10 research outputs found
In Situ Derived Ni<sub><i>x</i></sub>Fe<sub>1–<i>x</i></sub>OOH/NiFe/Ni<sub><i>x</i></sub>Fe<sub>1–<i>x</i></sub>OOH Nanotube Arrays from NiFe Alloys as Efficient Electrocatalysts for Oxygen Evolution
Herein, Ni<sub><i>x</i></sub>Fe<sub>1–<i>x</i></sub>OOH/NiFe/Ni<sub><i>x</i></sub>Fe<sub>1–<i>x</i></sub>OOH
sandwich-structured nanotube arrays (SNTAs) supported on carbon fiber
cloth (CFC) (Ni<sub><i>x</i></sub>Fe<sub>1–<i>x</i></sub>OOH/NiFe/Ni<sub><i>x</i></sub>Fe<sub>1–<i>x</i></sub>OOH SNTAs–CFC) have been developed as flexible
high-performance oxygen evolution reaction (OER) catalysts by a facile
in situ electrochemical oxidation of NiFe metallic alloy nanotube
arrays during oxygen evolution process. Benefiting from the advantages
of high conductivity, hollow nanotube array, and porous structure,
Ni<sub><i>x</i></sub>Fe<sub>1–<i>x</i></sub>OOH/NiFe/Ni<sub><i>x</i></sub>Fe<sub>1–<i>x</i></sub>OOH SNTAs–CFC exhibited a low overpotential of ∼220
mV at the current density of 10 mA cm<sup>–2</sup> and a small
Tafel slope of 57 mV dec<sup>–1</sup> in alkaline solution,
both of which are smaller than those of most OER electrocatalysts.
Furthermore, Ni<sub><i>x</i></sub>Fe<sub>1–<i>x</i></sub>OOH/NiFe/Ni<sub><i>x</i></sub>Fe<sub>1–<i>x</i></sub>OOH SNTAs–CFC exhibits excellent stability
at 100 mA cm<sup>–2</sup> for more than 30 h. It is believed
that the present work can provide a valuable route for the design
and synthesis of inexpensive and efficient OER electrocatalysts
Defect Structure, Phase Separation, and Electrical Properties of Nonstoichiometric Tetragonal Tungsten Bronze Ba<sub>0.5–<i>x</i></sub>TaO<sub>3–<i>x</i></sub>
New
insight into the defect chemistry of the tetragonal tungsten bronze
(TTB) Ba<sub>0.5–<i>x</i></sub>TaO<sub>3–<i>x</i></sub> is established here, which is shown to adapt to
a continuous and extensive range of both cationic and anionic defect
stoichiometries. The highly nonstoichiometric TTB Ba<sub>0.5–<i>x</i></sub>TaO<sub>3–<i>x</i></sub> (<i>x</i> = 0.25–0.325) compositions are stabilized via the
interpolation of Ba<sup>2+</sup> cations and (TaO)<sup>3+</sup> groups
into pentagonal tunnels, forming distinct Ba chains and alternate
Ta-O rows in the pentagonal tunnels along the <i>c</i> axis.
The slightly nonstoichiometric Ba<sub>0.5–<i>x</i></sub>TaO<sub>3–<i>x</i></sub> (<i>x</i> = 0–0.1) compositions incorporate framework oxygen and tunnel
cation deficiencies in the TTB structure. These two mechanisms result
in phase separation within the 0.1< <i>x</i> < 0.25
nonstoichiometric range, resulting in two closely related (TaO)<sup>3+</sup>-containing and (TaO)<sup>3+</sup>-free TTB phases. The highly
nonstoichiometric (TaO)<sup>3+</sup>-containing phase exhibits Ba<sup>2+</sup> cationic migration. The incorporation of (TaO)<sup>3+</sup> units into the pentagonal tunnel and the local relaxation of the
octahedral framework around the (TaO)<sup>3+</sup> units are revealed
by diffraction data analysis and are shown to affect the transport
and polarization properties of these compositions
Defect Structure, Phase Separation, and Electrical Properties of Nonstoichiometric Tetragonal Tungsten Bronze Ba<sub>0.5–<i>x</i></sub>TaO<sub>3–<i>x</i></sub>
New
insight into the defect chemistry of the tetragonal tungsten bronze
(TTB) Ba<sub>0.5–<i>x</i></sub>TaO<sub>3–<i>x</i></sub> is established here, which is shown to adapt to
a continuous and extensive range of both cationic and anionic defect
stoichiometries. The highly nonstoichiometric TTB Ba<sub>0.5–<i>x</i></sub>TaO<sub>3–<i>x</i></sub> (<i>x</i> = 0.25–0.325) compositions are stabilized via the
interpolation of Ba<sup>2+</sup> cations and (TaO)<sup>3+</sup> groups
into pentagonal tunnels, forming distinct Ba chains and alternate
Ta-O rows in the pentagonal tunnels along the <i>c</i> axis.
