Gull and Gill's theory

Foundations of physics and/or philosophy of physics, and in particular, posts on unresolved or controversial issues

Re: Gull and Gill's theory

Postby gill1109 » Fri Nov 06, 2020 7:06 pm

local wrote:
gill1109 wrote: At least, it further reduces the set of “Joy Christian believers” to a tiny cargo cult.


Of course, maybe they are right!

This stuff is why you have zero credibility. You acknowledge that “Joy Christian believers” (already a slur) may be right, but you have no problem dismissing it as a "tiny cargo cult". Shame on you!

But if Joy Christian talks about “Bell believers” that is not a slur? If he talks disparagingly about statisticians, that is not a slur? Don’t feel insulted. Don’t take it personally. Wear the epithet as a badge of honour!

Karl Hess discovered that though there are many people who believe that Bell was wrong, they cannot agree with one another. They each go off on their own track. That’s just the “state of play”. Time for something new. We should take a look at what Tim Palmer and Sabine Hossenfelder are doing. Understand how it is related to what Bell’s work tells us.

But anyway - this thread is about computer science (distributed computing, with classical computers). Gull, and earlier Gill, argued that a certain distributed computing task was doomed to failure. The fastest way to prove us wrong is to come up with a computer simulation of two separated computers, each receiving inputs (setting angles) from two outside experimentalists. Computer A receives an input file (list of setting angles), and generates an output file (list of +/-1’s). Computer B, idem. After the two computers have independently done their work, the output data is analysed. Note: inputs come from outside. Data analysis is done outside.

You may ask: where is the source of the pairs of photons or electrons or whatever? Where are the local hidden variables? My answer is, they can be written into the programs of both computers A and B, at the outset. Suppose for instance you have figured out separate physical mechanisms involving separate, local, random processes at a source, in the transmission lines from source to A and B, at the detector A, and at the detector B. You’ll program these using pseudo random generators. Well: put all the needed pseudo random generators into one program. Fix the parameters of the generators, and the initial seeds of the generators, as constants, in the initial definitions and declarations of the program. You run the same, completely deterministic, program, on both computers A and B. You just flip the outputs of computer B so that with the same list of input setting angles, the two computers produce lists of equal and opposite outcomes, instead of equal outcomes.

If you want to see different outcomes for the same inputs, you write a different RNG seed into the header of the program, and you recompile it.

So to prove Gill and Gull wrong, you don’t even need to do complicated simulations of computer networks. Just write one program, which we will use twice: once to simulate source plus detector A, once to simulate source plus detector B. The second time, we’ll flip the outcomes. We won’t tell you in advance what the two input lists will be. We reserve the right to run the same program many times with varying inputs. We will check that it satisfies the specifications. For each n, n’th output depends only on n and on the n’th input. Same inputs -> same outputs.
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Re: Gull and Gill's theory

Postby FrediFizzx » Fri Nov 06, 2020 8:28 pm

gill1109 wrote:
FrediFizzx wrote:
gill1109 wrote:
FrediFizzx wrote:You have NO proof so it can't be a theorem. It is now just a theory. But if Nature does in fact do it, then your theory is most likely shot down.

Please read my paper. It’s been on arXiv for 19 years, it’s been peer reviewed and published for 17. The main result has been improved, sharpened, both by myself and by others. It was used in all four 2015 loophole free experiments. The experimentalists cited my work and acknowledged my contribution.

Nature does it, using quantum entanglement.

Sorry, Jay Yablon shot down quantum entanglement with his successful demonstration that QM is local for the EPR-Bohm scenario. So, you really should get off that nonsense. All the experiments do is validate QM. Nothing more since ALL the "proofs" of Bell's junk physics theory are shot down.
.

Jay redefined “local”. He is not the first to resolve the problem in this way. ...

