An abstract long-distance correlation experiment

[strangerep]

Modern relativity is the claim that Nature is ruled by Lorentz invariant laws, nothing else.

But I disagree with the "nothing else" part.

I'd have said that (special) relativity encompasses at least the Poincare group, restricted by some other empirically-motivated principles such as the (apparent) non-existence of tachyons, and +ve energy. I.e., causality is certainly part of modern relativity (else "modern relativity" would make false predictions).

 

[dextercioby]

Yes, modern relativity in the absence of gravity. It's one of the puzzles of physics how the Wigner theory (which starts with Poincaré invariance) leads to the theoretical possibility of tachyons, thus to a breach of the theory it started from.

 

[stevendaryl]

IMO those two choices (say a and b) are completely independent. But, wondering if this next is an acceptable statement, I would like to add: The detectors are not independent.

The spacelike-separated detectors are correlated by a simple function of the two independent choices, the scalar product of a and b. So with C = a.b: C = +1 = parallel, C = 0 = orthogonal, C = -1 = anti-parallel, with physically-meaningful intermediate values. So IMO independent inputs do not deliver independent detectors when it comes to correlation. This seems to me to be a basis for understanding the correlation in "An abstract long-distance correlation experiment" before any experiment has been done.

I'm not sure that I understand your point, but I'm not saying that there is no correlation between the detectors. What I'm trying to do is to factor the influences on the outcomes of the detectors into things that are shared between the two detectors, and the things that are not shared. So if the outcome at Alice's detector is determined (and that seems to be what A. Neumaier is saying--that if you could take into account the entire rest of the environment, that the outcomes become deterministic, in the same way that a coin flip is deterministic, if you only knew enough about breezes and the distribution of mass, etc.) and there are no FTL influences, then it would seem that Alice's result must be a deterministic function of what Alice and Bob share, plus what influences Alice alone. In my earlier post, $\lambda$ represents everything that Alice and Bob had in common, and $\alpha$ represents what was unique to Alice (e.g., her lump of uranium, if that's what she's using to pick her detector setting), and $\beta$ represents what's unique to Bob (his lump of uranium). So if $\alpha$ and $\beta$ are independent, then that would seem to me to mean that Alice's result depends only on $\alpha$ and $\lambda$, while Bob's result depends only on $\beta$ and $\lambda$. It doesn't actually matter whether $\lambda$ itself is local, or nonlocal. It only matters that Alice's result cannot depend on $\beta$ and Bob's result cannot depend on $\alpha$.

 

[ddd123]

Instead of uranium they could be using light from distant galaxies from two antipodal regions of the sky. It's not far-fetched if you do the experiment on the ISS. Honestly, I think it drives superdeterminism to utter absurdity.

 

[zonde]

That (unlike $\lambda$, if I interpret its definition correctly) it is not determined by local information.

It does not matter how $\gamma$ is determined as long as it is independent from Alice's and Bob's measurement settings. Then it is shared information just like $\lambda$ .

It is a nontrivial restriction to assume that every piece of information must have originated at a single local point. It is this restriction that excludes nonlocal correlations.

There is no such assumption. There can be information that appears at two different locations independently. We even have a name for such information. It's called "coincidence".

 

[A. Neumaier]

What I'm trying to do is to factor the influences on the outcomes of the detectors into things that are shared between the two detectors, and the things that are not shared.

The possibility of such a separation assumes that the ''things'' are located at points. But it is precisely this idealization that plays havoc, already in classical relativity. In quantum field theory, it also causes initially problems (infinite interactions), which are then removed by renormalization. But renormalization turns point particles into point-like particles, which are (in principle infinitely) extended.

 

[A. Neumaier]

(special) relativity encompasses at least the Poincare group

Yes, special relativity encompasses the Poincare group, but relativity as such doesn't, as field theory in curved spaces (where the translation group is explictly broken but the local Lorentz groups are still intact) shows.

In quantum field theory we have to add unitaity and local commutativity, which automatically excludes tachyons. Classically, tachyons are not forbidden, and indeed Crenkov radiation is a tachyonic classical feature though it happens inside matter and not in vacuum.

 

[A. Neumaier]

There can be information that appears at two different locations independently.

But in extended objects the independentce is questionablle. The environment consists not of independent point objects.

