- #106
atyy
Science Advisor
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RUTA said:atyy's last point might relate to what I don't understand about QBism. The problem I pointed out was that Alice and Bob see "nonlocality" when they construct the M4 depiction of the experiment after exchanging measurement outcomes. That problem exists in the realm "we are agents." If Bob, say, rather sticks to "I am an agent" and records only what he observes (to include his observation of Alice's results sent to him in null or time-like fashion), and he doesn't bother to put her results in an M4 depiction to give credence to her as an agent, then he has no ontological basis for nonlocality. Am I on the right track?
Yes. I believe that QBism can in some sense consistently assert locality, as long as it expunges statements like "We are agents". In the technical sense, Bell nonlocality has to do with P(a,b|λ), where a and b are classical outcomes of measurements. If one denies that b "exists" far away, then one cannot form the Bell inequality. Now one also cannot then define locality by satisfaction of the inequality. However, one can use other definitions like the existence of a classical M4. So the solution is one agent, one classical M4, one quantum wavefunction for everything else except the agent. I think this is consistent.