The Nature of the Wave Function by Edwin Eugene Klingman

Edwin

There are so many important truisms in your essay and so densely packed it's hard to pick one out. Waves certainly real fluctuations not metaphysical. Particles key actors in propagation, QM real and local (and deriving relativity). The list goes on.

Do you think 'probability' may just be the incomputability of complex interactions between real waves beyond our comprehension? If Heisenberg considered diffraction related to uncertainty it may be so, and again be just interpretation that's nonsense. If you consider a dozen particles driving along a motorway at different speeds emitting different real waves, could we compute how they interact at any point? But given certain information we can at least arrive at a most 'likely' value at any point and moment. For 'likely' then perhaps read 'probable.' This would fit with my derivation of observed SR effects from a QM. How else would the waves interact in a complex scenario?

Best wishes

Peter

Dear Edwin,

You do seem to have given a clear and well presented argument, though I lack the expertise to comment on its validity. It is relevant as you clearly point out an error in understanding of a physical phenomenon. Your diagrams are nice too.

I found the beginning bit about the evidence for a real wave rather than wave packet very interesting. Also the part about vortices and the aircraft.

I have appreciated your feedback on my various ideas and essay in this contest. I hope you get lots of readers who are able to appreciate what you have written and give it the score it deserves. Good luck in the competition.

Dear Edwin,

you are kind to me. I wish I had the ability to really appreciate what you have written and say something so nice in return. I have read some of the other very complementary comments on this thread, which show that it is my shortcoming and not your essay that is at fault. Good luck.

Hi Edwin,

I really enjoyed this paper -- I could overlook every nit which I question, and come away only with the argument that the wave function is not probabilistic -- and still be satisified.

So I offer the following as commentary, not criticism.

You write: "We can safely ignore wave functions of infinite extent, but all treatments of atomic orbits are based upon the assumption of an integral number of wavelengths--the link that connects wavefunction to both energy and probability."

Measured experimental outcomes are always integral (no such thing as half an event). I was both puzzled and impressed in first being exposed to Joy's framework, that he was addressing a quantum experiment and there was no probability function in it. None at all. It was only after some time that I was able to work out that the absence of a probability function implies absence of boundary conditions at every scale, which implies absence of reference coordinate frame, which can be explained only by a continuous function in a topological model. Eureka, as our friend from Belgium would say.

We also reach Joy's derivation of -a.b by different paths. To me, it's clear in his one-page paper that the result is the reduction to an input argument for a function continuous from a topological initial condition. That's not saying that it can't be derived another way.

Just one more comment, concerning dialogue here with Daryl, and the characterization of solutions to polynomial equations as analagous to superposition -- just shows how differently physicists and mathematicians think. The number of solutions corresponding to polynomial degree are *all* real solutions, not in superposition. That's the fundamental theorem of algebra! LOL!

Anyway -- thanks for a good read, and best wishes in the competition.

Tom

Yo, E.E.K., you asked me, back on the thread of G.F.R. Ellis, F.R.S., to say something here.

I'm afraid I'm far from sure that the mathematics of the QM formalism refers to anything apart from the probability of observing certain quantum events under defined experimental conditions. "Wave function" may be simply an attempt (of precisely the kind Bohr -- yes, I know: hiss the villain -- warned against) to picture that which cannot meaningfully be pictured or diagrammed. Bohr blamed complex numbers and noted that the trend had already surfaced in relativity ... first Minkowski's imaginary time axis, then later the Friedmann universe model adopted by Einstein. QM soon picked up the ball and ran with it.

Micro-wise you first diverge from classical physics with half-integer spin and right off the bat there's a choice: you either accept that a realm of reality exists in which a sphere has the properties of a Moebius strip or else face the possibility that the math you're employing so productively doesn't refer to anything you can concretely envision: its terms are purely symbolic. (Feynman never claimed his diagrams were literal pictures of reality either: they're high-class equivalents of the cheat-notes Sarah Palin jots on her left palm.) Ditto the thing we call Wave Function, this Cosa Nostra.

(Exits hurriedly)

Oh, Bell ...

I know for a fact that BT is NOT violated in macroworld experiments using sets of separable physical objects. It's solid classical mathematical logic, as Venn-diagramming it conclusively proves. So it's sound stuff.

Since it's obviously violated in quantum experiments I accept that quantum ontology is significantly different from classical ontology. I also buy into the idea that we're coarse-grained measuring instruments up here and that's probably why we don't perceive violations.

Hi nmann,

You wrote: "BT is NOT violated in macroworld experiments using sets of separable physical objects."

How on earth do you know that? There has never been a single experiment carried out to check what you are claiming. In fact I put my last penny on my claim that Bell-CHSH inequality would be violated as strongly in the macroworld as it is in the microworld, provided an appropriate experiment in the macroscopic domain is carried out. Below I am attaching a proposal for just such a macro-experiment. This proposal also appears as Chapter 3 of my book.

I categorically claim that if my proposed experiment is carried out, then the violation of Bell-CHSH inequality would be confirmed in the macroworld and Bell's theorem would be finally put in its rightful place---i.e., in the graveyard.

Joy ChristianAttachment #1: 32_0806.3078v2.pdf

Joy Christian:

Material similar to this has been around for decades. We used to try violating BT as a game. We'd use letters in words in blocks of text. Bunches of coins or keys, or coins and keys together. Food containers pulled at random from kitchen shelves. All you do is define your set, select three characteristics applicable to the set members that can be answered Yes or No (longer than, shorter than, lighter than, heavier than, boxed or not, tinned or not, picture of product on container (or not) ... use your imagination. Set up your truth table and go for it.

http://www.upscale.utoronto.ca/GeneralInterest/Harrison/BellsTheorem/BellsTheorem.html

I'm too lazy to follow the proper link protocol. Now ... BT can be "violated" macroscopically by simulating entanglement, the probably most notable example of that trick being Dirk Aerts' two-vessels-connected-by-a-tube gedanken. (By the way, he says he contacted you once re: algebra but you were too busy fighting off the attacks on one of your early papers to be of help.) It's not the same thing as a genuine violation, however.

