9 research outputs found
Photoinduced Electron Transfer Dynamics of Cyclometalated Ruthenium (II)āNaphthalenediimide Dyad at NiO Photocathode
Both forward and backward electron
transfer kinetics at the sensitizer/NiO
interface is critical for p-type dye-sensitized photocathodic device.
In this article, we report the photoinduced electron transfer kinetics
of a RuĀ(II) chromophoreāacceptor dyad sensitized NiO photocathode.
The dyad (O26) is based on a cyclometalated RuĀ(N<sup>ā§</sup>C<sup>ā§</sup>N)Ā(N<sup>ā§</sup>N<sup>ā§</sup>N)
(RuĀ[II]) chromophore and a naphthalenediimide (NDI) acceptor, where
N<sup>ā§</sup>C<sup>ā§</sup>N represents 2,2ā²-(4,6-dimethyl-phenylene)-bispyridine
and N<sup>ā§</sup>N<sup>ā§</sup>N represents 2,2ā²,6ā²,6ā³-terpyridine
ligand. When the dyad is dissolved in a CH<sub>3</sub>CN solution,
electron transfer to form the RuĀ(III)āNDI<sup>ā</sup> occurs with a rate constant <i>k</i><sub>f</sub> = 1.1
Ć 10<sup>10</sup> s<sup>ā1</sup> (Ļ<sub>f</sub> =
91 ps), and electronāhole pair recombines to regenerate ground
state with a rate constant <i>k</i><sub>b</sub> = 4.1 Ć
10<sup>9</sup> s<sup>ā1</sup> (Ļ<sub>b</sub> = 241 ps).
When the dyad is adsorbed on a NiO film by covalent attachment through
the carboxylic acid group, hole injection takes place first within
our instrument response time (ā¼180 fs) followed by the subsequent
electron shift onto the NDI to produce the interfacial charge-separated
state [NiOĀ(h<sup>+</sup>)āRuĀ(II)āNDI<sup>ā</sup>] with a rate constant <i>k</i><sub>f</sub> = 9.1 Ć
10<sup>11</sup> s<sup>ā1</sup> (Ļ<sub>f</sub> = 1.1 ps).
The recovery of the ground state occurs with a multiexponential rate
constant <i>k</i><sub>b</sub> = 2.3 Ć 10<sup>9</sup> s<sup>ā1</sup> (Ļ<sub>b</sub> = 426 ps). The charge
recombination rate constant is slightly slower than a reference cyclometalated
ruthenium compound (O25) with no NDI group (Ļ<sub>b</sub> =
371 ps). The fast formation of interfacial charge separated state
is a result of ultrafast hole injection resulting in the reduced form
of sensitizer, which provides a larger driving force for NDI reduction.
The kinetic study suggests that RuĀ(II) chromophoreāacceptor
dyads are promising sensitizers for the NiO photocathode devices
Electrochromic Graphene Molecules
Polyclic aromatic hydrocarbons also called Graphene Molecules (GMs), with chemical composition C<sub>132</sub>H<sub>36</sub>(COOH)<sub>2</sub> were synthesized <i>in situ</i> on the surface of transparent nanocrystalline indium tin oxide (<i>nc</i>-ITO) electrodes and their electronic structure was studied electrochemically and spectro-electrochemically. Variations in the potential applied onto the <i>nc</i>-ITO/GM electrodes induce only small changes in the observed current, but they produce dramatic changes in the absorption of the GMs, which are associated with their oxidation and reduction. Analysis of the absorption changes using a modified Nernst equation is used to determine standard potentials associated with the individual charge transfer processes. For the GMs prepared here, these were found to be <i>E</i><sub>1,ox</sub><sup>0</sup> = 0.77 Ā± 0.01 V and <i>E</i><sub>2,ox</sub><sup>0</sup> = 1.24 Ā± 0.02 V <i>vs</i> NHE for the first and second oxidation and <i>E</i><sub>1,red</sub><sup>0</sup> = ā1.50 Ā± 0.04 V for the first reduction. The charge transfer processes are found to be nonideal. The nonideality factors associated with the oxidation and reduction processes are attributed to strong interactions between the GM redox centers. Under the conditions of potential cycling, GMs show rapid (seconds) color change with high contrast and stability. An electrochromic application is demonstrated wherein the GMs are used as the optically active component
p-Type Dye-Sensitized Solar Cells Based on Delafossite CuGaO<sub>2</sub> Nanoplates with Saturation Photovoltages Exceeding 460 mV
Exploring new p-type semiconductor nanoparticles alternative to
the commonly used NiO is crucial for p-type dye-sensitized solar cells
(p-DSSCs) to achieve higher open-circuit voltages (<i>V</i><sub>oc</sub>). Here we report the first application of delafossite
CuGaO<sub>2</sub> nanoplates for p-DSSCs with high photovoltages.
In contrast to the dark color of NiO, our CuGaO<sub>2</sub> nanoplates
are white. Therefore, the porous films made of these nanoplates barely
compete with the dye sensitizers for visible light absorption. This
presents an attractive advantage over the NiO films commonly used
in p-DSSCs. We have measured the dependence of <i>V</i><sub>oc</sub> on the illumination intensity to estimate the maximum obtainable <i>V</i><sub>oc</sub> from the CuGaO<sub>2</sub>-based p-DSSCs.
