RESUMEN
The thermal decomposition of methyl and ethyl formates has been extensively studied due to their importance in the oxidation of several fuels, pesticidal properties and their presence in interstellar space. We hitherto present the study of the thermal decomposition of methyl and ethyl fluoroformates, which could help in the elucidation of the reaction mechanisms. The reaction mechanisms were studied using FTIR spectroscopy in the temperature range of 453-733 K in the presence of different pressures of N2 as bath gas. For FC(O)OCH3 two different channels were observed; the unimolecular decomposition which is favored at higher temperatures and has a rate constant kFC(O)OCH3 = (5.3 ± 0.5) × 1015 exp[-(246 ± 10 kJ mol-1/RT)] (in units of s-1) and a bimolecular channel with a rate constant kFC(O)OCH3 = (1.6 ± 0.5) × 1011 exp[-(148 ± 10 kJ mol-1/RT)] (in units of s-1 (mol L)-1). However for ethyl formate, only direct elimination of CO2, HF and ethylene operates. The rate constants of the homogeneous first-order process fit the Arrhenius equation kFC(O)OCH2CH3 = (2.06 ± 0.09) × 1013 exp[-(169 ± 6 kJ mol-1/RT)] (in units of s-1). The difference between the mechanisms of the two fluoroformates relies on the stabilization of a six-centered transition state that only exists for ethyl formate. First principles calculations for the different channels were carried out to understand the dynamics of the decomposition.
RESUMEN
Unraveling the photochemical behaviour of the green fluorescent protein chromophore has lately attracted widespread attention among scientists. In this paper we present the study of the photochemical isomerization Z â E and the back reaction of the chromophore analog, 5-arylmethylene-2- thioxoimidazolidin-4-one. Experimental results are supported with ab initio calculations at the DFT, (B3LYP/6-31+g(d,p)), TD-DFT (B3LYP/6-311++g(3df,3pd)) and CASSCF levels. A first excitation to the S2 state, where the isomerization occurs, is proposed followed by two conical intersections to S1 and S0 respectively. Three different mechanisms were analyzed for thermal reversion, concluding that the preferred channel involves an intersystem crossing between the S0 and T1 states with the formation of a biradical.