The Refutation of Bohmian Mechanics

  • #61
A. Neumaier said:
When we hear something, it can count as an observation, though no position variable is observed.
Oh, yes it is. When your ear hears something, the nerves in your ear vibrate. And vibration is nothing but a change of a POSITIONS of parts of an elastic object.

A. Neumaier said:
When we see a star, which position variable do we observe?
The position of nerves in the eye.

Of course, it's not that you really "observe" these positions in the psychological sense, but the point is that colors and sounds are ENCODED in the positions of something.
 
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  • #62
Demystifier said:
OK, now we are at the territory of statistical mechanics. In statistical mechanics there is a Boltzmann H-theorem that provides that entropy never decreases. Perhaps this theorem is not perfectly rigorous (it does not use ergodicity),
It assumes instead the Stosszahlansatz, which is taken as an unproved assumption.
(For a gas of hard spheres, the Stosszahlansatz can be justified by an ergodic theorem).

Moreover, stating that entropy doesn't decrease is very far from stating that entropy reaches its global maximum (the equilibrium state). For example, one can deduce from the Boltzmann equations in some approximation the Euler equations - there the total entropy is constant, but the dynamics is still highly nontrivial - very far from the equilibrium state. Thus the H-theorem says nothing at all about approach to equilibrium. (In simple terms: if I am climbing a hill and never go downwards, I can still end up anywhere above my current position, no matter how long I wait. No guarantee to reach the hill top.)

Finally, Boltzmann's approach only works for the classical ideal gas.
Demystifier said:
but in Bohmian mechanics there is an analogous equally (non)rigorous theorem that entropy measuring closeness to the quantum equilibrium also never decreases. So what we have in BM are
1) A theorem, probably not perfectly rigorous, and
2) Many explicit numerical simulations which agree with the theorem
I can agree that more work is needed in order to establish a completely satisfying proof, but the above is certainly a strong evidence (if not the proof).
It is as much evidence for reaching quantum equilibrium as Boltzmann's H-therorem is evidence for the universe being in global equilibrium - nil!
 
  • #63
A. Neumaier said:
Because, as you said, none of the pointer variables is ''correct''. How else would you then describe the dynamics of an unobserved system of spins?
Bohmian mechanics describes the dynamics of wave functions and particle positions, period. It does that both for observed and unobserved systems. However, Bohmian mechanics, at the fundamental level, does not describe the dynamics of spins or any other "observables". It is only in the context of specific measurements that certain configurations of particles and wave functions can be INTERPRETED as spins or other "observables".

Just as classical optics is only about electromagnetic waves and not about colors, even though some wavelengths can be interpreted as colors in specific measurement configurations.
 
  • #64
A. Neumaier said:
It is as much evidence for reaching quantum equilibrium as Boltzmann's H-therorem is evidence for the universe being in global equilibrium
With that I agree ...

A. Neumaier said:
- nil!
... but with that I don't. Anyway, I am glad that now you have a clearer picture what BM, in its current state of development, has achieved and what it has not. Just because some branch of science is not fully developed yet, it is not a reason to abandon it.
 
  • #65
Demystifier said:
Oh, yes it is. When your ear hears something, the nerves in your ear vibrate. And vibration is nothing but a change of a POSITIONS of parts of an elastic object.


The position of nerves in the eye.

Of course, it's not that you really "observe" these positions in the psychological sense, but the point is that colors and sounds are ENCODED in the positions of something.

Ah. So the only pointer variables that count are those in the head of people. For if we observe the pointer of an instrument, all we really observe is also the position of nerves in the eye?

And I never before heard that the nerves in the eye move in response to light. What moves are the electrons inside the eye. But these are not a ''POSITION variable (at the macroscopic level)''.
 
  • #66
Demystifier said:
Bohmian mechanics describes the dynamics of wave functions and particle positions, period. It does that both for observed and unobserved systems.

My question was - how, for an unobserved spin system. Your dogmatic position is of no help in answering that.
 
  • #67
Demystifier said:
With that I agree ...... but with that I don't.