You sure do love spewing nonsense. Jay's measurement functions are 100 percent local. You probably don't even understand how Jay did it or even have read his paper. Tell me what equation numbers I'm talking about and I will explain it to you.
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Re: Gull and Gill's theory

Postby FrediFizzx » Fri Nov 06, 2020 8:37 pm

gill1109 wrote:
FrediFizzx wrote:
gill1109 wrote:
FrediFizzx wrote:You have NO proof so it can't be a theorem. It is now just a theory. But if Nature does in fact do it, then your theory is most likely shot down.

Please read my paper. It’s been on arXiv for 19 years, it’s been peer reviewed and published for 17. The main result has been improved, sharpened, both by myself and by others. It was used in all four 2015 loophole free experiments. The experimentalists cited my work and acknowledged my contribution.

Nature does it, using quantum entanglement.

Sorry, Jay Yablon shot down quantum entanglement with his successful demonstration that QM is local for the EPR-Bohm scenario. So, you really should get off that nonsense. All the experiments do is validate QM. Nothing more since ALL the "proofs" of Bell's junk physics theory are shot down.
.
...
Nobody has found errors in the mathematical proofs that the networked computer simulation is impossible. ...

LOL! You have no proof. Gull was your last chance at any kind of proof. So, they are all shot down. And it is pretty foolish of you to be making a 64,000 euro bet when you have no proof. :mrgreen: Look how complicated it was for Perelman to solve the Poincaré conjecture. It is just a very complex problem to solve but someone will eventually shoot down your theory.
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Re: Gull and Gill's theory

Postby Austin Fearnley » Sat Nov 07, 2020 7:25 am

FrediFizzx wrote:
Austin Fearnley wrote:What a shame! There ought to be a mathematical law against it (against Heinera's point). Gull presumably thought so?

Functions A and B, if they were to exist, need to be step functions as the measurement outputs are 1 or 0 {or 1 and -1}. For example, "measurement A = 1 if particle vector > alpha degrees else A = 0". So you have an average of products of two step functions in the p++ cell of the 2x2 results table of a Bell experiment. It seems easy to sympathise with Gull in assuming (if that is what he did) that you cannot model such an angular 'curve' (composed of step-function products) using only two terms of a fourier series.

Is there no way of showing that the products of step functions are straight lines? The classical correlation is the sawtooth curve, 2*θ/π -1, which is a straight line in (0, pi/2). The value in the first cell of the 2x2 Bell results table is also proportional to θ.

The Fourier series in Wolfram for θ (that is for a straight line) gives
iexp(-iθ) - iexp(iθ) - (1/2)iexp(-2iθ) + (1/2)iexp(2iθ)
+ (1/3)iexp(-3iθ) - (1/3)iexp(3iθ) etc ... with many terms...

It seems very anti the spirit of Fourier (but what do know as I learned it in the 1960s and haven't used it since) to take one 'straight curve' and fit an infinite number of Fourier component curves to it to get a good match asymptotically ... but then to worry that we could have found a match with just two Fourier curves if only we knew those two curves.

It seems essential to show that an average of products of step functions is a straight line? And afterwards, is it only intuition that you need a lot of Fourier terms (>>2) to model a straight line?

Well, the problem I'm seeing with doing simulations is the sign function. Which is basically a step function. The sign function is essentially a linear function. So, I have been trying to think of a novel way of generating the +/-1 outcomes using a function that is not so linear.
.

A good point. But first some general discussion of why we are doing this.

Bell's Inequalities cannot be broken in R^3/flatland. The Bell Theorem says so and, moreover, I have run simple simulations using random particle spin directions together with step functions for measurements and cannot beat correl = 0.5 for theta=45 deg for large numbers of pairs. Getting nowhere near the QM correl of 0.707.

My own solution is by using a communication loophole via antiparticles travelling backwards in time. This enforces measurements on particles to be made on polarised beams. Note that there is some use of backwards-in-time effects for antiparticles in QED but always with the proviso that there is no genuine backwards causation.

