11 research outputs found
A Terahertz-Transparent Electrochemical Cell for In Situ Terahertz Spectroelectrochemistry
Terahertz spectroscopy is broadly
applicable for the study of a
wide variety of materials, but spectroelectrochemistry has not been
performed in the THz range because of the lack of a THz-transparent
electrochemical cell. While THz-transparent electrodes do exist, they
have never been utilized in a complete three-electrode cell, which
is the configuration required for accurate potential control in aqueous
media. We have designed and constructed a THz-transparent three-electrode
electrochemical cell and have performed THz spectroelectrochemistry
of a SnO<sub>2</sub> thin film. The cell utilizes a custom-made reference
electrode and tubing which allows the composition of electrolyte to
be changed during an experiment. THz spectroelectrochemical measurements
show a decrease in THz transmission at potentials where SnO<sub>2</sub> conduction band states are potentiostatically filled. We also describe
a simple method for measuring the uncompensated resistance and RC
time constant
Dynamics of Electron Recombination and Transport in Water-Splitting Dye-Sensitized Photoanodes
Water-splitting dye-sensitized photoelectrochemical
cells (WS-DSPECs)
use visible light to split water using molecular sensitizers and water
oxidation catalysts codeposited onto mesoporous TiO<sub>2</sub> electrodes.
Despite a high quantum yield of charge injection and low requirement
for the catalytic turnover rate, the quantum yield of water splitting
in WS-DSPECs is typically low (<1%). Here we examine the charge
separation and recombination processes in WS-DSPECs photoanodes functionalized
with varying amounts of IrO<sub>2</sub> nanoparticle catalyst. Charge
extraction and transient open-circuit voltage decay measurements provide
insight into the relationship between light intensity, conduction
band electron density, open-circuit photovoltage, and recombination
time scale. We correlate these results with electrochemical impedance
spectroscopy and present the first complete equivalent circuit model
for a WS-DSPEC. The data show quantitatively that recombination of
photoinjected electrons with oxidized sensitizer molecules and scavenging
by the water oxidation catalyst limit the concentration of conduction
band electrons and by extension the photocurrent of WS-DSPECs
Frequency-Dependent Terahertz Transient Photoconductivity of Mesoporous SnO<sub>2</sub> Films
The
transient photoconductive properties of tinĀ(IV) oxide (SnO<sub>2</sub>) mesoporous films have been studied by time-resolved terahertz
(THz) spectroscopy. We gain insight into carrier dynamics by measuring
overall injection and trapping lifetimes using optical pumpāTHz
probe spectroscopy, as well as the frequency-dependent complex conductivity
at various pumpāprobe delay times. It is found that the method
of charge generation, either direct above band gap excitation (at
267 nm) or dye-sensitized electron injection (at 400 nm), has a dramatic
effect on the overall injection and trapping dynamics of mobile charge
carriers on the picosecond to nanosecond time scale. In the presence
of aqueous electrolyte, direct band gap excitation of nonsensitized
SnO<sub>2</sub> films results in instrument response limited subpicosecond
injection lifetimes, while dye-sensitized films require tens of picoseconds
for interfacial electron transfer to complete. On the other hand,
the rate for trapping of mobile charges is at least 2 orders of magnitude
faster in the nonsensitized films compared to the dye-sensitized films,
which is likely due to photoinduced charges being more highly concentrated
in the nonsensitized films. Finally, we find that the transient photoconductivity
deviates from the behavior described by standard conductivity models
such as the Drude and DrudeāSmith models. This is due to the
contribution from a photoinduced change in the permittivity of the
SnO<sub>2</sub> films
Rutile TiO<sub>2</sub> as an Anode Material for Water-Splitting Dye-Sensitized Photoelectrochemical Cells
Water-splitting
dye-sensitized photoelectrochemical cells (WS-DSPECs)
use a wide bandgap metal oxide semiconductor functionalized with a
light-absorbing dye and water-oxidation catalyst to harvest light
and drive water oxidation, respectively. We demonstrate here that
the rutile polymorph of TiO<sub>2</sub> (r-TiO<sub>2</sub>) is a promising
anode material for WS-DSPECs. Recombination between the injected electron
