6 research outputs found
Interfacial MetalāOxide Interactions in Resistive Switching Memories
Metal
oxides are commonly used as electrolytes for redox-based resistive
switching memories. In most cases, non-noble metals are directly deposited
as ohmic electrodes. We demonstrate that irrespective of bulk thermodynamics
predictions an intermediate oxide film a few nanometers in thickness
is always formed at the metal/insulator interface, and this layer
significantly contributes to the development of reliable switching
characteristics. We have tested metal electrodes and metal oxides
mostly used for memristive devices, that is, Ta, Hf, and Ti and Ta<sub>2</sub>O<sub>5</sub>, HfO<sub>2</sub>, and SiO<sub>2</sub>. Intermediate
oxide layers are always formed at the interfaces, whereas only the
rate of the electrode oxidation depends on the oxygen affinity of
the metal and the chemical stability of the oxide matrix. Device failure
is associated with complete transition of short-range order to a more
disordered main matrix structure
Understanding the Role of Single Molecular ZnS Precursors in the Synthesis of In(Zn)P/ZnS Nanocrystals
Environmentally friendly nanocrystals
(NCs) such as InP are in
demand for various applications, such as biomedical labeling, solar
cells, sensors, and light-emitting diodes (LEDs). To fulfill their
potential applications, the synthesis of such high-quality āgreenā
InP NCs required further improvement so as to achieve better stability,
higher brightness NCs, and also to have a more robust synthesis route.
The present study addresses our efforts on the synthesis of high-quality
InĀ(Zn)ĀP/ZnS coreāshell NCs using an air- and moisture-stable
ZnS single molecular precursor (SMP) and InĀ(Zn)P cores. The SMP method
has recently emerged as a promising route for the surface overcoating
of NCs due to its simplicity, high reproducibility, low reaction temperature,
and flexibility in controlling the reaction. The synthesis involved
heating the InĀ(Zn)P core solution and ZnĀ(S<sub>2</sub>CNR<sub>2</sub>) (where R = methyl, ethyl, butyl, or benzyl and referred to as ZDMT,
ZDET, ZDBT, or ZDBzT, respectively) in oleylamine (OLA) to 90ā250
Ā°C for 0.5ā2.5 h. In this work, we systematically studied
the influence of different SMP end groups, the complex formation and
stability between the SMP and oleylamine (OLA), the reaction temperature,
and the amount of SMP on the synthesis of high-quality InĀ(Zn)ĀP/ZnS
NCs. We found that thiocarbamate end groups are an important factor
contributing to the low-temperature growth of high-quality InĀ(Zn)ĀP/ZnS
NCs, as the end groups affect the polarity of the molecules and result
in a different steric arrangement. We found that use of SMP with bulky
end groups (ZDBzT) results in nanocrystals with higher photoluminescence
quantum yield (PL QY) and better dispersibility than those synthesized
with SMPs with the shorter alkyl chain groups (ZDMT, ZDET, or ZDBT).
