11 research outputs found
Synthesis and In Situ Xāray Diffraction Characterization of Two-Dimensional Perovskite-Type Oxide Colloids with a Controlled Molecular Thickness
A series of two-dimensional (2D) niobate nanosheets with
a thickness
controllable in increments of 0.4ā0.5 nm were synthesized by
chemically delaminating precursory layered perovskites into their
unilamellar layers. The homologous layered compounds of KCa<sub>2</sub>Na<sub><i>n</i>ā3</sub>Nb<sub><i>n</i></sub>O<sub>3<i>n</i>+1</sub> for <i>n</i> =
4ā6 were prepared as starting materials by repeated solid-state
calcination of KCa<sub>2</sub>Nb<sub>3</sub>O<sub>10</sub> (<i>n</i> = 3 analog) and NaNbO<sub>3</sub> at 1573 K. These compounds
were then converted into protonic forms and were further reacted with
a tetrabutylammonium hydroxide solution to yield a translucent colloidal
suspension. Nearly perfect delamination was confirmed by in situ X-ray
diffraction (XRD) measurements on glue-like colloids centrifuged from
the suspension, which showed total loss of basal diffraction series
and an evolution of a broad, wavy pattern instead. The characteristic
oscillating profile was dependent on <i>n</i>, or the layer
thickness, and could be consistently reproduced by simulation in terms
of X-ray scattering from the individual 2D fundamental unit of perovskite-type
oxides or diffraction from ultrathin crystallites with a defined repeating
(<i>n</i> times) unit composed of NbO<sub>6</sub> octahedra
and Ca/Na. Atomic force microscopy (AFM) observation of samples deposited
on a Si substrate detected micrometer-sized sheets with a thickness
of 2.7 nm (<i>n</i> = 4), 3.1 nm (<i>n</i> = 5),
and 3.6 nm (<i>n</i> = 6), results that are compatible with
the dimensions for <i>n</i> of corner-shared octahedra.
In addition, in-plane XRD data showed sharp lines attributable to
a 2D square lattice (<i>a</i> = 0.39 nm) of perovskite structures.
These results along with chemical analysis data indicate the formation
of a novel class of 2D perovskite oxides, Ca<sub>2āĪ“</sub>(Na,K)<sub><i>n</i>ā3+Ī“</sub>Nb<sub><i>n</i></sub>O<sub>3<i>n</i>+1</sub><sup>ā</sup> (<i>n</i> = 4ā6), with a progressively increasing
thickness by 0.4ā0.5 nm. These nanosheets showed intense absorption
of ultraviolet (UV) light due to their semiconducting nature. The
bandgap energy was estimated as 3.96, 3.81, and 3.77 eV, being dependent
on <i>n</i>, which may reflect the relaxing degree of size
quantization with the nanosheet thickness. Aggregated nanosheets flocculated
with a solution containing KCl and trace amounts of RuCl<sub>3</sub> were heated at 773 K to produce photocatalytic materials loaded
with RuO<sub>2</sub> as a cocatalyst. The resulting samples underwent
water splitting under UV irradiation. The evolution of H<sub>2</sub> and O<sub>2</sub> gas in a 2:1 ratio proceeded on the material from
the <i>n</i> = 4 nanosheet, while deviation from stoichiometric
decomposition as well as deterioration of activity were observed for
the samples from the thicker nanosheets
Soft-Chemical Exfoliation of RbSrNb<sub>2</sub>O<sub>6</sub>F into Homogeneously Unilamellar Oxyfluoride Nanosheets
Interlayer Rb<sup>+</sup> of the perovskite-type layered
oxyfluoride RbSrNb<sub>2</sub>O<sub>6</sub>F was ion-exchanged with
H<sup>+</sup>, and the protonated phase was reacted with aqueous solution
of tetrabutylammonium hydroxide to exfoliate it into nanosheets. The
resulting nanosheet suspension exhibits Tyndall scattering of a laser
beam, indicating its colloidal nature. Elemental composition of the
nanosheet was estimated as Sr<sub>0.98</sub>Nb<sub>2</sub>O<sub>6</sub>F<sub>0.97</sub><sup>Ī“ā</sup>, which was quite close
to that of the layer unit of the precursor. The homogeneously unilamellar
nature of this nanosheet was confirmed by atomic force and transmission
electron microscopy observations and X-ray scattering results. The
optical absorption edge of the nanosheet suspension was observed around
at 293 nm, and two well-defined peaks with their maxima at 229 and
278 nm were observed. Furthermore, the aqueous suspension of the nanosheet
exhibits fluorescence emission in the UV-blue region. These properties
