Articles you may be interested inAutodetachment spectroscopy and dynamics of dipole bound states of negative ions: 2 A 1-2 B 1 transitions of H2CCC− Long range potential of the A1∑+ u state of Na2 using modulated gain spectroscopy AIP Conf.Rotation-vibration levels in the energy region near the HCP↔HPC X 1 ⌺ ϩ isomerization barrier ͑i.e., the HPC geometry͒ were observed by HCP à -X and C -X stimulated emission pumping ͑SEP͒ spectroscopy. Unlike HCN↔HNC, where the unstable isomer corresponds to a local minimum on the potential energy surface, the HPC isomer corresponds to a saddle point. In the à -X SEP spectra, the lϭ0 and 2 components of pure bend overtone levels ͑0,26рv 2 р42,0͒ and the bend-CP stretch combination levels, ͑0,24,1͒ and ͑0,26,1͒, were sampled. On the other hand, in the C -X SEP spectra, which sample lϭ0 components exclusively, 2 2 :1 3 polyads were identified. These polyads appeared in the SEP spectra as a regular, easily recognizable pattern. Since the C -X SEP spectra appeared to be almost totally Franck-Condon nonselective ͑a large fraction of the predicted total density of lϭ0 levels was observed͒, the polyad pattern was the key to vibrational assignments of highly excited vibrational levels. It was found that the bending vibration exhibits very regular ͑Morse-type͒ behavior up to at least v 2 ϭ42. However, an abrupt change was found in the v 2 -dependence of all of the vibrational fine structure constants above v 2 ϭ36, E ͑0,36,0͒ ϭ22 048 cm Ϫ1 . In addition, a sudden turning on of perturbations in the pure bend overtone levels was also observed to occur at v 2 ϭ32. These abrupt changes in the level structure could be related to an abrupt change in curvature of the potential energy surface along directions perpendicular to the bending coordinate when the bending coordinate is far from equilibrium.