The photoelectrochemistry of the aqueous iodide/iodine redox system at n-type MoSe2-electrodes

The aqueous iodide/iodine redox system has proved, at present, to be the most favorable electrolyte in designing efficient and stable electrochemical solar cells based on layered semiconducting materials. A systematic study of the kinetic and energetic situation of this redox electrolyte in contact with n-type MoSe₂-electrodes has been performed. It was found that photogenerated holes are consumed by two competing reaction channels, oxidation of the donor iodide and surface recombination. The latter process is very fast and can only be surpassed by a large iodide concentration. Small amounts of elementary iodine, however, specifically interact with surface states and deactivate their efficiency as recombinative centers.

High amounts of iodine, can on the other hand, interact readily with other parts of the surface and generate surface states with donor and acceptor character. Charge of either sign can be trapped in these states which causes large changes of the potential drop in the Helmholtz double layer and shifts in the energy position of the band edges, respectively. This leads to the conclusion that the light conversion efficiency of a solar cell based on this system will critically depend on the iodine content of the redox electrolyte which must be optimized for the particular working conditions.     

Phase segregation phenomena in poly(ethylene oxide):LiN(CF3SO2)2 electrolyte studied by local Raman spectroscopy

Polymer electrolyte composed of poly(ethylene oxide) PEO with dissolved lithium bis (trifluoromethanesulfonyl)imide salt LiTFSI of molar ratio EO:Li 16:1 was prepared by casting from solution. The electrolyte has been investigated by microscope observation simultaneous with impedance spectroscopy, differential scanning calorimetry and local Raman spectroscopy. The presented results provide direct support for model of phase segregation which takes place in PEO:LiTFSI electrolytes. According to the model proposed in our earlier publications, crystallization of PEO or PEO:salt complexes causes rejection or drainage of salt from specific regions of electrolyte. Thus, a resulting semicrystalline electrolyte is divided into large domains of different composition. In the case of investigated PEO:LiTFSI 16:1 electrolyte, the results obtained by local Raman spectroscopy indicated, that in areas situated within large circular spherulites the concentration of salt is lower than in molten (amorphous) electrolyte. In areas situated outside of these spherulites, the concentration of salt was considerably higher than for amorphous electrolyte. This is in good agreement with the assumption that the circular spherulites have the crystalline skeleton of pure PEO, whereas the PEO₆:LiTFSI crystalline phase dominates in the areas between their borders.     

A novel LiTi2(PO4)3/MnO2 hybrid supercapacitor in lithium sulfate aqueous electrolyte

In this work, carbon-coated lithium-ion intercalated compound LiTi₂(PO₄)₃ and MnO₂ have been synthesized and they deliver a capacity of 90 and 60 mAh/g in 1 M Li₂SO₄ neutral aqueous electrolyte within safe potentials without O₂ and H₂ evolution, respectively. The novel hybrid supercapacitor in which MnO₂ was used as a positive electrode and carbon-coated LiTi₂(PO₄)₃ as a negative electrode was assembled and the LiTi₂(PO₄)₃/MnO₂ hybrid supercapacitor showed a sloping voltage profile from 0.7 to 1.9 V, at an average voltage near 1.3 V, and delivers a capacity of 36 mAh/g and an energy density of 47 Wh/kg based on the total weight of the active electrode materials. It exhibits a desirable profile and maintains over 80% of its initial energy density after 1000 cycles. The hybrid supercapacitor also exhibit an excellent rate capability, even at a power density of 1000 W/kg, it has a specific energy 25 Wh/kg compared with 43 Wh/kg at the power density about 200 W/kg.     

