Is an experiment planned to discern determinism and randomness in QM

In summary: Since the measurements can be arranged to be space-like, this experiment proves that the measurements CANNOT be random, and have to be predetermined.
  • #71
AndreiB said:
OK, do you agree with the conclusion that EPR proves that locality implies hidden variables?
He does not, because he does not agree with the EPR criterion of reality.
 
Physics news on Phys.org
  • #72
vanhees71 said:
The EPR argument is disproven by observation!
No logical argument has ever been disproved by observation. An observation may disprove an assumption in the argument, but not the argument itself. A logical argument can only be disproved by logic (and its derivatives, such as math).

On the other hand, the assumptions of the EPR argument are QM and locality. I'm sure you don't think that any of those assumptions has been disproved.

The thing in the EPR argument with which you actually disagree is the EPR criterion of reality. Or more precisely, that's what you would disagree with if you understood the EPR argument (without chaning your general opinions about quantum foundations). I know it, because I understand both you and EPR (I studied both for many years).
 
  • Like
Likes Jazzdude
  • #73
Can you then explain what you think is wrong in my understanding of the EPR criterion and with what you think I actually disagree?

Here's what I think:

What I disagree (in agreement with QT) with is the conclusion that due to the 100% correlations described by entangledment the corresponding observables must take determined values before measurement and thus QT were incomplete. One way out is the assumption of hidden variables which we don't know and thus can only describe with probabilities but which always determine the values of all observables.

In the EPR paper, as far as I understand it, they mean by reality indeed that the values must be predetermined, as I take from the statement: "...when the operators corresponding to two physical quantities that do not commute the two quantities cannot have simultaneous reality." I'd not say "cannot have simultaneous reality" but "usually cannot be both determined". Indeed usually two non-commuting self-adjoint operators do not have common eigenvalues, and thus there's no state where the corresponding observables both take determined values.

[Of course, there are exceptions: E.g., two non-collinear components of orbital angular momentum are represented by non-commuting self-adjoint operators but in states with ##\ell=0## all angular-momentum components simultaneously have the determined value 0, but that's not the point here.]

What I conclude from this is that EPR mean by "an observable has reality" that this observable takes a determined value.
 
  • #74
AndreiB said:
The hidden variables are certainly measurable. It is what you actually measure.
Bell makes no such assumption. A hidden variable model can have the hidden variables as measurable, but it is not required to.
 
  • Like
Likes vanhees71
  • #75
AndreiB said:
Fast Vacuum Fluctuations and the Emergence of Quantum Mechanics
Gerard 't Hooft
Found.Phys. 51 (2021) 3, 63
DOI: 10.1007/s10701-021-00464-7

"Fast moving classical variables can generate quantum mechanical behavior. We demonstrate how this can happen in a model. The key point is that in classically (ontologically) evolving systems one can still define a conserved quantum energy. ..."

May I ask: what does 't Hooft mean by "fast moving classical variables"? Is he including or requiring or implying superluminal transportation of some form of information for his argument?
 
  • #76
Demystifier said:
I have no idea what are you trying to say. For example, how does Bohmian mechanics imply non-determinism?
It doesn't. Contextuality *implies* non-determinism... but not strictly so. After all, it is the measurement context that provides us the information about correlations, and nothing else. Surely it must seem odd that no one has ever been able to pinpoint experimentally any prior cause that explains the apparently random outcomes. Again, this is not a strict argument.
 
  • #77
AndreiB said:
EPR is based on only 2 premises:

1. locality (space-like events do not cause each other)
2. The predicted perfect correlations exist.

As far as I can tell, nothing you said here, about delayed choices, has anything to do with these two premises. So, the conclusion of the argument (hidden variables exist) necessary follows.

No, it is based on more than these 2. You skipped the following crucial assumption (quoting from EPR):

"Indeed, one would not arrive at our conclusion if one insisted that two or more physical quantities can be regarded as simultaneous elements of reality only when they can be simultaneously measured or predicted. On this point of' view, since either one or the other, but not both simultaneously, of the quantities P and Q can be predicted, they are not simultaneously real. This makes the reality of P and Q depend upon the process of measurement carried out on the first system, which does, not disturb the second system in any way. No reasonable definition of reality could be expected to permit this."

