This article should really be called "Patching the argumentative flaw in the Sequences created by the Quantum Physics Sequence".
There's only one big thing wrong with that Sequence: the central factual claim is wrong. I don't mean the claim that the Many Worlds interpretation is correct; I mean the claim that the Many Worlds interpretation is obviously correct. I don't agree with the ontological claim either, but I especially don't agree with the epistemological claim. It's a strawman which reduces the quantum debate to Everett versus Bohr - well, it's not really Bohr, since Bohr didn't believe wavefunctions were physical entities. Everett versus Collapse, then.
I've complained about this from the beginning, simply because I've also studied the topic and profoundly disagree with Eliezer's assessment. What I would like to see discussed on this occasion is not the physics, but rather how to patch the arguments in the Sequences that depend on this wrong sub-argument. To my eyes, this is a highly visible flaw, but it's not a deep one. It's a detail, a bug. Surely it affects nothing of substance.
However, before I proceed, I'd better back up my criticism. So: consider the existence of single-world retrocausal interpretations of quantum mechanics, such as John Cramer's transactional interpretation, which is descended from Wheeler-Feynman absorber theory. There are no superpositions, only causal chains running forward in time and backward in time. The calculus of complex-valued probability amplitudes is supposed to arise from this.
The existence of the retrocausal tradition already shows that the debate has been represented incorrectly; it should at least be Everett versus Bohr versus Cramer. I would also argue that when you look at the details, many-worlds has no discernible edge over single-world retrocausality:
- Relativity isn't an issue for the transactional interpretation: causality forwards and causality backwards are both local, it's the existence of loops in time which create the appearance of nonlocality.
- Retrocausal interpretations don't have an exact derivation of the Born rule, but neither does many-worlds.
- Many-worlds finds hope of such a derivation in a property of the quantum formalism: the resemblance of density matrix entries to probabilities. But single-world retrocausality finds such hope too: the Born probabilities can be obtained from the product of ψ with ψ*, its complex conjugate, and ψ* is the time reverse of ψ.
- Loops in time just fundamentally bug some people, but splitting worlds have the same effect on others.
I am not especially an advocate of retrocausal interpretations. They are among the possibilities; they deserve consideration and they get it. Retrocausality may or may not be an element of the real explanation of why quantum mechanics works. Progress towards the discovery of the truth requires exploration on many fronts, that's happening, we'll get there eventually. I have focused on retrocausal interpretations here just because they offer the clearest evidence that the big picture offered by the Sequence is wrong.
It's hopeless to suggest rewriting the Sequence, I don't think that would be a good use of anyone's time. But what I would like to have, is a clear idea of the role that "the winner is ... Many Worlds!" plays in the overall flow of argument, in the great meta-sequence that is Less Wrong's foundational text; and I would also like to have a clear idea of how to patch the argument, so that it routes around this flaw.
In the wiki, it states that "Cleaning up the old confusion about QM is used to introduce basic issues in rationality (such as the technical version of Occam's Razor), epistemology, reductionism, naturalism, and philosophy of science." So there we have it - a synopsis of the function that this Sequence is supposed to perform. Perhaps we need a working group that will identify each of the individual arguments, and come up with a substitute for each one.
I've made a sketch to illustrate the simplest version of the problem.
Horizontal direction is spacelike, vertical direction is timelike. On the left we have a classically relativistic theory. Everything reduces to properties localized at individual space-time points (the blue dots), so there's no significance to a change of slicing (black vs pink), you're just grouping and re-grouping the dots differently.
On the right we have a quantum theory. There's a quantum state on each slice. A red circle around two dots indicates entanglement. How can we apply relativity here? Well, we can represent the same slicing differently in two coordinate systems, changing the space-time "tilt" of the slices (this is what I've illustrated). But if you adopt a truly different slicing, one that cuts across the original slicing (as pink cuts across black on the far left), you don't have a recipe for specifying what the quantum states on the new slices should be; because the quantum states on the original slicing do not decompose into properties located solely at single space-time points. The entanglement is made up of properties depending on two or more locations at once.
In practical QFT, the situation isn't usually this straightforward. E.g. perturbation theory is often introduced by talking about pure momentum states which notionally fill the whole of space-time, and not just a single slice. The Feynman diagrams which add up to give S-matrix elements then appear to represent space-time networks of point interactions between completely delocalized objects. I think it's just incredibly un-obvious how to turn that into a clear wavefunction-is-real ontology. What's the master wavefunction containing all the diagrammatic processes? What space is it defined over? Does this master wavefunction have a representation in terms of an instantaneous wavefunction on slicings that evolves over time? If it does, how do you change slicings? If it doesn't, what's the relation between the whole (master wavefunction) and the parts (history-superpositions as summed up in a Feynman diagram)?
And even that is all still rather elementary compared to the full complexity of what people do in QFT. So how to define relativistic MWI is a major challenge. I hope that the "simplest version of the problem", that I started with, conveys some of why this is so.
Entanglement is over mutually-timelike regions, not merely simultaneous moments, so your diagrams are misleading. Try redrawing your ellipses of entanglement so they're legal spacetime entities. If you redraw ALL of the entanglement this way, then it will transform just fine.