The slightly nonstoichiometric Ba<sub>0.5–<i>x</i></sub>TaO<sub>3–<i>x</i></sub> (<i>x</i> = 0–0.1) compositions incorporate framework oxygen and tunnel
cation deficiencies in the TTB structure. These two mechanisms result
in phase separation within the 0.1< <i>x</i> < 0.25
nonstoichiometric range, resulting in two closely related (TaO)<sup>3+</sup>-containing and (TaO)<sup>3+</sup>-free TTB phases. The highly
nonstoichiometric (TaO)<sup>3+</sup>-containing phase exhibits Ba<sup>2+</sup> cationic migration. The incorporation of (TaO)<sup>3+</sup> units into the pentagonal tunnel and the local relaxation of the
octahedral framework around the (TaO)<sup>3+</sup> units are revealed
by diffraction data analysis and are shown to affect the transport
and polarization properties of these compositions
Chemically Lithiated TiO<sub>2</sub> Heterostructured Nanosheet Anode with Excellent Rate Capability and Long Cycle Life for High-Performance Lithium-Ion Batteries
A new form of dual-phase heterostructured
nanosheet comprised of
oxygen-deficient TiO<sub>2</sub>/Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> has been successfully synthesized and used as anode material
for lithium ion batteries. With the three-dimensional (3D) Ti mesh
as both the conducting substrate and the Ti<sup>3+</sup>/Ti<sup>4+</sup> source, blue anatase Ti<sup>3+</sup>/TiO<sub>2</sub>nanosheets were
grown by a hydrothermal reaction. By controlling the chemical lithiation
period of TiO<sub>2</sub> nanosheets, a phase boundary was created
between the TiO<sub>2</sub> and the newly formed Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub>, which contribute additional capacity benefiting
from favorable charge separation between the two phase interfaces.
Through further hydrogenation of the 3D TiO<sub>2</sub>/Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> heterostructured nanosheets (denoted
as H-TiO<sub>2</sub>/LTO HNS), an extraordinary rate performance with
capacity of 174 mAh g<sup>–1</sup> at 200 C and outstanding
long-term cycling stability with only an ∼6% decrease of its
initial specific capacity after 6000 cycles were delivered. The heterostructured
nanosheet morphology provides a short length of lithium diffusion
and high electrode/electrolyte contact area, which could also explain
the remarkable lithium storage performance. In addition, the full
battery assembled based on the H-TiO<sub>2</sub>/LTO anode achieves
high energy and power densities
High Energy Density Asymmetric Quasi-Solid-State Supercapacitor Based on Porous Vanadium Nitride Nanowire Anode
To push the energy density limit
of asymmetric supercapacitors
(ASCs), a new class of anode materials is needed. Vanadium nitride
(VN) holds great promise as anode material for ASCs due to its large
specific capacitance, high electrical conductivity, and wide operation
windows in negative potential. However, its poor electrochemical stability
severely limits its application in SCs. In this work, we demonstrated
high energy density, stable, quasi-solid-state ASC device based on
porous VN nanowire anode and VO<sub><i>x</i></sub> nanowire
cathode for the first time. The VO<sub><i>x</i></sub>//VN-ASC
device exhibited a stable electrochemical window of 1.8 V and excellent
cycling stability with only 12.5% decrease of capacitance after 10 000
cycles. More importantly, the VO<sub><i>x</i></sub>//VN-ASC
device achieved a high energy density of 0.61 mWh cm<sup>–3</sup> at current density of 0.5 mA cm<sup>–2</sup> and a high power
density of 0.85 W cm<sup>–3</sup> at current density of 5 mA
cm<sup>–2</sup>. These values are substantially enhanced compared
to most of the reported quasi/all-solid-state SC devices. This work
constitutes the first demonstration of using VN nanowires as high
energy anode, which could potentially improve the performance of energy
storage devices
Stabilized TiN Nanowire Arrays for High-Performance and Flexible Supercapacitors
Metal nitrides have received increasing attention as
electrode
materials for high-performance supercapacitors (SCs). However, most
of them are suffered from poor cycling stability. Here we use TiN
as an example to elucidate the mechanism causing the capacitance loss.
