Abstract
The dissociations of CH2 CHCN into CH2 CH+CN and CH2 C+HCN in the S0, T1, and π 1 2 π CN (definitions of π orbitals can refer to computational details) states, have been explored at the complete active space self-consistent field level of theory employing the Dunning correlation consistent triple-zeta basis set. The lowest energy points of the surface crossing seams have been searched. Two conical intersections, from π 1 CN π 1 to π 1 2 π 1 (CI1) and from π 1 2 π 1 to S0 (CI2), and one intersystem crossing point (T1 / S0) have been located. The energies of all critical points have been recomputed with the multiconfigurational second-order perturbation method. At each conical intersection, derivative coupling and unscaled gradient difference vectors have been analyzed to determine the relaxation channels that the molecule may evolve in after nonradiative decay. Once the molecule is photoexcited to the π 1 2 π 1 or π 1 CN π 1 state, it would relax along the similar pathway: funneling through CI1 and then CI2, and finally populate the ground state. Our results show that upon 193 nm photoexcitation, the most probable reaction channel is the ground-state HCN elimination following radiationless decays from excited states through surface crossings, which consists with experimental results J. Chem. Phys. 108, 5784 (1998). The investigated dissociation channels on the π 1 2 π CN surface, which are inaccessible upon 193 nm photoexcitation, may provide information for reactions induced by higher energy excitations.
| Original language | English |
|---|---|
| Article number | 174309 |
| Journal | Journal of Chemical Physics |
| Volume | 129 |
| Issue number | 17 |
| DOIs | |
| Publication status | Published - 2008 |
| Externally published | Yes |
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