Bohmian Interpretation: Equivalent or not to Standard QM

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  • #1
JustinLevy
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(My previous thread on Bohm Interpretation quickly became 4 pages of mostly unrelated discussion. So I'm restarting here with more precise questions.)

Okay, I've read some references on the Bohm Interpretation and I am still confused. As one paper mentioned, some extensions have stochastic elements, so the main purpose of these lines of interpretation seem to be to remove the "classical measurement" from the standard interpretation. Yet even that aspect seems unclear to me.


The fact that it hasn't been soundly refuted in 50 years suggests that I am still misunderstanding it. Continuing with that assumption, please, help me understand why it hasn't been refuted. For currently, the theories do not appear equivalent to me. I will try to be as clear as possible with my questions, so please try to be as clear as possible with your answers. In particular, please clearly define any terms you use that I appear to be misunderstanding, as I am probably unaware that I am misunderstanding them.


Question 1:
All measurements are supposed to boil down to a measurement of position in the Bohmian interpretation. What IS a position measurement in the Bohmian interpretation?

discussion:
comment A - In BM, the configuration and evolution of a system is specified in totality by the wavefunction, Hamiltonian, and particle positions.

comment B - In BM, the wavefunction is not a function of the particle position, but the possible particle positions (the position configuration space). Given N particles in D dimensions, the wavefunction maps points in the space Reals^(ND) to a complex number. The actual positions of the particles evolves according to a functional of the wavefunction. Note: the particle position evolution depends on the wavefunction but not the other way around.

comment C - Since the wavefunction evolution does not depend on the particle positions, the portion of the wavefunction corresponding to the measurement device cannot depend on the particle positions.

comment D - this leaves us in the same situation as standard quantum mechanics. A measurement just entangles you with what you are measuring. Nothing explains how you get a discrete answer instead of a superposition ... since the result up to this point should be a superposition. The very thing BM was supposed to supply, it appears to fail to accomplish. You need to rely on decoherence, or many minds, etc. other interpretations to get anything out despite adding additional information in.


Question 2:
The particle position is updated according to only the phase of the wavefunction, so BM uses a different definition of momentum than the standard quantum mechanics. This appears to make BM quantifiably falsifiable (ie. it is a different theory, not a different interpretation of the underlying math). What IS a momentum or momentum^2 measurement in the Bohmian interpretation?

discussion:
comment E - Since the ground state wavefunction of a bound system can often (always?) be written as a real valued function * exp(-i E hbar / t), the velocity of any particle in the system is exactly zero. The average velocity squared of a particle is therefore zero.

comment F - This alone appears to refute the BM theory. But also consider momentum conservation. Since the two theories differ, it is unclear to me how momentum can possibly be conserved in BM (especially when considering collisions of particles that can result in bound states).

comment G - Similarly, it is unclear how energy is conserved with this change in p^2 (proportional to kinetic energy). Regardless on whether they use the correct definition of KE, it is also unclear to me on general grounds if a conserved energy can be defined at all. While possibly a solved question, I'm unclear on whether the hamiltonian can be converted to a lagrangian which can be used with Noether's theorem if the number of variables are infinite (fields) AND the configuration has non-local interactions.


Question 3:
In standard quantum mechanics, spin is an internal degree of freedom of a particle. In BM, this degree of freedom is included in the wavefunction by borrowing from derivations in standard quantum mechanics. BM however does not give it a definitive value like it does position. Notice however, that since the wavefunction has two components for each spin (1/2) particle now, to consider evolution of the position, we MUST consider the position to have two components as well (which need not evolve similarly, so even the "real" particle positions are superpositions now!). And you cannot consider these as two individual particles, since they are not conserved (only by considering them together is particle number conserved). So in BM, while <Sx,Sy,Sz> can have any value, a system really truely does not have a known spin direction which seems contrary to a hidden variable theory and also which is distinct to orbital angular momentum due to real trajectories of particles. So what IS angular momentum and spin in the Bohmian interpretation?

discussion:
comment H - Since momentum is defined differently, again we have the same issue as before that it is unclear how angular momentum is conserved. However it now has the additional hurdle due to the true "unknowingness" of spin while the orbital trajectory is definite.

comment I - Because the L=1,m=0 state of the hydrogen atom can be written as a real valued wavefunction, again we have the issue that the particles are stationary. But now, the particles are stationary even though there is orbital angular momentum. So not only does it seem to contradict experiment, but it seems internally inconsistent.

comment J - A change in basis can change the wavefunction from real valued to complex (consider using the Lz basis, or the Lx basis). So the evolution of the position states seems to depend on the choice of basis. BM can't even seem to say definitively whether their hidden particles are moving or not.

comment K - Every derivation I've seen of the spin statistics theorem relied on locality. Is there a way to get this in Bohmian mechanics as well, or does it just borrow this verbatum from standard QM as well.



Any help in answering (please, not speculating, nor hand-waving, as the theory seems vague enough to me currently as it is) these questions would be greatly appreciated.
 
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  • #2
Demystifier
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JustinLevy, since you ask too many questions, most of them being answered elsewhere, I have a deal for you. I will give you a paper where many of these questions are answered in a concise but pedagogic way. You will read it (only a few pages) carefully, and then you will tell me what is still unclear to you. After that, I will answer your remaining questions.
Deal?
 
  • #3
JustinLevy
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Of course that is a deal, as that sounds perfect!
 
  • #4
Demystifier
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OK, all you have to read for a start is the Appendix of
http://xxx.lanl.gov/abs/quant-ph/0208185
It is only two pages long, but read it carefully. Pay particular attention to the fact that it is a GENERAL theory of measurement, so it explains how measurement of ANY quantity is explained by BM in a manner consistent with the predictions of standard QM, including position, energy, momentum, angular momentum, spin, whatever.
 
  • #5
JustinLevy
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That does not appear to answer my questions at all. To give extra benefit of the doubt, I read it again, thought about it that night, took a sleep on it, thought about it some more, and read it again today. It doesn't seem to answer any questions... to me it just rephrases stuff as if it is an answer.

Let me try to explain as succintly as possible. You say in your paper:
The dBB theory of particle motion is based on the postulate that the velocity v of the particle is given by [itex] v = \frac{1}{m} \partial_x S(x,t)[/itex](eq 38), where S(x, t) is the phase of the wave function. This postulate provides that the statistical distribution of particle positions is given by [itex]\left| \psi (x, t) \right|^2[/tex] for any time t, provided that this distribution is given by [itex]\left| \psi (x, t_0) \right|^2[/tex] for some initial time t0.

Thus, if there is such an initial distribution, then if you describe the entire system (measuring device and thing you are measuring) quantum mechanically you can never make a measurement of the position as the system will remain distributed as such. If the initial distribution is not as such, then Bohmian mechanics is not compatible with quantum mechanics. Either way, there is a problem.

When trying to explain measurement, invariably all the Bohmian interpretation sources I've read refer to the measurement of something classical. Essentially, they say: To measure a particle position couple it with a 'macroscopic' system and measure the position of the 'macroscopic' system. All you are doing is transferring the problem! You never actually answered how to measure anything.
 
  • #6
Demystifier
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JustinLevy, I must admit that it is not clear to me what exactly is not clear to you.
But you could help me if you could explain what is YOUR favoured interpretation of QM.
In particular, what do you think about the von Neumann measurement scheme and what do you think about decoherence.
 
  • #7
JustinLevy
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I prefer a mathematical model with local evolution and non-unitary "imposed" measurements, essentially the standard, as many call it here, "shut up and calculate" 'interpretation'. Basically, if there is something we don't quite understand yet (foundational issues) to me it seems more appropriate to limit the theory's range of applicability until we learn more experimentally, instead of ad-hoc removing symmetries that we see experimentally. If really pressed, I choose the "many worlds" interpretation since it maintains all previous features, and just essentially says "measurement" is our state entangling with the world ... it seems closest to what taking quantum mechanics 'literally' would result in.

However, it is useful to be aware of such discussion on foundational issues. If the standard truly was "shut up an calculate" we wouldn't discuss and marvel at Bell's inequalities. So I want to understand what is and isn't possible as far as interpretation. In this case, I really truly do not understand how Bohmian mechanics provides the same predictions in all situations. So there must be a flaw in my understanding of these foundational issues, and it can't hurt to be a little more well rounded in the subject.

JustinLevy, I must admit that it is not clear to me what exactly is not clear to you.
What is not clear? I want to know how measurement works in your theory. Your answer boils down to we make a measurement by having a particle affect something else which we then measure. See the problem there? Your answer is circular.

Furthermore, your theory doesn't seem to even allow any measurement. Let's say we somehow knew the wavefunction and Hamiltonian of an entire experiment (in principle, this is possible in standard quantum mechanics). Can the experiment, in principle, determine the bohmian position of a particle? Because you say the wavefunction is always the statistical distribution of the particle position, the answer seems to have to be NO.

----

If you are having trouble understanding my confusion, let's focus on an example. Let's work with non-relativistic quantum mechanics. Consider the Stern-Gerlach experiment: a wavefunction of an electron and a measuring device start out separable. The electron starts as a small wave-packet with the particle having spin Sz=+1/2. Now it goes through a region of a magnetic field gradient in the y direction, which splits the wave-packet into two wave-packets. The electron now slams into a CCD imager. The wavefunction of the system is no longer separable. So, what do we measure? Let's say we knew the bohmian particle position ahead of time, can you show the math that explains how only one result comes out? I'm not sure how you'd even due this in Bohmian mechanics since the electron wavefunction has two components which seems to require the electron position to have two components ... so since Sz and Sy do not commute, it seems to me you still get a superposition of the position in Bohmian mechanics (and not just statistically, but an actual superposition of the Bohmian positions themselves).

