14 research outputs found
Effects of Alkali Cations and Sulfate/Chloride Anions on the Flux Growth of {001}-Faceted β‑Li<sub>2</sub>TiO<sub>3</sub> Crystals
The β-Li<sub>2</sub>TiO<sub>3</sub> crystal is an important
material in several energy-related applications, and the control of
its morphology and exposed facets is an important issue. Herein, we
comprehensively studied the flux growth of β-Li<sub>2</sub>TiO<sub>3</sub> crystals under different conditions and demonstrated the
efficient anisotropic growth of {001}-faceted β-Li<sub>2</sub>TiO<sub>3</sub> single crystals from the Na<sub>2</sub>SO<sub>4</sub> flux. By examining the effects of the cation and anion in the alkali
metal salt-based flux, we found that Na<sub>2</sub>SO<sub>4</sub> flux
is best for growing large, faceted β-Li<sub>2</sub>TiO<sub>3</sub> crystals. In this flux at 1000 °C, the optimal solute concentration
is 20 mol % for growing large (∼15.0 μm in lateral size),
platy, and faceted β-Li<sub>2</sub>TiO<sub>3</sub> crystals.
Observations from varying the holding time and cooling rate indicated
that these crystals were anisotropically grown. Transmission electron
microscopy images with clear electron diffraction spots revealed that
the flux-grown platy β-Li<sub>2</sub>TiO<sub>3</sub> crystals
are single crystalline solids with the {001} plane being the dominant
facet. This anisotropic crystal growth could be attributed to the
concerted effects of the preferential attachment of sodium cations
on the {001} faces, and efficient dissolution of β-Li<sub>2</sub>TiO<sub>3</sub> crystals as well as the solvation of the resulting
O<sup>2–</sup> ions in the sulfate anion-based flux
Fabrication of La<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub> Crystals Using an Alkali-Metal Molybdate Flux Growth Method and Their Nitridability To Form LaTiO<sub>2</sub>N Crystals under a High-Temperature NH<sub>3</sub> Atmosphere
Flux
growth is a promising method that allows one to control over the crystalline
phase, crystal shape, crystal size, and crystal surface through the
selection of a suitable flux. In this work, lanthanum titanate (La<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub>) crystals with different morphologies
were grown using the Na<sub>2</sub>MoO<sub>4</sub>, K<sub>2</sub>MoO<sub>4</sub>, NaCl, and mixed NaCl + K<sub>2</sub>MoO<sub>4</sub> (molar
ratio = 3:7) fluxes, and their nitridability to form LaTiO<sub>2</sub>N crystals under a high-temperature NH<sub>3</sub> atmosphere was
also investigated. The effects of the solute concentration and cooling
rate on the growth of the La<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub> crystals were also studied. The X-ray diffraction results revealed
that the {100} plane was dominant in the La<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub> platelet crystals grown using the alkali-metal molybdate
fluxes. When the solute concentration was increased from 1 to 20 mol
%, the average size of the crystals decreased without considerable
alteration of the overall crystal morphology. The La<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub> crystals with the preferred ⟨010⟩
and ⟨001⟩ growth directions along the <i>b</i> and <i>c</i> axes were grown using the Na<sub>2</sub>MoO<sub>4</sub> and K<sub>2</sub>MoO<sub>4</sub> fluxes, respectively. Compared
to the Na<sub>2</sub>MoO<sub>4</sub> flux, the K<sub>2</sub>MoO<sub>4</sub> flux did not show a cooling-rate-dependent effect on the
growth of the La<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub> crystals.