It was precisely this assumption, and no other, that Bell challenged - and it was found wanting. This assumption is essentially that reality is not subjective... i.e. is NOT contextual.
 
  • Like
Likes Lord Jestocost
  • #78
DrChinese said:
No, it is based on more than these 2. You skipped the following crucial assumption (quoting from EPR):

"Indeed, one would not arrive at our conclusion if one insisted that two or more physical quantities can be regarded as simultaneous elements of reality only when they can be simultaneously measured or predicted. On this point of' view, since either one or the other, but not both simultaneously, of the quantities P and Q can be predicted, they are not simultaneously real. This makes the reality of P and Q depend upon the process of measurement carried out on the first system, which does, not disturb the second system in any way. No reasonable definition of reality could be expected to permit this."

You are right that EPR argued for the simultaneous existence of hidden variables corresponding to non-commuting properties. This argument fails for the reason you exposed earlier, QM is a contextual theory. So, I've tried to make clear that I only look at the properties that are actually measured. So, if the X-spins are measured we can conclude that the X-spins existed before measurement. If the Y-spins are measured we can conclude that the Y-spins existed before measurement, and so on for any other orientation.

If the A measurement of the X-spin does not disturb B (locality) it follows that the A measurement should let B in the same state it was before the A measurement. this is what "not disturb" means. We know that after the A measurement B is in a state of well defined spin, so, B had to be in the same state, of well defined spin, (since it was not disturbed) even before.

DrChinese said:
It was precisely this assumption, and no other, that Bell challenged - and it was found wanting. This assumption is essentially that reality is not subjective... i.e. is NOT contextual.

Contextual means that the property of interest depends on the experimental context. The experimental context is simply the way the experimental parts are arranged, it's as objective as you can get.

A theory is contextual when the objects described by that theory interact. In order to predict Earth's future state it's not enough to know its present position and momentum, you also need "contextual" information, like what other massive objects are, where they are and where they are going. You need to know about the Sun, Moon, Jupiter, the rest of the galaxy and so on. QM is the same. It has nothing to do with subjectivity. the outcome of an experiment only depends on how the experimental parts are arranged, not on the mood of the experimenter. A two slit experiment does not show interference if a particle detector is placed at the slits even if the experimenter does not know about the detectors. It's the objective description of the experiment that matters.
 
  • Skeptical
Likes PeroK
  • #79
AndreiB said:
In order to predict Earth's future state it's not enough to know its present position and momentum, you also need "contextual" information, like what other massive objects are, where they are and where they are going. You need to know about the Sun, Moon, Jupiter, the rest of the galaxy and so on. QM is the same.
QM is not the same as classical mechanics! There never has been any viable classical model of the atom. QM didn't replace CM at the subatomic level, because CM was never successful in that case.

Forget about entanglement and the Bell theorem, and focus solely on electron spin. First, there must be a lot of hidden variables. You cannot model electron spin by specifying a single axis of rotation. There must be a hidden variable for every conceivable measurement angle.

This is where Einstein was being slightly disingenuous IMHO. Of course, electron spin could theoretically be governed by hidden variables. But, it's incredibly messy to say how those variables are organised.

Einstein was already on shaky ground even without entanglement. That's why Bohr, Heisenberg and the rest were convinced of QM decades before the tests of Bell's theorem.

The battleground shifted to entanglement because Einstein believed that would undermine QM. But of course, the results vindicated QM and further undermined hidden variables. Not the reverse.

Leaving aside BM, the battleground after the test of Bell's theorem has shifted to ever more bizarre reworking of determinism, such as superdeterminism. Whereas, those who broadly support orthodox QM have hardly had to modify their understanding in a century.

You have this whole debate back to front. There is no solid deterministic edifice. Instead, there is a solid QM edifice, which the determinists by hook or by crook are hoping to topple. But, again leaving BM aside, there is no solid deterministic edifice waiting to replace QM. Only wishful thinking held together by a belief in unknown laws that result in almost magical correlations.

That's why QM is mainstream science and hidden variables are not.
 
  • Like
Likes mattt, DrChinese, vanhees71 and 2 others
  • #80
DrChinese said:
This assumption is essentially that reality is not subjective... i.e. is NOT contextual.
I strongly disagree with identification subjective=contextual. If something depends on the apparatus, but not on a conscious perception, then I would call it contextual but not subjective. It is only QBism that strictly identifies contextual with subjective.
 
