A Bell Theorem with no locality assumption?

In summary, the conversation revolves around the concept of realism and its relationship to Bell and other HV no-go theorems. It also discusses the interchangeability of Hidden Variables and Realism, as well as the idea of elements of reality as a starting point for discussions. The discussion is based on papers by Charles Tresser, specifically focusing on versions of Bell's Theorem that do not assume locality and the implications of classical realism versus locality. The conversation also touches on the concept of naive realism and its relation to non-locality. The idea of an any-all distinction in quantum mechanics and its connection to the Uncertainty Principle is also mentioned. The conversation concludes with a discussion of a simple classical model that captures aspects of this
  • #1
DrChinese
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I am opening a new thread to continue discussion of some interesting ideas around EPR and Bell. Specifically, this is about the idea of realism, and whether it is tenable in light of Bell and other HV no-go theorems. Note: I usually use Hidden Variables (HV) and Realism interchangeably although some people see these as quite different. I also tend to use Realism as being an extension of EPR's "elements of reality" as a starting point for most discussions. After all, if a physical measurement can be predicted with certainty without disturbing what is measured... well, I would call that as real as it gets.

charlylebeaugossehad thrown out a few ideas in another thread - especially around some papers by Charles Tresser. So I suggest we discuss around these:

http://arxiv.org/abs/quant-ph/0608008
We prove here a version of Bell Theorem that does not assume locality. As a consequence classical realism, and not locality, is the common source of the violation by nature of all Bell Inequalities.

http://arxiv.org/abs/quant-ph/0503006
In Bohm's version of the EPR gedanken experiment, the spin of the second particle along any vector is minus the spin of the other particle along the same vector. It seems that either the choice of vector along which one projects the spin of the first particle influences at superluminal speed the state of the second particle, or naive realism holds true i.e., the projections of the spin of any EPR particle along all the vectors are determined before any measurement occurs). Naive realism is negated by Bell's theory that originated and is still most often presented as related to non-locality, a relation whose necessity has recently been proven to be false. I advocate here that the solution of the apparent paradox lies in the fact that the spin of the second particle is determined along any vector, but not along all vectors. Such an any-all distinction was already present in quantum mechanics, for instance in the fact that the spin can be measured along any vector but not at once along all vectors, as a result of the Uncertainty Principle. The time symmetry of the any-all distinction defended here is in fact reminiscent of (and I claim, due to) the time symmetry of the Uncertainty Principle described by Einstein, Tolman, and Podolsky in 1931, in a paper entitled ``Knowledge of Past and Future in Quantum Mechanics" that is enough to negate naive realism and to hint at the any-all distinction. A simple classical model is next built, which captures aspects of the any-all distinction: the goal is of course not to have a classical exact model, but to provide a caricature that might help some people.

http://arxiv.org/abs/quant-ph/0501030
We prove here a version of Bell's Theorem that is simpler than any previous one. The contradiction of Bell's inequality with Quantum Mechanics in the new version is not cured by non-locality so that this version allows one to single out classical realism, and not locality, as the common source of all false inequalities of Bell's type.
 
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  • #2
Well ok, i'll start.

I'm a layman so the math is well over my head, a bit like the moon, unless I'm not looking at it, in which case it doesn't exist, until i look at it, and then it does, and did when i wasn't looking at it. Didn't it?
 
  • #3
DrChinese said:
I am opening a new thread to continue discussion of some interesting ideas around EPR and Bell. Specifically, this is about the idea of realism, and whether it is tenable in light of Bell and other HV no-go theorems. Note: I usually use Hidden Variables (HV) and Realism interchangeably although some people see these as quite different. I also tend to use Realism as being an extension of EPR's "elements of reality" as a starting point for most discussions. After all, if a physical measurement can be predicted with certainty without disturbing what is measured... well, I would call that as real as it gets.

charlylebeaugossehad thrown out a few ideas in another thread - especially around some papers by Charles Tresser. So I suggest we discuss around these:

http://arxiv.org/abs/quant-ph/0608008
We prove here a version of Bell Theorem that does not assume locality. As a consequence classical realism, and not locality, is the common source of the violation by nature of all Bell Inequalities.

http://arxiv.org/abs/quant-ph/0503006
In Bohm's version of the EPR gedanken experiment, the spin of the second particle along any vector is minus the spin of the other particle along the same vector. It seems that either the choice of vector along which one projects the spin of the first particle influences at superluminal speed the state of the second particle, or naive realism holds true i.e., the projections of the spin of any EPR particle along all the vectors are determined before any measurement occurs). Naive realism is negated by Bell's theory that originated and is still most often presented as related to non-locality, a relation whose necessity has recently been proven to be false. I advocate here that the solution of the apparent paradox lies in the fact that the spin of the second particle is determined along any vector, but not along all vectors. Such an any-all distinction was already present in quantum mechanics, for instance in the fact that the spin can be measured along any vector but not at once along all vectors, as a result of the Uncertainty Principle. The time symmetry of the any-all distinction defended here is in fact reminiscent of (and I claim, due to) the time symmetry of the Uncertainty Principle described by Einstein, Tolman, and Podolsky in 1931, in a paper entitled ``Knowledge of Past and Future in Quantum Mechanics" that is enough to negate naive realism and to hint at the any-all distinction. A simple classical model is next built, which captures aspects of the any-all distinction: the goal is of course not to have a classical exact model, but to provide a caricature that might help some people.

http://arxiv.org/abs/quant-ph/0501030
We prove here a version of Bell's Theorem that is simpler than any previous one. The contradiction of Bell's inequality with Quantum Mechanics in the new version is not cured by non-locality so that this version allows one to single out classical realism, and not locality, as the common source of all false inequalities of Bell's type.