Polarised beams are what are inputted into Malus's Law experiments. That leads to needing to know the difference between polarised (non-random) and unpolarised (random) beams for use in a Malus simulation: that is, in a regular forwards-in-time simulation. Anyway, I simulated a Malus experiment using (my own) classical formulae for polarised beams and obtained results agreeing with Malus's Law. To do that, I used a step function for measurements but incorporated a random element before applying the step function.

As I obtained Malus results in my simulation I assume that nature uses polarised beams and step functions and some specific randomisation in a Bell experiment (and a backwards-in-time nature of antiparticles).

If one uses completely random particle spin directions then one has no freedom to use randomness in the step function. Randomness (in large runs) usually leads to noise and lowering of a correlation (via attenuation). And one does not want the absolute correl value of 0.5 to drop any lower than it already is. But using polarised beams together with randomness gets 0.707 for the Malus correlation.

The Malus intensity for electrons measured at a polarising angle of 45 deg is cos^2(45/2 deg) = 0.8536. Further, dividing by 2 gives p++ [that is because Bell uses a 2x2 table of results while Malus uses a 2x1 table]. This corresponds to the term (1- correl)/4 in the 2x2 Bell results table in the Gull paper. So Bell correl = 1- 4*(0.8536/2) = -0.707. So the Malus intensity is equivalent to the magnitude of a Bell correlation coefficient.

So IMO there is little point in trying to add randomness in a large N simulation using random particle spin directions. Richard seems to have added randomness of some kind in his feb 2020 paper on spinning chaotic coloured disks but I am not sure of the purpose.

I gave, in my June 2020 vixra paper, the VB code for adding randomness to the step function measurement. I still have two variants of how to interpret this randomness. One of them is something new to me and gives me a physical insight of why there are only two different spins after a measurement: say up and down. In this the up spin is pointing mostly up but also points anywhere in the 'up' hemisphere. The spin directions fit a statistical distribution.

Having the full statistical distribution information in each polarised particle means that one can get polarised effects particle-at-a-time with slowly released particles.

A Malus experiment has no entangled pairs but still produces the Malus intensity equivalent in magnitude to the Bell correlation. This shows that entanglement need not be causing the Bell correlation in a Bell experiment. All you need to know for a simulation is whether you have a +hbar/2 polarised particle or a -hbar/2 polarised particle after the intialising polarising filter (say Alice's). Alice's polarising measurement on the antiparticle classifies and records whether the spin is +hbar/2 polarised particle or -hbar/2. That spin is passed on to the pair partner particle via entanglement at the source/oven. The exact spin vector is not relevant (to Malus or Bell) as all the information required for a QM measurement by Bob is stored within +hbar/2 or -hbar/2 as long as these particles are polarised appropriately. And backwards-in-time antiparticles do polarise these particle partners appropriately.

There seems to be some idea that all Bell loopholes are cheating strategies. As you have often wrote, the Bell Inequalities are likely not broken in nature and IMO that means nature uses a Bell loophole.
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Re: Gull and Gill's theory

Postby local » Sat Nov 07, 2020 9:55 am

Austin Fearnley wrote: Bell Inequalities are likely not broken in nature and IMO that means nature uses a Bell loophole.

If the inequalities are not broken in nature, why is a 'loophole' needed?

One school of thought asserts that -a.b cannot be obtained in space-like separated EPRB (for normal 3D space), and that the experiments claiming to show it are all wrongly designed, implemented, and/or interpreted. You can pile up as many stupid and/or fake experiments you like; it doesn't make separated -a.b any more plausible.
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Re: Gull and Gill's theory

Postby gill1109 » Sat Nov 07, 2020 10:05 am

Austin Fearnley wrote:Richard seems to have added randomness of some kind in his feb 2020 paper on spinning chaotic coloured disks but I am not sure of the purpose.