  • Like
Likes mattt and vanhees71
  • #81
PhilDSP said:
May I ask: what does 't Hooft mean by "fast moving classical variables"? Is he including or requiring or implying superluminal transportation of some form of information for his argument?
No, 't Hooft's model is a cellular automaton, an array of cells, each cell updating at some time interval according to some local rule (the state of a cell changes based on its previous state and the states of the surrounding cells). At each "tick" all cells update. This implements a speed limit, so the theory is local.

Nothing actually moves, it's like a TV screen. The pixels change color, but the pixels themselves don't move. The perceived motion is limited at one cell/update time.

By "fast" variables I think he means variables that change their state very quickly (still not faster than the update time). The on/off state of a pixel will change, say 60 times/s, this would be "fast". But the color of the pixel needs not change that fast, so it would be "slow". Or you can think of a piece of wood floating on water. It's position is ultimately determined by the water molecules it interacts with. The motion of those molecules is much faster than the motion of the wood.
 
  • #82
AndreiB said:
So, if the X-spins are measured we can conclude that the X-spins existed before measurement. If the Y-spins are measured we can conclude that the Y-spins existed before measurement, and so on for any other orientation.
PeroK said:
Forget about entanglement and the Bell theorem, and focus solely on electron spin. First, there must be a lot of hidden variables. You cannot model electron spin by specifying a single axis of rotation. There must be a hidden variable for every conceivable measurement angle.
Have you tried to work out how this predetermination of the spin works in BM? Let me try myself ... how do I actually model the fact that the X-spins have been measured by both Alice and Bob?

PeroK said:
Leaving aside BM, the battleground after the test of Bell's theorem has shifted to ever more bizarre reworking of determinism, such as superdeterminism.
Well, superdeterminism is both a label for an assumption (its absence) in Bell's theorem, and a label for some absurd mechanism people imagined how it could be used to produce the correlations predicted by QM. But there is a deeper issue, namely that our ignorance of initial conditions does not always come with a probability distribution (or improper Bayesian prior) for that unknow part. There is a probability distribution for the particle positions in BM, but note that we are also ignorant about most parts and details of the wavefunction. And there seems to be no canonical probability distribution for that part.
 
  • #83
DrChinese said:
No, it is based on more than these 2. You skipped the following crucial assumption (quoting from EPR):

"Indeed, one would not arrive at our conclusion if one insisted that two or more physical quantities can be regarded as simultaneous elements of reality only when they can be simultaneously measured or predicted. On this point of' view, since either one or the other, but not both simultaneously, of the quantities P and Q can be predicted, they are not simultaneously real. This makes the reality of P and Q depend upon the process of measurement carried out on the first system, which does, not disturb the second system in any way. No reasonable definition of reality could be expected to permit this."

It was precisely this assumption, and no other, that Bell challenged - and it was found wanting. This assumption is essentially that reality is not subjective... i.e. is NOT contextual.
EPR overlook that the entangled particles are one system. The very definition of entanglement is that, well, subsystems are entangled or, as Einstein said in a way better than the EPR paper in 1948, inseparable.

A. Einstein, Quantenmechanik und Wirklichkeit, Dialectica 2,
320 (1948),
https://doi.org/10.1111/j.1746-8361.1948.tb00704.x

I don't know, how you come to the conclusion that QT is not objective though. Are you a qubist now?
 
  • #84
PeroK said:
QM is not the same as classical mechanics!
I didn't say that.

PeroK said:
There never has been any viable classical model of the atom. QM didn't replace CM at the subatomic level, because CM was never successful in that case.
I guess you wanted to say "QM DID replace CM". Agreed.

PeroK said:
Forget about entanglement and the Bell theorem, and focus solely on electron spin. First, there must be a lot of hidden variables. You cannot model electron spin by specifying a single axis of rotation. There must be a hidden variable for every conceivable measurement angle.
Indeed.
PeroK said:
This is where Einstein was being slightly disingenuous IMHO. Of course, electron spin could theoretically be governed by hidden variables. But, it's incredibly messy to say how those variables are organised.

I didn't say its easy. The problem is that I have a sound logical argument that links the existence of those hidden variables to locality, and locality is very likely to be true. I think it is perfectly reasonable to choose a "messy" and local theory over a simple and non-local one. You need to take into account that modern physics is not only QM, it's also GR. Making GR indeterministic and non-local does not seem to work, right?

