Issue 0, 1980

Quantum-resolved dynamics of excited states. Part 6.—Radiative lifetime and collisional deactivation rates in BrF (B)

Abstract

Selected ro-vibrational levels (v′, J′) in electronically-excited BrF B3Π(0+) have been populated by absorption in the B–X system, using pulses of narrow-band dye laser radiation. The decay of laser-induced fluorescence in real time has been used to redetermine the radiative lifetime τR of BrF (B) and to investigate vibrational transfer and quenching within the B-state manifold. The results give improved values for τR in the range 64.2 µs µS [gt-or-equal]τR[gt-or-equal] 55.5 µs for 7 [gt-or-equal]v[gt-or-equal] 3.

Broad-band wavelength-resolution of fluorescence and computer modelling were used to obtain rate constants at 293 K for quenching, kQ,M, and for vibrational transfer, kv,M, for collisions of BrF (B) with bath gases M = O2, Cl2, Ar, CHFCl2 and HCl. Values of kQ,M/cm3 molecule–1 s–1 ranged from ca. 1.2 × 10–11 for M = HCl, down to < 1 × 10–13 for M = Ar. Values of kv,M/cm3 molecule–1 s–1 were generally greater than those of kQ,M and, as expected, increased with an increase in v′. For example, in the case of M = O2, k3,O2= 3.6 × 10–11, which was one order of magnitude greater than the magnitude of kQ,O2, namely 2.6 × 10–12. Thus, in the case of BrF (B)+ O2 collisions, vibrational relaxation of the initial (v′, J′) state is much faster than electronic quenching.

Article information

Article type
Paper

J. Chem. Soc., Faraday Trans. 2, 1980,76, 1569-1585

Quantum-resolved dynamics of excited states. Part 6.—Radiative lifetime and collisional deactivation rates in BrF (B)

M. A. A. Clyne and J. P. Liddy, J. Chem. Soc., Faraday Trans. 2, 1980, 76, 1569 DOI: 10.1039/F29807601569

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