7 research outputs found
Morphology-Dependent Enhancement of the Pseudocapacitance of Template-Guided Tunable Polyaniline Nanostructures
Polyaniline
is one of the most investigated conducting polymers
as supercapacitor material for energy storage applications. The preparation
of nanostructured polyaniline with well-controlled morphology is crucial
to obtaining good supercapacitor performance. We present here a facile
chemical process to produce polyaniline nanostructures with three
different morphologies (i.e., nanofibers, nanospheres, and nanotubes)
by utilizing the corresponding tunable morphology of MnO<sub>2</sub> reactive templates. A growth mechanism is proposed to explain the
evolution of polyaniline morphology based on the reactive templates.
The morphology-induced improvement in the electrochemical performance
of polyaniline pseudocapacitors is as large as 51% due to the much
enhanced surface area and the porous nature of the template-guided
polyaniline nanostructures. In addition, and for the first time, a
redox-active electrolyte is applied to the polyaniline pseudocapacitors
to achieve significant enhancement of pseudocapacitance. Compared
to the conventional electrolyte, the enhancement of pseudocapacitance
in the redox-active electrolyte is 49%–78%, depending on the
specific polyaniline morphology, reaching the highest reported capacitance
of 896 F/g for polyaniline full cells so far
Substrate Dependent Self-Organization of Mesoporous Cobalt Oxide Nanowires with Remarkable Pseudocapacitance
A scheme of current collector dependent self-organization
of mesoporous
cobalt oxide nanowires has been used to create unique supercapacitor
electrodes, with each nanowire making direct contact with the current
collector. The fabricated electrodes offer the desired properties
of macroporosity to allow facile electrolyte flow, thereby reducing
device resistance and nanoporosity with large surface area to allow
faster reaction kinetics. Co<sub>3</sub>O<sub>4</sub> nanowires grown
on carbon fiber paper collectors self-organize into a brush-like morphology
with the nanowires completely surrounding the carbon microfiber cores.
In comparison, Co<sub>3</sub>O<sub>4</sub> nanowires grown on planar
graphitized carbon paper collectors self-organize into a flower-like
morphology. In three electrode configuration, brush-like and flower-like
morphologies exhibited specific capacitance values of 1525 and 1199
F/g, respectively, at a constant current density of 1 A/g. In two
electrode configuration, the brush-like nanowire morphology resulted
in a superior supercapacitor performance with high specific capacitances
of 911 F/g at 0.25 A/g and 784 F/g at 40 A/g. In comparison, the flower-like
morphology exhibited lower specific capacitance values of 620 F/g
at 0.25 A/g and 423 F/g at 40 A/g. The Co<sub>3</sub>O<sub>4</sub> nanowires with brush-like morphology exhibited high values of specific
power (71 kW/kg) and specific energy (81 Wh/kg). Maximum energy and
power densities calculated for Co<sub>3</sub>O<sub>4</sub> nanowires
with flower-like morphology were 55 Wh/kg and 37 kW/kg respectively.
Both electrode designs exhibited excellent cycling stability by retaining
∼91–94% of their maximum capacitance after 5000 cycles
of continuous charge–discharge
Enhanced Rate Performance of Mesoporous Co<sub>3</sub>O<sub>4</sub> Nanosheet Supercapacitor Electrodes by Hydrous RuO<sub>2</sub> Nanoparticle Decoration
Mesoporous cobalt oxide (Co<sub>3</sub>O<sub>4</sub>) nanosheet
electrode arrays are directly grown over flexible carbon paper substrates
using an economical and scalable two-step process for supercapacitor
applications. The interconnected nanosheet arrays form a three-dimensional
network with exceptional supercapacitor performance in standard two
electrode configuration. Dramatic improvement in the rate capacity
of the Co<sub>3</sub>O<sub>4</sub> nanosheets is achieved by electrodeposition
of nanocrystalline, hydrous RuO<sub>2</sub> nanoparticles dispersed
on the Co<sub>3</sub>O<sub>4</sub> nanosheets. An optimum RuO<sub>2</sub> electrodeposition time is found to result in the best supercapacitor
performance, where the controlled morphology of the electrode provides
a balance between good conductivity and efficient electrolyte access
to the RuO<sub>2</sub> nanoparticles. An excellent specific capacitance
of 905 F/g at 1 A/g is obtained, and a nearly constant rate performance
of 78% is achieved at current density ranging from 1 to 40 A/g. The
sample could retain more than 96% of its maximum capacitance even
after 5000 continuous charge-discharge cycles at a constant high current
density of 10 A/g. Thicker RuO<sub>2</sub> coating, while maintaining
good conductivity, results in agglomeration, decreasing electrolyte
access to active material and hence the capacitive performance
Effect of Postetch Annealing Gas Composition on the Structural and Electrochemical Properties of Ti<sub>2</sub>CT<sub><i>x</i></sub> MXene Electrodes for Supercapacitor Applications
Two-dimensional Ti<sub>2</sub>CT<sub><i>x</i></sub> MXene
nanosheets were prepared by the selective etching of Al layer from
Ti<sub>2</sub>AlC MAX phase using HF treatment. The MXene sheets retained
the hexagonal symmetry of the parent Ti<sub>2</sub>AlC MAX phase.
