Quantum Mechanics with HV is Local!

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

Re: Quantum Mechanics with HV is Local!

Postby Joy Christian » Sat Jun 22, 2019 3:18 am

gill1109 wrote:
Joy Christian wrote:
The inconsistency is in your understanding of what the model is all about. I am not going to keep repeating my replies over and over again. For the last time, all four combinations of outcomes, ++, --, +- and -+ are possible. They come about, locally, because of the geometry of the 3-sphere. If they did not, then the correlation could not have been E(a, b) = -a.b.

You can say what you like. Your formulas tell another story. :D

Our measurement functions defined in eqs. (8) and (9) give the outcomes +1 or -1, depending on the parameters a and b, chirality lambda, and the corresponding geometry of the 3-sphere.

***
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Re: Quantum Mechanics with HV is Local!

Postby Heinera » Sat Jun 22, 2019 4:05 am

Joy Christian wrote:Our measurement functions defined in eqs. (8) and (9) give the outcomes +1 or -1, depending on the parameters a and b, chirality lambda, and the corresponding geometry of the 3-sphere.

***

There is no need to discuss this any further. For the first time for this model, the functions A and B are presented with actually computable mathematical expressions. Anyone can just fix some numerical value for a and lambda, "shut up and calculate" A and see if they sometimes get +1 and sometimes -1, if they're still unsure.
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Re: Quantum Mechanics with HV is Local!

Postby Joy Christian » Sat Jun 22, 2019 4:23 am

Heinera wrote:
Joy Christian wrote:
Our measurement functions defined in eqs. (8) and (9) give the outcomes +1 or -1, depending on the parameters a and b, chirality lambda, and the corresponding geometry of the 3-sphere.

There is no need to discuss this any further. For the first time for this model, the functions A and B are presented with actually computable mathematical expressions. Anyone can just fix some numerical value for a and lambda, "shut up and calculate" A and see if they sometimes get +1 and sometimes -1, if they're still unsure.

Of course, one can invent his or her own model --- let us call it Heinera model or flatland model --- and declare that that is our model. In that case, they can get what they wish to get.

***
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Re: Quantum Mechanics with HV is Local!

Postby Heinera » Sat Jun 22, 2019 4:33 am

Joy Christian wrote:
Heinera wrote:
Joy Christian wrote:
Our measurement functions defined in eqs. (8) and (9) give the outcomes +1 or -1, depending on the parameters a and b, chirality lambda, and the corresponding geometry of the 3-sphere.

There is no need to discuss this any further. For the first time for this model, the functions A and B are presented with actually computable mathematical expressions. Anyone can just fix some numerical value for a and lambda, "shut up and calculate" A and see if they sometimes get +1 and sometimes -1, if they're still unsure.

Of course, one can invent his or her own model --- let us call it Heinera model or flatland model --- and declare that that is our model. In that case, they can get what they wish to get.

***

Why should I invent my own model when I can just calculate the functions A and B from the paper?
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Re: Quantum Mechanics with HV is Local!

Postby Joy Christian » Sat Jun 22, 2019 4:36 am

Heinera wrote:
Joy Christian wrote:
Heinera wrote:
Joy Christian wrote:
Our measurement functions defined in eqs. (8) and (9) give the outcomes +1 or -1, depending on the parameters a and b, chirality lambda, and the corresponding geometry of the 3-sphere.

There is no need to discuss this any further. For the first time for this model, the functions A and B are presented with actually computable mathematical expressions. Anyone can just fix some numerical value for a and lambda, "shut up and calculate" A and see if they sometimes get +1 and sometimes -1, if they're still unsure.

Of course, one can invent his or her own model --- let us call it Heinera model or flatland model --- and declare that that is our model. In that case, they can get what they wish to get.

***

Why should I invent my own model when I can just calculate the functions A and B from the paper?

You are assuming that you can calculate. I haven't seen any evidence of that.

****
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Re: Quantum Mechanics with HV is Local!

Postby Heinera » Sat Jun 22, 2019 5:14 am

Joy Christian wrote:You are assuming that you can calculate. I haven't seen any evidence of that.