PeroK said:
The battleground shifted to entanglement because Einstein believed that would undermine QM.
He proved QM incomplete or non-local. That result still stands. The mistake of EPR was that they insisted on the existence of HV for non-commuting properties, allowing Bohr to escape. But the argument works fine for only the measured values. Had Bohr been presented with this, simplified argument, he would have been defeated.

PeroK said:
But of course, the results vindicated QM and further undermined hidden variables. Not the reverse.
What results? EPR assumed QM gives the right predictions, so QM's predictions being confirmed could not possibly undermine the argument. QM predicts perfect correlations. Local randomness would predict correlations 50% of the time. Local randomness is falsified, end of story.

PeroK said:
Leaving aside BM, the battleground after the test of Bell's theorem has shifted to ever more bizarre reworking of determinism, such as superdeterminism.
This is not bizarre. Since EPR proved local indeterminism impossible, and Bell proved a type of local determinism impossible, the only local option remains superdeterminism. What I find even more bizarre is the belief in logically impossible fundamental theories, like local and non-deterministic ones.

PeroK said:
Whereas, those who broadly support orthodox QM have hardly had to modify their understanding in a century.
This is why the unification program along string theory is such a success. As long as the local/non-local character of QM is irrelevant (as in the case of optimising a superconductor), the theory works fine and one is free to ignore EPR. When locality matters, such is the case of unification program, nature hits the indeterminist hard, again and again.

PeroK said:
You have this whole debate back to front. There is no solid deterministic edifice.
Yes, there is. Locality is very likely right, there is no evidence against it, all our theories accept it, including GR. We have a sound argument proving that locality implies determinism. I cannot think of any better evidence for determinism than that. 100% correlations between space-like measurements utterly falsify indeterminism.

PeroK said:
Instead, there is a solid QM edifice, which the determinists by hook or by crook are hoping to topple.
You simply assume QM is fundamentally indeterministic, instead of a statistical theory. This assumption is unjustified. What's wrong with a solid statististical edifice?

PeroK said:
But, again leaving BM aside, there is no solid deterministic edifice waiting to replace QM.
Indeed.

PeroK said:
Only wishful thinking held together by a belief in unknown laws that result in almost magical correlations.

You seem not to understand that determinism is imposed by locality as a conclusion of a sound argument. Determinism is not an assumption. It's not about what one desires or finds philosophically pleasing. The correlations are "magical" only for the non-determinist. For a determinist they are just another case of past common cause, an explanation that always worked till now.
 
  • Skeptical
Likes PeroK
  • #85
@AndreiB I'm not sure we've ever had anyone on here before who has argued that the 20th Century provided an unbroken and unassailable vindication of deterministic mechanics!

What you are posting is, IMHO, pure nonsense.

The QM model of the atom is the only viable model there has ever been. There's no other explanation for chemistry, nor has there ever been.
 
  • Like
Likes EPR and vanhees71
  • #86
Demystifier said:
He does not, because he does not agree with the EPR criterion of reality.

i don't think the criterion can be denied. The criterion says that if you an element of reality exists if you can predict that quantity without disturbing the system. Now, if you don't disturb B by your A measurement, and QM says that your A measurement leaves B in well-defined spin state it logically follows that B was in a well-defined spin state before your A measurement. As Tim Maudlin said, the criterion is "analytic", it necessary follows from the meaning of the words. The only way out is to deny that A does not disturb B (and accept non-locality) or deny the QM prediction (that the state after the A measurement is a well-defined spin, opposite to the one found at A.
 
  • #87
Logic only tells you formal rules to deduce from the assumptions on the truth of propositions the truth of other propositions.

An important part we have learned about Nature is the atomistic structure of matter, which implies that it is impossible to measure the "atoms" without disturbing them, because we need at least one other "atom" to measure. There's no way to measure anything without interacting with it in such a way as to disturb the system.

That's also true in a way when measuring far distant entangled parts of a quantum system. Though there is no non-local interaction by measurement at A's position on the part at B's position, nevertheless the system as a whole is disturbed in such a way that the entanglement is destroyed. This is unavoidable. You can also gain information on the outcome of certain measurements at B having measured A, but this does not in any way justify EPR's conclusion that this measured value at B was predetermined before A's measurement. To the contrary, for a maximally entangled system the observables of the parts are both usually maximally indetermined.
 
