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note
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Note that it is an interesting problem in its own right to investigate the influence of correlated initial conditions such that time evolution of the state of the distinguished system no longer corresponds to a completely positive map. This is relevant, e.g., when considering a charged quantum particle coupled to the radiation field, where the assumption of product initial conditions is typically not invariant under gauge transformations [16].
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The mass of the particle will set to unity and units will be employed where ℏ = 1 and k = 1.
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This is meant in the sense that for any ε > 0 there exists a ζ > 0 such that |B∞ - T| ø ε.
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Needless to say, there is a certain degree of ambiguity in the choice of the pointer states here. The key argument is that the final state after a finite time can be exactly represented as a convex combination of these reasonable pointer states.
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