Working out that example would be very helpful.
 
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  • #8
Demystifier
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What is not clear? I want to know how measurement works in your theory. Your answer boils down to we make a measurement by having a particle affect something else which we then measure. See the problem there? Your answer is circular.
I think I understand now what you are saying.
The answer is the following. According to BM, everything consists of particles, just as in classical mechanics. In a measurement, particles affect other particles. The result of a measurement may be a position of a needle of the measuring apparatus, and this needle also consists of many particles. The role of wave function is analogous to a potential in classical mechanics, i.e., it plays a secondary role, because it only tells particles how to move for given initial conditions. Do you still find it circular?

Can the experiment, in principle, determine the bohmian position of a particle? Because you say the wavefunction is always the statistical distribution of the particle position, the answer seems to have to be NO.
See again the Appendix that I suggested to you. What you actually observe is the position of needle (or some other macroscopic configuration of particles of the measuring apparatus), represented by y. If the value of y turns out to be in the support of chi_a, then the measured particle behaves as if it was described only by psi_a. Furthermore, if your measurement procedure is aimed to be a measurement of the position of x, then psi_a is a localized wave function, in which case you know with certainty that the particle is localized within psi_a.
Is it clearer now?

If you are having trouble understanding my confusion, let's focus on an example. Let's work with non-relativistic quantum mechanics. Consider the Stern-Gerlach experiment: a wavefunction of an electron and a measuring device start out separable. The electron starts as a small wave-packet with the particle having spin Sz=+1/2. Now it goes through a region of a magnetic field gradient in the y direction, which splits the wave-packet into two wave-packets. The electron now slams into a CCD imager. The wavefunction of the system is no longer separable. So, what do we measure?
We measure y. But y is strongly correlated with x due to (42). Therefore, we can say that we indirectly measure x as well.

Let's say we knew the bohmian particle position ahead of time, can you show the math that explains how only one result comes out?
Of course. y(t) is a single-valued function, so only one result can come out.

I'm not sure how you'd even due this in Bohmian mechanics since the electron wavefunction has two components which seems to require the electron position to have two components ...
No, the electron position x(t) is a single-valued function as well, even though the wave function has two components.

See also Ref. [2] which also contains a good pedagogic explanation of the theory of quantum measurements.
 
  • #9
JustinLevy
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I think I understand now what you are saying.
The answer is the following. According to BM, everything consists of particles, just as in classical mechanics. In a measurement, particles affect other particles. The result of a measurement may be a position of a needle of the measuring apparatus, and this needle also consists of many particles. The role of wave function is analogous to a potential in classical mechanics, i.e., it plays a secondary role, because it only tells particles how to move for given initial conditions. Do you still find it circular?
No, the wavefunction is more than that. Because here you are also requiring the wavefunction to always give you the particle distributions. This is quite unlike a potential.

If the evolution makes the wavefunction of the needle become a superposition of two outcomes, but you see the needle in only one position, then you have violated the postulate I quoted from your paper.

See again the Appendix that I suggested to you. What you actually observe is the position of needle (or some other macroscopic configuration of particles of the measuring apparatus), represented by y. If the value of y turns out to be in the support of chi_a, then the measured particle behaves as if it was described only by psi_a. Furthermore, if your measurement procedure is aimed to be a measurement of the position of x, then psi_a is a localized wave function, in which case you know with certainty that the particle is localized within psi_a.
Is it clearer now?
No that is not clearer. You are presenting a dichotomy between the microscopic and macroscopic and saying essentially that we can obviously measure something macroscopic, so by entangling with something microscopic, that let's us measure the microscopic. But your theory claims to not make such a dichotomy and so it is not obvious how we measure anything let alone something macroscopic.

Furthermore, the wavefunction evolution doesn't depend on the bohmian particle positions. Therefore, for the wavefunction to collapse to a localised one due to the experiment, cannot depend on the bohmian particle positions, and thus can in no way be considered a "measurement" of the bohmian particle position.

We measure y. But y is strongly correlated with x due to (42). Therefore, we can say that we indirectly measure x as well.
Arrgh. I'm trying to figure out how to make a measurement in your theory. Your answer: "We measure y."
This is just transfering the measurement problem to a different entity.

The wavefunction will be in a super-position of two outcomes. If you actually measured y, then by your own explanations, the wavefunction should only be of that one value.


JustinLevy said:
Let's say we knew the bohmian particle position ahead of time, can you show the math that explains how only one result comes out?
Of course. y(t) is a single-valued function, so only one result can come out.
Then can you please show the math for that example. Seeing some actual math for an example could be very helpful. Math can speak clearer than prose.

No, the electron position x(t) is a single-valued function as well, even though the wave function has two components.
That makes no sense. If the wavefunction has two components, then so does the magnitude and phase of the wavefunction. It is possible to apply your equations and get something like
[tex] v(t) = \frac{1}{m}\partial_x S(x,t) = \frac{1}{m} \frac{1}{\sqrt{2}}
\left( \begin{array}{c}
1 \\
-1 \end{array} \right)
[/tex]
The velocity is not single valued. How can you claim the position is?
 
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  • #10
Demystifier
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No, the wavefunction is more than that. Because here you are also requiring the wavefunction to always give you the particle distributions. This is quite unlike a potential.
It is true that the wave function plays this additional role, but this role can in fact be DERIVED from the first one, as a property that is valid in the equilibrium. (I will not present here this derivation, but I will give you the references if you wish.)

If the evolution makes the wavefunction of the needle become a superposition of two outcomes, but you see the needle in only one position, then you have violated the postulate I quoted from your paper.
You mean
"This postulate provides that the statistical distribution of particle positions is given by |psi (x, t)|^2 for any time t, provided that this distribution is given by |psi (x, t_0) |^2 for some initial time t0."?
You misunderstood that. The particle allways has only one position, but the distribution says what is the probability of a particular position. Of course, this is an a priori probability, which makes sense only before you determine this position.

No that is not clearer. You are presenting a dichotomy between the microscopic and macroscopic and saying essentially that we can obviously measure something macroscopic, so by entangling with something microscopic, that let's us measure the microscopic. But your theory claims to not make such a dichotomy and so it is not obvious how we measure anything let alone something macroscopic.
Well, in BM it is considered obvious that you can observe macroscopic things, simply because you are macroscopic as well. If you have problems with this, then you probably even have problems with measurements in classical physics. Do you? Anyway, I do not find any dichotomy with this, or at least not more than in classical physics.

Furthermore, the wavefunction evolution doesn't depend on the bohmian particle positions. Therefore, for the wavefunction to collapse to a localised one due to the experiment, cannot depend on the bohmian particle positions, and thus can in no way be considered a "measurement" of the bohmian particle position.
The total wave function does not depend on particle positions. Yet, the conditional wave function, i.e., the wave function that describes your updated knowledge after you measured some particle positions, does depend on these positions.

The wavefunction will be in a super-position of two outcomes. If you actually measured y, then by your own explanations, the wavefunction should only be of that one value.
Again, you should distinguish the total wave function form the conditional (effective) wave function.

If the wavefunction has two components, then so does the magnitude and phase of the wavefunction. I can apply your equations and get something like
[tex] v(t) = \frac{1}{m}\partial_x S(x,t) = \frac{1}{m} \frac{1}{\sqrt{2}}
\left( \begin{array}{c}
1 \\
-1 \end{array} \right)
[/tex]
The velocity is not single valued. How can you claim the position is?
Eq. (38) is valid without spin. With spin, (38) is slightly modified, such that velocity is single valued. If you want the exact equation in the case of spin, I can write this as well for you.

Do we make any progress?
 
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  • #11
JustinLevy
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You mean
"This postulate provides that the statistical distribution of particle positions is given by |psi (x, t)|^2 for any time t, provided that this distribution is given by |psi (x, t_0) |^2 for some initial time t0."?
You misunderstood that. The particle allways has only one position, but the distribution says what is the probability of a particular position. Of course, this is an a priori probability, which makes sense only before you determine this position.
If the wavefunction initially gives the probability distribution, then it always does according to your theory. Therefore the total wavefunction (not some "conditional" wavefunction that you are introducing below) must represent the probability distribution at all times. If you have measured the position, and the total wavefunction does not collapse, you have violated one of your postulates.

If at any point the total wavefunction no longer holds to the "equilibrium hypothesis", then your theory differs in predictions from standard quantum mechanics.

Well, in BM it is considered obvious that you can observe macroscopic things, simply because you are macroscopic as well. If you have problems with this, then you probably even have problems with measurements in classical physics. Do you? Anyway, I do not find any dichotomy with this, or at least not more than in classical physics.
How can you possibly not consider that a dichotomy!?
Please, please, reread what you just wrote.
You are treating macroscopic objects differently from microscopic objects, despite claiming your theory doesn't.

Following Schrodinger's equation the wavefunction for your classical object will evolve a superposition of answers. What collapses the wavefunction to only one result? Based on your "conditional wavefunction" comments you seem to be devolving into a 'consistent histories'/'many worlds' interpretation.

The total wave function does not depend on particle positions.
Good, we have at least one definitive thing to start building a common ground from.

Yet, the conditional wave function, i.e., the wave function that describes your updated knowledge after you measured some particle positions, does depend on these positions.
But the evolution only depends on the total wavefunction, correct?
Your equilibrium hypothesis only stays true if you consider the total wavefunction. If you now consider the probability to be expressed by the conditional wave function, then you have lost some probability (you have done a projection on the states, the very thing you seem to dislike that copenhagen does).

