7 research outputs found
Probing the Relationship Between Large-Amplitude Motions in H<sub>5</sub><sup>+</sup> and Proton Exchange Between H<sub>3</sub><sup>+</sup> and H<sub>2</sub>
Understanding the spectroscopy and
dynamics of H<sub>5</sub><sup>+</sup> is central in gaining insights
into the H<sub>3</sub><sup>+</sup> + H<sub>2</sub> → H<sub>5</sub><sup>+</sup> →
H<sub>2</sub> + H<sub>3</sub><sup>+</sup> proton transfer reaction.
This molecular ion exhibits large-amplitude vibrations, which allow
for the transfer of a proton between H<sub>3</sub><sup>+</sup> and
H<sub>2</sub> even in its ground vibrational state. With vibrational
excitation, the number of open channels for permutations of protons
increase. In this work, the minimized energy path variant of diffusion
Monte Carlo is used to investigate how the energetically accessible
proton permutations evolve as H<sub>5</sub><sup>+</sup> is dissociated
into H<sub>3</sub><sup>+</sup> + H<sub>2</sub>. Two mechanisms for
proton permutation are investigated. The first is the proton hop,
which correlates to large-amplitude vibrations of the central proton
in H<sub>5</sub><sup>+</sup>. The second is the exchange of a pair
of hydrogen atoms between H<sub>3</sub><sup>+</sup> and H<sub>2</sub>. This mechanism requires several proton hops along with a 120°
rotation of H<sub>3</sub><sup>+</sup> within the H<sub>5</sub><sup>+</sup> molecular ion. This analysis shows that while there is a
narrow region of configuration space over which both isomerization
processes are energetically accessible, full permutation of the five
protons in H<sub>5</sub><sup>+</sup> more likely occurs through a
stepwise mechanism. Such full permutation of the protons becomes accessible
when the shared proton stretch is excited to the <i>v</i><sub>pt</sub> = 2 or 3 excited state. The effects of deuteration
and rotational excitation of the H<sub>2</sub> and H<sub>3</sub><sup>+</sup> products are also investigated. Deuteration inhibits permutation
of protons, while rotational excitation has only a small impact on
these processes
Investigation of the Structure and Spectroscopy of H<sub>5</sub><sup>+</sup> Using Diffusion Monte Carlo
The results of diffusion Monte Carlo
(DMC) calculations of the
ground and selected excited states of H<sub>5</sub><sup>+</sup> and its deuterated analogues are presented.
Comparisons are made between the results obtained from two recently
reported potential surfaces. Both of these surfaces are based on CCSDÂ(T)
electronic energies, but the fits display substantial differences
in the energies of low-lying stationary points. Little sensitivity
to these features is found in the DMC results, which yield zero-point
energies based on the two surfaces that differ by between 20 and 30
cm<sup>–1</sup> for all twelve isotopologues of H<sub>5</sub><sup>+</sup>. Likewise,
projections of the ground state probability amplitudes, evaluated
for the two surfaces, are virtually identical. By using the ground
state probability amplitudes, vibrationally averaged rotational constants
and dipole moments were calculated. On the basis of these calculations,
all isotopologues are shown to be near-prolate symmetric tops. Further,
in cases where the ion had a nonzero dipole moment, the magnitude
of the vibrationally averaged dipole moment was found to range from
0.33 to 1.15 D, which is comparable to the dipole moments of H<sub>2</sub>D<sup>+</sup> and HD<sub>2</sub><sup>+</sup>. Excited states with up to three quanta
in the shared proton stretch and one quantum in the in-phase stretch
of the outer H<sub>2</sub> groups were also investigated. Trends in
the energies and the properties of these states are discussed
Rotation/Torsion Coupling in H<sub>5</sub><sup>+</sup>, D<sub>5</sub><sup>+</sup>, H<sub>4</sub>D<sup>+</sup>, and HD<sub>4</sub><sup>+</sup> Using Diffusion Monte Carlo
Two methods for studying the rotation/torsion
coupling in H<sub>5</sub><sup>+</sup> are described. The first involves
a fixed-node treatment in which the nodal surfaces are obtained from
a reduced dimensional calculation in which only the rotations of the
outer H<sub>2</sub> groups are considered. In the second, the torsion
and rotation dependence of the wave function is described in state
space, and the other internal coordinates are described in configuration
