- #36
rodsika
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JesseM said:Momentum and position eigenstates are axes in Hilbert space, each one forming a different "basis". It's like how in 3D space you can have coordinate system #1 made up of x-y-z axes, as well as coordinate system #2 made up of x'-y'-z' axes pointing in different directions, and you can use either coordinate system to describe points and vectors in that space.
If two observables commute (like position and spin), then one meaning of that is that in terms of the Hilbert space, you can find a set of basis vectors such that each vector is an eigenvector of both those observables. If they don't commute, then an eigenvector of one will be a superposition of different eigenvectors of the other, and vice versa. So, another way of stating the preferred basis problem is that you have to pick a complete set of commuting observables as your basis, if the vectors are position eigenvectors (definite position states) then they won't be momentum eigenvectors (each vector will be a superposition of different momentum states) and vice versa.
A more intuitive physical meaning of commuting vs. not commuting is that that if two observables commute, you can measure one without disturbing the value of the other--if you measure position, then immediately after that (a negligible time interval) measure spin, then immediately after that measure position again, then if the time between measurements is arbitrarily small the second position measurement will be arbitrarily close to the first one (in the limit as the time goes to infinity the change in position goes to zero). But if you measure position, then immediately measure momentum, then immediately measure position again, then no matter how small the time intervals the probability distribution for position will be significantly changed, by an amount which can be calculated from the position/momentum uncertainty relation.
Ok. After continuous reading of many references. I came across this paper by Maximilian Schlosshauer "Decoherence, the measurement problem, and interpretations of quantum mechanics":".. the results thus far suggest that the selected properties are in agreement with our observation: for mesoscopic and macroscopic objects the distance-dependent scattering interaction with surrounding air molecules, photons, etc., will in general give rise to immediate decoherence into spatially localized wave packets and thus select position as the preferred basis. On the other hand, when the environment is comparably "slow," as is frequently the case for microscopic systems, environment-induced superselection will typically yield energy eigenstates as teh preferred states."
So Environmental Superselection is the key to the Prefered Basis Problem. So what's the mystery left to solve? Pls. give an example of the subtle problem, thanks.
Also is this just particulars to Many World? Preferred basis problem also exist in pure Copenhagen and Bohmian Mechanics and other interpretations because Decoherence is the general mechanism that replaces wavefunction collapse.