Dear Edwin,

There are many claims in your paper that need to be discussed, but perhaps it is best to start with the main one. You claim to have produced a local theory that nonetheless predicts violations of Bell's inequality. But the theory simply does not appear to be local in Bell's sense. Of course, if one enforces certain global conservation restrictions on a system, that will have consequences for what is observed. The perfect anti-correlation between results for spin measurements in the same direction on particles prepared in the singlet state, for example, is predicted by enforcing 0 net spin for the system. But if each particle is not in a state which predetermines the outcome of the experiment, and is completely unaffected by whatever distant experiment is carried out, then enforcing the global conservation means that theory is not local in Bell's sense.

Let's put is more directly. Suppose that a system has two, widely separated parts and I carry out experiments on the parts at space-like separation. And suppose that as a consequence of carrying out an experiment on one part, the energy of that part changes. If I now enforce global energy conservation, so the energy that disappears from one side must appear on the other space-like-separated side, then the theory is not local in Bell's or Einstein's sense. Calling this non-local interaction between the sides "energy exchange" does not change this: energy exchange between space-like separated subsystems is a violation of locality. So it is not a surprise that your model can generate violations of Bell's inequality: it is not a local model.

The claim that your model is local is critical part of the paper: if it were true, then you wold have shown that there is some flaw in Bell's reasoning. As for your remarks on Bell's argument, you seem to have mistaken an illustrative example that he gives for part of the theorem itself, which it is not. The theorem is about any theory--whether the theory uses quantum-mechanical formalism or a completely different formalism in which there is no talk at all of eigenstates or eigenvalues--that makes certain predictions about correlations between outcomes of distant experiments. Because of this complete generality, it is not even correct to us the term "hidden variables" to describe the theorem, since that term itself is used only in connection with quantum theory. Peres, who you cite, has it right here. Since Bell's theorem only refers to the results of experiments and their correlations, he makes no assumptions at all of any kind about the theory predicting those results, save that it is local. His theorem does not apply to "energy exchange physics" because in this setting the energy exchange would not be a local process, and the theory would not be local. It is therefore not a counterexample to Bell's theorem.

    Tim,

    "If I now enforce global energy conservation, so that the energy that disappears from one side must appear on the other space-like-separated side..."

    Where does he say that? A particle need not refer to a point exterior of itself to know its initial orientation to its state of motion. That is clearly implied by our definition of inertia globally, regardless of relative local energy transfers. If you are in a closed spacecraft intergalactically and the interior appears to be tumbling around you, is it? Gently, jrc

    Dear Edwin,

    Thank you, your reply deserves a careful and thought-out response. Unfortunately, the next couple weeks or so will be very busy for me, so let me just say that I wish to continue our discussion, but there will be a little time lag time before I have a chance to fully engage in it. I do want to do it because this may well be one of those (relatively rare) kinds of discussions where both parties can learn from each other.

    Best wishes,

    Armin

    Rob,

    Thanks for your reply. You confirmed my last comment, as I was sure you would. You are effectively ignoring the QM assumption of a 3-component vector by replacing it with your own 1-bit interpretation of reality.

    Thus all your arguments are based on your own idea of 1-bit events that match your fixation on Shannon and agree neither with the quantum mechanical interpretation nor with my local model. As your results will never agree with the 3-D realistic world we can only agree to disagree on spin.

    I still find your view of superposition generally compatible with mine and hope to address this later, but there's no point in responding to the details of your above comment because they concern a different model of reality.

    Thanks very much for your clarification,

    Edwin Eugene Klingman

    Dear Tim,

    Thanks for reading my essay and responding. As I understand your comment you make three points:

    1. Global energy conservation across space is non-local.

    2. Bell's suppression of theta physics is illustrative, not basic.

    3. Bell's theorem is about any theory, not just quantum mechanics.

    If I understand you correctly, you state that global conservation (compatible with the perfect anti-correlation case) will have consequences for what is observed, but is not local in Bell's sense.