 

[stevendaryl]

The possibility of such a separation assumes that the ''things'' are located at points. But it is precisely this idealization that plays havoc, already in classical relativity. In quantum field theory, it also causes initially problems 9infinite interactions), which are then removed by renrmalization. But renormalization turns point particles into point-like particles, which are (in principle infinitely) extended.

Well, let's look at the specific example I gave, namely the decay of uranium atoms. Alice has a blob of uranium. Bob has a blob of uranium. Yes, this situation has a description in terms of quantum field theory, with lepton and baryon fields. But are you saying that, because there is a description in terms of fields, the Geiger counter clicks at Alice and Bob are correlated in a nonlocal way?

 

[stevendaryl]

Well, let's look at the specific example I gave, namely the decay of uranium atoms. Alice has a blob of uranium. Bob has a blob of uranium. Yes, this situation has a description in terms of quantum field theory, with lepton and baryon fields. But are you saying that, because there is a description in terms of fields, the Geiger counter clicks at Alice and Bob are correlated in a nonlocal way?

Anyway, if it is true that the approximation that Alice's choice of detector settings and Bob's choice are not really independent, that seems like the superdeterminism loophole of Bell's theorem.

 

[A. Neumaier]

But are you saying that, because there is a description in terms of fields, the Geiger counter clicks at Alice and Bob are correlated in a nonlocal way?

Because of the description by means of quantum fields, the answer must of course be yes, since it is known that this produces results in accordance with the standard quantum mechanical calculations.

But the general reason is indepedent of quantum fields, namely the one given in https://www.physicsforums.com/posts/5364662 (post #132), that Bell inequality derivations assume more than just Lorentz invariance. They assume a very strong form of causality that doesn't follow from relativity. That the inequality is violated in experiments proves that a causality assumption of this form is far too strong.

A deterministic universe can be based on Lorentz invariant laws, and of course implies superdeterminism. But again, one doesn't have to assume superdeterminism to have doubts that your 3-way classification is complete.

 

[morrobay]

Because of the description by means of quantum fields, the answer must of course be yes, since it is known that this produces results in accordance with the standard quantum mechanical calculations.

But the general reason is indepedent of quantum fields, namely the one given in https://www.physicsforums.com/posts/5364662 (post #132), that Bell inequality derivations assume more than just Lorentz invariance. They assume a very strong form of causality that doesn't follow from relativity. That the inequality is violated in experiments proves that a causality assumption of this form is far too strong.

A deterministic universe can be based on Lorentz invariant laws, and of course implies superdeterminism. But again, one doesn't have to assume superdeterminism to have doubts that your 3-way classification is complete.

From post # 132 referenced above : Quote, 1 . Given locality and space like separation Alice's detector setting and measurement result have no effect on Bob's measurement result
Reply: This form of locality is not realized in nature.

Then what are the examples in nature where this form of locality does not apply and how
can this produce Bell inequality violations ?

 

[strangerep]

Yes, special relativity encompasses the Poincare group, but relativity as such doesn't, as field theory in curved spaces (where the translation group is explictly broken but the local Lorentz groups are still intact) shows.

Both special and general relativity give a light (bi-)cone structure on spacetime -- which is the important thing for causality analysis in Bell-type scenarios. I'd argue that light cone structure is implied by relativity, via the constraint that relative speed between 2 (co-located) observers is limited by $c$: there is at least an infinitesimal light cone structure associated with each observer.

The more complicated light cone structure in GR is essentially just a way to knit many infinitesimal light cones together in a continuous manner.

 

[A. Neumaier]

what are the examples in nature where this form of locality does not apply and how can this produce Bell inequality violations ?

Long distance entanglement combined with sufficient shielding from decoherence. This creates a coherent system extended over a considerable amount of space, for which our simplifying intuition of pointwise causality is misleading and (as proved by the experiments) indeed fails completely.

 

[A. Neumaier]

Both special and general relativity give a light (bi-)cone structure on spacetime -- which is the important thing for causality analysis in Bell-type scenarios. I'd argue that light cone structure is implied by relativity, via the constraint that relative speed between 2 (co-located) observers is limited by $c$: there is at least an infinitesimal light cone structure associated with each observer.

Yes, but the light cone structure is an expression of local Lorentz invariance and not of Poincare invariance. On a curved manifold you don't have a consistent notion of translation, hence no Poincare group.

Moreover, for the analysis of Bell-type scanarios one must figure out what precisely is implied by local Lorentz invariance. The very strong form implied by malines post #130 and confirmed in his post #136 to be much stronger than Lorentz invariance is a hidden assumption that impairs the argument!