Eq. (38) is valid without spin. With spin, (38) is slightly modified, such that velocity is single valued. If you want the exact equation in the case of spin, I can write this as well for you.
Yes, I would like to see that.
Again, a simple example presented with math would speak volumes here. Can you please work out the Stern-Gerlach experiment?
 
  • #12
Demystifier
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If the wavefunction initially gives the probability distribution, then it always does according to your theory. Therefore the total wavefunction (not some "conditional" wavefunction that you are introducing below) must represent the probability distribution at all times. If you have measured the position, and the total wavefunction does not collapse, you have violated one of your postulates.
Come on, you should first learn some basics of probability theory. It is pointless to discuss foundations of QM if, for example, you do not understand the concept of conditional probability. After that, you should learn some basics of classical statistical physics as well. Only then we can discuss foundations of QM.

I have no intention to teach you these non-quantum stuff, as I am sure that there are many people here that can do that as well.
 
  • #13
akhmeteli
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OK, all you have to read for a start is the Appendix of
http://xxx.lanl.gov/abs/quant-ph/0208185
It is only two pages long, but read it carefully. Pay particular attention to the fact that it is a GENERAL theory of measurement, so it explains how measurement of ANY quantity is explained by BM in a manner consistent with the predictions of standard QM, including position, energy, momentum, angular momentum, spin, whatever.

Demystifier, I am afraid I am not sure how to answer the following question, so I wonder if you could explain:

What is the status of the projection postulate in dBB? Is it an approximation, or does it hold precisely, or maybe it does not hold at all?

There is the following phrase in the Appendix that you cited (and there are similar phrases in other texts on dBB measurement theory):

"To see how this problem resolves, it is essential to realize
that, when the system consisting of the variables $x$ and $y$ can be considered as a configuration suitable for measurement of the $x$ subsystem, the total wave function is {\em not} of the form $\psi(x,t)\chi(y,t)$. Instead, the interaction between the $x$ subsystem and the $y$ subsystem should be such that the total wave function takes the form
[tex]
\begin{equation}\label{app4}
\Psi(x,y,t)=\sum_a c_a(t)\psi_a(x)\chi_a(y),
\end{equation}
[/tex]
where the normalized wave functions $\chi_a(y)$ with different labels $a$ do not overlap in the $y$ space."

However, if some wave functions do not overlap at some time point, they'll overlap later, as wave functions disperse in space with time. Of course, you can say that the measurement device is macroscopic, so its wave function does not disperse, to all practical intents and purposes. However, strictly speaking, this is not a precise statement, but an approximation, so my conclusion is that the projection postulate is an approximation as well. Is this correct or not?
 
  • #14
JustinLevy
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I do not appreciate you trying to sweep this away as me not understanding basic math.
I understand basic math just fine thank you. I have taken plenty of physics classes, taught physics classes, and have physics degrees.

I am trying very hard to understand what you mean here, and instead you just keep giving circular answers or resorting to what appears to be a micro/macro dichotomy or many worlds on a whim. I understand that you feel you are describing your theory clearly, but it is coming off very vague. I am not asking these questions in a vacuum either ... I am trying to read up on it, but it appears there are physicists who believe BM is just many-worlds with additional hidden structure, which (to me) your views on measurement seem to support. So I am not alone in thinking these things. But I am trying, and asking earnest questions.


So let's please try this again.

So far we have agreed on:
A] The total wave function does not depend on particle positions.

Do you agree:
1] If at any time the total wavefunction no longer holds to the "equilibrium hypothesis", then your theory differs in predictions from standard quantum mechanics.

2] If you gain some information about the particle, so that you can neglect some of the total wavefunction and consider only the 'conditional wavefunction' then the total wavefunction no longer holds to the "equilibrium hypothesis".

3] The evolution of the particle positions depends on the total wavefunction, not the 'conditional wavefunction'.

Questions (hopefully just yes/no questions):
4] My understanding of your answer to "how do you make a measurement" was that you feel that regardless of whether the wavefunction of a macroscopic object evolves to contain a superposition of answers, the position of the object can be observed directly because it is "obvious" what the positions of "macroscopic things" are. Is this understanding correct?

5] Previously I asked if in a closed system in which the hamiltonian and initial wavefunction was known, if additional information as a bohmian particle position could be determined. My understanding is that your answer is yes. Is this understanding correct?

6] Consider an external observer also knew the hamiltonian and initial wavefunction of this box, and calculated the probabilities of some results when he looks in later. Would the experimenter in the box, using his additional knowledge of the system, be able to predict the final measurements to better accuracy than the experimenter outside the box?



I'm still interested in seeing the details of the evolution of an non-relativistic electron with a spin in an external magnetic field if you can provide a reference. Trying to find info, I found a paper claiming that there is experimental difference between the theories http://arxiv.org/PS_cache/arxiv/pdf/0903/0903.3878v1.pdf
 
  • #15
conway
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Justin, the last thing I want to do is derail your attempted engagement with Demystifier. It's obvious to me you're putting quite a lot of effort into trying to communicate here and I know how frustrating these discussions can be. I also somewhat share your frustration with what seems to be his glib answer as to what constitutes a measurement in the Stern-Gerlach experiment. So I don't really want to interfere in the discussion...BUT: I'm going to ask the question:

Is Bohmian Mechanics simply the identification of two real-valued functions, a position density and a velocity density, as derived from the ordinary wave function? And as such is the bottom line for any Bohmian calculation simply the idea that you transform back to the Schroedinger function, do the time evolution, and then re-convert back to the Bohmian position and velocities? If this is all there is to it, what insight can it possibly give to the problem of the collapse of the wave function?

Sorry if this if way off topic.
 
  • #16
zenith8
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My previous thread on Bohm Interpretation quickly became 4 pages of mostly unrelated discussion. So I'm restarting here..

Look guys, can we not just give Demystifier a break here? He is genuinely trying to help and all your stuff about 'glib answers' and 'your theory' seems to me unnecessarily rude. Your (far too many) questions are all based on standard misunderstandings - they are not some deal-killing problems with an 80 year-old theory which you are the first to notice. Why don't you just read the standard references that you were actually given in the previous thread which you claim is 'mostly unrelated', instead of effectively asking him to copy them out for you?

In particular, the http://www.tcm.phy.cam.ac.uk/~mdt26/pilot_waves.html" [Broken] was suggested (the Lecture 4 on measurement theory answers most of your current questions).

Dr. Chinese also suggested:

Passon (2006): What you always wanted to know about BM but were afraid to ask...

Nikolic (2006): QM: Myths and facts

Passon (2004): Why isn't every physicist a Bohmian?

to which one might add

Tumulka (2007) Understanding Bohmian mechanics

(see Cambridge course 'Further reading' section for the links to these).

Reading the above it seems to me you cannot continue to imply that the theory is incompatible with standard QM.

Just to state the answer to the question implied in your thread title, the Bohm interpretation/pilot-wave theory is certainly equivalent to standard QM. How could it be otherwise? As stated in the previous thread, the entire thing flows from standard QM by assuming the psi squared means the probability of the N particles being in those positions, rather than the probability of being found there in a suitable measurement. This assumption - hardly very revolutionary when you think about it - implies that the particles continue to exist between measurements.

In a stationary state, the probability distribution doesn't move. So the now continuously-existing particles must either be actually stationary or moving in some constant repeating pattern (distributed as psi squared over an ensemble). In a non-stationary state, the probability distribution changes in time, so the particles must move - the 'guidance equation' follows from the expression of the probability current of the moving distribution which is already in standard QM (it is often mistakenly presented as some extra maths grafted onto standard QM, which may account for your confusion).

It is the same mathematical theory, so it must make the same predictions. And for free, you get mathematical derivations of the Born postulate, the classical limit, measurement theory (with no collapse, splitting universes, observer-induced magic, or other weird stuff) etc. etc. It is a mathematical formulation of QM equivalent in status to (say) Feynman's path-integral formulation (rather than just an interpretation) because one can use it to do predictive calculations (e.g. calculate the propagator by integrating the quantum Lagrangian along the one actual path followed by the particle, rather than the classical Lagrangian along the infinite number of all possible paths as in Feynman).

A final interesting point is that while it is equivalent to standard QM, it is actually of wider scope in that it also describes the 'non-equilibrium' case where the particles are not distributed as the square of the wave function. In this respect one finds (theoretically or through numerical simulation) that particles with any initial distribution which are 'stirred' by the 'pilot-wave' psi in the way suggested become distributed as psi squared in the course of time, and once so distributed, remain so. It can be shown that psi squared is the only distribution with this property.

This is interesting since it seems to imply possible experimental tests of pilot-wave theory (admittedly in fairly extreme conditions such as the beginning of the universe/black holes etc..). See relevant work by Valentini, and the second half of Cambridge Lecture 5.
 
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  • #17
Ilja
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Question 1:
All measurements are supposed to boil down to a measurement of position in the Bohmian interpretation. What IS a position measurement in the Bohmian interpretation?

In the paper I'm currently writing I question this claim. My position is that measurements have to be (and are, in the standard equivalence proof) reduced to actual states of the beables (positions), but not to their measurements.

comment C - Since the wavefunction evolution does not depend on the particle positions, the portion of the wavefunction corresponding to the measurement device cannot depend on the particle positions.

comment D - this leaves us in the same situation as standard quantum mechanics. A measurement just entangles you with what you are measuring. Nothing explains how you get a discrete answer instead of a superposition ... since the result up to this point should be a superposition.

No. You have the actual values of the configuration. They allow to reduce the wave function of the universe to an effective wave function of the part we consider.

The definition is almost tautological

[tex]\psi(q_S) = \Psi(q_S, q_{env})[/tex]

We do not have to measure the [tex]q_{env}[/tex], but have to use their actual values. Else, the explanation would be circular: A measurement explained by measurement results.

