Thoughts about Bell, Bohm, Christian, et al.

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

Re: Thoughts about Bell, Bohm, Christian, et al.

Postby Heinera » Fri Jun 12, 2015 1:51 pm

AnotherGuest wrote:
I think that the whole discussion is not actually about "reality" (whatever that is!) but about mathematical models of reality. And about whether those mathematical models can be extended so as to include also "what would have happened if ...". And about whether that extended model still satisfies natural locality properties.

Exactly. Bell's theoroem is a theorem about mathematical models, and counterfactual definiteness simply means that a model is counterfactually definite if, in the model, it is possible to compute the predictions for both as well as .
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Re: Thoughts about Bell, Bohm, Christian, et al.

Postby Schmelzer » Fri Jun 12, 2015 2:24 pm

Heinera wrote:In the context of Bell's theorem, what is needed for the theorem to hold is counterfactual definiteness (realism), and the property that in the theory, the value is independent of the setting in the other wing, i.e., it always computes to the same value in the theory. This latter property is called locality in the context of Bell's theorem. A theory that use information outside the light-cone of the station would still be called "local" in the Bell sense, as long as this information does not contain the setting in the other wing.


Don't forget that the counterfactual definiteness of the outcomes of the measurement is derived from the EPR argument. Thus, you only need the EPR criterion of reality. Essentially, you only need causality (Reichenbach's common cause principle).
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Re: Thoughts about Bell, Bohm, Christian, et al.

Postby minkwe » Fri Jun 12, 2015 2:55 pm

FrediFizzx wrote:Did you mean, "...measurement by Bob along axis "a" must produce outcome -1..."?

That is right Fred, just a typo.
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Re: Thoughts about Bell, Bohm, Christian, et al.

Postby minkwe » Fri Jun 12, 2015 3:40 pm

AnotherGuest wrote:Very good question, Minkwe.

We can speak meaningfully about what would happen if ... . All physics is about saying what would happen if ....

But we are examining the definition of "counterfactual definiteness" used in the literature, and are finding that either they come up short or they also apply to QM. I didn't come up with the definition.
Counterfactual definiteness goes, I think, beyond that. It is about the question whether all those other things which could have happened if .. are to be considered just as real as the one thing that does actually happen in the circumstances which will actually hold.

But according to QM, if Alice obtains +1 along "a", Bob must also definitely obtain -1 if he measures along "a". It does not matter whether Bob actually measured along a different axis "b". QM says if Bob had measured along "a", he would definitely have obtained -1. This is counterfactual definiteness according to the definition being used in the literature. If you disagree could you please show a source where counterfactual definiteness is defined differently such that it does not apply to this situation. We are not just playing with words, we are decifering exactly what people talk about when they use those terms. First we found that when people say "locality" they don't actually mean "locality", they mean "setting and outcome independence", which applies equally to local or non-local situations. Now we are finding that when people say "counterfactual definiteness", they either mean something else than their own definitions claim it means, or if their definitions are to be followed, it should apply to QM just the same.

Word games for philosophers. But as soon as we start talking about mathematical models, then we do get onto something interesting, I think.

There is a reason why when you get a terminal degree it is called a PhD -- Doctor of philosophy. Philosophy is an integral part of any scientific endeavor. It is very unfortunate that "philosophy" is nowadays considered a derogatory term in some mathematics/physics circles.
We can ask the question: is there a mathematical model which reproduces the predictions of quantum mechanics,

Indeed that is an interesting question. But our focus at the moment is on a specific but different question: What are the physical assumptions required to obtain Bell's inequalities. We've seen that despite popular belief, "locality" is not one of those assumptions. Now we are seeing that the "popular" definition of "counterfactual definiteness" actually applies to Bell's description of the QM prediction too. The concept of couterfactual definiteness is completely irrelevant if our goal is to develop a model for .

but which also goes beyond those predictions and allows, within the mathematics, "existence" of counterfactual outcomes of not performed measurements, alongside of actual outcomes of actually performed measurements
...
I think that the whole discussion is not actually about "reality" (whatever that is!) but about mathematical models of reality. And about whether those mathematical models can be extended so as to include also "what would have happened if ...". And about whether that extended model still satisfies natural locality properties.

So you believe the statement Does not apply to QM? Is that a mathematical model?

