17 research outputs found
Visualization 1: Enhancement of light-matter interaction and photocatalytic efficiency of Au/TiO<sub>2</sub> hybrid nanowires
Real-time view of Au growth along hybrid nanowires driven by local UV illumination. Originally published in Optics Express on 11 July 2016 (oe-24-14-15171
Enhanced Local and Nonlocal Photoluminescence of Organic Rubrene Microrods using Surface Plasmon of Gold Nanoparticles: Applications to Ultrasensitive and Remote Biosensing
Nonlocal photoluminescence (PL) signal
transfer through semiconducting
nanostructures has been intensively studied for its potential applicability
in photonic circuits, optical communications, and optical sensing.
In this study, organic semiconducting rubrene microrods (MRs) were
synthesized and hybridized with functionalized gold nanoparticles
(Au-NPs) to optimize both their optical and biosensing properties.
The steady-state local PL intensity of the rubrene MR was considerably
enhanced by the Au-NPs’ hybridization due to the energy-transfer
effect from the surface plasmon (SP) coupling. It was clearly observed
that the nonlocal PL signal-transfer efficiency of rubrene/Au-NPs
hybrid MRs drastically increased along crystalline axes with the aid
of the SP effect. The coupling of exciton polaritons in the luminescent
rubrene MR with the SP as well as the scattering effect contribute
to the variation of the exciton decay rate, resulting in a change
in the PL signal-transfer efficiency for the hybrid MRs. The enhancement
of the local and nonlocal PL emission of the rubrene/Au-NPs hybrid
MRs was applied to ultrasensitive and remote biosensing. We observed
PL signal transfer of fluorescent-dye attached DNA along the MR and
successfully detected target-DNA with a concentration of 100 picomole
using rubrene/Au-NPs/probe–DNA hybrid MR
Spectroscopic Visualization of Grain Boundaries of Monolayer Molybdenum Disulfide by Stacking Bilayers
Polycrystalline growth of molybdenum disulfide (MoS<sub>2</sub>) using chemical vapor deposition (CVD) methods is subject to the formation of grain boundaries (GBs), which have a large effect on the electrical and optical properties of MoS<sub>2</sub>-based optoelectronic devices. The identification of grains and GBs of CVD-grown monolayer MoS<sub>2</sub> has traditionally required atomic resolution microscopy or nonlinear optical imaging techniques. Here, we present a simple spectroscopic method for visualizing GBs of polycrystalline monolayer MoS<sub>2</sub> using stacked bilayers and mapping their indirect photoluminescence (PL) peak positions and Raman peak intensities. We were able to distinguish a GB between two MoS<sub>2</sub> grains with tilt angles as small as 6° in their grain orientations and, based on the inspection of several GBs, found a simple empirical rule to predict the location of the GBs. In addition, the large number of twist angle domains traced through our facile spectroscopic mapping technique allowed us to identify a continuous evolution of the coupled structural and optical properties of bilayer MoS<sub>2</sub> in the vicinity of the 0° and 60° commensuration angles which were explained by elastic deformation model of the MoS<sub>2</sub> membranes
Efficient Energy Transfer (EnT) in Pyrene- and Porphyrin-Based Mixed-Ligand Metal–Organic Frameworks
Designing and synthesizing
the ordered light-harvesting systems,
possessing complementary absorption and energy-transfer process between
the chromophores, are essential steps to accomplish successful mimicking
of the natural photosynthetic systems. Metal–organic frameworks
(MOFs) can be considered as an ideal system to achieve this due to
their highly ordered structure, superior synthetic versatility, and
tailorable functionality. Herein, we have synthesized the new light-harvesting
mixed-ligand MOFs (MLMs, MLM-1–3) via solvothermal reactions
between a Zr<sub>6</sub> cluster and a mixture of appropriate ratio
of 1,3,6,8-tetrakisÂ(<i>p</i>-benzoic acid)Âpyrene and [5,10,15,20-tetrakisÂ(4-carboxy-phenyl)Âporphyrinato]-ZnÂ(II)
ligands. The identical symmetry and connectivity of the two ligands
of the MLMs was the key parameter of successful synthesis as a single
MOF form, and the ample overlap between the emission spectrum of pyrene
and the absorption spectrum of porphyrin provided the ideal platform
to design an efficient-energy transfer (EnT) process within the MLMs.