There is no randomness in the model, beyond the hidden variable, which is the orientation of the disk. I just generated lots of models of this type (coloured disks) by sampling the parameters of the model. https://arxiv.org/abs/1312.6403, https://www.mdpi.com/1099-4300/22/3/287
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Re: Gull and Gill's theory

Postby gill1109 » Sat Nov 07, 2020 11:03 am

FrediFizzx wrote:LOL! You have no proof. Gull was your last chance at any kind of proof. So, they are all shot down. And it is pretty foolish of you to be making a 64,000 euro bet when you have no proof. :mrgreen: Look how complicated it was for Perelman to solve the Poincaré conjecture. It is just a very complex problem to solve but someone will eventually shoot down your theory.

I have a proof (which convinces me) that I won’t lose the 64,000 Euro. I put it on arXiv in 2001. I was preparing a bet with Luigi Accardi. He saw my proof and withdrew from the bet. Nobody has “shot it down”. My proof is older and stronger than Gull’s. We don’t need Gull’s “proof”. It would be very exciting if someone blew up my proof. Go ahead and do it! I recommend you learn something about martingale theory first, so you understand what you are up against. You just need to write one computer program for one computer. We’ll just switch the sign of the outcome when we use it to play “detector B”. Remember: you include the RNG and a seed of the RNG in the program so it is completely deterministic.
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Re: Gull and Gill's theory

Postby Austin Fearnley » Sat Nov 07, 2020 11:42 am

local wrote:
Austin Fearnley wrote: Bell Inequalities are likely not broken in nature and IMO that means nature uses a Bell loophole.

If the inequalities are not broken in nature, why is a 'loophole' needed?

One school of thought asserts that -a.b cannot be obtained in space-like separated EPRB (for normal 3D space), and that the experiments claiming to show it are all wrongly designed, implemented, and/or interpreted. You can pile up as many stupid and/or fake experiments you like; it doesn't make separated -a.b any more plausible.

IMO in nature the particle pairs are not generated in random spin directions. That is because of retrocausal effects. So Bell's Theorem is over-restrictive, compared with nature, in its requirements of randomness and is therefore a Theorem associated with loopholes.
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Re: Gull and Gill's theory

Postby Austin Fearnley » Sat Nov 07, 2020 11:50 am

gill1109 wrote:
Austin Fearnley wrote:Richard seems to have added randomness of some kind in his feb 2020 paper on spinning chaotic coloured disks but I am not sure of the purpose.

There is no randomness in the model, beyond the hidden variable, which is the orientation of the disk. I just generated lots of models of this type (coloured disks) by sampling the parameters of the model. https://arxiv.org/abs/1312.6403, https://www.mdpi.com/1099-4300/22/3/287

1. Thanks for the explanation, Richard.
So the use of the coloured disks is to cause a non-uniform random sampling scheme?

2. I saw your paper and it contained a lot of nice pictures of sets of straight lines for the classical correlation!
If it takes an infinite series of Fourier terms to get one straight line then there is not a lot of difference, wrt Fourier Series, between one line and obtaining ten straight lines? Just one infinity versus ten infinities?
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Re: Gull and Gill's theory

Postby gill1109 » Sat Nov 07, 2020 10:19 pm

Austin Fearnley wrote:
gill1109 wrote:
Austin Fearnley wrote:Richard seems to have added randomness of some kind in his feb 2020 paper on spinning chaotic coloured disks but I am not sure of the purpose.

There is no randomness in the model, beyond the hidden variable, which is the orientation of the disk. I just generated lots of models of this type (coloured disks) by sampling the parameters of the model. https://arxiv.org/abs/1312.6403, https://www.mdpi.com/1099-4300/22/3/287

1. Thanks for the explanation, Richard.
So the use of the coloured disks is to cause a non-uniform random sampling scheme?

2. I saw your paper and it contained a lot of nice pictures of sets of straight lines for the classical correlation!
If it takes an infinite series of Fourier terms to get one straight line then there is not a lot of difference, wrt Fourier Series, between one line and obtaining ten straight lines? Just one infinity versus ten infinities?

