Fragment ion yields in the C 1s → Rydberg excitation region of CO 2 were measured in the 90° and 0° directions relative to the electric vector of the linearly polarized light. The C 1s → ns ( n = 3, 4), n pπ and n pσ ( n = 3−7), and n d ( n = 3, 4) Rydberg transitions are clearly observed and show some vibrational structures. The dipole-forbidden C 1s(σ g ) → 3sσ g Rydberg transition is the strongest of all the Rydberg transitions, and the ion yield in the 90° direction is dominant. This indicates that the bending vibration is predominantly coupled with the 3sσ g Rydberg state and the intensity-lending dipole-allowed state is a very strong π* resonance, only 2 eV lower than the 3sσ g state. On the other hand, in the 4sσ g Rydberg state the vibronic coupling through the antisymmetric stretching mode is strongly observed in the 0° direction. This is probably because the 4sσ g state approaches another intensity-lending state with Σ u + symmetry and goes away from the π* resonance. The angle-resolved ion-yield technique is very powerful for elucidating the vibronic coupling mechanism.
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Adachi et al. (1996) studied this question.
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