28 research outputs found
Cucurbit[6]uril: A Possible Host for Noble Gas Atoms
Density
functional and ab initio molecular dynamics studies are
carried out to investigate the stability of noble gas encapsulated
cucurbit[6]uril (CB[6]) systems. Interaction energy, dissociation
energy and dissociation enthalpy are calculated to understand the
efficacy of CB[6] in encapsulating noble gas atoms. CB[6] could encapsulate
up to three Ne atoms having dissociation energy (zero-point energy
corrected) in the range of 3.4–4.1 kcal/mol, whereas due to
larger size, only one Ar or Kr atom encapsulated analogues would be
viable. The dissociation energy value for the second Ar atom is only
1.0 kcal/mol. On the other hand, the same for the second Kr is −0.5
kcal/mol, implying the instability of the system. The noble gas dissociation
processes are endothermic in nature, which increases gradually along
Ne to Kr. Kr encapsulated analogue is found to be viable at room temperature.
However, low temperature is needed for Ne and Ar encapsulated analogues.
The temperature–pressure phase diagram highlights the region
in which association and dissociation processes of Kr@CB[6] would
be favorable. At ambient temperature and pressure, CB[6] may be used
as an effective noble gas carrier. Wiberg bond indices, noncovalent
interaction indices, electron density, and energy decomposition analyses
are used to explore the nature of interaction between noble gas atoms
and CB[6]. Dispersion interaction is found to be the most important
term in the attraction energy. Ne and Ar atoms in one Ng entrapped
analogue are found to stay inside the cavity of CB[6] throughout the
simulation at 298 K. However, during simulation Ng<sub>2</sub> units
in Ng<sub>2</sub>@CB[6] flip toward the open faces of CB[6]. After
1 ps, one Ne atom of Ne<sub>3</sub>@CB[6] almost reaches the open
face keeping other two Ne atoms inside. At lower temperature (77 K),
all the Ng atoms in Ng<sub><i>n</i></sub>@CB[6] remain well
inside the cavity of CB[6] throughout the simulation time (1 ps)
DataSheet1_OsB9−: An Aromatic Osmium-Centered Monocyclic Boron Ring.docx
Transition-metal-centered monocyclic boron wheels are important candidates in the family of planar hypercoordinate species that show intriguing structure, stability and bonding situation. Through the detailed potential energy surface explorations of MB9− (M = Fe, Ru, Os) clusters, we introduce herein OsB9− to be a new member in the transition-metal-centered borometallic molecular wheel gallery. Previously, FeB9− and RuB9− clusters were detected by photoelectron spectroscopy and the structures were reported to have singlet D9h symmetry. Our present results show that the global minimum for FeB9− has a molecular wheel-like structure in triplet spin state with Cs symmetry, whereas its heavier homologues are singlet molecular wheels with D9h symmetry. Chemical bonding analyses show that RuB9− and OsB9− display a similar type of electronic structure, where the dual σ + π aromaticity, originated from three delocalized σ bonds and three delocalized π bonds, accounts for highly stable borometallic molecular wheels.</p
Donor–Acceptor vs Electron-Shared Bonding: Triatomic Si<sub><i>n</i></sub>C<sub>3–<i>n</i></sub> (<i>n</i> ≤ 3) Clusters Stabilized by Cyclic Alkyl(amino) Carbene
SinC3–n (n ≤ 3) clusters are interstellar
species that are transient in nature at ambient conditions. Herein,
the structure, stability, and nature of bonding in cyclic alkyl(amino)
carbene (cAAC) protected SinC3–n (n ≤ 3) clusters are studied in silico. The Si3(cAAC)3 complex
was previously reported to be synthesized in large scale. The present
results indicate that because the C–CcAAC bond is
stronger than the Si–CcAAC bond, C3(cAAC)3 and SiC2(cAAC)3 complexes have significantly
larger stability with respect to ligand dissociation than the Si3(cAAC)3 complex, while Si2C(cAAC)3 has almost the same stability as in the latter complex. Moreover,
considering the Si3(cAAC)3 complex as a precursor,
the hypothetical successive single Si substitution process by a single
C atom in Si3(cAAC)3 complex is exergonic in
nature. The bonding situation is analyzed by employing natural bond
orbital (NBO), electron density, and energy decomposition analyses
in combination with the natural orbital for chemical valence theory.