Ionic conductivity of PEO9: Cu(CF3SO3)2: Al2O3 nano-composite solid polymer electrolyte

Cu⁺⁺ ion containing solid polymer electrolytes exhibit interesting electrochemical properties. In particular, the polymer electrolyte PEO₉:Cu(CF₃SO₃)₂ made by complexing copper triflate (CuTf₂) with PEO appears to show scientifically intriguing transport properties. Although some copper ion transport in these systems has been seen from plating stripping processes, the detailed mechanism of ionic transport and the species involved are yet to be established. In order to obtain enhanced ionic conductivities and also to contribute towards understanding the ionic transport process in Cu⁺⁺ ion containing, PEO based composite polymer electrolytes, we have studied the system PEO₉: CuTf₂: Al₂O₃ incorporating 10 wt.% of alumina filler particles of grain size 10 μm, 37 nm, 10–20 nm and also particles of pore size 5.8 nm. Thermal and electrical measurements show that the system remains amorphous down to room temperature. The composite electrolyte is predominantly an ionic conductor with electronic conductivity less than 2%. The triflate (CF₃SO₃⁻) anions appear to be the dominant carriers. The presence of alumina grains has enhanced the conductivity significantly from room temperature up to 100 °C. The nano-porous grains with 5.8 nm pore size and 150 m²/g specific surface area exhibited the maximum conductivity enhancement. This enhancement has been attributed to Lewis acid–base type surface interactions of ionic species with O²⁻ and OH⁻ groups on the filler grain surface.     

Mediated electron transfer demonstrated with [Ru(BIPY)2Cl poly(4-vinylpyridine)]Cl coated MoSe2 and WSe2 photoanode

It is shown that at illuminated n-MoSe₂ and n-WSe₂ electrodes the charge transfer of a hole from the crystal valence band to certain redox ions in solution is catalyzed by a [Ru(bipy)₂Cl poly(r-vinyl- pyridine)]Cl covering layer attached at the crystal surface. The coating behaves like a solid redox system taking over the holes from the crystal valence band and passing them to the electrolyte. The oxidized polymer can inject holes into the valence band of the crystal. Possible applications of this and similar surface coatings for photoelectrochemical solar cells are discussed.     

Water-induced bulk Ba(NO3)2 formation from NO2 exposed thermally aged BaO/Al2O3

Phase changes in high temperature treated (>900 °C) 8 or 20 wt% BaO supported on γ-Al₂O₃ model lean NO_x trap (LNT) catalysts, induced by NO₂ and/or H₂O adsorption, were investigated with powder X-ray diffraction (XRD), solid state ²⁷Al magic angle spinning nuclear magnetic resonance (MAS NMR) spectroscopy, and NO₂ temperature programmed desorption (TPD) experiments. After calcination in dry air at 1000 °C, the XRD and solid state ²⁷Al MAS NMR results confirm that stable surface BaO and bulk BaAl₂O₄ phases are formed for 8 and 20 wt% BaO/Al₂O₃, respectively. Following NO₂ adsorption over these thermally treated samples, some evidence for nanosized Ba(NO₃)₂ particles are observed in the XRD results, although this may represent a minority phase. However, when water was added to the thermally aged samples after NO₂ exposure, the formation of bulk crystalline Ba(NO₃)₂ particles was observed in both samples. Solid state ²⁷Al MAS NMR is shown to be a good technique for identifying the various Al species present in the materials during the processes studied here. NO₂ TPD results demonstrate a significant loss of uptake for the 20 wt% model catalysts upon thermal treatment. However, the described phase transformations upon subsequent water treatment gave rise to the partial recovery of NO_x uptake, demonstrating that such a water treatment of thermally aged catalysts can provide a potential method to regenerate LNT materials.     

