I’ve seen variants of MWI that were explicitly MWI, so what you’re calling MWI would be straight Everettian MWI. But really, here, I’m asking: “Does this theory have multiple worlds in it?” I care significantly less what it’s called.
For instance, Consistent Histories looks at things quite differently, but if you ask the critical questions of it, it looks like it has many worlds in it. It primes you to zero in on one of them, but if you’re going to stick with the wavefunction being real then the histories you don’t observe are going to be equally real, just less relevant. On the other hand if you say it’s just a trick for finding the probabilities, well, then it’s just a formalized ontological collapse and not MWI. I don’t see any middle ground or ground off to the side here (aside from throwing your hands in the air and saying you don’t know, which is perfectly legitimate but it isn’t an interpretation).
The associations of the hermitian operators corresponding to observable quantities are very type-2. We should feel about as justified using them as using the Born rule.
The point of mentioning objective collapse in the last 2 paragraphs was as a reference point for the non-equality of type-2 postulates. I know it’s terrible, and you know it’s terrible—that’s the point.
But really, here, I’m asking: “Does this theory have multiple worlds in it?” I care significantly less what it’s called
Right- in consistent histories there is 1 world. When you make a measurement, you get one answer. In ensemble quantum mechanics there is 1 world. Remember- the creators of consistent histories (Hartle, for instance) consider it a formalized and clarified copenhagen variant (though inspired by many worlds). Maybe think about it like Bohmian mechanics- the “world” that the Bohmian particle actually sits in is the ‘real’ one. Similarly, in consistent histories, the answer you get picks out a set of projection operators as “real.”
Side question- do you know a many worlds variant (in the sense of more than one world) that makes explicit what its “type 2” postulate is? The only variant I know of is many minds, which I find sort of abhorrent and disregard out of hand. The reason I insist that “many worlds” is incomplete is that the only formalized version I know is Everettian many worlds (which we both seem to agree IS incomplete).
The associations of the hermitian operators corresponding to observable quantities are very type-2.
But also type 1, because it defines the system (hermitian operators on a Hilbert space). What would you consider the type 2 postulates of Newtonian mechanics? What would you consider the type 2 postulates of GR?
In that case, Consistent Histories is both not WMI and I didn’t say it was, because it doesn’t consider the wavefunction fully real in its own right (there were two criteria, not just one, in that sentence)*. Just as Bohm isn’t, on the same grounds.
Type 1 vs type 2: Normally we don’t even talk about these types—if it were a matter of discussion, we wouldn’t be using these terms! With the observables, using them in the theory is type 1. Associating each one to a part of the world we experience is type 2.
As for the incompleteness of Everett, I hold that you can deduce that the Born Rule is one possible way of finding sapience within wavefunctions. I am not at all sure that you can prove that there aren’t others, so barring such a proof, a postulate is necessary to exclude them—“The way of getting to a perceivable world from this theory is… THIS one, not any others.”
ETA: and in this case Consistent Histories deserves every bit of scorn that Eliezer heaped on Copenhagen in the ‘what does it have to do, kill a puppy’ rant.
I’ve seen variants of MWI that were explicitly MWI, so what you’re calling MWI would be straight Everettian MWI. But really, here, I’m asking: “Does this theory have multiple worlds in it?” I care significantly less what it’s called.
For instance, Consistent Histories looks at things quite differently, but if you ask the critical questions of it, it looks like it has many worlds in it. It primes you to zero in on one of them, but if you’re going to stick with the wavefunction being real then the histories you don’t observe are going to be equally real, just less relevant. On the other hand if you say it’s just a trick for finding the probabilities, well, then it’s just a formalized ontological collapse and not MWI. I don’t see any middle ground or ground off to the side here (aside from throwing your hands in the air and saying you don’t know, which is perfectly legitimate but it isn’t an interpretation).
The associations of the hermitian operators corresponding to observable quantities are very type-2. We should feel about as justified using them as using the Born rule.
The point of mentioning objective collapse in the last 2 paragraphs was as a reference point for the non-equality of type-2 postulates. I know it’s terrible, and you know it’s terrible—that’s the point.
Right- in consistent histories there is 1 world. When you make a measurement, you get one answer. In ensemble quantum mechanics there is 1 world. Remember- the creators of consistent histories (Hartle, for instance) consider it a formalized and clarified copenhagen variant (though inspired by many worlds). Maybe think about it like Bohmian mechanics- the “world” that the Bohmian particle actually sits in is the ‘real’ one. Similarly, in consistent histories, the answer you get picks out a set of projection operators as “real.”
Side question- do you know a many worlds variant (in the sense of more than one world) that makes explicit what its “type 2” postulate is? The only variant I know of is many minds, which I find sort of abhorrent and disregard out of hand. The reason I insist that “many worlds” is incomplete is that the only formalized version I know is Everettian many worlds (which we both seem to agree IS incomplete).
But also type 1, because it defines the system (hermitian operators on a Hilbert space). What would you consider the type 2 postulates of Newtonian mechanics? What would you consider the type 2 postulates of GR?
In that case, Consistent Histories is both not WMI and I didn’t say it was, because it doesn’t consider the wavefunction fully real in its own right (there were two criteria, not just one, in that sentence)*. Just as Bohm isn’t, on the same grounds.
Type 1 vs type 2: Normally we don’t even talk about these types—if it were a matter of discussion, we wouldn’t be using these terms! With the observables, using them in the theory is type 1. Associating each one to a part of the world we experience is type 2.
As for the incompleteness of Everett, I hold that you can deduce that the Born Rule is one possible way of finding sapience within wavefunctions. I am not at all sure that you can prove that there aren’t others, so barring such a proof, a postulate is necessary to exclude them—“The way of getting to a perceivable world from this theory is… THIS one, not any others.”
ETA: and in this case Consistent Histories deserves every bit of scorn that Eliezer heaped on Copenhagen in the ‘what does it have to do, kill a puppy’ rant.