5 research outputs found
Geometrical and Electronic Characteristics of Au<i><sub>n</sub></i>O<sub>2</sub><sup>–</sup> (<i>n</i> = 2–7)
Most
density functionals do not properly describe the characteristics
of superoxide (O<sub>2</sub><sup>–</sup>) (i.e., first two
vertical electron detachment energies and the excitation energies
of neutralized singlet state) of small even-numbered Au<i><sub>n</sub></i>O<sub>2</sub><sup>–</sup> clusters. However,
the second-order Møller–Plesset theory (MP2) shows significant
charge transfer from Au cluster anions to oxygen molecule and so provides
proper electronic characteristics of superoxide of small even-numbered
Au<i><sub>n</sub></i>O<sub>2</sub><sup>–</sup> clusters.
This has allowed us to properly describe the properties of even-numbered
Au<i><sub>n</sub></i>O<sub>2</sub><sup>–</sup> clusters.
Even in the case of odd-numbered Au<i><sub>n</sub></i>O<sub>2</sub><sup>–</sup> clusters, we find that Au<sub>5</sub><sup>–</sup> is a chemically O<sub>2</sub>-adsorbed singlet state
at 0 K, against a commonly accepted physisorbed triplet state. This
is further evidenced by our extensive coupled cluster with single,
double, and perturbative triple excitations [CCSDÂ(T)] calculations,
including the relativistic effect. However, the entropy effect makes
the physisorbed triplet state more stable than the chemisorbed singlet
state at higher temperatures, consistent with the experiment. The
weak O<sub>2</sub> binding by odd-numbered cluster anions (<i>n</i> = 3, 5, and 7) could be further weakened by the entropic
effect, which results in van der Waals complexes at high temperatures.
The present study reports the geometrical and electronic characteristics
of small Au<i><sub>n</sub></i>O<sub>2</sub><sup>–</sup> (<i>n</i> = 2–7) clusters including isomers, which
match the corresponding photoelectron spectra (PES)
Triazine-Based Microporous Polymers for Selective Adsorption of CO<sub>2</sub>
Propeller-shaped triazine was used
to synthesize microporous polycarbazole
materials through an inexpensive FeCl<sub>3</sub>-catalyzed reaction
using direct oxidative coupling (PCBZ) and extensive cross-linking
(PCBZL) polymerization routes. PCBZL has a Brunauer–Emmett–Teller
specific surface area of 424 m<sup>2</sup> g<sup>–1</sup> and
shows larger CO<sub>2</sub> uptake (64.1 mg g<sup>–1</sup> at
273 K, 1 atm). Selective adsorption of CO<sub>2</sub> over N<sub>2</sub> calculated using the ideal adsorbed solution theory shows that both
PCBZ (125) and PCBZL (148) exhibit selectivity at 298 K, which is
significantly higher than PCBZ (110) and PCBZL (82) at 273 K. These
values of selectivity are among the highest reported for any triazine-based
microporous material. By introducing the electron-rich carbazole structure
into the nitrogen fertile triazine-based system, the adsorption enthalpy
is increased drastically, which in turn contributes to high selective
adsorption values. The larger existing binding energy between CO<sub>2</sub> and propeller specifies more stable and favorable interactions
between adsorbent and adsorbate, which transforms into reasonable
adsorption capacity at low pressure and eventually high selectivity.
