14 research outputs found
Investigation of Factors That Affect Excited-State Lifetime Distribution of Dye-Sensitized Nanoparticle Films
We investigate the
influence of potential determining ions and
applied electric potentials on the excited-state lifetime distribution
of sensitized TiO<sub>2</sub> nanoparticle films by using time-correlated
single photon counting to measure the time-dependent photoluminescence
decay. The data are consistent with quenching by excited-state electron
injection into localized semiconductor acceptor states that are distributed
in energy. We show that the characteristic lifetime and the amount
of dispersion in the lifetime distribution exhibit a strong correlation
that is the same for all of the chemical additives and for the applied
bias conditions. The universal nature of this correlation under conditions
that affect the distribution of available acceptor states differently
may be due to the exponential form of the TiO<sub>2</sub> sub-bandgap
density of states
Power-Law Kinetics in the Photoluminescence of Dye-Sensitized Nanoparticle Films: Implications for Electron Injection and Charge Transport
Dye-sensitized solar cells have provided a model to inexpensively
harness solar energy, but the underlying physics that limit their
efficiency are still not well understood. We probe electron injection
in sensitized nanocrystalline TiO<sub>2</sub> films using time-correlated
single photon counting (TCSPC) to measure time-dependent chromophore
photoluminescence quenching. The time-dependent emission exhibits
kinetics that become faster and more dispersive with increasing ionic
concentrations in both water and acetonitrile; we quantify these trends
by fitting the data using several kinetic models. Even more notably,
we show that the residual emission under conditions that favor efficient
electron injection exhibits a power-law decay in time. We attribute
this highly dispersive kinetic behavior to electron injection from
the dye into localized acceptor states of the TiO<sub>2</sub> nanoparticle
film, which exhibits a distribution of injection rate constants that
depend on the energetic distribution of sub-band-gap trap states
Stabilization of a Ruthenium(II) Polypyridyl Dye on Nanocrystalline TiO<sub>2</sub> by an Electropolymerized Overlayer
The
long-term performance of dye-sensitized solar and photoelectrochemical
cells is strongly dependent on the stability of surface-bound chromophores
and chromophore–catalyst assemblies at metal oxide interfaces.
We report here electropolymerization as a strategy for increasing
interfacial stability and as a simple synthetic route for preparing
spatially controlled, multicomponent films at an interface. We demonstrate
that [Fe(v-tpy)<sub>2</sub>]<sup>2+</sup> (v-tpy = 4′-vinyl-2,2′:6′,2″-terpyridine)
can be reductively electropolymerized on nanocrystalline TiO<sub>2</sub> functionalized with a phosphonate-derivatized Ru(II) polypyridyl
chromophore. The outer:inner Fe:Ru ratio can be controlled by the
number of reductive electrochemical scan cycles as shown by UV–visible
absorption and energy dispersive X-ray spectroscopy measurements.
Overlayer electropolymerization results in up to 30-fold enhancements
in photostability compared to the surface-bound dye alone. Transient
absorbance measurements have been used to demonstrate that photoexcitation
and electron injection by the MLCT excited state(s) of the surface-bound
Ru<sup>II</sup> complex is followed by directional, outside-to-inside,
Fe<sup>II</sup> → Ru<sup>III</sup> electron transfer. This
strategy is appealing in opening a new approach for synthesizing surface-stabilized
chromophore–catalyst assemblies on nanocrystalline metal oxide
films
Light-Driven Water Splitting with a Molecular Electroassembly-Based Core/Shell Photoanode
An electrochemical procedure for
preparing chromophore-catalyst
assemblies on oxide electrode surfaces by reductive vinyl coupling
is described. On core/shell SnO<sub>2</sub>/TiO<sub>2</sub> nanoparticle
oxide films, excitation of the assembly with 1 sun (100 mW cm<sup>–2</sup>) illumination in 0.1 M H<sub>2</sub>PO<sub>4</sub><sup>–</sup>/HPO<sub>4</sub><sup>2–</sup> at pH 7 with
an applied bias of 0.4 V versus SCE leads to water splitting in a
DSPEC with a Pt cathode. Over a 5 min photolysis period, the core/shell
photoanode produced O<sub>2</sub> with a faradaic efficiency of 22%.
Instability of the surface bound chromophore in its oxidized state
in the phosphate buffer leads to a gradual decrease in photocurrent
and to the relatively modest faradaic efficiencies
Synthesis, Electrochemistry, and Excited-State Properties of Three Ru(II) Quaterpyridine Complexes
The complexes [Ru(qpy)LL′]<sup>2+</sup> (qpy = 2,2′:6′,2″:6″,2‴-quaterpyridine),
with <b>1</b>: L = acetonitrile, L′= chloride; <b>2</b>: L = L′= acetonitrile; and <b>3</b>: L = L′=
vinylpyridine, have been prepared from [Ru(qpy) (Cl)<sub>2</sub>].