of the oxyfluoride nanosheets are quite different from those of its
oxide analogues without F<sup>ā</sup>, such as LnNb<sub>2</sub>O<sub>7</sub><sup>ā</sup> nanosheets (Ln = La<sup>3+</sup>, Eu<sup>3+</sup>, Sm<sup>3+</sup>), suggesting that anion-site replacement
of oxide nanosheets can be utilized to optimize or induce various
properties
New Family of Lanthanide-Based InorganicāOrganic Hybrid Frameworks: Ln<sub>2</sub>(OH)<sub>4</sub>[O<sub>3</sub>S(CH<sub>2</sub>)<sub><i>n</i></sub>SO<sub>3</sub>]Ā·2H<sub>2</sub>O (Ln = La, Ce, Pr, Nd, Sm; <i>n</i> = 3, 4) and Their Derivatives
We report the synthesis and structure characterization
of a new family of lanthanide-based inorganicāorganic hybrid
frameworks, Ln<sub>2</sub>(OH)<sub>4</sub>[O<sub>3</sub>SĀ(CH<sub>2</sub>)<sub><i>n</i></sub>SO<sub>3</sub>]Ā·2H<sub>2</sub>O (Ln = La, Ce, Pr, Nd, Sm; <i>n</i> = 3, 4), and their
oxide derivatives. Highly crystallized samples were synthesized by
homogeneous precipitation of Ln<sup>3+</sup> ions from a solution
containing Ī±,Ļ-organodisulfonate salts promoted by slow
hydrolysis of hexamethylenetetramine. The crystal structure solved
from powder X-ray diffraction data revealed that this material comprises
two-dimensional cationic lanthanide hydroxide {[LnĀ(OH)<sub>2</sub>(H<sub>2</sub>O)]<sup>+</sup>}<sub>ā</sub> layers, which are
cross-linked by Ī±,Ļ-organodisulfonate ligands into a three-dimensional
pillared framework. This hybrid framework can be regarded as a derivative
of UCl<sub>3</sub>-type LnĀ(OH)<sub>3</sub> involving penetration
of organic chains into two {LnO<sub>9</sub>} polyhedra. Substitutional
modification of the lanthanide coordination promotes a 2D arrangement
of the {LnO<sub>9</sub>} polyhedra. A new hybrid oxide, Ln<sub>2</sub>O<sub>2</sub>[O<sub>3</sub>SĀ(CH<sub>2</sub>)<sub><i>n</i></sub>SO<sub>3</sub>], which is supposed to consist of alternating
{[Ln<sub>2</sub>O<sub>2</sub>]<sup>2+</sup>}<sub>ā</sub> layers
and Ī±,Ļ-organodisulfonate ligands, can be derived from
the hydroxide form upon dehydration/dehydroxylation. These hybrid
frameworks provide new opportunities to engineer the interlayer chemistry
of layered structures and achieve advanced functionalities coupled
with the advantages of lanthanide elements
Electronic Band Structure of Exfoliated Titanium- and/or Niobium-Based Oxide Nanosheets Probed by Electrochemical and Photoelectrochemical Measurements
Exfoliated two-dimensional (2D) unilamellar nanosheets
of Ca<sub>2</sub>Nb<sub>3</sub>O<sub>10</sub><sup>ā</sup>,
TiNbO<sub>5</sub><sup>ā</sup>, Ti<sub>2</sub>NbO<sub>7</sub><sup>ā</sup>, and Ti<sub>5</sub>NbO<sub>14</sub><sup>3ā</sup> were deposited
layer-by-layer to produce multilayer films on indiumātināoxide
(ITO)-coated glass electrodes, and their electrochemical and photoelectrochemical
properties were explored. The layer-by-layer assembly process via
sequential adsorption with counter polycations was monitored by UVāvisible
absorption spectra and X-ray diffraction measurements, which confirmed
the successful growth of films, where nanosheets and polycations are
alternately stacked at a separation of 1.6ā2.4 nm. Exposure
to UV light totally removed polycations, producing inorganic films.
Cyclic voltammetry on Ti and/or Nb oxide nanosheet electrodes thus
fabricated showed reduction/oxidation (Ti<sup>3+</sup>/Ti<sup>4+</sup> and Nb<sup>4+</sup>/Nb<sup>5+</sup>) peaks associated with insertion/extraction of Li<sup>+</sup> ions into/from intersheet galleries of the films. The extent
of the redox reaction is found to be governed by the cation density
in the nanosheet gallery. Anodic photocurrents of the oxide nanosheet
electrodes were observed under UV light irradiation. These action
spectra showed close resemblance to optical absorption profiles of
the colloidal nanosheets, indicating that the photocurrent was generated
from the nanosheets. Their analysis indicates that the nanosheets
of Ca<sub>2</sub>Nb<sub>3</sub>O<sub>10</sub><sup>ā</sup>,
TiNbO<sub>5</sub><sup>ā</sup>, Ti<sub>2</sub>NbO<sub>7</sub><sup>ā</sup>, and Ti<sub>5</sub>NbO<sub>14</sub><sup>3ā</sup> are all indirect transition-type wide-gap semiconductors with bandgap
energies of 3.44, 3.68, 3.64, and 3.53 eV, respectively.