Note that in Bell's derivation of the inequalities, the actual details of the functions are irrelevant. The derivations rely entirely on the symbols and the outcomes of the functions, not the models. In fact, I presented a derivation above which used just the three outcomes , no functions. Therefore it is a grave mistake to think that Bell's derivation is about any mathematical models. It is about series of triplets of bivalued numbers. Besides, if a model were to provide a definition for the function , there would be no reason whatsoever for that model to include any concept of counterfactual definiteness in the function. What use would that be?

In other words, local-ness or not local-ness is a property of a model

I agree, locality or non-locality can be a property of a model. But I claim that counterfactual definiteness is not a property of a model. A model is local if its definition of the function A_a(...) uses only information within the light-cone. It is non-local if its definition of the function uses information from outside the light-cone. But what does it mean for a model to be counterfactually definite? It is a completely irrelevant concept as far as models of the outcomes in the EPRB experiment are concerned. In other words, counterfactual definiteness is completely irrelevant to the question of whether or not a model reproduces the QM predictions. The only reason we are discussing it is because it was invoked by Bell in deriving his inequalities.

I do not contest the fact that Bell's inequality as far as it applies to experimental tests, includes a mixture of actual and counterfactual outcomes. It is not the theory that forces Bell to do that, it is Bell himself who simply introduced that into his inequality.
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Re: Thoughts about Bell, Bohm, Christian, et al.

Postby Schmelzer » Fri Jun 12, 2015 4:00 pm

minkwe wrote: But our focus at the moment is on a specific but different question: What are the physical assumptions required to obtain Bell's inequalities.


A quite meaningless question.

There may be very different theorems, all giving, as the result, Bell's inequalities.

T1: A1+ A2 + A3 -> BI
T2: A3+ A4+ A5 -> Bi
T3: A1+A4 -> BI

So, for every assumption, from A1 to A5, there is a theorem which gives BI where it is not used as an assumption. Thus, none of these assumptions is required to obtain the BI.

On the other hand, every variant of a Bell-like theorem, from T1 to T3, makes nontrivial assumptions. Without making notrivial assumptions, to prove the BI would be impossible.
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Re: Thoughts about Bell, Bohm, Christian, et al.

Postby FrediFizzx » Fri Jun 12, 2015 11:34 pm

Schmelzer wrote:
minkwe wrote: But our focus at the moment is on a specific but different question: What are the physical assumptions required to obtain Bell's inequalities.


A quite meaningless question.

There may be very different theorems, all giving, as the result, Bell's inequalities.

T1: A1+ A2 + A3 -> BI
T2: A3+ A4+ A5 -> Bi
T3: A1+A4 -> BI

So, for every assumption, from A1 to A5, there is a theorem which gives BI where it is not used as an assumption. Thus, none of these assumptions is required to obtain the BI.

On the other hand, every variant of a Bell-like theorem, from T1 to T3, makes nontrivial assumptions. Without making notrivial assumptions, to prove the BI would be impossible.


I don't think Michel was talking about "theorems". He wants to know what are the physical assumptions necessary to obtain the inequality that Bell obtained. For me they are basically Bell's "conditions" based on EPR-Bohm. It is not a meaningless question at all.
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Re: Thoughts about Bell, Bohm, Christian, et al.

Postby minkwe » Sat Jun 13, 2015 4:03 am

Thanks Fred, since Ilja is on my ignore list. I don't see his comments unless you quote it in your reply. I'm not missing much.

Until now, we have been addressing Bell's inequality as presented by Bell in his original paper, and the assumptions required to derive them, not Bell's theorem, which is quite a different thing, not variants of it.

In the mean time, we have found that no physical assumptions are required to obtain the inequality, despite widespread belief in the false dogma of "nontrivial assumptions".

Besides we are not yet done with Counterfactual Definiteness, we have just scratched the surface of Bell's problems. Counterfactual Definiteness is a logical concept, not a physical one. I await a definition from anyone, which discriminates one of physical theory from another.
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Re: Thoughts about Bell, Bohm, Christian, et al.

Postby Schmelzer » Sat Jun 13, 2015 4:32 am

FrediFizzx wrote:I don't think Michel was talking about "theorems". He wants to know what are the physical assumptions necessary to obtain the inequality that Bell obtained. For me they are basically Bell's "conditions" based on EPR-Bohm. It is not a meaningless question at all.


But, then, explain what is the difference. Between " to obtain the inequality that Bell obtained" and a theorem which proves them, starting with some assumptions. And between "the physical assumptions necessary to obtain" and the assumptions used in such a theorem.

And we have, already today, a large number of different variants of theorems, all of them obtaining Bell inequalities or other, essentially equivalent things like CHSH or so. Which use quite a large number of different assumptions.

minkwe wrote:Until now, we have been addressing Bell's inequality, and the assumptions required to derive them, not Bell's theorem, which is quite a different thing.


