Articles you may be interested inKinetic and dynamic studies of the Cl(2 P u) + H2O( X ̃ 1 A 1) → HCl( X ̃ 1Σ+) + OH( X ̃ 2Π) reaction on an ab initio based full-dimensional global potential energy surface of the ground electronic state of ClH2O J. Chem. Phys. 139, 074302 (2013); 10.1063/1.4817967 Time-dependent quantum wave packet study of the Ar+H2 +→ArH++H reaction on a new ab initio potential energy surface for the ground electronic state (12 A′) J. Chem. Phys. 138, 174305 (2013); 10.1063/1.4803116 Accurate ab initio potential energy surface, thermochemistry, and dynamics of the Br(2P, 2P3/2) + CH4 → HBr + CH3 reaction J. Chem. Phys. 138, 134301 (2013); 10.1063/1.4797467Unimolecular decomposition of chemically activated triplet C 4 HD 3 complexes: A combined crossed-beam and ab initio study Ab initio molecular orbital and density functional characterization of the potential energy surface of the N 2 O+Br reaction Density functional B3LYP/6-311ϩG(3d f )//B3LYP/6-31G* calculations of potential energy surfaces ͑PES͒ have been performed for the TiϩCO 2 →TiOϩCO reaction in the triplet, quintet, and singlet electronic states. The results indicate that in the ground triplet state the most favorable reaction mechanism involves insertion of the Ti atom into a CO bond ͓via a 2 -C,O coordinated t-͑TiOC͒O complex͔ to produce a triplet t-OTiCO molecule with the energy gain of 43.9 kcal/mol and the latter can further dissociate to TiO( 3 ⌬)ϩCO with the total reaction exothermicity of ϳ30 kcal/mol. The addition mechanism leading to the same TiO( 3 ⌬)ϩCO products via a metastable 2 -O,O complex t-cyc-TiCO 2 is also feasible at ambient temperatures since the highest barrier on the reaction pathway is only 4.7 kcal/mol. The reaction mechanisms in excited singlet and quintet electronic states have many similar features with the ground state reaction but also exhibit some differences. In the singlet state, the reaction can follow 1 AЉ and 1 AЈ pathways, of those the insertion via a s-͑TiOC͒O ( 1 AЈ) complex leading to s-OTiCO ( 1 AЈ) and then to TiO( 1 ⌬)ϩCO does not have an activation barrier. The insertion mechanism on the 1 AЉ PES depicts a low barrier of 1.8 kcal/mol and leads to s-OTiCO ( 1 AЉ), which dissociates into TiO( 1 ⌬)ϩCO. The addition pathways via 2 -O,O coordinated complexes require to overcome significant barriers, 7.8 and 34.9 kcal/mol for the 1 AЉ and 1 AЈ states, respectively. In the quintet state, the reaction at low and ambient temperatures can proceed only by coordination of Ti( 5 F) toward CO 2 with formation of 2 -C,O q-͑TiOC͒O, 2 -O,O q-cyc-TiCO 2 , and 1 -O q-TiOCO bound by 9.7, 6.1, and 4.6 kcal/mol, respectively, relative to the reactants. The 2 -C,O and 1 -O coordinations occur without barriers, while the 2 -O,O coordination has an entrance barrier of 4.2 kcal/mol. The calculated PESs show that the carbon dioxide reforming into CO in the presence of Ti atoms should take place spontaneously.