  • #88
PeroK said:
@AndreiB I'm not sure we've ever had anyone on here before who has argued that the 20th Century provided an unbroken and unassailable vindication of deterministic mechanics!

I didn't make such a claim. Local indeterminism has been refuted, not indeterminism per se. If you disagree with the argument, please present your refutation here! here is the argument again:

If the A measurement of the X-spin does not disturb B (locality) it follows that the A measurement should let B in the same state it was before the A measurement. this is what "not disturb" means. We know that after the A measurement B is in a state of well defined spin, so, B had to be in the same state, of well defined spin, (since it was not disturbed) even before.

OK? Explain me what is wrong with the above argument!

PeroK said:
The QM model of the atom is the only viable model there has ever been. There's no other explanation for chemistry, nor has there ever been.

This does not prove that QM must be fundamentally indeterministic. A correct, yet statistical approximate theory could do the job.
 
  • #89
AndreiB said:
I guess you wanted to say "QM DID replace CM". Agreed.
Be very careful with such comments. They might indicate a missing effort from your side to try to understand what your communication partner was saying.

AndreiB said:
The problem is that I have a sound logical argument that links the existence of those hidden variables to locality, and locality is very likely to be true.
Even so the word "local" has a clear meaning, it is a property of something in some context. Asserting "locality is true" is a pretty meaningless statement, as long as no context is given, and even with context you should still try to clarify what it is that is asserted to be local.

For example, in a classical computer, communication of information is normally local. Storage of information can be local too, but sometimes error correction codes are used to explicitly avoid locality of storage, for example on CD/DVDs. The state in QM behaves like such error correction codes in certain ways, and seems to exhibit a similar kind of nonlocality (or inseparability as many people here prefer to say).
 
  • #90
AndreiB said:
i don't think the criterion can be denied. The criterion says that if you an element of reality exists if you can predict that quantity without disturbing the system. Now, if you don't disturb B by your A measurement, and QM says that your A measurement leaves B in well-defined spin state it logically follows that B was in a well-defined spin state before your A measurement. As Tim Maudlin said, the criterion is "analytic", it necessary follows from the meaning of the words. The only way out is to deny that A does not disturb B (and accept non-locality) or deny the QM prediction (that the state after the A measurement is a well-defined spin, opposite to the one found at A.
I think there is a logical third way out. I can predict what will be the result of measuring B at the time when I measure B, but I can deny that B had any value at all before I measured it. That's indeed how Copenhagenish (non-realist) type of interpretations work.
 
  • #91
vanhees71 said:
An important part we have learned about Nature is the atomistic structure of matter, which implies that it is impossible to measure the "atoms" without disturbing them, because we need at least one other "atom" to measure. There's no way to measure anything without interacting with it in such a way as to disturb the system.
True.
vanhees71 said:
That's also true in a way when measuring far distant entangled parts of a quantum system. Though there is no non-local interaction by measurement at A's position on the part at B's position, nevertheless the system as a whole is disturbed../

Relativity precludes the existence of extended systems that are "disturbed" simultaneously in all locations. If you have a rod connecting A to B and you rotate the A end, the B end will not rotate until a light signal could reach it from A. Rigid rods are impossible in relativity. So, by speaking about "the system as a whole is disturbed" you commit to non-locality.
vanhees71 said:
You can also gain information on the outcome of certain measurements at B having measured A, but this does not in any way justify EPR's conclusion that this measured value at B was predetermined before A's measurement.
Let's say the A measurement was UP. QM says that the state of B is DOWN (regardless if B was measured or not). If the A measurement did not change B and B is DOWN what was the state of B before the A measurement? The only answer is DOWN. If it was UP before the A measurement, and DOWN after the measurement it means that the A measurement did change B. If it was in an undecided state before the A measurement, and DOWN after the measurement it means that the A measurement did change B. If it was a 6-dimentional pink rabbit before the A measurement, and DOWN after the measurement it means that the A measurement did change B. And so on. The only state B could have had before the A measurement that is consistent with the requirement that it was not changed by the A measurement is DOWN. So, for that particular experiment we proved that the DOWN state of B is predetermined.
vanhees71 said:
To the contrary, for a maximally entangled system the observables of the parts are both usually maximally indetermined.
 