The coloured disks are just a representation of a zero-one valued measurement function. I explain in the introduction how I start with assuming existence of a hidden variables theory which is to reproduce the singlet correlations. Because of perfect correlation at opposite angles and perfect anti-correlation at equal angles, and because of rotational symmetry, it has to be a spinning disk model. I *assume* the hidden variable is a direction; I *assume* a rotationally invariant model; I *assume* perfect correlation and perfect anti-correlation at opposite and equal measurement directions, respectively. It follows that the hidden variables model is a uniformly randomly spun black-and-white coloured disk model. A kind of fairground spinning wheel of fate. Black and white are always opposite. Half the disk is black and half is white. You pick Alice and Bob’s angles, add pi to Bob’s, spin the disk, and see what colours come up at the two positions picked by Alice and Bob in this way. I argue that up to measurability issues which I consider generalised abstract nonsense (I.e., just word play), I.e., for physical purposes, any coloured disk model must be well approximated by a coloured disk with just a finite number of switches from black to white and from white to white. Bell’s theorem is now easy to prove, in Bell’s 1964 way. You can’t get the singlet correlations in this way. I vastly improved that theorem in my 2003 paper on Luigi Accardi’s chameleon model. Gull offers an alternative line of proof but I have not yet figured out if it can be made rigorous. The theorem is the same theorem always, it’s Bell’s theorem. The question is just can it be proved in other ways than “the usual” way? Can it be strengthened? I strengthened it, back in 2001, in order to show that Luigi’s simulation only worked by cheating.

I was inspired by Caroline Thompson’s chaotic spinning ball model.
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Re: Gull and Gill's theory

Postby gill1109 » Sun Nov 08, 2020 5:32 am

https://aflb.minesparis.psl.eu/AFLB-321/aflb321m555.htmThis is another proof of Bell's theorem, similar to Gull's. It seems to me to be a whole lot more complete.

Annales de la Fondation Louis de Broglie, Volume 32, no 1, 2007, pp 69-76
A New Proof of Bell’s Theorem Based on Fourier Series Analysis
Habibollah Razmi, 37185-359, Qom, I.RR. Iran
Department of Physics, The University of Qom, I. R. Iran
razmi@qom.ac.ir & razmiha@hotmail.com
ABSTRACT. We want to prove Bell’s theorem using Fourier series expansion analysis. Comparing to already known algebraic methods, this is a new calculus-based model. Although the notation and procedure we use here is based on the Clauser-Horne model, the corresponding Fourier series method can be simply applied to different versions of Bell’s theorem.

See also https://aflb.minesparis.psl.eu/AFLB-341/aflb341m641.pdf, "Comment on “A New Proof of Bell’s Theorem Based on Fourier Series Analysis” " by Roderich Tumulka, and https://aflb.minesparis.psl.eu/AFLB-341/aflb341m641b.htm, "Reply to “Comment on A New Proof of Bell’s Theorem Based on Fourier Series Analysis” by Roderich Tumulka", by Habibollah Razmi.
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Re: Gull and Gill's theory

Postby gill1109 » Sun Nov 08, 2020 6:03 am

local wrote:
Austin Fearnley wrote: Bell Inequalities are likely not broken in nature and IMO that means nature uses a Bell loophole.

If the inequalities are not broken in nature, why is a 'loophole' needed?

One school of thought asserts that -a.b cannot be obtained in space-like separated EPRB (for normal 3D space), and that the experiments claiming to show it are all wrongly designed, implemented, and/or interpreted. You can pile up as many stupid and/or fake experiments you like; it doesn't make separated -a.b any more plausible.