These polymeric networks also show moderate working capacity with
high regenerability factors. The combination of a simple inexpensive
synthesis approach, high thermal/chemical stability, and reasonable
selective adsorption make these materials potential candidates for
CO<sub>2</sub> storage and separation applications
Anion Binding by Electron-Deficient Arenes Based on Complementary Geometry and Charge Distribution
Extended electron-deficient arenes are investigated as potential neutral receptors for polyanions. Anion binds via σ interaction with extended arenes, which are composed solely of C and N ring atoms and CN substituents. As a result, the positive charge on the aromatic C is enhanced, consequently maximizing binding strength. Selectivity is achieved because different charge distributions can be obtained for target anions of a particular geometry. The halides F<sup>–</sup> and Cl<sup>–</sup> form the most stable complex with <b>6</b>, while the linear N<sub>3</sub><sup>–</sup> interacts most favorably with <b>7</b>. The trigonal NO<sub>3</sub><sup>–</sup> and tetrahedral ClO<sub>4</sub><sup>–</sup> fit the 3-fold rotational axis of <b>6</b> but do not form stable complexes with <b>5</b> and <b>7</b>. The Y-shaped HCOO<sup>–</sup> forms complexes with <b>4</b>, <b>5</b>, and <b>7</b>, with the latter being the most stable. Thus, the anion complexes exhibit strong binding and the best geometrical fit between guest and host, reminiscent of Lego blocks
CO<sub>2</sub> Capturing Mechanism in Aqueous Ammonia: NH<sub>3</sub>-Driven Decomposition−Recombination Pathway
Capturing CO<sub>2</sub> by aqueous ammonia has recently received much attention due to its advantages over other state-of-the-art CO<sub>2</sub>-capture technology. Thus, understanding this CO<sub>2</sub>-capturing mechanism, which has been causing controversy, is crucial for further development toward advanced CO<sub>2</sub> capture. The CO<sub>2</sub> conversion mechanism in aqueous ammonia is investigated using ab initio calculations and kinetic simulations. We show full details of all reaction pathways for the NH<sub>3</sub>-driven conversion mechanism of CO<sub>2</sub> with the pronounced effect of microsolvation. Ammonia performs multiple roles as reactant, catalyst, base, and product controller. Both carbamic and carbonic acids are formed by the ammonia-driven trimolecular mechanism. Ammonia in microsolvation makes the formation of carbamic acid kinetically preferred over carbonic acid. As the concentration of CO<sub>2</sub> increases, the dominant product becomes carbonic acid. The conversion from carbamic acid into carbonic acid occurs through the decomposition−recombination pathway. This understanding would be exploited for the optimal CO<sub>2</sub> capture technology
Halogen−π Interactions between Benzene and X<sub>2</sub>/CX<sub>4</sub> (X = Cl, Br): Assessment of Various Density Functionals with Respect to CCSD(T)
Various
types of interactions between halogen (X) and π moiety
(X−π interaction) including halogen bonding play important
roles in forming the structures of biological, supramolecular, and
nanomaterial systems containing halogens and aromatic rings. Furthermore,
halogen molecules such as X<sub>2</sub> and CX<sub>4</sub> (X = Cl/Br)
can be intercalated in graphite and bilayer graphene for doping and
graphene functionalization/modification. Due to the X−π
interactions, though recently highly studied, their structures are
still hardly predictable. Here, using the coupled-cluster with single,
double, and noniterative triple excitations (CCSDÂ(T)), the Møller–Plesset
second-order perturbation theory (MP2), and various flavors of density
functional theory (DFT) methods, we study complexes of benzene (Bz)
with halogen-containing molecules X<sub>2</sub> and CX<sub>4</sub> (X = Cl/Br) and analyze various components of the interaction energy
using symmetry adapted perturbation theory (SAPT). As for the lowest
energy conformers (S1), X<sub>2</sub>–Bz is found to have the
T-shaped structure where the electropositive X atom-end of X<sub>2</sub> is pointing to the electronegative midpoint of CC bond of the Bz
ring, and CX<sub>4</sub>–Bz has the stacked structure. In addition
to this CX<sub>4</sub>–Bz (S1), other low energy conformers
of X<sub>2</sub>–Bz (S2/S3) and CX<sub>4</sub>–Bz (S2)
are stabilized primarily by the dispersion interaction, whereas the
electrostatic interaction is substantial. Most of the density functionals
show noticeable deviations from the CCSDÂ(T) complete basis set (CBS)
limit binding energies, especially in the case of strongly halogen-bonded
conformers of X<sub>2</sub>–Bz (S1), whereas the deviations
are relatively small for CX<sub>4</sub>–Bz where the dispersion
is more important. The halogen bond shows highly anisotropic electron
density around halogen atoms and the DFT results are very sensitive
to basis set. The unsatisfactory performance of many density functionals
could be mainly due to less accurate exchange. This is evidenced from
the good performance by the dispersion corrected hybrid and double
hybrid functionals. B2GP-PLYP-D3 and PBE0-TSÂ(Tkatchenko-Scheffler)/D3
are well suited to describe the X−π interactions adequately,
close to the CCSDÂ(T)/CBS binding energies (within ∼1 kJ/mol).
This understanding would be useful to study diverse X−π
interaction driven structures such as halogen containing compounds
intercalated between 2-dimensional layers