8 research outputs found
From GaN to ZnGa<sub>2</sub>O<sub>4</sub> through a Low-Temperature Process: Nanotube and Heterostructure Arrays
We
demonstrate a method to synthesize GaN–ZnGa<sub>2</sub>O<sub>4</sub> core–shell nanowire and ZnGa<sub>2</sub>O<sub>4</sub> nanotube arrays by a low-temperature hydrothermal process
using GaN nanowires as templates. Transmission electron microscopy
and X-ray photoelectron spectroscopy results show that a ZnGa<sub>2</sub>O<sub>4</sub> shell forms on the surface of GaN nanowires
and that the shell thickness is controlled by the time of the hydrothermal
process and thus the concentration of Zn ions in the solution. Furthermore,
ZnGa<sub>2</sub>O<sub>4</sub> nanotube arrays were obtained by depleting
the GaN core from GaN–ZnGa<sub>2</sub>O<sub>4</sub> core–shell
nanowire arrays during the reaction and subsequent etching with HCl.
The GaN–ZnGa<sub>2</sub>O<sub>4</sub> core–shell nanowires
exhibit photoluminescence peaks centered at 2.60 and 2.90 eV attributed
to the ZnGa<sub>2</sub>O<sub>4</sub> shell, as well as peaks centered
at 3.35 and 3.50 eV corresponding to the GaN core. We also demonstrate
the synthesis of GaN–ZnGa<sub>2</sub>O<sub>4</sub> heterojunction
nanowires by a selective formation process as a simple route toward
development of heterojunction nanodevices for optoelectronic applications
Dynamic Visualization of Axial p–n Junctions in Single Gallium Nitride Nanorods under Electrical Bias
We demonstrate a direct visualization method based on secondary electron (SE) imaging in scanning electron microscopy for mapping electrostatic potentials across axial semiconductor nanorod p–n junctions. It is found that the SE doping contrast can be directly related to the spatial distribution of electrostatic potential across the axial nanorod p–n junction. In contrast to the conventional SE doping contrast achieved for planar p–n junctions, the quasi-one-dimensional geometry of nanorods allows for high-resolution, versatile SE imaging under high accelerating voltage, long working distance conditions. Furthermore, we are able to delineate the electric field profiles across the axial nanorod p–n junction as well as depletion widths at different reverse biases. By using standard p<i>–</i>n junction theory and secondary ion mass spectroscopy, the carrier concentrations of p- and n-regions can be further extracted from the depletion widths under reverse biasing conditions. This direct imaging method enables determination of electrostatic potential variation of p–n junctions in semiconductor nanorod and nanowire devices with a spatial resolution better than 10 nm
The Growth and Optical Properties of ZnO Nanowalls
Nanowalls are novel nanostructures whose networked morphology holds potential for applications such as solar cells and gas sensors. The realization of such nanowall-based devices depends directly on a comprehensive understanding of the nanowall growth, namely, its competition with nanowire growth and the role of seed particles. We induced a morphological evolution from nanowires to nanowalls by increasing source flux during vapor transport and condensation growth. Nanowall growth kinetics indicates that their morphological dominance was driven by a time-dependent curvature of the nanowall growth facet. Nanowalls have excellent crystalline quality and strong near-band-edge luminescence and were found to grow by a combination of Au- and nonassisted mechanisms, resulting in Au nanoparticles within 300 nm of the substrate whose positions were associated with the origin of green luminescence. These results imply that the growth mechanism causes nanoscale structural variations, which in turn locally affect the optical properties of nanowalls
Optoelectronic Properties of Single-Crystalline Zn<sub>2</sub>GeO<sub>4</sub> Nanowires
In
this work, Zn<sub>2</sub>GeO<sub>4</sub> nanowires (NWs) were
successfully synthesized on Si(100) substrates through carbon thermal
reduction and a vapor–liquid–solid method. The NWs were
of around 100 nm diameter and high aspect ratio (AR > 150). High-resolution
transmission electron microscopy studies indicate that the NWs are
single-crystalline with [110] growth direction. Moreover, the atomic
resolution high-angle annular dark-field and bright-field images of
scanning transmission electron microscopy have distinguished the different
elements. They also further identified the structure of Zn<sub>2</sub>GeO<sub>4</sub> and located the positions of the elements. Additionally,
we have fabricated devices and measured the electrical properties
of a single NW. It is remarkable that individual Zn<sub>2</sub>GeO<sub>4</sub> NW devices exhibited excellent optoelectronic properties
with fast switching speed under 254 nm UV illuminations. Furthermore,
with short wavelength UV illumination, as we soaked Zn<sub>2</sub>GeO<sub>4</sub> NWs in methyl orange solution, the methyl orange
was degraded. Therefore, Zn<sub>2</sub>GeO<sub>4</sub> NWs have potential
applications in UV photodetectors and degradation of organic pollutants
Sequential Cation Exchange Generated Superlattice Nanowires Forming Multiple p–n Heterojunctions
Fabrication of superlattice nanowires (NWs) with precisely controlled segments normally requires sequential introduction of reagents to the growing wires at elevated temperatures and low pressure. Here we demonstrate the fabrication of superlattice NWs possessing multiple p–n heterojunctions by converting the initially formed CdS to Cu<sub>2</sub>S NWs first and then to segmented Cu<sub>2</sub>S–Ag<sub>2</sub>S NWs through sequential cation exchange at low temperatures. In the formation of Cu<sub>2</sub>S NWs, twin boundaries generated along the NWs act as the preferred sites to initiate the nucleation and growth of Ag<sub>2</sub>S segments. Varying the immersion time of Cu<sub>2</sub>S NWs in a AgNO<sub>3</sub> solution controls the Ag<sub>2</sub>S segment length. Adjacent Cu<sub>2</sub>S and Ag<sub>2</sub>S segments in a NW were found to display the typical electrical behavior of a p–n junction
All-Color Plasmonic Nanolasers with Ultralow Thresholds: Autotuning Mechanism for Single-Mode Lasing
We report on the first demonstration
of broadband tunable, single-mode
plasmonic nanolasers (spasers) emitting in the full visible spectrum.
