9 research outputs found
Monolithic Quasi-Solid-State Dye Sensitized Solar Cells Prepared Entirely by Printing Processes
A complete printing process was developed to fabricate
the quasi-solid-state
dye-sensitized solar cells with monolithic structures (m-QS-DSSCs).
First, a structure of m-DSSCs was constructed by sequentially printing
TiO2 layers (main and scattering), a ZrO2 insulating
layer, and a carbon counter electrode (CE) onto an FTO substrate (FTO/TiO2/ZrO2/carbon CE). Then, a quasi-solid-state printable
electrolyte (QS-PE), prepared using polyethylene oxide/polymethyl
methacrylate, was printed directly on top of the porous carbon counter
electrode (CE), enabling the m-QS-DSSCs to be prepared entirely by
printing processes. In this study, the porous structures and characteristics
of the ZrO2 and carbon layers were optimized by controlling
the film thicknesses and heat treatment conditions; furthermore, the
Pt layer was coated to improve the catalytic activity of carbon CEs.
The results revealed that an appropriate porous structure of carbon
and ZrO2 films could be obtained by heating the films from
200 to 500 °C. Through these porous layers, the QS-PE can penetrate
well into the photoelectrodes, increasing the charge transport in
the cells and at the electrode/electrolyte interfaces; therefore,
the m-QS-DSSCs can achieve an efficiency of 6.79% under 1 sun illumination.
Furthermore, the structures can also be utilized to fabricate liquid
cells for application in a dim light environment. The m-QS-DSSCs remained
stable during a long-term stability test at room temperature
Performance Enhancement of Quantum-Dot-Sensitized Solar Cells by Potential-Induced Ionic Layer Adsorption and Reaction
Successive ionic layer adsorption
and reaction (SILAR) technique has been commonly adopted to fabricate
quantum-dot-sensitized solar cells (QDSSCs) in the literature. However,
pore blocking and poor distribution of quantum dots (QDs) in TiO<sub>2</sub> matrices were always encountered. Herein, we report an efficient
method, termed as potential-induced ionic layer adsorption and reaction
(PILAR), for in situ synthesizing and assembling CdSe QDs into mesoporous
TiO<sub>2</sub> films. In the ion adsorption stage of this process,
a negative bias was applied on the TiO<sub>2</sub> film to induce
the adsorption of precursor ions. The experimental results show that
this bias greatly enhanced the ion adsorption, accumulating a large
amount of cadmium ions on the film surface for the following reaction
with selenide precursors. Furthermore, this bias also drove cations
deep into the bottom region of a TiO<sub>2</sub> film. These effects
not only resulted in a higher deposited amount of CdSe, but also a
more uniform distribution of the QDs along the TiO<sub>2</sub> film.
By using the PILAR process, as well as the SILAR process to replenish
the incorporated CdSe, an energy conversion efficiency of 4.30% can
be achieved by the CdSe-sensitized solar cell. This performance is
much higher than that of a cell prepared by the traditional SILAR
process
Poly(ethylene oxide)-co-Poly(propylene oxide)-Based Gel Electrolyte with High Ionic Conductivity and Mechanical Integrity for Lithium-Ion Batteries
Using gel polymer electrolytes (GPEs)
for lithium-ion batteries usually encounters the drawback of poor
mechanical integrity of the GPEs. This study demonstrates the outstanding
performance of a GPE consisting of a commercial membrane (Celgard)
incorporated with a polyÂ(ethylene oxide)-co-polyÂ(propylene oxide)
copolymer (PÂ(EO-co-PO)) swelled by a liquid electrolyte (LE) of 1
M LiPF<sub>6</sub> in carbonate solvents. The proposed GPE stably
holds LE with an amount that is three times that of the Celgard-PÂ(EO-co-PO)
composite. This GPE has a higher ionic conductivity (2.8 × 10<sup>–3</sup> and 5.1 × 10<sup>–4</sup> S cm<sup>–1</sup> at 30 and −20 °C, respectively) and a wider electrochemical
voltage range (5.1 V) than the LE-swelled Celgard because of the strong
ion-solvation power of PÂ(EO-co-PO). The active ion-solvation role
of PÂ(EO-co-PO) also suppresses the formation of the solid–electrolyte