Excitingly, a saturation photovoltage of 464 mV has been observed
when a polypyridyl Co<sup>3+/2+</sup>(dtb-bpy) electrolyte was used.
Under 1 Sun AM 1.5 illumination, a <i>V</i><sub>oc</sub> of 357 mV has been achieved. These are among the highest values
that have been reported for p-DSSCs
Probing the Low Fill Factor of NiO pāType Dye-Sensitized Solar Cells
p-Type dye-sensitized solar cells (<i>p</i>-DSCs) have
attracted increasing attention recently, but they suffer from low
fill factors (FFs) and unsatisfactory efficiencies. A full comprehension
of the hole transport and recombination processes in the NiO <i>p</i>-DSC is of paramount importance for both the fundamental
study and the practical device optimization. In this article, NiO <i>p</i>-DSCs were systematically probed under various bias and
illumination conditions using electrochemical impedance spectroscopy
(EIS), intensity modulated photocurrent spectroscopy (IMPS), and intensity
modulated photovoltage spectroscopy (IMVS). Under the constant 1 sun
illumination, the recombination resistance (<i>R</i><sub>rec</sub>) of the cell deviates from an exponential relationship
with the potential and saturates at ā¼130 Ī© cm<sup>2</sup> under the short circuit condition, which is ascribed to the overwhelming
recombination with the reduced dye anions. Such a small <i>R</i><sub>rec</sub> results in the small dc resistance, which decreases
the āflatnessā of the <i>JāV</i> curve.
The quantitative analysis demonstrates that the FF value is largely
attenuated by the recombination of holes in NiO with the reduced dyes.
Our analysis also shows that if this recombination can be eliminated,
then an FF value of 0.6 can be reached, which agrees with the theoretical
calculation with a <i>V</i><sub>oc</sub> of 160 mV
Synthesis, Photophysics, and Photovoltaic Studies of Ruthenium Cyclometalated Complexes as Sensitizers for pāType NiO Dye-Sensitized Solar Cells
We report the first application of cyclometalated ruthenium
complexes
of the type RuĀ[(N<sup>ā§</sup>N)<sub>2</sub>(C<sup>ā§</sup>N)]<sup>+</sup> as sensitizers for p-type NiO dye-sensitized solar
cells (NiO p-DSCs). These dyes exhibit broad absorption in the visible
region. The carboxylic anchoring group is attached to the phenylpyridine
ligand, which results in efficient hole injection. Moreover, the distance
between the RuĀ[(N<sup>ā§</sup>N)<sub>2</sub>(C<sup>ā§</sup>N)]<sup>+</sup> core and the carboxylic anchoring group is systematically
varied by inserting rigid phenylene linkers. Femtosecond transient
absorption (TA) studies reveal that the interfacial charge recombination
rate between reduced sensitizers and holes in the valence band of
NiO decreases as the number of phenylene linkers increases across
the series. As a result, the solar cell made of the dye with the longest
spacer (O12) exhibits the highest efficiency with both increased short-circuit
current (<i>J</i><sub>sc</sub>) and open-circuit voltage
(<i>V</i><sub>oc</sub>). The incident photon-to-current
conversion efficiency (IPCE) spectra match well with the absorption
spectra of sensitizers, suggesting the observed cathodic current is
generated from the dye sensitization. In addition, the absorbed photon-to-current
conversion efficiencies (APCEs) display an increment across the series.
We further studied the interfacial charge recombination of our solar
cells by electrochemical impedance spectroscopy (EIS). The results
reveal an enhanced hole lifetime as the number of phenylene linkers
increases. This study opens up opportunities of using cyclometalated
Ru complexes for p-DSCs
In Situ Synthesis of Graphene Molecules on TiO<sub>2</sub>: Application in Sensitized Solar Cells
We present a method for preparation
of graphene molecules (GMs),
whereby a polyphenylene precursor functionalized with surface anchoring
groups, preadsorbed on surface of TiO<sub>2</sub>, is oxidatively
dehydrogenated in situ via a Scholl reaction. The reaction, performed
at ambient conditions, yields surface adsorbed GMs structurally and
electronically equivalent to those synthesized in solution. The new
synthetic approach reduces the challenges associated with the tendency
of GMs to aggregate and provides a convenient path for integration
of GMs into optoelectronic applications. The surface synthesized GMs
can be effectively reduced or oxidized via an interfacial charge transfer
and can also function as sensitizers for metal oxides in light harvesting
applications. Sensitized solar cells (SSCs) prepared from mesoscopic
TiO<sub>2</sub>/GM films and an iodide-based liquid electrolyte show
photocurrents of ā¼2.5 mA/cm<sup>2</sup>, an open circuit voltage
of ā¼0.55 V and fill factor of ā¼0.65 under AM 1.5 illumination.
The observed power conversion efficiency of Ī· = 0.87% is the
highest reported efficiency for the GM sensitized solar cell. The
performance of the devices was reproducible and stable for a period
of at least 3 weeks. We also report first external and internal quantum
efficiency measurements for GM SSCs, which point to possible paths
for further performance improvements