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.
Tim Maudlin developed an ingenious objection to the transactional interpretation which, to my knowledge, has not been adequately resolved as of yet. According to the TI, offer waves are sent forward in time from particle sources to absorbers. Each absorber responds by sending a confirmation wave backwards in time to the source. One of these transactions is selected with a probability given by the amplitude of the confirmation wave.
Here's Maudlin's objection: Suppose we have a beam splitter that can splits incoming beams of particles along two paths, call them a and b. On path a, at a distance l from the splitter, is a detector A. Let us suppose that a particle would cover the distance l in time t. There is another detector B that is initially also on path a, at a distance 2l from the source, behind A. If the detector A does not detect a particle within time t of the start of the experiment, then the detector B automatically swings onto path b, where it will also be at a distance 2l from the splitter.
Let's say the beam splitter sends half of the particles along path a and half along path b. This means that, for an individual particle, ordinary quantum mechanics predicts it will be detected by detector A with probability 1/2 (in which case B won't swing over to the other path), and with probability 1/2 B will swing over to path b and the particle will be detected at B. If the TI is to replicate these probabilities, then the confirmation waves sent backwards to the source from detectors A and B must have equal amplitude. But remember, a confirmation wave is sent back from an absorber only if an offer wave hits the absorber. So a confirmation wave will be sent backwards from detector B only if the offer wave from the source can reach B. But this is only possible if B has swung onto path b (otherwise the offer wave would be blocked by A), which in turn will only happen if the particle is not detected at A.
So if a confirmation wave is returned from detector B, then the particle must be detected at B. But if the QM probabilities are to be recovered according to the TI formulation, this confirmation wave's amplitude must be 1/2, since detections at B only occur half of the time. So the recipe for recovering probabilities in TI is incoherent. The confirmation wave returned from B both guarantees that the particle is detected at B and sets the probability of the particle being detected at B as 1/2. There have been a number of attempts to deal with this problem in the literature, but I haven't come across a wholly satisfactory attempt yet. The Wikipedia article on TI lists four articles that purportedly deal with this objection. I've read all of them, and don't think any of the proposed resolutions work.
I agree, more or less. For me, TI is significant as the best-known recent attempt to explain QM with retrocausality. But it has several concrete problems and this is one of them. When I liken the status of retrocausal interpretations to that of many-worlds, I have this in mind too.