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

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    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

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    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

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    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

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    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

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    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

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    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

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    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

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    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

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    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

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    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
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