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Quantum Annoyance (EPR and Bell's Inequality related).

  1. Oct 25, 2008 #1
    I'm still having difficulty trying to make sense of this data:

    It may look familiar to some of you; it came from here. This set of data in particular is important because it says that whenever the electrons both have +1/2 spin or both have -1/2 spin, the lights will both be Red or Green.

    How can we prove this by creating a computer program? Also, can someone give me an heuristic explanation how this phenomena actually takes place? In other words, why do the lights light 1/2 the time rather than 5/9'th the time?
     
  2. jcsd
  3. Oct 26, 2008 #2

    Doc Al

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    The data represents the results of performing Mermin's gedanken experiment many times. One thing that it says is that when both detectors are set to the same angle, the outcomes (Red or Green) are 100% correlated.

    What do you mean "prove this"? The results of the experiment are arranged to be consistent with what quantum mechanics tells us.
    What do you mean by "heuristic explanation"? If you're asking if there's a simple way to understand how this could happen using some kind of local mechanism (see Mermin's "instruction sets"), the point of the article is that there is no such local mechanism that can reproduce those results.

    The quantum mechanical algorithm for producing the data is explained in the paper.
     
  4. Oct 26, 2008 #3
    I think what I was trying to say was that we can create a computer algorithm around the Gedanken experiment.

    For example, we can randomly generate a triune listing of the R and G lights (such as the spreadsheet I have in the OT). Then randomly generate the switch setting, 1 through 3.
    Then see if we can get the R and G lights to flash the same color 1/2 the time, as experiment shows, or 5/9ths the time, as is presumed by Bell's Inequality.

    Assuming we make a computer algorithm that represents the singlet-state particle with a random spin, and that particle ends up in a computerized representation of the bin at random (the triune R and G bin--my spreadsheet in the OT had 45 such 'bins', or R-G combinations), and that the bins are ascribed to a computerized representation of the randomly-generated 1 through 3 switch setting, can we get agreement with this computer model as we do in the Gedanken experiment?

    IN OTHER WORDS:

    The Gedanken experiment has:
    • A singlet-state particle emitter. It emits two particles at a time.
    • Two detectors. Each detector has:
      [*]Eight bins. Each bin has three slots.​
      [*]Each slot may either be a Red slot or a Green slot.​
    • Each of the two detectors also has two lights on top: a Red light and a Green light.
    This is what makes up the Gedanken experiment.
    What happens is two singlet-state particle are emitted from the emitter. Each particle shoots toward one of the two detectors.
    The particle will then fall upon any of the eight bins (a "bin" is a3-slot receiver coded with R's and G's. Therefore, a singlet-state particle will reach any one of eight bins that have coded on it: RRR,RGG GGG GRR, etc.
    These bins themselves are hard-wired to three detector switch settings (switch settings 1 through 3), and the switch settings are assigned completely at random (so if a particle lands on a G in the three-slot bin, and if the G happens to be hardwired to a switch setting of 1, the Green light on top of the detector will light).
    After the singlet-state particle falls on its bin, it will trigger either the Red light to flash or the Green light to flash, depending on whether or not the singlet-state particle hit an R or a G, and wheter or not that R or G was hardwired to the randomly-selected switch setting.

    This can all be recreated using a simple computer program (or computer algorithm, if you will). Simply replace:
    • The emitter of the singlet-state particle with a random number generator (the "RNG") that randomly generates a 1/2 or a -1/2. There will be a 50-50 percent chance of this random number generator generating a 1/2. Obviously, the results are correlated, as they are in nature.
    • Create another random number generator for each of the eight bins; a '1' and a '2', each in numbers of three. Thus, the RNG will generate, at random, numbers like: 112 122 111 211 122 221 222, etc. Replace the bins with this number generator.
    • Create yet another random number generator that generates a 1, 2 or 3 at random. Replace the switches and their switch settings with this number generator.

    Now run this computer program, under the same way the Gedanken experiment was run.
    Will we get the lights to flash R 1/2 the time and G 1/2 the time, as they did in the Gedanken experiment?
     
  5. Oct 27, 2008 #4

    Doc Al

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    Short answer: No.

    I'm going to assume that your computer program is an attempt to duplicate the gedanken experiment using Mermin's "instruction sets" assigned randomly to the particle pairs, with detector readings that depend only upon the random setting of the detector and the random instruction set of the particle that it detects. If so, the results of the computer simulation will not duplicate the results of the original gedanken experiment with the "Mermin Contraption" (which represents the results of real experiments).
     