X-ray photoelectron spectroscopy analyses revealed that the instability
is due to the irreversible electrochemical oxidation of TiN during
the charging/discharging process. Significantly, we demonstrate for
the first time that TiN can be stabilized without sacrificing its
electrochemical performance by using poly(vinyl alcohol) (PVA)/KOH
gel as the electrolyte. The polymer electrolyte suppresses the oxidation
reaction on electrode surface. Electrochemical studies showed that
the TiN solid-state SCs exhibit extraordinary stability up to 15 000
cycles and achieved a high volumetric energy density of 0.05 mWh/cm<sup>3</sup>. The capability of effectively stabilizing nitride materials
could open up new opportunities in developing high-performance and
flexible SCs
Localization of Oxygen Interstitials in CeSrGa<sub>3</sub>O<sub>7+δ</sub> Melilite
The
solubility of Ce in the La<sub>1–<i>x</i></sub>Ce<sub><i>x</i></sub>SrGa<sub>3</sub>O<sub>7+δ</sub> and
La<sub>1.54–<i>x</i></sub>Ce<sub><i>x</i></sub>Sr<sub>0.46</sub>Ga<sub>3</sub>O<sub>7.27+δ</sub> melilites
was investigated, along with the thermal redox stability in air of
these melilites and the conductivity variation associated with oxidization
of Ce<sup>3+</sup> into Ce<sup>4+</sup>. Under CO reducing atmosphere,
the La in LaSrGa<sub>3</sub>O<sub>7</sub> may be completely substituted
by Ce to form the La<sub>1–<i>x</i></sub>Ce<sub><i>x</i></sub>SrGa<sub>3</sub>O<sub>7+δ</sub> solid solution,
which is stable in air to ∼600 °C when <i>x</i> ≥ 0.6. On the other side, the La<sub>1.54–<i>x</i></sub>Ce<sub><i>x</i></sub>Sr<sub>0.46</sub>Ga<sub>3</sub>O<sub>7.27+δ</sub> compositions displayed much lower
Ce solubility (<i>x</i> ≤ 0.1), irrespective of the
synthesis atmosphere. In the as-made La<sub>1–<i>x</i></sub>Ce<sub><i>x</i></sub>SrGa<sub>3</sub>O<sub>7+δ</sub>, the conductivity increased with the cerium content, due to the
enhanced electronic conduction arising from the 4f electrons in Ce<sup>3+</sup> cations. At 600 °C, CeSrGa<sub>3</sub>O<sub>7+δ</sub> showed a conductivity of ∼10<sup>–4</sup> S/cm in
air, nearly 4 orders of magnitude higher than that of LaSrGa<sub>3</sub>O<sub>7</sub>. The oxidation of Ce<sup>3+</sup> into Ce<sup>4+</sup> in CeSrGa<sub>3</sub>O<sub>7+δ</sub> slightly reduced the
conductivity, and the oxygen excess did not result in apparent increase
of oxide ion conduction in CeSrGa<sub>3</sub>O<sub>7+δ</sub>. The Ce doping in air also reduced the interstitial oxide ion conductivity
of La<sub>1.54</sub>Sr<sub>0.46</sub>Ga<sub>3</sub>O<sub>7.27</sub>. Neutron powder diffraction study on CeSrGa<sub>3</sub>O<sub>7.39</sub> composition revealed that the extra oxygen is incorporated in the
four-linked GaO<sub>4</sub> polyhedral environment, leading to distorted
GaO<sub>5</sub> trigonal bipyramid. The stabilization and low mobility
of interstitial oxygen atoms in CeSrGa<sub>3</sub>O<sub>7+δ</sub>, in contrast with those in La<sub>1+<i>x</i></sub>Sr<sub>1–<i>x</i></sub>Ga<sub>3</sub>O<sub>7+0.5<i>x</i></sub>, may be correlated with the cationic size contraction
from the oxidation of Ce<sup>3+</sup> to Ce<sup>4+</sup>. These results