  • #92
AndreiB said:
Let's say the A measurement was UP. QM says that the state of B is DOWN (regardless if B was measured or not). If the A measurement did not change B and B is DOWN what was the state of B before the A measurement? The only answer is DOWN.
If two particles are entangled they do not have individual states before measurement: that is the definition of entangled. In QM you cannot talk about the state of each particle before measurement.

This question and your answer reveal that you do not understand quantum entanglement. And, crucially, you are imposing your own realist ideas in place of quantum mechanics.

All your arguments in this thread are based on a lack of understanding of QM.
 
  • #93
AndreiB said:
Let's say the A measurement was UP. QM says that the state of B is DOWN (regardless if B was measured or not). If the A measurement did not change B and B is DOWN what was the state of B before the A measurement? The only answer is DOWN. If it was UP before the A measurement, and DOWN after the measurement it means that the A measurement did change B. If it was in an undecided state before the A measurement, and DOWN after the measurement it means that the A measurement did change B. If it was a 6-dimentional pink rabbit before the A measurement, and DOWN after the measurement it means that the A measurement did change B. And so on. The only state B could have had before the A measurement that is consistent with the requirement that it was not changed by the A measurement is DOWN. So, for that particular experiment we proved that the DOWN state of B is predetermined.
I have a pair of new identical socks. I put one, let's call it A, on my left foot and it beomes a left sock. Instantaniously the other sock, let's call it B, becomes a right sock. Was B a right sock all along or did the sock A change it? Is there a cause and effect relationship? I personally don't have a problem with my socks to not have a predetermined value of their left/right-ness, and I don't need a spooky action at a distance to explain any of the above.
 
  • Like
Likes gentzen
  • #94
Demystifier said:
I think there is a logical third way out. I can predict what will be the result of measuring B at the time when I measure B, but I can deny that B had any value at all before I measured it. That's indeed how Copenhagenish (non-realist) type of interpretations work.

This is not a way out. The A measurement leaves B in a spin DOWN state. If A measurement did not disturb B, B was in a spin DOWN before the A measurement, and also before the B measurement (in some reference frame).

What you are saying refers to the meaning of a spin DOWN state. Is there a "real" particle or it's just a propensity for the instrument to give a "DOWN" outcome? It does not matter. EPR proves that the DOWN propensity was there before both A and B measurements. Since a DOWN propensity is experimentally distinguishable from an UP propensity or no propensity at all, they cannot negate it.
 
  • #95
AndreiB said:
This is not a way out. The A measurement leaves B in a spin DOWN state. If A measurement did not disturb B, B was in a spin DOWN before the A measurement, and also before the B measurement (in some reference frame).

What you are saying refers to the meaning of a spin DOWN state. Is there a "real" particle or it's just a propensity for the instrument to give a "DOWN" outcome? It does not matter. EPR proves that the DOWN propensity was there before both A and B measurements. Since a DOWN propensity is experimentally distinguishable from an UP propensity or no propensity at all, they cannot negate it.
I've constructed an explicit hidden variable model in which those arguments are invalid.
https://arxiv.org/abs/1112.2034
 
  • Like
Likes gentzen and PeroK
  • #96
martinbn said:
I have a pair of new identical socks. I put one, let's call it A, on my left foot and it beomes a left sock. Instantaniously the other sock, let's call it B, becomes a right sock. Was B a right sock all along or did the sock A change it? Is there a cause and effect relationship? I personally don't have a problem with my socks to not have a predetermined value of their left/right-ness, and I don't need a spooky action at a distance to explain any of the above.
In your example the correlation has nothing to do with the socks, but with the "instruments", your feet. The socks simply reveal a pre-existing correlation between the instruments. Since your "instruments" will always give you the same result, the left foot will only give "left" socks, and the right one only right socks the experiment fails to reproduce the EPR setup. Anyway, the explanation for the observed correlations is still in terms of deterministic "hidden variables". The left and right feet were there before the experiment, the results were predetermined.
 
