In this contribution
we present a mixed quantum-classical dynamical
approach for the computation of vibronic absorption spectra of molecular
aggregates and their nonadiabatic dynamics, taking into account the
coupling between local excitations (LE) and charge-transfer (CT) states.
The approach is based on an adiabatic (Ad) separation between the
soft degrees of freedom (DoFs) of the system and the stiff vibrations,
which are described by the quantum dynamics (QD) of wave packets (WPs)
moving on the coupled potential energy surfaces (PESs) of the LE and
CT states. These PESs are described with a linear vibronic coupling
(LVC) Hamiltonian, parameterized by an overlap-based diabatization
on the grounds of time-dependent density functional theory computations.
The WPs time evolution is computed with the multiconfiguration time-dependent
Hartree method, using effective modes defined through a hierarchical
representation of the LVC Hamiltonian. The soft DoFs are sampled with
classical molecular dynamics (MD), and the coupling between the slow
and fast DoFs is included by recomputing the key parameters of the
LVC Hamiltonians, specifically for each MD configuration. This method,
named Ad-MD|gLVC, is applied to a perylene diimide (PDI) dimer in
acetonitrile and water solutions, and it is shown to accurately reproduce
the change in the vibronic features of the absorption spectrum upon
aggregation. Moreover, the microscopic insight offered by the MD trajectories
allows for a detailed understanding of the role played by the fluctuation
of the aggregate structure on the shape of the vibronic spectrum and
on the population of LE and CT states. The nonadiabatic QD predicts
an extremely fast (∼50 fs) energy transfer between the two
LEs. CT states have only a moderate effect on the absorption spectrum,
despite the fact that after photoexcitation they are shown to acquire
a fast and non-negligible population, highlighting their relevance
in dictating the charge separation and transport in PDI-based optical
devices.