interphase layer. When assembling the GPE in a Li/LiFePO<sub>4</sub> battery, the PÂ(EO-co-PO) network hinders anionic transport, producing
a high Li<sup>+</sup> transference number of 0.5 and decreased the
polarization overpotential. The Li/GPE/LiFePO<sub>4</sub> battery
delivers a discharge capacity of 156–135 mAh g<sup>–1</sup> between 0.1 and 1 C-rates, which is approximately 5% higher than
that of the Li/LE/LiFePO<sub>4</sub> battery. The IR drop of the Li/GPE/LiFePO<sub>4</sub> battery was 44% smaller than that of the Li/LE/LiFePO<sub>4</sub>. The Li/GPE/LiFePO<sub>4</sub> battery is more stable, with
only a 1.2% capacity decay for 150 galvanostatic charge–discharge
cycles. The advantages of the proposed GPE are its high stability,
conductivity, Li<sup>+</sup> transference number, and mechanical integrity,
which allow for the assembly of GPE-based batteries readily scalable
to industrial levels
Graphite Oxide with Different Oxygenated Levels for Hydrogen and Oxygen Production from Water under Illumination: The Band Positions of Graphite Oxide
Graphite oxide (GO) photocatalysts derived from graphite oxidation can have varied electronic properties by varying the oxidation level. Absorption spectroscopy shows the increasing band gap of GO with the oxygen content. Electrochemical analysis along with the Mott–Schottky equation show that the conduction and valence band edge levels of GO from appropriate oxidation are suitable for both the reduction and the oxidation of water. The conduction band edge shows little variation with the oxidation level, and the valence band edge governs the bandgap width of GO. The photocatalytic activity of GO specimens with various oxygenated levels was measured in methanol and AgNO<sub>3</sub> solutions for evolution of H<sub>2</sub> and O<sub>2</sub>, respectively. The H<sub>2</sub> evolution was strong and stable over time, whereas the O<sub>2</sub> evolution was negligibly small due to mutual photocatalytic reduction of the GO with upward shift of the valence band edge under illumination. The conduction band edge of GO showed a negligible change with the illumination. When NaIO<sub>3</sub> was used as a sacrificial reagent to suppress the mutual reduction mechanism under illumination, strong O<sub>2</sub> evolution was observed over the GO specimens. The present study demonstrates that chemical modification can easily modify the electronic properties of GO for specific photosynthetic applications
Tuning the Electronic Structure of Graphite Oxide through Ammonia Treatment for Photocatalytic Generation of H<sub>2</sub> and O<sub>2</sub> from Water Splitting
Graphite
oxide (GO) synthesized from the oxidation of graphite powders exhibits
p-type conductivity and is active in photocatalytic H<sub>2</sub> evolution
from water decomposition. The p-type conductivity hinders hole transfer
for water oxidation and suppresses O<sub>2</sub> evolution. Treating
GO with NH<sub>3</sub> gas at room temperature tunes the electronic
structure by introducing amino and amide groups to its surface. The
ammonia-modified GO (NGO) exhibits n-type conductivity in photoelectrochemical
analysis and has a narrower optical band gap than GO. Electrochemical
analysis attributes the band gap reduction to a negative shift of
the valence band. An NGO-film electrode exhibits a substantially higher
incident photo-to-current efficiency in the visible light region than
a GO electrode. Photoluminescence analyses demonstrate the above-edge
emission characteristic of GO and NGO. NH<sub>3</sub> treatment enhances
the emission by removing nonirradiative epoxy and carboxyl sites on
the GO. In half-reaction tests of water decomposition, NGO effectively
catalyzes O<sub>2</sub> evolution in an aqueous AgNO<sub>3</sub> solution
under mercury-lamp irradiation, whereas GO is inactive. NGO also effectively
catalyzes H<sub>2</sub> evolution in an aqueous methanol solution
but shows less activity than GO. Under illumination with visible light
(λ > 420 nm), NGO simultaneously catalyzes H<sub>2</sub> and
O<sub>2</sub> evolutions, but with a H<sub>2</sub>/O<sub>2</sub> molar
ratio below 2. The n-type conductivity of NGO may hinder electron
transfer and form peroxide species instead of H<sub>2</sub> molecules.