    Then you claim that "if I now enforce global energy conservation, so the energy that disappears from one side must appear on the other space-like separated side, then the theory is not local in Bell's or Einstein's sense."

    While this is probably a true statement, it has nothing to do with my model, in which there is no hint of energy disappearing from one side and appearing on the other.

    My model assumes local conservation of energy; (which, I believe, generates global conservation of energy,) energy does not "disappear" locally. It transforms, which is the meaning of my Energy-Exchange theorem. The precession energy, which locally is transformed into deflection energy is not "lost" locally. It is converted into deflection energy, and can be measured by the position measurements that Stern-Gerlach performs, yielding the initial angle that spin makes with the local field, which is the "hidden variable" in my model.

    You also claim that Bell's suppression of this theta physics is merely an illustrative case, and not part of his theorem. While technically this may be true, it is a de facto result of the constraints he imposes in his theorem, and it also illustrates his thinking that underlies his model. The results are the same, whether one considers the suppression of theta a basic assumption or a consequence of another basic assumption.

    As for your statement, which agrees with Peres, that Bell's theorem is about any theory, whether the theory uses quantum mechanical formalism or is a completely different formalism in which there is no talk of eigenstates or eigenvalues, I would ask you to explain just how the +1 and -1 constraints show up in a non-quantum-mechanical theory.

    To summarize the 3 points:

    1. is a mistaken interpretation of my model.

    2. the logic is the same whether theta suppression is a basic assumption or follows from another basic assumption.

    3. is an editorial point, and has bearing on the logic of my argument only if you can explain why 'any' theory must erase information in a way that mimics imposition of QM eigenvalue constraints.

    Finally, I sincerely thank you for stating that if my model is local then I have shown a flaw in Bell's reasoning. You claim my model is not local because "energy-exchange physics" is not local. But that is mistaken because the energy exchange in my model is completely, 100%, local.

    Thanks again for your consideration,

    Edwin Eugene Klingman

    Dear Joe Fisher,

    Thank you for your kind comments. I am in general agreement with the point you have been making for several years now, concerning the integrity and unity of reality. I also agree with your focus on the abstraction implicit in Gisin's statement. By the way, I was not agreeing with Gisin, but used his statement to underscore the view that Bell's theorem has propagated. While I agree with you that reality is a single entity, it is an entity that supports local causality, Bell's oversimplified arguments notwithstanding.

    Thanks again for your comments; I appreciate them.

    Edwin Eugene Klingman

    Edwin,

    It is true that 1-bit events do not agree with the standard quantum mechanical interpretations. But they do agree with both classical and QM observations. That could be just a marvelous coincidence, but I think not.

    Best Regards,

    Rob

    Dear Edwin Eugene Klingman

    I hope you will forgive me for not commenting until now after your comment on my essay.

    Bell's theorem, EPR, Bohm's suggested experiment, the 1982 Aspect experiment, all seem very interesting to me. Your essay indicated there are interesting conceptual issues still outstanding regarding entanglement. Although I have some familiarity with Korzybski's general semantics (you refer to him on page 1), I do not feel I know enough about QM to comment on the math in your article.

    You write: (p. 2:) One must apply the right map at the right place. You quote: "Complex problems have simple, easy to understand, wrong answers." (P.2).

    My comment: Maybe (and I wonder if this might be the case) entanglement would be a simpler problem with an easier to understand solution in a different conceptual reference frame. That seems to be an implicit possibility raised by your article.

    Thank you for your article, and all your comments on the various essays.

    Best wishes.

    Bob Shour

      Dear Bob Shour,

      Thanks for looking at my essay and responding. Let me take this opportunity to say again how refreshing I found your essay, and how novel your points.

      As you note, Bell's theorem and associated physics and philosophy are quite interesting, but significantly complex. That is why Bell's oversimplified model has stood for 50 years. As I have pointed out, if Bell had simply said, "My simple model does not work," there would be no problem. But Bell attempts to overthrow our intuitive understanding of reality and replace it with a mystical connection. The mere fact that one can graphically illustrate 'entanglement' as the shaded area in the graphic at the bottom of page 6 does not in the least detract from the inherent mystical nature of entanglement.

