We have investigated the suitability
of Time-Dependent Density
Functional Theory (TD-DFT) to describe vertical low-energy excitations
in naked and hydrated titanium dioxide nanoparticles. Specifically,
we compared TD-DFT results obtained using different exchange-correlation
(XC) potentials with those calculated using Equation-of-Motion Coupled
Cluster (EOM-CC) quantum chemistry methods. We demonstrate that TD-DFT
calculations with commonly used XC potentials (e.g., B3LYP) and EOM-CC
methods give qualitatively similar results for most TiO2 nanoparticles investigated. More importantly, however, we also show
that, for a significant subset of structures, TD-DFT gives qualitatively
different results depending upon the XC potential used and that only
TD-CAM-B3LYP and TD-BHLYP calculations yield results that are consistent
with those obtained using EOM-CC theory. Moreover, we demonstrate
that the discrepancies for such structures originate from a particular
combination of defects that give rise to charge-transfer excitations,
which are poorly described by XC potentials that do not contain sufficient
Hartree–Fock like exchange. Finally, we consider that such
defects are readily healed in the presence of ubiquitously present
water and that, as a result, the description of vertical low-energy
excitations for hydrated TiO2 nanoparticles is nonproblematic.