Don't call it a "loophole" then. But a theorem is a theorem. Quantum mechanics is incompatible with locality + realism + no-conspiracy. Sabine Hossenfelder's most recent work is a paper claiming to show that no "fine-tuning" is need to get Bell violations out of a local realistic theory. Tim Palmer uses p-adic analysis and chaos theory and claims to prove the same thing. Their maths is too difficult for me. Austin Fearnley, Jarek Duda and others claim that the solution lies in retrocausality.

You say that there is a school of thought which says that you cannot obtain -a.b. There certainly was such a school of thought. In 2003, I even pointed out myself that this was a possibility acknowledged by Bell: quantum mechanics itself could prevent a loophole free experiment from ever being successful. I called this "Bell's fifth position" in https://arxiv.org/abs/quant-ph/0301059. I am not sure that it is very viable these days. Especially since the Delft and the Munich experiments do get something pretty close to -a.b (but with much too small sample sizes for anyone really to write home about the results of those experiments).
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Re: Gull and Gill's theory

Postby gill1109 » Sun Nov 08, 2020 7:58 am

gill1109 wrote:https://aflb.minesparis.psl.eu/AFLB-321/aflb321m555.htmThis is another proof of Bell's theorem, similar to Gull's. It seems to me to be a whole lot more complete.

Annales de la Fondation Louis de Broglie, Volume 32, no 1, 2007, pp 69-76
A New Proof of Bell’s Theorem Based on Fourier Series Analysis
Habibollah Razmi, 37185-359, Qom, I.RR. Iran
Department of Physics, The University of Qom, I. R. Iran
razmi@qom.ac.ir & razmiha@hotmail.com
ABSTRACT. We want to prove Bell’s theorem using Fourier series expansion analysis. Comparing to already known algebraic methods, this is a new calculus-based model. Although the notation and procedure we use here is based on the Clauser-Horne model, the corresponding Fourier series method can be simply applied to different versions of Bell’s theorem.

See also https://aflb.minesparis.psl.eu/AFLB-341/aflb341m641.pdf, "Comment on “A New Proof of Bell’s Theorem Based on Fourier Series Analysis” " by Roderich Tumulka, and https://aflb.minesparis.psl.eu/AFLB-341/aflb341m641b.htm, "Reply to “Comment on A New Proof of Bell’s Theorem Based on Fourier Series Analysis” by Roderich Tumulka", by Habibollah Razmi.

More stuff by Razmi: https://iopscience.iop.org/article/10.1088/0305-4470/38/16/013
Is the Clauser–Horne model of Bell's theorem completely stochastic?
H Razmi

Journal of Physics A: Mathematical and General, Volume 38, Number 16

Abstract
The stochastic Clauser–Horne (CH) model of Bell's theorem [1] is considered and by applying the locality condition it is shown that this (local) model, as far as applied to the singlet-state and without using quantum mechanical formalism, is not completely stochastic (i.e. there are possible configurations for which the model is deterministic).
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Re: Gull and Gill's theory

Postby local » Sun Nov 08, 2020 7:59 am

More boring and condescending lectures from Gill telling us stuff we already know! The experiments are stupid and/or fake (where's the Nobel prize?), and to get -a.b in space-like separated EPRB, superluminal information transfer is required. Passion-at-a-distance is nonsense; it doesn't matter whether signalling is possible or not. And I am not talking about Gill's silly "fifth position". I do not claim that QM is wrong, nor that QM prevents a valid experiment, only that Luders rule is inapplicable for EPRB with space-like separation.

Intelligent people understand that 'quantum nonlocality' is a joke. I feel sorry for the others that have wasted their careers on nonsense.
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Re: Gull and Gill's theory

Postby gill1109 » Sun Nov 08, 2020 8:56 am

What I call Bell's fifth position was promoted vigorously by Emilio Santos. https://arxiv.org/abs/quant-ph/0410193 Bell's theorem and the experiments: Increasing empirical support to local realism.

