2006
DOI: 10.1016/j.cplett.2006.01.001
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Selective control of HOD photodissociation using low quanta O–D excitation and field optimized initial state (FOIST) based combination of states and colors

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Cited by 9 publications
(2 citation statements)
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“…This finding can be explained by the difference in masses between deuterium and proton, which results in different bond stretching frequencies when they are allowed to move on the same repulsive potential. Previous investigations on the photodissociation of HOD on its first excited-state PES gave similar results. It is important to mention that classical trajectory calculations on HOD 2+ gave the value of branching ratio 8.6, which is quite different from quantum results.…”
Section: Resultssupporting
confidence: 66%
See 1 more Smart Citation
“…This finding can be explained by the difference in masses between deuterium and proton, which results in different bond stretching frequencies when they are allowed to move on the same repulsive potential. Previous investigations on the photodissociation of HOD on its first excited-state PES gave similar results. It is important to mention that classical trajectory calculations on HOD 2+ gave the value of branching ratio 8.6, which is quite different from quantum results.…”
Section: Resultssupporting
confidence: 66%
“…Influence of other initial conditions, like initial rotational and vibrational states of HOD molecule, on dissociation dynamics of HOD 2+ is yet to understand. Previous studies showed that weak-field unimolecular photodissociation dynamics of HOD strongly depends on the initial vibrational state of HOD molecule. In this article, we would like to answer the question: Does the dissociation dynamics of HOD 2+ depend on the initial vibrational state of HOD molecule as in the case of HOD photodissociation?…”
Section: Introductionmentioning
confidence: 99%