19 research outputs found
Nonvalence Correlation-Bound Anion States of Spherical Fullerenes
We present a one-electron model Hamiltonian
for characterizing
nonvalence correlation-bound anion states of fullerene molecules.
These states are the finite system analogs of image potential states
of metallic surfaces. The model potential accounts for both atomic
and charge-flow polarization and is used to characterize the nonvalence
correlation-bound anion states of the C<sub>60</sub>, (C<sub>60</sub>)<sub>2</sub>, C<sub>240</sub>, and C<sub>60</sub>@C<sub>240</sub> fullerene systems. Although C<sub>60</sub> is found to have a single
(s-type) nonvalence correlation-bound anion state, the larger fullerenes
are demonstrated to have multiple nonvalence correlation-bound anion
states
Theoretical Characterization of the Minimum-Energy Structure of (SF<sub>6</sub>)<sub>2</sub>
MP2 and symmetry-adapted perturbation
theory calculations are used
in conjunction with the aug-cc-pVQZ basis set to characterize the
SF<sub>6</sub> dimer. Both theoretical methods predict the global
minimum structure to be of <i>C</i><sub>2</sub> symmetry,
lying 0.07–0.16 kJ/mol below a <i>C</i><sub>2<i>h</i></sub> saddle point structure, which, in turn, is predicted
to lie energetically 0.4–0.5 kJ/mol below the lowest-energy <i>D</i><sub>2<i>d</i></sub> structure. This is in contrast
with IR spectroscopic studies that infer an equilibrium <i>D</i><sub>2<i>d</i></sub> structure. It is proposed that the
inclusion of vibrational zero-point motion gives an averaged structure
of <i>D</i><sub>2<i>d</i></sub> symmetry
Establishing the Ground State of the Disjoint Diradical Tetramethyleneethane with Quantum Monte Carlo
The nature of the electronic ground
state of the tetramethyleneethane
(TME) diradical has proven to be a challenge for both experiment and
theory. Through the use of quantum Monte Carlo (QMC) methods and multireference
perturbation theory, we demonstrate that the lowest singlet state
of TME is energetically lower than the lowest triplet state at all
values of the torsional angle between the allyl subunits. Moreover,
we find that the maximum in the potential energy curve for the singlet
state occurs at a torsional angle near 45°, in contrast to previous
calculations that placed the planar structure of the singlet state
as the highest in energy. We also show that the CASPT2 method when
used with a sufficiently large reference space and a sufficiently
flexible basis set gives potential energy curves very close to those
from the QMC calculations. Our calculations have converged the singlet–triplet
gap of TME as a function of methodology and basis set. These results
provide insight into the level of theory required to properly model
diradicals, in particular disjoint diradicals, and provide guidelines
for future studies on more complicated diradical systems
Mechanism of Oxygen Exchange between CO<sub>2</sub> and TiO<sub>2</sub>(101) Anatase
The mechanism of oxygen exchange
between CO<sub>2</sub> and a defective
anatase (101) surface was investigated by density functional theory
calculations including corrections for long-range dispersion interactions
and for on-site Coulomb interactions. The calculations identify a
carbonate-like configuration at a surface oxygen defect site as the
key intermediate species responsible for the oxygen exchange. The
stability of this species, its vibrational frequencies, and the reaction
barriers involved in the oxygen exchange mechanism are found to be
highly dependent on the specific value of the Hubbard <i>U</i> correction used to describe the on-site Coulomb interactions within
the GGA+U procedure. <i>U</i> parameter values that result
in CO<sub>2</sub> adsorption energies and reaction barriers for oxygen
exchange consistent with the results of room-temperature experiments
are smaller (<i>U</i> ≤ 2.5 eV) than those that reproduce
the experimental band gap or location of defect states in the band
gap of the reduced TiO<sub>2</sub> crystal
Diffusion of CO<sub>2</sub> on the Rutile TiO<sub>2</sub>(110) Surface
The diffusion of CO<sub>2</sub> molecules on a reduced
rutile TiO<sub>2</sub>(110)-(1×1) surface has been investigated
using scanning
tunneling microscopy (STM) and density functional theory (DFT) calculations.
The STM feature associated with a CO<sub>2</sub> molecule at an oxygen
vacancy (V<sub>O</sub>) becomes increasingly streaky with increasing
temperature, indicating thermally activated CO<sub>2</sub> diffusion
from the V<sub>O</sub> site. From temperature-dependent tunneling
current measurements, the barrier for diffusion of CO<sub>2</sub> from
the V<sub>O</sub> site is estimated to be 3.31 ± 0.23 kcal/mol.
The corresponding value from the DFT calculations is 3.80 kcal/mol.