In some sense, you need some elements of decoherence to prove that [tex]\psi(q_S) [/tex] follows an effective Schroedinger equation. But only as far as decoherence is part of standard QM anyway, not on the fundamental (and wrong) applications of decoherence.

The particle position is updated according to only the phase of the wavefunction, so BM uses a different definition of momentum than the standard quantum mechanics. This appears to make BM quantifiably falsifiable (ie. it is a different theory, not a different interpretation of the underlying math). What IS a momentum or momentum^2 measurement in the Bohmian interpretation?

It does not make BM different from QM (falsifiable is something different - BM is as falsifiable as QM). Simply there are two notions of momentum - the result of the quantum measurement, and the expression mv for the velocity along the trajectory. Only the first is an observable in BM. The second isn't.

But there are situations where above have the same values: This is the classical case.


In standard quantum mechanics, spin is an internal degree of freedom of a particle. In BM, this degree of freedom is included in the wavefunction by borrowing from derivations in standard quantum mechanics. BM however does not give it a definitive value like it does position. Notice however, that since the wavefunction has two components for each spin (1/2) particle now, to consider evolution of the position, we MUST consider the position to have two components as well (which need not evolve similarly, so even the "real" particle positions are superpositions now!).

There is no such necessity. The evolution equation for the single position is in this case
[tex]mv = \hbar\Im (\psi^* \nabla \psi)/\psi^*\psi[/tex]

Because the L=1,m=0 state of the hydrogen atom can be written as a real valued wavefunction, again we have the issue that the particles are stationary. But now, the particles are stationary even though there is orbital angular momentum. So not only does it seem to contradict experiment, but it seems internally inconsistent.

No. Angular momentum, as an observable, has the known QM relation to momentum, as a QM observable, and nothing to do with some rotations of the particle position.

comment J - A change in basis can change the wavefunction from real valued to complex (consider using the Lz basis, or the Lx basis). So the evolution of the position states seems to depend on the choice of basis. BM can't even seem to say definitively whether their hidden particles are moving or not.

For every particular specification of the theory, there is a well-defined answer.

That for hidden variable theories there are different possible answers is quite straightforward, at least something we should expect. Else, they would not really be hidden.

comment K - Every derivation I've seen of the spin statistics theorem relied on locality. Is there a way to get this in Bohmian mechanics as well, or does it just borrow this verbatum from standard QM as well.

Why not borrow? Once SQM is true (derived) in BM, we have any right to do this.
 
  • #18
JustinLevy
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Ilja,
Thanks for the responses. When you finish your paper on measurement, please post a link here as I'd be interested in reading it.

-------
Look guys, can we not just give Demystifier a break here? He is genuinely trying to help and all your stuff about 'glib answers' and 'your theory' seems to me unnecessarily rude.
The original questions were not addressed specifically to Demystifier. I felt it appropriate to refer to some of his responses as "his" theory because 1) he started by giving me a reference to his paper and 2) from what I have read, his responses in this thread don't match what other people have presented for bohmian mechanics. I meant no offense by calling it "his" theory. I was merely trying to be specific in my responses.

In particular, he is claiming that a closed system can obtain more information than is obtained in the wavefunction. This lead to difficulty in understanding his positions, since it seemed to contradict what I've read of other presentations of BM. (The cambridge one says "In pilot-wave theory, [the wavefunction] is a real physical field which influences particle trajectories. At the same time it represents the greatest possible information about the system.")

If my frustration shows it was because he kept answering that to make a measurement on one thing we measure something else... which doesn't answer the question. I apologize if this frustration came off as rudeness.

Your (far too many) questions are all based on standard misunderstandings - they are not some deal-killing problems with an 80 year-old theory which you are the first to notice. Why don't you just read the standard references that you were actually given in the previous thread which you claim is 'mostly unrelated', instead of effectively asking him to copy them out for you?
That thread IS mostly unrelated. I only made one post in that thread and it became 4 pages of mostly other discussion. That doesn't mean some responses weren't useful, nor does it mean those were ignored.

As I mentioned, I have read several papers and presentations of the bohmian theory.
I've also read papers that seem to refute it. I'm not claiming I'm going to come up with anything new. I'm asking about what I do not currently understand, or feel is contradictory to claims, in order to better understand discusions of the theory.

The more I read, the more I am coming to the opinion that this theory is not equivalent to standard QM. But I don't feel I can really come to a conclusion without better understanding the bohmian theory ... I want to make sure that if I decide to dismiss it, that it is for a valid reason. If I learn why I can't dismiss it, then I learn something useful as well.

In particular, the http://www.tcm.phy.cam.ac.uk/~mdt26/pilot_waves.html" [Broken] was suggested (the Lecture 4 on measurement theory answers most of your current questions).
I am not a proponent of pilot wave theory, and even I find that webpage to be a disservice to the theory. It comes off like an almost crackpot page. Look how much time he wastes on non-scientific stuff and phrasing of 'persecution'. A scientific discussion would be to present the theory as succintly and non-ambiguously as possible, then demonstrate its usefulness by making contact with current theory and make some example calculations. Everything else only does disservice to the theory.

Regardless, his webpage does present a lot of material. It doesn't answer how a measurement is made in BM... he assumes we can measure some of the hidden variables for a macroscopic object, and with this assumption we can then map any measurement to a measurement of the macroscopic object hidden variables. Basically, he too tries to explain measurement by saying we entangle it with another object and then measure the position of that second object. This is circular... or even if accepted that some hidden variables can be obtained, would allow for distinctions with standard quantum mechanics (since a closed system can learn more than what the wavefunction contains).

Passon (2006): What you always wanted to know about BM but were afraid to ask...
This too assumes we can measure the position of macroscopic objects to explain measurement. This is circular, unless you want to introduce an artificial micro/macro dichotomy.

Just to state the answer to the question implied in your thread title, the Bohm interpretation/pilot-wave theory is certainly equivalent to standard QM. How could it be otherwise?
How could it not be!? Because showing that an ensemble of particles has the same distribution as the wavefunction^2 is not equivalent. It must reproduce all correlations of the distributions as well ... which as has been argued in the past, cannot be done.

As stated in the previous thread, the entire thing flows from standard QM by assuming the psi squared means the probability of the N particles being in those positions, rather than the probability of being found there in a suitable measurement. This assumption - hardly very revolutionary when you think about it - implies that the particles continue to exist between measurements.
No, the assumption is more than that. It is that the particle exists in one place at any specific time between measurements. This is indeed revolutionary, and from what I have read, incompatible with quantum mechanics.

A final interesting point is that while it is equivalent to standard QM, it is actually of wider scope in that it also describes the 'non-equilibrium' case where the particles are not distributed as the square of the wave function. In this respect one finds (theoretically or through numerical simulation) that particles with any initial distribution which are 'stirred' by the 'pilot-wave' psi in the way suggested become distributed as psi squared in the course of time, and once so distributed, remain so. It can be shown that psi squared is the only distribution with this property.
Are you saying that despite the knowledge of position "effectively" collapsing the total wavefunction to the "conditional" wavefunction as Demystifier puts it, that over time the distribution must redistribute to the total wavefunction again? That seems to be what you are claiming here.

Besides, the fact that the distribution is ever less than that implied by the total wavefunction means the equilibrium hypothesis is wrong at that point and can be used to distinguish with regular quantum mechanics. I fail to see how the theories are equivalent.
 
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  • #19
Demystifier
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Demystifier, I am afraid I am not sure how to answer the following question, so I wonder if you could explain:

What is the status of the projection postulate in dBB? Is it an approximation, or does it hold precisely, or maybe it does not hold at all?

There is the following phrase in the Appendix that you cited (and there are similar phrases in other texts on dBB measurement theory):

"To see how this problem resolves, it is essential to realize
that, when the system consisting of the variables $x$ and $y$ can be considered as a configuration suitable for measurement of the $x$ subsystem, the total wave function is {\em not} of the form $\psi(x,t)\chi(y,t)$. Instead, the interaction between the $x$ subsystem and the $y$ subsystem should be such that the total wave function takes the form
[tex]
\begin{equation}\label{app4}
\Psi(x,y,t)=\sum_a c_a(t)\psi_a(x)\chi_a(y),
\end{equation}
[/tex]
where the normalized wave functions $\chi_a(y)$ with different labels $a$ do not overlap in the $y$ space."

However, if some wave functions do not overlap at some time point, they'll overlap later, as wave functions disperse in space with time. Of course, you can say that the measurement device is macroscopic, so its wave function does not disperse, to all practical intents and purposes. However, strictly speaking, this is not a precise statement, but an approximation, so my conclusion is that the projection postulate is an approximation as well. Is this correct or not?
Yes, it is an approximation. However, due to decoherence, this is an extremely good approximation. Essentially, this approximation is as good as the second law of thermodynamics is a good approximation.
 
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  • #20
Demystifier
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1] If at any time the total wavefunction no longer holds to the "equilibrium hypothesis", then your theory differs in predictions from standard quantum mechanics.
Agree.

2] If you gain some information about the particle, so that you can neglect some of the total wavefunction and consider only the 'conditional wavefunction' then the total wavefunction no longer holds to the "equilibrium hypothesis".
Agree.

3] The evolution of the particle positions depends on the total wavefunction, not the 'conditional wavefunction'.
Agree and disagree. The evolution is described by both, because both predict the same evolution if the initial position is in the support of both. This is the crucial point.

4] My understanding of your answer to "how do you make a measurement" was that you feel that regardless of whether the wavefunction of a macroscopic object evolves to contain a superposition of answers, the position of the object can be observed directly because it is "obvious" what the positions of "macroscopic things" are. Is this understanding correct?
Yes.

