8 research outputs found
Synthesis of Hafnium Oxide-Gold Core–Shell Nanoparticles
Developing cheap composite nanoparticle systems that
combines a
high dielectric constant with good conductivity is important for the
future of the electronic industry. In this study, two different sizes,
7.3 ± 2.2 and 5.6 ± 1.9 nm, of HfO<sub>2</sub>@Au core–shell
nanoparticles are prepared by using a high-temperature reduction method.
The core–shell nanoparticles are characterized by powder X-ray
diffraction, high-resolution transmission electron microscopy (HRTEM),
energy dispersive X-ray analysis (EDX), and UV–visible absorption
spectroscopy. HfO<sub>2</sub> exhibits no absorption in the visible
region, but the HfO<sub>2</sub>@Au core–shell nanoparticles
show a plasmon absorption band at 555 nm that is 25 nm red-shifted
as compared to pure gold nanoparticles. According to transmission
electron microscopy and energy dispersive X-ray analysis, the HfO<sub>2</sub> particles are coated with approximately three atomic layers
of gold
Fe and Ni Dopants Facilitating Ammonia Synthesis on Mn<sub>4</sub>N and Mechanistic Insights from First-Principles Methods
Cyclic
step-catalysis enables intermittent, atmospheric ammonia
production, and can be integrated with sustainable and renewable energy
sources. By employing metal (e.g., Mn) nitride, a nitrogen carrier,
the rate-limiting N<sub>2</sub> activation step is bypassed. In this
work, molecular-level pathways, describing the reduction of Mn<sub>4</sub>N by dissociatively adsorbed hydrogen, were investigated using
periodic density functional theory (DFT). The established mechanism
confirmed that Fe and Ni doped in the nitride sublayer and top layer
can disturb local electronic structures and be exploited to tune the
ammonia production activity. The strength of N–M (M = Mn, Fe,
Ni) and H–M bonds both determine the overall reduction thermochemistry.
DFT-based modeling further showed that the low concentration of Fe
or Ni in the Mn<sub>4</sub>N sublayer facilitates N diffusion by lowering
the diffusion energy barrier. Also, these heteroatom dopant species,
particularly Ni, decrease the reduction endergonicity, thanks to the
strong hydrogen binding with the surface Ni dopant. The Brønsted–Evans–Polanyi
relationship and linear scaling relationships have been developed
to reveal ammonia evolution kinetic and energetic trends for a series
of idealized Fe- and Ni-doped Mn<sub>4</sub>N. Deviations from the
linear scaling relationship have been observed for certain doped systems,
indicating potentially more complex behaviors of metal nitrides and
intriguing promises for greater ammonia synthesis materials design
opportunities
Rapid Induction and Microwave Heat-Up Syntheses of CdSe Quantum Dots
The production of nanoparticles on
an industrial scale requires
an approach other than the widely used hot-injection method. In this
work, two heat-up methods are applied to nanoparticle synthesis. The
induction heating method produces CdSe quantum dots with ultrasmall
properties in seconds. Initial flow-through experiments demonstrate
that induction heating continuously produces quantum dots. These results
are compared with those from microwave synthesis, which produces quantum
dots on a longer timescale but provides fast, continuous heating.
Both methods can produce quantum dots within seconds because of rapid
heating. In addition, different precursors, single source and separate
source, give different results, ultimately providing a handle to control
quantum dot properties
Investigation of Charge Transfer Interactions in CdSe Nanorod P3HT/PMMA Blends by Optical Microscopy
CdSe nanorods and dilute poly(3-hexylthiophene) (P3HT) dispersed in poly(methyl methacrylate) (PMMA) films are investigated by wide field fluorescence microscopy and by analysis of single-point time transients. The data depict enhanced band-edge luminescence from nanorod/P3HT films, consistent with filling of CdSe surface traps by static charge transfer from P3HT. Band-edge luminescence from the nanorods is also shown to be enhanced by photoactivated (e.g., dynamic) charge transfer from P3HT to surface trap states on the CdSe nanorods. The role played by charge transfer in enhanced CdSe luminescence is further demonstrated by differences observed in the CdSe nanorod blinking behavior in P3HT and PMMA films
Investigation of Fluorescence Emission from CdSe Nanorods in PMMA and P3HT/PMMA Films
Complementary
fluorescence microscopy and ultrafast transient absorption
spectroscopy measurements spanning a range of time scales from seconds
to femtoseconds probe the interfacial dynamics of charge carriers
in CdSe nanorod/polymer blends. Together, these very different techniques
provide new information about the origin and dynamics of below-band-edge
emission from CdSe nanorods in CdSe/PMMA and CdSe/P3HT/PMMA films
[PMMA = polyÂ(methyl methacrylate); P3HT = polyÂ(3-hexylthiophene)].
