1992
DOI: 10.1021/j100181a046
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Measurement of product branching ratios of the cyanato + nitric oxide reaction

Abstract: The reaction NCO + NO -products was studied at room temperature using pulsed laser photolysis with time-resolved infrared diode laser detection. C02, CO, and N20 reaction products were detected by infrared absorption under quantum-state relaxed conditions to provide absolute number densities of each species. The results indicate that three product channels are active: C02 + N2 is the most important channel, with CO + N2 + 0 and N 2 0 + CO also contributing significantly.

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Cited by 78 publications
(70 citation statements)
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“…The calculated bond-breaking barrier was 8.23 kcal/mol (TS 11-P3 ). However, the 1,2 H-shift from 8 may form a very stable conformer, 10, 30.72 kcal/mol lower than the reactants, and the barrier for this transfer was 46.93 kcal/mol, TS [8][9][10] . From our calculation it seemed unlikely to proceed further from 10 to produce P3 or P4, since it needed to form 12 or 13 first.…”
Section: Table 2: Ground State Electronic Energies (Au) and The Relatmentioning
confidence: 96%
“…The calculated bond-breaking barrier was 8.23 kcal/mol (TS 11-P3 ). However, the 1,2 H-shift from 8 may form a very stable conformer, 10, 30.72 kcal/mol lower than the reactants, and the barrier for this transfer was 46.93 kcal/mol, TS [8][9][10] . From our calculation it seemed unlikely to proceed further from 10 to produce P3 or P4, since it needed to form 12 or 13 first.…”
Section: Table 2: Ground State Electronic Energies (Au) and The Relatmentioning
confidence: 96%
“…[c0(u'3120@r = @dt[CNIO,Br (14 The initial concentration [CN]O,B~ of the C N radical used in eq IC is given by the following expression where US, is the absorption cross section of BrCN at 193 nm, ,$er is the laser illuminance used for the photolysis of BrCN, p~~ is the density of BrCN, and +er is the quantum yield for the production of C N from BrCN a t 193 nm. Substitution of this expression for [CN]O,B~ from eq 11 into eq IC and defining @dt = @to&",Br, where @tot = gives eq Id.…”
mentioning
confidence: 99%
“…Since we probe only the ground vibrational state, the nascent vibrational distribution must be relaxed to a Boltzmann distribution in order for the molecular number densities to be reliably measured. SF 6 has previously been shown to be an efficient relaxer of vibrational excitation for N 2 O and CO 2 [14][15][16], and probably also relaxes HCNO as well. Under the experimental conditions of 1.0 Torr of SF 6 , this relaxation still takes about 50 sec for N 2 O and CO 2 , but is essentially complete on a timescale short compared to the slow decay, which is attributed to diffusion of molecules out of the probed volume.…”
Section: Product Branching Ratiosmentioning
confidence: 99%