5] Previously I asked if in a closed system in which the hamiltonian and initial wavefunction was known, if additional information as a bohmian particle position could be determined. My understanding is that your answer is yes. Is this understanding correct?
I don't understand the question. Can you rephrase it?

6] Consider an external observer also knew the hamiltonian and initial wavefunction of this box, and calculated the probabilities of some results when he looks in later. Would the experimenter in the box, using his additional knowledge of the system, be able to predict the final measurements to better accuracy than the experimenter outside the box?
Yes.

I'm still interested in seeing the details of the evolution of an non-relativistic electron with a spin in an external magnetic field if you can provide a reference.
The details are presented in the book
P. R. Holland, The Quantum Theory of Motion, Sec. 9.5
Unfortunately, it is not available online.
 
  • #21
Demystifier
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Besides, the fact that the distribution is ever less than that implied by the total wavefunction means the equilibrium hypothesis is wrong at that point and can be used to distinguish with regular quantum mechanics. I fail to see how the theories are equivalent.
This is exactly what standard QM predicts as well. Namely, standard QM says that a wave-function collapse occurs, so the probability is no longer described by the total uncollapsed wave function. What the Bohmian interpretation does is to explain an effective collapse without introducing a true collapse.
 
  • #22
akhmeteli
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Yes, it is an approximation. However, due to decoherence, this is an extremely good approximation. Essentially, this approximation is as good as the second law of thermodynamics is a good approximation.

Thank you very much
 
  • #23
JustinLevy
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Your answer to #1 and #2 lead to the obvious conclusion that Bohmian mechanics is NOT equivalent to standard QM in regards to experimental predictions.

Additionally, #4 shows that you can't answer how a measurement is made without introducing an extraneous a priori dichotomy between microscopic and macroscopic physics (so Bohmian mechanics does not improve the understanding of quantum mechanics either).


Furthermore, if you accept what zenith8 stated:
"A final interesting point is that while it is equivalent to standard QM, it is actually of wider scope in that it also describes the 'non-equilibrium' case where the particles are not distributed as the square of the wave function. In this respect one finds (theoretically or through numerical simulation) that particles with any initial distribution which are 'stirred' by the 'pilot-wave' psi in the way suggested become distributed as psi squared in the course of time, and once so distributed, remain so. It can be shown that psi squared is the only distribution with this property."


Then even with your "effective" collapse, in time the narrow distribution that you measured the particle to be within will redistribute to the total wavefunction. Therefore no collapse occurred at all. This gives yet another way to distinguish the theory from standard quantum mechanics.

My conclusion, like many other physicists, is that indeed this interpretation is not equivalent to standard quantum mechanics. The more I read, the more convinced I am of this. The sheer hand-waviness of how a measurement is made appears to allow "followers" to shift their answers as is convenient for the moment, almost like the difficulty in trying to disprove a crackpot's pet theory that you cannot get to nail down his theory.
 
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  • #24
Ilja
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Your answer to #1 and #2 lead to the obvious conclusion that Bohmian mechanics is NOT equivalent to standard QM in regards to experimental predictions.

The wave function of the universe is not accessible, nor in pilot wave theory, nor in quantum theory. What matters is the effective wave function, and the system is in quantum equilibrium with it.

Additionally, #4 shows that you can't answer how a measurement is made without introducing an extraneous a priori dichotomy between microscopic and macroscopic physics (so Bohmian mechanics does not improve the understanding of quantum mechanics either).

Pilot wave theory allows to describe the collapse of the effective (conditional) wave function in time in detail, as far as we consider the global wave function and the configuration of the universe as given.


Furthermore, if you accept what zenith8 stated:
"A final interesting point is that while it is equivalent to standard QM, it is actually of wider scope in that it also describes the 'non-equilibrium' case where the particles are not distributed as the square of the wave function. In this respect one finds (theoretically or through numerical simulation) that particles with any initial distribution which are 'stirred' by the 'pilot-wave' psi in the way suggested become distributed as psi squared in the course of time, and once so distributed, remain so. It can be shown that psi squared is the only distribution with this property."


Then even with your "effective" collapse, in time the narrow distribution that you measured the particle to be within will redistribute to the total wavefunction.

That's plain wrong, these are functions on different spaces: The global wave function is defined on all possible configurations of the universe, the effective wave function on all configurations of the system.

Therefore no collapse occurred at all. This gives yet another way to distinguish the theory from standard quantum mechanics.

No. The effective wave function collapses, the global one not.

My conclusion, like many other physicists, is that indeed this interpretation is not equivalent to standard quantum mechanics. The more I read, the more convinced I am of this. The sheer hand-waviness of how a measurement is made appears to allow "followers" to shift their answers as is convenient for the moment, almost like the difficulty in trying to disprove a crackpot's pet theory that you cannot get to nail down his theory.

There is an equivalence theorem, and I would not recommend you to ignore proven theorems. There is no hand-waviness, except in postings in forums, which are obviously not scientific articles.

But it is, of course, your choice if you want to become one of the "BM inequivalent to QM"-cranks or not. (This type of crankiness is widely distributed among professional physicists, and not really dangerous, if one does not work in the foundations of QT. Despite this, it is a form of crankiness. None-crank physicists acknowledge known theorems.)
 
  • #25
JustinLevy
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The wave function of the universe is not accessible, nor in pilot wave theory, nor in quantum theory. What matters is the effective wave function, and the system is in quantum equilibrium with it.
But you are defining how the "effective" wave function evolves using something outside of your theory. This problem arises from an attempt in BM to use the wavefunction as two things: a probability distribution, and a potential used to determine evolution of the particle positions. You say the particle positions evolve unitarily, and the wavefunction evolves unitarily ... so, without adding something extraneous to your theory's postulates, the probability distribution must also evolve unitarily. In essence, your theory cannot describe measurement. It is adhoc outside of the theories postulates. Yes it is frustrating that copenhagen can't describe measurement quantum mechanically, but at least its postulates handle measurement. If you want to treat everything unitarily, then you have many worlds interpretation (ie. measurement merely means the wavefunction is no longer seperable into a wavefunction of you and a wavefunction of the object investigated).

Pilot wave theory allows to describe the collapse of the effective (conditional) wave function in time in detail, as far as we consider the global wave function and the configuration of the universe as given.
No it doesn't. Nothing in the theory's postulates cover evolution of the conditional wave function. In fact, even an 'after the fact' addition to the theory can only say that this evolution occurs during measurement, and cannot describe measurement itself. How do you measure something in BM? The resounding answer from Demystifier and many other sources are: you measure something classical. They don't explain how this measurement works... they just introduce a dichotomy, where the measurement device is somehow outside the prevue of the theory and "obviously" can be measured. They try to explain away how to make a measurement by related it to yet another measurement.

That's plain wrong, these are functions on different spaces: The global wave function is defined on all possible configurations of the universe, the effective wave function on all configurations of the system.
Are you disagreeing with zenith8? Because many "Bohmians" make the same comments zenith8 did (which I merely explained the consequences of) which is that if the probability distribution what NOT equilibrium, then over time would the probability distribution would evolve to equilibrium with the total wavefunction.

No. The effective wave function collapses, the global one not.
Exactly. That is what I argued.
The point is that the distribution (initially from phi^2 of the "effective" wave function) will distribute to equilibrium of the total wavefunction in time ... and therefore the "effective" wavefunction becomes the global one over time.

There is an equivalence theorem, and I would not recommend you to ignore proven theorems.
...
But it is, of course, your choice if you want to become one of the "BM inequivalent to QM"-cranks or not.
...
None-crank physicists acknowledge known theorems.
Any equivalence theorem would first have to define how measurement is made in the Bohmian interpretation.

Until then, they can only claim that, due to defining the wavefunction to be in equilibrium (the probability distribution of positions is as according to standard quantum mechanics) then all measurements that can be derived from a position measurement has an equivalent distribution. This follows practically from definition of how the theory was setup. But because the theory claims there is only one actual particle, intuitively one would expect there to be correlations between multiple measurements that are not equivalent to QM. Since measurements are very ill defined in BM, this is difficult to discuss.

Just like with crackpots, if "outsiders" try to do calculations and disprove it, the Bohmians claim Oh, you are using the theory wrong. If a theory was truly completely mathematical it wouldn't "belong" to anyone. Everyone should be able to use it and test it. The ambiguities allow the Bohmists to dismiss out of hand anything they do not like.

You want to see "cranky", check out this link:
In particular, the http://www.tcm.phy.cam.ac.uk/~mdt26/pilot_waves.html" [Broken] was suggested
that is similar to how many Bohmians argue their theory. It just screams crankiness.


By the way, if the position of a macroscopic object can just be "obviously" known despite it's wavefunction being spread, then this means your theory fails the Legett inequalities and mathematically fails a "no-go" theorem. As you say, "None-crank physicists acknowledge known theorems." Of course, you'll probably argue that I'm not understanding how a measurement is made in BM, but I took that practically verbatum from what Demystifier said.


To summarize:
I have NOT been asking questions in a vaccuum. I have talked to several researchers around me, read up on several papers, read many pro-bohmian articles, and tried to follow up in the literature on some comments made here. If my conclusions are wrong, then by all means explain mathematical details why this is so. However, please stop claiming I and many other physicists of the same opinion are wrong by using the same tired excuses without providing substantive detail on your theory. By all means, lay out your theory with full mathematical detail.
 
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  • #26
Ilja
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But you are defining how the "effective" wave function evolves using something outside of your theory.

