5 research outputs found
Second-Order Nonlinear Optical Response of Electron Donor–Acceptor Hybrids Formed between Corannulene and Metallofullerenes
A charge
transfer (CT) complex was formed between C<sub>20</sub>H<sub>10</sub> and Li<sup>+</sup>@C<sub>60</sub> in the ground state
by the concave–convex π–π CT interaction.
Herein, the structures, binding interactions, electronic absorption
spectra, and first hyperpolarizabilities of a series of Li<sup>+</sup> and Li atom in contact with C<sub>60</sub> have been explored with
density functional theory methods. It is found that independent of
the doping position, doping Li atom can significantly narrow the wide
gap between the highest occupied molecular orbital (HOMO) and the
lowest unoccupied molecular orbital (LUMO) (<i>E</i><sub>gap</sub> = 2.82 eV) of the pure C<sub>20</sub>H<sub>10</sub>/C<sub>60</sub> in the range of 0.86–0.99 eV. Among them, the Li-doped
outer isomer C<sub>20</sub>H<sub>10</sub>/LiC<sub>60</sub> can exhibit
the intriguing n-type characteristic, where a high energy level containing
the excess electron is introduced as the new HOMO orbital in the original
gap of C<sub>20</sub>H<sub>10</sub>/C<sub>60</sub>. Furthermore, the
diffuse excess electron also brings C<sub>20</sub>H<sub>10</sub>/C<sub>60</sub> the considerable first hyperpolarizability, which is 3.53
× 10<sup>–29</sup> esu. When Li<sup>+</sup> and Li were
encapsulated into the C<sub>60</sub> cage, inner complexes C<sub>20</sub>H<sub>10</sub>/Li<sup>+</sup>@C<sub>60</sub> and C<sub>20</sub>H<sub>10</sub>/Li@C<sub>60</sub> of enhanced static first hyperpolarizabilities
(5.39 and 2.13 × 10<sup>–29</sup> esu, respectively) are
also delivered due to that encapsulated Li<sup>+</sup>@C<sub>60</sub> and Li@C<sub>60</sub> show enhanced electron acceptability as compared
to pristine C<sub>60</sub>, leading to more obvious intermolecular
CT transitions. From a certain point of view, such systems can be
considered as high-performance NLO materials that combine the basic
characteristics of a classical donor–acceptor superstructure
and systems with cations and easily polarizable excess electrons
Impact of Redox Stimuli on Ferrocene–Buckybowl Complexes: Switchable Optoelectronic and Nonlinear Optical Properties
A series of redox-active complexes <b>1</b>–<b>3</b> (1,1′-diquadrannulenylferrocene,
1,1′-dicorannulenylferrocene,
1,1′-disumanenylferrocene) and their corresponding conformational
isomers that are composed of ferrocene donor and various acceptors
of different buckybowl (open bowl-shaped polyaromatic hydrocarbon)
subunits have been investigated by density functional theory. The
nature of the redox property makes it possible to develop novel examples
of chromophores that are amenable to molecular switches, which can
therefore be used in optical devices. The complexes <b>1</b>–<b>3</b>, with high thermal and chemical stabilities,
show π–π stacking interaction between two buckybowl
subunits, and support for the presence of significant donor–acceptor
interaction was obtained from the employment of the natural bond orbital
charge and charge decomposition analysis. Both one-electron oxidation
and one- and two-electron reduction have been considered. The results
show some important electronic structure changes upon oxidation/reduction
that are accompanied by significant differences in the corresponding
absorption spectra and second-order nonlinear optical properties.
These differences are due to a change in the charge transfer pattern.
The redox switch ability suggests that these ferrocene–buckybowl
complexes can be viewed as redox-triggered nonlinear optical switches
with one of the complexes having an on/off ratio of 100.2 for the
hyperpolarizability values. Thus, our work has helped to establish
ferrocene–buckybowl complexes as versatile and fascinating
nonlinear optical switching compounds with a promising future
Second-Order Nonlinear Optical Responses and Concave–Convex Interactions of Size-Selective Fullerenes/Corannulene Recognition Pairs: The Effect of Fullerene Size
The
size-selective formation of eight molecular recognition pairs
between the host corannulene and fullerene guest of various size have
been studied by taking advantage of concave–convex π–π
interactions. Herein, the structures, binding interactions, electronic
absorption spectra, and first hyperpolarizabilities have been explored
using density functional theory calculations. It is found that with
the aim to maximize the concave–convex shape complementarity,
the base of fullerene can be modified at certain angles with the central
ring plane of C<sub>20</sub>H<sub>10</sub> (0° for complexes <b>1</b>–<b>4</b> and 46°, 34°, 19°,
and 5° for complexes <b>5</b>–<b>8</b>, respectively).