Hi nmann,

Thanks for the link. I do not want to pollute Edwin's blog space with our own private discussion, but let me make two quick remarks: (1) I do not recall being contacted by Dirk Aerts. I think I would have remembered and responded. Perhaps there was some communication problem. (2) I do not mean the kind of violations of BI you mention. I mean genuine violations using the correct macroscopic analogue of the microscopic EPR correlation. That is what I have proposed in the paper linked above. But thanks anyway for your comments.

Joy

Joy,

Dated 21 July 2008, part of an online discussion (on GUTalk, now defunct) of "The Violation of Bell Inequalities in the Macroworld". I pretty much facilitated the whole thing by first mentioning the paper and then dragging him into the resulting debate. (I told him people were calling him silly and crazy. As in fact they were. That piqued his interest. He's a fine gentleman, BTW.) You and others here might find this interesting in general:

"Yes, I have read Christian's work. It is, in my opinion, a good example of seeing too much the mathematics and not the rude engineers-like physics reality. One is not in the first place interested in the signs of observables with respect to the Bell-inequality situation, but in the (ordinary) probability of outcomes. By the way, Marek Czachor and myself contacted Christian with respect to his model when it appeared on the archives a year ago, most of all because we also are working with Clifford Algebra's (using them to built a computation with all the advantages of quantum computation but without the need of quantum structures in Hilbert space, see for example http://uk.arxiv.org/abs/quant-ph/0611279 ), but he is very much struggling defending his stuff at the moment (see his reactions to some of the critiques). Now, what he does is interesting, but for a different reason, namely Clifford Algebra structures indeed manage to capture some of the quantum structure, which is also why we have been able to use them for a kind of quantum-like computation. It remains hence an interesting question, since Clifford Algebra structures refer to classical geometric structures in physics, in which way this may lead to getting a better grip on the way that some of the quantum structure can also be found in ordinary geometric structures of macroscopic reality. However, I don't think it will be in the way that Christian puts forward in these recent papers, and it is my guess that Bell's theorem is not touched by it for what it means for the nature of reality with respect to locality and hidden variables."

nmann,

Interesting discussion. Yes, Marek Czachor did get in touch with me just after my first paper on Bell came out back in 2007. Dirk's comments about my work, however, are outdated and miss the point about my program. Unfortunately he is not the only one to miss the point. My program is misunderstood by many, including some of its supporters. I urge you to read at least the one-page paper of mine I am attaching below to see for yourself how outdated Dirk's comments are. More details of my program can be found in the second paper I am attaching. I am taking liberty to attach these papers here with hopes that Edwin won't mind, because he is interested in my work and discusses it in his essay.

JoyAttachment #1: 14_disproof.pdfAttachment #2: 8_Origins.pdf

I am very concerned about my argument against Bell's theorem being misconstrued even further than it already is. Therefore---at a risk of displeasing Edwin---let me reproduce my comments on his essay here from the "Disproofs" blog:

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Dear Edwin,

Thank you very much for discussing my work in your essay and citing my book and a paper. I have just looked at it very briefly. You have discussed your ideas very clearly, and with beautiful pictures.

I am sorry to say, however, that your argument against Bell does not address his concerns, as far as I can see. In particular, your model does not satisfy his "free will" requirement (i.e., the requirement 6 among the 8 requirements I have listed in Chapter 5 of my book). According to his "free will" requirement Alice and Bob should be completely free to choose any measurement directions at will, for each run (or trial) of the experiment. To show you why your model violates this requirement, let Alice and Bob choose to keep their respective measurement directions *fixed* for all runs of the experiment. They are perfectly entitled to do so under the "free will" requirement. But then your model cannot reproduce the correlation -a.b, since it depends on Alice having chosen a smaller angle than Bob's chosen angle for one half of the runs of the experiment and a greater angle than Bob's chosen angle for the other half of the runs of the experiment. This also makes the model non-local. For how is Alice to ensure the 50/50 balance without knowing which angle Bob has chosen for all runs of the experiment? You cannot simply hope that the balance will turn out to be 50/50. There has to be a mechanism (or "common cause") in the model that ensures that balance.

In short, your model is not a counterexample to Bell's theorem, or a local model for the EPR correlations. It is not that easy to construct a counterexample to Bell's theorem. In fact it is very nearly impossible.

I nevertheless wish you good luck with your essay, for you have discussed many other things besides Bell's theorem. I am sure they will turn out to be both interesting and valuable to many.

With best wishes,

Joy

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tom :) I am happy to have friends.

You know the domains , universal are so essential ! How can you have a correct superimposing if the foundamentals are forgotten? The parallelizations must be analyzed in the continuous function with specific limits and series .The simulations and the predictions are correct if and only if all the datas , encoded are dterminsitic respecting all our foundamental laws at all 3D scales.

The fractalization of an universal finite serie is a finite serie, with only an infinite when we add or multiplicate this serie of uniquenss.After all, it depends of what we want to explain.

Edwin, I don't agree about what you said. The maths and physics are the same, the universal essence and its distribution of numbers is in harmony when the mathematical tools are utilized with the most important rationalism. The maths help for a real understanding of our physical laws. These two topics are unified and in harmony.The maths are inside this physicality! It does not really exist differences between maths and physics. An anti thesis is just like a symmetry. Like when we see our face in the miror, it exists only one singularity and its codes...

Regards