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1
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85037239445
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Proceedings of the Conference on Ultrafast Phenomena IX, edited by P. F. Barbara, W. H. Knox, G. A. Mourou, and A. H. Zewail (Springer-Verlag, Berlin, 1994); Proceedings of the Conference on Ultrafast Phenomena X, edited by P. F. Barbara, J. G. Fujimoto, W. H. Knox, and W. Zintu (Springer-Verlag, Berlin, 1996)
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Proceedings of the Conference on Ultrafast Phenomena IX, edited by P. F. Barbara, W. H. Knox, G. A. Mourou, and A. H. Zewail (Springer-Verlag, Berlin, 1994); Proceedings of the Conference on Ultrafast Phenomena X, edited by P. F. Barbara, J. G. Fujimoto, W. H. Knox, and W. Zintu (Springer-Verlag, Berlin, 1996).
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2
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85037220912
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So far there exists no condensed phase analog
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So far there exists no condensed phase analog.
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3
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17444430082
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JOBPDE
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S. Augst, D. D. Meyerhofer, D. Strickland, and S. L. Chin, J. Opt. Soc. Am. B 8, 858 (1991).JOBPDE
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9
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85037221215
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Atomic and Molecular Beam Methods, edited by G. Scoles (Oxford University Press, Oxford, 1988), Vol. I, Chap. 2
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Atomic and Molecular Beam Methods, edited by G. Scoles (Oxford University Press, Oxford, 1988), Vol. I, Chap. 2.
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10
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4243099175
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PLRAAN
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P. Dietrich, D. T. Strickland, M. Laberge, and P. B. Corkum, Phys. Rev. A 47, 2305 (1993).PLRAAN
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13
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85037195512
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A small fraction of the dissociating molecules are expected to be projected onto an (Formula presented) potential. However, the low collection efficiency of (Formula presented) ions resulting from this channel makes the observation difficult
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A small fraction of the dissociating molecules are expected to be projected onto an (Formula presented) potential. However, the low collection efficiency of (Formula presented) ions resulting from this channel makes the observation difficult.
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14
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85037203225
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A chirped pump pulse is not dealt with in this paper
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A chirped pump pulse is not dealt with in this paper.
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16
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85037191072
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At a wavelength of 625 nm there is also a small probability that the (Formula presented) potential of (Formula presented) is excited
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At a wavelength of 625 nm there is also a small probability that the (Formula presented) potential of (Formula presented) is excited 15. This is not included in the simulation since the dissociation dynamics of a wave packet launched on the (Formula presented) potential will be essentially identical to one launched in the (Formula presented) potential.
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17
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85037203629
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fact, even some ionization of (Formula presented) is observed when only the pump pulse is applied
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In fact, even some ionization of (Formula presented) is observed when only the pump pulse is applied.
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18
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85037189968
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Actually, the Coulomb energy is not completely negligible at a delay of 20 ps. This is taken into account in the calculation of the predicted positions of the peaks, assuming that the (Formula presented) explosion channel is the dominant one
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Actually, the Coulomb energy is not completely negligible at a delay of 20 ps. This is taken into account in the calculation of the predicted positions of the peaks, assuming that the (Formula presented) explosion channel is the dominant one.
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19
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85037181709
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The exact shape of the wave packet will not only depend on the population in the vibrational levels but also on the Franck-Condon overlaps involved in the excitation
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The exact shape of the wave packet will not only depend on the population in the vibrational levels but also on the Franck-Condon overlaps involved in the excitation.
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20
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11944264176
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SCIEAS
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A. M. Weiner, D. E. Leaird, G. P. Wiederbrecht, and K. A. Nelson, Science 247, 1317 (1990).SCIEAS
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85037185241
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H. Sakai et al(unpublished).
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