Of course, Bell's theorem is a reasonable theorem, to look for "assumptions required to derive" whatever is, instead, simply nonsense, because one can always invent another set of assumptions which does not include the "assumptions required to derive" it.

Say, minkwe finds that to derive X the assumption Y is required. I, instead, use an assumption Z which has nothing to do with Y, and prove the trivial theorem "From Z and (X or not Z) follows X". Thus, I can derive X from Z and (X or not Z), thus, I don't need Y to derive X.
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Re: Thoughts about Bell, Bohm, Christian, et al.

Postby Heinera » Sat Jun 13, 2015 5:24 am

minkwe wrote:Besides we are not yet done with Counterfactual Definiteness, we have just scratched the surface of Bell's problems. Counterfactual Definiteness is a logical concept, not a physical one.

Yes.
I await a definition from anyone, which discriminates one of physical theory from another.


A theory has counterfactual definiteness if it is possible within the theory to compute predictions for both as well as .
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Re: Thoughts about Bell, Bohm, Christian, et al.

Postby Joy Christian » Sat Jun 13, 2015 5:38 am

Heinera wrote:A theory has counterfactual definiteness if it is possible within the theory to compute predictions for both as well as .

According to this definition QM "has counterfactual definiteness." :lol:
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Re: Thoughts about Bell, Bohm, Christian, et al.

Postby Heinera » Sat Jun 13, 2015 5:57 am

Joy Christian wrote:
Heinera wrote:A theory has counterfactual definiteness if it is possible within the theory to compute predictions for both as well as .

According to this definition QM "has counterfactual definiteness." :lol:

It is not hard to create a model with counterfactual definiteness that exactly produce the QM-correlations:

http://rpubs.com/heinera/16727

Not that I would recommend thinking about QM in this way. In the way QM is usually formulated, the theory does not compute individual outcomes at all, only probability distributions. This means that the question whether QM posesses counterfactual definiteness or not is open to one's favorite interpretation.
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Re: Thoughts about Bell, Bohm, Christian, et al.

Postby AnotherGuest » Sat Jun 13, 2015 6:42 am

minkwe wrote:
AnotherGuest wrote:Very good question, Minkwe.

We can speak meaningfully about what would happen if ... . All physics is about saying what would happen if ....

But we are examining the definition of "counterfactual definiteness" used in the literature, and are finding that either they come up short or they also apply to QM. I didn't come up with the definition.
Counterfactual definiteness goes, I think, beyond that. It is about the question whether all those other things which could have happened if .. are to be considered just as real as the one thing that does actually happen in the circumstances which will actually hold.

But according to QM, if Alice obtains +1 along "a", Bob must also definitely obtain -1 if he measures along "a". It does not matter whether Bob actually measured along a different axis "b". QM says if Bob had measured along "a", he would definitely have obtained -1. This is counterfactual definiteness according to the definition being used in the literature. If you disagree could you please show a source where counterfactual definiteness is defined differently such that it does not apply to this situation. We are not just playing with words, we are decifering exactly what people talk about when they use those terms. First we found that when people say "locality" they don't actually mean "locality", they mean "setting and outcome independence", which applies equally to local or non-local situations. Now we are finding that when people say "counterfactual definiteness", they either mean something else than their own definitions claim it means, or if their definitions are to be followed, it should apply to QM just the same.

Word games for philosophers. But as soon as we start talking about mathematical models, then we do get onto something interesting, I think.

There is a reason why when you get a terminal degree it is called a PhD -- Doctor of philosophy. Philosophy is an integral part of any scientific endeavor. It is very unfortunate that "philosophy" is nowadays considered a derogatory term in some mathematics/physics circles.
We can ask the question: is there a mathematical model which reproduces the predictions of quantum mechanics,

Indeed that is an interesting question. But our focus at the moment is on a specific but different question: What are the physical assumptions required to obtain Bell's inequalities. We've seen that despite popular belief, "locality" is not one of those assumptions. Now we are seeing that the "popular" definition of "counterfactual definiteness" actually applies to Bell's description of the QM prediction too. The concept of counterfactual definiteness is completely irrelevant if our goal is to develop a model for .

but which also goes beyond those predictions and allows, within the mathematics, "existence" of counterfactual outcomes of not performed measurements, alongside of actual outcomes of actually performed measurements
...
I think that the whole discussion is not actually about "reality" (whatever that is!) but about mathematical models of reality. And about whether those mathematical models can be extended so as to include also "what would have happened if ...". And about whether that extended model still satisfies natural locality properties.

