More evidence that the wavefunction is ontologically real?

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  • #2
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The paper makes no sense at all as long as the concept of "measurement" is not precisely dynamically defined within quantum theory. These are just words with no precise meaning. Of course this what physicists do at the present time. Extraordinary claims need extraordinary proofs.
 
  • #3
jfizzix
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Apparently, if we say that reality is objectively defined, we can ask whether or not quantum states are objectively defined as well.

In particular, if the state of all information in reality pertaining to a quantum system is given by some set of variables [itex]\lambda[/itex], we can ask whether the quantum state [itex]|\psi\rangle[/itex] is uniquely defined by [itex]\lambda[/itex].

It's a bit tricky, but what they try to show is that different states [itex]|\psi\rangle[/itex] correspond to different (disjoint) sets of [itex]\lambda[/itex].

Since they appear to affirm this experimentally (within certain tolerances), it would mean that if one wants to consider the information encoding reality as objective, then one must also consider the quantum state of a system as objectively determined, and not something particular to the observer's state of knowledge.

Pretty awesome work, I must say!
 
  • #4
jfizzix
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I would need to go through the paper in more detail, but if I've read it correctly, this seems... profoundly significant.
 
  • #6
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Here is a free link:
http://arxiv.org/pdf/1412.6213v2.pdf

Note what it says:
'Assuming that some underlying reality exists, our results strengthen the view that the entire wavefunction should be real'

Its the same thing as the PBR theorem - its simply that if you assume some kind of reality in the first place, even in a weak sort of way, the wave function is in a stronger sense real. Interesting and likely quite important, but that assumption of reality, even in a weak sense, is precisely what many interpretations reject.

For example it doesn't apply to the ignorance ensemble interpretation - and quite a few others.

Thanks
Bill
 
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  • #7
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So lets assume the wave function is real. does that mean that qm needs no further interpretations? (consciousness, many worlds, etc)
 
  • #8
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So lets assume the wave function is real. does that mean that qm needs no further interpretations? (consciousness, many worlds, etc)

No.

It changes none of the various interpretations where the wavefunction is real eg BM, MW, nelson stochastics, primary state diffusion etc.

Thanks
Bill
 
  • #9
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One difference between this paper and PBR is that these authors do not rely on the assumption of preparation independence. They write:
Crucially, our theoretical derivation and conclusions do not require any assumptions beyond the ontological models framework, such as preparation independence, symmetry or continuity...
What is confusing (to me) is that the authors appear to argue that this assumption of preparation independence used by the PBR theorem is analogous to Bell's local causality. They write:
For example, Pusey et al. assume that independently-prepared systems have independent physical states. This requirement has been challenged as being analogous to Bell's local causality, which is already ruled out by Bell's theorem.
I still don't understand this. I didn't think that preparation independence and local causality are analogous? Regardless, the fact that one can narrow down the available "realistic" interpretations that are still viable is still progress.
 
  • #10
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Hello,

What is the meaning to be "ontologically real" in the framework of the physics ?

Patrick
 
  • #11
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What is the meaning to be "ontologically real" in the framework of the physics ?
That the wave function is a mathematical entity/map that represents/refers to something that actually exists in the world, independently of any observer or agent.
 
  • #12
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That the wave function is a mathematical entity/map that represents/refers to something that actually exists in the world, independently of any observer or agent.

The wavefunction is simply the representation of the state in the position basis. The state is the key thing.

To understand the issue see post 137 of the following:
https://www.physicsforums.com/threads/the-born-rule-in-many-worlds.763139/page-7

The state and its physical interpretation by the Born rule is in fact derivable from the operator formalism of QM - that's the import of Gleason's theorem the modern version of which the above link proved. This raises the question of is it real or simply something required by the math. Gleason's theorem suggests it's simply a mathematical requirement - but opinions vary.

Thanks
Bill
 
  • #13
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Wave functions are well described using complex numbers

Complex numbers are like a two part epoxy, having A and B components

Would the reality of the blobular blobulous wave function imply, that at some nano scoptic fempto scopic Planckoscoptic scale, that there actually is some two-component field, of which particles are storm like disturbances, which whirlwinds obey the SWE ?
 
  • #14
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Would the reality of the blobular blobulous wave function imply, that at some nano scoptic fempto scopic Planckoscoptic scale, that there actually is some two-component field, of which particles are storm like disturbances, which whirlwinds obey the SWE ?

Sorry - but that's utter gibberish.

The reason we have complex numbers is the need for continuous transformations between pure states:
http://arxiv.org/pdf/quant-ph/0101012.pdf

Thanks
Bill
 
  • #15
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Sorry - but that's utter gibberish.

The reason we have complex numbers is the need for continuous transformations between pure states:
http://arxiv.org/pdf/quant-ph/0101012.pdf

Thanks
Bill
Why do complex numbers accurately model real experimental results?