      Of course you may be right that entanglement might be easier to understand in a different conceptual reference frame, but I have no idea what this frame might be, and I am aware of no suggestions as to what it might be.

      The gist of the matter is that physicists have interpreted Bell to mean that "no local model can yield quantum mechanical correlations between remotely conducted measurements." I have produced a local model, based on classical physics, that does produce this correlation unless the local information is erased, as is required by Bell. As 'entanglement' represents the difference between the quantum mechanical cosine curve and Bell's (constrained) 'local-model-based' straight line, if a local model can agree with quantum mechanics (and real experiments) then the shaded difference disappears and the very rationale for entanglement vanishes.

      Thanks again for your kind remarks, in my best wishes to you.

      Edwin Eugene Klingman

      Dear Sir,

      You have rightly quoted Korzybski to say that math is the map and the physical world is the territory. But the map is not "any" territory - it describes the physical boundaries of a specified territory. This is what we say mathematics is not the sole languages of Nature, but only exhibits its quantitative aspect. We may have many "maps" of the universe, but each represents different features. Geometry, the mathematics of maps, always relates to two or three dimensional fields or structures, where the mathematics is always non-linear (distance is linear and its calculation is not geometry), even though both lead to perception of relations and patterns. Problems arise when we treat fields to represent integers. Fields are always analog, whereas eigenvalues are always discrete. The processes are dynamical, because all mathematical operations involve dynamics of the constituents. You have also said "the eigenvalues are generally taken to be truly representative of the system". Analog fields cannot be the sole representation of integers, as numbers are discrete and linear. The unit makes them non-linear. You also imply the same thing when you say: "Once a counter produces a number, another machine can add (subtract) this number to a different number to yield a new number".

      We prefer mathematically simple theories to complex ones because Nature is economical. All thermo-dynamical processes lead to entropy to finally reach equilibrium. Each step takes the minimum energy to evolve in time subject to what you call as eigenvalue maps. Two spin eigenvalue maps differ because they are different or as you quote Messiah: "the initial states are statistically distributed over a somewhat extended domain".

      You are right that a local model does produce correlation, based on energy-exchange physics. But when we analyze the underlying physics, some assumptions of quantum mechanics become questionable. A statistical model cannot ensure that all relevant parameters have been woven into it simply because our measurement processes are unitary - we measure limited aspects of a system over limited time. Generalizing the result of such measurement is fraught with the dangers of embracing uncertainty. As we have often said, uncertainty is not a law of Nature. It is the result of natural laws relating to measurement related to causality that reveal a kind of granularity at certain levels of existence. Since time evolution is not uniform, but conditional on interactions, we do not see each step from the flapping of the wings of the butterfly till it turns into tempest elsewhere. The creation is highly ordered and there is no randomness or chaos. We fault Nature to hide our inability to know.

      For example, contrary to general belief (especially with reference to EPR), entanglement does not extend infinitely, but breaks down after some distance like a rubber string. Or it may remain exclusively like a pair of socks, though used only in pairs. Energies behave like a pair of socks - they co-exist. Interdependence of every system in the universe with all other systems makes one 'energy' to act, when a 'related energy' acts. This is not truly energy exchange. This principle also applies to your model, which Bell suppressed. Because of interdependence, no local model could reproduce the quantum mechanical prediction based on limited data over limited space and time. This is what Bell tells the hidden variables. Your constant field shows local equilibrium. The inhomogeneous field shows interdependence, which, as you say, can cause transitions. When Bell says: "No physical theory of local hidden variables can ever reproduce all of the predictions of quantum mechanics", he ignored this interdependence.

      Congratulations for presenting a complex model in fairly simple manner. We have clarified your comments in our post.