It was found that conversion of the La<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub> crystals to the LaTiO<sub>2</sub>N crystals was strongly
dependent on the flux used to grow the precursor La<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub> crystals. That is, the La<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub> crystals grown using the K<sub>2</sub>MoO<sub>4</sub> and NaCl fluxes were nearly completely converted into the
LaTiO<sub>2</sub>N crystals, while conversion of the La<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub> crystals grown using the Na<sub>2</sub>MoO<sub>4</sub> and mixed NaCl + K<sub>2</sub>MoO<sub>4</sub> fluxes
to the LaTiO<sub>2</sub>N crystals seemed to be not completed yet
even after nitridation at 950 °C for 15 h using NH<sub>3</sub> because of the larger crystal size and the presence of unintentional
impurities (sodium and molybdenum from the flux) in the La<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub> crystal lattice. Nevertheless, the LaTiO<sub>2</sub>N crystals fabricated by nitriding the La<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub> crystals grown using the K<sub>2</sub>MoO<sub>4</sub> and NaCl fluxes should be suitable for direct solar water
splitting
Facile Morphological Modification of Ba<sub>5</sub>Nb<sub>4</sub>O<sub>15</sub> Crystals Using Chloride Flux and in Situ Growth Investigation
The
cation-deficient layered perovskite oxide Ba<sub>5</sub>Nb<sub>4</sub>O<sub>15</sub> is one of the functional materials that exhibits
a microwave-responsive dielectric property and an ultraviolet-active
photocatalytic property. Although systematic control of the morphology
of Ba<sub>5</sub>Nb<sub>4</sub>O<sub>15</sub> is beneficial for improving
these properties, synthesized Ba<sub>5</sub>Nb<sub>4</sub>O<sub>15</sub> usually has a plate-like shape owing to its crystal structure, with
a particle size less than 5 μm. For systematic morphological
control of Ba<sub>5</sub>Nb<sub>4</sub>O<sub>15</sub>, the crystal
growth was studied by using a chloride-based flux method. Idiomorphic
plate-like Ba<sub>5</sub>Nb<sub>4</sub>O<sub>15</sub> crystals up
to 50 μm in size and polyhedron ones ∼10 μm in
size were obtained using a BaCl<sub>2</sub> flux by changing the solute
concentration to 5–20 mol % and 50 mol %, respectively. The
growth of the Ba<sub>5</sub>Nb<sub>4</sub>O<sub>15</sub> crystals
was investigated by thermogravimetric and differential thermal analysis
and in situ X-ray diffraction analysis. These analyses revealed the
flux-growth manner of Ba<sub>5</sub>Nb<sub>4</sub>O<sub>15</sub> as
follows: (I) Ba<sub>5</sub>Nb<sub>4</sub>O<sub>15</sub> was formed
by a solid-state reaction above ∼650 °C. (II) After the
melting of BaCl<sub>2</sub> above ∼962 °C, the Ba<sub>5</sub>Nb<sub>4</sub>O<sub>15</sub> crystals became larger and assumed
idiomorphic shapes, indicating that they were somewhat dissolved in
the flux and that the crystal growth was promoted. Increasing the
holding time yielded an increased number of crystals larger than 28
μm. This indicates that Ostwald ripening effectively yields
Ba<sub>5</sub>Nb<sub>4</sub>O<sub>15</sub> crystals up to 50 μm
in size. Chloride fluxes with different alkaline or alkaline earth
cation fluxes did not produce such large crystals. It is assumed that
the common ion effect of Ba<sup>2+</sup> in the solute and flux provides
an effective reaction field to facilitate Ostwald ripening
Protonated Oxide, Nitrided, and Reoxidized K<sub>2</sub>La<sub>2</sub>Ti<sub>3</sub>O<sub>10</sub> Crystals: Visible-Light-Induced Photocatalytic Water Oxidation and Fabrication of Their Nanosheets
Protonated
lanthanum titanium oxide H<sub>2</sub>La<sub>2</sub>Ti<sub>3</sub>O<sub>10</sub> and oxynitride H<sub>2</sub>La<sub>2</sub>Ti<sub>3</sub>O<sub>10–3/2<i>x</i></sub>N<sub><i>x</i></sub> crystals were synthesized from the oxide, nitrided,
and reoxidized layered K<sub>2</sub>La<sub>2</sub>Ti<sub>3</sub>O<sub>10</sub> crystals prepared by solid-state reaction through proton
exchange. Here, we investigated the holding time of nitridation of
oxide K<sub>2</sub>La<sub>2</sub>Ti<sub>3</sub>O<sub>10</sub> crystals
influencing their crystal structure, shape, and absorption wavelength
and band gap energy. The XRD and SEM results confirmed that the crystal
structure and plate-like shape of the parent oxide were maintained
after nitridation at 800 °C for 10 h, and the color of crystals
was changed from white to dark green. However, no clear absorption
edges were observed in the UV–vis diffuse reflectance spectra
of the nitrided crystals due mainly to the reduced titanium species
(Ti<sup>3+</sup>), which act as the recombination center of the photogenerated
charge carriers. To decrease the amount of the reduced titanium species,
the nitrided crystals were further reoxidized at 400 °C for 6
h. After partial reoxidation, the absorption intensity in the longer
wavelength region was reduced, and the absorption edges appeared at
about 449–460 nm. The photocatalytic activity for the water
oxidation half-reaction was evaluated only for the protonated samples.
The protonated reoxidized K<sub>2</sub>La<sub>2</sub>Ti<sub>3</sub>O<sub>10</sub> crystals showed the O<sub>2</sub> evolution rate of
180 nmol·h<sup>–1</sup> (for the photocatalytic water
oxidation) under visible-light irradiation, and the unexpected photocatalytic
decomposition of N<sub>2</sub>O adsorbed onto the photocatalyst surfaces
was observed for the protonated oxide and protonated nitrided layered
K<sub>2</sub>La<sub>2</sub>Ti<sub>3</sub>O<sub>10</sub> crystals.
