I A computational model of Bell correlations

PAllen
Science Advisor
Messages
9,318
Reaction score
2,530
I am no expert on the nuances of assumptions of various formulations of Bell theorem(s), but wonder if the following model is adequate to explain the correlations without any non-local features. If this is a known, flawed, approach, a pointer to its refutation (or an explanation) would be appreciated.

Consider a model that any state vector implicitly includes a 'true random' seed. In Copenhagen type interpretations, when a measurement is made, this seed feeds a universal pseudo-random number generator to produce the result. Then, entangled particles simply have the feature that each one's state vector share the same 'true random seed' that is 'generated' at preparation time.

If this works, the only causal relation is between each measurement and the preparation, and there is no influence at all between spacelike separated measurements.
 
Physics news on Phys.org
I would recommend trying to explicitly derive the correlation function between measurement results for two entangled particles as a function of the measurement settings. I think you will find that it will factorize (i.e., it will be a product of two functions, one that depends only on the settings at measurement #1, and the other that depends only on the settings at measurement #2--both will also depend on the shared seed, of course). If this is the case, then your model cannot produce correlations that violate the Bell inequalities--that's the theorem that Bell proved.
 
PAllen said:
I am no expert on the nuances of assumptions of various formulations of Bell theorem(s), but wonder if the following model is adequate to explain the correlations without any non-local features. If this is a known, flawed, approach, a pointer to its refutation (or an explanation) would be appreciated.

Consider a model that any state vector implicitly includes a 'true random' seed. In Copenhagen type interpretations, when a measurement is made, this seed feeds a universal pseudo-random number generator to produce the result. Then, entangled particles simply have the feature that each one's state vector share the same 'true random seed' that is 'generated' at preparation time.

Adding to PeterDonis' comment:

There are 2 main variations to the "random" seed concept, and both fail (as you must certainly expect).

a. There is a polarization at some random angle that both express. This fails because the resulting correlation function is separable and will NOT produce "perfect" correlations at all angles. Only entangled particles produce those correlations.

b. There is a random (and possibly different) polarization for all possible angles. This produces perfect correlations at all angles. However: this fails because the resulting correlation function cannot match the predictions of QM at most other angles. You can hand select the results and it still won't work UNLESS you know the angles you plan to test in advance (which defeats the purpose of this exercise, as the observers Alice and Bob choose their angles freely). This is what we learned from Bell.

It's easy to gloss over these points when you are saying the "state vector implicitly includes a 'true random' seed". So you really have to lay out some examples for yourself so you can see what is going on with the angles. I suggest working it out with 0, 120 and 240 degrees and imagine you have an entangled pair of photons that match at the same angles (perfect correlations). If you can't do that condition, you can't go to step b. And in this simple situation, when the Alice/Bob angles are different, the experimental match rate will be 25% (per QM). However, for any example where you pick values for all 3 of those angles in advance, you can't get it less than 33%.
 
Last edited:
PAllen said:
Then, entangled particles simply have the feature that each one's state vector share the same 'true random seed' that is 'generated' at preparation time.
If you can make two copies of the seed you can make three copies of the seed just as well. Now measure one seed at zero angle, second seed at small angle to the "left" and the third seed small angle to the "right". If correlation between first and second result produce predicted value and correlation between first and third produce predicted value there is no way how correlation between second and third can produce predicted result.
 
Nice thread, but I don't see how the OP's suggestion might further our understanding of light, or of Bell's Theorem.

My reading of Bell is that he showed that hidden variable models (hvm) can't reproduce the predictions of quantum theory, and that even though it can be done if the two wings of the experiment are allowed to communicate ftl, Bell's Theorem doesn't imply ftl communication which is ruled out because of a lack of evidence for it, and because it's contradicted by accepted theory.

So what we're left with is the same lack of a deep understanding of light as before Bell's Theorem and associated works.

This is not to disparage Bell's Theorem, which is fascinating.
 
shochner said:
Nice thread, but I don't see how the OP's suggestion might further our understanding of light, or of Bell's Theorem.