Those preprints where not published not rewritten to be more final so far, but someone posted the link to the paper that appeared on European J. of Phys. in the thread on action at a distance and EPR. One of the papers cited by DrC (thanks again for opening the thread)
relates more to the issue of ANY is not ALL in QM in the sense that in Classical Mechanics, ANY observation doable means ALL observation doable (at once) while this is not true in QM: in forward time because of the UP, in backward time, because of the time reversed UP of Einstein, Tolman, and Rosen (ETP). ETP also tels us that a single observale can hardly have a definite value before measurement, the first PROOF of non-realism, but his does not apply to EPR particles where two conjugate observable can pre-exist measurement if one measurement is made on each of the 2 particles. Then one had ANY but not ALL, while for generic particle, one does not even have any observable. Notice than the EPR case, the values are retrodictive (before the measurement, something that was accepted by Bohr and Heisenberg, at least until ETP showed that problematic). In some sense, the ANY is not ALL issue is a Bell-EPR type of issue but does not belong PRECISELY to this thread (but who cares?).

I have uploaded (after all, it's easy) two more recent things that I have about the title of the thread: a copy of the paper and a preprint that makes part of the paper more precise (in fact the Bell theorem part as the GHZ part remains untouched). People interested in this thread might need some time to go through these two papers (or at least the preprint as the paper has been out for a few weeks) before expressing opinions or asking questions.

This being said it seems to me that one essential ingredient in the "Bell Theory with no locality assumption" story is the hypothesis: Effect After Cause Principle. It states that for any Lorentz observer no effect can be observed and then be changed by a later caused. Yet the effect may happen after the cause (if one assumes Non-Locality to hold true, for instance), or one can ALSO assume Locality in which case of course the COMBINED hypothesis is not much different from locality. Once the EACP is recognized as not being nor implying locality, and in fact being weaker an hypothesis than locality, it remains of course to see if the proof is fine. As this is not math but physics, the issue does not reduce to a formal correctness issue.
CleBG
 

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  • #4
questions said:
Well ok, i'll start.

I'm a layman so the math is well over my head, a bit like the moon, unless I'm not looking at it, in which case it doesn't exist, until i look at it, and then it does, and did when i wasn't looking at it. Didn't it?

The hardest math in there is trigonometry, a bit of proba, and simple considerations about convergence issues.Where is the block. As for the moon, that is another issue: should we really start on that here?
 
  • #5
Hi DrC! Nice topic. Thanks, and to CleBG, for the links.
 
  • #6
One so yearns for dots to be connected. For instance: how does Tresser relate to Leggett-Garg (specifically in re: the Gisin group and Zeilinger group experiments?). CleBG's remark about the Effect After Cause Principle feels so much like the Suarez (and Gisin) Before-Before stuff ...
 
  • #7
charlylebeaugosse said:
is the hypothesis: Effect After Cause Principle. It states that for any Lorentz observer no effect can be observed and then be changed by a later caused.

Could you provide a clear definition of that principle?
Lets forget about the definition of Cause and Effect: they both are Events, and the definition of Event in QM is interpretation-dependent. But this is irrelevant now. Just assume that Cause and Effect are 2 events in the BlockTime.

How you define the difference between Cause and Effect? For me, Effect is in the lightcone of Cause, nothing more. (In CTL it could be laso vice versa). But then (in flat spacetime) Effect is always after the Cause - just by definition!

Finally, the part about "then be changed..." denies the blocktime postulating (even imaginary) possibility of a "butterfly effect".

I would say, this "principle" is lyrics, not physics.
 
  • #8
Dmitry67 said:
I would say, this "principle" is lyrics, not physics.
"In science one tries to tell people, in such a way as to be understood by everyone, something that no one ever knew before. But in poetry, it's the exact opposite."
Paul Dirac
 
  • #9
Great quote Demystifier! And funny! :smile:
 
  • #10
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  • #11
DevilsAvocado said:
Great quote Demystifier! And funny! :smile:
Thanks! If you want more, visit my blog. :smile:
 
  • #12
Demystifier said:
Thanks! If you want more, visit my blog. :smile:

Bin there, done that! :wink:

(And all your quotes are great!)
 
  • #13
Dmitry67 said:
Could you provide a clear definition of that principle?
Lets forget about the definition of Cause and Effect: they both are Events, and the definition of Event in QM is interpretation-dependent. But this is irrelevant now. Just assume that Cause and Effect are 2 events in the BlockTime.

How you define the difference between Cause and Effect? For me, Effect is in the lightcone of Cause, nothing more. (In CTL it could be laso vice versa). But then (in flat spacetime) Effect is always after the Cause - just by definition!

Finally, the part about "then be changed..." denies the blocktime postulating (even imaginary) possibility of a "butterfly effect".

I would say, this "principle" is lyrics, not physics.

I'll answer to my best, as a physicist as I have a fair voice but lyrism is not my thing. Others may have better words to explain, and the question is nice but too bad to have it in an aggressive tone. While Chaos is really my main forte since the mid 1970's, I must say that I need explanation on what the butterfly effect is doing here. I'll answer to anon-aggressive version of the question/argument till the word "Finally".


I am not a non-localist, but the direct effect of non-locality is that effects (values of spin projection observed by Alice, or inferred as existing at Alice's location as a consequence of the chosen realism hypothesis (and I am not a realism believer either) ) depend on a cause
(the axis used by Bob to make his measurement) that is spatially remote. So by you position you refuse non-locality, and the paper also tries to recuse non-locality, but without starting from the opinion that locality is right.

