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Lifetimes of C-2 in rotational levels of the B̃2Σ+u state in the gas phase

✍ Scribed by Samuel Leutwyler; John P. Maier; Liubomir Misev


Publisher
Elsevier Science
Year
1982
Tongue
English
Weight
250 KB
Volume
91
Category
Article
ISSN
0009-2614

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✦ Synopsis


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 oscdlator s!rength&, = 0.044 5 0.004.


📜 SIMILAR VOLUMES


Lifetimes of vibrational levels in the B
✍ Joseph D. Tobiason; Eric A. Rohlfing 📂 Article 📅 1996 🏛 Elsevier Science 🌐 English ⚖ 771 KB

We measure the fluorescence decays for low-lying rotational states in the first eight vibrational levels of HCO B 2.aL Some long-lived decays exhibit weak quantum beats that we attribute to a higher-order hyperfine perturbation in the 13 state. We estimate fluorescence quantum yields by combining me

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✍ T.Howard McGee; Ralph E. Weston Jr. 📂 Article 📅 1977 🏛 Elsevier Science 🌐 English ⚖ 501 KB

Using the single-photon time correlation sxtetf'od, we have determined the lifetime of the Sz (B 3X3) state from the decay rate of the fluorescence at 370 nm. A lifetime of 45.0 t 0.6 n5 was measured, and the cross section for fluorescence quenching by Sz as found to be 8J -3 t 4.7 A\*. A slight dep

Comment on “Lifetimes of vibrational lev
✍ H. Bitto; Robert T. Carter 📂 Article 📅 1996 🏛 Elsevier Science 🌐 English ⚖ 131 KB

Arguments are put forward that the quantum beats in the B 2~ electronic state of HCO attributed to a higher-order hyperfine perturbation by Tobiason and Rohlfing are most likely due to well-known hyperfine quantum beats. In contrast to Tobiason and Rohlfing's interpretation, hyperfine perturbations

Reply to the comment on “Lifetimes of vi
✍ Joseph D. Tobiason; Eric A. Rohlfing 📂 Article 📅 1996 🏛 Elsevier Science 🌐 English ⚖ 110 KB

The preceding Comment by Bitto and Carter objects to our interpretation of the weak quantum beats observed for particular rovibrational states of B 2K HCO in the title article and postulates that the observed beats are anisotropic hyperfine quantum beats. We concur with their Comment, acknowledge th