So you believe the statement Does not apply to QM? Is that a mathematical model?


Regarding "counterfactual definiteness" see http://en.citizendium.org/wiki/Entanglement_(physics)#Counterfactual_definiteness

I think that counterfactual definiteness is a property of a model.

Example: An event-based simulation model of a "one-trial" experiment is effectively a mathematical model which allows us to define, within some mathematical model, for all lambda, a and b. Note the introduction of "lambda". Note the oresence of both settings! I think "counterfactual definiteness" is synonymous with "existence of HV's" or "has an event-based simulation model".

Here, regarding an event-based simulation, lambda stands for the seeds of all random number generators needed to produce the outcomes for just one trial. The function A is the program.

The user of the simulation program can choose a and b freely, independently of lambda ("no conspiracy").

After we have counterfactual definiteness, we can ask ourselves, do we also have "locality"? "Locality" is does not depend on b.

BTW I have a PhD and I'm proud of it. I think "metaphysics" is just as important as "physics". I do not belong to the "shut up and calculate" school.

I am not sure what to think about "reality". Language, thought are just models. We are stuck with them. We only have indirect knowledge of "reality": our sense impressions. Can you define "locality" in terms of sense-impressions only? I think we can only define it within the context of, and relative to, some model.
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Re: Thoughts about Bell, Bohm, Christian, et al.

Postby Heinera » Sat Jun 13, 2015 12:49 pm

Very good indeed, AnotherGuest. And let me in particular highlight one sentence in your comment:
AnotherGuest wrote:I think "counterfactual definiteness" is synonymous with "existence of HV's" or "has an event-based simulation model".

Yes.
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Re: Thoughts about Bell, Bohm, Christian, et al.

Postby minkwe » Sat Jun 13, 2015 3:31 pm

AnotherGuest, Heinera,

Please tell us what is wrong with these definitions of "Counterfactual definiteness", and provide a different definition if you disagree with these:

    Wikipedia: In quantum mechanics, Counterfactual definiteness (CFD) is the ability to speak meaningfully of the definiteness of the results of measurements that have not been performed (i.e. the ability to assume the existence of objects, and properties of objects, even when they have not been measured).
    Gill (http://arxiv.org/pdf/1207.5103v6.pdf): Its formulation refers to outcomes of measurements which are not actually performed, so we have to assume their existence, alongside of the outcomes of those actually performed: the principle of realism, or more precisely, counterfactual definiteness.
    http://arxiv.org/pdf/1007.4281.pdf: the assumption that a measurement that was not performed had a single definite result.

Furthermore, you might notice this nugget on the wikipedia page:

    Counterfactual definiteness is present in any interpretation of quantum mechanics that regards quantum mechanical measurements to be objective descriptions of a system's state independent of the measuring process, but also if regarded as an objective description of the system and the measurement apparatus.

If you are not able to state clearly what is wrong with the above definitions, the please explain why exactly Bell's 3rd & 4th sentence of the 2nd paragraph on page 2 is not counterfactual definiteness in QM.

Bell wrote:Measurements can be made, say by Stern-Gerlach magnets, on selected components of the spins and . If measurement of the component , where is some unit vector, yields the value +1 then, according to quantum mechanics, measurement of must yield the value -1 and vice versa.


This is not difficult question. Does QM say the un-performed experiment has a definite value or not. You guys are disowning your own definitions of "counterfactual definiteness", yet unable to enunciate a replacement. The citizendium page cited above is just a mess. And why was "event-based simulation program even brought up? It is completely irrelevant to the discussion at this point. Bell is not talking about simulations in his 1964 paper which we are discussing at the present time.
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Re: Thoughts about Bell, Bohm, Christian, et al.

Postby minkwe » Sat Jun 13, 2015 3:49 pm

Okay guys, let me turn up the heat just a little:

Bell introduced counterfactual definiteness at the very top of page 406 where he says:
Bell wrote:It follows that is another unit vector
...
(15)


Here Bell says even though measurements were done along and , there should exist a definite outcome along another axis . He then proceeds to derive equation 15 with that consideration. Do you disagree with this?

Note that this is in line with the various definitions of counterfactual definiteness, I've quoted previously (which you both now wish to disown). Furthermore, in equation (15), since represents a counterfactual axis, , , are therefore counterfactual expectation values. That is, they represent results of measurements that could have been done but were not done, in addition to the measurement P(a,b) that was actually done. Do you disagree with this?