VO2(A) nanorods: One-pot synthesis,formation mechanism and thermal transformation to VO2(M)

The monoclinic VO₂(M) has promising applications in intelligent devices but its preparation still requires improvement to permit cost-effective mass production. In this work, we report a 2-stage approach for producing VO₂(M) nanorods by (1) hydrothermal reduction of vanadium pentoxide by sodium bisulfate at 220?°C to form VO₂(A), and (2) subsequent thermal activated phase transformation of VO₂(A) to VO₂(M) at 350–450?°C in vacuum. The obtained VO₂(M) nanorods showed a reversible phase transition temperature at about 62.5?°C and a narrow thermal hysteresis width of 10?°C. The mechanism of the hydrothermal reduction was studied by combined ex situ microscopic and diffraction characterization of cooled samples as well as in situ PXRD experiments, in which the hydrothermal synthesis was monitored in real time by time-resolved diffraction datasets. It was found that the hydrothermal synthesis of VO₂(A) is a 4-step process: (1) reduction of V₂O₅ to form VO₂(B) nanoparticles, (2) oriented attachment of VO₂(B) nanoparticles along the [110] direction, (3) formation of VO₂(B) nanorods as a results of oriented attachments, and (4) hydrothermal transformation of the metastable intermediate VO₂(B) nanorods to VO₂(A) nanorods. This clear understanding of the mechanism will help the further optimization of synthesis temperature and time for preparing VO₂(A). This method provides a low temperature thermal treatment alternative and hence helps the reduction of cost for the production of VO₂(M), bring the mass application of VO₂(M) one step closer.     

Differences in reactivity of pulverised coal in air (O2/N2) and oxy-fuel (O2/CO2) conditions

The reactivity of four pulverised Australian coals were measured under simulated air (O₂/N₂) and oxy-fuel (O₂/CO₂) environments using a drop tube furnace (DTF) maintained at 1673 K and a thermogravimetric analyser (TGA) run under non-isothermal (heating) conditions at temperatures up to 1473 K. The oxygen concentration, covering a wide and practical range, was varied in mixtures of O₂/N₂ and O₂/CO₂ in the range of 3 to 21 vol.% and 5 to 30 vol.%, respectively. The apparent volatile yield measured in CO₂ in the DTF was greater than in N₂ for all the coals studied. Pyrolysis experiments in the TGA also revealed an additional mass loss in a CO₂ atmosphere, not observed in a N₂ atmosphere, at relatively high temperatures. The coal burnout measured in the DTF at several O₂ concentrations revealed significantly higher burnouts for two coals and similar burnouts for the other two coals in oxy-fuel conditions. TGA experiments with char also revealed higher reactivity at high temperatures and low O₂ concentration. The results are consistent with a char–CO₂ reaction during the volatile yield experiments, but additional experiments are necessary to resolve the mechanisms determining the differences in coal burnout.     

Photoinduced activation of CO2 on TiO2 surfaces: Quantum chemical modeling of CO2 adsorption on oxygen vacancies

Chemical processes that utilize CO₂ emissions from coal-fired power plants will be required as the world progresses towards reducing CO₂ emissions. The conversion of CO₂ using light energy (CO₂ photoreduction) has the potential to produce useful fuels or valuable chemicals while decreasing CO₂ emissions from the use of fossil fuels such as coal. Computational studies on the initial steps of photoinduced CO₂ activation on TiO₂ surfaces, necessary to develop a mechanistic understanding of CO₂ photoreduction are a focus of this article.The results from previous quantum mechanical modeling studies conducted by the authors indicated that stoichiometric TiO₂ surfaces likely do not promote electron transfer to CO₂. Therefore, the role of oxygen vacancies in promoting the light-induced conversion of CO₂ (CO₂ photoreduction) on TiO₂ surfaces was examined in this study. Two different side-on bonded bent-CO₂ (bridging Ti-CO₂^δ•−-Ti species) were formed on the reduced rutile (110) and anatase (010), (001) surfaces, indicating charge transfer from the reduced surface to CO₂. Further steps in the photoexcitation of these bent-CO₂ species were investigated with density functional theory calculations. Consistent with CO₂ adsorption and photodesorption on other n-type metal oxides such as ZrO₂, the results suggest that the bent-CO₂ species do not gain further charge from the TiO₂ surface under illumination and are likely photodesorbed as neutral species. Additionally, although the formation of species such as CO and HCHO is thermodynamically possible, the energy needed to regenerate the oxygen vacancy on TiO₂ surfaces (~ 7 eV) is greater than that available through band-gap illumination (3.2 eV). Therefore, CO₂ reactions with water on irradiated anatase TiO₂ surfaces are likely to be stoichiometric.     

