Sidney Coleman's opinion on interpretation in his Dirac lecture

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  • #31
martinbn said:
Ok, so for you an interpretation doesn't have a clear ontology unless the state of the systems is ontological (whether if is #\psi## or something else). Is that right?
Yes, you can put it this way.
 
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  • #32
Demystifier said:
I mean this thread, post #25.
Ah, didn't see it after the edit.
Demystifier said:
The beable of an interpretation is the thing that physically exists even when it is not measured. For example, when you say that particle exists even when it is not measured, then particle is supposed to be the beable in your interpretation. However, the problem with your interpretation is that your beable is not represented by a mathematical object. In particular, it cannot be a wave function, because an entangled 2-particle wave function does not represent a single particle. The beable λ must be represented by a mathematical object, otherwise it is not well defined.
I don't understand what the objection is. If you have an entangled system why should the subsystems be represented mathmatically. They are not even well-defined. One can only loosly walk about the subsystems.
 
  • #33
martinbn said:
This is hard to understand. What does it mean for the physical systems not to exist at all times? If they don't exist at a given time, then don't we just have an empty space-time? Why would they start to exist later on?

I can understand what it means for the physical systems not to be fundamental. I am strugling with the non-existence.
Within non-relativistic quantum mechanics, as you say, a tension arises between these two concepts because spacetime is assumed to be classical. Ultimately, if the gravitational field were inherently quantum and we interpreted it in the same way, there would also be no instants in time when the system doesn't exist. That is, what would exist are transitions between specific configurations of all degrees of freedom, including the gravitational field/spacetime. Indeed, the relational interpretation arose from Rovelli's earlier work on loop quantum gravity.

Lucas.
 
  • #34
martinbn said:
Ah, didn't see it after the edit.

I don't understand what the objection is. If you have an entangled system why should the subsystems be represented mathmatically. They are not even well-defined. One can only loosly walk about the subsystems.
Fine, but does it mean that the subsystem is not ontological, i.e., that the subsystem does not exist in a strict sense? For example, if the system consists of a proton and an electron in an entangled state, would you say that the electron does not exist?
 
  • #35
Demystifier said:
Fine, but does it mean that the subsystem is not ontological, i.e., that the subsystem does not exist in a strict sense? For example, if the system consists of a proton and an electron in an entangled state, would you say that the electron does not exist?
No, i wouldn't say that they don't exist.
 
  • #36
martinbn said:
If you have an entangled system why should the subsystems be represented mathmatically. They are not even well-defined. One can only loosly walk about the subsystems.
Of course they are well-defined. In a long distance Bell experiment, Alice sees the effects of one of the entangled photons, not even knowing whether there is an entangled partner somewhere. For her, the only system is the subsystem, and it has all the properties a single photon has.

This is the typical situation everywhere. Most systems in the world are entangled, since the Schrödinger equation entangles them. Even should they be for one moment disentangled, this is destroyed by interactions in the next moment. But we only care about the subsystem our attention is on (which may be different for different observers or agents), and it has properties as well-defined as one can expect from a quantum system.
 
  • #37
A. Neumaier said:
Of course they are well-defined. In a long distance Bell experiment, Alice sees the effects of one of the entangled photons, not even knowing whether there is an entangled partner somewhere. For her, the only system is the subsystem, and it has all the properties a single photon has.

This is the typical situation everywhere. Most systems in the world are entangled, since the Schrödinger equation entangles them. Even should they be for one moment disentangled, this is destroyed by interactions in the next moment. But we only care about the subsystem our attention is on (which may be different for different observers or agents), and it has properties as well-defined as one can expect from a quantum system.
Then the problem @Demystifier discribes doesn't exist.
 
  • #38
martinbn said:
No, i wouldn't say that they don't exist.
So you would say that they exist, but can't be represented mathematically, right? The Bell's analysis then can't be applied to them, because the Bell theorem assumes that all ontological stuff can be represented by some mathematical object ##\lambda##. That's how the Bell's conclusion, that there must be some non-local action at a distance, can be avoided: the Bell's theorem is a mathematical theorem, so if there is some physical stuff not represented by mathematics, the theorem does not apply to it. That's a legitimate position, but I find it problematic. Nevertheless, it would help me understand you if you could confirm that this, more or less, is your position.
 
  • #39
martinbn said:
Then the problem @Demystifier discribes doesn't exist.
Right, it doesn't exist in the Neumaier's interpretation, but it exists in your interpretation.
 
  • #40
Demystifier said:
So you would say that they exist, but can't be represented mathematically, right? The Bell's analysis then can't be applied to them, because the Bell theorem assumes that all ontological stuff can be represented by some mathematical object ##\lambda##. That's how the Bell's conclusion, that there must be some non-local action at a distance, can be avoided: the Bell's theorem is a mathematical theorem, so if there is some physical stuff not represented by mathematics, the theorem does not apply to it. That's a legitimate position, but I find it problematic. Nevertheless, it would help me understand you if you could confirm that this, more or less, is your position.
I thought we were talking about the ontology of RQM. How did it turn to Bell's theorem and nonlocality!
 
  • #41
Demystifier said:
Right, it doesn't exist in the Neumaier's interpretation, but it exists in your interpretation.
What interpretation of mine! Aren't we talking about RQM!
 
  • #42
We are talking about the Coleman's interpretation (which is not RQM), for which you said that you find convincing, so I thought that's your interpretation too. For any interpretation, one of the most important questions is how it interprets the Bell theorem.
 
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  • #43
Demystifier said:
We are talking about the Coleman's interpretation (which is not RQM), for which you said that you find convincing, so I thought that's your interpretation too. For any interpretation, one of the most important questions is how it interprets the Bell theorem.
No, i said that i find that particular argument convincing (Mott's from 1929), which is interpretation indipendent. Coleman's interpretation is some version of MWI.
 
  • #44
martinbn said:
No, i said that i find that particular argument convincing (Mott's from 1929), which is interpretation indipendent.
Coleman's version of Mott's argument just uses a self-adjoint "straight line"/"linearity" operator L and the corresponding spectral version of Born's rule.

I don't think that this is an interpretation independent argument, because it doesn't directly apply to MWI or BM.

martinbn said:
Coleman's interpretation is some version of MWI.
Whether Coleman's opinion really tends towards MWI is part of my initial question. My impression after following the discussion here and reading the corresponding sections is rather that Coleman tends towards a mix between Mott and Zurek. And Zurek in particular has always been pretty ambiguous with respect to MWI, which Coleman seems to mirror a bit.
 

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