****

I can only assume that after a lot of thinking, this was the most insightful reply you could come up with :lol:
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Re: Quantum Mechanics with HV is Local!

Postby Joy Christian » Sat Jun 22, 2019 5:46 am

Heinera wrote:
Joy Christian wrote:You are assuming that you can calculate. I haven't seen any evidence of that.

****

I can only assume that after a lot of thinking, this was the most insightful reply you could come up with :lol:

I still do not see any evidence that you can calculate.

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Re: Quantum Mechanics with HV is Local!

Postby FrediFizzx » Sat Jun 22, 2019 7:23 pm

Hi Folks,

Since a, b and s can be all random, the Stern-Gerlach polarizer action should be random up or down also so let's try these functions,

Image
.
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Re: Quantum Mechanics with HV is Local!

Postby gill1109 » Sat Jun 22, 2019 10:56 pm

FrediFizzx wrote:Hi Folks,

Since a, b and s can be all random, the Stern-Gerlach polarizer action should be random up or down also so let's try these functions,

Image
.

I think we need to know your definition of "limit as +/-s converges to a". And why is there a "plus or minus" there?

I would say that a and b are chosen by the experimenter. Sometimes the experimenter will choose them by tossing coins. I think that in this formula, a and b are just any given directions. I would say that s is what some mathematicians informally call a "dummy variable'"; it also takes values in the set of spatial directions. (Logicians talk about free variables and bound variables, I can never remember which is which).

What we really need to know is what is the limit as the pair s, s' converges to a, b of the pair , where f and g are those complicated functions - each depending on four arguments - in the two big formulas. (I suppose that R and sigma are fixed. Maybe R is just a name, not a variable... sigma is the vector of the three Pauli spin matrices. It's a fixed variable ;) ). If a limit of the pair exists, it would have to be (-1,-1), or (-1, +1), or (+1, -1), or (+1, +1). And we need all four limits to be possible for different values of lambda. Hence I think we need lambda to take on at least four different values.

If you want to identify s and s' then you have to say what is the single value to which both are converging.
Last edited by gill1109 on Sat Jun 22, 2019 11:15 pm, edited 1 time in total.
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Re: Quantum Mechanics with HV is Local!

Postby FrediFizzx » Sat Jun 22, 2019 11:14 pm

gill1109 wrote:
FrediFizzx wrote:Hi Folks,

Since a, b and s can be all random, the Stern-Gerlach polarizer action should be random up or down also so let's try these functions,

Image
.

I think we need to know your definition of "limit as +/-s converges to a". And why is there a "plus or minus" there?

I would say that a and b are chosen by the experimenter. Sometimes the experimenter will choose them by tossing coins. I think that in this formula, a and b are just any given directions. I would say that s is what some mathematicians informally call a ``dummy variable''; it also takes values in the set of spatial directions.

What we really need to know is what is the limit of the pair . If it exists, it would have to be (-1,-1), or (-1, +1), or (+1, -1), or (+1, +1). And we need all four limits to be possible for different values of lambda.

Do you know how a Stern-Gerlach polarizer works? It splits a beam of randomly polarized spin 1/2 particles into beams of up and down spins. The up and down are the plus and minus on s.

In the model, a and b can be chosen at any random angle and even in 3D directions. This is a theory; not an experiment. And the theory still works just fine with completely random settings. Yes, the spin vector for s can be and usually is, pointing in any 3D direction randomly also.

All four outcome possibilities come out the same as predicted for QM. You can easily calculate that for yourself.
.
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Re: Quantum Mechanics with HV is Local!

Postby gill1109 » Sun Jun 23, 2019 12:26 am

FrediFizzx wrote:
gill1109 wrote:
FrediFizzx wrote:Hi Folks,

Since a, b and s can be all random, the Stern-Gerlach polarizer action should be random up or down also so let's try these functions,

Image
.

I think we need to know your definition of "limit as +/-s converges to a". And why is there a "plus or minus" there?

I would say that a and b are chosen by the experimenter. Sometimes the experimenter will choose them by tossing coins. I think that in this formula, a and b are just any given directions. I would say that s is what some mathematicians informally call a ``dummy variable''; it also takes values in the set of spatial directions.

