8 research outputs found
Crown Ether-Substituted Carbazole Dye for Dye-Sensitized Solar Cells: Controlling the Local Ion Concentration at the TiO<sub>2</sub>/Dye/Electrolyte Interface
The conduction band edge potentials
(<i>E</i><sub>CB</sub>) and electron lifetimes (Ï„)
of the TiO<sub>2</sub> electrodes
in dye-sensitized solar cells (DSSCs) are affected by ion concentrations
(e.g., Li<sup>+</sup> and I<sup>–</sup>/I<sub>3</sub><sup>–</sup>) at the TiO<sub>2</sub>/dye/electrolyte interface. To control the
local concentrations of these ions in the vicinity of the TiO<sub>2</sub> surface, a novel carbazole-based dye incorporating a 12-crown-4
ether on the carbazole donor (MK-70) was synthesized as a DSSC sensitizer.
The interactions between Li<sup>+</sup>/I<sup>–</sup>/I<sub>3</sub><sup>–</sup> and MK-70 were compared with those between
Li<sup>+</sup>/I<sup>–</sup>/I<sub>3</sub><sup>–</sup> and MK-1, an analogue lacking the crown ether. The crown ether did
not affect the <i>E</i><sub>CB</sub> level of TiO<sub>2</sub>, but it did decrease Ï„ at a high electrolytic Li<sup>+</sup> concentration. Results suggest that localized Li<sup>+</sup> ions
associated with the crown ethers electrostatically attract surplus
I<sub>3</sub><sup>–</sup> from the bulk electrolyte even though
the crown ethers are located far from the TiO<sub>2</sub> surface.
After the cells were aged, negative shifts in the <i>E</i><sub>CB</sub> levels of the TiO<sub>2</sub> electrode and blueshifts
of the MK-70 absorption spectra were observed with electrolytes that
included I<sup>–</sup>/I<sub>3</sub><sup>–</sup> and
Li<sup>+</sup>. The aging behavior may be determined by the balance
between two attractive forces, <i>K</i><sub>1</sub> (I<sup>–</sup>/I<sub>3</sub><sup>–</sup> and Li<sup>+</sup> at the TiO<sub>2</sub> surface) and <i>K</i><sub>2</sub> (dye interactions with I<sup>–</sup>/I<sub>3</sub><sup>–</sup> and Li<sup>+</sup>)
Efficiency Enhancement of ZnO-Based Dye-Sensitized Solar Cells by Low-Temperature TiCl<sub>4</sub> Treatment and Dye Optimization
ZnO
is a promising candidate as a low-cost porous semiconductor material
for photoelectrodes in dye-sensitized solar cells (DSSCs). However,
ZnO-based DSSCs tend to exhibit lower energy conversion efficiencies
than do those based on TiO<sub>2</sub>. In this study, the performance
of ZnO porous electrodes was enhanced using a surface treatment carried
out by immersion in cold aqueous TiCl<sub>4</sub> solution that resulted
in TiO<sub>2</sub>-coated ZnO (<i>Z</i>/<i>T</i>) electrodes. The <i>Z</i>/<i>T</i> electrodes
were sensitized with either the Ru complex dye N719 or the organic
indoline dye D149. For each dye, the DSSCs with the <i>Z</i>/<i>T</i> photoelectrodes showed the highest open-circuit
voltage (<i>V</i><sub>oc</sub>), short circuit current (<i>J</i><sub>sc</sub>), and power conversion efficiency compared
to those with ZnO, TiO<sub>2</sub>, or TiO<sub>2</sub>-coated TiO<sub>2</sub> (<i>T</i>/<i>T</i>) electrodes. To study
the effects of the TiCl<sub>4</sub> treatment, the relationships between
the electron lifetime (Ï„), cell voltage, and electron density
(<i>n</i>) of the cells prepared with each electrode, with
each of the two dyes, or without either dye were assessed. It was
found that the TiCl<sub>4</sub> treatment negatively shifted the conduction
band edge (CBE) potential of the ZnO electrodes by more than 100 mV
for both dyes and also in the absence of a dye. In addition, Ï„
increased with the use of the organic D149 and in the absence of a
dye. The DSSC with a D149-sensitized <i>Z</i>/<i>T</i> layer showed the highest efficiency of 4.89% under 100 mW cm<sup>–2</sup> irradiation
Structural Effect of Donor in Organic Dye on Recombination in Dye-Sensitized Solar Cells with Cobalt Complex Electrolyte
The effect of the