So one starts from 2 hypothesis:
Effect After Cause Principle (formulated so that it is compatible with non-locality) and realism to get a Bell inequality incompatible with QM.The oddness that you see in the EACP are not new when compared to usual non-locality sort of consideration. Most people in awe of Bell Theorem tell that the way violation is avoided by Nature is that Locality is false. The goal of the mentioned paper (in the title of this thread) is not to tell people convinced of locality that only locality makes sense among locality and non-locality. The goal is to prove a Bell Theorem without using locality so that non-locality cannot save the day. Now I do believe that it is microscopic realism that is the issue among the hypotheses of Bell's inequality (and in all form of Bell's Theorem, with or without inequalities as GHZ). More particularly, I believe that microphysics does not allow two EPR-Bohm particles to have a total of at least 3 projections of the spin defined at once (or two projections on each side for a total of four direction in the CHSH form of Boole-Bell inequality (for the role of name of Boole, see the work of Pitowsky, for the stat theory behind that, see the papers of Fine in J. Math Phys and the paper in PRL at about the same time). With less than 3 projections making sense at once for the two EPR-B particles together, be it 0, one, or two, there is no Bell inequality: more precisely, there is no Boole type inequality incompatible with the correlations that are compatible with quantum mechanics.

But it was a question worse rising: hope the answer satisfied most people troubled by the question. It has been known for a long time (relatively) that non-locality violates the intuition of time we learned from Special Relativity. Gisin considers that since speed of light as a limit is new to physics, it i not too much a big deal if we have to abandon that. The worse part is that some time ago, he still had the support of very bizarre sects (perhaps still does). Physics is hill: the trauma brought to that science by people who like Bell (but also other masters) defended non-locality of QM, and realism in the case of Bell is very troublesome: for me it is as if Algebra would be under the control who tell you that equation must have both sides multiplied by zero to hold true, or some other non-sense.
The great Antony Leggett wrote, more than once, that among physicists, it is essentially consensual that out of the two hypotheses of Bell's Theorem, the one that is false is realism: statitics by people around Marland Scully tell us just the contrary. I would be troubled by one QM supporting classical microscopic realism in a major US university (or UK, or French, or German, or Italian, or Japanese (any country with some tradition of geat physics where no criminals came to power like in Argentina). Science is at risk: as it goes, this beautiful invention going back to the Greeks will disapear very soon: are physicists (who would be recognized as such by Einstein, Feynman, Bohr, etc...) an endangered specie??
What is clear to me is that with the level of lack of professionalism in citations and quotation, another discipline, in particular one using less science, would already have fully disappeared.

Sad, no? But do I have a pessimistic view?
Or am I about right?
And then what should we do?
CleBG

PS: Ask for specific uploads, and I'll provide what I can (i.e., what I have in soft form or what I know where to find in the www, but others have provided competent help in the threads that I have seen: uploading is a bit too hard for me to do it right away).
 
  • #14
nikman said:
One so yearns for dots to be connected. For instance: how does Tresser relate to Leggett-Garg (specifically in re: the Gisin group and Zeilinger group experiments?). CleBG's remark about the Effect After Cause Principle feels so much like the Suarez (and Gisin) Before-Before stuff ...
Can you make precise what should be connected to what:papers and indications on what to look at said papers. For me Leggett-Garg is about realism consequences at the macroscopic level. Several people have participated to that debate following them. As for the massive production of the Switz and Austrian groups, they are so massive that pointers are unavoidable. The experiments are most often great, the theory often to par but Gisin has written many papers that are causes of confusion and the position of Zeilinger on realism and locality is hard for me to read so that I'd love to have pointers. I remember having seen things I id not like more that Gisin's but I was still much more new to the field. And when you say "Tresser relates", do you mean the person, or a particular point of the positions taken in the papers. Anyway, any mean to see better in the massive production that you have mentioned would be great, as well as understanding all of Leggett's contributions (alone or accompanied) to the subject.

Someone else has raised the issue of comparing the EACP with things of Gisin but the allusion is both lacking precision and lacking a precise reference (or several as appropriate).
 
  • #15
I read the paper twice. I did not see any problems with it; which does not mean it is without problems!
What bothers me is that 1. It seems to rule out dBB (which most HV nogo theorems do not). 2. It is four years old and is not a BIG DEAL. What am I missing?

Skippy
 
  • #16
skippy1729 said:
I read the paper twice. I did not see any problems with it; which does not mean it is without problems!
What bothers me is that 1. It seems to rule out dBB (which most HV nogo theorems do not). 2. It is four years old and is not a BIG DEAL. What am I missing?

Skippy
Not sure of what dBB means. In such precise matters, guessing would be inappropriate.
The paper has just been published and went mostly unnoticed for a long time. What I got from the analysis of a very serious physicist whom I would not name here without his consent, is that in a first approximation, each time the paper was refused, any argument against it for one referee was mostly the main argument in favor for another referee who would also have his/her critics similarly matched. Frankly, the first version were very unclear to my opinion and even the version that got published still needed the corrections in the version for Pierre Coullet's 60th birthday where the EACP's compatibility with non-locality (and with locality, but this is not the issue, except to make clear that the EACP is neither of Locality ad Non-Locality) was more explicitly used and the effect of the other side on the pair is more carefully analyzed.

Now, if the paper is as right as you seem to consider, AND if enough people know what is in there and agree with you appreciation, then the impact should be visible as this paper
seriously support the viewpoint that it is classical realism and not locality that is the false hypothesis in Bell's theory, and that the old masters where right to support non existence of microscopic realism, on which the opinion of Einstein seems to have been dramatically miss-represented (in order to let people like Gisin and other present themselves as better than Einstein) if we believe the historical work of Jammer and Fine. Miss quotations and miss refereeing is rampant in this field as if it would be closer to politics than to science.
One useful thing that Gisin did (beside some nice experiments) was to lacye when it became kosher to write about Bell'sTheory and non-locality: a paer of Ekert that is patently false (as I explain in a pre-print that cries for a co-author to help me). A joint friend has proposed to Ekert (or so he told me) to write a paper with me to explain the mistake he did when invoking Bell theorem in his method for QM-based cryptography. I never heard back from Ekert who wrote the paper that made Bell's theory Kosher: his paper is in fact more cited than the original paper on Q-cryptography (Bennett-Brassard), but Bennett, with Brassard and with and without Mermin, made serious crimes of lack of scholarly acceptable
attitude.

