4 research outputs found
Water Oxidation and Oxygen Monitoring by Cobalt-Modified Fluorine-Doped Tin Oxide Electrodes
Electrocatalytic
water oxidation occurs at fluoride-doped tin oxide
(FTO) electrodes that have been surface-modified by addition of CoÂ(II).
On the basis of X-ray photoelectron spectroscopy and transmission
electron microscopy measurements, the active surface site appears
to be a single site or small-molecule assembly bound as CoÂ(II), with
no evidence for cobalt oxide film or cluster formation. On the basis
of cyclic voltammetry measurements, surface-bound CoÂ(II) undergoes
a pH-dependent 1e<sup>–</sup>/1H<sup>+</sup> oxidation to CoÂ(III),
which is followed by pH-dependent catalytic water oxidation. O<sub>2</sub> reduction at FTO occurs at −0.33 V vs NHE, allowing
for in situ detection of oxygen as it is formed by water oxidation
on the surface. Controlled-potential electrolysis at 1.61 V vs NHE
at pH 7.2 resulted in sustained water oxidation catalysis at a current
density of 0.16 mA/cm<sup>2</sup> with 29 000 turnovers per
site over an electrolysis period of 2 h. The turnover frequency for
oxygen production per Co site was 4 s<sup>–1</sup> at an overpotential
of 800 mV at pH 7.2. Initial experiments with CoÂ(II) on a mesoporous,
high-surface-area <i>nano</i>FTO electrode increased the
current density by a factor of ∼5
Photoinduced Interfacial Electron Transfer within a Mesoporous Transparent Conducting Oxide Film
Interfacial
electron transfer to and from conductive Sn-doped In<sub>2</sub>O<sub>3</sub> (ITO) nanoparticles (NPs) in mesoporous thin
films has been investigated by transient absorption measurements using
surface-bound [Ru<sup>II</sup>(bpy)<sub>2</sub>(dcb)]<sup>2+</sup> (bpy is 2,2′-bipyridyl and dcb is 4,4′-(COOH)<sub>2</sub>-2,2′-bipyridyl). Metal-to-ligand charge transfer excitation
in 0.1 M LiClO<sub>4</sub> MeCN results in efficient electron injection
into the ITO NPs on the picosecond time scale followed by back electron
transfer on the nanosecond time scale. Rates of back electron transfer
are dependent on thermal annealing conditions with the rate constant
increasing from 1.8 × 10<sup>8</sup> s<sup>–1</sup> for
oxidizing annealing conditions to 8.0 × 10<sup>8</sup> s<sup>–1</sup> for reducing conditions, presumably due to an enhanced
electron concentration in the latter
Solution-Processed, Antimony-Doped Tin Oxide Colloid Films Enable High-Performance TiO<sub>2</sub> Photoanodes for Water Splitting
Photoelectrochemical
(PEC) water splitting and solar fuels hold
great promise for harvesting solar energy. TiO<sub>2</sub>-based photoelectrodes
for water splitting have been intensively investigated since 1972.
However, solar-to-fuel conversion efficiencies of TiO<sub>2</sub> photoelectrodes
are still far lower than theoretical values. This is partially due
to the dilemma of a short minority carrier diffusion length, and long
optical penetration depth, as well as inefficient electron collection.
We report here the synthesis of TiO<sub>2</sub> PEC electrodes by
coating solution-processed antimony-doped tin oxide nanoparticle films
(nanoATO) on FTO glass with TiO<sub>2</sub> through atomic layer deposition.
The conductive, porous nanoATO film-supported TiO<sub>2</sub> electrodes,
yielded a highest photocurrent density of 0.58 mA/cm<sup>2</sup> under
AM 1.5G simulated sunlight of 100 mW/cm<sup>2</sup>. This is approximately
3× the maximum photocurrent density of planar TiO<sub>2</sub> PEC electrodes on FTO glass. The enhancement is ascribed to the
conductive interconnected porous nanoATO film, which decouples the
dimensions for light absorption and charge carrier diffusion while
maintaining efficient electron collection. Transient photocurrent
measurements showed that nanoATO films reduce charge recombination
by accelerating transport of photoelectrons through the less defined
conductive porous nanoATO network. Owing to the large band gap, scalable
solution processed porous nanoATO films are promising as a framework
to replace other conductive scaffolds for PEC electrodes
A Sensitized Nb<sub>2</sub>O<sub>5</sub> Photoanode for Hydrogen Production in a Dye-Sensitized Photoelectrosynthesis Cell
Orthorhombic Nb<sub>2</sub>O<sub>5</sub> nanocrystalline
films
functionalized with [RuÂ(bpy)<sub>2</sub>(4,4′-(PO<sub>3</sub>H<sub>2</sub>)<sub>2</sub>bpy)]<sup>2+</sup> were used as the photoanode
in dye-sensitized photoelectrosynthesis cells (DSPEC) for hydrogen
generation. A set of experiments to establish key propertiesî—¸conduction
band, trap state distribution, interfacial electron transfer dynamics,
and DSPEC efficiencyî—¸were undertaken to develop a general protocol
for future semiconductor evaluation and for comparison with other
wide-band-gap semiconductors. We have found that, for a T-phase orthorhombic
Nb<sub>2</sub>O<sub>5</sub> nanocrystalline film, the conduction band
potential is slightly positive (<0.1 eV), relative to that for
anatase TiO<sub>2</sub>. Anatase TiO<sub>2</sub> has a wide distribution
of trap states including deep trap and band-tail trap states. Orthorhombic
Nb<sub>2</sub>O<sub>5</sub> is dominated by shallow band-tail trap
states. Trap state distributions, conduction band energies, and interfacial
barriers appear to contribute to a slower back electron transfer rate,
lower injection yield on the nanosecond time scale, and a lower open-circuit
voltage (<i>V</i><sub>oc</sub>) for orthorhombic Nb<sub>2</sub>O<sub>5</sub>, compared to anatase TiO<sub>2</sub>. In an
operating DSPEC, with the ethylenediaminetetraacetic tetra-anion (EDTA<sup>4–</sup>) added as a reductive scavenger, H<sub>2</sub> quantum
yield and photostability measurements show that Nb<sub>2</sub>O<sub>5</sub> is comparable, but not superior, to TiO<sub>2</sub>