In what sense is QM not understood ?

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In summary, some people think that quantum mechanics is "not understood" because it is a field of mathematics that deals with probabilities of measuring final states, rather than the 1 input --> 1 output style of classical mechanics. Others say that this is because the founders of QM did not understand what they were doing, and that it was a complex process that led to incorrect guesses. It seems that the best way to understand quantum mechanics is to first learn the formalism and then think about the "interpretation" of it.
  • #141


kith said:
I don't see why EPR correlations are weird beyond the general measurement problem.

Yes, I would say that the only thing weird about quantum mechanics is the measurement problem.

And if we are able to explain the measurement problem (which I think is done in various interpretations), we have a clear mechanism how these correlations occur.

I don't think that we really have solved the measurement problem. Decoherence certainly doesn't solve it. What decoherence does is to explain why, even though we may start off with the system described by a pure state, we might end up with the system described by a mixed state. But what is a mixed state? It describes an ensemble. So there isn't just one world, but an ensemble of possible worlds. But what is a "world"?
 
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  • #142


stevendaryl said:
I don't think that we really have solved the measurement problem. Decoherence certainly doesn't solve it. What decoherence does is to explain why, even though we may start off with the system described by a pure state, we might end up with the system described by a mixed state. But what is a mixed state? It describes an ensemble. So there isn't just one world, but an ensemble of possible worlds. But what is a "world"?
Are you familiar with the ensemble interpretation, the many worlds interpretation and the interpretation of de Broglie and Bohm? All of them answer this question.
 
  • #143


kith said:
Are you familiar with the ensemble interpretation, the many worlds interpretation and the interpretation of de Broglie and Bohm? All of them answer this question.

Yes, I'm familiar with those, and I don't find any of them very satisfactory.
 
  • #144


stevendaryl said:
Yes, I'm familiar with those, and I don't find any of them very satisfactory.
Whether these interpretations are satisfactory or not is a question with various aspects. Personally, I prefer the Copenhagen interpretation because it is very close to the way science works. This is more important for me than solving the measurement problem, but I am aware of the fact that it is simply not there in other interpretations. So I don't think we need a new theory to explain it and I don't expect us to understand these things better in future theories.
 
  • #145


stevendaryl said:
Yes, I would say that the only thing weird about quantum mechanics is the measurement problem.
I don't think that we really have solved the measurement problem. Decoherence certainly doesn't solve it. What decoherence does is to explain why, even though we may start off with the system described by a pure state, we might end up with the system described by a mixed state. But what is a mixed state? It describes an ensemble. So there isn't just one world, but an ensemble of possible worlds. But what is a "world"?

and by the way decoherence can be Intrinsic, Extrinsic, and Environmental
intrisc from an autonomous nonlinear quantum mechanics and solves the measurement problem.
enviromental from an environment induced supeselection (zurek joos and zeh) and do not solves the measurement problem.
 
  • #146


yoda jedi said:
intrisc from an autonomous nonlinear quantum mechanics and solves the measurement problem.
What are you talking about here?
 
  • #147


Fredrik said:
What are you talking about here?

an inherently nonlinear quantum mechanics in an opposition to a non inheherently nonlinear theory like CSL which the nonlinnearity is induced by a stochastic field.
 
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  • #148


But the question is, does such a theory really exist, or are you just speculating about some new theory that might be able to resolve the measurement problem by replacing the linear simplicity of quantum mechanics with some nonlinear complexity? For my own part, I'd rather have the measurement problem!
 
  • #149


Ken G said:
In my experience, Bohr detractors generally just don't understand him. He did clarify something-- he clarified that we must address the role of the physicist in physics, expressly because the physicist perceives nonunitary evolution, and the postulates of QM are about unitary evolution.

It seems strange to say that "we must address the role of the physicist in physics", because for practical purposes, we DON'T address the role of the physicist in physics. We use various rules of thumb for interpreting quantum predictions, and a deep understanding of the relationship between the physicist and the physics is just not important. Which is good, because we don't have any such deep understanding.

I think your understanding of Bell's theorem is rather incomplete. Your description sounds more like Bertlmann's socks, a common misconception about Bell's theorem.

I don't know why you would say that. The weird thing about QM is that it DOESN'T have a "Bertlmann's socks" interpretation of nondeterminism and correlation. I don't know why you would say that I believe the opposite of what I believe.
 
  • #150


bhobba said:
Exactly. Decoherence for all practical purposes resolves the collapse of a wavefunction issue. IMHO its purely philosophical waffle if you don't like it - to some people such things are important - for me I couldn't care less.

I don't see a big difference between that notion of "resolving the issue" and just deciding not to worry about it. You don't actually need decoherence to decide not to worry about it--you can just stick to the recipe for quantum predictions.
 