A polyblend electrolyte (PVP/PEG+KI+I2) for dye-sensitized nanocrystalline TiO2 solar cells

A novel polyblend electrolyte consisting of KI and I₂ dissolved in a blending polymer of polyvinyl pyrrolidone (PVP) and polyethylene glycol (PEG) was prepared. The formation of ⁻I₃ in the polymer electrolyte was confirmed by X-ray photoelectron spectroscopy (XPS) characterization. Due to the coordinating and plasticizing effect by PVP, the ionic conductivity of the polyblend electrolyte is enhanced. The highest ionic conductivity of 1.85 mS cm⁻¹ for the polyblend electrolyte was achieved by optimizing the compositions as 40 wt.% PVP + 60 wt.% PEG + 0.05 mmol g⁻¹ I₂ + 0.10 mmol g⁻¹ KI. Based on the polyblend electrolyte, a DSSC with fill factor of 0.59, short-circuit density of 9.77 mA cm⁻², open-circuit voltage of 698 mV and light-to-electricity conversion efficiency of 4.01% was obtained under AM 1.5 irradiation (100 mW cm⁻²).     

纳米粉体（CeO2）0.9—x（GdO1.5）x（Sm2O3）0.1的溶胶—凝胶低温燃烧合成

采用溶胶-凝胶法与低温燃烧法相结合,合成了(CeO2)0.9-x(GdO1.5)x(Sm2O3)0.1系列粉体.结果表明由硝酸盐与柠檬酸混合形成的凝胶,可在较低温度(200～300℃)点火并燃烧,其火焰温度达900℃以上.经TEM,XRD测试,燃烧后即直接形成了粒径为20～30nm,具有萤石结构的单相粉体,由该粉体制备的固体电解质在中温下电导率为5.8×10S/cm,组装的单个H2-O2燃料电池最大功率密度达70mW/cm.     

Gibbs free energy of formation of Bi2O3 from EMF cells with δ-Bi2O3 solid electrolyte

Determination of thermodynamic data on the formation of Bi₂O₃ was established by emf measurements as a function of temperature in the range 660–820°C on the system Metal, Bi(1)|Bi₂O₃|Pt, O₂. From the results using a tungsten electrode the following relation was found: ΔG⁰ = ?(134.7 ± 1.2) + (64.0 ± 1.2) × 10^?3 T kcal mole^?1 (validity range: 940–1080 K). Standard thermodynamic data at 298 K were calculated as ΔG⁰ = ?119.2 ± 2.1 kcal mole^?, ΔH⁰ = ?139.0 ± 1.2 kcal mole^?1, and ΔS⁰ = ?66.3 ± 1.2 eu.     

Electrochemical properties of TiP2O7 and LiTi2(PO4)3 as anode material for lithium ion battery with aqueous solution electrolyte

Some polyanionic compounds, e.g. TiP₂O₇ and LiTi₂(PO₄)₃ with 3D framework structure were proposed to be used as anodes of lithium ion battery with aqueous electrolyte. The cyclic voltammetry properties TiP₂O₇ and LiTi₂(PO₄)₃ suggested that Li-ion de/intercalation reaction can occur without serious hydrogen evolution in 5 M LiNO₃ aqueous solution. The TiP₂O₇ and LiTi₂(PO₄)₃ give capacities of about 80 mAh/g between potentials of −0.50 V and 0 V (versus SHE) and 90 mAh/g between −0.65 V and −0.10 V (versus SHE), respectively. A test cell consisting of TiP₂O₇/5 M LiNO₃/LiMn₂O₄ delivers approximately 42 mAh/g (weight of cathode and anode) at average voltage of 1.40 V, and LiTi₂(PO₄)₃/5 M LiNO₃/LiMn₂O₄ delivers approximately 45 mAh/g at average voltage of 1.50 V. Both as-assembled cells suffered from short cycle life. The capacity fading may be related to deterioration of anode material.     