At the optimal conditions, the PL QY of red emission InĀ(Zn)ĀP/ZnS NCs
is 55 Ā± 4%, which is one of the highest values reported. On the
basis of structural (XAS, XPS, XRD, TEM) and optical characterization,
we propose a mechanism for the growth of a ZnS shell on an InĀ(Zn)ĀP
core
Structural Analyses of Phase Stability in Amorphous and Partially Crystallized Ge-Rich GeTe Films Prepared by Atomic Layer Deposition
The local bonding
structures of Ge<i><sub>x</sub></i>Te<sub>1ā<i>x</i></sub> (<i>x</i> = 0.5, 0.6, and 0.7) films prepared
through atomic layer deposition (ALD) with GeĀ(NĀ(SiĀ(CH<sub>3</sub>)<sub>3</sub>)<sub>2</sub>)<sub>2</sub> and ((CH<sub>3</sub>)<sub>3</sub>Si)<sub>2</sub>Te precursors were investigated using Ge K-edge X-ray
absorption spectroscopy (XAS). The results of the X-ray absorption
fine structure analyses show that for all of the compositions, the
as-grown films were amorphous with a tetrahedral Ge coordination of
a mixture of GeāTe and GeāGe bonds but without any signature
of GeāGeTe decomposition. The compositional evolution in the
valence band electronic structures probed through X-ray photoelectron
spectroscopy suggests a substantial chemical influence of additional
Ge on the nonstoichiometric GeTe. This implies that the ALD process
can stabilize Ge-abundant bonding networks like āTeāGeāGeāTeā
in amorphous GeTe. Meanwhile, the XAS results on the Ge-rich films
that had undergone post-deposition annealing at 350 Ā°C show that
the parts of the crystalline Ge-rich GeTe became separated into Ge
crystallites and rhombohedral GeTe in accordance with the bulk phase
diagram, whereas the disordered GeTe domains still remained, consistent
with the observations of transmission electron microscopy and Raman
spectroscopy. Therefore, amorphousness in GeTe may be essential for
the nonsegregated Ge-rich phases and the low growth temperature of
the ALD enables the achievement of the structurally metastable phases
Conformal Formation of (GeTe<sub>2</sub>)<sub>(1ā<i>x</i>)</sub>(Sb<sub>2</sub>Te<sub>3</sub>)<sub><i>x</i></sub> Layers by Atomic Layer Deposition for Nanoscale Phase Change Memories
Phase change random access memory appears to be the strongest
candidate
for next-generation high density nonvolatile memory. The fabrication
of ultrahigh density phase change memory (ā«1 Gb) depends heavily
on the thin film growth technique for the phase changing chalcogenide
material, most typically containing Ge, Sb and Te (GeāSbāTe).
Atomic layer deposition (ALD) at low temperatures is the most preferred
growth method for depositing such complex materials over surfaces
possessing extreme topology. In this study, [(CH<sub>3</sub>)<sub>3</sub>Si]<sub>2</sub>Te and stable alkoxy-Ge (GeĀ(OCH<sub>3</sub>)<sub>4</sub>) and alkoxy-Sb (SbĀ(OC<sub>2</sub>H<sub>5</sub>)<sub>3</sub>) metalāorganic precursors were used to deposit various
layers with compositions lying on the GeTe<sub>2</sub>āSb<sub>2</sub>Te<sub>3</sub> tie lines at a substrate temperature as low
as 70 Ā°C using a thermal ALD process. The adsorption of Ge precursor
was proven to be a physisorption type while other precursors showed
a chemisorption behavior. However, the adsorption of Ge precursor
was still self-regulated, and the facile ALD of the pseudobinary solid
solutions with composition (GeTe<sub>2</sub>)<sub>(1āx)</sub>(Sb<sub>2</sub>Te<sub>3</sub>)<sub><i>x</i></sub> were
achieved. This chemistry-specific ALD process was quite robust against
process variations, allowing highly conformal, smooth, and reproducible
film growth over a contact hole structure with an extreme geometry.