Abstract: It is argued that local realism is a fundamental principle, which might be rejected only if experiments clearly show that it is untenable. A critical review is presented of the derivations of Bell's inequalities and the performed experiments, with the conclusion that no valid, loophole-free, test exists of local realism vs. quantum mechanics. It is pointed out that, without any essential modification, quantum mechanics might be compatible with local realism. This suggests that the principle may be respected by nature. Published in Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics Volume 36, Issue 3, September 2005, Pages 544-565, DOI: 10.1016/j.shpsb.2005.05.007, https://www.sciencedirect.com/science/article/abs/pii/S1355219805000419. Bell agreed in correspondence with Santos that it was a logical possibility. It seems that "local" would agree. I don't know why he or she is talking about Luder's postulate. I do not use it anywhere. I am not talking about quantum nonlocality, either. Santos hasn't changed his mind, despite the 2015 experiments. See https://www.frontiersin.org/articles/10.3389/fphy.2020.00191/full.

The 2012 Nobel prize in physics went to Serge Haroche and David J. Wineland https://www.nobelprize.org/prizes/physics/2012/summary/. I think you'll find that these guys use Luders' postulate a lot. Their work certainly enabled the 2015 Bell experiments.
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Re: Gull and Gill's theory

Postby local » Sun Nov 08, 2020 9:02 am

You are being disingenuous (not a surprise). That Nobel was not awarded for the discovery of 'quantum nonlocality'. If you want -a.b for separated EPRB, you must use Luders' rule. You cannot use the quantum joint solution for separated measurement. If you doubt it, please present your quantum theory derivation of -a.b for two separated measurements (one after the other), i.e., not using the inapplicable joint measurement solution.

You have only a dilettantish understanding of projection and its relevance to EPRB. Do your homework!

Finally, I do accept that CH/CHSH et al are valid. But I agree with Fred (possibly for different reasons) that nothing can violate them for separated EPRB, not even quantum theory!
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Re: Gull and Gill's theory

Postby FrediFizzx » Sun Nov 08, 2020 9:15 am

gill1109 wrote:
FrediFizzx wrote:LOL! You have no proof. Gull was your last chance at any kind of proof. So, they are all shot down. And it is pretty foolish of you to be making a 64,000 euro bet when you have no proof. :mrgreen: Look how complicated it was for Perelman to solve the Poincaré conjecture. It is just a very complex problem to solve but someone will eventually shoot down your theory.

I have a proof (which convinces me) that I won’t lose the 64,000 Euro. I put it on arXiv in 2001. I was preparing a bet with Luigi Accardi. He saw my proof and withdrew from the bet. Nobody has “shot it down”. My proof is older and stronger than Gull’s. We don’t need Gull’s “proof”. It would be very exciting if someone blew up my proof. Go ahead and do it! I recommend you learn something about martingale theory first, so you understand what you are up against. You just need to write one computer program for one computer. We’ll just switch the sign of the outcome when we use it to play “detector B”. Remember: you include the RNG and a seed of the RNG in the program so it is completely deterministic.

I didn't see any "proof" in that paper. Looks like you just proved the inequalities but that is trivial. Joy shot down your "proof" in 2007. You have no proof. Nature is tricking you. About time you realized that. You are eventually going to lose that 64,000 Euros.
.
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Re: Gull and Gill's theory

Postby FrediFizzx » Sun Nov 08, 2020 9:22 am

FrediFizzx wrote:
gill1109 wrote:
FrediFizzx wrote:
gill1109 wrote:Please read my paper. It’s been on arXiv for 19 years, it’s been peer reviewed and published for 17. The main result has been improved, sharpened, both by myself and by others. It was used in all four 2015 loophole free experiments. The experimentalists cited my work and acknowledged my contribution.

Nature does it, using quantum entanglement.

Sorry, Jay Yablon shot down quantum entanglement with his successful demonstration that QM is local for the EPR-Bohm scenario. So, you really should get off that nonsense. All the experiments do is validate QM. Nothing more since ALL the "proofs" of Bell's junk physics theory are shot down.
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Jay redefined “local”. He is not the first to resolve the problem in this way. ...