  6. Oct 27, 2008 #5

    DrChinese

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    As Doc Al mentions, no deterministic computer program can yield results consistent with actual experiment. The only way to get results which match experiment is to bias them according to the choice of which 2 measurement settings are chosen. But as long as those are selected randomly or otherwise without any preferential bias, you won't be able to get results that match either QM or experiment.

    Based on this outcome, you are forced to a) reject realism (i.e. that there are instruction sets); b) reject locality; or c) live in denial (hey, a lot of people fall in this category at some point). :)
     
  7. Oct 27, 2008 #6
    We know we can create a computer program based on SR or GR and that program can even show us what things look like in intensely powerful gravitational fields or under very high rates of relative speeds.
    We can also create all kinds of computer programs that likewise show how Mother Nature works: Young's double-slit can be duplicated via computer, nuclear fusion, stimulated emission in a laser, etc.

    So why can't we do the same when mimiking the Gedanken experiment in a computer program? Could it be that the bias to which you alluded to can be the missing piece in our understanding of this apparently non-localized physical phenomena?
    We can even make computer programs around the uncertainty relation. Why not this Gedanken experiment? It's like the only thing we can't replicate on computer for some reason!
     
  8. Oct 27, 2008 #7

    Doc Al

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    Of course you can create a computer program to duplicate the expected (and verified) results of quantum mechanics. You just can't create one using "instruction sets" in the manner you described. As DrChinese said, you'd have to build in a bias between the measurements of the paired particles--per the quantum prescription.
     
  9. Oct 27, 2008 #8
    What is your justification for saying a program cannot be made to reflect the results (lights both flashing same color 1/2 the time instead of 5/9 the time) of the Mermin contraption? Is saying, "Bible Thumper, it just won't work if you don't have instruction sets, OKAY?" justification enough?

    Doc Al, Dr. Chinese--feel free to explain how a computer might have "bias built in" to the program to execute results identical to the Gedanken experiment. How might we write the code for the program? Explaining specifically what this "bias" will look like as code would be helpful. What would this "bias" look like? We know what everything else looks like (SR, GR, stimulated emission, etc) when we write code for it. Or can it not be done because we don't know how to write code that would reflect the characteristic of this "bias" due to our failure in understanding the nature of the "bias"?

    Also, I found this paper, and it's a fairly recent one. It tells me that seasoned physicists to this day are still struggling with this very same problem!:

    Can you guys help me instead of saying it can't be explained?

    P/S: Woohoo! My 77th post! 700 more posts to go until my favorite number! W00t w00t! :)
     
    Last edited: Oct 27, 2008
  10. Oct 28, 2008 #9

    Doc Al

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    If you model the experiment by randomly assigning "instruction sets" to the particles and have those instruction sets determine the particle measurements, then you will not get results that agree with quantum mechanics. This is clearly explained by Mermin in the paper you quote--did you actually read it?

    If you understand Mermin's argument, then there's no need to write a computer program to demonstrate such. (See the top of page 44 in the original paper.) But instead of talking about it, why don't you just write it and see! You should have no trouble writing such a program; no knowledge of quantum mechanics is required.

    Again, writing a program that models the results of quantum mechanics (and Mermin's Gedanken experiment) is straightforward. Here's one way. Randomly generate detector settings (1, 2, or 3) for each detector. Then randomly have one of the particles measured as R or G with 50% probability. Then randomly assign the measurement of the other particle per the quantum prescription--again, explained in the paper! The probability of the two particles having the same measured value is given by cos²θ, where θ is the angle between detector settings. (Detector positions 1, 2, & 3 correspond to angles 0, 120, and 240 degrees.)

    I assure you that none of the (ever diminishing number of) physicists worrying about loopholes in Bell experiments would have the slightest problem in understanding Mermin's argument. In fact, Mermin's argument provides their motivation for (desperately) seeking such loopholes.
    What do you mean "it can't be explained"? What you can't do is explain the Bell results using a local model of particle-detector interaction where the results of the measurement depend only on some local variable that travels with the particle.
     
  11. Oct 28, 2008 #10

    vanesch

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    There seem to be misunderstandings here. There are two different statements.