      Regards,

      basudeba

        Dear Edwin,

        To say that it is "de facto true" that Bell's example about spin is just illustrative and no part of the theorem does not address the point. The entire discussion of the detailed model makes no contact with the theorem. The theorem holds of any theory at all that is local (in the sense Bell articulates) and makes certain statistical predictions. That these are predictions about anything called "spin" or anything treated quantum-mechanically is no part of the theorem at all. All one needs are the conditional probabilities for outcomes of certain experiments, which need not be described in any more detail than "Instrument 1 is set to setting A" and "the outcome is outcome 1" or "outcome 2" One can use "spin measurements" in quantum theory as instances of this sort of thing, where the setting is the orientation of the Stern Gerlach magnet and the outcome is a spot on a screen appearing in one place or another. Clearly any theory at all might make such predictions. Since the theorem is only about these sorts of conditional probabilities, it is in no way "about" quantum theory.

        Your initial characterization of the question Bell was asking is not accurate. He was not asking whether one could somehow find a theory that predicts the outcomes of experiments deterministically, he was interested rather in whether any local theory at all (deterministic or probabilistic) could recover a certain set of predictions. He insisted on this many times, and complained that his point had been almost universally missed. In fact, the paper relies on an understanding of the EPR argument, which had already established that locality can only be recovered in a situation with perfect EPR correlations if the theory is deterministic, but, as Bell says, "It is important to note that the limited degree to which determinism plays a role in the EPR argument, it is not assumed but inferred. What is held sacred is the principle of 'local causality'-or 'n o action at a distance'. Since the EPR correlation are recoverable by a local theory only if it is also deterministic, one can then ask about constraints on such theories. Bell demonstrates such constraints.

        On p. 4, you list what you call "Bell's key physical assumptions". None of these are assumptions or premises of his theorem. The theorem applies to any situation in which the outcomes of certain experiments can be categorized as, e.g., "outcome 1" or "outcome 2", and correlations between the outcomes on different sides predicted. The theorem, which is not particularly about spin, has none of these assumptions as premises, so no discussion of them can have any significance for the theorem.

        What is particularly odd about your presentation is that you claim that Bell has a "hidden constraint" in his proof, but nowhere actually discuss the proof itself, but rather only the illustrative example. It would help if you would actually point out where in the proof the supposed constraint appears. Your rather extensive discussion of the toy model makes no direct contact with the theorem itself.

        As for your own model, let me try to understand the claim that you make. Your equation 4 has the consequence, as you say, that the deflections produced by Stern-Gerlach magnets will not be quantized, that is, that we cannot, as a practical matter, distinguish the outcomes into two classes, usually denominated "spin-up" and "spin down", determined by the location of the detected particle. If that is correct, then your model certainly does not reproduce the actual phenomenology reported in the lab, nor the predictions of quantum theory. Since the correlations discussed by Bell are correlations between the outcomes on the two sides, which are taken to always be either "spin-up" or "spin-down", and since these are also the predictions of quantum theory, then it would appear that your model actually makes no contact with Bell's topic. You do not explain how the top graph on p. 7 was created, or even what it means. Here is a key sentence from that page: "If I throw away this θ -information by truncating the measurement data, i.e., setting the results to A, B = ±1 , my constrained model cannot produce the correct correlations." The obvious reading of this sentence is that in your model, the outcomes of the experiments are not categorized into two classes, spin-up and spin-down outcomes, and that if one requires such a categorization of the outcomes then you get Bell's result. But it is an observed fact that the outcomes do sort into these two classes, and it is a prediction of the quantum theory that they will, and furthermore if they do not then it is not at all clear what the meaning of "correlation" in your theory is, since the predicted correlations are between these binary results. So you it would help if you could do these things:

        1) point out where the supposed "hidden constraint" actually appears in Bell's theorem.

        2) Explain, if your model does not predict quantized outcomes for spin experiments, what bearing it has on quantum theory, or Bell's theorem, and what you even mean by a "correlation" between the results on the two sides.

