Nonlinear optical
(NLO) materials have several uses in many fields
such as solid physics, biology, medicine, nuclear physics, and material
research. Therefore, a series of nonfullerene-based derivatives (
CC10D1
–
CC10D8
) with a D−π–A
configuration was planned for the NLO investigation using
CC10R
as the reference molecule with structural alternations at acceptor
moieties. Natural bonding orbital (NBO), UV–vis spectra, frontier
molecular orbitals (FMOs), global reactivity parameters (GRPs), transition
density matrix (TDM), and density of states (DOS) were analyzed using
the M06/6-311G(d,p) functional in chloroform solvent to understand
the NLO responses of
CC10R
and
CC10D1
–
CC10D8
. The highest occupied molecular orbital (HOMO)–lowest
unoccupied molecular orbital (LUMO) band gaps of
CC10D1
–
CC10D6
were illustrated to be lower than that
of
CC10R
, with the larger bathochromic shift (726.408–782.674
nm) resulting in a significant NLO response. Along with the band gap,
the FMO method also identified an efficient interfacial charge transfer
from D to A moieties
via
a π-bridge, which
was further supported by the DOS and TDM map. Moreover, NBO calculations
demonstrated that extended hyperconjugation and strong internal molecular
interactions were important in their stabilization. The dipole moment
(μ), linear polarizability ⟨α⟩, hyperpolarizability
(β
total
), and second-order hyperpolarizability (γ
total.
) were studied for
CC10R
and
CC10D1
–
CC10D8
. Among all of the derivatives,
CC10D2
was proven to be the most appropriate candidate because
of its suitable NLO behavior such as being well-supported by a reduced
band gap (2.093 eV) and having a suitable maximum absorption wavelength
(782.674 nm). Therefore,
CC10D2
was reported to have
a greater value of first hyperpolarizability (208 659.330 a.u.)
compared with other derivatives and
CC10R
. For the second
hyperpolarizability, a greater value was obtained for
CC10R
(5.855 × 10
7
a.u.), and its derivatives showed results
comparable to that of the parent chromophore for γ
total
. This theoretical framework reveals that structural customization
with different acceptor units plays a significant role in obtaining
attractive NLO materials for optoelectronic applications.