These nanolasers are based on a single metal–oxide–semiconductor
nanostructure platform comprising of InGaN/GaN semiconductor nanorods
supported on an Al<sub>2</sub>O<sub>3</sub>-capped epitaxial Ag film.
In particular, all-color lasing in subdiffraction plasmonic resonators
is achieved via a novel mechanism based on a property of weak size
dependence inherent in spasers. Moreover, we have successfully reduced
the continuous-wave (CW) lasing thresholds to ultrasmall values for
all three primary colors and have clearly demonstrated the possibility
of “thresholdless” lasing for the blue plasmonic nanolaser
Complete Replacement of Metal in Metal Oxide Nanowires via Atomic Diffusion: In/ZnO Case Study
Atomic diffusion is a fundamental
process that dictates material
science and engineering. Direct visualization of atomic diffusion
process in ultrahigh vacuum in situ TEM could comprehend the fundamental
information about metal–semiconductor interface dynamics, phase
transitions, and different nanostructure growth phenomenon. Here,
we demonstrate the in situ TEM observations of the complete replacement
of ZnO nanowire by indium with different growth directions. In situ
TEM analyses reveal that the diffusion processes strongly depend and
are dominated by the interface dynamics between indium and ZnO. The
diffusion exhibited a distinct ledge migration by surface diffusion
at [001]-ZnO while continuous migration with slight/no ledges by inner
diffusion at [100]-ZnO. The process is explained based on thermodynamic
evaluation and growth kinetics. The results present the potential
possibilities to completely replace metal-oxide semiconductors with
metal nanowires without oxidation and form crystalline metal nanowires
with precise epitaxial metal–semiconductor atomic interface.
Formation of such single crystalline metal nanowire without oxidation
by diffusion to the metal oxide is unique and is crucial in nanodevice
performances, which is rather challenging from a manufacturing perspective
of 1D nanodevices
Aqueous Synthesis of Concave Rh Nanotetrahedra with Defect-Rich Surfaces: Insights into Growth‑, Defect‑, and Plasmon-Enhanced Catalytic Energy Conversion
The control of morphology in the
synthesis of Rh nanocrystals can
be used to precisely tailor the electronic surface structure; this
in turn directly influences their performance in catalysis applications.
Many works have brought attention to the development of Rh nanostructures
with low-index surfaces, but limited effort has been devoted to the
study of high-index and surface defect-enriched nanocrystals as they
are not favored by thermodynamics because of the involvement of high-energy
surfaces and increased surface-to-volume ratios. In this work, we
demonstrate an aqueous synthesis of concave Rh nanotetrahedra (CTDs)
serving as efficient catalysts for energy conversion reactions. CTDs
are surface defect-rich structures that form through a slow growth
rate and follow the four-step model of metallic nanoparticle growth.
Via the tuning of the surfactant concentration, the morphology of
Rh CTDs evolved into highly excavated nanotetrahedra (HETDs) and twinned
nanoparticles (TWs). Unlike the CTD surfaces with abundant adatoms
and vacancies, HETDs and TWs have more regular surfaces with layered
terraces. Each nanocrystal type was evaluated for methanol electrooxidation
and hydrogen evolution from hydrolysis of ammonia borane, and the
CTDs significantly showed the best catalytic performance because of
defect enrichment, which benefits the surface reactivity of adsorbates.
In addition, both CTDs and HETDs have strong absorption near the visible
light region (382 and 396 nm), for which they show plasmon-enhanced
performance in photocatalytic hydrogen evolution under visible light
illumination. CTDs are more photoactive than HETDs, likely because
of more pronounced localized surface plasmon resonance hot spots.
This facile aqueous synthesis of large-surface-area, defect-rich Rh
nanotetrahedra is exciting for the fields of nanosynthesis and catalysis