7 research outputs found
Hydrogen Generation from Hydrolysis and Methanolysis of Guanidinium Borohydride
Metal-catalyzed hydrolysis and methanolysis of guanidinium
borohydride
(CÂ(NH<sub>2</sub>)<sub>3</sub>BH<sub>4</sub> or GBH) for hydrogen
generation are reported. GBH is comparatively stable in water with
only 0.3 equiv of H<sub>2</sub> liberated in 24 h at 25 °C while
it reacts vigorously with methanol, releasing more than 3.2 equiv
of H<sub>2</sub> within only 17 min. Even at 0 °C, there was
still nearly 2.0 equiv of H<sub>2</sub> released after 2 h, but no
H<sub>2</sub> liberation was observed for hydrolysis under the same
conditions. Various metal chlorides were adopted to enhance the reaction
kinetics of the hydrolysis and methanolysis, of which CoCl<sub>2</sub> exhibits the highest activity in both cases. With the addition of
2.0 mol % CoCl<sub>2</sub> at 25 °C, the methanolysis of GBH
could generate 4 equiv of H<sub>2</sub> within 10 min with a maximum
hydrogen generation rate of 9961.5 mL·min<sup><b>–</b>1</sup>·g<sup><b>–</b>1</sup> while only 1.8 equiv
of H<sub>2</sub> was obtained under the same conditions at a maximum
hydrogen generation rate of 692.3 mL·min<sup><b>–</b>1</sup>·g<sup><b>–</b>1</sup> for hydrolysis. Compared
with hydrolysis, methanolysis of GBH possesses much faster reaction
kinetics, rendering it an advantage for hydrogen generation, especially
at subzero areas. It was proposed that the faster reaction kinetics
of methanolysis of BH<sub>4</sub><sup>–</sup> containing compounds
is ascribed to the more electron donating methoxy group than that
of hydroxyl group. Moreover, a comparison between hydrolysis and methanolysis
of GBH indicates that the loss of the first H from BH<sub>4</sub><sup>–</sup> controls the hydrolysis kinetics instead of the cleavage
of the O–H bond
Vertically Aligned Nanocomposite BaTiO<sub>3</sub>:YMnO<sub>3</sub> Thin Films with Room Temperature Multiferroic Properties toward Nanoscale Memory Devices
Self-assembled epitaxial
BaTiO<sub>3</sub>:YMnO<sub>3</sub> (BTO:YMO)
vertically aligned nanocomposite thin films have been fabricated on
SrTiO<sub>3</sub> (001) substrates using pulsed-laser deposition.
A room temperature multiferroic response has been demonstrated in
the thin films. Enormous strain has been generated in both phases
(e.g., 1.4% compressive strain in BTO and 6.8% tensile strain in YMO
out-of-plane) because of the large lattice mismatch. By tuning the
deposition frequency, the microstructure and strain of the nanocomposite
films are tailored, which leads to the property tuning in the nanocomposite
films. It is found that strain plays an important role on the magnetic
ordering of YMO and thus results in the room temperature ferromagnetic
response. Combined with the ferroelectric response in the BTO:YMO
nanocomposite thin films, a new room temperature multiferroic two-phase
nanocomposite has been demonstrated. The room temperature magnetoelectric
coupling has been demonstrated for this new system. Overall, the BTO:YMO
thin film presents promising applications in sensors, data storage,
and memory devices
Vertically Aligned Nanocomposite BaTiO<sub>3</sub>:YMnO<sub>3</sub> Thin Films with Room Temperature Multiferroic Properties toward Nanoscale Memory Devices
Self-assembled epitaxial
BaTiO<sub>3</sub>:YMnO<sub>3</sub> (BTO:YMO)
vertically aligned nanocomposite thin films have been fabricated on
SrTiO<sub>3</sub> (001) substrates using pulsed-laser deposition.