Well to be short(er) at last, in a subject dominated by supporters of Bell (who often ignore that they defend a strong supporter of realism) a paper posted for 4 years on arXive and always refused has little chance of making an impact. Let's see if a published paper, and hopefully more to go, change the status of all that so the we can come back to real issues and advance physics in what is probably its main sub-discipline, i.e., QM and more precisely micro-physics in the non-relativistic and then in the relativistic regimes, with then progress in all issues that could benefit from a better understanding of the basics.
 
  • #17
charlylebeaugosse said:
Not sure of what dBB means.

dBB = http://en.wikipedia.org/wiki/De_Broglie%E2%80%93Bohm_theory" [Broken]

(also called the pilot-wave theory, Bohmian mechanics, and the causal interpretation)
 
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  • #18
charlylebeaugosse said:
Can you make precise what should be connected to what:papers and indications on what to look at said papers. For me Leggett-Garg is about realism consequences at the macroscopic level. Several people have participated to that debate following them. As for the massive production of the Switz and Austrian groups, they are so massive that pointers are unavoidable. The experiments are most often great, the theory often to par but Gisin has written many papers that are causes of confusion and the position of Zeilinger on realism and locality is hard for me to read so that I'd love to have pointers. I remember having seen things I id not like more that Gisin's but I was still much more new to the field. And when you say "Tresser relates", do you mean the person, or a particular point of the positions taken in the papers. Anyway, any mean to see better in the massive production that you have mentioned would be great, as well as understanding all of Leggett's contributions (alone or accompanied) to the subject.

Someone else has raised the issue of comparing the EACP with things of Gisin but the allusion is both lacking precision and lacking a precise reference (or several as appropriate).

The most illuminating Zeilinger paper IMO is one he did back in 2005 with Brukner. "Quantum Physics as a Science of Information". SpringerLink sits on it unless you want to give them money. But fortunately the gods have smiled it's available in toto via Google books:

http://tinyurl.com/2aoydkx

Leggett-Garg incorporates a nonlocality assumption and tests for "realism" (counterfactual definiteness, whatever). Inferentially or by default that's what Tresser also does. Or not? Anyway, how are they different?

Gisin indeed has become awfully hard to follow. He's hiking deep into the woods. As I read him (and this interpretation of mine may very well be of absolutely no value whatsoever) it's all somehow coming back to the measurement problem. Hopefully what he's up to will become clear in time.
 
  • #19
nikman said:
The most illuminating Zeilinger paper IMO is one he did back in 2005 with Brukner. "Quantum Physics as a Science of Information". SpringerLink sits on it unless you want to give them money. But fortunately the gods have smiled it's available in toto via Google books:

http://tinyurl.com/2aoydkx

Leggett-Garg incorporates a nonlocality assumption and tests for "realism" (counterfactual definiteness, whatever). Inferentially or by default that's what Tresser also does. Or not? Anyway, how are they different?

Gisin indeed has become awfully hard to follow. He's hiking deep into the woods. As I read him (and this interpretation of mine may very well be of absolutely no value whatsoever) it's all somehow coming back to the measurement problem. Hopefully what he's up to will become clear in time.

With Leggett this paper shares the essential point that it is realsim and not locality that is the false asumption in Bell's theory. The author hope to soon write down "proofs" of that in terms of new experiments proposals and a discussion on the basis of the old superposition principle. One tool will be revisiting the Welcher Weg discussion, with views that are not new to Dirac, but new to Einstein, Bohr, Wheeler, Feyman, and many others, including Zeilinger whose views on locality are not fully clear, are they?

As for Gisin, he loves to explain why he is smarter than Einstein and is smart enough indeed to know that the paper that HE points out as THE start of the fashion for Bell theorem in PRL is a fraud.
Like many other localists, he cannot be (also) stupid enough despite his remarkable technical expertise in theory (beside experiments) for not let one think that he is not deeply lacking scientific honesty. Look at who support him: not so long ago (and for now I did not check) he had the support of some strange sect. This stinks, for me and I do not see any of that behind the paper being discussed. My understanding is that within a few month, another paper by the same author will be posted on QuantPh Arxive on
WW, superposition and taking the issue of local realism out of metaphysics into physics with application to interferences with or without delay. I am not privy of the title to look for, nor of the exact content. The Bell paper took about 4-5 years to be accepted (while long ago Pitowsky told the author that there were so many new ideas in there that the paper should appear anyway, or something of that sort).
 
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  • #20
DevilsAvocado said:
dBB = http://en.wikipedia.org/wiki/De_Broglie%E2%80%93Bohm_theory" [Broken]

(also called the pilot-wave theory, Bohmian mechanics, and the causal interpretation)

That's what I thought, but I wanted to be sure: sonce that paper is anti-realist, it is as anti dBB as possible, siding strongly with Pauli and Einstein on that matter.
 
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  • #21
charlylebeaugosse said:
With Leggett this paper shares the essential point that it is realsim and not locality that is the false asumption in Bell's theory.