    The first one is: can one write a computer program that reproduces the outputs of ideal EPR experiments in a statistical way ? And the answer is of course an obvious yes. That answers the question: can we distinguish between the datastream of a "real" ideal EPR experiment and of such a computer program ? And there the obvious answer is: no. As a computer can perfectly reproduce the statistical properties of such a dataset, there's no statistical test that is going to make the difference.

    The second statement is: could we write a computer program that generates the outcomes following an algorithm in which the outcomes are calculated as a function of independently generated particle data, and detector response, when the detector choice is random and not dependent on the particle data (and the particle data are not dependent on the detector choice) ? Then the answer is no. The proof is Bell's theorem.

    This is what Doc Al is saying, but I don't know if the OP sees the difference between both. In the second case, we put specific constraints on the algorithm and it are these constraints which make the task impossible.
     
  12. Oct 28, 2008 #11

    DrChinese

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    We have some philosophical issues mixed in here among the ones related to physics.

    1. No one knows the answer to why the laws of physics are as they are. Bell made a discovery that precludes a computer program of the type you describe, and Mermin explains why Bell's discovery does so. There are 2 pieces to his proof:

    a) The lowest correlation ratio (i.e. matches) is 5/9, or .555. Do you follow Mermin's logic for that? If you are not sure, I can easily explain it and would be happy to do so.

    b) The Quantum Mechanical prediction is 1/2. This is simply the addition of two weighted probabilities:

    i) Same settings occurs 3/9 of the time: 11, 22, 33. The QM prediction for these cases (0 degrees apart) is cos^2(0 degrees) or 1.0 (100%).
    ii) Different settings occur 6/9 of the time: 12, 13, 21, 23, 31, 32. The QM prediction for these cases (120 degrees apart) is cos^2(120 degrees) or .25 (25%).

    So we weight the probabilities as follows:

    QM = i) + ii)
    = (3/9 * 1.0) + (6/9 * .25)
    = .333 + .167
    = .500

    So the "instruction set" prediction is at least .555, while the QM prediction is .500. This explains why the computer program (using instruction sets) will never work using the ground rules provided. If you violate the ground rules, of course, as has already been mentioned, then you can write such a computer program.


    2. There are SOME scientists who believe the perfect Bell experiment has not yet been run. Of course, there are also scientists who believe the perfect test of General Relativity has not yet been run. There is really no serious controversy, it is more a matter of degree and semantics. Ask anyone who has tried, the major scientific journals routinely refuse to publish theoretical studies postulating local realism (i.e. in defiance of Bell's Theorem). This should indicate that the conclusion is on very solid scientific ground.
     
  13. Oct 28, 2008 #12

    vanesch

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    :uhh: :eek: :bugeye: I really hope that they are rejected because they are wrong and not because of consensus reasons!
     
  14. Oct 28, 2008 #13

    DrChinese

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    I couldn't say... we saw about Peter's travails recently.

    I think that Bell+Aspect has put a tremendous burden on the counter argument, and it is going to take a well-fashioned and well-developed hypothesis to get much attention. As a practical matter (at least for entanglement scenarios), there is nothing at all wrong with QM and testable differences are hard to come by.

    Of course, there is a lively sub-culture on arxiv.org regarding this subject and there seems to be no end to the viewpoints expressed. I see at least one "disproof" of Bell every few months. So I don't think anything too critical is being ignored.
     
  15. Oct 29, 2008 #14
    Doc Al, Vanesch and Dr. Chinese in particular, I am indebted to you guys. Thanks, Dr. Chinese for the excellent and clear explanation you provided me in post #11; you explained it when Mermin could not (this should tell you how concise and pithy your explanations are, and that perhaps it may be in your interest to take up writing on subjects related to physics).
    Again, please accept my abundant thanks! :)
     
  16. Oct 29, 2008 #15
    But Dr. Chinese, I'm still having difficulties. You cleared up my interpretation of the 5/9'ths versus 1/2's,
    (this is what you had to say:)
    ...Which totally cleared that problem up for me.
    but still, what about those same-result detectors (the times when both detectors get the same switch settings ; 1 thru 3) getting both G's OR both R's to flash?
    How can it be that one detector will get, by random, a "1" for a switch setting; the other detector likewise getting a "1", and they both flash the same exact color light?!
    How on G-d's green earth is this possible?

    The only thing I don't know is why should we get a same-color flash for a same-switch setting even though there is no instruction set.
     