  • #151


Ken G said:
If the universe is fundamentally probabilistic, then it is not fundamentally unitary in its time evolution. If I can prepare two particles as spin up, and do a sideways spin measurement, I can get left or right for different particles with equal probability, which we might regard as just fundamentally how the universe works. But since the initial states were superpositions of left and right, and the final states are one or the other, that's not unitary, if it's fundamentally probabilitistic. That does imply a lack of unitary evolution when you do an observation and only get one outcome.

I see what you mean. However, it's really not clear what it would "mean" to see superpositions, so the fact that we don't see superpositions is sort of a mystery, but doesn't really contradict any assumption about unitary evolution.

To "notice" that a system is in a superposition of states means that it's possible to make a decision based on whether the state is pure or not. But there is no way to do that. There is no way to make a machine that prints out "yes" if the system it observes is in a superposition of states and "no" otherwise.
 
  • #152


stevendaryl said:
It seems strange to say that "we must address the role of the physicist in physics", because for practical purposes, we DON'T address the role of the physicist in physics.
The "must" means, at the least, "in order to not have threads about why we don't understand quantum mechanics", and at the most, to obtain the next great theory of physics.
We use various rules of thumb for interpreting quantum predictions, and a deep understanding of the relationship between the physicist and the physics is just not important.
It's not important if you don't mind having threads like this one, and you don't mind a theory that cannot (yet) be merged with gravity, or be applied to arbitrary energy scales.
I don't know why you would say that. The weird thing about QM is that it DOESN'T have a "Bertlmann's socks" interpretation of nondeterminism and correlation.
You claimed, above, that what was strange was that you could get 100% certainty about what one particle would do based on observations of another particle. But that's not strange at all, that's Bertlmann's socks. Classical physics works the same way, it has nothing to do with quantum mechanics until you look at subtle (Bell-type) correlations among the indeterminacies that are unique to quantum mechanics.
 
  • #153


stevendaryl said:
However, it's really not clear what it would "mean" to see superpositions, so the fact that we don't see superpositions is sort of a mystery, but doesn't really contradict any assumption about unitary evolution.
The two issues are so tightly connected there's no reason to separate them into two different problems. The "why we don't see superpositions" problem and the "why we don't see unitary evolution" problem is the same problem, called the measurement problem. It's a disconnect between the postulates of the theory, and what we see. The fundamental postulate is that time evolution is unitary, which says superpositions evolve into superpositions, or into mixed states if you project onto a subspace of a system interacting with its environment. But we don't see either superpositions or mixed states for individual particles-- we see definite outcomes. So what we observe is just not unitary. So you can either say (as Bohr did) that the unitary part is only part of what is happening (since what the physicist observes must be the full result, and it's non-unitary), or (as Everett did) that the unitary part is everything but we don't see all of it because the physicist doesn't perceive the full picture, or (as Bohm did) that the unitary part is just the evolution of the pilot wave that influences the fully classical-like behavior in a hidden way, such that we don't see the unitary evolution because we are incompletely describing these hidden variables. But none of those interpretation restrict themselves to the basic structure of unitary evolution of superposition states-- they all have to add some kind of overhead to that basic postulate to get it to agree with what we observe.
There is no way to make a machine that prints out "yes" if the system it observes is in a superposition of states and "no" otherwise.
That's because it is never the observation that says a particle is in a superposition state, it is always the postulates of quantum mechanics that says that. That's the issue in this thread-- the difficulty in reconciling the postulates of quantum mechanics that statistically explain what we observe, with what we actually do observe. That's the measurement problem.
 
  • #154


Ken G said:
with what we actually do observe. That's the measurement problem.




to observe something has to exist before.
 
  • #155


sigma.alpha said:
to observe something has to exist before.

That the problem - you run into the Kochen-Specher Theorem - it can't have a definite value before observation unless something else comes into play - IMHO that something else is decoherence. It transforms a superposition into a mixed state - but a mixed state where the states are eigenstates of what you are measuring. This means it does exist as what the measurement shows it is before measurement but we simply do not know which state of the mixture it exists in - however it is in some eigenstate 100% for sure.

Thanks
Bill
 
  • #156


bhobba said:
it can't have a definite value before observation unless something else comes into play
Thanks
Bill

which, "it" ?
 
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  • #157


Ken G said:
The two issues are so tightly connected there's no reason to separate them into two different problems. The "why we don't see superpositions" problem and the "why we don't see unitary evolution" problem is the same problem, called the measurement problem. It's a disconnect between the postulates of the theory, and what we see. The fundamental postulate is that time evolution is unitary, which says superpositions evolve into superpositions, or into mixed states if you project onto a subspace of a system interacting with its environment. But we don't see either superpositions or mixed states for individual particles-- we see definite outcomes.