I genuinely don't get this. BOTH locality and realism may be false assumptions in Bell's theory. For a long time, in the wake of the Aspect experiments, it was thought that only one of them actually had to be a false assumption and the other (whichever other) might go free. Following that line of thinking Bell personally opted for the false assumption being locality, not realism, and went with Bohm and nonlocality in order to salvage realism. Then, much more recently, along come Leggett and Tresser who say okay, let's indeed assume locality is an unnecessary assumption. Accept nonlocality as read. But the Bell test results may indicate that realism is a false assumption also (Leggett is a scientist of genuine integrity: he's willing to help prove himself wrong if that's how things work out). Nothing in Bell forecloses that outcome. Both locality and realism could be false assumptions. So let's assume the truth of nonlocality and then see if realism can be tested independently.

Bell's brilliance had nothing to do with his initial belief (out of reverence for Einstein) that the conclusions of EPR ought to be correct, because they're not, nor with his acceptance of Bohmism. What he did was grasp how EPR might be tested by subjecting the assumptions of locality and realism to physical experiment. This was an unprecedented accomplishment. He was just never able to figure out how to unarguably separate locality and realism on the basis of experimental results because not even he could do everything.
 
  • #22
nikman said:
I genuinely don't get this. BOTH locality and realism may be false assumptions in Bell's theory. For a long time, in the wake of the Aspect experiments, it was thought that only one of them actually had to be a false assumption and the other (whichever other) might go free. Following that line of thinking Bell personally opted for the false assumption being locality, not realism, and went with Bohm and nonlocality in order to salvage realism. Then, much more recently, along come Leggett and Tresser who say okay, let's indeed assume locality is an unnecessary assumption. Accept nonlocality as read. But the Bell test results may indicate that realism is a false assumption also (Leggett is a scientist of genuine integrity: he's willing to help prove himself wrong if that's how things work out). Nothing in Bell forecloses that outcome. Both locality and realism could be false assumptions. So let's assume the truth of nonlocality and then see if realism can be tested independently.

Bell's brilliance had nothing to do with his initial belief (out of reverence for Einstein) that the conclusions of EPR ought to be correct, because they're not, nor with his acceptance of Bohmism. What he did was grasp how EPR might be tested by subjecting the assumptions of locality and realism to physical experiment. This was an unprecedented accomplishment. He was just never able to figure out how to unarguably separate locality and realism on the basis of experimental results because not even he could do everything.

Bell+Aspect do not allow to distinguish the false hypothesis, you are right here, but there are many indication to the contrary (including in the papers of Leggett and Tresser), while both consider that the issue is not yet settled for good. Now the 1931 paper of Einstein, Tolman, and Podolsky (ETP) is quite often overlooked. It proves that for generic particles (although they do not make the distinction, but clearly their argument does not apply to EPR particles) there is a UP when going back in time, something that seems to me very hardly compatible with realism, and certainly not with realism of the form needed by Bell:
according to ETP, if one measurement is made, perhaps that observable pre-exist but not the conjugate ones. Now Bell, after Bohm, considers the case when one spin projection is measured on each particle: how can the other spin that he needs (or the two other spin needed by CHSH, hence also by Aspect et al.) make any sense. This is why I always tell that Einstein (as well as others of his size, and as Feynman apparently did by throwing
Clauser out of his office as told in a popular book: is that true?) would have laughed of Bell paper and dismissed it as being as naive as dBB theories.

- For Einstein making fun of dBB, see the correspondence with Born;
- For the opinion by Born in that book according to which Einstein beleived in HVs, see what I wrote recently about QM compatible HVs in the thread about "Is action at a distance possible as..." , and see in the Born-Einstein correspondence how much Born lacked any understanding of what Einstein was trying to tell him about EPR type issues.
Thus, I do not consider that Bell was fair when he cited Born against Einstein or that he was even decent in the way he responded to Jammer's remarks that Einstein did not defend (naive) HVs.

So Bell was surely a brilliant scientist but the way he quoted things was not exemplary, AND the 1931 ETP is certainly what should let us have a bit less consideration for that part of Bell's work (whose job at CERN was not to take care of foundational issues).

Now, while history is fun, the real issue is physics and yes, it is unknown whether it is locality, or realism or both that have to be blamed of the contradiction, but while research has to progress in a free way, there are good reasons to believe that realism (in the naive
and microscopic sense) is what is wrong. Personaly my scientific life contains alsmost as many proofs of what I thought false as proofs of what I thought right a few years (or weeks) before (of course "proofs" means arguments in favor of something when working as physicist,but I share my time between math and physics and else). The fact is that non-locality and other things of that kind have invaded physics and the sound foundations are melting away, all helped by the lack of professionalism of most contributors to the www culture.
Let us hope that reason and good science will win at the end. I'd love to be (again) convinced of non-locality. After all, that is the beauty of two forms of information (Classical and Quantum) traveling at different speed (c and infinity) that I "learned about" when talking to Charles Bennett that lead me back to Quantum Mechanics after a long carrier in Classical Physics. Unfortunately I began to see misquotations all over the places and then many false arguments. I have feared non-realism most of my life (forgetting that even a realist word is mostly empty, forgetting that we are mostly empty). Please convince me or anyone else a bit cautious that realism holds true,even if almost empty.
 
  • #23
charlylebeaugosse said:
Let us hope that reason and good science will win at the end. ...

Of course they will and are! We aren't going backwards! :smile:

There was a spirited debate many years back over Big Bang versus Continuous Creation. BB won after the 1965 discovery of the CMBR of course. That same year saw the publication of Bell. I think it is safe to say that future discoveries will help us to sort things out. I too have a slight bias towards throwing out realism, but could be swayed anytime by a good paper.

As nikman says, clearly separating locality and realism is not so simple given experimental setups. For example: even in situations in which non-locality appears to be demonstrated, there are ways to construe the "action" such that there are no FTL influences at all. But now we draw the causal direction of time into the equation, making things really strange.
 