In addition, the DFT calculations give a barrier for diffusion of
CO<sub>2</sub> along Ti rows of only 1.33 kcal/mol
Water Chain Formation on TiO<sub>2</sub>(110)
The adsorption of water on a reduced rutile TiO<sub>2</sub>(110)-(1×1)
surface has been investigated using scanning tunneling microscopy
(STM) and density functional theory (DFT) calculations. The STM measurements
show that at a temperature of 50 K, an isolated water monomer adsorbs
on top of a TiÂ(5f) atom on the Ti row in agreement with earlier studies.
As the coverage increases, water molecules start to form one-dimensional
chain structures along the Ti row direction. Supporting DFT calculations
show that the formation of an H-bonded one-dimensional water chain
is energetically favorable compared to monomer adsorption. In the
chain, there are H-bonds between adjacent water molecules, and the
water molecules also form H-bonds to neighboring bridging oxygens
of TiO<sub>2</sub>(110). Thermal annealing at <i>T</i> =
190 K leads to the formation of longer chains facilitated by the diffusion
of water on the surface. The results provide insight into the nature
of the hydrogen bonding in the initial stage of wetting of TiO<sub>2</sub>
Correlation Consistent Gaussian Basis Sets for H, B–Ne with Dirac–Fock AREP Pseudopotentials: Applications in Quantum Monte Carlo Calculations
In
this paper, we introduce correlation consistent Gaussian-type
orbital basis sets for the H and B–Ne atoms for use with the
CASINO Dirac–Fock AREP pseudopotentials. These basis sets are
tested in coupled cluster calculations on H<sub>2</sub>, B<sub>2</sub>, C<sub>2</sub>, N<sub>2</sub>, O<sub>2</sub>, and F<sub>2</sub> as
well as in quantum Monte Carlo calculations on the water monomer and
dimer and the water–benzene complex, where they are found to
give low variances in variational Monte Carlo calculations and to
lead to reduced time step errors and improved convergence in diffusion
Monte Carlo calculations compared to the use of nonoptimized basis
sets. The use of basis sets with a large number of contracted <i>s</i> and <i>p</i> primitives is found to be especially
important for the convergence of the energy in the diffusion Monte
Carlo calculations
Dispersion-Corrected Density Functional Theory and Classical Force Field Calculations of Water Loading on a Pyrophyllite(001) Surface
Water adsorption on the (001) surface of pyrophyllite
[AlÂ(OH)Â(Si<sub>2</sub>O<sub>5</sub>)] was investigated using density
functional
theory (DFT) with dispersion corrections and force field calculations.
The DFT calculations show that a water molecule can bind either to
one or to two basal oxygen atoms of the surface, with adsorption energies
varying from −0.10 to −0.19 eV depending on the binding
configuration and binding site. Because the water–water interactions
are stronger than the water–surface interactions, the energetically
preferred structures with two or more molecules on the surface are
clusters reminiscent of their gas-phase counterparts. The trend in
water–surface binding energies with the number of water molecules
obtained from force field calculations qualitatively agrees with that
predicted by the dispersion-corrected DFT calculations. However, the
force field calculations give a low-energy structural motif with a
water molecule coordinated to a hydroxyl group associated with the
octahedral layer of the pyrophyllite surface. This binding motif is
found to be unstable in the DFT calculations
Molecular Dynamics Simulations of Turbostratic Dry and Hydrated Montmorillonite with Intercalated Carbon Dioxide
Molecular dynamics simulations using
classical force fields were
carried out to study energetic and structural properties of rotationally
disordered clay mineral–water–CO<sub>2</sub> systems
at pressure and temperature relevant to geological carbon storage.
The simulations show that turbostratic stacking of hydrated Na- and
Ca-montmorillonite and hydrated montmorillonite with intercalated
carbon dioxide is an energetically demanding process accompanied by
an increase in the interlayer spacing. On the other hand, rotational
disordering of dry or nearly dry smectite systems can be energetically
favorable. The distributions of interlayer species are calculated
as a function of the rotational angle between adjacent clay layers
Assessing the Performances of Dispersion-Corrected Density Functional Methods for Predicting the Crystallographic Properties of High Nitrogen Energetic Salts
Several density functional methods
with corrections for long-range
dispersion interactions are evaluated for their capabilities to describe
the crystallographic lattice properties of a set of 26 high nitrogen-content
salts relevant for energetic materials applications. Computations
were done using methods that ranged from adding atom–atom dispersion
corrections with environment-independent and environment-dependent
coefficients, to methods that incorporate dispersion effects via dispersion-corrected
atom-centered potentials (DCACP), to methods that include nonlocal
corrections. Among the functionals tested, the most successful is
the nonlocal optPBE-vdW functional of Klimeš and Michaelides
that predicts unit cell volumes for all crystals of the reference
set within the target error range of ±3% and gives individual
lattice parameters with a mean average percent error of less than
0.81%. The DCACP, Grimme’s D3, and Becke and Johnson’s
exchange-hole (XDM) methods, when used with the BLYP, PBE, and B86b
functionals, respectively, are also quite successful at predicting
the lattice parameters of the test set