2006
DOI: 10.1016/j.chemphys.2006.03.024
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Selective vibrational population transfer between electronic states of the Na2 molecule with ultrashort laser pulses

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Cited by 9 publications
(2 citation statements)
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“…Because the population is initially distributed around the equilibrium of state Xñ | and the interaction time of the femtosecond laser is relatively short, the transition is then considered to mainly occur around R 0 . The same definition has been used in previous calculations of this system or others (see, e.g., [34,35,37]). In this work, we consider the twophoton resonant transition, i.e., 0 D = , and 1 2 D = -D .…”
Section: T I Sinmentioning
confidence: 99%
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“…Because the population is initially distributed around the equilibrium of state Xñ | and the interaction time of the femtosecond laser is relatively short, the transition is then considered to mainly occur around R 0 . The same definition has been used in previous calculations of this system or others (see, e.g., [34,35,37]). In this work, we consider the twophoton resonant transition, i.e., 0 D = , and 1 2 D = -D .…”
Section: T I Sinmentioning
confidence: 99%
“…By using a counterintuitive sequence of light pulses, the population has been transferred from the lowest vibrational level of the ground electronic state (X 1 g S + ) to the lowest vibrational level of the second excited electronic state (2 1 g P ), with the first excited electronic state (A 1 u S + ) serving as an intermediate. Also based on this molecule, the APLIP scheme has been extended by introducing the chirped pulses [18], an addition electronic state (four-electronicpotential model) [19], and the femtosecond pulses [34,35].…”
Section: Introductionmentioning
confidence: 99%