40 research outputs found
Li <i>K</i>-edge XAS spectra of Li<sub>2</sub>O.
<p>The spectra were collected on fresh surface, the same spot with 0.5 hour soft x-ray exposure, and 12 hours of soft x-ray exposure.</p
Soft x-ray irradiation effect on Li<sub>2</sub>O<sub>2</sub> revealed by Li <i>K</i>-edge XAS spectra.
<p>(top) The XAS spectrum of Li<sub>2</sub>O<sub>2</sub> evolves towards that of the Li<sub>2</sub>O upon increasing the radiation exposure. The top spectrum is the first one collected from spot A. From top to bottom, the first ten spectra were collected every ten minutes, with an hour of x-ray exposure at the same spot to maximize the dosage, then the measurements resumed with again ten minute each spectrum. The bottom red spectrum is collected on Li<sub>2</sub>O for comparison. (bottom) Li<sub>2</sub>O<sub>2</sub> Li <i>K</i>-edge XAS spectrum measured from a new spot B on the same sample stored in the ultra-high vacuum chamber for one week.</p
O <i>K</i>-edge XAS spectra of Li<sub>2</sub>O<sub>2</sub>, Li<sub>2</sub>CO<sub>3</sub>, and Li<sub>2</sub>O.
<p>O <i>K</i>-edge XAS spectra of Li<sub>2</sub>O<sub>2</sub>, Li<sub>2</sub>CO<sub>3</sub>, and Li<sub>2</sub>O.</p
Soft x-ray irradiation effect on Li<sub>2</sub>CO<sub>3</sub> revealed by Li <i>K</i>-edge XAS spectra.
<p>The XAS lineshape of Li<sub>2</sub>CO<sub>3</sub> (from top to bottom) evolve towards that of Li<sub>2</sub>O (red) after exposed to the soft x-rays. Each spectrum was taken with 10 minute x-ray exposure. The bottom panel shows the Li<sub>2</sub>CO<sub>3</sub> Li <i>K</i>-edge XAS spectrum collected from a new spot B on the same sample.</p
Crystal structure of Li<sub>2</sub>O<sub>2</sub>, Li<sub>2</sub>CO<sub>3</sub>, and Li<sub>2</sub>O.
<p>Red (largest) spheres represent oxygen atoms, green (smaller) spheres represent lithium atoms and purple (smallest) spheres are carbon atoms. Li-O polygons are drawn for better view.</p
Thermal stability and unfolding pathways of hyperthermophilic and mesophilic periplasmic binding proteins studied by molecular dynamics simulation
<p>The ribose binding protein (RBP), a sugar-binding periplasmic protein, is involved in the transport and signaling processes in both prokaryotes and eukaryotes. Although several cellular and structural studies have been reported, a description of the thermostability of RBP at the molecular level remains elusive. Focused on the hyperthermophilic <i>Thermoytoga maritima</i> RBP (tmRBP) and mesophilic <i>Escherichia coli</i> homolog (ecRBP), we applied molecular dynamics simulations at four different temperatures (300, 380, 450, and 500Â K) to obtain a deeper insight into the structural features responsible for the reduced thermostability of the ecRBP. The simulations results indicate that there are distinct structural differences in the unfolding pathway between the two homologs and the ecRBP unfolds faster than the hyperthermophilic homologs at certain temperatures in accordance with the lower thermal stability found experimentally. Essential dynamics analysis uncovers that the essential subspaces of ecRBP and tmRBP are non-overlapping and these two proteins show different directions of motion within the simulations trajectories. Such an understanding is required for designing efficient proteins with characteristics for a particular application.</p
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Mussel-Inspired Conductive Polymer Binder for Si-Alloy Anode in Lithium-Ion Batteries
The excessive volume
changes during cell cycling of Si-based anode
in lithium ion batteries impeded its application. One major reason
for the cell failure is particle isolation during volume shrinkage
in delithiation process, which makes strong adhesion between polymer
binder and anode active material particles a highly desirable property.
Here, a biomimetic side-chain conductive polymer incorporating catechol,
a key adhesive component of the mussel holdfast protein, was synthesized.
