I started a new thread since this was off-topic in the TEW thread.
I thought Böhm’s interpretation was completely non-relativistic.
Bohm’s original theory was a replacement for standard NRQM, yes. But since then people have found ways to do for (allegedly) relativistic quantum theories (e.g., multi-particle Dirac theory, QFT) what Bohm did for NRQM. Some of the extensions are controversial and/or ongoing research programs, but still.
A signal, or information, does have a meaning independent of human interpretation. It’s something that has a causal effect.
I can tell you’re not really up on the literature on quantum foundations or Bell in particular. People seriously interested in these issues use “signal” as a term of art referring specifically to the human activity of signalling (transmitting “information”), which is not coextensive with causal influences. Sending a superluminal signal requires some underlying causal influences that propagate superluminally, but the latter is not a sufficient condition for the former. The relevant causation must, for example, be sufficiently “controllable” that humans can harness it for their desired purposes. This distinction is important, because all the theorems proving that “relativistic” quantum theories are consistent with relativity actually only prove that those theories don’t support superluminal signaling – *not* that the theories don’t contain superluminal causation and not that they don’t require extra-relativistic spacetime structure.
In response to my claim that (even) orthodox QM requires such extra spacetime structure, you asked:
How so?
The collapse postulate. When a measurement occurs anywhere, the wave function describing (previously-entangled) degrees of freedom anywhere else in the universe changes *instantaneously*. And of course “instantaneously” is not a relativistically invariant concept.
Once again, I’m not sure how this is. I’m only a student, but I’ve been familiar with quantum field theory for a while, but the axioms (with a few modifications to use the Heisenberg picture instead of the Schrödinger, and to account for the infinitely many degrees of freedom) have seemed to work just fine. Perfectly Minkowski spacetime and all.
It is made to look that way by the fact that all you are ever asked to calculate in QFT courses is matrix elements (so you can calculate scattering cross sections and whatnot). But if you actually step back and think about the story the theory is telling for the evolution of the physical world over time, and what happens when somebody somewhere makes a measurement, and how other things have to evolve subsequently, you’ll realize that there’s no relevant difference between QFT and NRQM. They both require a collapse postulate to get the right answers, and formulating that precisely requires some un-relativistic concept of a dynamically privileged space-like hypersurface.
I believe many world myself (just to say), but because it has wavefunction collapse as an emergent phenomenon rather than something fundamental. Seems more parsimonious. But it’s just metaphysics, and is indistinguishable from Copenhagen empirically, so I don’t really argue it. And I’ve never seen it as “necessary” to relativistic QM.
Wavefunction collapse doesn’t “emerge” in MWI. Unless you put it back in by hand at the world-mind interface (i.e., unless you cheat).
In response to my claim that Bell’s theorem is not actually premised on “hidden variables” (popular belief to the contrary notwithstanding), you wrote:
This isn’t true.
That’s not much of an argument, so in response I’ll just say: “Yes, it is.” And: maybe you should go read some of Bell’s own papers. I’d recommend starting with “Bertlmann’s socks and the nature of reality” (conveniently reprinted in the book “Speakable and Unspeakable”). It is a brilliant paper. Nothing in the secondary Bell literature (and certainly not whatever textbook you got your information from) comes anywhere close. Pay special attention to footnote 10, where Bell states clearly that his “own first paper on this subject [his 1964 paper that first presented what is now known as Bell’s theorem] starts with a summary of the EPR argument from locality to determinstic hidden variables. But the commentators have almost universally reported that it begins with deterministic hidden variables.”
In regard to Bohmian Mechanics you wrote:
It is speculative because it postulates the existence of things that we have no evidence for. There are particles and pilot waves, and they are separate things. And the particles have a well-defined classical trajectory. If this is true, there should exist an experiment that confirms the pilot wave theory and at the same time contradicts quantum mechanics on some scale.
Actually we do have evidence that there are particles (think: spots on detector screens or tracks in bubble chambers), and evidence that the motion of the particles is somehow guided by a wave (think: all the little spots make an interference pattern as they accumulate). And by the way, according to Bohm’s theory, when you measure the position of a particle, what you “see” is the actual pre-measurement position of the particle. So people who think that these particle positions are somehow “hidden” or “metaphysical” or “unempirical” are just wrong. If anything, it’s the wave function that has that status. But I don’t see anybody complaining about the wave function in other theories. I don’t know what you mean by the word “classical” in the middle sentence. Yes, particles in Bohm’s theory follow trajectories. But they are certainly not the trajectories predicted by classical physics. As to the last sentence, it would be nice. But it’s of course fallacious to say that, in a situation that two different theories make the same predictions, one of them should be considered “verified” when its predictions are borne out, while the other should be dismissed a priori simply for making the same (empirically verified) predictions. It would be just as valid to say that orthodox QM should be dismissed until or unless it makes some prediction that is different from the predictions of Bohm’s theory. The point is, when two theories make the same predictions, and those predictions are correct, you can’t cite experiment directly as favoring either one. You’ll have to appeal to some other standards, e.g., clarity, seriousness, parsimony, etc. And if you do that, Bohm is going to win over orthodox QM hands down.
Anyway, if we’re going to mix relativity with QM (which has been successfully done), I may as well throw in some relativistic jargon and metaphysics. Everything has to be described from an observer’s point of view, an observer within the universe who obeys the laws of physics. We’ll call this observer Mufasa, because I’m sick of Anne and Bob.
I strongly disagree with your whole approach here. It’s fine to describe physical reality “from an observer’s point of view” – if you mean, for example, using some particular reference frame for defining coordinates and whatnot. But this is very different from giving up the whole attempt to describe physical reality and instead just tossing around symbols, one term from which eventually is supposed to correspond to some kind of subjective conscious experience for some particular subject.
Trying to talk about the actual events of both measurements as though from an omniscient observer whose observing powers violate relativity is meaningless, by contrast, since relativity and QM both teach us (albeit in different ways) that observers are bound to the laws of physics.
I think you misunderstand what relativity is all about. You seem to be confusing it with solipsism.