Their absorption spectra in CH<sub>3</sub>CN exhibit broad metal-to-ligand
charge transfer (MLCT) absorptions arising from overlapping <sup>1</sup>A<sub>1</sub> → <sup>1</sup>MLCT transitions. Photoluminescence
is not observed at room temperature, but all three are weakly emissive
in 4:1 ethanol/methanol glasses at 77 K with broad, featureless emissions
observed between 600 and 1000 nm consistent with MLCT phosphorescence.
Cyclic voltammograms in CH<sub>3</sub>CN reveal the expected Ru<sup>III/II</sup> redox couples. In 0.1 M trifluoroacetic acid (TFA), <b>1</b> and <b>2</b> undergo aquation to give [Ru<sup>II</sup>(qpy)(OH<sub>2</sub>)<sub>2</sub>]<sup>2+</sup>, as evidenced by
the appearance of waves for the couples [Ru<sup>III</sup>(qpy)(OH<sub>2</sub>)<sub>2</sub>]<sup>3+</sup>/[Ru<sup>II</sup>(qpy)(OH<sub>2</sub>)<sub>2</sub>]<sup>2+</sup>, [Ru<sup>IV</sup>(qpy)(O)(OH<sub>2</sub>)]<sup>2+</sup>/[Ru<sup>III</sup>(qpy)(OH<sub>2</sub>)<sub>2</sub>]<sup>3+</sup>, and [Ru<sup>VI</sup>(qpy)(O)<sub>2</sub>]<sup>2+</sup>/[Ru<sup>IV</sup>(qpy)(O)(OH<sub>2</sub>)]<sup>2+</sup> in cyclic
voltammograms
A Dye-Sensitized Photoelectrochemical Tandem Cell for Light Driven Hydrogen Production from Water
Tandem junction photoelectrochemical
water-splitting devices, whereby
two light absorbing electrodes targeting separate portions of the
solar spectrum generate the voltage required to convert water to oxygen
and hydrogen, enable much higher possible efficiencies than single
absorber systems. We report here on the development of a tandem system
consisting of a dye-sensitized photoelectrochemical cell (DSPEC) wired
in series with a dye-sensitized solar cell (DSC). The DSPEC photoanode
incorporates a tris(bipyridine)ruthenium(II)-type chromophore
and molecular ruthenium based water oxidation catalyst. The DSPEC
was tested with two more-red absorbing DSC variations, one utilizing
N719 dye with an I<sub>3</sub><sup>–</sup>/I<sup>–</sup> redox mediator solution and the other D35 dye with a tris(bipyridine)cobalt
([Co(bpy)<sub>3</sub>]<sup>3+/2+</sup>) based mediator. The tandem
configuration consisting of the DSPEC and D35/[Co(bpy)<sub>3</sub>]<sup>3+/2+</sup> based DSC gave the best overall performance and
demonstrated the production of H<sub>2</sub> from H<sub>2</sub>O with
the only energy input from simulated solar illumination
Synthesis of Phosphonic Acid Derivatized Bipyridine Ligands and Their Ruthenium Complexes
Water-stable,
surface-bound chromophores, catalysts, and assemblies are an essential
element in dye-sensitized photoelectrosynthesis cells for the generation
of solar fuels by water splitting and CO<sub>2</sub> reduction to
CO, other oxygenates, or hydrocarbons. Phosphonic acid derivatives
provide a basis for stable chemical binding on metal oxide surfaces.
We report here the efficient synthesis of 4,4′-bis(diethylphosphonomethyl)-2,2′-bipyridine
and 4,4′-bis(diethylphosphonate)-2,2′-bipyridine, as
well as the mono-, bis-, and tris-substituted ruthenium complexes,
[Ru(bpy)<sub>2</sub>(Pbpy)]<sup>2+</sup>, [Ru(bpy)(Pbpy)<sub>2</sub>]<sup>2+</sup>, [Ru(Pbpy)<sub>3</sub>]<sup>2+</sup>, [Ru(bpy)<sub>2</sub>(CPbpy)]<sup>2+</sup>, [Ru(bpy)(CPbpy)<sub>2</sub>]<sup>2+</sup>, and [Ru(CPbpy)<sub>3</sub>]<sup>2+</sup> [bpy = 2,2′-bipyridine;
Pbpy = 4,4′-bis(phosphonic acid)-2,2′-bipyridine; CPbpy
= 4,4′-bis(methylphosphonic acid)-2,2′-bipyridine]
Redox Mediator Effect on Water Oxidation in a Ruthenium-Based Chromophore–Catalyst Assembly
The synthesis, characterization, and redox properties
are described
for a new ruthenium-based chromophore–catalyst assembly, [(bpy)<sub>2</sub>Ru(4-Mebpy-4′-bimpy)Ru(tpy)(OH<sub>2</sub>)]<sup>4+</sup> (<b>1</b>, [Ru<sub>a</sub><sup>II</sup>-Ru<sub>b</sub><sup>II</sup>-OH<sub>2</sub>]<sup>4+</sup>; bpy = 2,2′-bipyridine;
4-Mebpy-4′-bimpy = 4-(methylbipyridin-4′-yl)-<i>N</i>-benzimid-<i>N</i>′-pyridine; tpy = 2,2′:6′,2″-terpyridine),
as its chloride salt. The assembly incorporates both a visible light
absorber and a catalyst for water oxidation. With added ceric ammonium
