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Wavepackets delocalization

As mentioned above, the correct description of the nuclei in a molecular system is a delocalized quantum wavepacket that evolves according to the Schrbdinger equation. In the classical limit of the single surface (adiabatic) case, when effectively 0, the evolution of the wavepacket density... [Pg.252]

In the full quantum mechanical picture, the evolving wavepackets are delocalized functions, representing the probability of finding the nuclei at a particular point in space. This representation is unsuitable for direct dynamics as it is necessary to know the potential surface over a region of space at each point in time. Fortunately, there are approximate formulations based on trajectories in phase space, which will be discussed below. These local representations, so-called as only a portion of the FES is examined at each point in time, have a classical flavor. The delocalized and nonlocal nature of the full solution of the Schtddinger equation should, however, be kept in mind. [Pg.257]


See other pages where Wavepackets delocalization is mentioned: [Pg.497]    [Pg.497]    [Pg.266]    [Pg.371]    [Pg.121]    [Pg.149]    [Pg.1462]    [Pg.102]    [Pg.371]    [Pg.248]    [Pg.279]    [Pg.146]    [Pg.2]    [Pg.153]    [Pg.24]    [Pg.110]    [Pg.110]   
See also in sourсe #XX -- [ Pg.502 ]




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