This study demonstrates that the functionality engineering of GO is
a promising technique to synthesize an industrially scalable photocatalyst
for overall water splitting
Graphene Oxide Sponge as Nanofillers in Printable Electrolytes in High-Performance Quasi-Solid-State Dye-Sensitized Solar Cells
A graphene oxide
sponge (GOS) is utilized for the first time as
a nanofiller (NF) in printable electrolytes (PEs) based on polyÂ(ethylene
oxide) and polyÂ(vinylidene fluoride) for quasi-solid-state dye-sensitized
solar cells (QS-DSSCs). The effects of the various concentrations
of GOS NFs on the ion diffusivity and conductivity of electrolytes
and the performance of the QS-DSSCs are studied. The results show
that the presence of GOS NFs significantly increases the diffusivity
and conductivity of the PEs. The introduction of 1.5 wt % of GOS NFs
decreases the charge-transfer resistance at the Pt-counter electrode/electrolyte
interface (<i>R</i><sub>pt</sub>) and increases the recombination
resistance at the photoelectrode/electrolyte interface (<i>R</i><sub>ct</sub>). QS-DSSC utilizing 1.5 wt % GOS NFs can achieve an
energy conversion efficiency (8.78%) higher than that found for their
liquid counterpart and other reported polymer gel electrolytes/GO
NFs based DSSCs. The high energy conversion efficiency is a consequence
of the increase in both the open-circuit potential (<i>V</i><sub>oc</sub>) and fill factor with a slight decrease in current
density (<i>J</i><sub>sc</sub>). The cell efficiency can
retain 86% of its initial value after a 500 h stability test at 60
°C under dark conditions. The long-term stability of the QS-DSSC
with GOS NFs is higher than that without NFs. This result indicates
that the GOS NFs do not cause dye-desorption from the photoanode in
a long-term stability test, which infers a superior performance of
GOS NFs as compared to TiO<sub>2</sub> NFs in terms of increasing
the efficiency and long-term stability of QS-DSSCs
Photocatalytically Reduced Graphite Oxide Electrode for Electrochemical Capacitors
Graphene sheets are an ideal carbon material with the highest area available for electrolyte interaction and can be obtained by reducing graphite oxide (GO). This study presents the photocatalytic reduction of GO in water with mercury-lamp irradiation. The specific capacitance of the reduced GO in an H<sub>2</sub>SO<sub>4</sub> aqueous solution reached levels as high as 220 F g<sup>–1</sup>. This is because of the double layer formation and the reversible pseudocapacitive processes caused by oxygen functionalities at the sheet periphery. The rate capability for charge storage increases with irradiation time due to the continued reduction of oxygenated sites on the graphene basal plane. Alternating current impedance analysis shows that prolonged light irradiation promotes electronic percolation in the electrode, significantly reducing the capacitive relaxation time. With a potential widow of 1 V, the resulting symmetric cells can deliver an energy level of 5 Wh kg<sup>–1</sup> at a high power of 1000 W kg<sup>–1</sup>. These cells show superior stability, with 92% retention of specific capacitance after 20 000 cycles of galvanostatic charge–discharge
Immobilization of Anions on Polymer Matrices for Gel Electrolytes with High Conductivity and Stability in Lithium Ion Batteries
This study reports on a high ionic-conductivity
gel polymer electrolyte (GPE), which is supported by a TiO<sub>2</sub> nanoparticle-decorated polymer framework comprising polyÂ(acrylonitrile-<i>co</i>-vinyl acetate) blended with polyÂ(methyl methacrylate),
i.e., PAVM:TiO<sub>2</sub>. High conductivity GPE-PAVM:TiO<sub>2</sub> is achieved by causing the PAVM:TiO<sub>2</sub> polymer framework
to swell in 1 M LiPF<sub>6</sub> in carbonate solvent. Raman analysis
results demonstrate that the polyÂ(acrylonitrile) (PAN) segments and
TiO<sub>2</sub> nanoparticles strongly adsorb PF<sub>6</sub><sup>–</sup> anions, thereby generating 3D percolative space-charge pathways
surrounding the polymer framework for Li<sup>+</sup>-ion transport.
The ionic conductivity of GPE-PAVM:TiO<sub>2</sub> is nearly 1 order
of magnitude higher than that of commercial separator-supported liquid
electrolyte (SLE). GPE-PAVM:TiO<sub>2</sub> has a high Li<sup>+</sup> transference number (0.7), indicating that most of the PF<sub>6</sub><sup>–</sup> anions are stationary, which suppresses PF<sub>6</sub><sup>–</sup> decomposition and substantially enlarges
the voltage that can be applied to GPE-PAVM:TiO<sub>2</sub> (to 6.5
V vs Li/Li<sup>+</sup>). Immobilization of PF<sub>6</sub><sup>–</sup> anions also leads to the formation of stable solid-electrolyte interface
(SEI) layers in a full-cell graphite|electrolyte|LiFePO<sub>4</sub> battery, which exhibits low SEI and overall resistances. The graphite|electrolyte|LiFePO<sub>4</sub> battery delivers high capacity of 84 mAh g<sup>–1</sup> even at 20 C and presents 90% and 71% capacity retention after 100
and 1000 charge–discharge cycles, respectively. This study
demonstrates a GPE architecture comprising 3D space charge pathways
for Li<sup>+</sup> ions and suppresses anion decomposition to improve
the stability and lifespan of the resulting LIBs
Elucidating Quantum Confinement in Graphene Oxide Dots Based On Excitation-Wavelength-Independent Photoluminescence
Investigating quantum confinement
in graphene under ambient conditions
remains a challenge. In this study, we present graphene oxide quantum
dots (GOQDs) that show excitation-wavelength-independent photoluminescence.
The luminescence color varies from orange-red to blue as the GOQD
size is reduced from 8 to 1 nm. The photoluminescence of each GOQD
specimen is associated with electron transitions from the antibonding
Ï€ (Ï€*) to oxygen nonbonding (n-state) orbitals. The observed
quantum confinement is ascribed to a size change in the sp<sup>2</sup> domains, which leads to a change in the π*−π
gap; the n-state levels remain unaffected by the size change. The
electronic properties and mechanisms involved in quantum-confined
photoluminescence can serve as the foundation for the application
of oxygenated graphene in electronics, photonics, and biology