If the wave function is real, and if a wave function is a complex valued field, then something corresponding to complex numbers would be real too, yes?
 
  • #16
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Why do complex numbers accurately model real experimental results?

Why not? Exactly what limits the mathematical objects that can be used in physical models?

Here is the reason they are required in QM.

Suppose we have a system in 2 states represented by the vectors [0,1] and [1,0]. These states are called pure. These can be randomly presented for observation and you get the vector [p1, p2] where p1 and p2 give the probabilities of observing the pure state. Such states are called mixed. Probability theory is basically the theory of such mixed states. Now consider the matrix A that say after 1 second transforms one pure state to another with rows [0, 1] and [1, 0]. But what happens when A is applied for half a second. Well that would be a matrix U^2 = A. You can work this out and low and behold U is complex. Apply it to a pure state and you get a complex vector. This is something new. Its not a mixed state - but you are forced to it if you want continuous transformations between pure states.

QM is basically the theory that makes sense of such weird complex pure states (which are required to have continuous transformations between pure states) - it does so by means of the so called Born rule.

If the wave function is real, and if a wave function is a complex valued field, then something corresponding to complex numbers would be real too, yes?

You do realise that complex numbers are specified by two real numbers? If the wave-function is real then its specified by two real numbers. But that view isn't required to understand what's going on. QM is a mathematical model - any mathematical entity can appear in such models - complex numbers, Grassmann numbers, tensors - the list is endless.

The mathematical objects of a model aren't real - the reality lies in the correspondence rules of the model. For example show me a negative number of apples - but if you have borrowed some apples from a friend and need to return them that would be a reasonable model.

Thanks
Bill
 
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  • #17
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I think there is nothing problematic with giving the wave function the status of reality. Because there exists, anyway, some real values which correspond to it.

The wave function is always the result of a preparation procedure. And a preparation procedure is a measurement. We measure something, so the measurement result exists. Really, without any doubt really. And this measurement result, together with the history of the experiment itself, which has also happened really, is what defines the wave function.

In de Broglie-Bohm theory, this dependence is explicit. We have a wave function of the whole preparation procedure, [itex]\psi(q_{system},q_{device},t)[/itex], and to obtain the effective wave function of the system, we need the trajetory of the measurement device: [itex]\psi(q_{system},t) = \psi(q_{system},q_{device}(t),t)[/itex].
 
  • #18
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I think there is nothing problematic with giving the wave function the status of reality.

Of course not.

There are many interpretations where its real.

Thanks
Bill
 
  • #19
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Suppose we have a system in 2 states represented by the vectors [0,1] and [1,0]. These states are called pure. These can be randomly presented for observation and you get the vector [p1, p2] where p1 and p2 give the probabilities of observing the pure state. Such states are called mixed. Probability theory is basically the theory of such mixed states. Now consider the matrix A that say after 1 second transforms one pure state to another with rows [0, 1] and [1, 0]. But what happens when A is applied for half a second. Well that would be a matrix U^2 = A. You can work this out and low and behold U is complex. Apply it to a pure state and you get a complex vector. This is something new. Its not a mixed state - but you are forced to it if you want continuous transformations between pure states.

Whoa, finally an explanation that I can understand. I kept reading this thing in the usually linked arxiv articles and not getting it. Are there any lectures or books you can suggest that explain C*-algebras for QM to non-mathematicians? I mean physicists trained in a standard way, no math gibberish (or yes, but explained from scratch).
 
  • #20
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Are there any lectures or books you can suggest that explain C*-algebras for QM to non-mathematicians?

No - its very hard even for trained mathematicians. Its an extremely mathematically advanced formulation of QM.

Thanks
Bill
 
  • #21
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I think there is nothing problematic with giving the wave function the status of reality. Because there exists, anyway, some real values which correspond to it.

[....]

In de Broglie-Bohm theory, this dependence is explicit

But in Bohm, given the ontological nature of the WF it's hard to see how you avoid infinite Many Worlds with 1 special particle world.
 
  • #22
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But in Bohm, given the ontological nature of the WF it's hard to see how you avoid infinite Many Worlds with 1 special particle world.
Sorry, but for me it is extremely difficult to see how one can obtain infinite many worlds out of a function defined on imaginable worlds.

Say, a function on all imaginable worlds can easily exist in my mind - as a collection about ideas about all such worlds. My mind really exists. Thus, the ideas about all these worlds also exists. But all these other worlds do not exist. Even if this example may be slightly artificial, but the conceptual problem that a function on some space of objects can easily exist without the objects
Of course not.
There are many interpretations where its real.
Ok, let's make the statement a little bit more nontrivial: It is not even a problem for an epistemic interpretation. Because one has to distinguish the epistemic interpretation of the wave function of the universe from the interpretation of the wave function of the particular subsystem.