My reading of Bell is that he showed that hidden variable models (hvm) can't reproduce the predictions of quantum theory, and that even though it can be done if the two wings of the experiment are allowed to communicate ftl, Bell's Theorem doesn't imply ftl communication which is ruled out because of a lack of evidence for it, and because it's contradicted by accepted theory.

So what we're left with is the same lack of a deep understanding of light as before Bell's Theorem and associated works.

This is not to disparage Bell's Theorem, which is fascinating.
The OP made a vague suggestion of how to replicate the correlations of entangled entities via local hidden variables. @PeterDonis, @DrChinese, and @zonde were attempting to help relieve him of this folly, so yes, not much new understanding there. And you're right Bell doesn't imply ftl.
However, there are accepted interpretations that assume ftl phenomena to "explain" Bell that are compatible with standard physics.
Yet indeed, light is a mystery, but so is gravity and why there is a universe, and ...
 
My reasoning is (often) thus: the correlation depends on the relative angle of the both detectors, and as such must have some sort of nonlocality.
 
Zafa Pi said:
The OP made a vague suggestion of how to replicate the correlations of entangled entities via local hidden variables. @PeterDonis, @DrChinese, and @zonde were attempting to help relieve him of this folly, so yes, not much new understanding there. And you're right Bell doesn't imply ftl.
However, there are accepted interpretations that assume ftl phenomena to "explain" Bell that are compatible with standard physics.
Yet indeed, light is a mystery, but so is gravity and why there is a universe, and ...
Hm, I'd say light is far from being a mystery but being among the best understood phenomena (with QED). You are right, gravitation is still a mystery in the sense that there's not yet a consistent quantum theory of the gravitational interaction.
 
entropy1 said:
My reasoning is (often) thus: the correlation depends on the relative angle of the both detectors, and as such must have some sort of nonlocality.
Can you prove ER = EPR (wormholes) is wrong?
 
  • #10
Zafa Pi said:
Can you prove ER = EPR (wormholes) is wrong?
I'm not familiar with that. Is that local?

Of course there is the option to drop realism.
 
Last edited:
  • #11
vanhees71 said:
Hm, I'd say light is far from being a mystery but being among the best understood phenomena (with QED). You are right, gravitation is still a mystery in the sense that there's not yet a consistent quantum theory of the gravitational interaction.
Mystery is certainly not a well defined term, but Feynman (well acquainted with QED) continually thought photons were a mystery. He claimed the double slit phenomena an ultimate mystery.

When I mentioned that gravity was a mystery I wasn't thinking about the problems related to quantum gravity. It is more along the lines of Newton's comment that he had no explanation for how masses pulled off his laws. The notion of a gravitational field or QFT (and their wonderful predictions) may satisfy you and others, but many still feel bereft as to how those fields get created, how mediators get exchanged, how entangled photons correlate themselves, how a photon interferes with itself at the slit.

If you think that is just the way of nature and we should just move on (a variation of shut up and calculate) well good for you. Perhaps you can console Feynman, and Einstein, in their repose. And me as well.:sorry:
 
  • Like
Likes M Saad
  • #12
entropy1 said:
I'm not familiar with that. Is that local?

Of course there is the option to drop realism.
Google ER = EPR and you decide. It seems so to me.
Indeed, dropping realism is an option, but it is hard to visualize.
 
  • #13
Zafa Pi said:
Can you prove ER = EPR (wormholes) is wrong?

ER = EPR doesn't refute Bell's Theorem. It is just a proposed "mechanism" for producing correlations that violate the Bell inequalities; it doesn't show that such correlations don't violate locality in the sense that Bell defined the term.
 
  • #14
PeterDonis said:
ER = EPR doesn't refute Bell's Theorem. It is just a proposed "mechanism" for producing correlations that violate the Bell inequalities; it doesn't show that such correlations don't violate locality in the sense that Bell defined the term.
Your first sentence can not be disputed, no physics can refute a mathematical theorem. I agree with the first half of your second sentence. I'm having difficulty with the second half due to several negatives, and a long dispute in another thread over Bell's sense of locality.

