12 research outputs found
SpinâOrbit Effect on the Molecular Properties of TeX<sub><i>n</i></sub> (X = F, Cl, Br, and I; <i>n</i> = 1, 2, and 4): A Density Functional Theory and Ab Initio Study
Density functional theory (DFT) and
ab initio calculations, including
spinâorbit coupling (SOC), were performed to investigate the
spinâorbit (SO) effect on the molecular properties of tellurium
halides, TeX<sub><i>n</i></sub> (X = F, Cl, Br, and I; <i>n</i> = 1, 2, and 4). SOC elongates the TeâX bond and
slightly reduces the vibrational frequencies. Consideration of SOC
leads to better agreement with experimental values. MøllerâPlesset
second-order perturbation theory (MP2) seriously underestimates the
TeâX bond lengths. In contrast, B3LYP significantly overestimates
them. SO-PBE0 and multireference configuration interactions with the
Davidson correction (MRCI+Q), which include SOC via a state-interaction
approach, give the TeâI bond length of TeI<sub>2</sub> that
matches the experimental value. On the basis of the calculated thermochemical
energy and optimized molecular structure, TeI<sub>4</sub> is unlikely
to be stable. The use of PBE0 including SOC is strongly recommended
for predicting the molecular properties of Te-containing compounds
Multireference Ab Initio Study of the Ground and Low-Lying Excited States of Cr(CO)<sub>2</sub> and Cr(CO)<sub>3</sub>
We
investigate the ground and low-lying excited states of unsaturated
chromium carbonyls, CrÂ(CO)<sub>2</sub> and CrÂ(CO)<sub>3</sub>, using
multiconfigurational ab initio perturbation theory. Unlike other chromium
carbonyls, there are discrepancies between the experiment and theory
on the identity of the ground states of CrÂ(CO)<sub>2</sub> and CrÂ(CO)<sub>3</sub>. From multireference ab initio calculations considering the
full valence orbitals of CrÂ(CO)<sub>2</sub> and CrÂ(CO)<sub>3</sub>, the differences in the molecular structures of their various electronic
states are explained by the electronic structure analysis. On the
basis of the result from CASPT2 and MS-CASPT2 calculations, we propose
that the ground states of CrÂ(CO)<sub>2</sub> and CrÂ(CO)<sub>3</sub> are the <sup>5</sup>Î <sub>g</sub> and <sup>1</sup>A<sub>1</sub> states, respectively, addressing the ambiguity regarding their ground
states. In addition, the multiconfigurational ab initio perturbation
theory calculations reveal that (1) the energy gaps between the ground
and first low-lying excited states of CrÂ(CO)<sub>2</sub> and CrÂ(CO)<sub>3</sub> are quite small and (2) the first low-lying excited states
of CrÂ(CO)<sub>2</sub> and CrÂ(CO)<sub>3</sub> have the same spin multiplicities
as the ground states of CrCO and CrÂ(CO)<sub>2</sub>, respectively,
which are the products of ligand dissociation. As a result, the apparent
spin-forbidden dissociation of CrÂ(CO)<sub>2</sub> and CrÂ(CO)<sub>3</sub> into CrCO and CrÂ(CO)<sub>2</sub>, respectively, are likely to
be facilitated by thermal excitation of the ground states of Cr(CO)<sub>2</sub> and Cr(CO)<sub>3</sub> into their first low-lying excited states, which then actually undergoes the spin-allowed
dissociation to the ground states of CrCO and CrÂ(CO)<sub>2</sub> with
the same spin multiplicities
Ab Initio Analysis of Auger-Assisted Electron Transfer
Quantum
confinement in nanoscale materials allows Auger-type electronâhole
energy exchange. We show by direct time-domain atomistic simulation
and analytic theory that Auger processes give rise to a new mechanism
of charge transfer (CT) on the nanoscale. Auger-assisted CT eliminates
the renown Marcus inverted regime, rationalizing recent experiments
on CT from quantum dots to molecular adsorbates. The ab initio simulation
reveals a complex interplay of the electronâhole and chargeâphonon
channels of energy exchange, demonstrating a variety of CT scenarios.
