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Can you better explain what do you mean by that? (Pinpoiting to the right part of your paper would be OK.)A. Neumaier said:##H## is a sum of integrals over multilocal operators
Can you better explain what do you mean by that? (Pinpoiting to the right part of your paper would be OK.)A. Neumaier said:##H## is a sum of integrals over multilocal operators
In my paper I didn't discuss the detailed form of the Hamiltonian of the universe. It depends on stuff yet to be discovered about how to represent quantum gravity. But the general form of the Hamiltonian is already visible from simpler quantum field theories such as QED, where it is derived as usual from the action, and later modified through renormalization.Demystifier said:Can you better explain what do you mean by that? (Pinpointing to the right part of your paper would be OK.)
charters said:Ok this I can agree is a workable and well understood solution to Bell's theorem. Basically, instead of saying a "pilot wave" is steering the deterministic time evolution of the local pointer variables, the TI says it is "multilocal variables" doing so.
I discuss nonlocality in Part II of my preprints, Section 4.5, mentioned in post #1 of the main thread on the TI (linked to in post #2 of the present thread) .indefinite_123 said:I do not understand how can one avoid a 'non-locality' of the kind of the pilot-wave theory if multi-local properties dependent on more than one space-like separated space-time regions are accepted. Are there any references on this?
Thank you very much!A. Neumaier said:I discuss nonlocality in Part II of my preprints, Section 4.5, mentioned in post #1 of the main thread on the TI (linked to in post #2 of the present thread) .
For a more polished account of bilocal quantities and nonlocality see my recent book also mentioned there.