19 research outputs found
Nonplanar Donor–Acceptor Chiral Molecules with Large Second-Order Optical Nonlinearities: 1,1,4,4-Tetracyanobuta-1,3-diene Derivatives
We
have investigated the chiroptical, linear, and second-order
nonlinear optical (NLO) properties of five 1,1,4,4-tetracyanobuta-1,3-diene
(TCBD) derivatives and elucidated structure–property relationships
from the micromechanism. The experimental UV–vis absorption
and circular dichroism (CD) spectra were well reproduced by our calculations
at TDB3LYP/6-31+G* level of theory. The electron transition property
and chiroptical origin have been assigned and analyzed. The results
show that the studied compounds possess large molecular first hyperpolarizabilities,
especially for compound <b>5</b> which has a value of 35 ×
10<sup>–30</sup> esu, which is comparable with the measured
value for highly π-delocalized phenyliminomethyl ferrocene complex
and about 200 times larger than the average first hyperpolarizability
of the organic urea molecule. Despite the nonplanarity of these compounds,
efficient intramolecular charge transfer (CT) from electron donor
to electron acceptor moieties was observed, which plays the key role
in determining the NLO response. The intramolecular charge transfer
cooperativity was also probed. In view of the first hyperpolarizability
values, intrinsic noncentrosymmetric electronic structure, and high
stability, the studied compounds have the possibility to be excellent
second-order NLO materials
A Stable, Magnetic, and Metallic Li<sub>3</sub>O<sub>4</sub> Compound as a Discharge Product in a Li–Air Battery
The
Li–air battery with the specific energy exceeding that of a
Li ion battery has been aimed as the next-generation battery. The
improvement of the performance of the Li–air battery needs
a full resolution of the actual discharge products. Li<sub>2</sub>O<sub>2</sub> has been long recognized as the main discharge product,
with which, however, there are obvious failures on the understanding
of various experimental observations (e.g., magnetism, oxygen K-edge
spectrum, etc.) on discharge products. There is a possibility of the
existence of other Li–O compounds unknown thus far. Here, a
hitherto unknown Li<sub>3</sub>O<sub>4</sub> compound as a discharge
product of the Li–air battery was predicted through first-principles
swarm structure searching calculations. The new compound has a unique
structure featuring the mixture of superoxide O<sub>2</sub><sup>–</sup> and peroxide O<sub>2</sub><sup>2–</sup>, the first such example
in the Li–O system. The existence of superoxide O<sub>2</sub><sup>–</sup> creates magnetism and hole-doped metallicity.
Findings of Li<sub>3</sub>O<sub>4</sub> gave rise to direct explanations
of the unresolved experimental magnetism, triple peaks of oxygen K-edge
spectra, and the Raman peak at 1125 cm<sup>–1</sup> of the
discharge products. Our work enables an opportunity for the performance
of capacity, charge overpotential, and round-trip efficiency of the
Li–air battery
Theoretical Study on the Chiroptical Optical Properties of Chiral Fullerene C<sub>60</sub> Derivative
Time-dependent density functional theory (TDDFT) calculations have been used to investigate UV/CD spectra and nonlinear optical (NLO) property of the C<sub>60</sub>-fullerene bisadduct (<i>R</i>,<i>R</i>,<sup>f,s</sup><i>A</i>)-[CD(+)280] for the first time. The electron transition natures of the four main measured bands are analyzed, and their results are used to designate the excited states involved in an electron-transfer process of the studied compound. On a comparative scale, the predicted excitation energies and oscillator strengths are in reasonable agreement with the observed values, demonstrating the efficiency of TDDFT in predicting the localized and charge transfer transitions. The good agreement between the experimental and the simulated CD spectra shows that TDDFT calculations can be used to assign the absolute configurations (ACs) of chiral fullerene C<sub>60</sub> derivatives with high confidence. The observed large dissymmetry ratio <i>g</i> (<i>g</i> = Δε/ε) at about 700 nm results from the orbital characters of the local fullerene excited state, which leads to large transition magnetic dipole moment and small transition electronic dipole moment. The different functionals and solvent effects on UV/CD spectra were also considered. The studied compound has a possibility to be an excellent second-order NLO material from the standpoint of transparency and large second-order polarizability value
Photophysical Properties of Chiral Tetraphenylethylene Derivatives with the Fixed Propeller-Like Conformation
The
recent synthesized helical tetraphenylethylene (TPE) exhibits
broad application prospects such as display, catalysis, and medical
imaging. A full understanding of the intricate relation between structure
and property is rather important to structural design and performance
improvement. Here, we employed density functional theory (DFT) and
time-dependent DFT to calculate their ground- and excited-state structures,
electron transition properties, optical rotation (OR), and second-order
nonlinear optical (NLO) properties. For compound <b>1</b>, the
simulated UV–vis/CD spectra and calculated OR value are in
reasonable agreement with the experimental ones, allowing us to reliably
assign the electron transition and determine the absolute configuration.