We obtained the nanoscale maps of the fluorescence intensities and
lifetimes of microsize MLM grains for unambiguous visualization of
EnT phenomena occurring between two ligands in MLMs. Moreover, due
to complementary absorption and energy transfer between the two ligands
in the MLMs, our MLMs performed as superior photoinduced singlet-oxygen
generators, verifying the enhanced light-harvesting properties of
the pyrene- and porphyrin-based MLMs
Local Enhancement of Exciton Emission of Monolayer MoS<sub>2</sub> by Copper Phthalocyanine Nanoparticles
Monolayer transition-metal
dichalcogenides (1L-TMDs) provide ideal
platforms to study light emission using two-dimensionally confined
excitons. Recent studies have shown that the exciton emissions of
1L-TMDs can be conveniently modulated by developing heterostructures
with zero-dimensional nanoparticles (NPs) or quantum dots. In this
study, we synthesized organic semiconducting copper phthalocyanine
(CuPc) NPs with sizes in the range of 30–70 nm by a re-precipitation
method and decorated the chemical vapor deposition-grown 1L-MoS<sub>2</sub> with these NPs. This hybrid system exhibited a 6 times larger
local photoluminescence (PL) at the positions of the CuPc NPs compared
with the pristine 1L-MoS<sub>2</sub> sample. The PL enhancement and
spectral modification of the 1L-MoS<sub>2</sub> decorated with CuPc
NPs were attributed to the p-doping effect of the CuPc NPs, confirmed
by spectral analysis and field-effect transistor measurements
Surface-Plasmonic-Coupled Photodetector Based on MAPbI<sub>3</sub> Perovskites with Au Nanoparticles: Significantly Enhanced Photoluminescence and Photodetectivity
Organic–inorganic metal halide perovskites (OMHPs)
are promising
active materials suitable for highly efficient solar cells, photodetectors,
light-emitting diodes, and sensors. In this study, methylammonium
lead iodide (MAPbI3) thin sheets (TSs) were synthesized
as OMHPs using both hybrid vapor-solution method for optical study
and anti-solvent solution method for the photodetector. π-Conjugated
polyelectrolyte (π-CPE), such as poly(9,9-bis(4′-sulfonatobutyl)fluorene-alt-1,4-phenylene)
potassium (FPS-K), was spin-coated on the MAPbI3 TS, and
functionalized gold nanoparticles (Au-NPs) were hybridized. The laser
confocal microscope photoluminescence (PL) intensity of the MAPbI3 TS was significantly enhanced after hybridization with Au-NPs/FPS-K,
owing to the passivating effect of the FPS-K and the generation of
extra-photoexcited charges by local surface plasmon resonance (LSPR)
coupling with Au-NPs. These results were supported by the variation
in the exciton lifetime measured from the time-resolved PL decay curves.
The photocurrent of the MAPbI3 photodetector increased
up to 1.1 Ă— 104 times, and the photoresponsivity (R) and photodetectivity (D*) increased
by 70 and 13 times, respectively, with the hybridization of Au-NPs/FPS-K.
The highest D* of the Au-NPs/FPS-K/MAPbI3 photodetector was measured to be 7.5 Ă— 1010 Jones
at 735 nm excitation. The power and wavelength dependencies of R and D* for the MAPbI3 photodetector
were also significantly improved by the Au-NPs/FPS-K hybrid. These
results support the development of high-performance perovskite photodetectors
utilizing LSPR coupling with the π-CPE layer
Composition-Tunable Synthesis of Large-Scale Mo<sub>1–<i>x</i></sub>W<sub><i>x</i></sub>S<sub>2</sub> Alloys with Enhanced Photoluminescence
Alloying
two-dimensional transition metal dichalcogenides (2D TMDs)
is a promising avenue for band gap engineering. In addition, developing
a scalable synthesis process is essential for the practical application
of these alloys with tunable band gaps in optoelectronic devices.
Here, we report the synthesis of optically uniform and scalable single-layer
Mo<sub>1–<i>x</i></sub>W<sub><i>x</i></sub>S<sub>2</sub> alloys by a two-step chemical vapor deposition (CVD)
method followed by a laser thinning process. The amount of W content
(<i>x</i>) in the Mo<sub>1–<i>x</i></sub>W<sub><i>x</i></sub>S<sub>2</sub> alloy is systemically
controlled by the co-sputtering technique. The post-laser process
allows layer-by-layer thinning of the Mo<sub>1–<i>x</i></sub>W<sub><i>x</i></sub>S<sub>2</sub> alloys down to
a single-layer; such a layer exhibits tunable properties with the
optical band gap ranging from 1.871 to 1.971 eV with variation in
the W content, <i>x</i> = 0 to 1. Moreover, the predominant
exciton complexes, trions, are transitioned to neutral excitons with
increasing W concentration; this is attributed to the decrease in
excessive charge carriers with an increase in the W content of the
alloy. Photoluminescence (PL) and Raman mapping analyses suggest that
the laser-thinning of the Mo<sub>1–<i>x</i></sub>W<sub><i>x</i></sub>S<sub>2</sub> alloys is a self-limiting
process caused by heat dissipation to the substrate, resulting in
spatially uniform single-layer Mo<sub>1–<i>x</i></sub>W<sub><i>x</i></sub>S<sub>2</sub> alloy films. Our findings
present a promising path for the fabrication of large-scale single-layer
2D TMD alloys and the design of versatile optoelectronic devices
Effects of TiO<sub>2</sub> Interfacial Atomic Layers on Device Performances and Exciton Dynamics in ZnO Nanorod Polymer Solar Cells
The
performances of organic electronic and/or photonic devices
rely heavily on the nature of the inorganic/organic interface. Control
over such hybrid interface properties has been an important issue
for optimizing the performances of polymer solar cells bearing metal-oxide
conducting channels. In this work, we studied the effects of an interfacial
atomic layer in an inverted polymer solar cell based on a ZnO nanorod
array on the device performance as well as the dynamics of the photoexcited
carriers. We adopted highly conformal TiO<sub>2</sub> interfacial
layer using plasma enhanced atomic layer deposition (PEALD) to improve
the compatibility between the solution-prepared active layer and the
ZnO nanorod array. The TiO<sub>2</sub> interfacial layer facilitated
exciton separation and subsequent charge transfer into the nanorod
channel, and it suppressed recombination of photogenerated carriers
at the interface. The presence of even 1 PEALD cycle of TiO<sub>2</sub> coating substantially improved the short-circuit current density
(<i>J</i><sub>sc</sub>), open circuit voltage (<i>V</i><sub>oc</sub>), and fill factor (FF), leading to more than 2-fold
enhancement in the power conversion efficiency (PCE). The dynamics
of the photoexcited carriers in our devices were studied using transient
absorption (TA) spectroscopy. The TA results clearly revealed that
the TiO<sub>2</sub> coating played a key role as an efficient quencher
of photogenerated excitons, thereby reducing the exciton lifetime.