A room temperature multiferroic response has been demonstrated in
the thin films. Enormous strain has been generated in both phases
(e.g., 1.4% compressive strain in BTO and 6.8% tensile strain in YMO
out-of-plane) because of the large lattice mismatch. By tuning the
deposition frequency, the microstructure and strain of the nanocomposite
films are tailored, which leads to the property tuning in the nanocomposite
films. It is found that strain plays an important role on the magnetic
ordering of YMO and thus results in the room temperature ferromagnetic
response. Combined with the ferroelectric response in the BTO:YMO
nanocomposite thin films, a new room temperature multiferroic two-phase
nanocomposite has been demonstrated. The room temperature magnetoelectric
coupling has been demonstrated for this new system. Overall, the BTO:YMO
thin film presents promising applications in sensors, data storage,
and memory devices
Continuous Tuning of Phase Transition Temperature in VO<sub>2</sub> Thin Films on <i>c</i>‑Cut Sapphire Substrates via Strain Variation
Vanadium dioxide
(VO<sub>2</sub>) thin films with controlled thicknesses
are deposited on <i>c</i>-cut sapphire substrates with Al-doped
ZnO (AZO) buffer layers by pulsed laser deposition. The surface roughness
of AZO buffer layers is varied by controlling oxygen pressure during
growth. The strain in the VO<sub>2</sub> lattice is found to be dependent
on the VO<sub>2</sub> thickness and the VO<sub>2</sub>/AZO interface
roughness. The semiconductor-to-metal transition (SMT) properties
of VO<sub>2</sub> thin films are characterized and the transition
temperature (<i>T</i><sub>c</sub>) is successfully tuned
by the VO<sub>2</sub> thickness as well as the VO<sub>2</sub>/AZO
interface roughness. It shows that the <i>T</i><sub>c</sub> of VO<sub>2</sub> decreases with the decrease of film thickness
or VO<sub>2</sub>/AZO interface roughness. Other SMT properties of
the VO<sub>2</sub> films are maintained during the <i>T</i><sub>c</sub> tuning. The results suggest that the strain tuning induced
by AZO buffer provides an effective approach for tuning <i>T</i><sub>c</sub> of VO<sub>2</sub> continuously
Strain and Interface Effects in a Novel Bismuth-Based Self-Assembled Supercell Structure
Bi<sub>2</sub>FeMnO<sub>6</sub> (BFMO)
thin films with both conventional pseudocubic structure and novel
supercell structure have been grown on SrTiO<sub>3</sub> (001) substrates
with different thicknesses of CeO<sub>2</sub> buffer layers (ranging
from 6.7 to 50.0 nm) using pulsed laser deposition. The correlation
between the thickness of the CeO<sub>2</sub> buffer layer and the
structure of the BFMO films shows that the CeO<sub>2</sub> buffer
layer, as thin as 6.7 nm, is sufficient in triggering the novel BFMO
supercell structure. This may be ascribed to the interfacial strain
between the BFMO supercell structure and the CeO<sub>2</sub> buffer
layer which also serves as a seed layer. The buffer layer thickness
is found to be critical to control the microstructure and magnetism
of the formed BFMO supercell structures. Thin seed layers can produce
a smoother interface between the BFMO film and the CeO<sub>2</sub> buffer layer, and therefore better ferrimagnetic properties. Our
results have demonstrated that strain and interface could be utilized
to generate novel thin film structures and to tune the functionalities
of thin films
Self-Assembled Magnetic Metallic Nanopillars in Ceramic Matrix with Anisotropic Magnetic and Electrical Transport Properties
Ordered
arrays of metallic nanopillars embedded in a ceramic matrix have recently
attracted considerable interest for their multifunctionality in advanced
devices. A number of hurdles need to be overcome for achieving practical
devices, including selections of metal–ceramic combination,
creation of tunable and ordered structure, and control of strain state.
In this article, we demonstrate major advances to create such a fine
nanoscale structure, i.e., epitaxial self-assembled vertically aligned
metal–ceramic composite, in one-step growth using pulsed laser
deposition. Tunable diameter and spacing of the nanopillars can be
achieved by controlling the growth parameters such as deposition temperature.
The magnetic metal–ceramic composite thin films demonstrate
uniaxial anisotropic magnetic properties and enhanced coercivity compared
to that of bulk metal. The system also presents unique anisotropic
electrical transport properties under in-plane and out-of-plane directions.
This work paves a new avenue to fabricate epitaxial metal–ceramic
nanocomposites, which can simulate broader future explorations in
nanocomposites with novel magnetic, optical, electrical, and catalytical
properties
Novel Layered Supercell Structure from Bi<sub>2</sub>AlMnO<sub>6</sub> for Multifunctionalities
Layered
materials, e.g., graphene and transition metal (di)Âchalcogenides,
holding great promises in nanoscale device applications have been
extensively studied in fundamental chemistry, solid state physics
and materials research areas. In parallel, layered oxides (e.g., Aurivillius
and Ruddlesden–Popper phases) present an attractive class of
materials both because of their rich physics behind and potential
device applications. In this work, we report a novel layered oxide
material with self-assembled layered supercell structure consisting
of two mismatch-layered sublattices of [Bi<sub>3</sub>O<sub>3+δ</sub>] and [MO<sub>2</sub>]<sub>1.84</sub> (M = Al/Mn, simply named BAMO),
i.e., alternative layered stacking of two mutually incommensurate
sublattices made of a three-layer-thick Bi–O slab and a one-layer-thick
Al/Mn–O octahedra slab in the out-of-plane direction. Strong
room-temperature ferromagnetic and piezoelectric responses as well
as anisotropic optical property have been demonstrated with great
potentials in various device applications. The realization of the
novel BAMO layered supercell structure in this work has paved an avenue
toward exploring and designing new materials with multifunctionalities