Note that von Neumann had proved the nonexistence of hidden varible theories by at the time very plausible arguments, regarded to be conclusivve until Bohm discovered his deterministic pilot wave model. Only then it was noticed that his arguments were based on assumptions that are not impeccable and could be violated by sensible models.

In general, a theoretical no-go theorem only applies to situations where its assumptions are satisfied. Thus if the assumptions are stronger than warranted, it does not exclude any situation where the strong assumptions are violated. This also applies to Bell-type reasoning. Since the first two points in maline's synopsis are argued by handwaving only, and since maline conceded that they make stronger assumptions than what is required from the relativity principle, Bell's theorem and its relatives say nothing about general deterministic settings satisfying the relativity principle, as long as they violate the strong form of causality assumed.

One can restate the current state of affairs by saying: Bell's arguments together with the experimental fact that Bell inequalities are violated in Nature implies that Bell's assumptions are too strong and don't apply to Nature. One possibility is to conclude that Nature is necessarily nondeterministic and has properties seemingly violating the principle of relativity. But a much more natural possibility is to conclude that Nature doesn't honor the strong assumptions implicit in steps 1 and 2 of maline's synopsis. They are simply too strong, and not justified by the relativity principle in the form we can be sure about at the present stage of our knowledge - which is just local Lorentz invariance. One day, soneone will perhaps find a deterministic and relativistic model showing this explicitly.

To close this gap in Bell's argument one would have to prove by a formal, conclusive argument (rather than the usual handwaving) that local Lorentz invariance alone implies Bell's locality assumption. I don't think this is possible.

 

[maline]

Since the first two points in maline's synopsis are argued by handwaving only, and since maline conceded that they make stronger assumptions than what is required from the relativity principle

Please don't attribute this specifically to me. I merely repeated what is explicit in every account of Bell's Theorem, including Bell's own.
Here is one that elaborates on the concept: (from wle's post above)
CERN-TH-2053 (1975)

 

[A. Neumaier]

Please don't attribute this specifically to me.
CERN-TH-2053 (1975)

This is just for easy reference. The present discussion is about physical contents, not about historical accuracy. I also do not mean to attack you, but just point out problems with the traditional argumentation.

 

[stevendaryl]

Because of the description by means of quantum fields, the answer must of course be yes, since it is known that this produces results in accordance with the standard quantum mechanical calculations.

But the general reason is indepedent of quantum fields, namely the one given in https://www.physicsforums.com/posts/5364662 (post #132), that Bell inequality derivations assume more than just Lorentz invariance. They assume a very strong form of causality that doesn't follow from relativity. That the inequality is violated in experiments proves that a causality assumption of this form is far too strong.

Well, if the point is to figure out what's weird about QM, then I think this issue is exactly what is weird about QM.

Classically, we can reason about variants of the universe: Alice announces that she will flip a coin, and decide what to do based on the coin result. We can reason about two variants of the actual universe: A universe in which the coin lands "heads-up", and a universe in which the coin lands "tails-up". The two universes would be exactly identical except for (presumably tiny) differences affecting the result of the coin tosses. Far away, Bob is also flipping coins. We assume that these two events are independent, in that we can come up with 4 variants of the universe that only differ near Alice and Bob: One where they both get "heads", one where they both get "tails", and two where they get different results.

A deterministic universe can be based on Lorentz invariant laws, and of course implies superdeterminism.

Superdeterminism is stronger than determinism. Newtonian mechanics is not superdeterministic, but it is deterministic.

Going back to my coin tosses above. It might be that the result of Alice's coin toss is deterministic, and so is the result of Bob's coin toss. The results in both cases are functions of the initial conditions of the universe. However, those initial conditions have enough leeway that the results can be treated as independent, for all practical purposes. Superdeterminism would say that there are no independent choices.

 

[stevendaryl]

I think that the direction of this discussion has changed from "Quantum mechanics is not weird" to "There is no conclusive proof that it is weird". The latter is a much weaker statement, and I guess I would agree with it.

 

[A. Neumaier]

those initial conditions have enough leeway that the results can be treated as independent, for all practical purposes. Superdeterminism would say that there are no independent choices.

Well, who knows? What is the argument for the first sentence, assuming a classical, Newtonian universe, and Alice and Bob being many-particle subsystems?

 

[stevendaryl]

Well, who knows? What is the argument for the first sentence, assuming a classical, Newtonian universe, and Alice and Bob being many-particle subsystems?

