CI-SD/ [ 3s2p] and MCSCF/ [ 3s2p] calculations were performed in order to obtain detailed information on the potential energy surface of Hz. Jahn-Teller distortions from the square geometry of H: are studied and it is shown that the optimal distorted geometries are slightly different from those obta
The potential energy surface of the jahn-teller-distorted 2E' ground state of copper trimer
β Scribed by Donald G. Truhlar; Todd C. Thompson; C.Alden Mead
- Publisher
- Elsevier Science
- Year
- 1986
- Tongue
- English
- Weight
- 462 KB
- Volume
- 127
- Category
- Article
- ISSN
- 0009-2614
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β¦ Synopsis
It is shown that the configuration interaction calculations of Walch and Laskowski for the ground 2E' state of Cus are consistent with truncating the potential energy at second order in the distance from the D,, conical intersection, which leads to a diabatic representation (the "quadratic coupling model") containing three parameters. Fitting these parameters to three of the vibronic spacings of Rohlfing and Valentini leads to a reasonable explanation of their spectrum. The resulting potential energy surfaces show a Jahn-Teller stabilization energy of 221 cm-' and a pseudorotation barrier of 95 cm-'.
π SIMILAR VOLUMES
Ab initio calculations elucidating the structure and the ring opening process of the cyclic CO, isomer are reported. An accurate electronic wavefunction is obtained by including all 16 valence electrons in the FORS model consisting of MCSCF calculations in the full space of all possible symmetry-res
Potential energy surface for methyl fluoride dimer has been studied theoretically with ab initio molecular orbital method, using a 4-31G basis set. Dimer dissociation energies, Mulliken electronic populations, and dipole moments were obtained.
The potential energy surface for the electronic ground state of CO 2 is refined by means of a two-step variational procedure using the exact rovibrational Hamiltonian in the bond length-bond angle coordinates. In the refinement, the observed rovibrational energy levels for J = 0-4 below 16,000 cm -1