  • #97
AndreiB said:
In your example the correlation has nothing to do with the socks, but with the "instruments", your feet. The socks simply reveal a pre-existing correlation between the instruments. Since your "instruments" will always give you the same result, the left foot will only give "left" socks, and the right one only right socks the experiment fails to reproduce the EPR setup. Anyway, the explanation for the observed correlations is still in terms of deterministic "hidden variables". The left and right feet were there before the experiment, the results were predetermined.
You are missing the point. Suppose I have two new socks, neither has been molded by my left or right foot. One of the socks is white, the other is black. Sometimes the outcome of my experiment will be a white left and a black right, sometimes a black left and a white write.

Also your complaint about the instruments applies to the EPR set up as well. You get 100% correlation only of you measure along the same axis.
 
  • #98
Demystifier said:
I've constructed an explicit hidden variable model in which those arguments are invalid.
https://arxiv.org/abs/1112.2034

You say:

"Presumably, any observation ultimately happens in some part of a (conscious) brain, which is an object well localized in space. In this sense, observations are local events. In particular, when an experimentalist (say, Alice) studies nonlocal EPR correlations, then all what she really observes are signals conveyed to her brain, even if some of these signals originated from a distant apparatus that measured spin of a distant member of the EPR pair. In this way Alice can insist that, from her point of view, entangled particles and the distant apparatus do not really exist. From her point of view, all what exists are her observations, which are local."

This line of argumentation, common to QBists is fallacious. The concept of a "local brain" presupposes an external objective world in which this brain exists at a certain location. If the QBist is serious, his brain is just another observation, an object in his mind. His mind is the whole universe, his brain is just an object "imagined" by his mind.

The QBist is then accustomed to "relativistic" observations. Of course, they all happen in his mind, like everything else. However, he notices that the speed of light limits the capability of his mind to imagine things. He can imagine Earth and Mars and he can imagine taking a picture of Mars from Earth with a camera but he is unable to imagine taking an "instantaneous" picture of Mars. for some reason, there is a time delay when his mind imagines distant things.

Then the QBist is exposed to the "quantum" EPR experiment and he is presented with two logical alternatives:

1. There is no time delay when distant things are imagined, his "relativistic" observations are wrong. (non-locality)
2. There are entities that his mind imagines but he is not conscious about them. (hidden variables)

So, he is back at square 1. The rejection of the external world moved the problem to his mind, but the problem remains. Solipsism cannot evade EPR.
 
  • #99
martinbn said:
You are missing the point. Suppose I have two new socks, neither has been molded by my left or right foot. One of the socks is white, the other is black. Sometimes the outcome of my experiment will be a white left and a black right, sometimes a black left and a white write.
The point is that the "measurement" results are predetermined. Your left foot was a left foot before the experiment, the right one was right before the experiment, the white sock was white, the black sock was black. The observed correlations are explained in terms of past causes that determine them. This is the conclusion of the EPR as well, I accept that conclusion, so I don't understand what you are arguing against.

martinbn said:
Also your complaint about the instruments applies to the EPR set up as well. You get 100% correlation only of you measure along the same axis.

A Stern Gerlach device does not always measure UP or always DOWN. Your left foot always "measures" left socks. This is my complain. But the conclusion of the argument stands anyway, only in this case the "element of reality" is not the color of the sock (which is always white, in your first example) but the shape of the foot.

In the second example the "elements of reality" are both the shape of the foot and the color of the sock.
 
  • #100
AndreiB said:
The point is that the "measurement" results are predetermined. Your left foot was a left foot before the experiment, the right one was right before the experiment, the white sock was white, the black sock was black. The observed correlations are explained in terms of past causes that determine them. This is the conclusion of the EPR as well, I accept that conclusion, so I don't understand what you are arguing against.
A Stern Gerlach device does not always measure UP or always DOWN. Your left foot always "measures" left socks. This is my complain. But the conclusion of the argument stands anyway, only in this case the "element of reality" is not the color of the sock (which is always white, in your first example) but the shape of the foot.

In the second example the "elements of reality" are both the shape of the foot and the color of the sock.
Ok, here is a new pair of socks. Can you point to the left one, please! Oh, you cannot! Then what is predetermined about the leftness/rightness of the socks?!
 
  • Haha
  • Like
Likes Demystifier and PeroK
  • #101
AndreiB said:
Then the QBist is exposed to the "quantum" EPR experiment and he is presented with two logical alternatives:

1. There is no time delay when distant things are imagined, his "relativistic" observations are wrong. (non-locality)
2. There are entities that his mind imagines but he is not conscious about them. (hidden variables)
I don't think that either of the alternatives makes sense from a QBist point of view.
1. In observations by a single observer, there are always time delays. It doesn't even depend on the interpretation.
2. What does it even mean that a mind imagines without being conscious?
 