I think it's an assumption. It would be very difficult to derive it, but you could certainly test it by having Alice and Bob flip coins a bunch of times, and check for correlations.

 

[ddd123]

Could someone recap the argument for me? What is Bell's assumption that is supposedly too strong and the more sensible Lorentz invariance assumption that could escape it? I got lost in quote hopping. Thanks.

 

[stevendaryl]

Could someone recap the argument for me? What is Bell's assumption that is supposedly too strong and the more sensible Lorentz invariance assumption that could escape it? I got lost in quote hopping. Thanks.

What Bell assumed is that if there are two separate measurements done far apart (too far apart for information to travel from one to affect the other), then they are only correlated through the intersection of their backwards lightcones. So Alice and Bob each perform some measurement, and Alice gets result $A$ and Bob gets result $B$. Let $\alpha$ be a description of the state of affairs near Alice, and let $\beta$ be a description of the state of affairs near Bob, and let $\lambda$ be the state of affairs in their common backward lightcone (that is, $\lambda$ includes everything that could have affected both Bob and Alice, under the assumption that influences travel at lightspeed or slower). Then Bell assumes that

$P(A \& B | \alpha, \beta, \lambda) = P(A | \alpha, \lambda) P(B | \beta, \lambda)$

Another way of saying this is that probabilities for distant events are independent, once you've taken into account all the causal factors that might be affecting them. This is definitely not the same as Lorentz Invariance.

 

[stevendaryl]

What Bell assumed is that if there are two separate measurements done far apart (too far apart for information to travel from one to affect the other), then they are only correlated through the intersection of their backwards lightcones. So Alice and Bob each perform some measurement, and Alice gets result $A$ and Bob gets result $B$. Let $\alpha$ be a description of the state of affairs near Alice, and let $\beta$ be a description of the state of affairs near Bob, and let $\lambda$ be the state of affairs in their common backward lightcone (that is, $\lambda$ includes everything that could have affected both Bob and Alice, under the assumption that influences travel at lightspeed or slower). Then Bell assumes that

$P(A \& B | \alpha, \beta, \lambda) = P(A | \alpha, \lambda) P(B | \beta, \lambda)$

Another way of saying this is that probabilities for distant events are independent, once you've taken into account all the causal factors that might be affecting them. This is definitely not the same as Lorentz Invariance.

Yet another way to put Bell's assumption is that correlation between events implies that one event influences the other, or that some third thing influences both of them. Plus the assumption that influences travel at lightspeed or slower.

 

[zonde]

that some third thing influences both of them.

You can include that third thing in $\lambda$ if does not influence $\alpha$ and $\beta$ directly.

 

[ddd123]

Yet another way to put Bell's assumption is that correlation between events implies that one event influences the other, or that some third thing influences both of them. Plus the assumption that influences travel at lightspeed or slower.

Thanks. But isn't this just the assumption that superdeterminism is to be ruled out?

 

[A. Neumaier]

Let me attempt to refocus on stage 3 (begun at post #119), and invite again comments.

I want to add some comments on the following:

The knowledge that Alice has feels more like what we know about an
(ideal) pendulum when its initial conditions are unknown - we know the
general structure of the possible configurations, but we don't know
anything about the configuation itself. If we take the analogy seriously
we conclude that [given Norbert's fixed signalling strategy]
Nature solves an initial-value problem with two inputs
(pointer settings) and two outputs (color of response) - that on Alice's
side and that on Bob's side. The joint output depends on both inputs.

Let us consider in a bit more detail the role of knowledge in classical predictions. In a classical dynamical system, the output is not yet determined if only half the initial conditions are known. Thus our quantum system is not extraordinary in this respect. However, in our experiment the output is not even determined when also half of the output is known. This seems a bit unnatural in a classical system, if we just count the number of degrees of freedom needed. But even in classical situations, knowing half the input and half the output of a dynamical system (leading to a boundary-value problem) doesn't always determine the state of the system. examples are resonances in a linear oscillating system, and many nonlinear systems where the boundary value problem has multiple solutions.

One such system is a long and thin bar under ingoing opposite forces at both ends, which has a symmetric solution (bar under tension) and a continuum of asymmetric solutions (the buckled bar). To pick the right solution, one needs additional information. Thus that what Alice knows still leaves room for activities of Bob also has a classical analogue. Of course, all details are different, but the purpose of my remark is that most of what we find in the quantum experiment is qualitatively not too far from classical behavior.