Let us go back to the second paragraph on the first page: According to quantum mechanics . If Alice measured along , and Bob measured along . According to quantum mechanics, Bob would still have obtained had he measured along , even though he did not measure along . This is what Bell means when he says:

Bell wrote:If measurement of the component , where is some unit vector, yields the value +1 then, according to quantum mechanics, measurement of must yield the value -1 and vice versa.


Do you disagree that this is counterfactual definiteness?
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Re: Thoughts about Bell, Bohm, Christian, et al.

Postby FrediFizzx » Sat Jun 13, 2015 5:51 pm

Schmelzer wrote:
FrediFizzx wrote:I don't think Michel was talking about "theorems". He wants to know what are the physical assumptions necessary to obtain the inequality that Bell obtained. For me they are basically Bell's "conditions" based on EPR-Bohm. It is not a meaningless question at all.


But, then, explain what is the difference. Between " to obtain the inequality that Bell obtained" and a theorem which proves them, starting with some assumptions. And between "the physical assumptions necessary to obtain" and the assumptions used in such a theorem.

And we have, already today, a large number of different variants of theorems, all of them obtaining Bell inequalities or other, essentially equivalent things like CHSH or so. Which use quite a large number of different assumptions.

minkwe wrote:Until now, we have been addressing Bell's inequality, and the assumptions required to derive them, not Bell's theorem, which is quite a different thing.


Of course, Bell's theorem is a reasonable theorem, to look for "assumptions required to derive" whatever is, instead, simply nonsense, because one can always invent another set of assumptions which does not include the "assumptions required to derive" it.

Say, minkwe finds that to derive X the assumption Y is required. I, instead, use an assumption Z which has nothing to do with Y, and prove the trivial theorem "From Z and (X or not Z) follows X". Thus, I can derive X from Z and (X or not Z), thus, I don't need Y to derive X.

This all appears to me to be some kind of strawmen arguments. I believe we are talking about physical assumptions here. And mainly about physical assumptions based on EPR-Bohm.
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Re: Thoughts about Bell, Bohm, Christian, et al.

Postby FrediFizzx » Sat Jun 13, 2015 6:13 pm

minkwe wrote:Okay guys, let me turn up the heat just a little:

Bell introduced counterfactual definiteness at the very top of page 406 where he says:
Bell wrote:It follows that is another unit vector
...
(15)

Jumping the gun here..., if we put the inequality like this,



Then one can see by simple inspection that the inequality is false when the three terms on the RHS are independent.


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Re: Thoughts about Bell, Bohm, Christian, et al.

Postby FrediFizzx » Sat Jun 13, 2015 8:02 pm

AnotherGuest wrote:BTW I have a PhD and I'm proud of it. I think "metaphysics" is just as important as "physics". I do not belong to the "shut up and calculate" school.

Great! Why don't you signup for a regular account on the forum then you won't have to wait for moderation?
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Re: Thoughts about Bell, Bohm, Christian, et al.

Postby minkwe » Sat Jun 13, 2015 8:09 pm

FrediFizzx wrote:[
Jumping the gun here..., if we put the inequality like this,



Then one can see by simple inspection that the inequality is false when the three terms on the RHS are independent.



Hi Fred,
We will get to that in due course, there is a lot more foundation to lay before. I was going to ask next if it is possible to experimentally verify a Counterfactual definite claim. For example, for the spin-half pair, Alice measured and Bob measured , but according to quantum mechanics, Bob would have obtained had he measured along instead.

How can this statement be verified experimentally?
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Re: Thoughts about Bell, Bohm, Christian, et al.

Postby FrediFizzx » Sat Jun 13, 2015 9:45 pm

minkwe wrote:
FrediFizzx wrote:[
Jumping the gun here..., if we put the inequality like this,



Then one can see by simple inspection that the inequality is false when the three terms on the RHS are independent.



Hi Fred,
We will get to that in due course, there is a lot more foundation to lay before. I was going to ask next if it is possible to experimentally verify a Counterfactual definite claim. For example, for the spin-half pair, Alice measured and Bob measured , but according to quantum mechanics, Bob would have obtained had he measured along instead.

How can this statement be verified experimentally?

Sorry about jumping the gun; I couldn't resist doing a preview.

The anti-correlation is just a result of the singlet state and is a Bell condition. If that doesn't happen, then you didn't have a singlet state to begin with. I suppose one could look at the data from recent experiments to validate it.
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