The wave function of the whole system, which prepares the particular system, is in itself not prepared - this would give an infinite regress. Thus, what we know about it? Nothing. And it is this nothingness which suggests that this unprepared wave function is epistemic. But, when, we compute the effective wave function of the subsystem, by using some element of reality - the trajectory of the measurement device. Thus, the effective wave function of the subsystem depends on elements of reality. Thus, it is not purely epistemic, but at least partially ontic.
 
  • #23
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.. It just happened that we have 2 measured/observed realities and each can be expressed in variety of ways. Some my favor that wavefunction behavior as a first order. Hence, the fundamental reality. But we really don't know except that we can see things to be this way. Nature is pretty deceiving; bizzare and it's not always what it seems or look like based on macro world idealization and i find QM to be very direct.


http://physics.stackexchange.com/questions/154431/are-wave-functions-real-physical-objects
 
  • #24
zonde
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I think there is nothing problematic with giving the wave function the status of reality.
But there are conjugate variables. Remember EPR paradox?

Because there exists, anyway, some real values which correspond to it.
There are only probabilities. Probabilities are not real.
 
  • #25
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There are only probabilities. Probabilities are not real.
Maybe in a classical continuous view but we don't have or can't proved that.. In general QM sense. The x always goes to infinite, states of which each is independent to one another -- individual states.
 
  • #26
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It seems to me that I have, in the past, been professorially chastised for questioning what quantum physics implies about "reality" at the fundamental level, as well as when I suggested that it seems in many ways that the only thing "real" about the quantum state of a physical system is the information that describes it. Despite that, it appears that this thread demands that those issues to be addressed.

First off, what does it mean for something to be "ontologically real"? The definition of "ontological" (according to i.word.com) is :"relating to or based upon being or existence." I interpret that to mean that it's something that actually "exists", in a substantive manner.

I think there is nothing problematic with giving the wave function the status of reality. Because there exists, anyway, some real values which correspond to it.

But, to what do the values correspond? What is it that actually "exists" that the values describe?

...the wave function is a mathematical entity/map that represents/refers to something that actually exists in the world, independently of any observer or agent.

The mathematical objects of a model aren't real - the reality lies in the correspondence rules of the model. For example show me a negative number of apples - but if you have borrowed some apples from a friend and need to return them that would be a reasonable model.

Yet, negative numbers don't actually "exist", in a substantive manner. For that matter, neither do positive numbers, nor arithmetic functions. They are mathematical constructs... abstract ideas. They have no substantive form.

Apparently, if we say that reality is objectively defined, we can ask whether or not quantum states are objectively defined as well.
......
Since they appear to affirm this experimentally (within certain tolerances), it would mean that if one wants to consider the information encoding reality as objective, then one must also consider the quantum state of a system as objectively determined, and not something particular to the observer's state of knowledge.

So, this leaves me with the question... Is the information content of the quantum state what is objectively "real". Is it, in fact, all that is "real"?
 
  • #27
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Measurements can only detect eigenvalue, so any problems beyond eigenvalue of the wavefunction is hard to answer. If wavefunction is ontologically real or not is one of such questions.
 
  • #28
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In the double slit experiment, the detector collapse the wave function in Copenhagen. If it doesn't collapse, then it automatically forms Many Worlds? or does the wave function simply vanish or no effect on this world (if no collapse occurs just for sake of discussions)?
 
  • #29
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The wave function of the whole system, which prepares the particular system, is in itself not prepared - this would give an infinite regress. Thus, what we know about it? Nothing. And it is this nothingness which suggests that this unprepared wave function is epistemic. But, when, we compute the effective wave function of the subsystem, by using some element of reality - the trajectory of the measurement device. Thus, the effective wave function of the subsystem depends on elements of reality. Thus, it is not purely epistemic, but at least partially ontic.

Sorry - but I don't get that at all eg why even the concept of 'prepared' is applicable to wave-function needs detailing before you can even introduce it in that context. In modern times state and preparation procedure are pretty much synonymous but that requires detailing of what it is in the first place - which is very interpretation dependant. To me it looks like typical philosophical 'waffle' that basically makes my eyes roll back and I want to switch off. Philosophically its what Wittgenstein said: 'Whereof one cannot speak, thereof one must be silent'

We have all sorts of interpretations where the state (I dislike wavefunction because that gives the position basis a privileged role) has all sorts of statuses. The fact they are valid interpretations means you cant say, a priori, anything about the status of the state. Arguments like the above must have a flaw - but since I don't even understand it what that is beats me.

Thanks
Bill
 
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  • #30
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But in Bohm, given the ontological nature of the WF it's hard to see how you avoid infinite Many Worlds with 1 special particle world.

You are mixing concepts from interpretations as if they were the same interpretation. That is, and very obviously so, flawed logic.

Thanks
Bill
 

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