  17. Oct 29, 2008 #16
    That's me?!!?!??! That I couldn't get a paper published in Nature, Nature Physics, Science, or Physics Today is not a surprise. I was trying to create a writing style that would make the jump to the big time, and didn't make it; I probably fell far short. If a paper of mine on quantum theory got in any of those, I would be celebrating; it didn't, so I will be reshaping my ideas over time, again, ... That's arXiv:0810.2545 [quant-ph], "The straw man of quantum physics", also on PF. But I got J.Phys.A to publish what to me is a definitive paper on "Bell inequalities for random fields", two years ago. J.Phys.A is a major Physics journal to most people (at the time, I searched J.Phys.A for papers on Bell inequalities, and found that they have only papers about Kaon experiments). Then there's a paper in last December's J.Math.Phys., developing why Physicists might or ought to be curious about what can be done with classical continuous random fields. A gradual progression is OK. Always aim for five or ten years time, never expect people to understand today what you're trying to do. Stop if you feel yourself getting bitter that people don't appreciate how brilliant you are. My newest attempt was posted on Monday at the FQXi essay contest web-page; I was quite pleased that the requirements imposed by that contest resulted fortuitously in what is for me a conceptually new starting point. Another day.

    Did you not mean me, Dr Chinese??? Oh well. Anyway, for me, not being published is not because of prejudice, it's because if it was easy it would have been done already. It's hard, the new concept of random fields has to be developed, and Physicists are too busy teaching, developing their own ideas, and doing departmental administration -- they have jobs -- so sometimes they make quick decisions on stuff they haven't seen before and have no investment in. Also, I don't write well enough, etc., etc., and I may just be barking round the wrong idea. Work at it!

    To the topic of the OP -- always a good idea -- you can try the work of Hans De Raedt's group, who have been publishing papers in various specialist journals about an interesting computational model that violates Bell inequalities. It has failings, but it's still interesting to understand why it can be said to fail, and it's better than most attempts. You can see my attempt at an assessment in arxiv:0801.1776 [quant-ph], which may help as a counterpoint to their point of view (this paper was rejected, rightly, by Phys.Rev.A because it doesn't do anything new; I didn't bother to try to publish it somewhere else).
     
  18. Oct 29, 2008 #17
    Guys: Is it true that without the experimental observing of the phenomena of entanglement, Bell's Inequality could never have been violated? Does it require a demonstration of entanglement and only entanglement to violate Bell's Inequality or can it be violated in alternate ways--ways that don't require entanglement?
     
  19. Oct 30, 2008 #18

    DrChinese

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    Peter,

    I was referring to you, but definitely not in a bad way!! I simply meant that it is a tough hill to climb, and that is a function of the success of QM and the power of Bell's Theorem.

    I definitely don't mean to imply in any way that the scientific "establishment" has it in for anyone on this subject, or that good arguments are not being heard. I believe there is more to be learned, and someone will discover something that will enlighten us all.

    -DrC
     
  20. Oct 30, 2008 #19

    DrChinese

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    Bell's Theorem does not require experimental support. Its conclusion is essentially as follows:

    No physical theory of local Hidden Variables can ever reproduce all of the predictions of Quantum Mechanics.

    You DO need entanglement to perform a Bell Test. The reason for that is that you are essentially limited by the Heisenberg Uncertainty Principle from knowing about a single particle's non-commuting observables. Entanglement was a "back door" way around that, as envisioned by EPR. But it turns out that does not work after all.

    Experimental violation of the Inequality shows that local realistic theories are not tenable.
     
  21. Oct 30, 2008 #20
    I think your question may be mixing up conceptual systems a little, BT. Bell inequalities can be constructed for classical particle property models with essentially no additional assumptions, and for classical random field models if we impose quite strong assumptions on them. Bell inequalities are violated by experiment. The empirically effective quantum mechanical models for experiments that violate Bell inequalities are entangled.

    I note, however, that entanglement --- superpositions of the tensor products of states of two subsystems --- is possible for a classical continuous random field, so entanglement does not distinguish quantum from classical in the conceptual arena of fields. That's because continuous random fields are mathematically almost identical to quantum fields. True that it's difficult-or-impossible to make entanglement make easy sense for simple-minded classical particle property models, but almost all Physicists set aside such models long ago.

    I think your question won't help you understand the experiments or the models, though I'm not certain.

    Piggy-backing a brief response to DrC here, I wanted to respond as much to the negativity of the post you were responding to as to your comments on my travails, to which I took no offense.
     
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