If the Boltzmann's H-therorem were any evidence for the universe being in global equilibrium then
e would observe this global equilibrium - which means we wouldn't exist, contradiction.

Thus the Boltzmann's H-therorem is no evidence at all evidence for reaching global equilibrium, and because you agreed to the first part of my statement, you have also no evidence for that the state of the universe reached quantum equilibrium in BM.
 
  • #68
A. Neumaier said:
Ah. So the only pointer variables that count are those in the head of people.
Not only they, but if you want to understand how something is observed by a human, then you cannot avoid them. They are crucial.

A. Neumaier said:
For if we observe the pointer of an instrument, all we really observe is also the position of nerves in the eye?
Irrespective of one's favored interpretation of QM, that is eventually so.

A. Neumaier said:
And I never before heard that the nerves in the eye move in response to light.
They don't, but the positions of the excited nerves determine the picture you will eventually see.
 
  • #69
A. Neumaier said:
If the Boltzmann's H-therorem were any evidence for the universe being in global equilibrium then
e would observe this global equilibrium - which means we wouldn't exist, contradiction.
Irrespective of physics, this chain of reasoning is logically totally wrong.
Namely, if A is some evidence for B, it does not mean that A implies B.
For example, being in grave is an evidence for being dead, but you can still be in grave without being dead.

Anyway, perhaps we are a statistical fluctuation?
 
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  • #70
A. Neumaier said:
My question was - how, for an unobserved spin system.
I'm not sure what kind of an answer do you expect here. Perhaps the straightest answer is: through the Schrodinger (or Schrodinger-Pauli, or Dirac, or Maxwell ...) equation and the associated equation for the particle trajectories - of the isolated system.
 
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  • #71
A. Neumaier said:
If I see that I was wrong, I correct myself immediately.

So, as you haven't corrected yourself at all, do I take it you don't accept that anything that you have said is wrong?

If this is not the case, would you mind listing for me the things about which you have changed your opinion as a result of this thread?
You have not the slightest idea about how much literature I have read and how much I am reading
while preparing my contributions to this forum.

As far as deBB is concerned, you appear to be entirely ignorant of everything that has been published since the 1990s, of a great many things published before that, and of absolutely everything that refutes your and Streater's "Bohmian mechanics is demonstrably incorrect" thesis. So I feel free to make certain assumptions.
Scientific dispute takes the free offering of information as a given that doesn't need special thanks.
I also do not expect being thanked for the information I provide on this forum.

That's not my point. No-one is asking for thanks. My complaint is the following. You have made multiple statements on this thread which are demonstrably incorrect. When told they are incorrect and you apparently have no further argument, you simply move onto another point without saying whether you agree with the correction or not. Anyone reading this thread and attempting to make sense of it needs to have that information if they are to draw a conclusion about who is right and who is wrong, otherwise they might simply assume because you are a big clever person and I am a student that you automatically win. Is that your intention? Because it certainly looks like it.
You seem to say a lot without first checking the facts. I am not a professor of quantum physics.

Then I apologize for suggesting that you were.

EDIT: though looking at http://arnold-neumaier.at/im/hs97_16.gif" , you can hardly blame me for my assumption. So you're a professor of mathematics who has the foundations of quantum mechanics as one of his main research interests. Huge difference, I agree. My original point therefore stands that - as a respectable professor at a major university - you have a responsibility not to make sweeping incorrect statements damning entire fields in public forums, since people will believe you merely because of who you are.
camboy said:
from the beginning of this thread, you have made pompous statements implying that everyone who studies de Broglie-Bohm theory is an idiot.

A. Neumaier said:
Please take this back. I never said such a thing.

Then what on Earth did you mean by statements such as "The worst thing about Bohmian mechanics is their low standards of quality", "Bohmians are not aware of many things", "Bohmian trickery is inapplicable" and all the rest. Are these supposed to be compliments?

Don't misunderstand me. I am happy to debate you, but not on the understanding that you are so goddamned clever that your so-called disproof of Bohmian mechanics is so obvious it doesn't need to be peer-reviewed, or when you persist in continually using such a sarcastic tone.
 