nitrate (Ce<sup>IV</sup>, or CAN), both <b>1</b> and <b>2</b>, [Ru(tpy)(Mebim-py)(OH<sub>2</sub>)]<sup>2+</sup> (Mebim-py = 2-pyridyl-<i>N</i>-methylbenzimidazole), catalyze water oxidation. Time-dependent
UV/vis spectral monitoring following addition of 30 equiv of Ce<sup>IV</sup> reveals that the rate of Ce<sup>IV</sup> consumption is
first order both in Ce<sup>IV</sup> and in an oxidized form of the
assembly. The rate-limiting step appears to arise from slow oxidation
of this intermediate followed by rapid release of O<sub>2</sub>. This
is similar to isolated catalyst <b>2</b>, with redox potentials
comparable to the [-Ru<sub>b</sub>-OH<sub>2</sub>]<sup>2+</sup> site
in <b>1</b>, but <b>1</b> is more reactive than <b>2</b> by a factor of 8 due to a redox mediator effect
Synthesis and Electrocatalytic Water Oxidation by Electrode-Bound Helical Peptide Chromophore–Catalyst Assemblies
Artificial
photosynthesis based on dye-sensitized photoelectrosynthesis
cells requires the assembly of a chromophore and catalyst in close
proximity on the surface of a transparent, high band gap oxide semiconductor
for integrated light absorption and catalysis. While there are a number
of approaches to assemble mixtures of chromophores and catalysts on
a surface for use in artificial photosynthesis based on dye-sensitized
photoelectrosynthesis cells, the synthesis of discrete surface-bound
chromophore–catalyst conjugates is a challenging task with
few examples to date. Herein, a versatile synthetic approach and electrochemical
characterization of a series of oligoproline-based light-harvesting
chromophore–water-oxidation catalyst assemblies is described.
This approach combines solid-phase peptide synthesis for systematic
variation of the backbone, copper(I)-catalyzed azide–alkyne
cycloaddition (CuAAC) as an orthogonal approach to install the chromophore,
and assembly of the water-oxidation catalyst in the final step. Importantly,
the catalyst was found to be incompatible with the conditions both
for amide bond formation and for the CuAAC reaction. The modular nature
of the synthesis with late-stage assembly of the catalyst allows for
systematic variation in the spatial arrangement of light-harvesting
chromophore and water-oxidation catalyst and the role of intrastrand
distance on chromophore–catalyst assembly properties. Controlled
potential electrolysis experiments verified that the surface-bound
assemblies function as water-oxidation electrocatalysts, and electrochemical
kinetics data demonstrate that the assemblies exhibit greater than
10-fold rate enhancements compared to the homogeneous catalyst alone
Visible Photoelectrochemical Water Splitting Based on a Ru(II) Polypyridyl Chromophore and Iridium Oxide Nanoparticle Catalyst
Preparation
of Ru(II) polypyridyl–iridium oxide nanoparticle (IrO<sub>X</sub> NP) chromophore–catalyst assemblies on an FTO|<i>nano</i>ITO|TiO<sub>2</sub> core/shell by a layer-by-layer procedure is described
for application in dye-sensitized photoelectrosynthesis cells (DSPEC).
Significantly enhanced, bias-dependent photocurrents with Lumencor
455 nm 14.5 mW/cm<sup>2</sup> irradiation are observed for core/shell
structures compared to TiO<sub>2</sub> after derivatization with [Ru(4,4′-PO<sub>3</sub>H<sub>2</sub>bpy)<sub>2</sub>(bpy)]<sup>2+</sup> (RuP<sub>2</sub>) and uncapped IrO<sub>X</sub> NPs at pH 5.8 in NaSiF<sub>6</sub> buffer with a Pt cathode. Photocurrents arising from photolysis
of the resulting photoanodes, FTO|<i>nano</i>ITO|TiO<sub>2</sub>|−RuP<sub>2</sub>,IrO<sub>2</sub>, are dependent on
TiO<sub>2</sub> shell thickness and applied bias, reaching 0.2 mA/cm<sup>2</sup> at 0.5 V vs AgCl/Ag with a shell thickness of 6.6 nm. Long-term
photolysis in the NaSiF<sub>6</sub> buffer results in a marked decrease
in photocurrent over time due to surface hydrolysis and loss of the
chromophore from the surface. Long-term stability, with sustained
photocurrents, has been obtained by atomic layer deposition (ALD)
of overlayers of TiO<sub>2</sub> to stabilize surface binding of −RuP<sub>2</sub> prior to the addition of the IrO<sub>X</sub> NPs