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18
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85034562212
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note
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0 would be meaningless. As to the Gaussian turn-off function, it is sufficiently long to ensure a practically adiabatic switching-off of the laser-molecule interactions. Yet, it is sufficiently short to ensure that the computational cost remains accessible.
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19
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85034539743
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note
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As shown in Refs. 20 and 21, the interaction between the field and the laser-induced anisotropic polarizability tends to place a molecular system in pendular states, i.e., rotational wave packets that are localized in angle space. These stales give probability distributions that are peaked along the laser field polarization, denoting laser-induced alignment. Here, this alignment is considered to be perfect, i.e., the rotational wave packet is assumed to be singularly localized in angle space. This idealization is introduced to reduce the wave packet simulations to one dimension, permitting a better focus to be made on new features that the permanent dipole moments produce in the wave packet dynamics.
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27
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85034562508
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note
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0), from which the particle is launched with some nonzero initial velocity, is made to account for the finite distance over which the actual initial wave packet is to be accelerated before acquiring a finite average momentum or velocity.
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28
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85034532930
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0 is increased, the dissociative character of the ballistic particle's trajectory increases, as the particle is found trapped over shorter and shorter times
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0 is increased, the dissociative character of the ballistic particle's trajectory increases, as the particle is found trapped over shorter and shorter times.
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