These studies show that the nature of bonding in C–CcAAC and Si–CcAAC bonds differs significantly from
each other. The former bonds are best described as an electron-shared
double bond, whereas the latter bonds are of donor–acceptor
type consisting of two components, Si←CcAAC σ-donation
and Si→CcAAC π-back-donation. Nevertheless,
in the former bonds, covalent character is larger than the ionic one
but in the latter bonds the reverse is true. For some Si–CcAAC bonds, the π-natural orbital cannot be located by
the NBO method, presumably because of slightly lower occupancy than
the cutoff values, but the electron density analysis confirms that
different Si–CcAAC bonds in a given complex are
almost equivalent in terms of electron density distribution. This
paper reports an interesting change in bonding pattern when one replaces
Si by a C atom in triatomic silicon carbide clusters stabilized by
a ligand
On the Validity of the Maximum Hardness Principle and the Minimum Electrophilicity Principle during Chemical Reactions
Hardness and electrophilicity values for several molecules
involved in different chemical reactions are calculated at various
levels of theory and by using different basis sets. Effects of these
aspects as well as different approximations to the calculation of
those values vis-à-vis the validity of the maximum hardness
and minimum electrophilicity principles are analyzed in the cases
of some representative reactions. Among 101 studied exothermic reactions,
61.4% and 69.3% of the reactions are found to obey the maximum hardness
and minimum electrophilicity principles, respectively, when hardness
of products and reactants is expressed in terms of their geometric
means. However, when we use arithmetic mean, the percentage reduces
to some extent. When we express the hardness in terms of scaled hardness,
the percentage obeying maximum hardness principle improves. We have
observed that maximum hardness principle is more likely to fail in
the cases of very hard species like F<sup>–</sup>, H<sub>2</sub>, CH<sub>4</sub>, N<sub>2</sub>, and OH appearing in the reactant
side and in most cases of the association reactions. Most of the association
reactions obey the minimum electrophilicity principle nicely. The
best results (69.3%) for the maximum hardness and minimum electrophilicity
principles reject the 50% null hypothesis at the 2% level of significance
Noble Gas Inserted Metal Acetylides (Metal = Cu, Ag, Au)
Metal
acetylides (MCCH, M = Cu, Ag, Au) were already experimentally
detected in molecular form. Herein, we investigate the possibility
of noble gas (Ng) insertion within the C–H bond of MCCH and
their stability is compared with those of the reported MNgCCH and
HCCNgH molecules. Our coupled-cluster-level computations show that
MCCNgH (Ng = Kr, Xe, Rn) systems are local minima on the corresponding
potential energy surfaces, whereas their lighter analogues do not
remain in the chemically bound form. Further, their stability is analyzed
with respect to all possible dissociation channels. The most favorable
dissociation channel leads to the formation of free Ng and MCCH. However,
there exists a high free energy barrier (29.3–46.9 kcal/mol)
to hinder the dissociation. The other competitive processes against
their stability include two-body and three-body neutral dissociation
channels, MCCNgH → MCC + NgH and MCCNgH → MCC + Ng +
H, respectively, which are slightly exergonic in nature at 298 K for
Ng = Kr, Xe and M = Cu, Ag, and for AuCCKrH. However, the Xe analogues
for Cu and Ag and AuCCKrH would be viable at a lower temperature.
