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The mentioned energy differences between the quintet, triplet and singlet states of the various isomers of the complex 2 have been obtained with the hybrid density functional, namely B3LYP, the accuracy of which, has been a subject of numerous investigations in the literature. (Khavratskii, I. V.; Musaev, D. G.; Morokuma, K. Inorg. Chem. 2003, 42, 2606-2621; Abashkin, Y. G.; Collins, J. R.; Burt, S. K. Inorg. Chem. 2001, 40, 4040-4048; Brandt, P.; Norrby, P.-O.; Daly, A. M.; Gilheany, D. G. Chem.-Eur. J. 2002, 8, 4299-4307; Reiher, M.; Salomon, O.; Hess, B. A. Theor. Chem. Acc. 2001, 107, 48-55) It is suspected that the hybrid B3LYP functional may overestimate energies of the low spin states, due to the Hartree-Fock contribution in the Becke's three parameter exchange functional (B3). Therefore, to estimate possible error margins in the referred energy splittings, we have performed single point energy calculations for the isomers 2-cis(O,N) and 2-cis(N,O) with nonhybrid BPW9I functional. In these calculations we used the geometries optimized at the B3LYP level.
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The mentioned energy differences between the quintet, triplet and singlet states of the various isomers of the complex 2 have been obtained with the hybrid density functional, namely B3LYP, the accuracy of which, has been a subject of numerous investigations in the literature. (Khavratskii, I. V.; Musaev, D. G.; Morokuma, K. Inorg. Chem. 2003, 42, 2606-2621; Abashkin, Y. G.; Collins, J. R.; Burt, S. K. Inorg. Chem. 2001, 40, 4040-4048; Brandt, P.; Norrby, P.-O.; Daly, A. M.; Gilheany, D. G. Chem.-Eur. J. 2002, 8, 4299-4307; Reiher, M.; Salomon, O.; Hess, B. A. Theor. Chem. Acc. 2001, 107, 48-55) It is suspected that the hybrid B3LYP functional may overestimate energies of the low spin states, due to the Hartree-Fock contribution in the Becke's three parameter exchange functional (B3). Therefore, to estimate possible error margins in the referred energy splittings, we have performed single point energy calculations for the isomers 2-cis(O,N) and 2-cis(N,O) with nonhybrid BPW9I functional. In these calculations we used the geometries optimized at the B3LYP level.
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5A-2-trans acylperoxo complex and estimated the barrier to be less than 6.0 kcal/mol.
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3A spin states, we applied the Yamaguchi correction scheme (Yamaguchi, K. Chem. Phys. Lett. 1988, 149, 537-542; Yamaguchi, K.; Fukui, H.; Fueno, T. Chem. Lett. 1986, 625-628) as described in our previous paper. (Khavrutskii, I. V.; Musaev, D. G.; Morokuma, K. Inorg. Chem. 2003, 42, 2606-2621)
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