Methyl
2-cyano-3,3-diphenylacrylate (MCDPA) shares the same molecular
skeleton with octocrylene (OCR) that is one of the most common molecules
used in commercially available sunscreens. However, its excited-state
relaxation mechanism is unclear. Herein, we have used the QM(CASPT2//CASSCF)/MM
method to explore spectroscopic properties, geometric and electronic
structures, relevant conical intersections and crossing points, and
excited-state relaxation paths of MCDPA in methanol solution. We found
that in the Franck–Condon (FC) region, the V(1ππ*)
state is energetically lower than the V′(1ππ*)
state only by 2.8 kcal/mol and is assigned to experimentally observed
maximum absorption band. From these two initially populated singlet
states, there exist three nonradiative relaxation paths to repopulate
the S0 state. In the first one, when the V(1ππ*) state is populated in the FC region, the system
diabatically evolves along the V(1ππ*) state
into its minimum where the internal conversion to S0 occurs.
In the second one, the V′(1ππ*) state
is populated in the FC region and the system adiabatically overcomes
a barrier of ca. 3.0 kcal/mol to approach the V(1ππ*)
minimum eventually leading to a V(1ππ*)-to-S0 internal conversion. In the third one, the V′(1ππ*) state first hops via the intersystem crossing
to the T2 state, which then decays through the internal
conversion to the T1 state. The T1 state is
finally converted to the S0 state via the T1/S0 crossing point. Our present work contributes to understanding
the photophysics of OCR and its variants.