49 research outputs found
Transdermal drug delivery by microneedles: does skin metabolism matter?
Microneedle arrays have been shown to increase skin permeability for the
transdermal delivery of drugs with high molecular weights. Various theoretical
studies have been proposed to predict the drug transport behaviour after drug injection
using microneedles. However it is important for the optimal design of
microneedle systems to consider the effects of biological factors such as skin
metabolism and variations in pharmacokinetic parameters as well as to improve
the enhancement of skin permeability. A mathematical model for microneedle
systems is introduced and applied to simulate the verapamil transport with metabolism
in the skin. A comparative analysis for a transdermal delivery of verapamil from
microneedles is presented in this paper. The results indicate that the skin metabolism
does not markedly affect the skin permeation after verapamil injection using microneedles
Synthesis, Direct Formation under High Pressure, Structure, and Electronic Properties of LiNbO<sub>3</sub>‑type Oxide PbZnO<sub>3</sub>
A novel LiNbO<sub>3</sub>-type (LN-type) lead zinc oxide, PbZnO<sub>3</sub>, was successfully
synthesized under high pressure and temperature. Rietveld structure
refinement using synchrotron powder X-ray diffraction (XRD) data demonstrated
that LN-type PbZnO<sub>3</sub> crystallized into a trigonal structure
with a polar space group (<i>R</i>3<i>c</i>).
The bond valence sum estimated from the interatomic distances indicated
that the sample possesses a Pb<sup>4+</sup>Zn<sup>2+</sup>O<sub>3</sub> valence state. Polarization could evolve as a result of the repulsion
between constituent cations because PbZnO<sub>3</sub> does not contain
a stereochemical 6s<sup>2</sup> cation or a Jahn–Teller active
d<sup>0</sup> cation. Distortion of ZnO<sub>6</sub> octahedra resulting
from cation shift is comparable with that of d<sup>0</sup> TiO<sub>6</sub> in ZnTiO<sub>3</sub> and MnTiO<sub>3</sub> with LN-type oxides,
which leads to stabilization of the polar structure. PbZnO<sub>3</sub> exhibited metallic behavior and temperature-independent diamagnetic
character. <i>In situ</i> XRD measurement revealed that
the formation of LN-type PbZnO<sub>3</sub> occurred directly without
the formation of a perovskite phase, which is unusual among LN-type
materials obtained by high-pressure synthesis
Polymer/Polymer Blend Solar Cells Improved by Using High-Molecular-Weight Fluorene-Based Copolymer as Electron Acceptor
The highest power conversion efficiency (PCE) of 2.7%
has been
achieved for all-polymer solar cells made with a blend of poly(3-hexylthiophene)
(P3HT, electron donor) and poly[2,7-(9,9-didodecylfluorene)-<i>alt</i>-5,5-(4′,7′-bis(2-thienyl)-2′,1′,3′-benzothiadiazole)]
(PF12TBT, electron acceptor). The PCE of the P3HT/PF12TBT solar cells
increases from 1.9% to 2.7% with an increase in the molecular weight
(<i>M</i><sub>w</sub>) of PF12TBT from 8500 to 78 000
g mol<sup>–1</sup>. In a device with high-molecular-weight
PF12TBT, efficient charge generation is maintained even at high annealing
temperatures because of the small phase separation on the length scale
of exciton diffusion due to an increase in the glass transition temperature
(<i>T</i><sub>g</sub>) and a reduced
diffusional mobility of the PF12TBT chains above <i>T</i><sub>g</sub>. On the other hand, efficient charge transport is also
achieved through the formation of interconnected networks of PF12TBT-rich
domains, which is facilitated by the high molecular weight of PF12TBT,
and the ordering of P3HT chains in P3HT-rich domains, which is a result
of high-temperature annealing. Thus, when high-molecular-weight PF12TBT
is used, an optimal blend morphology that supports efficient charge
generation as well as charge transport can be obtained by thermal
annealing, and consequently, the highest PCE reported so far for an
all-polymer solar cell is achieved
High-Energy-Density Rechargeable Lithium–Nickel Chloride Aqueous Solution Batteries
High-energy-density rechargeable
batteries with performance beyond
that of lithium-ion batteries are required for next-generation electric
vehicles. We propose a novel rechargeable battery with a lithium anode
and a NiCl<sub>2</sub> aqueous cathode that is separated Li<sub>1.4</sub>Al<sub>0.4</sub>Ge<sub>0.2</sub>Ti<sub>1.4</sub>(PO<sub>4</sub>)<sub>3</sub> as a water-stable lithium-ion-conducting solid electrolyte.