Emission below the band edge of the CdSe nanorods is associated with
surface defects (traps) at the nanoparticle/polymer interface, where
conduction band electrons radiatively relax to the intraband defect
sites. The fluorescence microscopy experiments simultaneously monitor
both the trap emission and the band edge emission from single nanoparticles,
and reveal that the two emission channels are distinct. Transitions
between the two emissive states occur on time scales longer than ∼20
ms, and always involve an intermediate dark state in which no emission
is observed. The presence of P3HT increases the relative band edge
emission intensity and reduces the fluorescence intermittency (blinking)
of both emissive states. The ultrafast transient absorption experiments
monitor the evolution of a stimulated emission band below the CdSe
band edge following excitation of P3HT. The measurements reveal ultrafast
electron transfer from photoexcited P3HT to the CdSe nanorods within
the instrument response time of approximately 140 fs, and confirm
that there is strong coupling between the nanorods and P3HT in these
dilute blends. Analysis of separate CdSe nanorod etching experiments
suggests that the trap states are formed by the removal of atoms from
the ends of the nanorods in the presence of chloroform. Mechanisms
for charge trapping at the nanoparticle/polymer interface are discussed
Investigation of Fluorescence Emission from CdSe Nanorods in PMMA and P3HT/PMMA Films
Complementary
fluorescence microscopy and ultrafast transient absorption
spectroscopy measurements spanning a range of time scales from seconds
to femtoseconds probe the interfacial dynamics of charge carriers
in CdSe nanorod/polymer blends. Together, these very different techniques
provide new information about the origin and dynamics of below-band-edge
emission from CdSe nanorods in CdSe/PMMA and CdSe/P3HT/PMMA films
[PMMA = polyÂ(methyl methacrylate); P3HT = polyÂ(3-hexylthiophene)].
Emission below the band edge of the CdSe nanorods is associated with
surface defects (traps) at the nanoparticle/polymer interface, where
conduction band electrons radiatively relax to the intraband defect
sites. The fluorescence microscopy experiments simultaneously monitor
both the trap emission and the band edge emission from single nanoparticles,
and reveal that the two emission channels are distinct. Transitions
between the two emissive states occur on time scales longer than ∼20
ms, and always involve an intermediate dark state in which no emission
is observed. The presence of P3HT increases the relative band edge
emission intensity and reduces the fluorescence intermittency (blinking)
of both emissive states. The ultrafast transient absorption experiments
monitor the evolution of a stimulated emission band below the CdSe
band edge following excitation of P3HT. The measurements reveal ultrafast
electron transfer from photoexcited P3HT to the CdSe nanorods within
the instrument response time of approximately 140 fs, and confirm
that there is strong coupling between the nanorods and P3HT in these
dilute blends. Analysis of separate CdSe nanorod etching experiments
suggests that the trap states are formed by the removal of atoms from
the ends of the nanorods in the presence of chloroform. Mechanisms
for charge trapping at the nanoparticle/polymer interface are discussed
Investigation of Fluorescence Emission from CdSe Nanorods in PMMA and P3HT/PMMA Films
Complementary
fluorescence microscopy and ultrafast transient absorption
spectroscopy measurements spanning a range of time scales from seconds
to femtoseconds probe the interfacial dynamics of charge carriers
in CdSe nanorod/polymer blends. Together, these very different techniques
provide new information about the origin and dynamics of below-band-edge
emission from CdSe nanorods in CdSe/PMMA and CdSe/P3HT/PMMA films
[PMMA = polyÂ(methyl methacrylate); P3HT = polyÂ(3-hexylthiophene)].
Emission below the band edge of the CdSe nanorods is associated with
surface defects (traps) at the nanoparticle/polymer interface, where
conduction band electrons radiatively relax to the intraband defect
sites. The fluorescence microscopy experiments simultaneously monitor
both the trap emission and the band edge emission from single nanoparticles,
and reveal that the two emission channels are distinct. Transitions
between the two emissive states occur on time scales longer than ∼20
ms, and always involve an intermediate dark state in which no emission
is observed. The presence of P3HT increases the relative band edge
emission intensity and reduces the fluorescence intermittency (blinking)
of both emissive states. The ultrafast transient absorption experiments
monitor the evolution of a stimulated emission band below the CdSe
band edge following excitation of P3HT. The measurements reveal ultrafast
electron transfer from photoexcited P3HT to the CdSe nanorods within
the instrument response time of approximately 140 fs, and confirm
that there is strong coupling between the nanorods and P3HT in these
dilute blends. Analysis of separate CdSe nanorod etching experiments
suggests that the trap states are formed by the removal of atoms from
the ends of the nanorods in the presence of chloroform. Mechanisms
for charge trapping at the nanoparticle/polymer interface are discussed
Exciton Dynamics in MoS<sub>2</sub>‑Pentacene and WSe<sub>2</sub>‑Pentacene Heterojunctions
We measured the exciton dynamics in van der Waals heterojunctions
of transition metal dichalcogenides (TMDCs) and organic semiconductors
(OSs). TMDCs and OSs are semiconducting materials with rich and highly
diverse optical and electronic properties. Their heterostructures,
exhibiting van der Waals bonding at their interfaces, can be utilized
in the field of optoelectronics and photovoltaics. Two types of heterojunctions,
MoS2-pentacene and WSe2-pentacene, were prepared
by layer transfer of 20 nm pentacene thin films as well as MoS2 and WSe2 monolayer crystals onto Au surfaces.
The samples were studied by means of transient absorption spectroscopy
in the reflectance mode. We found that A-exciton decay by hole transfer
from MoS2 to pentacene occurs with a characteristic time
of 21 ± 3 ps. This is slow compared to previously reported hole
transfer times of 6.7 ps in MoS2-pentacene junctions formed
by vapor deposition of pentacene molecules onto MoS2 on
SiO2. The B-exciton decay in WSe2 shows faster
hole transfer rates for WSe2-pentacene heterojunctions,
with a characteristic time of 7 ± 1 ps. The A-exciton in WSe2 also decays faster due to the presence of a pentacene overlayer;
however, fitting the decay traces did not allow for the unambiguous
assignment of the associated decay time. Our work provides important
insights into excitonic dynamics in the growing field of TMDC-OS heterojunctions