1981
DOI: 10.1021/ar00072a002
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The semiclassical way to molecular spectroscopy

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Cited by 1,415 publications
(838 citation statements)
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“…In this ͑theoretical͒ limit the laser pulse simply promotes to the excited electronic state a replica of the initial nuclear state-times the transition dipole moment of the electronic transition-which then evolves under field-free conditions ͑a Franck-Condon wave packet͒. 16,17 This provides a simple picture of the photoinduced dynamics and it can be shown that the branching ratio dictated by the Franck-Condon wave packet is identical to the branching ratio obtained by a cw laser, when the full absorption band is scanned uniformly over all frequencies. 9 In fact, the dynamics created by any laser-pulse shape-in the weak-field ͑first-order perturbation theory͒ limit-can be described as a superposition of Franck-Condon wave packets excited at different times.…”
Section: ͑1͒mentioning
confidence: 99%
“…In this ͑theoretical͒ limit the laser pulse simply promotes to the excited electronic state a replica of the initial nuclear state-times the transition dipole moment of the electronic transition-which then evolves under field-free conditions ͑a Franck-Condon wave packet͒. 16,17 This provides a simple picture of the photoinduced dynamics and it can be shown that the branching ratio dictated by the Franck-Condon wave packet is identical to the branching ratio obtained by a cw laser, when the full absorption band is scanned uniformly over all frequencies. 9 In fact, the dynamics created by any laser-pulse shape-in the weak-field ͑first-order perturbation theory͒ limit-can be described as a superposition of Franck-Condon wave packets excited at different times.…”
Section: ͑1͒mentioning
confidence: 99%
“…In order to do so, we first calculate the a 1g vibrational envelope of the first absorption band assuming one single electronic origin, 5 f 3 1 ⌫ 8u ( 4 I 9/2 )→ 5 f 2 6d(t 2g ) 1 1 ⌫ 8g ( 4 K 11/2 ). ͓We use the semiclassical time-dependent approach of Heller, 50,51 with bond distances and a 1g vibrational frequencies taken from Table IV. Detailed formulas can be found in Refs.…”
Section: àmentioning
confidence: 99%
“…The involvement of indirect modes appears as an individual band in the spectrum and is interpreted as resonance in the time-independent approach and recurrence in the time-dependent picture. Recurrence appears as peaks in the norm of the autocorrelation function in the time domain and the Fourier transformation of the autocorrelation function produces the spectrum in the energy domain [55] as shown in the right-lower part of Figure 1. These are included in most theoretical studies for moderately small molecules by using the wave-packet propagation method (X-NO stands for the molecules like Cl-NO, HO-NO, and CH 3 O-NO, etc.…”
Section: (6) Analysis Of the Propagated Resultsmentioning
confidence: 99%