space. Such treatments are necessary for molecules, like H<sub>5</sub><sup>+</sup>, where there is a very low-energy barrier to internal
rotation. The results of the two approaches are found to be in good
agreement with previously reported energies for <i>J</i> = 0. The diffusion Monte Carlo treatment allows us to extend the
calculations to low <i>J</i>, and results are reported for
the three lowest energy torsion excited states with <i>J</i> ≤ 3. For the level of rotational and vibrational excitation
investigated, only modest changes in the vibrational wave functions
are found. The effects of deuteration are also investigated, focusing
on D<sub>5</sub><sup>+</sup> and the symmetric variants of H<sub>4</sub>D<sup>+</sup> and HD<sub>4</sub><sup>+</sup>
Hierarchically Designed Germanium Microcubes with High Initial Coulombic Efficiency toward Highly Reversible Lithium Storage
Germanium
has been investigated intensively for its high specific
capacity and tough nature, which make it a promising candidate anode
for high energy lithium-ion batteries. However, the rational design
of a germanium electrode with enhanced electrochemical performances
is still a big challenge. Herein, we designed and synthesized germanium microcubes with a hierarchical
structure directly on titanium foil via a simple hydrogen reduction
method. An ultrahigh initial Coulombic efficiency of 91.8% was acquired
due to the high crystallinity of germanium for reversible lithium
insertion and extraction, less adverse side reaction for irreversible
lithium loss, and unique hierarchical structure for easier electrolyte
penetration. In addition, the Li<sub>2</sub>CO<sub>3</sub>-predominated
solid electrolyte interface contributes significantly to the excellent
cycling and rate performances of the anode. Both half and full cell
performances demonstrate that germanium has potential applications
in high-performance lithium-ion batteries
Kinetics and Structural Changes of Li-Rich Layered Oxide 0.5Li<sub>2</sub>MnO<sub>3</sub>·0.5LiNi<sub>0.292</sub>Co<sub>0.375</sub>Mn<sub>0.333</sub>O<sub>2</sub> Material Investigated by a Novel Technique Combining in Situ XRD and a Multipotential Step
Li-rich
layered oxide 0.5Li<sub>2</sub>MnO<sub>3</sub>·0.5LiNi<sub>0.292</sub>Co<sub>0.375</sub>Mn<sub>0.333</sub>O<sub>2</sub> was
prepared by an aqueous solution–evaporation route. X-ray powder
diffraction (XRD) showed that the as-synthesized material was a solid
solution consisting of layered α-NaFeO<sub>2</sub>-type LiMO<sub>2</sub> (M = Ni, Co, Mn) and monoclinic Li<sub>2</sub>MnO<sub>3</sub>. The superlattice spots in the selected area electron diffraction
pattern indicated the ordering of lithium ions with transition metal
(TM) ions in TM layers in this Li-rich layered oxide. Electrochemical
performance testing showed that the as-synthesized material could
deliver an initial discharge capacity of 267.7 mAh/g, with a capacity
retention of 88.5% after 33 cycles. A new combination technique, multipotential
step in situ XRD (MPS in situ XRD) measurement, was applied for the
first time to investigate the Li-rich layered oxide. Using this approach,
the relationships between kinetics and structural variations can be
obtained simutaneously. In situ XRD results showed that the <i>c</i> parameter decreased from 3.70 to 4.30 V and increased
from 4.30 to 4.70 V, whereas the <i>a</i> parameter underwent
a decrease above 4.30 V during the first charge process. Below 3.90
V during the first discharge process, a slight decrease in the <i>c</i> parameter was found along with an increase in the <i>a</i> parameter. During the first charge process, the value
of the coefficient of diffusion for lithium ions (<i>D</i><sub>Li+</sub>) decreased to its mininum at 4.55 V, which might be
associated with Ni<sup>2+</sup> migration, as indicated by both Ni
occupancy in 3b sites (Ni<sub>3b</sub>%) in the Li<sup>+</sup> layers
and complicated chemical reactions. Remarkably, a lattice distortion
might occur within the local domain in the host stucture during the
first discharge process, indicated by a slight splitting of the (003)
diffraction peak at 3.20 V
Insights into Magneto-Optics of Helical Conjugated Polymers
Materials with magneto-optic (MO)
properties have enabled critical
fiber-optic applications and highly sensitive magnetic field sensors.