Intriguingly, TPE derivatives are excellent candidates for the second-order
NLO materials in view of the large first hyperpolarizability values
and intrinsic asymmetric structures. The intramolecular charge transfer
cooperativity for this kind of compound was achieved through involvement
of the donor and acceptor substituent groups or their combinations.
The charge transfer within TPE plays a key role in determining the
chiral origin and electron transition properties, whereas the contribution
of peripheral phenyl rings is fairly small. Moreover, the designed
compounds <b>5</b> and <b>7</b> are potential materials
for the fluorescent probe
Silicon Framework-Based Lithium Silicides at High Pressures
The bandgap and optical properties
of diamond silicon (Si) are
not suitable for many advanced applications such as thin-film photovoltaic
devices and light-emitting diodes. Thus, finding new Si allotropes
with better bandgap and optical properties is desirable. Recently,
a Si allotrope with a desirable bandgap of ∼1.3 eV was obtained
by leaching Na from NaSi<sub>6</sub> that was synthesized under high
pressure [<i>Nat. Mater.</i> <b>2015</b>, <i>14</i>, 169], paving the way to finding new Si allotropes. Li
is isoelectronic with Na, with a smaller atomic core and comparable
electronegativity. It is unknown whether Li silicides share similar
properties, but it is of considerable interest. Here, a swarm intelligence-based
structural prediction is used in combination with first-principles
calculations to investigate the chemical reactions between Si and
Li at high pressures, where seven new compositions (LiSi<sub>4</sub>, LiSi<sub>3</sub>, LiSi<sub>2</sub>, Li<sub>2</sub>Si<sub>3</sub>, Li<sub>2</sub>Si, Li<sub>3</sub>Si, and Li<sub>4</sub>Si) become
stable above 8.4 GPa. The Siî—¸Si bonding patterns in these compounds
evolve with increasing Li content sequentially from frameworks to
layers, linear chains, and eventually isolated Si ions. Nearest-neighbor
Si atoms, in <i>Cmmm</i>-structured LiSi<sub>4</sub>, form
covalent open channels hosting one-dimensional Li atom chains, which
have similar structural features to NaSi<sub>6</sub>. The analysis
of integrated crystal orbital Hamilton populations reveals that the
Siî—¸Si interactions are mainly responsible for the structural
stability. Moreover, this structure is dynamically stable even at
ambient pressure. Our results are also important for understanding
the structures and electronic properties of Liî—¸Si binary compounds
at high pressures
Barium in High Oxidation States in Pressure-Stabilized Barium Fluorides
The
oxidation state of an element influences its chemical behavior
of reactivity and bonding. Finding unusual oxidation state of elements
is a theme of eternal pursuit. As labeled by an alkali-earth metal,
barium (Ba) invariably exhibits an oxidation state of +2 by a loss
of two 6s valence electrons while its inner 5p closed shell is known
to remain intact. Here, we show through the reaction with fluorine
(F) at high pressure that Ba exhibits a hitherto unexpected high oxidation
state greater than +2 in three pressure-stabilized F-rich compounds
BaF<sub>3</sub>, BaF<sub>4</sub>, and BaF<sub>5</sub>, where Ba takes
on the role of a 5p element by opening up its inert 5p shell. Interestingly
enough, these pressure-stabilized Ba fluorides share common structural
features of Ba-centered polyhedrons but exhibit a diverse variety
of electronic properties showing semiconducting, metallic, and even
magnetic behaviors. Our work modifies the traditional knowledge on
the chemistry of alkali-earth Ba element established at ambient pressure
and highlights the major role of pressure played in tuning the oxidation
state of elements
Pressure-Induced Stable Beryllium Peroxide
Beryllium
oxides, at ambient pressure, have been extensively studied due to
their unique chemical bonds and applications. However, the long-desirable
target beryllium peroxide (BeO<sub>2</sub>) has not been reported,
thus far. Currently, the application of pressure has become a powerful
tool in finding unusual stoichiometric compounds with exotic properties.