Furthermore, lanthanum titanium oxide [La<sub>2</sub>Ti<sub>3</sub>O<sub>10</sub>]<sup>2–</sup> and oxynitride [La<sub>2</sub>Ti<sub>3</sub>O<sub>10–3/2<i>x</i></sub>N<sub><i>x</i></sub>]<sup>2–</sup> nanosheets were successfully
fabricated by proton exchange and mechanical exfoliation (sonication)
of the oxide, nitrided, and reoxidized K<sub>2</sub>La<sub>2</sub>Ti<sub>3</sub>O<sub>10</sub> crystals. The TEM results revealed that
the lateral sizes of the fabricated nanosheets grown along the ⟨001⟩
direction are 270–620 nm. Apparently, the colloidal suspensions
of the fabricated nanosheets showed a Tyndall effect, implying their
good dispersion and stability for several weeks in water
Flux-Mediated Topochemical Growth of Platelet-Shaped Perovskite LiNbO<sub>3</sub> Single Crystals from Layered Potassium Niobate Crystals
Well-defined, platelet-shaped LiNbO<sub>3</sub> single crystals
were prepared by a flux-mediated topochemical reaction from platelet
K<sub>4</sub>Nb<sub>6</sub>O<sub>17</sub> crystals with a mixture
of LiNO<sub>3</sub> solute and alkali metal nitrate (LiNO<sub>3</sub>, NaNO<sub>3</sub>, and KNO<sub>3</sub>) fluxes at 600 °C. Crystallographic
structural characterizations revealed that the LiNbO<sub>3</sub> crystals
inherited the K<sub>4</sub>Nb<sub>6</sub>O<sub>17</sub> crystal shape
with well-developed {012} faces. The topochemical reaction in molten
KNO<sub>3</sub> promoted smooth surface formation, in contrast to
LiNO<sub>3</sub> and NaNO<sub>3</sub>, which formed rough surfaces.
We further found that the dissolution and deposition reaction occurs
repeatedly in the vicinity of the LiNbO<sub>3</sub> crystal and KNO<sub>3</sub> flux interface. It is considered that the KNO<sub>3</sub> flux hybridized with the LiNO<sub>3</sub> solute provides a moderate
solubility and dissolution rate suitable for crystal growth. We also
achieved reed-shaped LiNbO<sub>3</sub> crystal growth by applying
the same technique to the KNb<sub>3</sub>O<sub>8</sub> crystal template
Environmentally Friendly Flux Growth of High-Quality, Idiomorphic Li<sub>5</sub>La<sub>3</sub>Nb<sub>2</sub>O<sub>12</sub> Crystals
High-quality, idiomorphic, single-phase Li<sub>5</sub>La<sub>3</sub>Nb<sub>2</sub>O<sub>12</sub> crystals were successfully
grown using
a LiOH flux cooling method at the relatively low temperature of 500
°C at a solute concentration of 5 mol %. The grown Li<sub>5</sub>La<sub>3</sub>Nb<sub>2</sub>O<sub>12</sub> crystals had polyhedral
shapes with well-developed, flat {211} and {110} faces. Their shapes
were relatively uniform, and the average crystal size was approximately
59.2 μm. No aggregation was observed in scanning electron microscopy
images. The high crystallinity of the Li<sub>5</sub>La<sub>3</sub>Nb<sub>2</sub>O<sub>12</sub> crystals was confirmed by transmission
electron microscopy images. Their lattice parameter was determined
from the X-ray diffraction pattern to be <i>a</i> = 1.281
nm, which is consistent with the literature value (<i>a</i> = 1.282 nm). Furthermore, the crystal phase, form, size, and crystallinity
of the flux-grown Li<sub>5</sub>La<sub>3</sub>Nb<sub>2</sub>O<sub>12</sub> crystals were obviously dependent on the growth conditions
including the solute concentration and holding temperature
Chloride Flux Growth of La<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub> Crystals and Subsequent Nitridation To Form LaTiO<sub>2</sub>N Crystals
Highly crystalline, platelike La<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub> were grown from a NaCl flux, and
LaTiO<sub>2</sub>N crystals
were obtained by subsequent nitridation under NH<sub>3</sub> flow.