What we really need to know is what is the limit of the pair . If it exists, it would have to be (-1,-1), or (-1, +1), or (+1, -1), or (+1, +1). And we need all four limits to be possible for different values of lambda.

Do you know how a Stern-Gerlach polarizer works? It splits a beam of randomly polarized spin 1/2 particles into beams of up and down spins. The up and down are the plus and minus on s.

In the model, a and b can be chosen at any random angle and even in 3D directions. This is a theory; not an experiment. And the theory still works just fine with completely random settings. Yes, the spin vector for s can be and usually is, pointing in any 3D direction randomly also.

All four outcome possibilities come out the same as predicted for QM. You can easily calculate that for yourself.
.

Fred, to be honest, I don't know how a Stern-Gerlach device works, and I don't want to know. Or to be more precise: I want to obtain some understanding of how it works through gaining a mathematical understanding of various mathematical models which have been proposed for the Stern-Gerlach experiment.

I am a mathematician. I am not a physicist. I can't make any sense whatever of the symbols in your formulas. They look like mathematics but they break the standard rules and conventions, so I am lost.

Do you know the epsilon-delta definition of a limit? Could you please try to relate your concept of limit to the standard mathematical concept?

https://en.wikipedia.org/wiki/(%CE%B5,_%CE%B4)-definition_of_limit

Of course, I can easily do the standard quantum mechanical computations myself. In the standard treatment, there is no limit being taken of a sum of products of two functions A(a, lambda) and B(b, lambda). Bell's theorem says that it is not possible to reproduce the quantum mechanical answers through a computation of the mean value, as lambda is chosen at random from some fixed probability distribution (fixed means: not depending on a or b), of a product A(a, lambda)B(b, lambda) where the two functions A and B take values in the set {-1, +1}. As we discussed elsewhere, Steve Gull sketched a direct proof of this "no-go" theorem using standard results from Fourier analysis which every STEM educated person knows by heart. I further elaborated on Steve's beautiful proof in a short paper on arXiv which is not yet submitted to a journal. I would love to find a co-author to help me finish it.

Incidentally, the epsilon-delta definition of limit was discovered by Augustin Cauchy as part of an attempt to repair the already highly successful Fourier theory, which unfortunately contained some embarrassing anomalies. Riemann's later work on integration theory was part of the same major research programme. Fourier theory had enormous engineering and military applications and mathematics had to be "fixed" so that people could use it with confidence. Later, Lebesgue's work was part of the same programme. Which finally led to Kolmogorovian probability theory as the solution of Hibert's sixth problem https://en.wikipedia.org/wiki/Hilbert%27s_sixth_problem. It's a pity most physicists stayed stuck in the 19th century regarding their ignorance and even disdain for probability theory and for statistics. It's high time they caught up. Fortunately, modern technology means that most theoretical physics PhDs, and most algebraic geometry PhDs, end up getting jobs in big data, machine learning, AI, and data science ... i.e. in statistics and probability.
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Re: Quantum Mechanics with HV is Local!

Postby Heinera » Sun Jun 23, 2019 12:40 am

FrediFizzx wrote:Hi Folks,

Since a, b and s can be all random, the Stern-Gerlach polarizer action should be random up or down also so let's try these functions,

Image
.


Like Richard, I have no idea of how should be interpreted mathematically. In fact, I'm pretty sure this is the first time in the history of mathematics anyone has written a limit like that. Could you show us some computer code as an example of how you intend that this should be calculated?
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Re: Quantum Mechanics with HV is Local!

Postby Mikko » Sun Jun 23, 2019 2:52 am

gill1109 wrote:Logicians talk about free variables and bound variables, I can never remember which is which.

Free variables are like a or λ in Fred's formulas that can be freely assigned specific values. Bound variables are bound to an operator (like lim or ∑ or ∀) that gives them as many values as it wants.
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Re: Quantum Mechanics with HV is Local!

Postby gill1109 » Sun Jun 23, 2019 4:16 am

Mikko wrote:
gill1109 wrote:Logicians talk about free variables and bound variables, I can never remember which is which.

Free variables are like a or λ in Fred's formulas that can be freely assigned specific values. Bound variables are bound to an operator (like lim or ∑ or ∀) that gives them as many values as it wants.