and oxidized sensitizer with r-TiO<sub>2</sub> is an order of magnitude
slower than with anatase TiO<sub>2</sub> (a-TiO<sub>2</sub>), with
injection yields approaching 100%. Studies with a reductive quencher
demonstrate that r-TiO<sub>2</sub> is significantly more efficient
than a-TiO<sub>2</sub>, while exhibiting greater dye stability. Furthermore,
comparison of direct band gap excitation photocurrent generation for
bare and sensitized r-TiO<sub>2</sub> suggests that the sensitizer
functions as a light harvester and redox mediator
Dynamics of Electron Injection in SnO<sub>2</sub>/TiO<sub>2</sub> Core/Shell Electrodes for Water-Splitting Dye-Sensitized Photoelectrochemical Cells
Water-splitting
dye-sensitized photoelectrochemical cells (WS-DSPECs)
rely on photoinduced charge separation at a dye/semiconductor interface
to supply electrons and holes for water splitting. To improve the
efficiency of charge separation and reduce charge recombination in
these devices, it is possible to use core/shell structures in which
photoinduced electron transfer occurs stepwise through a series of
progressively more positive acceptor states. Here, we use steady-state
emission studies and time-resolved terahertz spectroscopy to follow
the dynamics of electron injection from a photoexcited ruthenium polypyridyl
dye as a function of the TiO<sub>2</sub> shell thickness on SnO<sub>2</sub> nanoparticles. Electron injection proceeds directly into
the SnO<sub>2</sub> core when the thickness of the TiO<sub>2</sub> shell is less than 5 Ć
. For thicker shells, electrons are injected
into the TiO<sub>2</sub> shell and trapped, and are then released
into the SnO<sub>2</sub> core on a time scale of hundreds of picoseconds.
As the TiO<sub>2</sub> shell increases in thickness, the probability
of electron trapping in nonmobile states within the shell increases.
Conduction band electrons in the TiO<sub>2</sub> shell and the SnO<sub>2</sub> core can be differentiated on the basis of their mobility.
These observations help explain the observation of an optimum shell
thickness for core/shell water-splitting electrodes
Ultrafast Electron Injection Dynamics of Photoanodes for Water-Splitting Dye-Sensitized Photoelectrochemical Cells
Efficient conversion
of solar energy into useful chemical fuels is a major scientific challenge.
Water-splitting dye-sensitized photoelectrochemical cells (WS-DSPECs)
utilize mesoporous oxide supports sensitized with molecular dyes and
catalysts to drive the water-splitting reaction. Despite a growing
body of work, the overall efficiencies of WS-DSPECs remain low, in
large part because of poor electron injection into the conduction
band of the oxide support. In this study, we characterize the ultrafast
injection dynamics of several proposed oxide supports (TiO<sub>2</sub>, TiO<sub>2</sub>/Al<sub>2</sub>O<sub>3</sub>, SnO<sub>2</sub>, SnO<sub>2</sub>/TiO<sub>2</sub>) under identical conditions using time-resolved
terahertz spectroscopy. In the absence of an Al<sub>2</sub>O<sub>3</sub> overlayer, we observe a two-step injection from the dye singlet
state into nonmobile surface traps, which then relax into the oxide
conduction band. We also find that, in SnO<sub>2</sub>-core/TiO<sub>2</sub>-shell configurations, electron injection into TiO<sub>2</sub> trap states occurs rapidly, followed by trapped electrons being
released into SnO<sub>2</sub> on the hundreds of picoseconds time
scale
Effects of Electron Trapping and Protonation on the Efficiency of Water-Splitting Dye-Sensitized Solar Cells
Water-splitting
dye-sensitized photoelectrochemical (WS-DSPECs)
cells employ molecular sensitizers to absorb light and transport holes
across the TiO<sub>2</sub> surface to colloidal or molecular water
oxidation catalysts. As hole diffusion occurs along the surface, electrons
are transported through the mesoporous TiO<sub>2</sub> film. In this
paper we report the effects of electron trapping and protonation in
the TiO<sub>2</sub> film on the dynamics of electron and hole transport
in WS-DSPECs. When the sensitizer bisĀ(2,2ā²-bipyridine)Ā(4,4ā²-diphosphonato-2,2ā²-bipyridine)ĀrutheniumĀ(II)
is adsorbed from aqueous acid instead of from ethanol, there is more
rapid hole transfer between photo-oxidized sensitizer molecules that
are adsorbed from strong acid. However, the photocurrent and open-circuit
photovoltage are dramatically lower with sensitizers adsorbed from
acid because intercalated protons charge-compensate electron traps
in the TiO<sub>2</sub> film. Kinetic modeling of the photocurrent
