is to violate neither of these propositions, but instead to violate the implicit, but mathematically unnecessary assuption of SR that information and light always go forward in time.

The way that you would do this is to stick to OCM. The state of one half of a set of entangled particles does not exist until you collapse the wave function. So, how does the other part of the set of entangled particles end up corollated?

Maybe, at the moment that one collapse happens, that information goes backwards in time (at a speed not greater than c) to the point of entanglement, and then goes forward in time from there to the other entangled particles, communicating the information to the second set without the message ever having traveled faster than c.

This looks like FTL, but it isn't. One of the keystones of entanglement is that it only happens to particles that have been physically local at some point in time, making this backward to forward in time communication possible.

Unlike a traditional hidden variable theory, nothing that has yet happened makes it possible to determine the final set of either part of the set of entangled particles.

But, only events within the light cone of the initial entanglement (the light cone of the global system if you will) can influence either result.

Does that make sense? Where have I gone wrong?
 
  • #85
Sherlock said:
This sounds like the way I've been thinking about it. Do you
happen to have any references handy?

I'll warn you again, that this is non-standard stuff. I'm also going to warn you that it involves non-measurable sets (if you don't know what this means, you might want to look into it a bit google unmeasurable sets, and banach-tarski for a taste).

That said, you might check out this thread:
https://www.physicsforums.com/showthread.php?t=30947&page=1&pp=15
 
  • #86
ohwilleke said:
It seems to me that one way to reconcile SR and OCM is to violate neither of these propositions, but instead to violate the implicit, but mathematically unnecessary assuption of SR that information and light always go forward in time.

Maybe, at the moment that one collapse happens, that information goes backwards in time (at a speed not greater than c) to the point of entanglement, and then goes forward in time from there to the other entangled particles, communicating the information to the second set without the message ever having traveled faster than c.

This looks like FTL, but it isn't. One of the keystones of entanglement is that it only happens to particles that have been physically local at some point in time, making this backward to forward in time communication possible.

This explanation makes AT LEAST as much sense as the other interpretations. Probably a lot more, since all physical laws are otherwise time symmetric. If the future were to exhibit SOME influence on the past, then it would appear to those in the past as being random (uncaused).

There are some articles out there which hint at this. See http://www.arxiv.org/abs/quant-ph/0507269 for example.
 

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