In post #7 @entropy1 said there must be some sort of nonlocality. I'm not sure what he meant by nonlocality, some mean ftl phenomina (see post #5). It seems possible in my mind that the ER = EPR "mechanism" can produce the correlations that violate Bell's inequality without invoking ftl. The distant entangled particles are not distant after all.
 
  • #15
Zafa Pi said:
I'm not sure what he meant by nonlocality

Bell's definition was very simple: "locality" means the function describing the correlation between the two measurement results factorizes (i.e., it is the product of two functions, each of which depends only on one of the two measurement settings); "nonlocality" means it doesn't.

Most discussions (probably including the one in the other thread you refer to) get bogged down because they don't give a precise definition to the term "locality" as Bell did.
 
  • #16
Zafa Pi said:
It seems possible in my mind that the ER = EPR "mechanism" can produce the correlations that violate Bell's inequality without invoking ftl.

No, it can't. ER = EPR does not create timelike or lightlike paths between the two measurement events, which is what would be needed for this.
 
  • #17
Zafa Pi said:
Mystery is certainly not a well defined term, but Feynman (well acquainted with QED) continually thought photons were a mystery. He claimed the double slit phenomena an ultimate mystery.
Well, at the same time, Feynman has among the best introductory chapters on QM. As Einstein said about theoretical physicsts: "Don't listen to their words but see their deeds."

http://www.feynmanlectures.caltech.edu/III_01.html
 
  • #18
Zafa Pi said:
I'm not sure what he meant by nonlocality
I mean the information required to constitute the correlation, when adopting realism, that is the detectors really yield the measurement result at the moment of measurement, is spacelike separated at first and can (to my understanding, yet) not be explained locally, that is, within the limits of lightspeed.

(unless you drop realism of course)
 
  • #19
PeterDonis said:
No, it can't. ER = EPR does not create timelike or lightlike paths between the two measurement events, which is what would be needed for this.
So is ER=EPR a local or a non-local theory (in the Bell sense)? I'm asking because the ER side is supposed to be described by general relativity, which is local.
 
  • #20
Demystifier said:
is ER=EPR a local or a non-local theory (in the Bell sense)?

Since AFAIK it makes the same predictions as standard QM, it would have to be nonlocal in the Bell sense, since its predictions violate the Bell inequalities.

Demystifier said:
I'm asking because the ER side is supposed to be described by general relativity, which is local.

GR is local in the sense of obeying relativistic causality. But that's not the same as the definition of "local" that Bell used. QFT is also "local" in the sense of obeying relativistic causality (in QFT that translates to "field operators commute at spacelike separations"), but it makes predictions which are nonlocal in the Bell sense, since they violate the Bell inequalities. AFAIK QFT in curved spacetime is the same as QFT in flat spacetime in this respect.

(Btw, "described by GR" is a bit of a misnomer for the "ER" side, since we are talking about quantum phenomena and GR is not a quantum theory. A better description would be that ER = EPR does QFT in a particular curved spacetime, the "Einstein-Rosen bridge" spacetime. At least that's my understanding.)
 
  • #21
Peter, you quote me saying, "I'm not sure what he meant by nonlocality", then respond with:
PeterDonis said:
Bell's definition was very simple: "locality" means the function describing the correlation between the two measurement results factorizes (i.e., it is the product of two functions, each of which depends only on one of the two measurement settings); "nonlocality" means it doesn't.

Most discussions (probably including the one in the other thread you refer to) get bogged down because they don't give a precise definition to the term "locality" as Bell did.
You make it appear that my "he" is Bell. A bit of deft editing. "He" was referring to @entropy1 (see post #14) as "he" points out in post #18.

I am aware of Bell's mathematically precise definition of locality being factorization (joint = product of marginals), but people want a more physical description of the consequences. In the extensive paper, the team of authors say,
"As we have stressed above, the crucial assumption from which one can derive various empirically-testable Bell-type inequalities is locality. (Bell sometimes also used the term local causality instead of locality). Bell explained the "principle of local causality" as follows:

The direct causes (and effects) of events are near by, and even the indirect causes (and effects) are no further away than permitted by the velocity of light.20
In relativistic terms, locality is the requirement that goings-on in one region of spacetime should not affect — should not influence — happenings in space-like separated regions."