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  • #72
A. Neumaier said:
Your claim that according to forum's rules, truth is dependent on peer reviews.
PF can decide upon what shall be discussed in its space but not upon what is true.

First, you may have noticed an emoticon by my "claim", second, strictly speaking, depending on peer reviews, truth either belongs here or not (so it is indeed "dependent" in this respect on peer reviews). With all due respect, your "truth" of post 7 does not belong here.

A. Neumaier said:
We don't need to agree. I won't defend my position here beyond whatt is already in the paper, also because of the PF rules. (However, note that my paper has been cited repeatedly in the published literature, among others in Streater's book on lost causes in physics, where he has a full chapter explaining why he thinks Bohmian mechanics is a lost cause..

No, we don't have to agree. And no, the fact that your paper has been cited does not make its discussion here appropriate. Rules are rules. I am not trying to look "holier than thou". I admit that I also sinned against this rule and got a heads-up from a mentor. Since then I tried to stick to the rules.

I am sure mentors here value your input, as I do, and would give you some slack, as I would do, if I were in their shoes, but you should not abuse our respect.

And again, if indeed the Bohm interpretation is a lost cause, so be it, but I specifically objected to your claim and was not trying to defend the interpretation. To explain my position I may mention that I had a longish discussion with a knowledgeable Bohmian here. Ironically, I also argued in that discussion that there is no clear indication of discrepancy between predictions of the Bohm interpretation and standard quantum mechanics.

A. Neumaier said:
I imagine instead that the universe is a hydrogen atom in the ground state - the electron will always stand still and the wrong statistics results.

In your example both the Bohm interpretation and standard quantum mechanics predict the same state forever. It is not at all obvious that the Bohmian interpretation gives wrong statistics in this case (unless you impose your very own theory of measurements on the Bohm interpretation, as you do in your paper). I believe this is just your personal theory.

A. Neumaier said:
Bohmians are not aware of many things; they probably never tried to bring quantum computing into their focus. The observables used there do not include a position variable, hence the Bohmian trickery is inapplicable.

If this is meant to be an argument, I fail to see how it is relevant. Maybe I just don't know enough about quantum computing though. However, I did not ask you for arguments, I asked about the status of your claim "no quantum computing in the Bohm interpretation." This is another strong claim, and I just tried to understand if that was common knowledge or just another personal theory of yours. If this is common knowledge, how about a reference? And if there is no peer-reviewed article supporting your claim, then your claim does not belong here. If this is your recent discovery, please publish it first and then discuss it here.

A. Neumaier said:
If you don't agree, then please tell me how to do quantum computing in Bohmian mechanics..

With all due respect, this is rich. You made a strong claim, and I just challenged you to support it with valid references. I am under no obligation to prove that your claim is wrong. Furthermore, I have no idea if it is indeed wrong or right.
 
  • #73
A. Neumaier said:
Bohmians are not aware of many things; they probably never tried to bring quantum computing into their focus. The observables used there do not include a position variable, hence the Bohmian trickery is inapplicable.

akhmeteli said:
If this is meant to be an argument, I fail to see how it is relevant. Maybe I just don't know enough about quantum computing though. However, I did not ask you for arguments, I asked about the status of your claim "no quantum computing in the Bohm interpretation." This is another strong claim, and I just tried to understand if that was common knowledge or just another personal theory of yours. If this is common knowledge, how about a reference? And if there is no peer-reviewed article supporting your claim, then your claim does not belong here. If this is your recent discovery, please publish it first and then discuss it here.

A. Neumaier said:
If you don't agree, then please tell me how to do quantum computing in Bohmian mechanics..

akhmeteli said:
With all due respect, this is rich. You made a strong claim, and I just challenged you to support it with valid references. I am under no obligation to prove that your claim is wrong. Furthermore, I have no idea if it is indeed wrong or right.


It is wrong. I supplied him with an appropriate reference demonstrating how to do deBB quantum computing in #22 (and again in #27 after he ignored it).

Of course he immediately dismissed it, not because of a coherent 'personal theory' but because "[deBB] can be coerced into accomodating anything - in this case by introducing artificial pointer coordinates that don't exist in the standard description". This simply means "[deBB] is not like standard QM, and I - the great Neumaier - don't like it". It is not an intellectual argument.
 
