Geometric optimization, potential energy surfaces

Fig. 21 HF/6-31 + G -optimized structures and main geometrical parameters of the stable (T-and T/ -type complexes located on the potential energy surface (PES) of protonated sec-butyl benzene (bond lengths in Angstrpms angles in degrees (in itabc)).

Fig. 1. Schematic representation of the potential energy surface for the electronic (el) ground state of a molecule existing in two tautomeric forms, A and B. Superscripts exp, HF, CNDO/2, MINDO/3 indicate that energy differences 8 a,b calculated for potential energy surfaces determined either experimentally (exp) or calculated by means of ab initio method in the Hartree-Fock (HF) approximation or by semiempirical methods (CNDO/2, MINDO/3). The symbol eq stands for the geometrical equilibrium of both tautomers, while 2a and Qb indicate nonequilibrium geometries of tautomers A and B, respectively. Note that the theoretical potential surface calculated by sophisticated quantum-mechanical methods ( exact solution of electronic Schrbdinger equation includes electron correlation with geometry optimization) should be the same (or very similar) as that determined experimentally [in this case i>eor) ei

In our recent work [89], the reaction of HO2 with CIO has been investigated by ab initio molecular orbital and variational transition state theory calculations. The geometric parameters of the reaction system HO2 + CIO were optimized at the B3LYP and BH HLYP levels of theory with the basis set, 6-311+G(3df,2p), which can be found in Ref. [89]. Both singlet and triplet potential energy surfaces were predicted by the G2M method, as shown in Fig. 24. 

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