The cell was discharged up to 93% of the theoretical cathode capacity
at 0.5 mA cm<sup>–2</sup> and 25 °C. The calculated energy
density, based on the weights of NiCl<sub>2</sub> and Li, and the
average discharge voltage of 2.4 V at 0.5 mA cm<sup>–2</sup>, was 852 Wh kg<sup>–1</sup>, which is more than twice as
high as that of conventional lithium-ion batteries. The cell was successfully
cycled for 50 cycles without any degradation of the charge and discharge
voltages at 0.5 mA cm<sup>–2</sup> and 25 °C for 5 h charge
and 5 h discharge, where the utilization of NiCl<sub>2</sub> was 80%
Charge Transport in Intermixed Regions of All-Polymer Solar Cells Studied by Conductive Atomic Force Microscopy
Charge
transport in intermixed regions of all-polymer solar cells based on
a blend of poly(3-hexylthiophene) (P3HT; electron donor) with
poly[2,7-(9,9-didodecylfluorene)-<i>alt</i>-5,5-(4′,7′-bis(2-thienyl)-2′,1′,3′-benzothiadiazole)]
(PF12TBT; electron acceptor) was studied by conductive atomic force
microscopy (C-AFM). For a blend film fabricated from a chlorobenzene
solution, intermixed regions were detected between the P3HT-rich and
PF12TBT-rich domains. The overall hole current in the intermixed regions
remained almost constant, both before and after thermal annealing
at 80 °C, but it increased in the P3HT-rich domains. For a blend
film fabricated from a chloroform solution, the entire observed area
constituted an intermixed region, both before and after thermal annealing.
The overall hole current in this film was significantly improved following
thermal annealing at 120 °C. These finely mixed structures with
efficient charge transport yielded a maximum power conversion efficiency
of 3.5%. The local charge-transport properties in the intermixed region,
as observed via C-AFM, was found to be closely related to the photovoltaic
properties, rather than the bulk-averaged properties or topological
features
High-Pressure Synthesis, Crystal Structure, and Phase Stability Relations of a LiNbO<sub>3</sub>‑Type Polar Titanate ZnTiO<sub>3</sub> and Its Reinforced Polarity by the Second-Order Jahn–Teller Effect
A polar
LiNbO<sub>3</sub>-type (LN-type) titanate ZnTiO<sub>3</sub> has been
successfully synthesized using ilmenite-type (IL-type)
ZnTiO<sub>3</sub> under high pressure and high temperature. The first
principles calculation indicates that LN-type ZnTiO<sub>3</sub> is
a metastable phase obtained by the transformation in the decompression
process from the perovskite-type phase, which is stable at high pressure
and high temperature. The Rietveld structural refinement using synchrotron
powder X-ray diffraction data reveals that LN-type ZnTiO<sub>3</sub> crystallizes into a hexagonal structure with a polar space group <i>R</i>3<i>c</i> and exhibits greater intradistortion
of the TiO<sub>6</sub> octahedron in LN-type ZnTiO<sub>3</sub> than
that of the SnO<sub>6</sub> octahedron in LN-type ZnSnO<sub>3</sub>. The estimated spontaneous polarization (75 μC/cm<sup>2</sup>, 88 μC/cm<sup>2</sup>) using the nominal charge and the Born
effective charge (BEC) derived from density functional perturbation
theory, respectively, are greater than those of ZnSnO<sub>3</sub> (59
μC/cm<sup>2</sup>, 65 μC/cm<sup>2</sup>), which is strongly
attributed to the great displacement of Ti from the centrosymmetric
position along the <i>c</i>-axis and the fact that the BEC
of Ti (+6.1) is greater than that of Sn (+4.1). Furthermore, the spontaneous
polarization of LN-type ZnTiO<sub>3</sub> is greater than that of
LiNbO<sub>3</sub> (62 μC/cm<sup>2</sup>, 76 μC/cm<sup>2</sup>), indicating that LN-type ZnTiO<sub>3</sub>, like LiNbO<sub>3</sub>, is a candidate ferroelectric material with high performance.
