Issue 0, 1972

Formation of the B3Π(0+) states of BrF and IF by atom recombination in the presence of singlet (1Δg, 1Σ +g) oxygen

Abstract

Combination of F 2P[fraction three-over-two] with Br 2P[fraction three-over-two] or I 2P[fraction three-over-two] ground state atoms in the presence of singlet O21Δg, 1Σ+g, leads to formation of BrF B3Π(0+) or IF B3Π(0+), which were detected by observation of their band emission spectra (975 [gt-or-equal]λ[gt-or-equal] 483 nm), B3Π(0+)→X1Σ+. It was shown that formation of BrF B3Π(0+) explicitly requires energy transfer from O21Δg or 1Σ+g. The most probable excitation process is envisaged to occur by combination of Br 2P[fraction three-over-two]+ F 2P[fraction three-over-two] atoms (in the presence of a third body) to give BrF A3Π(1)(or possibly 3Π(2, 0)), followed by collisional energy transfer from singlet oxygen with BrF A3Π(1) to BrF B3Π(0+).

At least 38 new bands of the BX system of BrF have been identified, and the previously uncertain vibrational numbering of the B3Π(0+) state has been confirmed. Vibrational constants are reported for the first time for levels of the X1Σ+ ground state up to v″= 10, corresponding to an energy of 6262 cm–1 above v″= 0. The available data on the dissociation energy of BrF are briefly surveyed, and a value of D°(BrF)= 2.384 eV is favoured.

For the BX system of IF, many new bands have been observed, and vibrational constants for levels up to v″= 19 (10 381 cm–1 above v″= 0) of the ground state are reported.

Article information

Article type
Paper

J. Chem. Soc., Faraday Trans. 2, 1972,68, 2134-2143

Formation of the B3Π(0+) states of BrF and IF by atom recombination in the presence of singlet (1Δg, 1Σ+g) oxygen

M. A. A. Clyne, J. A. Coxon and L. W. Townsend, J. Chem. Soc., Faraday Trans. 2, 1972, 68, 2134 DOI: 10.1039/F29726802134

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