Abstract
A model consisting of two electronic states with different symmetries and an arbitrary number of vibrational modes which couple these states is considered. After a series of canonical transformations the hamiltonian is brought into a form suited to study effects of anharmonic and vibronic couplings. Divergences typical for non-adiabatic coupling terms are avoided.
Original language | English |
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Pages (from-to) | 367-372 |
Number of pages | 6 |
Journal | Chemical Physics Letters |
Volume | 91 |
Issue number | 5 |
DOIs | |
State | Published - 24 Sep 1982 |