While traditional MO materials are inorganic in nature, new generations
of MO materials based on organic semiconducting polymers could allow
increased versatility for device architectures, manufacturing options,
and flexible mechanics. However, the origin of MO activity in semiconducting
polymers is far from understood. In this paper, we report high MO
activity observed in a chiral helical poly-3-(alkylsulfone)Âthiophene
(<b>P3AST</b>), which confirms a new design for the creation
of a giant Faraday effect with Verdet constants up to (7.63 ±
0.78) × 10<sup>4</sup> deg T<sup>–1</sup> m<sup>–1</sup> at 532 nm. We have determined that the sign of the Verdet constant
and its magnitude are related to the helicity of the polymer at the
measured wavelength. The Faraday rotation and the helical conformation
of <b>P3AST</b> are modulated by thermal annealing, which is
further supported by DFT calculations and MD simulations. Our results
demonstrate that helical polymers exhibit enhanced Verdet constants
and expand the previous design space for polythiophene MO materials
that was thought to be limited to highly regular lamellar structures.
The structure–property studies herein provide insights for
the design of next-generation MO materials based upon semiconducting
organic polymers
Facile Synthesis of The Li-Rich Layered Oxide Li<sub>1.23</sub>Ni<sub>0.09</sub>Co<sub>0.12</sub>Mn<sub>0.56</sub>O<sub>2</sub> with Superior Lithium Storage Performance and New Insights into Structural Transformation of the Layered Oxide Material during Charge–Discharge Cycle: In Situ XRD Characterization
In
this work, the Li-rich oxide Li<sub>1.23</sub>N<sub>i0.09</sub>Co<sub>0.12</sub>Mn<sub>0.56</sub>O<sub>2</sub> was synthesized through
a facile route called aqueous solution-evaporation route that is simple
and without waste water. The as-prepared Li<sub>1.23</sub>N<sub>i0.09</sub>Co<sub>0.12</sub>Mn<sub>0.56</sub>O<sub>2</sub> oxide was confirmed
to be a layered LiMO<sub>2</sub>–Li<sub>2</sub>MnO<sub>3</sub> solid solution through ex
situ X-ray diffraction (ex situ XRD) and transmission electron microscopy
(TEM). Electrochemical results showed that the Li-rich oxide Li<sub>1.23</sub>N<sub>i0.09</sub>Co<sub>0.12</sub>Mn<sub>0.56</sub>O<sub>2</sub> material can deliver a discharge capacity of 250.8 mAhg<sup>–1</sup> in the 1st cycle at 0.1 C and capacity retention
of 86.0% in 81 cycles. In situ X-ray diffraction technique (in situ
XRD) and ex situ TEM were applied to study structural changes of the
Li-rich oxide Li<sub>1.23</sub>N<sub>i0.09</sub>Co<sub>0.12</sub>Mn<sub>0.56</sub>O<sub>2</sub> material during charge–discharge cycles.
The study allowed observing experimentally, for the first time, the
existence of β-MnO<sub>2</sub> phase that is appeared near 4.54
V in the first charge process, and a phase transformation of the β-MnO<sub>2</sub> to layered Li<sub>0.9</sub>MnO<sub>2</sub> is occurred in
the initial discharge process by evidence of in situ XRD pattrens
and selected area electron diffraction (SAED) patterns at different
states of the initial charge and discharge process. The results illustrated
also that the variation of the in situ X-ray reflections during charge–discharge
cycling are clearly related to the changes of lattice parameters of
the as-prepared Li-rich oxide during the charge–discharge cycles