My point is that we don't really know what it would mean to see a superposition, or a mixed state. To be able to reason from observations to what that implies about reality, you have to be able to do counterfactual reasoning: If X were true, then we would see Y. We don't see Y, so X is not true. What would we see if there were superpositions? It's hard to know.
 
  • #158


Ken G said:
The "must" means, at the least, "in order to not have threads about why we don't understand quantum mechanics", and at the most, to obtain the next great theory of physics.
It's not important if you don't mind having threads like this one, and you don't mind a theory that cannot (yet) be merged with gravity, or be applied to arbitrary energy scales.

It's vaguely possible that the philosophical problems about the meaning of quantum mechanics might come into play in resolving the problems with quantum gravity, but I don't see any reason to think so.

You claimed, above, that what was strange was that you could get 100% certainty about what one particle would do based on observations of another particle. But that's not strange at all, that's Bertlmann's socks.

My point was that there is NOT anything weird about correlations, if they have a "Bertlmann's socks" type explanation. But quantum correlations aren't like Bertlmann's socks. In particular, Bertlmann's socks don't violate Bell's inequalities.
 
  • #159


stevendaryl said:
But if Bob happens to be measuring the spin of the other particle along the same axis A, he's guaranteed to get the same value as Alice. That correlation isn't a matter of "Alice's measurement disturbed the system being measured".

It's the things about quantum mechanics that are certain that makes it mysterious, not the things that are uncertain.

My point was that there is NOT anything weird about correlations, if they have a "Bertlmann's socks" type explanation. But quantum correlations aren't like Bertlmann's socks. In particular, Bertlmann's socks don't violate Bell's inequalities.
I know, that's why the weirdness does not appear when outcomes are certain. Bertlmann's socks are certain, Bell violations are all examples of indeterminacy. Classical physics doesn't have indeterminacy, and it doesn't have Bell violations-- that's what's weird about quantum mechanics. Since the measurements are still definite, but the mathematical description involves indeterminacy, this disconnect is called the measurement problem.
 
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  • #160
I believe I "understand" QM.

I rely on this august group of physicists to disabuse me of my illusion.

I begin by assuming the two most accurate and proven theories in physics are correct; QM and general relativity.

1. Relativity says that we exist in a 4 dimensional universe that we apprehend as a 3 dimensional universe. Einstein believed that this was an "illusion."

2. It is the force of electromagnetism that causes us to think the universe is 3 dimensional. This is the force that defines matter as we experience it in its various forms. It is also the force that defines time. The constant speed of C is what defines how much time elapses for us depending on our own speed through space and/or the gravitational force we are subjected to. It is also the force that provides time with its arrow. The sum of the speed through space and the speed through time must always equal C. As C is the limit of speed through space, it is impossible for speed through time to be negative without requiring speed through space to exceed C.

3. Essentially, we live in a 3 dimensional subset of the 4 dimensional universe that is "knocked down" by the reality of electromagnetism, which we are made of and live under.

4. The Schrödinger equation describes particles as waves that permeate all of space-time, i.e. existing in a 4 dimensional "block universe" that we find particularly difficult to conceptualize.

5. Decoherence occurs when these waves encounter electromagnetic forces that compel them to appear as particles in that particular 3 dimensional subset. Information theory has shown that additional dimensions add enormously to the amount of information that can be held by any bit. This is why waves in 4 dimensions appear to us in 3 dimensions as particles. The old "Flatland" metaphor illustrates this perfectly.

6. "Measurement" is simply one way of forcing these waves to decohere. Consciousness has nothing whatsoever to do with it. We rely on the force of electromagnetism for any measurement we make.

7. Once decohered, these waves appear to us as particles in our 3 dimensional subset universe. They continue to behave as waves in the 4 dimensional block universe.

8. The wave nature of matter is necessitated by the relativity of simultaneity. Each observer's reality is equally valid, even though it doesn't agree with other observers traveling through space at a different speed or subjected to different gravitational forces. This truth would simply be impossible if matter were particles. Waves allow matter to appear anywhere in the 4 dimensional block universe where it happens to get decohered through the force of electromagnetism.

9. This is also why quantum indeterminacy is a foregone conclusion once one accepts the relativity of simultinaity.

Bottom line, if you believe relativity is correct, quantum "weirdness" is a necessary result. Without wave-particle duality and quantum indeterminacy, relativity would have to be wrong. With it, it works like a charm.

Please help me understand why the above has been proven to be incorrect.

I'm searching for experimentally proven facts to blow this "understanding" out of the water!
 