Here, swarm structural searches in combination with first-principles
calculations disclosed that the reaction of BeO and oxygen, at pressures
above 89.6 GPa, yields BeO<sub>2</sub>. Interestingly, this reaction
pressure is lower than the phase transition pressure (106 GPa) of
pure BeO. BeO<sub>2</sub> crystallizes in FeS<sub>2</sub>-type structure,
whose remarkable feature is that it contains peroxide group (O<sub>2</sub><sup>2–</sup>) with an O–O distance of 1.40
Å at 100 GPa. Notably, O<sub>2</sub><sup>2–</sup> is maintained
in the pressure range of 89.6–300 GPa. The chemical bonding
analysis shows that the uniformly distributed ionic Be–O and
covalent O–O bonding network plays a key role in determining
its structural stability. BeO<sub>2</sub> is a direct band gap nonmetal,
and its band gap becomes larger with increase of pressure, which is
in sharp contrast with BaO<sub>2</sub>. Moreover, phase diagram of
Be–O binary compounds with various Be<sub><i>x</i></sub>O<sub><i>y</i></sub> (<i>x</i> = 1–3, <i>y</i> = 1–6) compositions at pressures of up to 300 GPa
was reliably built. Our results are also important for enriching the
understanding of beryllium oxides
Structure and Electronic Properties of Fe<sub>2</sub>SH<sub>3</sub> Compound under High Pressure
Inspired
by the diverse properties of hydrogen sulfide, iron sulfide, and iron
hydrides, we combine first-principles calculations with structure
prediction to find stable structures of Fe–S–H ternary
compounds with various Fe<sub><i>x</i></sub>S<sub><i>y</i></sub>H<sub><i>z</i></sub> (<i>x</i> = 1–2; <i>y</i> = 1–2; <i>z</i> = 1–6) compositions under high pressure with the aim of finding
novel functional materials. It is found that Fe<sub>2</sub>SH<sub>3</sub> composition stabilizes into an orthorhombic structure with <i>Cmc</i>2<sub>1</sub> symmetry, whose remarkable feature is that
it contains dumbbell-type Fe with an Fe–Fe distance of 2.435
Ã… at 100 GPa, and S and H atoms directly bond with the Fe atoms
exhibiting ionic bonding. The high density of states at the Fermi
level, mainly coming from the contribution of Fe-3d, indicates that
it satisfies the Stoner ferromagnetic condition. Notably, its ferromagnetic
ordering gradually decreases with increasing pressure, and eventually
collapses at a pressure of 173 GPa. As a consequence, magnetic and
nonmagnetic transition can be achieved by controlling the pressure.
In addition, there is a very weak electron–phonon coupling
in <i>Cmc</i>2<sub>1</sub>-structured Fe<sub>2</sub>SH<sub>3</sub>. The different superconducting mechanisms between Fe<sub>2</sub>SH<sub>3</sub> and H<sub>3</sub>S were compared and analyzed
Gold as a 6p-Element in Dense Lithium Aurides
The
negative oxidation state of gold (Au) has drawn a great attention
due to its unusual valence state that induces exotic properties in
its compounds, including ferroelectricity and electronic polarization.
Although monatomic anionic gold (Au<sup>–</sup>) has been reported,
a higher negative oxidation state of Au has not been observed yet.
Here we propose that high pressure becomes a controllable method for
preparing high negative oxidation state of Au through its reaction
with lithium. First-principles calculations in combination with swarm
structural searches disclosed chemical reactions between Au and Li
at high pressure, where stable Li-rich aurides with unexpected stoichiometries
(e.g., Li<sub>4</sub>Au and Li<sub>5</sub>Au) emerge. These compounds
exhibit intriguing structural features like Au-centered polyhedrons
and a graphene-like Li sublattice, where each Au gains more than one
electron donated by Li and acts as a 6p-element. The high negative
oxidation state of Au has also been achieved through its reactions
with other alkali metals (e.g., Cs) under pressures. Our work provides
a useful strategy for achieving diverse Au anions
Gold with +4 and +6 Oxidation States in AuF<sub>4</sub> and AuF<sub>6</sub>
An important goal
in chemistry is to prepare compounds with unusual
oxidation states showing exciting properties. For gold (Au), the relativistic
expansion of its 5d orbitals makes it form high oxidation state compounds.
Thus far, the highest oxidation state of Au known is +5. Here, we
propose high pressure as a controllable method for preparing +4 and
+6 oxidation states in Au via its reaction with fluorine. First-principles
swarm-intelligence structure search identifies two hitherto unknown
stoichiometric compounds, AuF<sub>4</sub> and AuF<sub>6</sub>, exhibiting
typical molecular crystal character. The high-pressure phase diagram
of Au fluorides is rather different from Cu or Ag fluorides, which
is indicated by stable chemical compositions and the pressures needed
for the synthesis of these compounds. This difference can be associated
with the stronger relativistic effects in Au relative to Cu or Ag.
Our work represents a significant step forward in a more complete
understanding of the oxidation states of Au