Mechanistic aspects of N2O and N2 formation in NO reduction by NH3 over Ag/Al2O3: The effect of O2 and H2

A mechanistic scheme of N₂O and N₂ formation in the selective catalytic reduction of NO with NH₃ over a Ag/Al₂O₃ catalyst in the presence and absence of H₂ and O₂ was developed by applying a combination of different techniques: transient experiments with isotopic tracers in the temporal analysis of products reactor, HRTEM, in situ UV/vis and in situ FTIR spectroscopy. Based on the results of transient isotopic analysis and in situ IR experiments, it is suggested that N₂ and N₂O are formed via direct or oxygen-induced decomposition of surface NH₂NO species. These intermediates originate from NO and surface NH₂ fragments. The latter NH₂ species are formed upon stripping of hydrogen from ammonia by adsorbed oxygen species, which are produced over reduced silver species from NO, N₂O and O₂. The latter is the dominant supplier of active oxygen species. Lattice oxygen in oxidized AgO_x particles is less active than adsorbed oxygen species particularly below 623 K. The previously reported significant diminishing of N₂O production in the presence of H₂ is ascribed to hydrogen-induced generation of metallic silver sites, which are responsible for N₂O decomposition.     

Synthesis, structure and photoluminescence of a novel palladium(I) compound: [Pd3(μ3-Cl)2(dppp)3][Pd2(μ2-Cl)3(PPh3)2](PPh3)2

Pd(PPh₃)₂Cl₂ reacts with PdCl₂ and 1,3-bis(diphenylphosphine)propane (dppp) in ethanol–DMF–pyridine mixed solvent to yield a novel palladium(I) compound [Pd₃(μ₃-Cl)₂(dppp)₃][Pd₂(μ₂-Cl)₃(PPh₃)₂](PPh₃)₂. It features an isolated structure based on [Pd₃(μ₃-Cl)₂(dppp)₃]⁺ cations having triangulo-palladium clusters and [Pd₂(μ₂-Cl)₃(PPh₃)₂]⁻ anions in which the coordination environment of palladium is an unusual tetrahedral geometry. Its photoluminescence is measured.     

Facile modified synthesis and intermediate temperature electrical properties of Sn0.95Al0.05P2O7/KSn2(PO4)3 composite electrolyte

In this study, Sn_0.95Al_0.05P₂O₇ and a novel dense Sn_0.95Al_0.05P₂O₇/KSn₂(PO₄)₃ composite electrolytes were synthesized. The structural characterization of X–ray diffraction (XRD) and microstructual properties of scanning electron microscopy (SEM) were carried out. The XRD results indicated that an in-situ reaction between Sn_0.95Al_0.05P₂O₇ and inorganic melt salt take place to form the Sn_0.95Al_0.05P₂O₇/KSn₂(PO₄)₃ composite. The intermediate temperature electrical properties were determined by using impedance spectroscopy, oxygen concentration cell and hydrogen concentration discharge cell. Finally, the H₂/O₂ fuel cell using the Sn_0.95Al_0.05P₂O₇/KSn₂(PO₄)₃ as electrolyte membrane was constructed and the obtained maximum power output densities were 67.7 mW cm^?2 and 142.1 mW cm^?2 at 650 °C and 700 °C, respectively.     

