Lifetimes of the vibrationless levels of the B state of CHJ and CDs1 have been measured using a tunable deep UV ( = 200 nm) femtosecond source. The lifetimes of the predissociated states are 1.38 + 0.20 and 1.84 k 0.13 ps, respectively. These values are compared with those obtained by indirect measu
Predissociation lifetimes of the B̃ and C̃ Rydberg states of CH3I
✍ Scribed by Jack A. Syage
- Publisher
- Elsevier Science
- Year
- 1993
- Tongue
- English
- Weight
- 457 KB
- Volume
- 212
- Category
- Article
- ISSN
- 0009-2614
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✦ Synopsis
Single-photon direct absorption and resonance-enhanced multiphoton ionization excitation spectra were recorded for CHJ in a jet-cooled molecular beam. The rovibrationally cold molecules yield lineshapes that are lifetime broadenend by predissociation.
Lorentzian fitswere used to extract lifetimes for specific vibronic excitation in the fj and c Rydberg states. The measured lifetimes of the B state are 0.87 ps (origin), 0.83 ps (ul), 0.92 ps (vg), and 0.67 ps (I& The e state origin has a lifetime of 0.25 ps. These results are compared to previous measurements and discussed in terms of possible mode-specific predissociation.
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Multiphoton optical-optical double-resonance spectroscopy via predissociating vibronic levels of the A state has been used to reveal hitherto uncharacterised vibrational modes of the B and c' Rydberg states of NH3 and ND,. The modes involved are Y, in the e state and VJ and vq in the B state; we pre
The monoalkyl zinc radical, CHJn, may be observed by laser-induced fluorescence following UV photodissociation of ( CH3)2Zn. The fluorescence spectrum obtained upon excitation of the 08 and the 2: bands of the A-2 transition was assigned. A very simple fluorescence spectrum is obtained upon excitat
Llteumcs OTC; m rotational levels of the E':i. d = 0, acet) Icnc and r~regas merastablcs and the 6'~: -%kg u' = I states have been measured. Cl was produced from bromotransltion uas laser excited The hfetlmes are constant wthm a vlbrdttonal level, 77 \* 8 ns for u' = 0 and 73 r 7 ns for v = I. The o
We report here how we have incorporated the effects of a nonzero total electron spin in the MORBID Hamiltonian and computer program [P. Jensen, J. Mol. Spectrosc. 128, 478-501 (1988); J. Chem. Soc. Faraday Trans. 2 84, 1315-1340 (1988); in "Methods in Computational Molecular Physics" (S. Wilson and