[lisper]

> It doesn’t mean, however, that there aren’t any initial conditions even prior to measurement.

This is the EPR argument.

> Bell’s inequality doesn’t negate this.

Bell shows that there is no measurement you can make, even in principle, that will give you the information you need to predict the outcome of a quantum experiment.

You can, if you wish, insist that those initial conditions exist notwithstanding our inability to measure them even in principle. But you could equally well insist that the outcomes of quantum experiments are determined by an invisible pink unicorn. Both hypotheses are equally unfalsifiable (if QM is correct).

I have actually coined the term IPU (Invisible Pink Unicorn) as an intentionally derisive description of hypothetical constructs that cannot be measured even in principle. Many QM interpretations contain IPUs. Bohmiam particle positions, for example, are an IPU.

[jostylr]

One thing to look at is how is the theory formulated. Standard QM seems to build its Hilbert space of wave functions from functions over R^3N. It has a Hamiltonian built out of the notions of that space. So configuration space seems pretty crucial. But configuration of what? If you say particles with positions do not exist, then what exactly is the relevance of this space? What is the primitive stuff whose behavior can be right or wrong from our perspective?

It is also odd to say that position cannot be measured. We can tell in an experiment whether something ended up over there or over here. It would be reasonable to then try to have a theory that correlates the position measurements with something that has a position. Now it is not necessarily the case that there has to be such a thing, but it seems like a reasonable first step.

We can even see trails of particles in cloud chambers and the like. Why is that an IPU?

I will grant that it does not have to be the case that the only possible explanation is that of particles with position. But it certainly seems like if there is such a theory (and, of course, there is), then it would seem reasonable to consider it as quite plausible.

It also helps to ask you what is real in your theory. Are wave functions real? They certainly can't be measured in their entirety. Are operators the real thing? We don't measure them, but rather get something close to their eigenvectors/eigenvalues. Are those real?

Many worlds is the closest version with nothing added, but even that requires some kind of mass density function to make explicit connection with our lived experience. While it doesn't add too much in the way of extra mathematical structure in the theory (integrate over the wave function in a certain way: https://arxiv.org/abs/0903.2211 ), the implication in terms of what it says reality is actually like certainly involves a heck of a lot of IPUs.

[lisper]

> If you say particles with positions do not exist, then what exactly is the relevance of this space?

That's a good question. The real answer is that no one actually knows. I think this is actually the biggest mystery in QM. But let me start with this, because I didn't make myself clear:

> It is also odd to say that position cannot be measured.

When I said that Bohmian positions are an IPU I did not intend that to mean that particle positions can't be measured. Obviously they can. The IPU-ness of Bohmian positions has to do with their ontological status, not their epistemic status. On Bohm's theory, a particle position considered along some axis is a real (in the mathematical sense) value, which is to say, it contains an infinite amount of information. But this information cannot be accessed in the same way that information stored in (say) a book can. I can open a book, even a book with an infinite number of pages, to any page and start reading it, and having read any page, I can go back and read that same page again. The information stored in Bohmian positions doesn't work that way. The laws of physics somehow conspire to hide all that information so that it can only be accessed serially and non-repeatably. The first time you measure a particle's position you get the most significant bits of its position. Those are then lost forever. You can never measure them again. The next time you measure a particle's position you get the next most significant bits of what that particle's position originally was, and so on. But you can never go back and do a second experiment to verify that the result you got for any of your measurements was actually correct and not a result of experimental error.

So the much-vaunted determinacy of Bohmian mechanics is not a reflection of the determinacy of the underlying metaphysical reality. It is really nothing more than a rhetorical trick. All the randomness is still there, it's just "pre-computed" and stored in particle positions in a way that it can only be accessed so that the world behaves exactly as if it were "really random" (whatever that means).

This same kind of trick is made manifest in a thought experiment [https://www.mathpages.com/rr/s9-07/9-07.htm] proposed by Kevin Brown. He points out that, if pi is normal (which is almost certainly is) then all of the results of all experiments ever conducted could be produced by a "cosmic Turing machine" computing the digits of pi. (See the two paragraphs beginning with "Even worse, there need be no simple rule of any kind relating the events of a deterministic universe.") Bohmian positions have exactly the same ontological status as the cosmic Turing machine. Only the window-dressing is different.

> It also helps to ask you what is real in your theory. Are wave functions real?

See http://blog.rongarret.info/2015/02/31-flavors-of-ontology.ht... for my answer to this.

> Many worlds ... involves a heck of a lot of IPUs.

Yep. That's why I'm not a big fan of the MWI either. See:

http://blog.rongarret.info/2019/07/the-trouble-with-many-wor...

[nobodyandproud]

And there it is.

We don’t know whether a non-local interpretation will lead to different, correct predictions.

One of the persistent hurdles is that gravity refuses to be folded into QM (or really, QCD).

Do you absolutely know whether hidden variable couldn’t be the missing factor?

Also—because I see you didn’t catch this—it’s possible Bell’s proof is incorrect because it assumes classical logic applies in QM.

In any case we’re done.

[lisper]

> We don’t know whether a non-local interpretation will lead to different, correct predictions.

Yes, we do. An interpretation cannot lead to different predictions. If it did, it would not be an interpretation, it would be a new theory.

> In any case we’re done.

Seems so.