shows that electron trapping is responsible for the rapid electrode
polarization that is observed in all WS-DSPECs. Electrochemical impedance
spectroscopy suggests that proton intercalation also plays an important
role in the slow degradation of WS-DSPECs, which generate protons
at the anode as water is oxidized to oxygen
Proton-Induced Trap States, Injection and Recombination Dynamics in Water-Splitting Dye-Sensitized Photoelectrochemical Cells
Water-splitting dye-sensitized photoelectrochemical
cells (WS-DSPECs) utilize a sensitized metal oxide and a water oxidation
catalyst in order to generate hydrogen and oxygen from water. Although
the Faradaic efficiency of water splitting is close to unity, the
recombination of photogenerated electrons with oxidized dye molecules
causes the quantum efficiency of these devices to be low. It is therefore
important to understand recombination mechanisms in order to develop
strategies to minimize them. In this paper, we discuss the role of
proton intercalation in the formation of recombination centers. Proton
intercalation forms nonmobile surface trap states that persist on
time scales that are orders of magnitude longer than the electron
lifetime in TiO<sub>2</sub>. As a result of electron trapping, recombination
with surface-bound oxidized dye molecules occurs. We report a method
for effectively removing the surface trap states by mildly heating
the electrodes under vacuum, which appears to primarily improve the
injection kinetics without affecting bulk trapping dynamics, further
stressing the importance of proton control in WS-DSPECs
Photovoltage Effects of Sintered IrO<sub>2</sub> Nanoparticle Catalysts in Water-Splitting Dye-Sensitized Photoelectrochemical Cells
Water-splitting dye-sensitized photoelectrochemical cells (WS-DSPECs)
utilize high surface area TiO<sub>2</sub> electrodes functionalized
with light absorbing sensitizers and water oxidation catalysts. Because
water splitting requires vectorial electron transfer from the catalyst
to the sensitizer to the TiO<sub>2</sub> surface, attaching both sensitizer
and catalyst to TiO<sub>2</sub> in the correct sequence and stabilizing
them under photoelectrochemical conditions has been a challenging
problem. Rutile-phase IrO<sub>2</sub> nanoparticles can be deposited
directly on the TiO<sub>2</sub> electrode by adsorbing citrate-capped
amorphous IrO<sub><i>x</i></sub> and then sintering at 450
Ā°C. Electrodes functionalized with these nanocrystalline particles
show higher activity than those made from ligand-capped amorphous
IrO<sub><i>x</i></sub> without sintering. In the WS-DSPEC,
the Coulombic efficiency for oxygen evolution from the sintered nanoparticle
photoelectrodes was near unity. The loading of colloidal IrO<sub><i>x</i></sub> and IrO<sub>2</sub> particles onto the porous TiO<sub>2</sub> electrodes was quantified by neutron activation analysis.
Photovoltage measurements suggest that at high catalyst loading the
dominant charge recombination pathway is from photoinjected electrons
to IrO<sub>2</sub>
High-Potential Porphyrins Supported on SnO<sub>2</sub> and TiO<sub>2</sub> Surfaces for Photoelectrochemical Applications
We
report CF<sub>3</sub>-substituted porphyrins and evaluate their
use as photosensitizers in water-splitting dye-sensitized photoelectrochemical
cells (WS-DSPECs) by characterizing interfacial electron transfer
on metal oxide surfaces. By using (CF<sub>3</sub>)<sub>2</sub>C<sub>6</sub>H<sub>3</sub> instead of C<sub>6</sub>F<sub>5</sub> substituents
at the meso positions, we obtain the desired high potentials while
avoiding the sensitivity of C<sub>6</sub>F<sub>5</sub> substituents
to nucleophilic substitution, a process that limits the types of synthetic
reactions that can be used. Both the number of CF<sub>3</sub> groups
and the central metal tune the ground and excited-state potentials.
A pair of porphyrins bearing carboxylic acids as anchoring groups
were deposited on SnO<sub>2</sub> and TiO<sub>2</sub> surfaces, and
the interfacial charge-injection and charge-recombination kinetics
were characterized by using a combination of computational modeling,
terahertz measurements, and transient absorption spectroscopy. We
find that both free-base and metalated porphyrins inject into SnO<sub>2</sub> and that recombination is slower for the latter case. These
findings demonstrate that (CF<sub>3</sub>)<sub>2</sub>C<sub>6</sub>H<sub>3</sub>-substituted porphyrins are promising photosensitizers
for use in WS-DSPECs