16 research outputs found
Solution-Processed Short-Wave Infrared PbS Colloidal Quantum Dot/ZnO Nanowire Solar Cells Giving High Open-Circuit Voltage
A systematic
investigation into the performance of PbS quantum
dot (QD)/ZnO nanowire (NW) solar cells in the near-infrared (NIR)
and short-wave infrared (SWIR) regions was carried out. The solar
cells were confirmed to convert a wide range of solar energy (3.54–0.62
eV, corresponding to 0.35–2.0 μm). We found that the
solar cells working in the SWIR region had a high open-circuit voltage
(<i>V</i><sub>oc</sub>). A relatively high <i>V</i><sub>oc</sub> of 0.25 V was achieved even in solar cells whose photocurrent
onsets were at approximately 0.64 eV (1.9 μm); this <i>V</i><sub>oc</sub> is as high as that of Ge solar cells, which
have been used for III–V compound semiconductor triple-junction
solar cells. Although short-circuit current density and fill factor
have to be further increased, these results indicate that solution-processed
colloidal QD solar cells with ZnO NWs are promising candidates for
the middle and/or bottom subcells of multijunction solar cells
Theoretical Study of the Surface Complex between TiO<sub>2</sub> and TCNQ Showing Interfacial Charge-Transfer Transitions
The surface complex of TiO<sub>2</sub> nanoparticles and TCNQ was studied using density functional theory (DFT) calculations. The structure of the surface complex was optimized, showing an IR spectrum analogous to the experimental spectrum. From time-dependent DFT calculations based on this optimized structure, we demonstrated that the interfacial charge-transfer transitions from the HOMO of the surface-bound TCNQ molecule to the unoccupied levels of the TiO<sub>2</sub> nanocluster occur in the visible to near-IR region
Effects of Chain Orientation in Self-Organized Buffer Layers Based on Poly(3-alkylthiophene)s for Organic Photovoltaics
Surface-segregated
monolayers (SSMs) based on two polyÂ(3-alkylthiophene)Âs with semifluoroalkyl
groups at either the side chains (P3DDFT) or one end of the main chain
(P3BT-F<sub>17</sub>) were used as self-organized buffer layers at
the electrode interfaces in bulk heterojunction (BHJ) organic photovoltaic
devices. Both of the SSMs greatly shifted the vacuum levels of the
BHJ films at the surface due to the aligned permanent dipole moments
of the semifluoroalkyl chains. Hole extraction in the BHJ of polyÂ(3-hexylthiophene)
(P3HT):[6,6]-phenyl C<sub>61</sub>-butyric acid methyl ester (PCBM)
became more efficient in the presence of the P3DDFT buffer layer,
resulting in an improved power conversion efficiency. In contrast,
the SSM of P3BT-F<sub>17</sub> induced changes in the chain orientation
of P3HT and the morphology of the BHJ films, resulting in decreased
performance. These results indicate that the molecular design of polymer-based
SSMs can affect not only the energy structure at the interface but
also the morphology and the molecular orientations in the BHJs
PbS-Quantum-Dot-Based Heterojunction Solar Cells Utilizing ZnO Nanowires for High External Quantum Efficiency in the Near-Infrared Region
The improvement of solar cell performance
in the near-infrared
(near-IR) region is an important challenge to increase power conversion
efficiency under one-sun illumination. PbS quantum-dot (QD)-based
heterojunction solar cells with high efficiency in the near-IR region
were constructed by combining ZnO nanowire arrays with PbS QDs, which
give a first exciton absorption band centering at wavelengths longer
than 1 μm. The morphology of ZnO nanowire arrays was systematically
investigated to achieve high light-harvesting efficiency as well as
efficient carrier collection. The solar cells with the PbS QD/ZnO
nanowire structures made up of densely grown thin ZnO nanowires about
1.2 μm long yielded a maximum incident-photon-to-current conversion
efficiency (IPCE) of 58% in the near-IR region (@1020 nm) and over
80% in the visible region (shorter than 670 nm). The power conversion
efficiency obtained on the solar cell reached about 6.0% under simulated
one-sun illumination
Enhancement of Near-IR Photoelectric Conversion in Dye-Sensitized Solar Cells Using an Osmium Sensitizer with Strong Spin-Forbidden Transition
A new osmium (Os) complex of the [OsÂ(tcterpy)-(4,4′-bisÂ(<i>p</i>-butoxystyryl)-2,2′-bipyridine)ÂCl]ÂPF<sub>6</sub> (Os-stbpy) has been synthesized and characterized for dye-sensitized
solar cells (DSSCs). The Os-stbpy dye shows enhanced spin-forbidden
absorptions around 900 nm. The DSSCs with Os-stbpy show a wide-band
spectral response up to 1100 nm with high overall conversion efficiency
of 6.1% under standard solar illumination
Nanostructured Two-Component Liquid-Crystalline Electrolytes for High-Temperature Dye-Sensitized Solar Cells
Nanostructured
liquid-crystalline (LC) ion transporters have been
developed and applied as new electrolytes for dye-sensitized solar
cells (DSSCs). The new electrolytes are two-component liquid crystals
consisting of a carbonate-based mesogen and an ionic liquid that self-assemble
into two-dimensional (2D) nanosegregated structures forming well-defined
ionic pathways suitable for the I<sup>–</sup>/I<sub>3</sub><sup>–</sup> redox couple transportation. These electrolytes
are nonvolatile and they show LC phases over wide temperature ranges.