  • #74
Demystifier said:
And I never before heard that the nerves in the eye move in response to light.
They don't, but the positions of the excited nerves determine the picture you will eventually see.
But in the Bohmian interpretationl, one interprets only changes in the pointer varibles as observables.. Thus the nerves won't serve as pointer variables to observe light.
 
  • #75
If the Boltzmann's H-therorem were any evidence for the universe being in global equilibrium then
e would observe this global equilibrium - which means we wouldn't exist, contradiction.[/QUOTE]
Irrespective of physics, this chain of reasoning is logically totally wrong.
Namely, if A is some evidence for B, it does not mean that A implies B.
For example, being in grave is an evidence for being dead, but you can still be in grave without being dead.[/QUOTE]
This means that you have very weak standards for what you regard as evidence for global thermal equilibrium and for quantum equilibrium. Your arguments deon't hold any water, as my example of the hill-climber showed.
Demystifier said:
Anyway, perhaps we are a statistical fluctuation?
No serious statistician rregards anything as a fluctuation that persists for so long.
 
  • #76
Demystifier said:
I'm not sure what kind of an answer do you expect here. Perhaps the straightest answer is: through the Schrodinger (or Schrodinger-Pauli, or Dirac, or Maxwell ...) equation and the associated equation for the particle trajectories - of the isolated system.

In standard QM, a spin system is given by N spins, basis states that tell which subset of spins is up (the complementary subset is down), their linear compinations as general statres, and a Hamiltonian that is an expression in the su(2) operators J^k_0, J^k_+ and J^k_-, one k for each spin. This determines the quantum dynamics via Schroedinger's equation i hbar psi(t)=H psi(t).

But it doesn't determine the Bohmian dynamics if there is no detector close by to give ontological meaning to the system.
 
  • #77
camboy said:
So, as you haven't corrected yourself at all, do I take it you don't accept that anything that you have said is wrong?
Indeed. I believe that my position regarding my paper is correct. Your arguments didn't convince me of a mistake.
camboy said:
If this is not the case, would you mind listing for me the things about which you have changed your opinion as a result of this thread?
For example, I had thought that Bohmian mechanics never considered quantum computing, and I learned that it had. Though the presentation given was not enough to convinve me that BM accounts for qunatum computing - see the still pending dialogue.
camboy said:
As far as deBB is concerned, you appear to be entirely ignorant of everything that has been published since the 1990s,
It may appear s to you,, but it isn't the case.
camboy said:
You have made multiple statements on this thread which are demonstrably incorrect.
more precisely, which seem incorrect to you. I didn't buy your arguments.
In questions of interpretation, there is a lot of room for differing opinions on the same statement.
camboy said:
When told they are incorrect and you apparently have no further argument, you simply move onto another point without saying whether you agree with the correction or not.
The point of a conversation on PF is not to be proved right or wrong but to provide information for readers so that they can make up their own mind. I write to contribute further information, not to justify myself.
camboy said:
Anyone reading this thread and attempting to make sense of it needs to have that information if they are to draw a conclusion about who is right and who is wrong.
They shouldn't take anything on authority if there are conflicting opinions. They should study the arguments of both sides and form their own picture.
camboy said:
looking at http://arnold-neumaier.at/im/hs97_16.gif" , you can hardly blame me for my assumption. So you're a professor of mathematics who has the foundations of quantum mechanics as one of his main research interests.
If you look at my list of research interests http://arnold-neumaier.at/#research , you'll find that quantum mechnaics is a minor part of my research interests. About 4% of my piblications are about quantum mechanics.
camboy said:
My original point therefore stands that - as a respectable professor at a major university - you have a responsibility not to make sweeping incorrect statements damning entire fields in public forums, since people will believe you merely because of who you are.
I don't make sweeping incorrect statements damning entire fields. Saying that Bohmian mechnaics contradicts quantum mechnaics doesn't damn the field. Classical mechnaics also contradicts QM, but nobody thinks that this implies that whoever does rersearch in classical mechanics is an idiot. Far from this!
camboy said:
Then what on Earth did you mean by statements such as "The worst thing about Bohmian mechanics is their low standards of quality", "Bohmians are not aware of many things", "Bohmian trickery is inapplicable" and all the rest. Are these supposed to be compliments?
The first means, for example, that they take things such as the establishment of quantum equilibrium for the universe to be proven although they have extremely little ''evidence'' for it. The second is a truism that holds for everyone, and must be read in context. The third is a statement asserttin that the machinery of Bohmian mechanics is not applicable. Calling it trickery is clearly a subjective statement implying that BM gives an appearance of reality to QM of the same kind as a juggler makes things appear real without being so. This is a nonrefutable statement since BM say often that the motion of the quantum particles is not observable. Thus considering it as trickery is legitimate.
 