Though what Bell did was perhaps even Nobel worthy I dislike reading him and modern treatments make it physically clearer to me what is going on. We have been on this topic before and I didn't find it enjoyable.
 
  • #22
PeterDonis said:
No, it can't. ER = EPR does not create timelike or lightlike paths between the two measurement events, which is what would be needed for this.
Seems like a waste of a wormhole.
 
  • Like
Likes anorlunda
  • #23
entropy1 said:
I mean the information required to constitute the correlation, when adopting realism, that is the detectors really yield the measurement result at the moment of measurement, is spacelike separated at first and can (to my understanding, yet) not be explained locally, that is, within the limits of lightspeed.

(unless you drop realism of course)
I sort of agree. I would put it this way: The correlations happen at greater than lightspeed (Classical information cannot move that fast.) I guess I would call that nonlocal.
 
  • Like
Likes entropy1
  • #24
Zafa Pi said:
I sort of agree. I would put it this way: The correlations happen at greater than lightspeed (Classical information cannot move that fast.) I guess I would call that nonlocal.
Yes, I mean the speed of information is limited to c.
 
  • #25
I would like to point out that Peter’s first post in this thread is a logically complete response to my questions: that my proposed model formally fits within Bell’s locality definition and thus cannot account for Bell violating correlations. (Further, I assumed there had to be something wrong with the proposed model because it was too simple a resolution). Dr. Chinese proposed an exercise to concretely demonstrate this for a model of the type I proposed. I hope to perform this exercise some time, and post results if I get around to it. Otherwise, for me, the rest of this thread is superfluous discussion of general questions extensively dealt with in other threads. I wouldn’t mind closure of this thread - I can open a new one if I get some possibly interesting results from how a concrete realization of the model breaks down.
 
  • Like
Likes martinbn and DrChinese
  • #26
I probably didn't understand your question too well... did you mean:

measurement result A <- pseudorandom generator A <- true random seed -> pseudorandom generator B -> measurement result B?
 
  • #27
entropy1 said:
I probably didn't understand your question too well... did you mean:

measurement result A <- pseudorandom generator A <- true random seed -> pseudorandom generator B -> measurement result B?
Almost, except the pseudorandom generator at A and B necessarily use the same algorithm (universal pseudorandom generator). The mistaken idea is that algorithmic universality might replicate nonlocal correlations.
 
  • #28
PAllen said:
Almost, except the pseudorandom generator at A and B necessarily use the same algorithm (universal pseudorandom generator). The mistaken idea is that algorithmic universality might replicate nonlocal correlations.
A and B can in principle change their angle any time before measuring, right? Hence, to yield a correlation corresponding to the relative angle, A and B need to convey their angle to the other side at most at lightspeed. The alternative is to let the true random seed encode the relative angle, but this contradicts the freedom of A and B to change their angles, right?
 
  • #29
entropy1 said:
A and B can in principle change their angle any time before measuring, right? Hence, to yield a correlation corresponding to the relative angle, A and B need to convey their angle to the other side at most at lightspeed. The alternative is to let the true random seed encode the relative angle, but this contradicts the freedom of A and B to change their angles, right?
Yes, that succinctly summarizes the flaw in the model.
 
  • Like
Likes entropy1
  • #30
I thought of this: you can also apply the model to a setting with fixed angles. In that case the flaw is that, given the 50/50 randomness of the bits generated at A and at B, that the correlation is 50/50 too.
 
  • #31
entropy1 said:
I thought of this: you can also apply the model to a setting with fixed angles. In that case the flaw is that, given the 50/50 randomness of the bits generated at A and at B, that the correlation is 50/50 too.
No, I think that case can produce 100% correlation due to the shared seed, for some set ups. But it can’t produce in between correlation percentages.
 