The interaction energies depend linearly on the convex surface area
and the size of the fullerene sphere. Further, the results of first
hyperpolarizabilities show that the shape of the fullerene is the
dominant factor for complexes <b>1</b>–<b>4</b> because of the intramolecular charge transfer (CT) within fullerene
cage. Among them, complex <b>4</b> presents the largest β<sub>tot</sub> value as 5.64 × 10<sup>–30</sup> esu because
of the more obvious intramolecular CT from the upper part to the bottom
part of the C<sub>70</sub> cage, derived from the larger height of
the cage. On the other hand, low-lying CT character accounts for a
large part of the first hyperpolarizability. The achieved understanding
provides the prospect of size-selective strategy for enhancing the
concave–convex interaction and second order nonlinear optical
response in the recognition of fullerenes
Large Nonlinear Optical Responses of Dimers Bearing a Donor and Acceptor: Long, Intradimer Multicenter Bonding
Unusual long, multicenter dimers
bearing a large electron donor
and acceptor have been the subject of great interest over the last
decades due to their better conducting, superconducting, magnetic,
or other physical properties. Two-electron, multicenter bonding between
two interplanar fragments has been recently recognized as a novel
and important bonding interaction. Herein, the [TTF]Â[TCNE], [TTF]Â[TCNQ],
[TTF]Â[TCNP], and [TTF]Â[TCNB] dimeric species have been studied by
quantum mechanics methods with the view of assessing their interactions
and first hyperpolarizabilities. It is found that the stabilities
of the dimers primarily originate from the electrostatic bonding component.
Although to a lesser extent, long, multicenter interactions due to
the overlap of the molecular orbitals of the monomers are important
also in the stability of these systems. Significantly, a severe hyperpolarizability
decrease with changing the acceptor monomers of the dimeric species
is qualitatively explained in terms of change in their charge transfer
patterns. It indicates that the first hyperpolarizabilities of these
dimers can be optimized by controlling their relative acceptor monomers.
We believe that these results shall provide important information
for further exploration of long, multicenter dimers with versatile
and fascinating nonlinear optical properties
Strategy for Enhancing Second-Order Nonlinear Optical Properties of the Pt(II) Dithienylethene Complexes: Substituent Effect, π‑Conjugated Influence, and Photoisomerization Switch
The second-order nonlinear optical
(NLO) properties of a series
of PtÂ(II) dithienylethene (DTE) complexes possessing the reversible
photochromic behavior have been investigated by density functional
theory (DFT) combined with the analytic derivatives method. The results
show that the calculated static first hyperpolarizabilities (β<sub>tot</sub>) of the open-ring and closed-ring systems significantly
increase in the range of 2.1–4.5 times through strengthening
of the electron-withdrawing ability of the substituent R (R = H, CF<sub>3</sub>, NO<sub>2</sub>) and an increase of the number of thiophene
rings. Moreover, there is a large enhancement of the β<sub>tot</sub> values from the open-ring systems to the corresponding closed-ring
systems. This efficient enhancement is attributed to the better delocalization
of the π-electron system, the more obvious degree of charge
transfer, and the larger <i>f</i><sub>os</sub>/<i>E</i><sub>gm</sub><sup>3</sup> (<i>f</i><sub>os</sub> is the
oscillator strength, and <i>E</i><sub>gm</sub> is the transition
energy between the ground and the excited states) values in the closed
forms according to the bond length alternation (BLA) and time-dependent
density functional theory (TDDFT) calculations. In addition, the dispersion
has less influence on the frequency-dependent first hyperpolarizabilities
(β<sub>tot</sub>(ω)) of the studied systems at the low-frequency
area ω (0.000–0.040 au). Our present work would be beneficial
for further theoretical and experimental studies on large second-order
NLO responses of metal complexes