The developed Marcus rate theory for Auger-assisted CT describes,
without adjustable parameters, the experimental plateau of the CT
rate in the region of large donorâacceptor energy gap. The
analytic theory and atomistic insights apply broadly to charge and
energy transfer in nanoscale systems
Mechanistic Investigation of Thermal and Photoreactions between Boron and Silane
Density
functional theory and high-level ab initio calculations
were performed to elucidate the detailed reaction mechanism from B
and SiH<sub>4</sub> to a structure with two bridging H atoms (SiÂ(Îź-H<sub>2</sub>)ÂBH<sub>2</sub>, silicon tetrahydroborate). On the basis of
the calculated results, this reaction mechanism includes both thermal
and photochemical reactions. Especially, thermal conversion of silylene
dihydroborate (H<sub>2</sub>BîťSiH<sub>2</sub>) to SiÂ(Îź-H<sub>2</sub>)ÂBH<sub>2</sub> is not feasible because two high energetic
barriers must be overcome. In contrast, the reverse reaction is feasible
because it is effectively only necessary to overcome a single barrier.
The characteristics of the excited states of H<sub>2</sub>BîťSiH<sub>2</sub> and SiÂ(Îź-H<sub>2</sub>)ÂBH<sub>2</sub> have been identified.
Two successive conical intersections (CIs) are involved in the photochemical
reaction. The BSiH<sub>4</sub> bending coordinate is almost parallel
to the reaction coordinate near the regions from the second CI to
SiÂ(Îź-H<sub>2</sub>)ÂBH<sub>2</sub>. The activated BSiH<sub>4</sub> bending mode lift the degeneracy of the second CI, thereby the reaction
readily proceeds to SiÂ(Îź-H<sub>2</sub>)ÂBH<sub>2</sub>. All calculated
results in this work reasonably well describe the recent experimental
observations
Ab Initio Investigation of the Ground States of F<sub>2</sub>P(S)N, F<sub>2</sub>PNS, and F<sub>2</sub>PSN
A recent
spectroscopic experiment identified difluorothiophosphoryl nitrene
(F<sub>2</sub>PÂ(S)ÂN) and found that it showed rich photochemistry.
However, a discrepancy between the experimental results and the quantum
chemical calculations was reported. Thus, high-level ab initio calculations
using the coupled cluster singles and doubles with perturbative triples
and second-order multiconfigurational perturbation theory were performed
to elucidate this inconsistency. The discrepancy arose due to the
failure to consider the triplet state of difluoroÂ(thionitroso)Âphosphine
(F<sub>2</sub>PNS). In this work, we identify that the global minimum
of the system is the triplet state of F<sub>2</sub>PNS, which allows
us to explain the inconsistency between the experimental and theoretical
results. All calculated results give consistent results with the recent
experimental results
Dynamics of Local Chirality during SWCNT Growth: Armchair versus Zigzag Nanotubes
We present an analysis of the dynamics of single-walled
carbon
nanotube (SWCNT) chirality during growth, using the recently developed
local chirality index (LOCI) method [Kim et al. Phys. Rev. Lett. 2011, 107, 175505] in conjunction with quantum chemical
molecular dynamics (QM/MD) simulations. Using (5,5) and (8,0) SWCNT
fragments attached to an Fe<sub>38</sub> catalyst nanoparticle, growth
was induced by periodically placing carbon atoms at the edge of the
SWCNT. For both armchair and zigzag SWCNTs, QM/MD simulations indicate
that defect healingî¸the process of defect removal during growthî¸is
a necessary, but not sufficient, condition for chirality-controlled
SWCNT growth. Time-evolution LOCI analysis shows that healing, while
restoring the pristine hexagon structure of the growing SWCNT, also
leads to changes in the local chirality of the SWCNT edge region and
thus of the entire SWCNT itself. In this respect, we show that zigzag
SWCNTs are significantly inferior in maintaining their chirality during
growth compared to armchair SWCNTs
Performance of Density Functional Theory and Relativistic Effective Core Potential for Ru-Based Organometallic Complexes
Herein
a performance assessment of density functionals used for
calculating the structural and energetic parameters of bi- and trimetallic
Ru-containing organometallic complexes has been performed. The performance
of four popular relativistic effective core potentials (RECPs) has
also been assessed. On the basis of the calculated results, the MN12-SX
