Abstract

The issue of the proper classical limit for approximate quantum dynamical methods is discussed, especially as it applies to liquid para-hydrogen. The conclusion is that a logical dilemma arises, in which the quantum system is in one thermodynamic state but the classical system for the same volume is in a different thermodynamic state. This dilemma also points to the likelihood that a certain class of approximate quantum dynamical methods, in which the initial conditions are weighted by a quantum distribution function but the dynamics are then run with classical trajectories, will contain a systematic error in the dynamical results for such systems.

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