The second harmonic generation (SHG) response of LN-type ZnTiO<sub>3</sub> is 24 times greater than that of LN-type ZnSnO<sub>3</sub>. The findings indicate that the intraoctahedral distortion, spontaneous
polarization, and the accompanying SHG response are caused by the
stabilization of the polar LiNbO<sub>3</sub>-type structure and reinforced
by the second-order Jahn–Teller effect attributable to the
orbital interaction between oxygen ions and d<sup>0</sup> ions such
as Ti<sup>4+</sup>
High-Pressure Synthesis of <i>A</i>‑Site Ordered Double Perovskite CaMnTi<sub>2</sub>O<sub>6</sub> and Ferroelectricity Driven by Coupling of <i>A</i>‑Site Ordering and the Second-Order Jahn–Teller Effect
We successfully synthesized a novel
ferroelectric <i>A</i>-site-ordered double perovskite CaMnTi<sub>2</sub>O<sub>6</sub> under
high-pressure and investigated its structure, ferroelectric, magnetic
and dielectric properties, and high-temperature phase transition behavior.
Optical second harmonic generation signal, by frequency doubling 1064
nm radiation to 532 nm, was observed and its efficiency is about 9
times as much as that of SiO<sub>2</sub> (α-quartz). This compound
possesses a tetragonal polar structure with space group <i>P</i>4<sub>2</sub><i>mc</i>. <i>P</i>-<i>E</i> hysteresis measurement demonstrated that CaMnTi<sub>2</sub>O<sub>6</sub> is also ferroelectric. A spontaneous polarization calculated
by use of point charge model and the observed remnant polarization
are 24 and 3.5 μC/cm<sup>2</sup>, respectively. CaMnTi<sub>2</sub>O<sub>6</sub> undergoes a ferroelectric–paraelectric order–disorder-type
phase transition at 630 K. The structural analysis implies that both
the ordering of shift of Mn<sup>2+</sup> from the square-planar and
the off-center displacement of Ti<sup>4+</sup> in TiO<sub>6</sub> octahedra
are responsible for ferroelectricity. CaMnTi<sub>2</sub>O<sub>6</sub> belongs to a new class of ferroelectrics in which <i>A</i>-site ordering and second-order Jahn–Teller distortion are
cooperatively coupled. The finding gave us a new concept for the design
of ferroelectric materials
Changes in functional connectivity in resting state networks.
<p>Regions showing significant changes in functional connectivity in the (A) right executive control network (RECN), (B) left executive control network (LECN), and (C) ventral default mode network (vDMN) (p < 0.05 TFCE-cluster corrected for multiple comparison). HC–healthy control, BT–patients with brain tumor. Resting state networks are shown in yellow. Center of the cursor locates maximum significance.</p
Spatial distribution of tumors in MNI standard space superimposed on a standard anatomical template.
<p>This frequency map shows the number of patients with tumor in a given voxel.</p
Regions correlated with the right angular gyrus (Fig. 2C) obtained using seed-based connectivity analysis in (A) healthy controls and (B) patients with gliomas.
<p>Correlations in several regions in the left hemisphere, indicated by yellow circle in (A), are no longer significant in patients with gliomas although only the region in the middle temporal gyrus showed statistical significance. The maps showed voxels with t values < 3.5.</p