  • #24
There is so much confusion that I would like to start my participation in this thread by suggesting that we each define what we mean by "realism".

To me, realism means, "elements of reality" exist independent of observation, or observability. To me realism has nothing to do with instrumental behaviour or whether these "elements" can be directly observed without disturbance or not. To me, when you say a photon is emitted but not detected, you are admitting to my definition as above. As far as I can tell from this thread so far, all participants believe realism as defined above is true even if they haven't explicitly admitted it. If anyone else thinks realism as defined above is false, please state it and I will show using your own quotes that you are lying. However, you may think "realism" means something else and it is important we all agree what we are arguing for or against to avoid confusion.

Now some will argue that the EPR definition of realism is the idea that a single particle (or entangled pair) will have definite spin projections at 3 different angles. I do not agree that this is the EPR definition but I am willing to grant that definition for the sake of argument, so long as we are not later on drawing conclusions about the previous definition I gave above, based on this so called "EPR definition". In any case, I will suggest first that we present clearly the definition of realism we would like to argue, and then when all the parameters of this version of "realism" have been exposed, it will then make sense to question whether QM or Experiments in anyway tell us anything about the "realism" we are discussing.
 
  • #25
DrChinese said:
There was a spirited debate many years back over Big Bang versus Continuous Creation. BB won after the 1965 discovery of the CMBR of course. That same year saw the publication of Bell.

Yes, and the funny thing is that Sir Fred Hoyle, who coined the term "Big Bang", stuck to his own Steady State theory until he passed away in 2001, denying BB aggressively! :smile:

And what is almost funnier is that Hoyle promoted the theory that life evolved in space, spreading through the universe via http://en.wikipedia.org/wiki/Panspermia" [Broken], and that evolution on Earth is driven by a steady influx of viruses arriving via comets. :biggrin:

It’s hard to be a heretic!


(P.S: Speak of the devil! )
 
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  • #26
billschnieder said:
1. To me, realism means, "elements of reality" exist independent of observation, or observability. To me realism has nothing to do with instrumental behaviour or whether these "elements" can be directly observed without disturbance or not. To me, when you say a photon is emitted but not detected, you are admitting to my definition as above. As far as I can tell from this thread so far, all participants believe realism as defined above is true even if they haven't explicitly admitted it.

2. Now some will argue that the EPR definition of realism is the idea that a single particle (or entangled pair) will have definite spin projections at 3 different angles. I do not agree that this is the EPR definition ...

1. I agree with this.

2. I miss how this is different than 1. EPR said it was reasonable to admit as "real" 2 or more elements even if they could not be predicted simultaneously. So 3 different angles would quality as EPR realism as I read it. So are you saying a) that you don't think EPR says this, or b) that you do not agree with this idea, regardless of whether EPR says it?
 
  • #27
DevilsAvocado said:
1. Yes, and the funny thing is that Sir Fred Hoyle, who coined the term "Big Bang", stuck to his own Steady State theory until he passed away in 2001, denying BB aggressively! :smile:

2. And what is almost funnier is that Hoyle promoted the theory that life evolved in space, spreading through the universe via http://en.wikipedia.org/wiki/Panspermia" [Broken], and that evolution on Earth is driven by a steady influx of viruses arriving via comets. :biggrin:

1. That is sad.

2. I guess anything is possible. I have been called a virus by some people...
 
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  • #28
DrChinese said:
1. I agree with this.

2. I miss how this is different than 1. EPR said it was reasonable to admit as "real" 2 or more elements even if they could not be predicted simultaneously. So 3 different angles would quality as EPR realism as I read it. So are you saying a) that you don't think EPR says this, or b) that you do not agree with this idea, regardless of whether EPR says it?

1) I'm not sure I understand your point. Are you agreeing that my definition of "realism" in (1) is correct, or are you admitting that whatever that definition entails about the universe is true. There is a difference there. There are four possibilities

a) You agree that "realism" is defined as I did, but believe that "realism" so defined is false.
b) You disagree that "realism" is defined as I did, in which case you probably have your own definition. In addition you also believe what my definition implies about the universe, is false.
c) You disagree that realism is defined as I did but believe that, what my definition implies about the universe is true. In this case you will still have to provide your own definition of "realism".
d) You agree that realism is defined as I did, and what it implies about the universe is also True. In this case, we are in total agreement and the discussion around Bell's theorem will have to be about something other than "realism".

2) My definition of realism says nothing about predictability or observability. All it says is that "there exists, elements of reality independent of observation". If somebody says "The moon does not exist when no one is looking", they are rejecting my definition.

The so called "EPR definition" is more restrictive in the following sense. If a particle has a pre-existing attribute, which can never be directly measured, but which together with an attribute of the instrument, produce a measurable phenomenon, the so called "EPR definition" will classify this as "unreal", even though it is very real according to my definition. In other words, if you define realism as "observables" must "pre-exist" the act of "observation", then you are proposing a more restrictive view which ignores the obvious fact that some observables are created during the measurement process.

In the EPR scenario you have a spin, but you do not measure the spin, you measure it's projection. But the projection is meaningless unless you project it to something, and this something is defined by the instrument angle. Therefore the spin projection of a particle is just one example of an obvious case in which the observable is created on observation. So if you have defined realism in such a narrow way, you can not then conclude that the spin of the particle does not exist until it is measured. This is why I say we have to be clear about what definition of realism we are using. You do not need Bell to see that such a narrowly defined "realism" which is often erroneously ascribed to EPR, is a naive definition.
 