The TEM analysis indicated that the flux-grown platelike La<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub> crystals are single-crystalline growing
along the <i>a</i> axis. The shapes and sizes of the LaTiO<sub>2</sub>N crystals were almost unchanged from the La<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub> precursor. In addition, LaTiO<sub>2</sub>N crystals
remained single-crystalline with a porous nanostructure. The optical
absorption edges of the La<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub> and
LaTiO<sub>2</sub>N crystals were approximately 320 and 600 nm
Low-Temperature Flux Growth and Upconversion Fluorescence of the Idiomorphic Hexagonal-System NaYF<sub>4</sub> and NaYF<sub>4</sub>:Ln (Ln = Yb, Er, Tm) Crystals
Idiomorphic NaYF<sub>4</sub> and NaYF<sub>4</sub>:Ln (Ln = Yb, Er, Tm) crystals with upconversion fluorescence were successfully grown by the NaNO<sub>3</sub> flux cooling method at a relatively low holding temperature. The grown NaYF<sub>4</sub> and NaYF<sub>4</sub>:Ln crystals had a hexagonal prismatic form, and their well-developed surfaces were relatively flat. TEM images indicated that the NaYF<sub>4</sub> crystals were of good crystallinity. Their size and shape were relatively uniform, and they were poorly aggregated. The crystal phase, form, and size depended on the growth temperature and the solute concentration. In contrast, the addition of dopant ions (Yb<sup>3+</sup>, Er<sup>3+</sup>, and Tm<sup>3+</sup>) did not affect the shape, morphology, or crystallinity of the flux-grown NaYF<sub>4</sub>:Ln crystals. Additionally, the upconversion fluorescence properties of NaYF<sub>4</sub>:Ln crystals were also dependent on the type and mixture ratio (i.e., starting composition) of the dopants. The green, orange, and blue upconversion fluorescences of NaYF<sub>4</sub>:10%Yb,1%Er, NaYF<sub>4</sub>:50%Yb,1%Er, and NaYF<sub>4</sub>:10%Yb,1%Tm crystals, respectively, were observed under 980 nm laser irradiation via two- or three-photon upconversion processes
NH<sub>3</sub>‑Assisted Flux Growth of Cube-like BaTaO<sub>2</sub>N Submicron Crystals in a Completely Ionized Nonaqueous High-Temperature Solution and Their Water Splitting Activity
As the 600 nm-class photocatalyst,
BaTaO<sub>2</sub>N is one of
the promising candidates of the perovskite-type oxynitride family
for photocatalytic water splitting under visible light. The oxynitrides
are routinely synthesized by nitriding corresponding oxide precursors
under a high-temperature NH<sub>3</sub> atmosphere, causing an increase
in the defect density and a decrease in photocatalytic activity. To
improve the photocatalytic activity by reducing the defect density
and improving the crystallinity, we here demonstrate an NH<sub>3</sub>-assisted KCl flux growth approach for the direct synthesis of BaTaO<sub>2</sub>N crystals. The effects of various fluxes, solute concentration,
and reaction time and temperature on the phase evolution and morphology
transformation of the BaTaO<sub>2</sub>N crystals were systematically
investigated. By changing the solute concentration from 10 to 50 mol
%, it was found that phase-pure BaTaO<sub>2</sub>N crystals could
only be grown with the solute concentrations of ≥10 mol % using
the KCl flux, and the solute concentration of 10 mol % was solely
favorable to directly grow cube-like BaTaO<sub>2</sub>N crystals with
an average size of about 125 nm and exposed {100} and {110} faces
at 950 °C for 10 h. The time- and temperature-dependent experiments
were also performed to postulate the direct growth mechanisms of cube-like
BaTaO<sub>2</sub>N submicron crystals. The BaTaO<sub>2</sub>N crystals
modified with Pt and CoO<sub><i>x</i></sub> nanoparticles
showed a reasonable H<sub>2</sub> and O<sub>2</sub> evolution, respectively,
due to a lower defect density and higher crystallinity achieved by
an NH<sub>3</sub>-assisted KCl flux method
High-Quality Ultralong Hydroxyapatite Nanowhiskers Grown Directly on Titanium Surfaces by Novel Low-Temperature Flux Coating Method
Idiomorphic, one-dimensional (1-D), and high-quality
hydroxyapatite
(HAp) nanocrystals were successfully, directly, and densely grown
on a Ti substrate at the relatively low temperature of 300 °C
using a KNO<sub>3</sub>–LiNO<sub>3</sub> flux coating method.
The grown HAp crystals have a 1-D shape with a very high aspect ratio
(much larger than 100) and an average size of 3250 × 25 nm (length
× width). The ultralong 1-D crystals grown at 300 °C were
identified as highly crystalline HAp by their X-ray diffraction (XRD)
patterns, which clearly displayed the four characteristic lines of
HAp between 31.5° and 34.5°. Additionally, high-resolution
transmission electron microscopy (HRTEM) images demonstrated that
these ultralong whiskers were high-quality because point and line
defects were not observed. From the energy-dispersive X-ray spectroscopy
(EDS) analysis, major components were homogeneously distributed in
the HAp whiskers. In addition, the effects of holding temperature
and starting composition on the forms and average sizes of the grown
HAp whiskers were investigated