donor in an organic dye on the electron lifetime
of dye-sensitized solar cells (DSSCs) employing a cobalt redox electrolyte
was investigated. We synthesized organic dyes with donor moieties
of carbazole, coumarin, triphenylamine, and <i>N</i>-phenyl-carbazole
and measured the current–voltage characteristics and electron
lifetimes of the DSSCs with these dyes. The cell with the triphenylamine
donor dye produced the highest open circuit voltage and longest electron
lifetime. On the other hand, the lowest open circuit voltage and shortest
electron lifetime was obtained with coumarin donor dye, suggesting
that the coumarin attracted the cobalt redox couples to the surface
of the TiO<sub>2</sub> layer, thus increasing the concentration of
cobalt complex. On the other hand, the longest electron lifetime with
triphenylamine was attributed to the blocking effect by steric hindrance
of the nonplanar structure of the donor
Synthesis of Oligo(thienylene-vinylene) by Regiocontrolled Deprotonative Cross-Coupling
Concise synthesis of oligoÂ(thienylene-vinylene)
with a head-to-tail
type structure is achieved by regioselective deprotonative coupling
of 3-hexylthiophene. The palladium catalyzed reaction of 3-hexylthiophene
with (<i>E</i>)-2-(2-bromoethenyl)-3-hexylÂthiophene
takes place to afford head-to-tail type <i>trans</i>-1,2-dithienylÂethene.
Further extension of a vinylthiophene unit is similarly performed
in an iterative manner
Crystallization Dynamics of Organolead Halide Perovskite by Real-Time X‑ray Diffraction
We analyzed the crystallization process
of the CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> perovskite by observing
real-time X-ray diffraction immediately after combining a PbI<sub>2</sub> thin film with a CH<sub>3</sub>NH<sub>3</sub>I solution.
A detailed analysis of the transformation kinetics demonstrated the
fractal diffusion of the CH<sub>3</sub>NH<sub>3</sub>I solution into
the PbI<sub>2</sub> film. Moreover, the perovskite crystal was found
to be initially oriented based on the PbI<sub>2</sub> crystal orientation
but to gradually transition to a random orientation. The fluctuating
characteristics of the crystallization process of perovskites, such
as fractal penetration and orientational transformation, should be
controlled to allow the fabrication of high-quality perovskite crystals.
The characteristic reaction dynamics observed in this study should
assist in establishing reproducible fabrication processes for perovskite
solar cells
Adjustment of Conduction Band Edge of Compact TiO<sub>2</sub> Layer in Perovskite Solar Cells Through TiCl<sub>4</sub> Treatment
Perovskite
solar cells (PSCs) without a mesoporous TiO<sub>2</sub> layer, that
is, planar-type PSCs exhibit poorer cell performance as compared to
PSCs with a porous TiO<sub>2</sub> layer, owing to inefficient electron
transfer from the perovskite layer to the compact TiO<sub>2</sub> layer
in the former case. The matching of the conduction band levels of
perovskite and the compact TiO<sub>2</sub> layer is thus essential
for enhancing PSC performance. In this study, we demonstrate the shifting
of the conduction band edge (CBE) of the compact TiO<sub>2</sub> layer
through a TiCl<sub>4</sub> treatment, with the aim of improving PSC
performance. The CBE of the compact TiO<sub>2</sub> layer was shifted
to a higher level through the TiCl<sub>4</sub> treatment and then
shifted in the opposite direction, that is, to a lower level, through
a subsequent heat treatment. These shifts in the CBE were reflected
in the PSC performance. The TiCl<sub>4</sub>-treated PSC showed an
increase in the open-circuit voltage of more than 150 mV, as well
as a decrease of 100 mV after being heated at 450 °C. On the
other hand, the short-circuit current decreased after the treatment
but increased after heating at temperatures higher than 300 °C.