  • #29
billschnieder said:
1) I'm not sure I understand your point. Are you agreeing that my definition of "realism" in (1) is correct, or are you admitting that whatever that definition entails about the universe is true. There is a difference there. There are four possibilities

a) You agree that "realism" is defined as I did, but believe that "realism" so defined is false.
b) You disagree that "realism" is defined as I did, in which case you probably have your own definition. In addition you also believe what my definition implies about the universe, is false.
c) You disagree that realism is defined as I did but believe that, what my definition implies about the universe is true. In this case you will still have to provide your own definition of "realism".
d) You agree that realism is defined as I did, and what it implies about the universe is also True. In this case, we are in total agreement and the discussion around Bell's theorem will have to be about something other than "realism".

2) My definition of realism says nothing about predictability or observability. All it says is that "there exists, elements of reality independent of observation". If somebody says "The moon does not exist when no one is looking", they are rejecting my definition.

The so called "EPR definition" is more restrictive in the following sense. If a particle has a pre-existing attribute, which can never be directly measured, but which together with an attribute of the instrument, produce a measurable phenomenon, the so called "EPR definition" will classify this as "unreal", even though it is very real according to my definition. In other words, if you define realism as "observables" must "pre-exist" the act of "observation", then you are proposing a more restrictive view which ignores the obvious fact that some observables are created during the measurement process.

In the EPR scenario you have a spin, but you do not measure the spin, you measure it's projection. But the projection is meaningless unless you project it to something, and this something is defined by the instrument angle. Therefore the spin projection of a particle is just one example of an obvious case in which the observable is created on observation. So if you have defined realism in such a narrow way, you can not then conclude that the spin of the particle does not exist until it is measured. This is why I say we have to be clear about what definition of realism we are using. You do not need Bell to see that such a narrowly defined "realism" which is often erroneously ascribed to EPR, is a naive definition.

1. I agree with your definition as stated. I don't necessarily agree that elements of reality exist independently of observation. I tend to reject that view.

2. According to EPR: if that spin's projection can be predicted with certainty, then the pre-existing spin must itself real - independent of the instrument by which it is measured.

If the EPR definition is more "restrictive" than yours: what does EPR define as unreal that you define as real? Because I cannot see the difference. EPR specifically defines as real observables whose values can be predicted - don't you? They say there is a matching element of reality to the observable. Not that the observable (projection) itself is real.

If your definition is less restrictive than EPR's, then more qualifies as real. Which would naturally make it easier to falsify. So I guess I see that point which you are making. But what evidence would you cite for us to accept your definition over EPR's? I mean, predicting with certainty seems like a pretty strong position.

(The EPR definition is LESS restrictive than the QM definition - which of course would be only those items which can be simultaneously predicted.)
 
  • #30
DrChinese said:
1. I agree with your definition as stated. I don't necessarily agree that elements of reality exist independently of observation. I tend to reject that view.
Fair enough.
2. According to EPR: if that spin's projection can be predicted with certainty, then the pre-existing spin must itself real - independent of the instrument by which it is measured.
It is the spin which pre-exists the observation, not the "spin projection", yet it is the "spin projection" which is observable not the spin. So clearly, if the EPR definition is that "observables must pre-exist measurement", it is not a reasonable definition because as you have agreed in (1), realism simply means "elements of reality" (not "observables") pre-exist observation". In other words, it is possible for realism as defined and agreed in (1) to be true, in a completely contextual universe in which nothing can be directly observed, but in which pre-existing elements of reality always interact with instruments to reveal observables. But contextual observables are not allowed in a universe in which observables must pre-exist observation.

If the EPR definition is more "restrictive" than yours: what does EPR define as unreal that you define as real? Because I cannot see the difference.
If the EPR definition is that "observables must pre-exist observation", then contextual observables are not allowed. But in my definition, contextual observables are fully consistent with pre-existing "elements of reality". But if you are willing to agree that underlined text above is not the EPR definition, and will rather say that my original definition which you agreed to is the EPR definition, then that is a good point to start, and we can proceed to discuss the burden of proof required to disprove it.
 
  • #31
DrChinese said:
I have been called a virus by some people...

Caroline H. Thompson? :smile:
 
  • #32
billschnieder said:
There is so much confusion that I would like to start my participation in this thread by suggesting that we each define what we mean by "realism".
It should definitely help to follow this discussion.

billschnieder said:
To me, realism means, "elements of reality" exist independent of observation, or observability. To me realism has nothing to do with instrumental behaviour or whether these "elements" can be directly observed without disturbance or not. To me, when you say a photon is emitted but not detected, you are admitting to my definition as above. As far as I can tell from this thread so far, all participants believe realism as defined above is true even if they haven't explicitly admitted it. If anyone else thinks realism as defined above is false, please state it and I will show using your own quotes that you are lying. However, you may think "realism" means something else and it is important we all agree what we are arguing for or against to avoid confusion.
I would say that while this definition is "true" it is not restrictive enough to have some value.
Because you can arrive at situation where "elements of reality" are completely independent from results of observations.
I think that definition should include some statement how "elements of reality" are related to observations. Say "elements of reality" ascribed to particle together with "elements of reality" ascribed to measurement equipment (conditions) determine observed result.

billschnieder said:
Now some will argue that the EPR definition of realism is the idea that a single particle (or entangled pair) will have definite spin projections at 3 different angles. I do not agree that this is the EPR definition but I am willing to grant that definition for the sake of argument, so long as we are not later on drawing conclusions about the previous definition I gave above, based on this so called "EPR definition". In any case, I will suggest first that we present clearly the definition of realism we would like to argue, and then when all the parameters of this version of "realism" have been exposed, it will then make sense to question whether QM or Experiments in anyway tell us anything about the "realism" we are discussing.
This is not EPR definition. EPR definition covers only the case when say projection of spin is predictable with certainty. And because this definition involves "prediction" it can start a looong discussion.
 