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  • #78
akhmeteli said:
First, you may have noticed an emoticon by my "claim", second, strictly speaking, depending on peer reviews, truth either belongs here or not (so it is indeed "dependent" in this respect on peer reviews). With all due respect, your "truth" of post 7 does not belong here.
If you think giving a reference to an unpublished arXiv paper without discussing it is a serious sin against the rules, you should report it to the PF management, quoting the present post for context.
akhmeteli said:
I am sure mentors here value your input, as I do, and would give you some slack, as I would do, if I were in their shoes, but you should not abuse our respect.
I fully respect the rules as I understand them.
akhmeteli said:
And again, if indeed the Bohm interpretation is a lost cause, so be it, but I specifically objected to your claim
But I cannot discuss my claim further because of the PF rules. So your objection standas like my assertion, and readers must make up their own mind.
akhmeteli said:
I asked about the status of your claim "no quantum computing in the Bohm interpretation." This is another strong claim, and I just tried to understand if that was common knowledge or just another personal theory of yours.
First, I qualified my statement with ''probably'' since I wasn't sure, and indeed, there was a very recent (2010) thesis that tackled it, as was pointed out by others. I immediately acknowledged the article, studied it, and found that it didn't treat spin systems by themselves but only spin systems coupled to an external pointer variable, thus justifying my remark ''The observables used there do not include a position variable, hence the Bohmian trickery is inapplicable.''. However, I learned that the author invented (or got from somewhere else) a new Bohmian trick - namely that one silently changes the system under study to a bigger one, in order to give it the appearance of fitting into the BM philosophy. This lead to a still ongoing discussion.
akhmeteli said:
if there is no peer-reviewed article supporting your claim, then your claim does not belong here.
If everyone were banned who made more than 10 claims that do not appear in a peer-reviewed article, PF would be nearly empty.
 
  • #79
A. Neumaier said:
But in the Bohmian interpretationl, one interprets only changes in the pointer varibles as observables.
No, that's not true. I never said that.
 
  • #80
A. Neumaier said:
In standard QM, a spin system is given by N spins, basis states that tell which subset of spins is up (the complementary subset is down), their linear compinations as general statres, and a Hamiltonian that is an expression in the su(2) operators J^k_0, J^k_+ and J^k_-, one k for each spin. This determines the quantum dynamics via Schroedinger's equation i hbar psi(t)=H psi(t).
That's correct.

A. Neumaier said:
But it doesn't determine the Bohmian dynamics if there is no detector close by to give ontological meaning to the system.
You are wrong. Bohmian dynamics is well defined and gives an ontology even without detectors. But in that case, the statistical predictions may differ from those of ordinary QM. Yet, there is no conflict with experiments because these deviations from ordinary QM cannot be detected (because there are no detectors).

What is true in that case is that there is no any meaningful SPIN ontology. Still, there is some ontology in terms of a wave function and particle positions.

Let me repeat the analogy with classical optics. Colors do not exist, except for the observers. Yet, light waves exist irrespective of the observers.
Similarly, in BM spins do not exist, except for the observers. Yet, wave functions and particle positions exist irrespective of the observers.
 
