LeandroMdO said:
Since one may prove, by construction, that there exist single world hidden variable theories (such as Aaronson's
flow model), it seems hard to justify speculation that single-world interpretations may be inconsistent. Either observers are describable within the mathematics of quantum mechanics (in which case they are also describable, or at least simulatable by the flow model or some other hidden variable model), or they aren't, in which case quantum mechanics itself is wrong regardless of interpretation.
Thanks for the link to Aaronson's paper. It's interesting, but I haven't completely studied it yet.
But the issue is not whether observers are describable within pure quantum mechanics, but whether observers with definite states are. In the quantum mechanics of a small number of particles, if a small subsystem is in a superposition of two states, and it interacts with a second small subsystem, then afterward, the composite system will be in a superposition.
Letting \Longrightarrow be interpreted as "evolves into" (after some specified amount of time T), then QM tells us:
If |u\rangle \otimes |\emptyset\rangle \Longrightarrow |u\rangle \otimes |U\rangle and |d\rangle \otimes |\emptyset\rangle \Longrightarrow |u\rangle \otimes |D\rangle then
(\alpha |u\rangle + \beta |d\rangle) \otimes |\emptyset\rangle \Longrightarrow \alpha |u\rangle \otimes |U\rangle + \beta \otimes |D\rangle
Informally, you have two systems, the system being measured, and the system doing the measurement. For simplicity, I'm assuming that the state being measured is a simple system with a two-state basis |u\rangle and |d\rangle, the eigenstates of an operator with two eigenvalues, spin-up and spin-down. I'm assuming that the second system is measuring the observable corresponding to that eigenvalue. To be a measurement device, the second system should evolve into a "pointer state" (either |U\rangle or |D\rangle) to indicate which value it measured.
If the measuring device is itself describable by QM, then if the initial state of the system to be measured is a superposition of eigenstates, then the composite system will evolve into a superposition of two possibilities: (1) the first system is in state |u\rangle and the second system is in state |U\rangle, or (2) the first system is in state |d\rangle and the second system is in state |D\rangle.
The final state is a "many-worlds" state, in that the measuring device is not in a definite measurement state.
To get a "single-world" from this, it seems to me that you need a second kind of dynamics (the hidden-variables of Aaronson, or Bohm) that selects one possibility out of the two possible measurement states.