  • #33
This violation of "Effect After Cause Principle" seems quite paradoxical. I think I agree with Dmitry:
Dmitry67 said:
For me, Effect is in the lightcone of Cause, nothing more. (In CTL it could be laso vice versa). But then (in flat spacetime) Effect is always after the Cause - just by definition!
If we can relate event that has happened before (memory) with another event that just happened (senses) then event in memory is cause by definition and event reported by senses is effect by definition and to say that effect and cause can swap places means that we should alter memory and simulate sensory information. But in that case we can't be sure about anything and I prefer to be sure about something rather than nothing.
 
  • #34
DevilsAvocado said:
Caroline H. Thompson? :smile:

Probably worse... :biggrin:
 
  • #35
billschnieder said:
Fair enough.

It is the spin which pre-exists the observation, not the "spin projection", yet it is the "spin projection" which is observable not the spin. So clearly, if the EPR definition is that "observables must pre-exist measurement", it is not a reasonable definition because as you have agreed in (1), realism simply means "elements of reality" (not "observables") pre-exist observation". In other words, it is possible for realism as defined and agreed in (1) to be true, in a completely contextual universe in which nothing can be directly observed, but in which pre-existing elements of reality always interact with instruments to reveal observables. But contextual observables are not allowed in a universe in which observables must pre-exist observation.


If the EPR definition is that "observables must pre-exist observation", then contextual observables are not allowed. But in my definition, contextual observables are fully consistent with pre-existing "elements of reality". But if you are willing to agree that underlined text above is not the EPR definition, and will rather say that my original definition which you agreed to is the EPR definition, then that is a good point to start, and we can proceed to discuss the burden of proof required to disprove it.

I'm pretty much OK with that as a working definition.

I don't really see the distinction though. EPR does not insist that the spin "projection" preexist the measurement, merely that there is an element which does. Since the result is certain, there is little point in distinguishing the two. You call that a contextual measurement, and I do not define as such. Because the result is certain, it is non-contextual. I view contextual as meaning that the entire context, including spacelike separated components, is relevant. That would not be possible in a classically local world (but would in a quantum local world).

Now of course this is true only in the case where there is an undisputed element of reality. Where my dispute arises is in the definition of simultaneous elements of reality which cannot be individually predicted with certainty. That is what Bell attacked.
 
<h2>1. What is the Bell Theorem with no locality assumption?</h2><p>The Bell Theorem with no locality assumption is a mathematical proof that shows certain predictions of quantum mechanics cannot be explained by any theory that relies on local hidden variables. This means that the outcomes of quantum experiments cannot be determined by any hidden variables that are confined to the local region.</p><h2>2. What is the significance of the Bell Theorem with no locality assumption?</h2><p>The Bell Theorem with no locality assumption has significant implications for our understanding of quantum mechanics and the nature of reality. It challenges the idea of local realism, which states that events can only be influenced by their immediate surroundings. This theorem shows that there are phenomena in the quantum world that cannot be explained by local hidden variables, and therefore, our understanding of reality may need to be revised.</p><h2>3. How was the Bell Theorem with no locality assumption discovered?</h2><p>The Bell Theorem with no locality assumption was first proposed by physicist John Stewart Bell in 1964. He developed a mathematical proof that showed the predictions of quantum mechanics could not be explained by local hidden variables. This proof was later refined and expanded upon by other scientists, including David Bohm and Alain Aspect.</p><h2>4. What are the practical applications of the Bell Theorem with no locality assumption?</h2><p>The Bell Theorem with no locality assumption has led to the development of technologies such as quantum cryptography and quantum teleportation. These technologies rely on the principles of quantum mechanics, which are supported by the Bell Theorem. Additionally, this theorem has also sparked further research and understanding of the fundamental principles of quantum mechanics.</p><h2>5. Is the Bell Theorem with no locality assumption widely accepted in the scientific community?</h2><p>Yes, the Bell Theorem with no locality assumption is widely accepted in the scientific community. It has been tested and confirmed through numerous experiments, and its predictions have been found to be consistent with the principles of quantum mechanics. However, there are still ongoing debates and discussions about the implications of this theorem for our understanding of reality.</p>

1. What is the Bell Theorem with no locality assumption?

The Bell Theorem with no locality assumption is a mathematical proof that shows certain predictions of quantum mechanics cannot be explained by any theory that relies on local hidden variables. This means that the outcomes of quantum experiments cannot be determined by any hidden variables that are confined to the local region.

2. What is the significance of the Bell Theorem with no locality assumption?

The Bell Theorem with no locality assumption has significant implications for our understanding of quantum mechanics and the nature of reality. It challenges the idea of local realism, which states that events can only be influenced by their immediate surroundings. This theorem shows that there are phenomena in the quantum world that cannot be explained by local hidden variables, and therefore, our understanding of reality may need to be revised.

3. How was the Bell Theorem with no locality assumption discovered?

The Bell Theorem with no locality assumption was first proposed by physicist John Stewart Bell in 1964. He developed a mathematical proof that showed the predictions of quantum mechanics could not be explained by local hidden variables. This proof was later refined and expanded upon by other scientists, including David Bohm and Alain Aspect.

4. What are the practical applications of the Bell Theorem with no locality assumption?

The Bell Theorem with no locality assumption has led to the development of technologies such as quantum cryptography and quantum teleportation. These technologies rely on the principles of quantum mechanics, which are supported by the Bell Theorem. Additionally, this theorem has also sparked further research and understanding of the fundamental principles of quantum mechanics.

5. Is the Bell Theorem with no locality assumption widely accepted in the scientific community?

Yes, the Bell Theorem with no locality assumption is widely accepted in the scientific community. It has been tested and confirmed through numerous experiments, and its predictions have been found to be consistent with the principles of quantum mechanics. However, there are still ongoing debates and discussions about the implications of this theorem for our understanding of reality.

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