In most implementations reported in the literature so far, DFT excitations used
for surface hopping are obtained either from linear-response time-dependent theory
or from bare KS gaps. Currently, we observe great effort from different research
groups to generalize the methods for different kinds of nonadiabatic interactions, to
provide better theoretical foundations, and to improve the hopping algorithms. The
availability of SH/DFT in a small amount of public computational-chemistry
software has also helped to popularize the method.
SH/DFT very successfully expanded the range of systems which can be
approached for nonadiabatic dynamics investigations. We should, however, be
aware that many methodological restrictions remain and must still be properly
addressed. Such restrictions involve intrinsic limitations in the semi-classical
local approach for nonadiabatic dynamics, in the sampling of statistical ensembles,
and, more fundamentally, in the quality of the DFT excited-state predictions. In
particular, the multireference character of regions of energy crossing between the
excited and the ground states is still a challenge waiting for better solutions than
those so far available.
Acknowledgments We would like to thank Dr. Michael Filatov for kindly providing the REKS
data for Fig. 3 and also Dr. W. Arbelo-Gonza ´lez, Dr. Fazzi, Dr. G. Rodrigues, and Dr. T. Very for
helpful discussions.
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