Articles you may be interested inA new accurate ground-state potential energy surface of ethylene and predictions for rotational and vibrational energy levels J. Chem. Phys. 141, 104301 (2014); 10.1063/1.4894419 Franck-Condon simulation, including anharmonicity, of the photodetachment spectrum of P2H−: Restricted-spin coupled-cluster single-double plus perturbative triple and unrestricted-spin coupled-cluster single-double plus perturbative triple -F12x potential energy functions of P2H and P2H− The calculated infrared spectrum of Cl − H 2 O using a new full dimensional ab initio potential surface and dipole moment surfaceTheoretical studies of the potential surface and vibrational spectroscopy of CH 3 OH and its deuterated analogs Ab initio potential energy and dipole moment surfaces, infrared spectra, and vibrational predissociation dynamics of the 35 Cl − H 2 / D 2 complexes A six-dimensional potential energy surface ͑PES͒ for the singlet electronic ground state of C 3 H Ϫ has been generated by electronic structure calculations using the coupled cluster CCSD͑T͒ approach. Two potential minima are located: the global one, corresponding to an aromatic, cyclic structure ( 1 A 1 ), and a local one, lying about 0.56 eV higher in energy, with a trans chain structure ( 1 AЈ). Both minima are found to be separated by a relatively high barrier on the singlet surface but the isomerization process can also proceed via a coupling between the singlet and triplet PESs with a lower barrier. Variational calculations for the vibrational levels (Jϭ0) up to 3000 cm Ϫ1 were carried out for both isomers, taking into account the full dimensionality of the problem. The present results allow a clear distinction between the singlet isomers by infrared experiments. The structure of the vibrational and rotational stacks in both isomers is very different. For some vibrational overtones and combination levels inverse anharmonicity was found. The high density of the vibrational levels particularly in the chain structure suggests the existence of strong anharmonic resonances. In the bent isomer, the excited in-plane 5 and out-of-plane 6 modes fall into near-degenerate clusters of levels. Assignment Energy/cm Ϫ1 Assignment Energy/cm Ϫ1 ͑0,0,0,0,0,0͒ 0 ͑0,0,0,0,0,1͒ 297 ͑0,͑1,0,0,0,0,0͒ 2723 TABLE VI. Vibrational energy levels of b-C 3 D Ϫ . aЈ aЉ Assignment Energy/cm Ϫ1 Assignment Energy/cm Ϫ1͑0,0,0,0,0,0͒ 0 ͑0,0,0,0,0,1͒ 285 ͑0,0,0,0,1,0͒ 342 ͑0,0,0,0,1,1͒ 623 ͑0,0,0,0,0,2͒ 513 ͑0,0,0,0,0,3͒ 775 ͑0,0,0,0,2,0͒ 680 ͑0,0,0,0,2,1͒ 959 ͑0,