The energetics of the loss of C2 units from Cw and C,a has been extensively studied experimentally, but no consensus has yet been reached as to the energy of C2 dissociation from these fullerenes. We have used the Hat-tree-Fock self-consistent field theory and a hybrid of Hartree-Fock and density fu
Theoretical studies of selected C60H2 and C70H2 isomers
โ Scribed by Craig C. Henderson; Celeste McMichael Rohlfing; Paul A. Cahill
- Publisher
- Elsevier Science
- Year
- 1993
- Tongue
- English
- Weight
- 467 KB
- Volume
- 213
- Category
- Article
- ISSN
- 0009-2614
No coin nor oath required. For personal study only.
โฆ Synopsis
Semi-empirical UNDO methods predict that 2 of 23 structurally distinct C6& isomers and 4 of 143 C7uH2 isomers have particularly low heats of formation. These isomers represent either 1 ,t-addition across a 6: 6-ring fusion or 1,4-addition across a ii-ring, with both hydrogens externally bound. Fully optimized ab initio structures are computed for these low-lying isomers at the Hartree-Fock level using 3-2 1 G and 6-3 1 G* basis sets. For C&I1, all three methods agree on the isomer ordering, and the lowest energy structure is also the only one that has been observed experimentally. The energy separations among the lowest four CI,-,Hz isomers are found to be quite small, but only the ab initio ordering is consistent with experimental results.
๐ SIMILAR VOLUMES
The relative energies of 18 isomers of C6oH 6 have been determined through geometry-optimized ab initio calculations. HF/6-31G\* computations on the two lowest energy structures determined at the HF/3-21G level indicate that 1,2,4,11,15,30-C6oH 6 (18, with a C6oBr6-1ike structure) lies only 0.4 kcal
The successive C-H bond dissociation energies of CH,, &Hz. C2H4, and H&O (ketene) are determined using large basis sets and a high level of correlation treatment. For CHI, C2H2, and C2H4 the computed values are in excellent agreement with experiment. Using our results we recommend 107.9 +2.0 and 96.
Ab initio molecular orbltal calculations on the transitton states and barrter heights for the addition of atomtc hydrogen to sllaethylene are carried out. The activation energy for the addition to the silicon site is lower than that to the carbon site, wlnle the exothermicity 1s smaller.
By combining photoionization and photodissociation measurements with ab initio Gaussian-Z (G2) calculations on the CZHSS and C2H$+ system, we have concluded that CHsCH2S is the dominant primary product formed in the 193 nm photodissociation of (CH,CH&S, while CH,CHSH+ is the product ion formed at th