Accurately known energy level structure of the A'∑u+b3 IIu complex of states from a recent global de-perturbation of these states has enabled additional assignments of 140 perturbation facilitated infrared-infrared...Accurately known energy level structure of the A'∑u+b3 IIu complex of states from a recent global de-perturbation of these states has enabled additional assignments of 140 perturbation facilitated infrared-infrared double resonance (PFIIDR) transitions to the 2^3△1g state from collisionally populated intermediate 1 + A Eu levels. Together with the 221 previously observed 2^3△1g←A1∑u+←X1∑g+ Eu X Eg double resonance lines [J. Chem. Phys. 128, 204313 (2008)], molecular constants and the Rydberg-Klein-Rees potential energy curve of the 23△1g state have been recalculated (excluding 54 perturbed levels). The centrifugal distortion constant has been determined and agrees well with the value calculated based on standard empirical formulas. The hyperfine structure of the 23△1g state, which has not resolved in our sub-Doppler excitation spectra of the 23△1g state, has been interpreted with a preliminary simulation.展开更多
文摘Accurately known energy level structure of the A'∑u+b3 IIu complex of states from a recent global de-perturbation of these states has enabled additional assignments of 140 perturbation facilitated infrared-infrared double resonance (PFIIDR) transitions to the 2^3△1g state from collisionally populated intermediate 1 + A Eu levels. Together with the 221 previously observed 2^3△1g←A1∑u+←X1∑g+ Eu X Eg double resonance lines [J. Chem. Phys. 128, 204313 (2008)], molecular constants and the Rydberg-Klein-Rees potential energy curve of the 23△1g state have been recalculated (excluding 54 perturbed levels). The centrifugal distortion constant has been determined and agrees well with the value calculated based on standard empirical formulas. The hyperfine structure of the 23△1g state, which has not resolved in our sub-Doppler excitation spectra of the 23△1g state, has been interpreted with a preliminary simulation.