AuCCNgH (Ng = Kr–Rn) molecules are the best candidates for
experimental realization, since they have higher dissociation energy
values and higher kinetic protection in the case of feasible dissociation
channels compared to the Cu and Ag systems. A detailed bonding analysis
indicates that the Ng–H bonds are genuine covalent bonds and
there is also a substantial covalent character in Ng–C contacts
of these molecules. Moreover, the possibility of insertion of two
Xe atoms in AuCCH resulting in AuXeCCXeH and the stability of XeAuXeCCXeH
are also tested herein
Comparative Study on the Noble-Gas Binding Ability of BeX Clusters (X = SO<sub>4</sub>, CO<sub>3</sub>, O)
Ab initio computations are carried
out to assess the noble gas
(Ng) binding capability of BeSO<sub>4</sub> cluster. We have further
compared the stability of NgBeSO<sub>4</sub> with that of the recently
detected NgBeCO<sub>3</sub> cluster. The Ng–Be bond in NgBeCO<sub>3</sub> is somewhat weaker than that in NgBeO cluster. In NgBeSO<sub>4</sub>, the Ng–Be bond is found to be stronger compared with
not only the Ng–Be bond in NgBeCO<sub>3</sub> but also that
in NgBeO, except the He case. The Ar–Rn-bound BeSO<sub>4</sub> analogues are viable even at room temperature. The Wiberg bond indices
of Be–Ng bonds and the degree of electron transfer from Ng
to Be are somewhat larger in NgBeSO<sub>4</sub> than those in NgBeCO<sub>3</sub> and NgBeO. Electron density and energy decomposition analyses
are performed in search of the nature of interaction in the Be–Ng
bond in NgBeSO<sub>4</sub>. The orbital energy term (Δ<i>E</i><sup>orb</sup>) contributes the maximum (ca. 80–90%)
to the total attraction energy. The Ar/Kr/Xe/Rn–Be bonds in
NgBeSO<sub>4</sub> could be of partial covalent type with a gradual
increase in covalency along Ar to Rn
Bonding in Binuclear Carbonyl Complexes M<sub>2</sub>(CO)<sub>9</sub> (M = Fe, Ru, Os)
Quantum-chemical density functional
theory calculations using the BP86 functional in conjunction with
a triple-ζ basis set and dispersion correction by Grimme with
Becke-Johnson damping D3(BJ) were performed for the title molecules.
The nature of the bonding was examined with the quantum theory of
atoms in molecules (QTAIM) and natural bond order (NBO) methods and
with the energy decomposition analysis in conjunction with the natural
orbital for chemical valence (EDA-NOCV) analysis. The energetically
lowest-lying form of Fe<sub>2</sub>(CO)<sub>9</sub> is the triply
bridged <i>D</i><sub>3<i>h</i></sub> structure,
whereas the most stable structures of Ru<sub>2</sub>(CO)<sub>9</sub> and Os<sub>2</sub>(CO)<sub>9</sub> are singly bridged <i>C</i><sub>2</sub> species. The calculated reaction energies for the formation
of the cyclic trinuclear carbonyls M<sub>3</sub>(CO)<sub>12</sub> from
the dinuclear carbonyls M<sub>2</sub>(CO)<sub>9</sub> are in agreement
with experiment, as the iron complex Fe<sub>2</sub>(CO)<sub>9</sub> is thermodynamically stable in these reactions, but the heavier
homologues Ru<sub>2</sub>(CO)<sub>9</sub> and Os<sub>2</sub>(CO)<sub>9</sub> are not. The metal–CO bond to the bridging CO ligands
is stronger than the bonds to the terminal CO ligands. This holds
for the triply bridged <i>D</i><sub>3<i>h</i></sub> structures as well as for the singly bridged <i>C</i><sub>2</sub> or <i>C</i><sub>2<i>v</i></sub> species.
