JesseM
Science Advisor
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I don't, but the problem of needing to find a preferred basis seems specific to DeWitt's version, so since you were asking questions about how to pick it I figured you were asking about that version.rodsika said:Why do you put so much weight on DeWitt.
Right, but with the decoherence version there is no precise definition of "worlds" and decoherence only approximately forces various subsystems into a mix of eigenstates of some observable like position, the interference terms don't entirely disappear and the whole business also depends on how you divide "subsystem" and "environment".rodsika said:Therefore why can't we just accept the Decoherence version of MWI as it needs the environment to define the Preferred basis.
We have to assume the same basic laws apply to all "worlds" in the MWI because you have to be able to represent the wavefunction of the universe as a single state vector evolving according to the Schroedinger equation. The paper you linked to earlier by Schlosshauer says that decoherence tends to drive subsystems towards an ensemble of position eigenstates, though in some cases it can be energy eigenstates instead, see page 14:rodsika said:Now in pure Decoherence version (without DeWitt Adhoc ness), is it possible other branches would have other environments (akin to parallel worlds with different laws of nature) such that the environment there with constants of nature that don't admit positions to have charge as the preferred basis?
(again, look at the actual paper to see the notation rendered correctly, I didn't feel like translating the various Hamiltonian symbols into LaTeX)In general, three different cases have typically been
distinguished (for example, in Paz and Zurek, 1999) for
the kind of pointer observable emerging from an interaction
with the environment, depending on the relative
strengths of the system’s self-Hamiltonian bHS and of the
system-environment interaction Hamiltonian bHSE :
(1) When the dynamics of the system are dominated
by bHSE , i.e., the interaction with the environment,
the pointer states will be eigenstates of bHSE (and
thus typically eigenstates of position). This case
corresponds to the typical quantum measurement
setting; see, for example, the model of Zurek (1981,
1982), which is outlined in Sec. III.D.2 above.
(2) When the interaction with the environment is weak
and bHS dominates the evolution of the system (that
is, when the environment is “slow” in the above
sense), a case that frequently occurs in the microscopic
domain, pointer states will arise that are energy
eigenstates of bHS (Paz and Zurek, 1999).
(3) In the intermediate case, when the evolution of
the system is governed by bHSE and bHS in roughly
equal strength, the resulting preferred states will
represent a “compromise” between the first two
cases; for instance, the frequently studied model
of quantum Brownian motion has shown the emergence
of pointer states localized in phase space,
i.e., in both position and momentum (Eisert, 2004;
Joos et al., 2003; Unruh and Zurek, 1989; Zurek,
2003b; Zurek et al., 1993).