The formation and thermal stability of spurrite,Ca5(SiO4)2CO3

The reversible equilibrium: 2Ca₂SiO₄ + CaO + CO₂ ? Ca₅(SiO₄)₂CO₃ has been studied using F^? and C?^? ions as mineralizers. A pressure-temperature curve is given for the reaction in the range of CO₂ pressures between 0.08 and 1 atmosphere. At these pressures, the decomposition temperatures of spurrite are 790 ± 5°C and 912 ± 5°C respectively. At a given CO₂ pressure the thermal stability of spurrite is greater than that of CaCO₃.     

Polymerization of 1,3-butadiene with VO(P204)2 and VO(P507)2 activated by alkylaluminum

The oxovanadium phosphonates (VO(P₂₀₄)₂ and VO(P₅₀₇)₂) activated by various alkylaluminums (AlR₃, R = Et, i-Bu, n-Oct; HAlR₂, R = Et, i-Bu) were examined in butadiene (Bd) polymerization. Both VO(P₂₀₄)₂ and VO(P₅₀₇)₂ showed higher activity than those of classical vanadium-based catalysts (e.g. VOCl₃, V(acac)₃). Among the examined catalysts, the VO(P₂₀₄)₂/Al(Oct)₃ system (I) revealed the highest catalytic activity, giving the poly(Bd) bearing M_n of 3.76 × 10⁴ g/mol, and M_w/M_n ratio of 2.9, when the [Al]/[V] molar ratio was 4.0 at 40 °C. The polymerization rate for I is of the first order with respect to the concentration of monomer. High thermal stability of I was found, since a fairly good catalytic activity was achieved even at 70 °C (polymer yield > 33%); the M_n value and M_w/M_n ratio were independent of polymerization temperature in the range of 40-70 °C. By IR and DSC, the poly(Bd)s obtained had high 1,2-unit content (>65%) with atactic configuration. The 1,2-unit content of the polymers obtained by I was nearly unchanged, regardless of variation of reaction conditions, i.e. [Al]/[V], ageing time, and reaction temperature, indicating the high stability of stereospecificity of the active sites.     

Synthesis of (C5H5)2Zr(O2C)CH3 and (C5H5)2Zr(O2C)CH2CH3 for olefin polymerization

Summary (C₅H₅)₂Zr(O₂C)CH₃ and (C₅H₅)₂Zr(O₂C)CH₂CH₃ complexes were synthesized, characterized and activated with MAO for ethylene polymerization. The highest catalytic activity was achieved at Al/Zr molar ratio of 3000 for both systems. The effects of the size of the R group in the carboxylate ligands, the Al/Zr molar ratio and reaction temperature on the catalytic activity and polymer properties were studied and discussed.     

Layered monodiphosphate Li9V3(P2O7)3(PO4)2: A novel cathode material for lithium-ion batteries

Single phase Li₉V₃(P₂O₇)₃(PO₄)₂ is synthesized at 750 °C via solid-state reaction method for the first time. The Rietveld refinement results show that the trigonal system (space group: ) with the lattice parameters a = 0.9724 nm, c = 1.3596 nm are obtained. Its intrinsic electrical conductivity of 1.43 × 10⁻⁸ S cm⁻¹ is higher than that of LiFePO₄ and as the same order of Li₃V₂(PO₃)₄. The electrochemical measurement results show that there are two plateaus (3.77 V and 4.51 V) and three plateaus (3.77 V, 4.51 V and 4.75 V) in the potential ranges of 2.0–4.6 V and 2.0–4.8 V, respectively. In the range of 2.0–4.6 V, two discharge plateaus (4.46 V and 3.74 V) can be observed and 110 mAh g⁻¹ of discharge capacity is achieved. The Rietveld refinement result of the X-ray diffraction (XRD) data at the end of discharge after the first cycle suggests that the structural reversibility can be retained during electrochemical reactions in Li₉V₃(P₂O₇)₃(PO₄)_2. In the range of 2.0–4.8 V, almost six lithium ions are extracted and the trigonal structure is still recovered after 30 cycles. Therefore, this novel layered vanadium monodiphosphate offers a promising candidate as cathode material for lithium-ion batteries.