The electrochemical impedance spectra (EIS) provided further evidence
that the TiO<sub>2</sub> atomic interfacial layer promoted the charge
transfer at the interface by suppressing recombination loss
Simultaneous Hosting of Positive and Negative Trions and the Enhanced Direct Band Emission in MoSe<sub>2</sub>/MoS<sub>2</sub> Heterostacked Multilayers
Heterostacking
of layered transition-metal dichalcogenide (LTMD)
monolayers (1Ls) offers a convenient way of designing two-dimensional
exciton systems. Here we demonstrate the simultaneous hosting of positive
trions and negative trions in heterobilayers made by vertically stacking
1L MoSe<sub>2</sub> and 1L MoS<sub>2</sub>. The charge transfer occurring
between the 1Ls of MoSe<sub>2</sub> and MoS<sub>2</sub> converted
the polarity of trions in 1L MoSe<sub>2</sub> from negative to positive,
resulting in the presence of positive trions in the 1L MoSe<sub>2</sub> and negative trions in the 1L MoS<sub>2</sub> of the same heterostacked
bilayer. Significantly enhanced MoSe<sub>2</sub> photoluminescence
(PL) in the heterostacked bilayers compared to the PL of 1L MoSe<sub>2</sub> alone suggests that, unlike other previously reported heterostacked
bilayers, direct band transition of 1L MoSe<sub>2</sub> in heterobilayer
was enhanced after the vertical heterostacking. Moreover, by inserting
hexagonal BN monolayers between 1L MoSe<sub>2</sub> and 1L MoS<sub>2</sub>, we were able to adjust the charge transfer to maximize the
MoSe<sub>2</sub> PL of the heteromultilayers and have achieved a 9-fold
increase of the PL emission. The enhanced optical properties of our
heterostacked LTMDs suggest the exciting possibility of designing
LTMD structures that exploit the superior optical properties of 1L
LTMDs
Impeding Exciton–Exciton Annihilation in Monolayer WS<sub>2</sub> by Laser Irradiation
Monolayer
(1L) transition metal dichalcogenides (TMDs) are two-dimensional
direct-bandgap semiconductors with promising applications of quantum
light emitters. Recent studies have shown that intrinsically low quantum
yields (QYs) of 1L-TMDs can be greatly improved by chemical treatments.
However, nonradiative exciton–exciton annihilation (EEA) appears
to significantly limit light emission of 1L-TMDs at a nominal density
of photoexcited excitons due to strong Coulomb interaction. Here we
show that the EEA rate constant (Îł) can be reduced by laser
irradiation treatment in mechanically exfoliated monolayer tungsten
disulfide (1L-WS<sub>2</sub>), causing significantly improved light
emission at the saturating optical pumping level. Time-resolved photoluminescence
(PL) measurements showed that γ reduced from 0.66 ± 0.15
cm<sup>2</sup>/s to 0.20 ± 0.05 cm<sup>2</sup>/s simply using
our laser irradiation. The laser-irradiated region exhibited lower
PL response at low excitation levels, however at the high excitation
level displayed 3Ă— higher PL intensity and QY than the region
without laser treatment. The shorter PL lifetime and lower PL response
at low excitation levels suggested that laser irradiation increased
the density of sulfur vacancies of 1L-WS<sub>2</sub>, but we attribute
these induced defects, adsorbed by oxygen in air, to the origin for
reduced EEA by hindering exciton diffusion. Our laser irradiation
was likewise effective for reducing EEA and increasing PL of chemically
treated 1L-WS<sub>2</sub> with a high QY, exhibiting the general applicability
of our method. Our results suggest that exciton–exciton interaction
in 1L-TMDs may be conveniently controlled by the laser treatment,
which may lead to unsaturated exciton emission at high excitation
levels