Atomic force microscopy-based single-molecule force measurements of
mussel-inspired conductive polymer binder contacting a silica surface
revealed a similar adhesion toward substrate when compared with an
effective Si anode binder, homo-polyÂ(acrylic acid), with the added
benefit of being electronically conductive. Electrochemical experiments
showed a very stable cycling of Si-alloy anodes realized via this
biomimetic conducting polymer binder, leading to a high loading Si
anode with a good rate performance. We attribute the ability of the
Si-based anode to tolerate the volume changes during cycling to the
excellent mechanical integrity afforded by the strong interfacial
adhesion of the biomimetic conducting polymer
Reducing Exciton Binding Energy by Increasing Thin Film Permittivity: An Effective Approach To Enhance Exciton Separation Efficiency in Organic Solar Cells
Photocurrent generation in organic
solar cells requires that excitons,
which are formed upon light absorption, dissociate into free carriers
at the interface of electron acceptor and donor materials. The high
exciton binding energy, arising from the low permittivity of organic
semiconductor films, generally causes low exciton separation efficiency
and subsequently low power conversion efficiency. We demonstrate here,
for the first time, that the exciton binding energy in B,O-chelated
azadipyrromethene (BO-ADPM) donor films is reduced by increasing the
film permittivity by blending the BO-ADPM donor with a high dielectric
constant small molecule, camphoric anhydride (CA). Various spectroscopic
techniques, including impedance spectroscopy, photon absorption and
emission spectroscopies, as well as X-ray spectroscopies, are applied
to characterize the thin film electronic and photophysical properties.
Planar heterojunction solar cells are fabricated with a BO-ADPM:CA
film as the electron donor and C<sub>60</sub> as the acceptor. With
an increase in the dielectric constant of the donor film from ∼4.5
to ∼11, the exciton binding energy is reduced and the internal
quantum efficiency of the photovoltaic cells improves across the entire
spectrum, with an ∼30% improvement in the BO-ADPM photoactive
region
High-Capacity, Aliovalently Doped Olivine LiMn<sub>1–3<i>x</i>/2</sub>V<sub><i>x</i></sub>□<sub><i>x</i>/2</sub>PO<sub>4</sub> Cathodes without Carbon Coating
A substantial amount of Mn<sup>2+</sup> has been aliovalently substituted
by V<sup>3+</sup> in cation-deficient LiMn<sub>1–3<i>x</i>/2</sub>V<sub><i>x</i></sub>□<sub><i>x</i>/2</sub>PO<sub>4</sub> (0 ≤ <i>x</i> ≤ 0.20)
by a low-temperature (<300 °C) microwave-assisted solvothermal
(MW-ST) process. The necessity of a low-temperature synthesis to achieve
higher levels of doping is demonstrated as the solubility of vanadium
decreases with the formation of impurity phases on heating the samples
to ≥575 °C. Soft X-ray absorption spectroscopy reveals
enhanced Mn–O hybridization in the vanadium-doped samples,
which is believed to facilitate an increase in capacity with increasing
vanadium content in the lattice. For example, a high capacity of 155
mAh/g is achieved above a cutoff voltage of 3 V without any carbon
coating for the <i>x</i> = 0.2 sample. The vanadium substitution
enhances the overall kinetics of the material by lowering the charge-transfer
impedance and increasing the lithium-diffusion coefficient
Probing LaMO<sub>3</sub> Metal and Oxygen Partial Density of States Using X‑ray Emission, Absorption, and Photoelectron Spectroscopy
We examined the electronic structure
in LaMO<sub>3</sub> perovskite
oxides (M = Cr, Mn, Fe, Co, Ni) by combining information from X-ray
emission, absorption, and photoelectron spectroscopy. Through first-principles
density functional theory simulations, we identified complementary
hybridization features present in the transition metal and oxygen
X-ray emission spectra. We then developed a method for the self-consistent
alignment of the emission data onto a common energy scale using these
features, providing a valuable supplementary technique to photoelectron
spectroscopy for studying the partial density of states in perovskites.
The combined information from X-ray emission and absorption was used
to explore trends in electronic structure characteristics under the
Zaanen–Sawatzky–Allen frameworknamely the extent
of metal–oxygen hybridization, band gap, and charge-transfer
gap. We further established a method that allows for the experimental
determination of the occupied and unoccupied band positions relative
to the oxide Fermi level, as well as on an absolute energy scale