  • #102
PeroK said:
If two particles are entangled they do not have individual states before measurement: that is the definition of entangled.
OK, so the state of B before measurement is "no individual state". The state after measurement is a DOWN state. So, the A measurement changed B. Welcome to nonlocality!
PeroK said:
In QM you cannot talk about the state of each particle before measurement.
False. You CAN talk about it, in the sense that such a "talk" does not contradict any postulate of QM. What is true is that QM does not describe those states, and this is the reason the EPR argument proves (assuming locality) that QM is not a complete theory.

PeroK said:
This question and your answer reveal that you do not understand quantum entanglement.
I'm not going to answer to this ad hominem.

PeroK said:
And, crucially, you are imposing your own realist ideas in place of quantum mechanics.
Can you quote the part of the argument where I "imposed" realism?

PeroK said:
All your arguments in this thread are based on a lack of understanding of QM.
Well, it should be easy for you to point the errors, isn't it? Till now you just admitted to non-locality, you learn fast!
 
  • #103
Demystifier said:
1. In observations by a single observer, there are always time delays. It doesn't even depend on the interpretation.
Yes, time delays consistent with the c limit. EPR contradicts that limit, so the QBist is in trouble.
Demystifier said:
2. What does it even mean that a mind imagines without being conscious?
A subconscious process, maybe? Sorry, but I don't know how to define the concept of hidden variables for a QBist. The idea is that he needs to postulate them somehow so that his relativistic observations do not contradict the quantum ones.

But it's very easy to see that the "locality" proof in your paper is wrong. Let's assume, for the sake of the argument, that a QBist is taken by Klingons, teleported instantly everywhere he likes, he takes pictures of distant places and those pictures prove to be identical to the ones obtained years later through a telescope from Earth. Now, if all this is not a proof of non-locality, nothing is. Yet, our QBist would not agree, because all are observations in his brain. So, the concept of non-locality becomes meaningless, a warp-10 klingon ship is just as local as an apple.

If you adjust your definition of locality so that it is able to distinguish between an apple and a Star Treck teleporter, the EPR proves QBism non-local.
 
  • #104
AndreiB said:
But it's very easy to see that the "locality" proof in your paper is wrong. Let's assume, for the sake of the argument, that a QBist is taken by Klingons, teleported instantly everywhere he likes, he takes pictures of distant places and those pictures prove to be identical to the ones obtained years later through a telescope from Earth. Now, if all this is not a proof of non-locality, nothing is. Yet, our QBist would not agree, because all are observations in his brain. So, the concept of non-locality becomes meaningless, a warp-10 klingon ship is just as local as an apple.
To me, all this is just an explanation why QBism is indeed a local interpretation.
 
  • #105
AndreiB said:
OK, so the state of B before measurement is "no individual state". The state after measurement is a DOWN state. So, the A measurement changed B. Welcome to nonlocality!
False. You CAN talk about it, in the sense that such a "talk" does not contradict any postulate of QM. What is true is that QM does not describe those states, and this is the reason the EPR argument proves (assuming locality) that QM is not a complete theory.I'm not going to answer to this ad hominem.Can you quote the part of the argument where I "imposed" realism?Well, it should be easy for you to point the errors, isn't it? Till now you just admitted to non-locality, you learn fast!
This whole response simply emphasises the point that we cannot debate quantum entanglement because, put simply, you do not understand it.

That you believe you do simply compounds the problem.

In an entangled pair only the system of two particles has a state. The state of B cannot change, because B had no state before measurement. The measurement breaks the entanglement after which A and B have single-particle states.

It's clear you do not understand this or its implications for EPR.
 
  • Like
Likes weirdoguy and martinbn

Similar threads

Replies
80
Views
4K
Replies
88
Views
7K
  • Quantum Interpretations and Foundations
Replies
17
Views
1K
Replies
75
Views
8K
  • Quantum Physics
2
Replies
43
Views
6K
Replies
10
Views
2K
  • Quantum Physics
Replies
9
Views
2K
  • Quantum Physics
5
Replies
157
Views
12K
  • Quantum Physics
3
Replies
94
Views
13K
Back
Top