No. The conditional (effective) wave function of the subsystem S for some decomposition q = (qS, qrest) is defined as [itex]\psi(q_S) = \Psi(q_S, q_{rest})[/itex]. What is used is, therefore, the wave function of the universe and the configuration of the remaining part of the universe. Above parts are well-defined and really existing objects of pilot wave theory. Thus, the effective wave function is also well-defined and really existing.

This problem arises from an attempt in BM to use the wavefunction as two things: a probability distribution, and a potential used to determine evolution of the particle positions. You say the particle positions evolve unitarily, and the wavefunction evolves unitarily ... so, without adding something extraneous to your theory's postulates, the probability distribution must also evolve unitarily.

I don't say that particle positions evolve unitarily, this makes no sense. Unitary evolution is defined in some Hilbert space, but the particle positions live in another space, the configuration space.

In essence, your theory cannot describe measurement. It is adhoc outside of the theories postulates. Yes it is frustrating that copenhagen can't describe measurement quantum mechanically, but at least its postulates handle measurement.

Sorry, you are simply wrong here.

If you want to treat everything unitarily, then you have many worlds interpretation (ie. measurement merely means the wavefunction is no longer seperable into a wavefunction of you and a wavefunction of the object investigated).

I don't want everything evolving unitarily, it is only the wave function of the universe which evolves unitarily. The conditional wave function does in general not evolve unitarily, but sometimes collapses.

No it doesn't. Nothing in the theory's postulates cover evolution of the conditional wave function.

Look at the definition above. BM defines the evolution of the wave function of the universe via Schroedinger equation as well as of qrest via the guiding equation. Thus, the evolution of all parts used in the definition of the conditional wave function is well-defined. Therefore, the evolution of the conditional wave function is also well-defined. If the resulting evolution of the conditional wave function is unitary or not uniquely follows from the theory, but depends on the global wave function as well as on qrest.

In fact, even an 'after the fact' addition to the theory can only say that this evolution occurs during measurement, and cannot describe measurement itself.

There is no "after the fact" addition to the theory. And how some measurement-like physical process leads to the collapse of the effective wave function is something everybody can compute from the equations if he likes.

How do you measure something in BM? The resounding answer from Demystifier and many other sources are: you measure something classical.

My answer sounds a little bit different. You have some interaction, and after this interaction your state qyou, which contains all the information you have observed, is correlated with the conditional wave function of the system you have observed in the way prescribed by the Born rule. This is a proven theorem, not wishful thinking.


Are you disagreeing with zenith8? Because many "Bohmians" make the same comments zenith8 did (which I merely explained the consequences of) which is that if the probability distribution what NOT equilibrium, then over time would the probability distribution would evolve to equilibrium with the total wavefunction.

I'm not disagreeing. There is no reason for disagreement.


The point is that the distribution (initially from phi^2 of the "effective" wave function) will distribute to equilibrium of the total wavefunction in time ... and therefore the "effective" wavefunction becomes the global one over time.

Read again the definition of the conditional wave function. It is a function on a different space, the space QS of configurations of the system, while the global wave function depends on the configuration Q of the whole universe. How can a function become another function with a different set of parameters?

Any equivalence theorem would first have to define how measurement is made in the Bohmian interpretation.

That's what is done, see my explanation above.

Until then, they can only claim that, due to defining the wavefunction to be in equilibrium (the probability distribution of positions is as according to standard quantum mechanics) then all measurements that can be derived from a position measurement has an equivalent distribution.

This is also not exactly the point, one should not derive all measurements from position measurements, but from actual positions. If you observe something different, than your actual configuration (the content of your brain cells) differs, but nobody observes these brain cells. Thus, the measurement results are actual positions of something in your brain.


But because the theory claims there is only one actual particle, intuitively one would expect there to be correlations between multiple measurements that are not equivalent to QM.

I have no such intuitions, and there is no necessity for them, because one can compute the results from the BM equations.

Since measurements are very ill defined in BM, this is difficult to discuss.

The only thing which is ill-defined is your version of it.

Just like with crackpots, if "outsiders" try to do calculations and disprove it, the Bohmians claim Oh, you are using the theory wrong. If a theory was truly completely mathematical it wouldn't "belong" to anyone. Everyone should be able to use it and test it. The ambiguities allow the Bohmists to dismiss out of hand anything they do not like.

Wrong. BM does not belong to anyone, everything is well-defined there, and everybody who knows it can use it. That many people make errors applying this is an unfortunate fact, but this is not a problem of BM, but a problem of those who don't know it sufficiently well to apply it correctly.

By the way, if the position of a macroscopic object can just be "obviously" known despite it's wavefunction being spread, then this means your theory fails the Legett inequalities and mathematically fails a "no-go" theorem.

Nonsense. The Legett inequalities are about some strange way to combine non-local realistic theories with relativity, which is not used in BM. The assumptions made in this inequality fail for BM.

Of course, you'll probably argue that I'm not understanding how a measurement is made in BM, but I took that practically verbatum from what Demystifier said.

I have not read everything he has written. Maybe he has failed somewhere in his explanations, may be you have failed to understand him correctly. Fact is that your understanding of the measurement process in BM is completely invalid, given that you have clearly not understood the basic definition of the conditional wave function.


I have NOT been asking questions in a vaccuum. I have talked to several researchers around me, read up on several papers, read many pro-bohmian articles, and tried to follow up in the literature on some comments made here. If my conclusions are wrong, then by all means explain mathematical details why this is so.

No problem. The first important mathematical detail you have to understand is the definition of the conditional wave function I have given, to see that it is well-defined, its evolution is well-defined, and it is something completely different from the global wave function. It seems, once you have understood this, your argumentation has to be modified somehow.

Then, there are (unfortunately) approaches to the equivalence proof which reduce general measurements to measurements of the configuration, instead of explaining them with the actual states of the configuration. While the first way is not plainly wrong, once the configuration is in principle exactly observable, it complicates the understanding. There may be different equivalence proofs, one easier and conceptually clearer than another, so I recommend you my way.

The key point of my way is that the configuration of the observer has to be included into the picture. Different measurement results are, then, described by different configurations of the observer after the measurement. These different configurations are part of qrest. Thus, different measurement results correspond to different values of qrest, which are then used to define the conditional (effective) wave function.

This way has the advantage that we never have to care about measurements of configurations.

However, please stop claiming I and many other physicists of the same opinion are wrong by using the same tired excuses without providing substantive detail on your theory. By all means, lay out your theory with full mathematical detail.

It is hard to do this in forum articles. But anyway I wanted to write an introduction into pilot wave theory. And I will try my best to explain you whatever problem with BM you have, in as much detail as you like.
 
  • #27
Hurkyl
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No. The conditional (effective) wave function of the subsystem S for some decomposition q = (qS, qrest) is defined as [itex]\psi(q_S) = \Psi(q_S, q_{rest})[/itex].
As written, that doesn't make sense. I assume you meant to include some sort of "projection" operator there -- e.g. the partial trace?
 
  • #28
Ilja
676
83
But you are defining how the "effective" wave function evolves using something outside of your theory.

No. The conditional (effective) wave function of the subsystem S for some decomposition q = (qS, qrest) is defined as [itex]\psi(q_S) = \Psi(q_S, q_{rest})[/itex]. What is used is, therefore, the wave function of the universe and the configuration of the remaining part of the universe. Above parts are well-defined and really existing objects of pilot wave theory. Thus, the effective wave function is also well-defined and really existing.

This problem arises from an attempt in BM to use the wavefunction as two things: a probability distribution, and a potential used to determine evolution of the particle positions. You say the particle positions evolve unitarily, and the wavefunction evolves unitarily ... so, without adding something extraneous to your theory's postulates, the probability distribution must also evolve unitarily.

I don't say that particle positions evolve unitarily, this makes no sense. Unitary evolution is defined in some Hilbert space, but the particle positions live in another space, the configuration space.

In essence, your theory cannot describe measurement. It is adhoc outside of the theories postulates. Yes it is frustrating that copenhagen can't describe measurement quantum mechanically, but at least its postulates handle measurement.

Sorry, you are simply wrong here.

If you want to treat everything unitarily, then you have many worlds interpretation (ie. measurement merely means the wavefunction is no longer seperable into a wavefunction of you and a wavefunction of the object investigated).

I don't want everything evolving unitarily, it is only the wave function of the universe which evolves unitarily. The conditional wave function does in general not evolve unitarily, but sometimes collapses.

No it doesn't. Nothing in the theory's postulates cover evolution of the conditional wave function.

Look at the definition above. BM defines the evolution of the wave function of the universe via Schroedinger equation as well as of qrest via the guiding equation. Thus, the evolution of all parts used in the definition of the conditional wave function is well-defined. Therefore, the evolution of the conditional wave function is also well-defined. If the resulting evolution of the conditional wave function is unitary or not uniquely follows from the theory, but depends on the global wave function as well as on qrest.

In fact, even an 'after the fact' addition to the theory can only say that this evolution occurs during measurement, and cannot describe measurement itself.

There is no "after the fact" addition to the theory. And how some measurement-like physical process leads to the collapse of the effective wave function is something everybody can compute from the equations if he likes.

How do you measure something in BM? The resounding answer from Demystifier and many other sources are: you measure something classical.

My answer sounds a little bit different. You have some interaction, and after this interaction your state qyou, which contains all the information you have observed, is correlated with the conditional wave function of the system you have observed in the way prescribed by the Born rule. This is a proven theorem, not wishful thinking.


Are you disagreeing with zenith8? Because many "Bohmians" make the same comments zenith8 did (which I merely explained the consequences of) which is that if the probability distribution what NOT equilibrium, then over time would the probability distribution would evolve to equilibrium with the total wavefunction.

I'm not disagreeing. There is no reason for disagreement.