Exactly. And s is apparently a bound variable, since it appears bound to the operator "lim".

Actually, in Fred's formulas, λ is often bound to a summation symbol or it has a subscript "k" which is bound to a summation ∑.

Bell has integrals. It's a pity Bell never leant measure theory, but of course, if he had used 20th century mathematics notation in the second half of the 20th century, no physicist would have been able to read his formulas.

I don't understand why Fred, Joy and Jay seem to use a very old fashioned (and unfashionable) von Mises - like definition of expectation value instead of the modern definition as an integral with respect to a measure. The measure might be counting measure, making the integral a sum. A sum over the possible outcomes of one trial. That's how we define expectation value in statistics 101. Not a sum over the elements of an infinite sequence of repeated trials.

Keynes said "in the long run we are all dead". Defining probability and expectation as long run limits of functions of outcomes of infinitely many independent repetitions is terribly early-20th-century.

Of course, later Kolmogorov somehow rehabilitated von Mises with his notions of computational complexity and definition of an infinite *random* sequence.
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Re: Quantum Mechanics with HV is Local!

Postby Joy Christian » Sun Jun 23, 2019 5:28 am

***
What a load of nonsense! Obfuscations, distractions and temper tantrums. I have seen them all before for the past twelve years.

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Re: Quantum Mechanics with HV is Local!

Postby gill1109 » Sun Jun 23, 2019 5:41 am

Joy Christian wrote:What a load of nonsense! Obfuscations, distractions and temper tantrums. I have seen them all before for the past twelve years.

Obfuscations and temper tantrums!!! What's that old English saying about the pot calling the kettle black? How about replying to the substance of the postings by various people? Take your time. Do a bit of background research first. It's a lovely day! :mrgreen:

I admit to deliberate obfuscation. But not to a temper tantrum. I never felt more joyful and contented and warmly disposed to everyone.
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Re: Quantum Mechanics with HV is Local!

Postby Joy Christian » Sun Jun 23, 2019 5:45 am

gill1109 wrote:
Joy Christian wrote:What a load of nonsense! Obfuscations, distractions and temper tantrums. I have seen them all before for the past twelve years.

Obfuscations and temper tantrums!!! What's that old English saying about the pot calling the kettle black? How about replying to the substance of the postings by various people? Take your time. Do a bit of background research first. It's a lovely day! :mrgreen:

There is no "substance" in "the postings by various people." When I see a genuine substance, or anything remotely useful for physics, I will reply. Until then I have better things to do.

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Re: Quantum Mechanics with HV is Local!

Postby FrediFizzx » Sun Jun 23, 2019 6:53 am

Heinera wrote:
FrediFizzx wrote:Hi Folks,

Since a, b and s can be all random, the Stern-Gerlach polarizer action should be random up or down also so let's try these functions,

Image
.


Like Richard, I have no idea of how should be interpreted mathematically. In fact, I'm pretty sure this is the first time in the history of mathematics anyone has written a limit like that. Could you show us some computer code as an example of how you intend that this should be calculated?

No computer code is needed. is the same as . Think of it that way if it helps you to connect the math to the way the polarizer works.
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Re: Quantum Mechanics with HV is Local!

Postby FrediFizzx » Sun Jun 23, 2019 6:59 am

gill1109 wrote:… I am a mathematician. I am not a physicist. I can't make any sense whatever of the symbols in your formulas. They look like mathematics but they break the standard rules and conventions, so I am lost.

Ok, let's get you un-lost. The limits are simple to understand. If -s --> a is the same as if s --> -a. And if +s --> a is the same as s --> a. Does that help? If so, then what is the next symbol you are having trouble with?
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Re: Quantum Mechanics with HV is Local!

Postby Heinera » Sun Jun 23, 2019 7:08 am

FrediFizzx wrote: is the same as . Think of it that way if it helps you to connect the math to the way the polarizer works.


But this was the thing you dropped because then you can't ensure that the outcomes are always opposite for equal detector settings on both sides:

FrediFizzx wrote:You were right that extra randomness. We took that out because it can give AB = +1 instead of AB = -1 when a = b.
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