        Regards,

        Tim

        Hi Edwin,

        I congratulate your professionally written essay.

        In another thread you said:

        "I built first in my mind and then built a theory around. I believe modeling physics in your mind and then describing it mathematically is to be preferred to studying math and trying to guess what physics it describes. I believe that much math does not describe 'reality' in the same sense that much fantasy and fiction do not describe reality."

        I agree with this statement completely. I followed this procedure to formulate Model Mechanics. Although we have different models of reality, but that is to be expected.

        I believe that there are many assumptions in relativity are wrong. Specifically the idea of Relativity of Simultaneity (RoS). Why? Because it is in conflict with the idea that the speed of light is isotropic in all frames.

        Regards,

        Ken Seto

          Tim,

          Is it your contention that an experiment must result in only outcome A or only outcome B, to be a valid experiment?

          The excluded middle in the spin operator Bell employs constricts vectors to ether parallel or perpendicular to the eigenvector of results. Lambda is constrained to +or- 1 by the artifice of the form of the set of three intervals being mixed half-open and closed. The final sign element is left open ended for the simple expedient of breaking symmetry, but wholly arbitrarily so at 'less than' (however infinitesimally) 180 degrees for either plus or minus rotation; lambda = 1(pi). A different choice of spin operator might conceivably have a form that would produce |0=

          Tim,

          sorry, my post got chopped. I'll continue...

          The point being that Bell's choice of operator was the standard of the industry at the time, which he tried to find a way around. A spin operator of a form producing a continuous relation |0=

          Dr. Klingman, if you will send your email address to genebarbee@msn.com, I will send you an excel spreadsheet with all of the meson and baryon energies and decay times almost perfectly matched.

          OOPS,

          the server is interpreting symbols as commands....

          ...A spin operator with a form producing a continuous relation of equal to or greater than zero, but lesser than 360 degrees, would still break symmetry at 2(pi) being a half-open interval, and the congruent +or- rotations would zero out. The lambda plotting perpendicular to the eigenvector would not experience any growth whether being set at 1 or less than 2. But the dispersion of results would plot different from the typical Bell thin cigar. And in conjunction with the Theta deflection could be expected to produce cluster results for +and- plots which if juxtaposed would approximate the real physical split dispersion pattern of detections in the original Stern-Gerlach experiments.

          I think this is the general point Dr. Klingman's arguments illuminate. Bell cannot be said to generalize to any and all theoretical predictions. Only those which obtain results in the form of only outcome A or only outcome B.

          I don't see John Bell as having been politically niave. He certainly didn't believe the universe to be binary, or reality to be 2-D Hilbert space. He exposed a dichotomy. He was simply being shrewd. jrc

          Dear Tim,

          In the interest of full disclosure, I should probably mention that when I sent you the 130 page precursor to my essay, detailing the local spin model and the Energy-Exchange theorem upon which my model is based, I did not realize that you had written a recent book explaining Bell's theorem and thus my model conflicts with your book. I know this would not cause you to obfuscate or distort my arguments in any way, but readers of the comments can at least realize what is at stake here.

          You are apparently implying that Bell did not have any physics in mind, or any quantum mechanical eigenvalue equations, and made no physical assumptions in analyzing EPR, Stern-Gerlach, spin, and QM correlations, despite that he discusses all of these in detail in his papers, and despite Bertlmann's statements to the contrary. Readers can decide whether this makes sense.

          Your first claim above was that my energy exchange model is global, but as you no longer mention this I assume you now realize it is a local model.

          So let me simply use your terminology. You state that Bell merely assumes an experiment in which there are two outcomes, outcome 1 and outcome 2, plus a probability distribution for outcomes. No constraint should be imposed other than local causality. That is exactly what my local model does.

