2010
DOI: 10.1016/j.chemphys.2009.10.017
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Accurate determination of the structure of 1,3,5-trifluorobenzene by femtosecond rotational Raman coherence spectroscopy and ab initio calculations

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Cited by 24 publications
(22 citation statements)
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“…The fitted ratio is 1.04 ± 0.06, which is in good agreement with the CCSD(T) calculated ratios of 0.996-1.051 given in Table III. There is practically no collisional dephasing in the supersonic jet, as we have shown experimentally for the symmetrictop molecules cyclohexane, trifluorobenzene, and hexafluorobenzene. 2,3,43 Due to the irregular spacing of the transition frequencies in asymmetric-top molecules, their RCS transients decays more rapidly with time than compared to symmetrictop molecules; this is already quite marked given the sizable asymmetry of p-DFB with κ = −0.87. Thus, the RCS transient of hexafluorobenzene shows observable recurrences up to t ∼ 5000 ps delay, 3 but the last observable recurrences of p-DFB lie at t ∼ 1375 ps, see Figure 3(i).…”
Section: A Supersonic Jet Measurements and Assignmentsmentioning
confidence: 95%
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“…The fitted ratio is 1.04 ± 0.06, which is in good agreement with the CCSD(T) calculated ratios of 0.996-1.051 given in Table III. There is practically no collisional dephasing in the supersonic jet, as we have shown experimentally for the symmetrictop molecules cyclohexane, trifluorobenzene, and hexafluorobenzene. 2,3,43 Due to the irregular spacing of the transition frequencies in asymmetric-top molecules, their RCS transients decays more rapidly with time than compared to symmetrictop molecules; this is already quite marked given the sizable asymmetry of p-DFB with κ = −0.87. Thus, the RCS transient of hexafluorobenzene shows observable recurrences up to t ∼ 5000 ps delay, 3 but the last observable recurrences of p-DFB lie at t ∼ 1375 ps, see Figure 3(i).…”
Section: A Supersonic Jet Measurements and Assignmentsmentioning
confidence: 95%
“…2,20,21 Briefly, three parallel laser beams from an amplified Ti:Sapphire laser system provide the ∼75 fs pulses at 800 nm employed for the stimulated Raman pump, dump, and probe steps. The stimulated Raman polarization induced by the pump/dump steps at time zero is detected by the DFWM signal generated from the time-delayed probe pulse.…”
Section: Experimental Methodsmentioning
confidence: 99%
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