The point is that the distribution (initially from phi^2 of the "effective" wave function) will distribute to equilibrium of the total wavefunction in time ... and therefore the "effective" wavefunction becomes the global one over time.

Read again the definition of the conditional wave function. It is a function on a different space, the space QS of configurations of the system, while the global wave function depends on the configuration Q of the whole universe. How can a function become another function with a different set of parameters?

Any equivalence theorem would first have to define how measurement is made in the Bohmian interpretation.

That's what is done, see my explanation above.

Until then, they can only claim that, due to defining the wavefunction to be in equilibrium (the probability distribution of positions is as according to standard quantum mechanics) then all measurements that can be derived from a position measurement has an equivalent distribution.

This is also not exactly the point, one should not derive all measurements from position measurements, but from actual positions. If you observe something different, than your actual configuration (the content of your brain cells) differs, but nobody observes these brain cells. Thus, the measurement results are actual positions of something in your brain.


But because the theory claims there is only one actual particle, intuitively one would expect there to be correlations between multiple measurements that are not equivalent to QM.

I have no such intuitions, and there is no necessity for them, because one can compute the results from the BM equations.

Since measurements are very ill defined in BM, this is difficult to discuss.

The only thing which is ill-defined is your version of it.

Just like with crackpots, if "outsiders" try to do calculations and disprove it, the Bohmians claim Oh, you are using the theory wrong. If a theory was truly completely mathematical it wouldn't "belong" to anyone. Everyone should be able to use it and test it. The ambiguities allow the Bohmists to dismiss out of hand anything they do not like.

Wrong. BM does not belong to anyone, everything is well-defined there, and everybody who knows it can use it. That many people make errors applying this is an unfortunate fact, but this is not a problem of BM, but a problem of those who don't know it sufficiently well to apply it correctly.

By the way, if the position of a macroscopic object can just be "obviously" known despite it's wavefunction being spread, then this means your theory fails the Legett inequalities and mathematically fails a "no-go" theorem.

Nonsense. The Legett inequalities are about some strange way to combine non-local realistic theories with relativity, which is not used in BM. The assumptions made in this inequality fail for BM.

Of course, you'll probably argue that I'm not understanding how a measurement is made in BM, but I took that practically verbatum from what Demystifier said.

I have not read everything he has written. Maybe he has failed somewhere in his explanations, may be you have failed to understand him correctly. Fact is that your understanding of the measurement process in BM is completely invalid, given that you have clearly not understood the basic definition of the conditional wave function.


I have NOT been asking questions in a vaccuum. I have talked to several researchers around me, read up on several papers, read many pro-bohmian articles, and tried to follow up in the literature on some comments made here. If my conclusions are wrong, then by all means explain mathematical details why this is so.

No problem. The first important mathematical detail you have to understand is the definition of the conditional wave function I have given, to see that it is well-defined, its evolution is well-defined, and it is something completely different from the global wave function. It seems, once you have understood this, your argumentation has to be modified somehow.

Then, there are (unfortunately) approaches to the equivalence proof which reduce general measurements to measurements of the configuration, instead of explaining them with the actual states of the configuration. While the first way is not plainly wrong, once the configuration is in principle exactly observable, it complicates the understanding. There may be different equivalence proofs, one easier and conceptually clearer than another, so I recommend you my way.

The key point of my way is that the configuration of the observer has to be included into the picture. Different measurement results are, then, described by different configurations of the observer after the measurement. These different configurations are part of qrest. Thus, different measurement results correspond to different values of qrest, which are then used to define the conditional (effective) wave function.

This way has the advantage that we never have to care about measurements of configurations.

However, please stop claiming I and many other physicists of the same opinion are wrong by using the same tired excuses without providing substantive detail on your theory. By all means, lay out your theory with full mathematical detail.

It is hard to do this in forum articles. But anyway I wanted to write an introduction into pilot wave theory. And I will try my best to explain you whatever problem with BM you have, in as much detail as you like.
 
  • #29
JustinLevy
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I agree with Hurkyl, what you have presented for the "conditional" wavefunction does not make sense, and at the very least is quite ill defined. Based on your comments you seem to be referring to a partial trace.

Before continuing, please note that what you are calling a conditional wavefunction is not what Demystifier was calling a conditional wavefunction. It is frustrating that measurement in BM is ill defined enough that reading many sources seems to provide many different theories. Bohmists don't seem to even agree what their theory is (this is especially true when looking at "extensions" to achieve relativistic quantum mechanics). And second, even if we do take your "trace" argument to define the conditional wavefunction, this still does not demonstrate collapse. There is still no measurement in your theory. Please be much more specific in your math, because as currently described all you have done is add yet another bizarre interpretation of measurement on top of Bohmian mechanics.

In particular, you claim that for the conditional wavefunction:
"its evolution is well-defined"
yet you also claim
"Thus, different measurement results correspond to different values of qrest, which are then used to define the conditional (effective) wave function."

You are defining the conditional wavefunction (and hence the supposed collapse) using the results of a measurement, instead of something intrinsic in your theory. That is a major point, you are adding something outside of BM evolution of the system to try to incorporate measurement. And like the "bohmians" before you, you cannot derive a measurement from your postulates but instead insert a measurement to explain another measurement.

Even worse is this..
This is also not exactly the point, one should not derive all measurements from position measurements, but from actual positions. If you observe something different, than your actual configuration (the content of your brain cells) differs, but nobody observes these brain cells. Thus, the measurement results are actual positions of something in your brain.
So all you've done is transfer the measurement of Demystifier's "obvious" measurement of a classical system, to the brain's consciousness somehow "obviously" knowing the actual position of its particle components in the wavefunction. At least Demystifier's a priori dichotomy was non anthropic (micro vs. macro), but you are adding in a dichotomy that consciousness can "obviously" know the positions of its particles.

This is far from an improvement, and all you did was define a measurement again in terms of another measurement.

-----------

I don't say that particle positions evolve unitarily, this makes no sense. Unitary evolution is defined in some Hilbert space, but the particle positions live in another space, the configuration space.
Consider the N particle positions to be a vector in R^3N space. I was hoping it was clear what is meant by unitary here. If not, the point is that the evolution is reversible.

I don't want everything evolving unitarily, it is only the wave function of the universe which evolves unitarily. The conditional wave function does in general not evolve unitarily, but sometimes collapses.
Since the fundamental evolution in your theory is unitary, then no collapse is possible.

There is no "after the fact" addition to the theory. And how some measurement-like physical process leads to the collapse of the effective wave function is something everybody can compute from the equations if he likes.
Then please give an explicit example.


Regarding the statement that if the probability distribution what NOT equilibrium, then over time would the probability distribution would evolve to equilibrium with the total wavefunction ...
I'm not disagreeing. There is no reason for disagreement.
Good we agree on something.

Nonsense. The Legett inequalities are about some strange way to combine non-local realistic theories with relativity, which is not used in BM. The assumptions made in this inequality fail for BM.
I've reread his paper "Nonlocal hidden-variable theories and quantum mechanics: An incompatibility theorem." and I don't see him assuming relativity anywhere. In fact he never even refers to relativity in the entire paper. As should be clear from the title, he quite explicitly allows theories with non-local interactions which violate relativity.

Again, from what I've read, the "equivalence" proofs of Bohmian mechanics merely show that measurements have the same distributions but doesn't prove they have the same correlations. That isn't a true proof of equivalence at all.
 
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  • #30
Ilja
676
83
As written, that doesn't make sense. I assume you meant to include some sort of "projection" operator there -- e.g. the partial trace?

No trace. Simply we put the actual values of qrest into the function depending on qS and qrest and obtain a function depending only on qS.
 
  • #31
Ilja
676
83
I agree with Hurkyl, what you have presented for the "conditional" wavefunction does not make sense, and at the very least is quite ill defined. Based on your comments you seem to be referring to a partial trace.

No trace, but inserting the actual value of qrest.

Before continuing, please note that what you are calling a conditional wavefunction is not what Demystifier was calling a conditional wavefunction. It is frustrating that measurement in BM is ill defined enough that reading many sources seems to provide many different theories. Bohmists don't seem to even agree what their theory is (this is especially true when looking at "extensions" to achieve relativistic quantum mechanics).

Given that you have not understood my definition of the conditional wave function, I feel free to ignore this. I have never experienced such feelings reading Bohmian theories. (But this rather nicely describes my initial feelings reading about many worlds.)

In particular, you claim that for the conditional wavefunction:
"its evolution is well-defined"
yet you also claim
"Thus, different measurement results correspond to different values of qrest, which are then used to define the conditional (effective) wave function."

You are defining the conditional wavefunction (and hence the supposed collapse) using the results of a measurement, instead of something intrinsic in your theory.

No, I don't use the result of some measurement of qrest, but the actual value of qrest(t) at the moment of time t when the observer sees the difference. qrest(t) exists and is intrinsic to the theory.

That is a major point, you are adding something outside of BM evolution of the system to try to incorporate measurement. And like the "bohmians" before you, you cannot derive a measurement from your postulates but instead insert a measurement to explain another measurement.

I don't. Now, given the fact that positions are observable in pilot wave theory, it is easy to mingle the actual values with some measured values. So some "Bohmians" can mingle them. In particular, such a confusion appears in a natural way if we follows the way we have learned in the CI: To describe the measurement using at first some quantum process, and, then, leaving everything else (the human observing the classical device) to the classical part of the CI. The better and more consistent way is to take the whole universe described in a Bohmian way, with the observer already being part of it, and its state described by some part of qrest.

So all you've done is transfer the measurement of Demystifier's "obvious" measurement of a classical system, to the brain's consciousness somehow "obviously" knowing the actual position of its particle components in the wavefunction.

