96 research outputs found
Crystalline–Crystalline Phase Transformation in Two-Dimensional In<sub>2</sub>Se<sub>3</sub> Thin Layers
We report, for the first time, the
fabrication of single-crystal
In<sub>2</sub>Se<sub>3</sub> thin layers using mechanical exfoliation
and studies of crystalline–crystalline (α → β)
phase transformations as well as the corresponding changes of the
electrical properties in these thin layers. Particularly, using electron
microscopy and correlative in situ micro-Raman and electrical measurements,
we show that, in contrast to bulk single crystals, the β phase
can persist in single-crystal thin layers at room temperature (RT).
The single-crystal nature of the layers before and after the phase
transition allows for unambiguous determination of changes in the
electrical resistivity. Specifically, the β phase has an electrical
resistivity about 1–2 orders of magnitude lower than the α
phase. Furthermore, we find that the temperature of the α →
β phase transformation increases by as much as 130 K with the
layer thickness decreasing from ∼87 nm to ∼4 nm. These
single-crystal thin layers are ideal for studying the scaling behavior
of the phase transformations and associated changes of the electrical
properties. For these In<sub>2</sub>Se<sub>3</sub> thin layers, the
accessibility of the β phase at RT, with distinct electrical
properties than the α phase, provides the basis for multilevel
phase-change memories in a single material system
Quantitative Heat Dissipation Characteristics in Current-Carrying GaN Nanowires Probed by Combining Scanning Thermal Microscopy and Spatially Resolved Raman Spectroscopy
Using an approach combining scanning thermal microscopy (SThM) and spatially revolved Raman spectroscopy, we have investigated quantitatively the heat dissipation characteristics in substrate-supported and suspended (with asymmetric type of contacts) current-carrying GaN nanowires with diameters of ∼40−60 nm, where the phonon confinement is expected to play an important role in thermal transport. In particular, this approach allows direct measurements of nanowire−substrate/electrode interface thermal resistances and the nanowire thermal conductivity. On the basis of these results, the nanowire−substrate thermal transfer was suggested to be the main heat dissipation route, counting for ∼80−93% of the total dissipated heat, whereas the nanowire−electrode interface plays a minor role. The relative significance of nanowire-substrate/electrode interfaces in dissipating heat was further demonstrated in suspended nanowire devices. The measured nanowire thermal conductivity (∼40−60 W/mK) is lower than that in bulk GaN, possibly due to the phonon confinement and boundary scattering effects. Besides providing quantitative insight into heat dissipation characteristics, our results also reveal aspects, particularly the topography-related thermal signals and the relative significance of various tip−sample thermal transfer processes, that are important to advancing the applications of SThM technique in nanoscale thermal characterizations
Electronically Driven Amorphization in Phase-Change In<sub>2</sub>Se<sub>3</sub> Nanowires
We show that the amorphization process in phase-change
In<sub>2</sub>Se<sub>3</sub> nanowires grown by chemical vapor deposition
can be
driven by electronic effects and does <i>not</i> require
the conventional thermal melt-quench process. In particular, using
transmission electron microscopy, in situ single-nanowire Raman spectroscopy,
scanning Kelvin probe microscopy, and finite-element simulations,
we demonstrate that the electronic amorphization can be achieved under
optical excitations at temperatures far below the thermal melting
point. The mechanism of this electronic amorphization is likely related
to the presence of atomic bonds with different strengths in the crystalline
phase In<sub>2</sub>Se<sub>3</sub> and the weakening of the weaker
bonds by nonequilibrium electrons. Our findings suggest that In<sub>2</sub>Se<sub>3</sub> is a promising candidate for phase-change memory
applications, with potential advantages including energy-efficient
memory switching due to the electronic amorphization process and highly
stable data storage as a result of a high melting point compared to
Ge/Sb–Te alloys. On a more general level, these results indicate
the need to take into account the electronic effects in modeling and
understanding the phase transition processes in phase-change memories
Synthesis and Ultrafast Carrier Dynamics of Single-Crystal Two-Dimensional CuInSe<sub>2</sub> Nanosheets
We
report, for the first time, the synthesis of single-crystal
two-dimensional (2D) CuInSe<sub>2</sub> nanosheets and the studies
of ultrafast carrier dynamics and transport in this 2D material. Particularly,
single-crystal 2D CuInSe<sub>2</sub> with various thicknesses in the
nanometer regime were fabricated by a solid-state chemical reaction
between Cu and single-crystal exfoliated In<sub>2</sub>Se<sub>3</sub> nanosheets. Characteristics of transient optical reflectivity, obtained
from femtosecond optical pump–probe measurements on single
CuInSe<sub>2</sub> nanosheets, suggest that the hot carrier cooling
process dominates the carrier dynamics within a few picoseconds following
the optical excitation. Spatially resolved pump–probe measurements,
coupled to simple model calculations, were used to obtain the ambipolar
hot carrier diffusion coefficient in single nanosheets. The dependence
of the hot carrier diffusion coefficient on the nanosheet thickness
provides insight into the limiting mechanisms of hot carrier transport
and can be used to gauge the possibility of efficient hot carrier
collection in nanostructured CuInSe<sub>2</sub> solar cells
Imaging Charged Exciton Localization in van der Waals WSe<sub>2</sub>/MoSe<sub>2</sub> Heterobilayers
Exciton
localization in transition-metal dichalcogenide monolayers
is behind a variety of interesting phenomena and applications, including
broad-spectrum solar cells and single-photon emissions. Strain fields
at the periphery of topographically distinct features such as nanoscopic
bubbles were recently associated with localized charge-neutral excitons.
Here, we use tip-enhanced photoluminescence (PL) to visualize excitons
in WSe2/MoSe2 heterobilayers (HBL). We find
strong optical emission from charged excitons, particularly positively
charged trions, in HBL supported by interlayer charge transfer. Our
results reveal strong trion confinement, with a localization length
scale comparable to the trion size, at the apex region inside individual
nanoscopic bubbles. Nano-PL mapping also shows sub-10-nm spatial variations
in the localized trion emission spectra, which stem from atomic-scale
potential energy fluctuations. These findings demonstrate the possibility
of confining charged exciton complexes that are electrically tunable,
opening up further opportunities to probe many-body exciton physics
and to explore additional possible sites for strong exciton localization
that can lead to quantum emission
Diameter-Dependent Surface Photovoltage and Surface State Density in Single Semiconductor Nanowires
Based on single-nanowire surface photovoltage measurements
and
finite-element electrostatic simulations, we determine the surface
state density, <i>N</i><sub>s</sub>, in individual n-type
ZnO nanowires as a function of nanowire diameter. In general, <i>N</i><sub>s</sub> increases as the diameter decreases. This
identifies an important origin of the recently reported diameter dependence
of the surface recombination velocity, which has been commonly considered
to be independent of the diameter. Furthermore, through the determination
of the surface carrier lifetime, we suggest that the diameter dependence
of the surface state density accounts for the rather abrupt transition
from bulk-limited to surface-limited carrier transport over a narrow
nanowire diameter regime (∼30–40 nm). These findings
are supported by the comparison between bulk-limited and surface-dependent
minority carrier diffusion lengths measured at various diameters
Multivariate analysis of RFS in classical PTC patients.
Multivariate analysis of RFS in classical PTC patients.</p
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