The DSSCs containing these electrolytes exhibit exceptional open-circuit
voltages (<i>V</i><sub>oc</sub>) and improved power conversion
efficiencies with increasing temperature. Remarkably, these solar
cells operate at temperatures up to 120 °C, which is, to the
best of our knowledge, the highest working temperature reported for
a DSSC. The nature of the LC electrolyte and the interactions at the
TiO<sub>2</sub> electrode/electrolyte interface lead to a partial
suppression of electron recombination reactions, which is key in the
exceptional features of these LC-DSSCs. Thus, this type of solar cells
are of interest, because they can produce electricity efficiently
from light at elevated temperatures
Widely Controllable Electronic Energy Structure of ZnSe–AgInSe<sub>2</sub> Solid Solution Nanocrystals for Quantum-Dot-Sensitized Solar Cells
I–III–VI<sub>2</sub>-semiconductor-based nanocrystals
of ZnSe–AgInSe<sub>2</sub> solid solution ((AgIn)<sub><i>x</i></sub>Zn<sub>2(1‑<i>x</i>)</sub>Se<sub>2</sub>, ZAISe) with average sizes of 3.5–6.2 nm were successfully
synthesized through thermal reaction of corresponding metal acetates
and selenourea in a hot oleylamine solution. The optical property
of ZAISe solid solution nanocrystals was tunable in a broad wavelength
region from visible to near-infrared light by changing the composition
of solid solution, where the energy gap of ZAISe nanocrystals was
enlarged from 1.44 to 3.00 eV with an increase in the fraction of
ZnSe in ZAISe, that is, with a decrease in <i>x</i> from
1.0 to 0. Both levels of conduction band and valence band edges, determined
by photoelectron spectroscopy in air, were monotonously shifted to
higher levels with an increase in the fraction of ZnSe. Quantum-dot-sensitized
solar cells were fabricated with porous TiO<sub>2</sub> film electrodes
immobilized with ZAISe nanocrystals using 3-mercaptopropionic acid
as a cross-linking agent. The light conversion efficiency of the thus-obtained
cells was enhanced by covering ZAISe nanocrystals with a CdS thin
layer by the SILAR method. The photocurrent action spectra agreed
well with absorption spectra of ZAISe nanocrystals immobilized on
TiO<sub>2</sub> electrodes. Maximum energy conversion efficiency of
1.9% was obtained for the cell fabricated with ZAISe nanocrystals
with <i>x</i> = 0.5 as a sensitizer under irradiation with
simulated solar light of AM 1.5G
Phase Control of Organometal Halide Perovskites for Development of Highly Efficient Solar Cells
To develop a highly efficient solar cell using organometal
halide
perovskites, its microscale structure control is one of the most important
factors because the microstructural defects inside the organometal
halide perovskite are harmful to charge carrier flow and, thus, degrade
device performance. In this study, we confirmed the existence of large
physical gaps at the grain boundary in a methylammonium iodide (MAPbI3, MA = CH3NH3) perovskite with transmission
electron microscopy (TEM) analysis and revealed that the physical
gap prevents charge carrier flow in the MAPbI3 perovskite.
To minimize the physical gap and its negative influences, the grain
size of the MAPbI3 perovskite was optimized by increasing
the portion of the cubic phase via microstructural phase control using
liquid nitrogen (LN2). Through microstructural phase control
of the MAPbI3 perovskite, its grain boundaries and physical
gap were significantly decreased, and 20.23% power conversion efficiency
(PCE) was achieved with a single cation MAPbI3 perovskite
solar cell
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
Liquid-Crystalline Dye-Sensitized Solar Cells: Design of Two-Dimensional Molecular Assemblies for Efficient Ion Transport and Thermal Stability
Nanostructured
liquid-crystalline (LC) electrolytes have been developed for efficient
and stable <i>quasi</i>-solid-state dye-sensitized solar
cells (DSSCs). Two types of ionic LC assemblies for electrolytes have
been designed: (i) noncovalent assemblies of two-component mixtures
consisting of I<sub>2</sub>-doped imidazolium ionic liquids and carbonate-terminated
mesogenic compounds (noncovalent type) and (ii) single-component mesogenic
compounds covalently bonding an imidazolium moiety doped with I<sub>2</sub> (covalent type). These mesogenic compounds are designed with
flexible oligooxyethylene spacers connecting the mesogenic and the
polar moieties. The oligooxyethylene-based material design inhibits
crystallization and leads to enhanced ion transport as compared to
alkyl-linked analogues due to the higher flexibility of the oligooxyethylene
spacer. The noncovalent type mixtures exhibit a more than 10 times
higher I<sub>3</sub><sup>–</sup> diffusion coefficient compared
to the covalent type assemblies. DSSCs containing the noncovalent
type liquid crystals show power conversion efficiencies (PCEs) of
up to 5.8 ± 0.2% at 30 °C and 0.9 ± 0.1% at 120 °C.
In contrast, solar cells containing the covalent type electrolytes
show significant increase in PCE up to 2.4 ± 0.1% at 120 °C
and show superior performance to the noncovalent type-based devices
at temperature above 90 °C. Furthermore, the LC-DSSCs exhibit
excellent long-term stability over 1000 h. These novel electrolyte
designs open unexplored paths for the development of DSSCs capable
of efficient conversion of light to electricity in a wide range of
temperatures