          One experimenter, Alice, selects control variable a, and the theory ('any' theory, as you state) should yield either outcome 1 or outcome 2, based on actual EPR splitting observed. Any model actually based on physics will use her setting plus the local physics (denoted by lambda) to produce outcome 1, denoted by +A(a, lambda) that belongs to class 'up' or outcome 2, denoted by -A(a, lambda) that belongs to class 'down'. As is both obvious from the SG data and according to a standard QM text at the time, each class is "statistically distributed over a somewhat extended range". [See p. 3]

          Bob's remotely operated experiment also yields two similar outcomes +B(b, lambda) and -B(b, lambda) which are based on the physics of the (any) local physical theory under consideration.

          Then, as you note, Bell takes the correlation between the outcome of the two sides (in pairwise fashion) using the standard formula for expectation values. The standard formula, applied to my model's local outcomes, and plotted against the angle between Alice's and Bob's control settings, yields the top figure on page 7, exactly as predicted by QM. This is the cosine curve -a.b that Bell claims to be impossible for any local theory.

          Now you ask where in his theorem do Bell's constraints appear. They appear in his first equation (1) where he states that +A(a, lambda) must equal +1, and -A(a, lambda) must be constrained to -1. There is no valid reason for these constraints, as they have the effect of throwing away the actual physics applied by (any) physical theory. I have explained why he erases this information in my essay and in more detail in my reference [4].

          It is Bell's constraints, imposed on any local physical theory, that results in failure to match QM predictions. My local model does produce QM predictions.

          Your use of 'toy model' is also incorrect, as toy models are 'reduced dimension' models. My model is full 3D and is a real physical model. Your statements about 'spin up' are also misleading, as I have explained in detail in reference [4]. In short, my model does predict quantized outcomes for spin, but the outcome of the experiment is not a direct measurement of spin, but a position measurement that reflects the physics of the spin scattered by the inhomogeneous field. Failure to recognize this has led to 50 years of non-intuitive nonsense about non-locality.

          Regards,

          Edwin Eugene Klingman

          Hi Ken Seto,

          Thanks for your nice comment. Based on your essay I'm not surprised that you agree that modeling physics in the mind and then describing it mathematically is to be preferred to searching for physics in mathematics. It is hard to think of any significant physics that was not found in this way.

          As for your comment about special relativity, have you seen the following:

          ">Scientists slow the speed of light](https://www.bbc.com/news/uk-scotland-glasgow-west-30944584

          )

          The arXiv paper is here: Photons slower than speed of light

          This may shakeup things, but then, some things certainly need to be shaken up.

          My best regards,

          Edwin Eugene Klingman

          Dear basudeba,

          Thank you for reading and for your fine comments. I will address specific statements. You recalled Messiah's quote that "the initial states are statistically distributed over a somewhat extended domain." This fact is interpreted differently according to the two eigenvalues maps usually associated with spin. These interpretations are discussed in detail in Spin: Newton, Maxwell, Einstein, Dirac, Bell.

          Then you note that my local model does produce the correct correlation, based on energy-exchange physics, and remark that some assumptions of quantum mechanics become questionable, as a statistical model cannot ensure that all relevant parameters have been woven into it.

          That is correct, as quantum mechanics does not take note of the initial spins upon entering the field, which determine the scattering or deflection of the particle is it traverses the non-constant field. Thus, as Einstein suggested, quantum mechanics is not complete. This conflicts with the Quantum Credo believed in by many physicists.

          Quantum mechanics is a marvelous statistical machine for those situations in which only certain outcomes occur, with energy-based distribution according to the partition function. In such cases it (apparently) cannot fail to predict the statistical outcome. But it is incomplete and there is an underlying level of reality that quantum mechanics does not see. That is in contrast to the current consensus belief that the classical world is a statistical overlay on QM. I discuss these interpretations on pages 104 - 113 in Quantum Spin and Local Reality

          Thanks for your, as always, informative comments.

          My best regards,

          Edwin Eugene Klingman

          Hi Edwin,

          Doing the math before the physics is the main problem of current string theories. All string theories posit extra space dimensions and there is no experiment to confirms the existence of these extra dimensions.

          Regards,

          Ken Seto