  • #32
PAllen said:
No, I think that case can produce 100% correlation due to the shared seed, for some set ups. But it can’t produce in between correlation percentages.
Yes, probably.
 
  • #33
Zafa Pi said:
The correlations happen

Why are you assuming that correlations are something that must "happen"? We don't know that. All we know are the correlations we calculate after the fact.
 
  • #34
Zafa Pi said:
You make it appear that my "he" is Bell.

Not on purpose. My response would apply just as well to @entropy1 in post #7--that is the only definition of "nonlocality" that we have a definite theorem for.
 
  • #35
entropy1 said:
I mean the speed of information is limited to c.

What is the "speed of information"?
 
  • #36
PeterDonis said:
What is the "speed of information"?
If information is available at A, then, to make it non-trivially available at B, that can't be done faster than lightspeed. Information in this case being knowledge about a situation in A.
 
  • #37
entropy1 said:
If information is available at A, then, to make it non-trivially available at B, that can't be done faster than lightspeed. Information in this case being knowledge about a situation in A.

None of this helps any. You still haven't rigorously defined what you mean by "information" (defining it as "knowledge" doesn't help because that term is just as vague as "information"), or rigorously explained why it has to "travel" somewhere. I know it seems intuitively obvious to you, but this is one of those cases where "intuitively obvious" doesn't cut it. You need to actually try to rigorously formulate your requirement in a way that can be mathematically analyzed and used to make predictions. (That's what Bell was trying to do with his definition of "locality".)
 
  • #38
PeterDonis said:
None of this helps any. You still haven't rigorously defined what you mean by "information" (defining it as "knowledge" doesn't help because that term is just as vague as "information"), or rigorously explained why it has to "travel" somewhere. I know it seems intuitively obvious to you, but this is one of those cases where "intuitively obvious" doesn't cut it. You need to actually try to rigorously formulate your requirement in a way that can be mathematically analyzed and used to make predictions. (That's what Bell was trying to do with his definition of "locality".)
Why not use your definition?
PeterDonis said:
That is why it is said that no information can be transmitted in this manner--information transmission requires the "source" to be able to affect the "receiver" in some controllable way.
All that is needed to transmit is a pair of bits from Alice to Bob at FTL in order to conspire and get any correlations you want. Too bad it can't be done.
 
  • #39
PeterDonis said:
Why are you assuming that correlations are something that must "happen"? We don't know that. All we know are the correlations we calculate after the fact.
I may not be reading you right, but the correlations have been taking place in extreme abundance in quantum optics labs since 1981. That is why they must "happen".
I see it as the same as why apples must fall.
 
  • #40
PeterDonis said:
None of this helps any. You still haven't rigorously defined what you mean by "information"
Perhaps that what travels at speed c or slower, which is practically everything.

And "traveling": Information X "travels" from A to B if B produces a record with meaning P if and only if A has produced record X with meaning P.
 
Last edited:
  • #41
Zafa Pi said:
the correlations have been taking place

Why must correlations be things that "take place"? As I said, we don't know that they "take place". All we know is that we can calculate them after the fact.

What does "take place" in quantum optics labs is that various preparation procedures are done, various measurements are made, and various results are recorded. Where in that do "correlations take place"?

This is the problem with using ordinary language instead of math. Ordinary language is vague, and it often includes implicit assumptions that are based on our classical intuitions and which are not valid--or at least not valid as assumptions--when quantum phenomena are involved.

entropy1 said:
Perhaps that what travels at speed c or slower, which is practically everything.

If "information" is defined as "what travels at speed c or slower", then by definition, information cannot travel at FTL. Problem solved. Are you satisfied with that?

entropy1 said:
Information X "travels" from A to B if B produces a record with meaning P if and only if A has produced record X with meaning P.

If A and B are spacelike separated, how do you know which one happened first? Your "if and only if" statement requires an invariant ordering: A has to come before B. But if A and B are spacelike separated, there is no invariant ordering.
 