You sure do love spewing nonsense. Jay's measurement functions are 100 percent local. You probably don't even understand how Jay did it or even have read his paper. Tell me what equation numbers I'm talking about and I will explain it to you.
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No response to this. Come on, show us how Jay "redefined" local. You can't because he didn't. Entanglement is a joke Nature is playing on you. :mrgreen:
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FrediFizzx
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Re: Gull and Gill's theory

Postby local » Sun Nov 08, 2020 9:58 am

FrediFizzx wrote:Entanglement is a joke.

I'll second that!

Back in the day some idiot was confused and didn't understand the distinction between joint and separated measurement, and stupidly assumed that -a.b was valid for separated EPRB, just because it can sometimes be valid for joint measurement. Nature is nonlocal he cried! Everyone bought that nonsense and started doing experiments to prove it. They weren't interested in the truth but just in proving this stupid thing. All kinds of stupid tricks were used to coerce the experiments to agree. Several early experiments did not agree but the researchers were bullied into excusing things as 'systematic errors' and other nonsense. In one case, a piece of glassware was blamed for being a little warped. Hey, you won't get grants for proving that special relativity is true; woo-woo stuff is needed. The birth of quantum mysticism! And now, when we understand theoretically that -a.b cannot be obtained for separated EPRB, these people are stuck in a corner desperately trying to protect their reputations, positions, and grants. It's bad enough to be a loser, but it's terrible to die a loser.
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Re: Gull and Gill's theory

Postby gill1109 » Sun Nov 08, 2020 11:33 am

local wrote:
FrediFizzx wrote:Entanglement is a joke.

I'll second that!

Back in the day some idiot was confused and didn't understand the distinction between joint and separated measurement, and stupidly assumed that -a.b was valid for separated EPRB, just because it can sometimes be valid for joint measurement. Nature is nonlocal he cried! Everyone bought that nonsense and started doing experiments to prove it. They weren't interested in the truth but just in proving this stupid thing. All kinds of stupid tricks were used to coerce the experiments to agree. Several early experiments did not agree but the researchers were bullied into excusing things as 'systematic errors' and other nonsense. In one case, a piece of glassware was blamed for being a little warped. Hey, you won't get grants for proving that special relativity is true; woo-woo stuff is needed. The birth of quantum mysticism! And now, when we understand theoretically that -a.b cannot be obtained for separated EPRB, these people are stuck in a corner desperately trying to protect their reputations, positions, and grants. It's bad enough to be a loser, but it's terrible to die a loser.

This thread is not about entanglement. It’s not about quantum mechanics. It’s not about locality or non-locality. It’s about a no-go theorem in (classical) computer science (sub field: distributed computing). Gull’s theorem (proof not complete, can it be saved?) and Gill’s theorem (posted on arXiv in 2001, published in 2003).

If Fred wants to win 64 000 Euro from me he just has to write one computer program which enables him to win my 2001 bet with Luigi Accardi. We’ll do a CHSH type experiment. I’ll supply, separately, two streams of settings chosen by fair coin tosses. We’ll do a big run of, say, four million trials. There will be about a million trials with each setting pair. Fred has to finish up with the CHSH function of four correlations (one correlation minus sum of the other three) nearer to 2 sqrt 2 than to 2. I’ll be generous, he wins from me if it ends up above 2.4. He must publish his computer programs so that everyone can verify that they work and do not break the rules. They must be strictly deterministic. The seed to his pseudo RNG must be written into his code, and the RNG must be programmed there too, or at least, fixed by the computer language, so we get the same results whether we use a Mac, PC or Linux machine.

I understand that Fred still thinks he can win this bet, he’s working hard on improving his GAViewer programs. I imagine that “local” realises that Fred probably can’t. Or is just not interested. No problem. This is 20 year old stuff, not terribly exciting, there are just some mathematical loose ends to tie up.
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