 

[maline]

Of course, all details are different, but the purpose of my remark is that most of what we find in the quantum experiment is qualitatively not too far from classical behavior.

I'm afraid I don't see the point of focusing on the aspects of QM that are not weird. How will that help us to come to terms with the parts that are? But go on...

 

[A. Neumaier]

I'm afraid I don't see the point of focusing on the aspects of QM that are not weird. How will that help us to come to terms with the parts that are? But go on...

The goal is understanding weirdness, thereby making it less weird. Looking at both the weird and the non-weird stuff clarifies the yardsticks that can be put on the arguments. Also, I want to know how convincing my arguments are. At the end, I want to write an Insight article summarizing my position as it developed after all these long threads, and I want to use there the most effective descriptions. Thus your critique now will help me to write a better final report...

 

[wle]

To close this gap in Bell's argument one would have to prove by a formal, conclusive argument (rather than the usual handwaving) that local Lorentz invariance alone implies Bell's locality assumption. I don't think this is possible.

You've misconstrued Bell's argument. The claim was that relativistic causality, or the idea that causal influences shouldn't propagate faster than light, contradicts predictions made by quantum physics (that have since been confirmed experimentally). Among other things, Bell, quoting Einstein, says in the nouvelle cuisine essay I referenced earlier:

In 1907 he [Einstein] pointed out that if an effect followed its cause sooner than light could propagate from the one place to the other, then in some other inertial frames of reference the 'effect' would come before the 'cause'! He wrote

...in my opinion, regarded as pure logic...it contains no contradictions; however it absolutely clashes with the character of our total experience, and in this way is proved the impossibility of the hypothesis...​

of a causal chain going faster than light.

And two paragraphs later, after an example involving a hypothetical murder with a tachyon gun (emphasis added):

What we have to do then is to add to the laws of relativity some responsible causal structure. To avoid causal chains going backward in time in some frames of reference, we require them to go slower than light in any frame of reference.

This is not a hidden assumption or handwaving or a misunderstanding of relativity. Bell is quite open that he is assuming something more than Lorentz invariance only.

 

[strangerep]

Yes, but the light cone structure is an expression of local Lorentz invariance and not of Poincare invariance. On a curved manifold you don't have a consistent notion of translation, hence no Poincare group.

Let's rewind a little bit. I originally thought this thread was in the context of SR (since that's usually the case for Bell-type analyses). That's why I mentioned the Poincare group. But then, in post #147, you mentioned curved spaces, so I generalized to light cone structure. Of course, I meant generalized light "cone" structures as applicable in a curved spacetime, constructed by producing null geodesics from a given point.

But is such an enlargement of this discussion to encompass curved spacetime really necessary? Bell-type experiments are usually performed in the absence of strong gravitational fields, and certainly without any singularities nearby.
Can we therefore restrict this discussion to SR for the sake of minimizing any red herring digressions?

Moreover, for the analysis of Bell-type scanarios one must figure out what precisely is implied by local Lorentz invariance. The very strong form implied by malines post #130 and confirmed in his post #136 to be much stronger than Lorentz invariance is a hidden assumption that impairs the argument!

To keep this subdiscussion self-contained, I'll summarize. Maline wrote:

1.Given locality, and spacelike separation, Alice's detector settings and measurement result have no effect on Bob's measurement result.

2.Therefore, Bob's results depend only on the signal in Bob's region, and his settings.

which are essentially just the usual Bell criteria, as Maline said.

Maline then also said:

[...] Yes, Bell locality is intended as a stronger assumption than "relativity holds". It is justified (for me) by:

1.The intuition that causation occurs from past to present to future, in an objective sense. Since relativity does not define regions outside the light-cone as "past" or "future", causation should be confined to this cone.

2.FTL signalling would imply a possibility of sending messages to the past, and I see no fundamental reason why signals should differ from other forms of influence.

Then,

Since the first two points in maline's synopsis are argued by handwaving only, and since maline conceded that they make stronger assumptions than what is required from the relativity principle, Bell's theorem and its relatives say nothing about general deterministic settings satisfying the relativity principle, as long as they violate the strong form of causality assumed.

The first point concerns how "past" is different from "future", specifically, that an observer can only send (resp. receive) signals to (resp. from) his/her forward (resp. backward) light cone.
The second point is about an observer not being able to send or receive signals at all from outside his/her light bicone.

