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 |
|---|---|
| Pages (from-to) | 367-372 |
| Number of pages | 6 |
| Journal | Chemical Physics Letters |
| Volume | 91 |
| Issue number | 5 |
| DOIs | |
| State | Published - 24 Sep 1982 |