17 research outputs found
Thiolate anchor in organotin(IV) induced amide deprotonation: Equilibrium and NMR spectroscopic studies of dimethyltin(IV) complexes formed N-(2-mercaptopropionyl)glycine and L-alanyl-glycine
Intrinsic Production of Hydrogen Peroxide by 172 nm Photolysis of Water and during the Photomineralization of Ibu- and Ketoprofen by 172 nm and/or by 185/254 nm Light
Formation of an electron hole doped film in the alpha Fe2O3 photoanode upon electrochemical oxidation
Solar hydrogen generation by water splitting in photoelectrochemical cells (PEC) is an appealing technology for a future hydrogen economy. Hematite is a prospective photoanode material in this respect because of its visible light conjugated band gap, its corrosion stability, its environmentally benign nature and its low cost. Its bulk and surface electronic structure has been under scrutiny for many decades and is considered critical for improvement of efficiency. In the present study, hematite films of nominally 500 nm thickness were obtained by dip-coating on fluorine doped tin oxide (FTO) glass slides and then anodised in 1 molar KOH at 500, 600, and 700 mV for 1, 10, 120 and 1440 minutes under dark conditions. X-ray photoelectron spectra recorded at the Fe 3p resonant absorption threshold show that the e(g) transition before the Fermi energy, which is well developed in the pristine hematite film, becomes depleted upon anodisation. The spectral weight of the e(g) peak decreases with the square-root of the anodisation time, pointing to a diffusion controlled process. The speed of this process increases with the anodisation potential, pointing to Arrhenius behaviour. Concomitantly, the weakly developed t(2g) peak intensity becomes enhanced in the same manner. This suggests that the surface of the photoanode contains Fe2+ species which become oxidized toward Fe3+ during anodisation. The kinetic behaviour derived from the experimental data suggests that the anodisation forms an electron hole doped film on and below the hematite surface
Formation of an electron hole doped film in the alpha-Fe2O3 photoanode upon electrochemical oxidation
Electrospun TiO<sub>2</sub> Fiber Composite Photoelectrodes for Water Splitting
This work has focused on the development
of electrospun TiO<sub>2</sub> fiber composite photoelectrodes for
hydrogen production by water splitting. For comparison, similar photoelectrodes
were also developed using commercial TiO<sub>2</sub> (Aeroxide P25)
nanoparticles (NPs). Dispersions of either fibers or P25 NPs were
used to make homogenous TiO<sub>2</sub> films on fluorine-doped SnO<sub>2</sub> (FTO) glass substrates by a doctor blade (DB) technique.
Scanning electron microscopy (SEM) analysis revealed a much lower
packing density of the DB fibers, with respect to DB-P25 TiO<sub>2</sub> NPs; this was also directly reflected by the higher photocurrent
measured for the NPs when irradiating the photoelectrodes at a light
intensity of 1.5AM (1 sun, 1000 W/m<sup>2</sup>). For a better comparison
of fibers vs. NPs, composite photoelectrodes by dip-coating (onto
FTO) TiO<sub>2</sub> sol-gel (SG) matrixes containing an equal amount
(5 or 20 wt %) of either fibers or P25 NPs were also investigated.
It emerged that the photoactivity of the fibers was significantly
higher. For composites containing 5 wt % TiO<sub>2</sub> fibers,
a photocurrent of 0.5 mA/cm<sup>2</sup> (at 0.23 V vs Ag/AgCl) was
measured, whereas 5 wt % P25 NPs only provided 0.2 mA/cm<sup>2</sup>. When increasing to 20 wt % fibers or NPs, the photocurrent
decreased, because of the formation of microcracks in the photoelectrodes,
because of the shrinkage of the sol–gel. The high photoactivity
of the fiber-based electrodes could be confirmed by incident photon
to current efficiency (IPCE) measurements. Remarkably, the IPCE of
composites containing 5 wt % fibers was between 35% and 40%
in the region of 380–320 nm, and when accounting for transmission/reflection
losses, the absorbed photon to current efficiency (APCE) was consistently
over 60% between 380 nm and 320 nm. The superior photoactivity is
attributed to the enhanced electron transport in the electrospun fibers,
with respect to P25 NPs. According to this study, it is clear that
the electronic connectivity ensured by the sol–gel also contributes
positively to the enhanced photocurrent
Preparation and XAFS studies of organotin(IV) complexes with adenosine and related compounds and calf thymus DNA
Critical evaluation of rate coefficients for hydroxyl radical reactions with antibiotics: A review
Between photocatalysis and photosynthesis: Synchrotron spectroscopy methods on molecules and materials for solar hydrogen generation
Energy research is to a large extent materials research, encompassing the physics and chemistry of materials, including their synthesis, processing toward components and design toward architectures, allowing for their functionality as energy devices, extending toward their operation parameters and environment, including also their degradation, limited life, ultimate failure and potential recycling. In all these stages, X-ray and electron spectroscopy are helpful methods for analysis, characterization and diagnostics for the engineer and for the researcher working in basic science. This paper gives a short overview of experiments with X-ray and electron spectroscopy for solar energy and water splitting materials and addresses also the issue of solar fuel, a relatively new topic in energy research. The featured systems are iron oxide and tungsten oxide as photoanodes, and hydrogenases as molecular systems. We present surface and sub-surface studies with ambient pressure XPS and hard X-ray XPS, resonant photoemission, light induced effects in resonant photoemission experiments and a photo-lectrochemical in situ/operando NEXAFS experiment in a liquid cell, and nuclear resonant vibrational spectroscopy (NRVS)