(range-separated hybrid functional) demonstrates good performance
for calculating the molecular structures, while MN12-L (local functional)
performs well for calculating the energetics, including that of the
RuâRu bond breaking process. The choice of appropriate density
functional is a crucial factor for calculating the energetics. The
LANL08 demonstrates the lowest performance of the RECPs for calculating
the molecular structures, especially the RuâRu bond length
Density Functional Theory Assessment of Molecular Structures and Energies of Neutral and Anionic Al<sub><i>n</i></sub> (<i>n</i> = 2â10) Clusters
We report the results of a benchmarking
study on hybrid, hybrid-meta,
long-range-corrected, meta-generalized gradient approximation (meta-GGA),
and GGA density functional theory (DFT) methods for aluminum (Al)
clusters. A range of DFT functionals, such as B3LYP, B1B95, PBE0,
mPW1PW91, M06, M06-2X, ĎB97X, ĎB97XD, TPSSh, BLYP, PBE,
mPWPW91, M06-L, and TPSS, have been used to optimize the molecular
structures and calculate the vibrational frequencies and four energetic
parameters for neutral and anionic Al<sub><i>n</i></sub> (<i>n</i> = 2â10) clusters. The performances of
these functionals are assessed systematically by calculating the vertical
ionization energy for neutral Al clusters and the vertical electron
detachment energy for anionic Al clusters, along with the cohesive
energy and dissociation energy. The results are compared with the
available experimental and high-level ab initio calculated results.
The calculated results showed that the PBE0 and mPW1PW91 functionals
generally provide better results than the other functionals studied.
TPSS can be a good choice for the calculations of very large Al clusters.
On the other hand, the B3LYP, BLYP, and M06-L functionals are in poor
agreement with the available experimental and theoretical results.
The calculated results suggest that the hybrid DFT functionals like
B3LYP do not always provide better performance than GGA functionals
Prospect of Retrieving Vibrational Wave Function by Single-Object Scattering Sampling
The exact shape of wave functions has never been directly measured
because an ensemble measurement is often overwhelmed by the contributions
of highly populated configurations. In this work, we explore the possibility
of directly obtaining vibrational wave functions by single-object
scattering sampling (SOSS) using intense, ultrashort X-ray pulses
provided by X-ray free electron lasers. Previously, single-molecule
diffraction experiments using femtosecond X-ray pulses have been proposed
with the prospect of determining three-dimensional structure of macromolecules
without the need of single-crystal samples. In contrast to the previous
proposals, SOSS is designed for obtaining the structural variations
of constantly fluctuating molecules by sampling many single-shot,
single-object scattering patterns. From the simulations on iodine
molecules adopting various pulse characteristics and molecular parameters,
we were able to reconstruct vibrational wave functions of molecular
iodine and found that SOSS is feasible under appropriate experimental
conditions
Prospect of Retrieving Vibrational Wave Function by Single-Object Scattering Sampling
The exact shape of wave functions has never been directly measured
because an ensemble measurement is often overwhelmed by the contributions
of highly populated configurations. In this work, we explore the possibility
of directly obtaining vibrational wave functions by single-object
scattering sampling (SOSS) using intense, ultrashort X-ray pulses
provided by X-ray free electron lasers. Previously, single-molecule
diffraction experiments using femtosecond X-ray pulses have been proposed
with the prospect of determining three-dimensional structure of macromolecules
without the need of single-crystal samples. In contrast to the previous
proposals, SOSS is designed for obtaining the structural variations
of constantly fluctuating molecules by sampling many single-shot,
single-object scattering patterns. From the simulations on iodine
molecules adopting various pulse characteristics and molecular parameters,
we were able to reconstruct vibrational wave functions of molecular
iodine and found that SOSS is feasible under appropriate experimental
conditions