Abstract

AbstractThe idea to derive the nonadiabatic coupling terms by solving the Curl equations (Avery, J.; Baer, M.; Billing, G. D. Mol Phys 2002, 100, 1011) is extended to a three‐state system where the first and second states form one conical intersection, i.e., τ12 and the second and the third states form another conical intersection, i.e., τ23. Whereas the two‐state Curl equations form a set of linear differential equations, the extension to a three‐state system not only increases the number of equations but also leads to nonlinear terms. In the present study, we developed a perturbative scheme, which guarantees convergence if the overlap between the two interacting conical intersections is not too strong. Among other things, we also revealed that the nonadiabatic coupling term between the first and third states, i.e., τ13 (such interactions do not originate from conical intersection) is formed due to the interaction between τ12 and τ23. © 2002 Wiley Periodicals, Inc. Int J Quantum Chem, 2002

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