  • #42
PeterDonis said:
What does "take place" in quantum optics labs is that various preparation procedures are done, various measurements are made, and various results are recorded. Where in that do "correlations take place"?
Smack-dab in the recorded results.

You strike me as a smart and educated guy so I believe you are thinking of something I am not picking up on.
Consider this example:
Experiment 1) trial consists of A preforming X and getting a 1 or 0, and B preforming Y and getting 1 or 0. After many runs the results look like flips of independent fair coins.
Experiment 2) trial is like above, but the coins are not independent, and A and B's results are always the same.

In 1) the results are uncorrelated (have correlation coefficient 0).
In 2) we find that the results are highly correlated (have correlation coefficient 1).
In 2) we find correlation. In measuring entangled particles we find correlations (depending on the axes of measurement).
Does my criterion for "find" make sense?
 
  • #43
Zafa Pi said:
Smack-dab in the recorded results.

I'm sorry, you still aren't grasping my point. See below.

Zafa Pi said:
You strike me as a smart and educated guy so I believe you are thinking of something I am not picking up on.

Indeed. The correlations are in the recorded results, yes. But the correlations in the recorded results are things that we extract from those results by analyzing them. That does not in any way mean the correlations "take place". The correlations are just mathematical calculations we make. At least, that's all that follows from your statement that the correlations are in the recorded results. So if you want to convince me that the correlations are something that had to "take place", you need to make some other argument.

Zafa Pi said:
Does my criterion for "find" make sense?

Sure, but it just means what I said above: we "find" the correlations by calculating them. It does not mean the correlations had to "take place". Something took place, yes. But that doesn't mean that something is properly described as "the correlations taking place".
 
  • Like
Likes zonde
  • #44
PeterDonis said:
So if you want to convince me that the correlations are something that had to "take place", you need to make some other argument.
I had a friend look at our discussion and I wrote 6 sentences to see if she could tell which ones you would find acceptable. She, and I were not sure.
At any rate I hope you agree that coral invasions take place.:rolleyes:
 
  • Like
Likes OCR
  • #45
Zafa Pi, I think you are making category error. Correlation is not a physical mechanism, instead physical mechanisms manifest themselves as correlations in data.
 
  • #46
Zafa Pi said:
At any rate I hope you agree that coral invasions take place.:rolleyes:
That coral invasion is in your past light cone.

As you describe the setup, the correlation take place some time/where between the start of the experiment, and the collection and transport of "information" for correlation checking where it is finally "placed".

That's a bit on the vague side of things.
 
  • #47
zonde said:
Correlation is not a physical mechanism, instead physical mechanisms manifest themselves as correlations in data.
I agree, but so what?
I find birds chirping in the forest. I find beauty in the forest.
Two perfectly reasonable sentences in spite of birds chirping and beauty being different categories.
"A disagreement has taken place between A and B. " is also a valid sentence. Halfway between?
 
  • #48
Zafa Pi said:
I find birds chirping in the forest. I find beauty in the forest.
Two perfectly reasonable sentences in spite of birds chirping and beauty being different categories.
That's because "find in" in two sentences have different meanings.
Let me rewrite your sentences like that:
I find that birds chirping takes place in the forest. I find that beauty takes place in the forest.
Now you can see that second sentence has lost it's meaning.
 
  • Like
Likes Boing3000
  • #49
PeterDonis said:
Sure, but it just means what I said above: we "find" the correlations by calculating them. It does not mean the correlations had to "take place". Something took place, yes. But that doesn't mean that something is properly described as "the correlations taking place".
zonde said:
instead physical mechanisms manifest themselves as correlations in data.
The correlation is the result of dependence of the stochastic variables representing the local measurement outcomes (ie A and B). Could we speak of this "dependence" "happening"? In the sense that it "manifests itself"? Because dependence suggests a physical cause?
 
Last edited:
  • #50
Zafa Pi said:
At any rate I hope you agree that coral invasions take place.

Sure. But if we observed coral invasions taking place in two widely separated locations and calculated correlations between them (comparing how much distance the coral invaded per unit time in each place, for example), would you say those calculated correlations "take place"?
 
Back
Top