provide a new comprehensive understanding of the accommodation and
conduction mechanism of the oxygen interstitials in the melilite structure
Multiple Nucleation and Crystal Growth of Barium Titanate
Crystal growth of cubic BaTiO<sub>3</sub> in the presence
of polyethylene
glycol-200 (PEG-200) is investigated step by step using powder X-ray
diffraction, scanning electron microscopy, and transmission electron
microscopy. Titanium precursor Ti(OC<sub>4</sub>H<sub>9</sub>)<sub>4</sub> aggregates with PEG to form spherical colloidal particles
at the very beginning. Multiple nucleation of BaTiO<sub>3</sub> takes
place on the surface of these colloidal particles. The nanocrystallites
then self-adjust their orientations likely under dipole–dipole
interaction and/or intercrystallite interactions enhanced by surface
adsorbed polymers, followed by an orientated connection and crystal
extension via an Ostwald ripening process. The final BaTiO<sub>3</sub> crystals have a novel dodecahedral morphology. The formation mechanism
is proposed to be attributed to the selective adsorption of PEG molecules
on the {110} crystal planes, significantly reducing the crystal growth
rate on these surfaces. A kinetic model is proposed based on the calculated
crystallite sizes using the Scherrer equation. The physical meaning
of the model and a significant fake reduction of the crystallite size
is discussed
Carbon Quantum Dot Surface-Engineered VO<sub>2</sub> Interwoven Nanowires: A Flexible Cathode Material for Lithium and Sodium Ion Batteries
The
use of electrode materials in their powdery form requires binders
and conductive additives for the fabrication of the cells, which leads
to unsatisfactory energy storage performance. Recently, a new strategy
to design flexible, binder-, and additive-free three-dimensional electrodes
with nanoscale surface engineering has been exploited in boosting
the storage performance of electrode materials. In this paper, we
design a new type of free-standing carbon quantum dot coated VO<sub>2</sub> interwoven nanowires through a simple fabrication process
and demonstrate its potential to be used as cathode material for lithium
and sodium ion batteries. The versatile carbon quantum dots that are
vastly flexible for surface engineering serve the function of protecting
the nanowire surface and play an important role in the diffusion of
electrons. Also, the three-dimensional carbon cloth coated with VO<sub>2</sub> interwoven nanowires assisted in the diffusion of ions through
the inner and the outer surface. With this unique architecture, the
carbon quantum dot nanosurface engineered VO<sub>2</sub> electrode
exhibited capacities of 420 and 328 mAh g<sup>–1</sup> at current
density rate of 0.3 C for lithium and sodium storage, respectively.
This work serves as a milestone for the potential replacement of lithium
ion batteries and next generation postbatteries
Green Light-Excitable Ce-Doped Nitridomagnesoaluminate Sr[Mg<sub>2</sub>Al<sub>2</sub>N<sub>4</sub>] Phosphor for White Light-Emitting Diodes
Green Light-Excitable Ce-Doped Nitridomagnesoaluminate
Sr[Mg<sub>2</sub>Al<sub>2</sub>N<sub>4</sub>] Phosphor for White Light-Emitting
Diode