1990
DOI: 10.1038/348225a0
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Direct femtosecond mapping of trajectories in a chemical reaction

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Cited by 130 publications
(77 citation statements)
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“…2). The oscillations of the activated complex within this covalent/ionic potential well, and its subsequent decay through the avoided crossing at 7 A, have been observed with FTS (7,9). With FTD, it will be possible to record the motion per se and obtain directly the different trajectories, as discussed below.…”
Section: Applicationsmentioning
confidence: 99%
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“…2). The oscillations of the activated complex within this covalent/ionic potential well, and its subsequent decay through the avoided crossing at 7 A, have been observed with FTS (7,9). With FTD, it will be possible to record the motion per se and obtain directly the different trajectories, as discussed below.…”
Section: Applicationsmentioning
confidence: 99%
“…A second, delayed probe pulse of different wavelength (A2) monitors the dynamics of the nuclear motion (e.g., dissociation) as the resulting fragments separate from each other. For a diatomic molecule (e.g., A-B), the free fragments A and B have different spectra (or ionization potentials) from that of the activated complex [A--Blt* of the transition region.The experiments on the NaI dissociation reaction (7,9) illustrate these concepts (8) (see Fig. 2).…”
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confidence: 99%
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“…One of the most successful techniques providing direct information in the time domain employs the so-called pump-probe scheme, where the first (pump) laser pulse initiates the molecular dynamics in a controlled way, i.e. launches a bound or continuum wave packet, while its time evolution is then probed with a second pulse arriving at variable delay times [3].…”
Section: Introductionmentioning
confidence: 99%
“…5 For the employed wavelength, a transition is possible only in the covalent region of the potential, i.e., excitation is most probable around a bond-length of 5.7 Å. Thus, the maxima of the signal occur at times when the vibrational wave packet is located in this region and the forth and back motion induces the double peak structure 14 at early times where the vibrational wave packet is well localized. The signal for the ͑ ʈ ͒ case is initially a factor of about 11 larger than the one for the ͑Ќ͒ polarization.…”
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confidence: 99%