  • #81
A. Neumaier said:
BM say often that the motion of the quantum particles is not observable.
That is an incorrect interpretation of BM. Just the opposite, the motion of the quantum particle is the only observable thing in BM. However, in order to observe it in practice, one must couple it with a macroscopic apparatus containing a large number of the degrees of freedom. Such a large number of degrees of freedom cannot be controlled on a fine level, which means that one cannot know the exact position-dependent phases of the wave functions involved. Without knowing the phases, one cannot predict the exact particle trajectories either. Therefore, one cannot experimentally confirm (or refute) that the measured trajectories coincide with those predicted by the theory.
 
  • #82
Demystifier said:
No, that's not true. I never said that.
You just repeated it:
Demystifier said:
the motion of the quantum particle is the only observable thing in BM.
 
  • #83
Demystifier said:
Bohmian dynamics is well defined and gives an ontology even without detectors. But in that case, the statistical predictions may differ from those of ordinary QM. Yet, there is no conflict with experiments because these deviations from ordinary QM cannot be detected (because there are no detectors).
Then please give me the dynamics of the unobserved spin system that I described in terms of standard QM in terms of BM.
 
  • #84
Demystifier said:
That is an incorrect interpretation of BM. Just the opposite, the motion of the quantum particle is the only observable thing in BM. However, in order to observe it in practice, one must couple it with a macroscopic apparatus containing a large number of the degrees of freedom. Such a large number of degrees of freedom cannot be controlled on a fine level, which means that one cannot know the exact position-dependent phases of the wave functions involved. Without knowing the phases, one cannot predict the exact particle trajectories either. Therefore, one cannot experimentally confirm (or refute) that the measured trajectories coincide with those predicted by the theory.

But this means (by any meaningful interpretation of the term ''observe'') that one cannot observe the particle position but only the pointer position of the macroscopic apparatus.
 
  • #85
A. Neumaier said:
But this means (by any meaningful interpretation of the term ''observe'') that one cannot observe the particle position but only the pointer position of the macroscopic apparatus.
Yes, but this macroscopic apparatus also consists of particles. So one does measure the particle positions, but of the apparatus. Not because the apparatus is fundamentally different, but simply because it is bigger.
 
  • #86
A. Neumaier said:
Then please give me the dynamics of the unobserved spin system that I described in terms of standard QM in terms of BM.
That's simple. Standard QM describes it in terms of a wave function for n particles. BM takes the same wave function and says additionally that there are n particles the velocities of which are calculated from this wave function (the exact equation is not important here).
 
  • #87
Demystifier said:
Yes, but this macroscopic apparatus also consists of particles. So one does measure the particle positions, but of the apparatus. Not because the apparatus is fundamentally different, but simply because it is bigger.

One measures a single mean position of the pointer, not the positions of any of the pointer particles.

But this brings me back to my question about the nerves: Where in the nerves is the measured particle whose position indicates whether or not I see a star, and which color it has?
 
  • #88
"No, that's not true. I never said that."

"the motion of the quantum particle is the only observable thing in BM."

OK, I admit, I was not sufficiently precise in the last sentence in quotation marks. By "motion" I meant "particle position as a function of time". Clearly, a particle at rest also has a position as a function of time. OK?
 
  • #89
Demystifier said:
That's simple. Standard QM describes it in terms of a wave function for n particles. BM takes the same wave function and says additionally that there are n particles the velocities of which are calculated from this wave function (the exact equation is not important here).

But in the standard QM picture, the wave function of a spin system (e.g. the Ising ferromagnet) has no position or momentum variables, and hence also no velocities associated with it. Given my specific description of the spin system, what is the BM dynamics? Please be as specific in your formal description, rather than using vague words that leave many things unsaid.
 
  • #90
Demystifier said:
"No, that's not true. I never said that."

"the motion of the quantum particle is the only observable thing in BM."

OK, I admit, I was not sufficiently precise in the last sentence in quotation marks. By "motion" I meant "particle position as a function of time". Clearly, a particle at rest also has a position as a function of time. OK?
OK. But measuring the particle at rest always gives the same measurement result. Thus the positions of the nonmoving nerves in the eye can hardly be used to tell the difference between seeing and not seeing a star.
 

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