Effect of the postetch annealing ambient (Ar, N<sub>2</sub>, N<sub>2</sub>/H<sub>2</sub>, and air) on the structure and electrochemical
properties of the MXene nanosheets was investigated in detail. After
annealing in air, the MXene sheets exhibited variations in structure,
morphology, and electrochemical properties as compared to HF treated
MAX phase. In contrast, samples annealed in Ar, N<sub>2</sub>, and
N<sub>2</sub>/H<sub>2</sub> ambient retained their original morphology.
However, a significant improvement in the supercapacitor performance
is observed upon heat treatment in Ar, N<sub>2</sub>, and N<sub>2</sub>/H<sub>2</sub> ambients. When used in symmetric two-electrode configuration,
the MXene sample annealed in N<sub>2</sub>/H<sub>2</sub> atmosphere
exhibited the best capacitive performance with specific capacitance
value (51 F/g at 1A/g) and high rate performance (86%). This improvement
in the electrochemical performance of annealed samples is attributed
to highest carbon content, and lowest fluorine content on the surface
of the sample upon annealing, while retaining the original two-dimensional
layered morphology and providing maximum access of aqueous electrolyte
to the electrodes
Surface Passivation of MoO<sub>3</sub> Nanorods by Atomic Layer Deposition toward High Rate Durable Li Ion Battery Anodes
We demonstrate an effective strategy
to overcome the degradation of MoO<sub>3</sub> nanorod anodes in lithium
(Li) ion batteries at high-rate cycling. This is achieved by conformal
nanoscale surface passivation of the MoO<sub>3</sub> nanorods by HfO<sub>2</sub> using atomic layer deposition (ALD). At high current density
such as 1500 mA/g, the specific capacity of HfO<sub>2</sub>-coated
MoO<sub>3</sub> electrodes is 68% higher than that of bare MoO<sub>3</sub> electrodes after 50 charge/discharge cycles. After 50 charge/discharge
cycles, HfO<sub>2</sub>-coated MoO<sub>3</sub> electrodes exhibited
specific capacity of 657 mAh/g; on the other hand, bare MoO<sub>3</sub> showed only 460 mAh/g. Furthermore, we observed that HfO<sub>2</sub>-coated MoO<sub>3</sub> electrodes tend to stabilize faster than
bare MoO<sub>3</sub> electrodes because nanoscale HfO<sub>2</sub> layer
prevents structural degradation of MoO<sub>3</sub> nanorods. Additionally,
the growth temperature of MoO<sub>3</sub> nanorods and the effect
of HfO<sub>2</sub> layer thickness was studied and found to be important
parameters for optimum battery performance. The growth temperature
defines the microstructural features and HfO<sub>2</sub> layer thickness
defines the diffusion coefficient of Li-ions through the passivation
layer to the active material. Furthermore, ex situ high resolution
transmission electron microscopy, X-ray photoelectron spectroscopy,
Raman spectroscopy, and X-ray diffraction were carried out to explain
the capacity retention mechanism after HfO<sub>2</sub> coating
Thermoelectric Properties of Strontium Titanate Superlattices Incorporating Niobium Oxide Nanolayers
A novel superlattice structure based
on epitaxial nanoscale layers
of NbO<sub><i>x</i></sub> and Nb-doped SrTiO<sub>3</sub> is fabricated using a layer-by-layer approach on lattice matched
LAO substrates. The absolute Seebeck coefficient and electrical conductivity
of the [(NbO<sub><i>x</i></sub>)<sub><i>a</i></sub>/(Nb-doped SrTiO<sub>3</sub>)<sub><i>b</i></sub>]<sub>20</sub> superlattices (SLs) were found to increase with decreasing layer
thickness ratio (<i>a</i>/<i>b</i> ratio), reaching,
at high temperatures, a power factor that is comparable to epitaxial
Nb-doped SrTiO<sub>3</sub> (STNO) films (∼0.7 W m<sup>–1</sup> K<sup>–1</sup>). High temperature studies reveal that the
SLs behave as n-type semiconductors and undergo an irreversible change
at a varying crossover temperature that depends on the <i>a</i>/<i>b</i> ratio. By use of high resolution X-ray photoelectron
spectroscopy and X-ray diffraction, the irreversible changes are identified
to be due to a phase transformation from cubic NbO to orthorhombic
Nb<sub>2</sub>O<sub>5</sub>, which limits the highest temperature
of stable operation of the superlattice to 950 K
Influence of Stacking Morphology and Edge Nitrogen Doping on the Dielectric Performance of Graphene–Polymer Nanocomposites
We demonstrate that functional groups
obtained by varying the preparation
route of reduced graphene oxide (rGO) highly influence filler morphology
and the overall dielectric performance of rGO-relaxor ferroelectric
polymer nanocomposite. Specifically, we show that nitrogen-doping
by hydrazine along the edges of reduced graphene oxide embedded in
polyÂ(vinylidene fluoride-trifluoroethylene-chlorofluoroethylene) results
in a dielectric permittivity above 10 000 while maintaining
a dielectric loss below 2. This is one of the best-reported dielectric
constant/dielectric loss performance values. In contrast, rGO produced
by the hydrothermal reduction route shows a much lower enhancement,
reaching a maximum dielectric permittivity of 900. Furthermore, functional
derivatives present in rGO are found to strongly affect the quality
of dispersion and the resultant percolation threshold at low loading
levels. However, high leakage
currents and lowered breakdown voltages offset the advantages of increased
capacitance in these ultrahigh-k systems, resulting in no significant
improvement in stored energy density