(The 1st first point is usually made plausible by the lack of tourists from the future, and variations on that theme.)

(I think the 2nd point does indeed follow from special relativity and is not merely "hand-waving", but I'll have to write a more extensive post to explain why.)

Which point do you think is too strong? And how do you propose to weaken it/them?

 

[stevendaryl]

Thanks. But isn't this just the assumption that superdeterminism is to be ruled out?

Yes, it definitely rules out superdeterminism, but I'm not sure that it's equivalent to ruling out superdeterminism.

 

[A. Neumaier]

This is the second and final part of my interpretation of weirdness in the present experimental setting. Its discussion will end Stage 3, and also Stage 2. Stage 4 will then address the implications for causality and relativity of what we did so far.

In our setting, assume for the moment that the nature of Norbert's signals are known to everyone, and are of the kind consistent with quantum mechanics but inconsistent with Bell-type assumptions.
Assume also that there is a human Alice behind the dumb machine Alice.

Under these conditions I want to discuss what the human Alice knows about Bob's results after she has completed her experiments.

My claim is that she knows nothing definite at all.

For the results Bob gets depend on what he is doing, and she is not informed about the latter. At best she can draw conditional inferences ''If Bob's pointer position was set to ... then his results were ...''.

Since there was no complaint about the above, it is perhaps common ground between the participants of this discussion.

How can Alice know this conditional knowledge? Only by believing the predictions of quantum mechanics. If she believes instead in a local hidden variable theory, she would have a different conditional knowledge about Bob's results. This makes it clear that what in this context is conventionally referred to as knowledge is in fact only subjective belief.

How can she believe in the predictions of quantum mechanics? Only if she has been exposed to sufficient indoctrination of the official doctrine through teaching or reading, or because in the past she had done many of these experiments herself.

But then how can she find it weird if she has seen it often enough as being real or as being convincingly conveyed to her as real? Only by an irrational act that

• (i) declares understanding based on reasoning from classical mechanics to be normal but understanding based on reasoning from quantum mechanics or from experience to be weird, while
  
• (ii) it declares predicting from classical mechanics as inappropriate but predicting from quantum mechanics or experience as trustworthy.

Thus the weirdness is in the contradictory mental attitude, not in the experimental setting or in the results obtained. It is like the weirdness in optical illusions that we have accepted as being amusing but not really weird.

 

[maline]

But then how can she find it weird if she has seen it often enough as being real or as being convincingly conveyed to her as real? Only by an irrational act that

• (i) declares understanding based on reasoning from classical mechanics to be normal but understanding based on reasoning from quantum mechanics or from experience to be weird, while
  
• (ii) it declares predicting from classical mechanics as inappropriate but predicting from quantum mechanics or experience as trustworthy.

Thus the weirdness is in the contradictory mental attitude, not in the experimental setting or in the results obtained.

In other words, "QM is correct, ergo it is not weird". Do you think that is helpful?

 

[A. Neumaier]

In other words, "QM is correct, ergo it is not weird". Do you think that is helpful?

These are your words, not mine.

I do not negate that some people find the results of bell-type experiments weird. I just explain it.

Note that my goal in this discussion is not to prove or disprove local realism in the conventional form, but (in line with the originating thread) to investigate weirdness in quantum mechanics and its dependence on the language chosen, using this specific experimental arrangement.

I said (less explicitly from the beginning, but now explicitly and substantiated) that weirdness comes from applying contradictory schemes to prediction and interpretation. This has nothing to do with correctness - whenever one applies contradictory schemes to the same situation it is likely to result in inconsistencies and the associated weirdness.

Indeed, perceived weirdness and the underlying contradictions are a sure sign of having applied somewhere something in an irrational way. It is the basis for discovering misunderstandings, and overcoming them through their analysis - not only in quantum mechanics but everywhere in science and in ordinary life.

We enjoy optical illusions because they appear weird to our senses and at the same time we understand how they come about. Therefore they don't appear weird to our intellect.

My analysis given above shows that something similar happens in certain quantum mechanical long-distance experiments. As in the case of optical illusions, one needs careful preparation of the situation in order to obtain the effect, since in the usual case (i.e., unless special efforts are made to suppress decoherence), entanglement ceases at macroscopically large distances. Our senses are trained on the latter only.

Therefore we feel irritated when confronted with special effects due to extraordinary preparation. Just as in the case of optical illusions - as you can readily verify by following the link. Enjoy!