Not at all. The brain does not have to know its own state. It simply is this state.

At least Demystifier's a priori dichotomy was non anthropic (micro vs. macro), but you are adding in a dichotomy that consciousness can "obviously" know the positions of its particles.

No. Different states of consciousness have to have different states of rest. This is a triviality. (It doesn't even matter here if you are a pure materialist or believe into some dualism. All we need is that if the brain states are identical, then the corresponding states of consciousness have to be identical too.

Consider the N particle positions to be a vector in R^3N space. I was hoping it was clear what is meant by unitary here. If not, the point is that the evolution is reversible.

Since the fundamental evolution in your theory is unitary, then no collapse is possible.

If I replace your "unitary" with "reversible", then this is the old objection how one can get thermodynamic equilibrium from reversible Newtonian mechanics. Of course, pilot wave theory uses the same ideas to get, in quantum equilibrium, an equilibrium out of a reversible theory. If you think that what is done in thermodynamics is in some sense inherently wrong, then, ok, quantum equilibrium is inherently wrong in the same sense. But this is nothing I have to care much, and clearly doesn't make BM cranky.

Then please give an explicit example.

Standard QM measurement theory (with decoherence) describes how the initial state

[itex](a_1\psi_1+a_2\psi_2)\phi[/itex] evolves into [itex]a_1\psi_1(q_S)\phi_1(q_{rest})+a_2\psi_2(q_s)\phi_2(q_{rest})[/itex]. Any description of Schroedingers cat uses this. We need that [itex]\phi_1,\phi_2[/itex] (the two resulting states of Schroedingers cat) have different support in qrest. If you see the cat alive or dead, the state of your brain will be different if the cat is alive and if it is dead.

Now, we put the actual state of qrest into the expression and obtain or [itex]a_1\psi_1(q_S)\phi_1(q_{rest})[/itex] or [itex]a_2\psi_2(q_s)\phi_2(q_{rest})[/itex], because [itex]\phi_i(q_{rest})=0[/itex] for the other i. Above are product states, thus, if we consider only experiments related with the subsystem, it can be handled now as equivalent to one of the [itex]\psi_i(q_S)[/itex].

But there is an evolution between the starting point where [itex]\phi_1=\phi_2=\phi(q_{rest})[/itex] and the final point where [itex]\phi_1\phi_2=0[/itex]. During this time, the state is not in a product state, and its evolution is not unitary.

There is no tracing over all possible values of qrest to defined the intermediate state, but one always uses the actual value of qrest(t).




I've reread his paper "Nonlocal hidden-variable theories and quantum mechanics: An incompatibility theorem." and I don't see him assuming relativity anywhere. In fact he never even refers to relativity in the entire paper. As should be clear from the title, he quite explicitly allows theories with non-local interactions which violate relativity.

AFAIR the whole game was based on different notions of "before" for measurement devices in relative motion. In a theory with preferred frame, there is no such incompatibility. The relativistic "before" of a moving measurement device is simply irrelevant.

Again, from what I've read, the "equivalence" proofs of Bohmian mechanics merely show that measurements have the same distributions but doesn't prove they have the same correlations. That isn't a true proof of equivalence at all.

How can one have the same distributions on the same global configuration space and not have the same correlations? Explain. One should, of course, consider the distribution of the whole configuration, not only the traces of the distribution for the different subsystems. But of course BM considers the global distribution.
 
  • #32
Hurkyl
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Standard QM measurement theory (with decoherence) describes how the initial state
...
Now, we put the actual state of qrest
In "standard QM measurement theory", qrest is a dummy variable; there isn't an an "actual state".

The thing I think you're thinking, but haven't really conveyed, is that you are taking the two-variable function [itex]\Psi(u, v)[/itex], and plugging {the positions of the corresponding Bohmian particles} in for v.

(I purposely changed the dummy variables to u and v to reduce the chance that they would be confused with something else)
 
  • #33
Ilja
676
83
In "standard QM measurement theory", qrest is a dummy variable; there isn't an an "actual state".

The thing I think you're thinking, but haven't really conveyed, is that you are taking the two-variable function [itex]\Psi(u, v)[/itex], and plugging {the positions of the corresponding Bohmian particles} in for v.

(I purposely changed the dummy variables to u and v to reduce the chance that they would be confused with something else)

Correct, that's the difference between QM and pilot wave: In pilot wave we have an actual state qrest(t) which we can put into it.

And, again, correct, I consider the wave function of the whole universe as a function depending on two parameter sets, qS and qrest, and put the actual value for qrest into it, to obtain a function of qS only. The function of qS only is the conditional wave function.
 
  • #34
JustinLevy
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And, again, correct, I consider the wave function of the whole universe as a function depending on two parameter sets, qS and qrest, and put the actual value for qrest into it, to obtain a function of qS only. The function of qS only is the conditional wave function.
Then "collapse" as you describe it can only happen if you already know some of the hidden variables (ie. quantum equilibrium is not fullfilled).

You keep talking as if you've fixed the "measurement problem", but you haven't. Just like Demystifier, you require:
1] entangling the position of what you wish to measure with a larger object
2] determining the position of the larger object

All you have done is transfer the problem of measurement to a problem of a different measurement. Demystifier did step #2 by creating a dichotomy between micro and macroscopic objects and declaring, outside of the theory, that one can "obviously" know the position of macroscopic objects. You indeed take a different approach, but it still does not solve anything. You instead state that a conscious object can obviously know more information that its wavefunction. You make a dichotomy between conscious and non-self aware objects. This is not an improvement. If anything it is worse than Demystifier's dichotomy, since his at least has a clear parameterization based on some variables (size), while yours is incredibly ill defined.

This is the problem of your theory in a nutshell:
A] If the hidden variables where known, the theory would not be equivalent to quantum mechanics for experimental predictions (the theory's postulate of quantum equilibrium would be wrong).
B] However, if the hidden variables are NOT accessible, then the theory cannot describe measurement.

This is a catch 22. Either way your theory is wrong.

Now, given the fact that positions are observable in pilot wave theory, it is easy to mingle the actual values with some measured values.
To do this, you would have to be able to ... using only the postulates of your theory ... have a closed system start in quantum equilibrium and be able to LEARN that it is NOT in quantum equilibrium. Are you saying a closed system can do experiments to learn it is not in quantum equilibrium? And if so, what prevents further experiments distinguishing the theory from standard quantum mechanics?

Not at all. The brain does not have to know its own state. It simply is this state.
But you are assuming the brain can distinguish between these states. That it can enumerate these states. That is what is needed for "knowing" the result. You are stating that the secret to obtaining information about hidden variables is through consciousness in objects.

If I replace your "unitary" with "reversible", then this is the old objection how one can get thermodynamic equilibrium from reversible Newtonian mechanics.
No, yours is the opposite problem. You start with equilibrium, and despite unitary evolution, claim collapse into a non-equilibrium state. Unitary evolution forbids this.

AFAIR the whole game was based on different notions of "before" for measurement devices in relative motion. In a theory with preferred frame, there is no such incompatibility. The relativistic "before" of a moving measurement device is simply irrelevant.
I am getting the strong impression you have never read this paper yourself.
Look, you made a complaint and I looked up the paper again ... it turned out your complaint wasn't valid. In response you make yet another claim without looking at the paper? Come on. I don't remember anything like that in the paper. As a double check I searched for "relativ" and saw no mention of relativity nor relative motion. Please stop arguing with what are effectively guesses. Please read the paper.

How can one have the same distributions on the same global configuration space and not have the same correlations? Explain. One should, of course, consider the distribution of the whole configuration, not only the traces of the distribution for the different subsystems. But of course BM considers the global distribution.
You are trying to replace the randomness in individual measurements, by cloaking it as the distribution of an ensemble of measurements. These concepts are by no means equivalent nor necessarily compatible.

As pointed out by other physicists, in the interaction picture, positions can become non-commuting observables. Bohmian mechanics cannot describe away such situations by an ensemble of measurements, because the positions, while hidden variables, are always definite and single valued.

Look, Newton made mistakes, Einstein made mistakes, we've all made mistakes. I truly hope you are not sweeping away any doubts on the theory due to Bohm's laurels. Bohm truly thought that experiments on Bell's inequality would show that quantum mechanics was incomplete. Instead, he ended up conceding that spin had to be treated, not classically, but quantum mechanically. Sure, BM was extended. Yet even then, several issues with BM have been pointed out by other physicists. What would it take for you to come to an understanding that Bohm's theory is incorrect, is a mistake?

Look how many posts, and papers, and websites, have been suggested and read and yet it is still unclear how BM can even explain measurement without falling into the catch 22 above. These complaints are by no means new ideas, but Bohmists seem to ignore all complaints and trudge on anyway.
 
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  • #35
Demystifier
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Look how many posts, and papers, and websites, have been suggested and read and yet it is still unclear how BM can even explain measurement without falling into the catch 22 above. These complaints are by no means new ideas, but Bohmists seem to ignore all complaints and trudge on anyway.
You are wrong that your complaints are not new. Other people complain for several reasons, but nobody complains about stuff that you do.
The reason is the following. Maybe you are right that the Bohmian interpretation does not COMPLETELY solve the measurement problem. But at least it solves it partially, by making it completely equivalent to the measurement problem in CLASSICAL mechanics. Namely, in classical mechanics it is also true that one can observe only macroscopic stuff, not microscopic. Not because there is a fundamental boundary between macroscopic and microscopic, but because the observers are macroscopic. Other people see no problems with it, because they do not see any fundamental problems with measurement in classical mechanics. You either do not realize the analogy between the measurement problems in classical and Bohmian mechanics, or consider the measurement problem in classical mechanics to be unsolved as well.
 

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