Potential-energy surfaces for ultrafast photochemistry - Static and dynamic aspects

Citation
M. Garavelli et al., Potential-energy surfaces for ultrafast photochemistry - Static and dynamic aspects, FARADAY DIS, (110), 1998, pp. 51-70
Citations number
46
Categorie Soggetti
Physical Chemistry/Chemical Physics
Journal title
Faraday discussions
ISSN journal
13596640 → ACNP
Issue
110
Year of publication
1998
Pages
51 - 70
Database
ISI
SICI code
1359-6640(1998):110<51:PSFUP->2.0.ZU;2-8
Abstract
The first singlet excited states (S-1) which control the ultrafast (i.e. su bpicosecond) photochemistry of 2-cis-penta-2,4-dieniminium cation (2-cis-C5 H6NH2+), all-trans-hexa-1,3,5-triene (all-trans-HT) and cyclohexa-1,3-diene (CHD) have been investigated using ab initio MCSCF and multireference MP2 theories. The structure of the corresponding potential energy surfaces (PES s) has been characterized by computing novel unconstrained and symmetry-con strained minimum-energy paths (MEP) starting from Franck-Condon and S-2/S-1 conical intersection points on S-1. Furthermore, analytical frequency comp utations have been used to produce quantitative information on the surface curvature. We show that the S-1 energy surface is characterized by two domains, region I and region II. Region I controls the initial acceleration of the excited state molecule. In contrast, region II is a low-lying region of S-1 and co ntrols the evolution towards fully efficient decay to the ground state. The energy surface structure indicates that the double-bond isomerization of 2 -cis-C5H6NH2+ and all-trans-MT and the ring-opening of CMD are prototypes o f three classes of barrierless reactions characterized by a different excit ed state dynamics. In 2-cis-C5H6NK2+ and, more loosely, in all-trans-HT the initial relaxation results in the production of a totally symmetric S-1 tr ansient. The following triggering of the S-1 -->S-0 decay requires energy r edistribution along a symmetry-breaking (torsional) mode leading to an S-2/ S-1 conical intersection (CI). In contrast, the shape of region I of CHD in dicates that an almost direct (i.e. impulsive) motion towards an asymmetric S-1/S-0 CI occurs upon initial relaxation. Previously reported and novel s emi-classical trajectory computations and the available experimental eviden ce seem to support these conclusions.