The detailed ALD behavior of binary compounds and incorporation behaviors
of the binary compounds in pseudobinary solid solutions were studied
in detail. This new composition material showed reliable phase change
and accompanying resistance switching behavior, which were slightly
better than the standard Ge<sub>2</sub>Sb<sub>2</sub>Te<sub>5</sub> material in the nanoscale. The local chemical environment was similar
to that of conventional Ge<sub>2</sub>Sb<sub>2</sub>Te<sub>5</sub> materials
Comparison of the Atomic Layer Deposition of Tantalum Oxide Thin Films Using Ta(N<sup><i>t</i></sup>Bu)(NEt<sub>2</sub>)<sub>3</sub>, Ta(N<sup><i>t</i></sup>Bu)(NEt<sub>2</sub>)<sub>2</sub>Cp, and H<sub>2</sub>O
The growth characteristics
of Ta<sub>2</sub>O<sub>5</sub> thin films by atomic layer deposition
(ALD) were examined using TaĀ(N<sup><i>t</i></sup>Bu)Ā(NEt<sub>2</sub>)<sub>3</sub> (TBTDET) and TaĀ(N<sup><i>t</i></sup>Bu)Ā(NEt<sub>2</sub>)<sub>2</sub>Cp (TBDETCp) as Ta-precursors, where <sup><i>t</i></sup>Bu, Et, and Cp represent <i>tert</i>-butyl, ethyl, and cyclopentadienyl groups, respectively, along with
water vapor as oxygen source. The grown Ta<sub>2</sub>O<sub>5</sub> films were amorphous with very smooth surface morphology for both
the Ta-precursors. The saturated ALD growth rates of Ta<sub>2</sub>O<sub>5</sub> films were 0.77 Ć
cycle<sup>ā1</sup> at
250 Ā°C and 0.67 Ć
cycle<sup>ā1</sup> at 300 Ā°C
using TBTDET and TBDETCp precursors, respectively. The thermal decomposition
of the amido ligand (NEt<sub>2</sub>) limited the ALD process temperature
below 275 Ā°C for TBTDET precursor. However, the ALD temperature
window could be extended up to 325 Ā°C due to a strong TaāCp
bond for the TBDETCp precursor. Because of the improved thermal stability
of TBDETCp precursor, excellent nonuniformity of ā¼2% in 200
mm wafer could be achieved with a step coverage of ā¼90% in
a deep hole structure (aspect ratio 5:1) which is promising for 3-dimensional
architecture to form high density memories. Nonetheless, a rather
high concentration (ā¼7 at. %) of carbon impurities was incorporated
into the Ta<sub>2</sub>O<sub>5</sub> film using TBDETCp, which was
possibly due to readsorption of dissociated ligands as small organic
molecules in the growth of Ta<sub>2</sub>O<sub>5</sub> film by ALD.
Despite the presence of high carbon concentration which might be an
origin of large leakage current under electric fields, the Ta<sub>2</sub>O<sub>5</sub> film using TBDETCp showed a promising resistive
switching performance with an endurance cycle as high as ā¼17āÆ500
for resistance switching random access memory application. The optical
refractive index of the deposited Ta<sub>2</sub>O<sub>5</sub> films
was 2.1ā2.2 at 632.8 nm using both the Ta-precursors, and indirect
optical band gap was estimated to be ā¼4.1 eV for both the cases
Giant Photoresponse in Quantized SrRuO<sub>3</sub> Monolayer at Oxide Interfaces
The
photoelectric effect in semiconductors is the main mechanism
for most modern optoelectronic devices, in which the adequate bandgap
plays the key role for acquiring high photoresponse. Among numerous
material categories applied in this field, the complex oxides exhibit
great possibilities because they present a wide distribution of band
gaps for absorbing light with any wavelength. Their physical properties
and lattice structures are always strongly coupled and sensitive to
light illumination. Moreover, the confinement of dimensionality of
the complex oxides in the heterostructures can provide more diversities
in designing and modulating the band structures. On the basis of this
perspective, we have chosen itinerary ferromagnetic SrRuO<sub>3</sub> as the model material, and fabricated it in one-unit-cell thickness
in order to open a small band gap for effective utilization of visible
light. By inserting this SrRuO<sub>3</sub> monolayer at the interface
of the well-developed two-dimensional electron gas system (LaAlO<sub>3</sub>/SrTiO<sub>3</sub>), the resistance of the monolayer can be
further revealed. In addition, a giant enhancement (>300%) of photoresponse
under illumination of visible light with power density of 500 mW/cm<sup>2</sup> is also observed. Such can be ascribed to the further modulation
of band structure of the SrRuO<sub>3</sub> monolayer under the illumination,
confirmed by cross-section scanning tunneling microscopy (XSTM). Therefore,
this study demonstrates a simple route to design and explore the potential
low dimensional oxide materials for future optoelectronic devices