The treated PSC subjected to subsequent heating at 300 °C exhibited
the best performance, with the power conversion efficiency of the
PSC being 17% under optimized conditions
Highly Efficient 17.6% Tin–Lead Mixed Perovskite Solar Cells Realized through Spike Structure
Frequently
observed high <i>V</i><sub>oc</sub> loss in
tin–lead mixed perovskite solar cells is considered to be one
of the serious bottle-necks in spite of the high attainable Jsc due
to wide wavelength photon harvesting. An amicable solution to minimize
the <i>V</i><sub>oc</sub> loss up to 0.50 V has been demonstrated
by introducing an n-type interface with spike structure between the
absorber and electron transport layer inspired by highly efficient
CuÂ(In,Ga)ÂSe<sub>2</sub> solar cells. Introduction of a conduction
band offset of ∼0.15 eV with a thin phenyl-C61-butyric acid
methyl ester layer (∼25 nm) on the top of perovskite absorber
resulted into improved <i>V</i><sub>oc</sub> of 0.75 V leading
to best power conversion efficiency of 17.6%. This enhancement is
attributed to the facile charge flow at the interface owing to the
reduction of interfacial traps and carrier recombination with spike
structure as evidenced by time-resolved photoluminescence, nanosecond
transient absorption, and electrochemical impedance spectroscopy measurements
Investigation of Interfacial Charge Transfer in Solution Processed Cs<sub>2</sub>SnI<sub>6</sub> Thin Films
Cesium
tin halide based perovskite Cs<sub>2</sub>SnI<sub>6</sub> has been
subjected to in-depth investigations owing to its potentiality
toward the realization of environment benign Pb free and stable solar
cells. In spite of the fact that Cs<sub>2</sub>SnI<sub>6</sub> has
been successfully utilized as an efficient hole transport material
owing to its p-type semiconducting nature, however, the nature of
the majority carrier is still under debate. Therefore, intrinsic properties
of Cs<sub>2</sub>SnI<sub>6</sub> have been investigated in detail
to explore its potentiality as light absorber along with facile electron
and hole transport. A high absorption coefficient (5 × 10<sup>4</sup> cm<sup>–1</sup>) at 700 nm indicates the penetration
depth of 700 nm light to be 0.2 μm, which is comparable to conventional
Pb based solar cells. Preparation of pure and CsI impurity free dense
thin films with controllable thicknesses of Cs<sub>2</sub>SnI<sub>6</sub> by the solution processable method has been reported to be
difficult owing to its poor solubility. An amicable solution to circumvent
such problems of Cs<sub>2</sub>SnI<sub>6</sub> has been provided utilizing
spray-coating in combination with spin-coating. The presence of two
emission peaks at 710 and 885 nm in the prepared Cs<sub>2</sub>SnI<sub>6</sub> thin films indicated coexistence of quantum dot and bulk
parts which were further supported by transmission electron microscopy
(TEM) investigations. Time-resolved photoluminescence (PL) and transient
absorption spectroscopy (TAS) were employed to investigate the excitation
carrier lifetime, which revealed fast decay kinetics in the picoseconds
(ps) to nanoseconds (ns) time domains. Time-resolved microwave photoconductivity
decay (MPCD) measurement provided the mobile charge carrier lifetime
exceeding 300 ns, which was also in agreement with the nanosecond
transient absorption spectroscopy (ns-TAS) indicating slow charge
decay lasting up to 20 μs. TA assisted interfacial charge transfer
investigations utilizing Cs<sub>2</sub>SnI<sub>6</sub> in combination
with n-type PCBM and p-type P3HT exhibited both intrinsic electron
and hole transport