The
geometries and energetics of the ground and lower-lying singlet
excited states S<sub>0</sub>, L<sub>a</sub>, and L<sub>b</sub> of
1-naphthol (NpOH)–(NH<sub>3</sub>)<sub><i>n</i></sub> (<i>n</i> = 0–5) clusters have been computed using
density functional theory (DFT) and time-dependent density functional
theory (TD-DFT) methods. Cluster size dependence of the excited state
proton transfer (ESPT) reaction was investigated by the vertical transitions
from the geometries that can be populated in the molecular beam experiments.
For the <i>n</i> = 3 and 4 clusters, the proton-transferred
geometries cannot be accessible without significant geometrical rearrangement
from the initially populated isomers. For the <i>n</i> =
5 clusters, the proton-transferred structure is found in the L<sub>a</sub> excited state of the isomer that can be populated in the
beam. Thus, ESPT is possible by the optically prepared L<sub>b</sub> state via internal conversion to L<sub>a</sub>. We concluded that
the threshold cluster size of ESPT is <i>n</i> = 5 under
the experimental condition with low excess energy.