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  • #161


I subscribe to the info interpretation of QM, so for me there is no such equivalence between "why we don't see unitary evolution" and "the measurement problem". The measurement problem is a result of (as Zeilinger puts it) the conservation of the irreducible bit of information that an individual system is. And your (Ken G) remark "The fundamental postulate is that time evolution is unitary, which says superpositions evolve into superpositions, or into mixed states if you project onto a subspace of a system interacting with its environment. But we don't see either superpositions or mixed states for individual particles-- we see definite outcomes.", come on, QM is not about the individual system. Yes, physics is, but the theory of QM (and of course its measurement problem also) only accounts for statistically relevant sets of measurements, not individual systems.

You're treading dangerously close to the worst QM interpretation in history, the spurious idea about conciusness having some role in things.
 
  • #162


In the information interpretation of QM the individual system is a "bit" of information (actually several bits over several components of the description).

QM is a theory which describes statistically relevant sets of observations of individual systems. Therefore QM describes a system as a "set" of information based upon a description.

The irrational process(which could also be called a non-unitary process) in the measurement problem results from a change in the preparation of the system (where the change in preparation may be an evolution of the state or a change in the preparation encountered by the system due to its movement).

Any change in preparation results in a demand for new information about the system because the new preparation implies it, a measurement (and it is important to distinguish this as an "in principle" measurement because no one has to actually observe anything).

Due to the conservation of the irriducible bit of information that the individual system is, only so much information can the system be. The system becomes the information demanded by the new preparation.

The rest is irrational, and yes this is a problem for physicists who would wish to explain away all of existence rationally, but for those of us whom enjoy the indeterministic side of life it is not a problem but rather a fair compromise with existence.
 
  • #163


al onestone said:
QM is not about the individual system. Yes, physics is, but the theory of QM (and of course its measurement problem also) only accounts for statistically relevant sets of measurements, not individual systems.
I agree, but then I favor the Copenhagen interpretation, which says the same thing ("there is no quantum world"). But the key point is, this is not a statement about quantum mechanics, it is a subjective choice about how to interpret quantum mechanics. I don't take a rationalistic perspective that physics is trying to describe reality as it actually is, but those who do must seem an interpretation where quantum mechanics does describe a closed system.
You're treading dangerously close to the worst QM interpretation in history, the spurious idea about conciusness having some role in things.
There's nothing spurious about that idea unless it is mishandled (as it often is). It is true that there seems to be little benefit in attributing a dynamical role to consciousness in the equations of physics, but an attempt to do that is rather missing the point of the role of consciousness. The role of consciousness is simply that physics is done by physicists, who are conscious beings, and who invariably invoke their consciousness when they do physics. Hence, the role of consciousness is quite demonstable, the only question is when do we need to think about it and and when can we get away with ignoring it. The latter answer is "virtually always", but quantum mechanics may be one of the places where we begin to encounter problems ignoring it. (Especially for those who take an informational interpretation-- for where is the only place that information is actually a demonstrable concept?)
 
  • #164


josephwouk said:
I'm searching for experimentally proven facts to blow this "understanding" out of the water!
Here's one: relativity was laid out decades before quantum mechanics, and was regarded as a complete theory in the absence of any quantum indeterminacy. What's more, the person most responsible for formulating relativity (Einstein) was also deeply involved in the discovery of wave/particle duality (his Nobel prize was on the photoelectric effect, not relativity), yet this person never accepted wave/particle duality or quantum indeterminacy as fundamental truths of nature, at the level of the fundamental truths of relativity. Today, most physicists take the opposite view, that quantum intedeterminacy is a more fundamental truth than the tenets of general relativity, yet even so, the two are not viewed as mutually necessary, and indeed are generally viewed as contradictory at the Planck scale, though no observations exist at that scale.
 
  • #165


What I wonder about is how the founders of QM figured out that the mathematics we use in QM (operators, bras, kets etc.) was the right thing to use. They didn't just pull it out of thin air, they must have reasoned their way to at least some of it, eg. Schrodinger didn't just get out a pen and write down HΨ=iℏddtΨ out of nowhere. Why isn't that considered "understanding" it?

Post #5 in this thread...

https://www.physicsforums.com/showthread.php?p=418069#post418069

...has a great explanation on the kind of thing that can be explained as the "origin" of QM postulates (or at least the Schrodinger equation).

All of the postulates follow from a large number of counterintuitive experimental results (for example, double slit experiment) and efforts to model experimental results (for example, Bohr's model). Obviously, since they're postulates, they can't be derived directly, only assumed because they explain experimental results.

In many ways, all of science is a large act in performing the logical fallacy of affirming the consequent, but in a good way.
 

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