11 research outputs found

    A Terahertz-Transparent Electrochemical Cell for In Situ Terahertz Spectroelectrochemistry

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    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

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    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

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    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 pumpā€“THz probe spectroscopy, as well as the frequency-dependent complex conductivity at various pumpā€“probe 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 Drudeā€“Smith 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

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    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

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    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 ƅ. 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

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    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

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    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(2,2ā€²-bipyridine)Ā­(4,4ā€²-diphosphonato-2,2ā€²-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

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    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

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    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

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    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
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