The analysis of the orbital interactions with the help of the EDA-NOCV
method suggests that the overall M→CO π backdonation
is always stronger than the M←CO σ donation. The bridging
carbonyls are more strongly bonded than the terminal CO ligands, and
they are engaged in stronger σ donation and π backdonation,
but the formation of bridging carbonyls requires reorganization energy,
which may or may not be compensated by the stronger metal–ligand
interactions. The lower-lying <i>D</i><sub>3<i>h</i></sub> form of Fe<sub>2</sub>(CO)<sub>9</sub> and <i>C</i><sub>2</sub> structures of Ru<sub>2</sub>(CO)<sub>9</sub> and Os<sub>2</sub>(CO)<sub>9</sub> are due to a delicate balance of several
forces
Data_Sheet_1_Modified Particle Swarm Optimization Algorithms for the Generation of Stable Structures of Carbon Clusters, Cn (n = 3–6, 10).doc
Particle Swarm Optimization (PSO), a population based technique for stochastic search in a multidimensional space, has so far been employed successfully for solving a variety of optimization problems including many multifaceted problems, where other popular methods like steepest descent, gradient descent, conjugate gradient, Newton method, etc. do not give satisfactory results. Herein, we propose a modified PSO algorithm for unbiased global minima search by integrating with density functional theory which turns out to be superior to the other evolutionary methods such as simulated annealing, basin hopping and genetic algorithm. The present PSO code combines evolutionary algorithm with a variational optimization technique through interfacing of PSO with the Gaussian software, where the latter is used for single point energy calculation in each iteration step of PSO. Pure carbon and carbon containing systems have been of great interest for several decades due to their important role in the evolution of life as well as wide applications in various research fields. Our study shows how arbitrary and randomly generated small Cn clusters (n = 3–6, 10) can be transformed into the corresponding global minimum structure. The detailed results signify that the proposed technique is quite promising in finding the best global solution for small population size clusters.</p
Structural Characterization and Bonding Analysis of [Hg{Fe(CO)<sub>5</sub>}<sub>2</sub>]<sup>2+</sup> [SbF<sub>6</sub>]<sup>−</sup><sub>2</sub>
The non-classical carbonyl complex [Hg{Fe(CO)5}2]2+ [SbF6]−2 is prepared by reaction of Hg(SbF6)2 and excess
Fe(CO)5 in anhydrous HF. The single-crystal X-ray structure
reveals a linear Fe–Hg–Fe moiety as well as an eclipsed
conformation of the eight basal CO ligands. Interestingly, the Hg–Fe
bond length of 2.5745(7) Å is relatively similar to the corresponding
Hg–Fe bonds in literature-known [Hg{Fe(CO)4}2]2– dianions (2.52–2.55 Å),
which intrigued us to analyze the bonding situation in both the dications
and dianions with the energy decomposition analysis with natural orbitals
for chemical valence (EDA-NOCV) method. Both species are best described
as Hg(0) compounds, which are also confirmed by the shape of the HOMO-4
and HOMO-5 of the dication and dianion, respectively, in which the
electron pair is located mainly at the Hg. Furthermore, for the dication
and the dianion, the σ back-donation from Hg into the [Fe(CO)5]22+ or the [Fe(CO)4]22– fragment is the most dominant orbital
interaction and surprisingly these interaction energies are also very
similar even in absolute values. The fact that both iron-based fragments
are missing two electrons explains their prominent σ-acceptor
properties
Generation and Characterization of the Charge-Transferred Diradical Complex CaCO<sub>2</sub> with an Open-Shell Singlet Ground State
The
CaCO2 complex is generated via the reaction of excited-state
calcium atom with carbon dioxide in a solid neon matrix. Infrared
absorption spectroscopy and quantum chemical calculations reveal that
the complex has a planar four-membered ring structure with a strongly
bent CO2 ligand side-on coordinated to the calcium center
in an η2–O, O manner. The complex has an open-shell
singlet ground state, which can be described as the bonding interactions
between a Ca+ (4s1) cation in the doublet ground
state and a doublet ground state CO2– anion. The analysis of the bonding situation suggests that the Ca-O2C bonds have a large (75%) electrostatic character. The covalent
(orbital) interactions come from the coupling of the unpaired electrons
of Ca+ and CO2– giving rise
to electron-sharing bonding and a stronger contribution from dative
bonding (Ca+)←(CO2–). The atomic orbitals (AOs) of Ca+ that are engaged in
the covalent bonds are the 4s AO for the electron-sharing bonds and
the 3d AOs for the dative bonds. This is further evidence for the
assignment of the heavier alkaline-earth atoms as transition metals
rather than main-group elements