These values are larger than those for corresponding parent layered
oxide compounds before delamination, suggesting confinement effects
into 2D nanosheet structure. Furthermore, the value was invariable
for the films with a different number of nanosheet layers, indicating
that quantized nanosheets were electronically isolated with each other.
In addition, photocurrent generation was measured as a function of
applied electrode potential, and the flatband potential was estimated
from the photocurrent onset values as ā1.12, ā1.33,
ā1.30, and ā1.29 V vs Ag/Ag<sup>+</sup>, for Ca<sub>2</sub>Nb<sub>3</sub>O<sub>10</sub><sup>ā</sup>, TiNbO<sub>5</sub><sup>ā</sup>, Ti<sub>2</sub>NbO<sub>7</sub><sup>ā</sup>, and Ti<sub>5</sub>NbO<sub>14</sub><sup>3ā</sup> nanosheets,
respectively, providing a diagram of electronic band structure for
the nanosheets
Bulk Functional Materials Design Using Oxide Nanosheets as Building Blocks: A New Upconversion Material Fabricated by Flocculation of Ca<sub>2</sub>Nb<sub>3</sub>O<sub>10</sub><sup>ā</sup> Nanosheets with Rare-Earth Ions
A new
upconversion (UC) material was designed by flocculating a
Ca<sub>2</sub>Nb<sub>3</sub>O<sub>10</sub><sup>ā</sup> nanosheet,
which acts as thermal and structural stabilizer, with Ho<sup>3+</sup> photoactivator, Yb<sup>3+</sup> sensitizer, and Y<sup>3+</sup> space
filler. The flocculated product consists of the restacked nanosheets
and the rare-earth ions in the internanosheet gallery. The restacked
sheet faces of the Ca<sub>2</sub>Nb<sub>3</sub>O<sub>10</sub><sup>ā</sup> nanosheet building blocks are self-organized in a
parallel manner, and their crystallographic coherency extends to three
layers on average. On the other hand, the nanosheet building blocks
are randomly staggered along the in-layer direction. Chemical composition
of the flocculated product was estimated as (Ho<sub>0.096</sub>Yb<sub>0.23</sub>Y<sub>0.164</sub>)ĀCa<sub>1.76</sub>ā”<sub>0.24</sub>Nb<sub>3</sub>O<sub>10</sub>Ā·1.4H<sub>2</sub>O. Heat treatment
of the flocculated product at 500 Ā°C was necessary in order to
suppress nonradiative energy loss via OH vibration and to induce UC
emission. Even after the heat treatment, perovskite-type atomic arrangement
of the Ca<sub>2</sub>Nb<sub>3</sub>O<sub>10</sub><sup>ā</sup> nanosheet building block was retained. Upon laser irradiation at
980 nm, two UC emission bands around 550 and 660 nm were observed,
and the emission was visible to the eye. The result from this study
suggests that flocculation of nanosheets, as building blocks, with
counterions is a promising way to design bulk functional materials
that are rather difficult or impossible to prepare by conventional
synthetic approaches
High Thermal Robustness of Molecularly Thin Perovskite Nanosheets and Implications for Superior Dielectric Properties
A systematic study has been conducted to examine the thermal stability of layer-by-layer assembled films of perovskite-type nanosheets, (Ca<sub>2</sub>Nb<sub>3</sub>O<sub>10</sub><sup>ā</sup>)<sub><i>n</i></sub> (<i>n</i> = 1ā10), which exhibit superior dielectric and insulating properties. In-plane and out-of-plane X-ray diffraction data as well as observations by atomic force microscopy and transmission electron microscopy indicated the high thermal robustness of the nanosheet films. In a monolayer film with an extremely small thickness of ā¼2 nm, the nanosheet was stable up to 800 Ā°C, the temperature above which segregation into CaNb<sub>2</sub>O<sub>6</sub> and Ca<sub>2</sub>Nb<sub>2</sub>O<sub>7</sub> began. The critical temperature moderately decreased as the film thickness, or the number of nanosheet layers, increased, and reached 700 Ā°C for seven- and 10-layer films, which is comparable to the phase transformation temperature for a bulk phase of the protonic layered oxide of HCa<sub>2</sub>Nb<sub>3</sub>O<sub>10</sub>Ā·1.5H<sub>2</sub>O as a precursor of the nanosheet. This thermal stabilization of perovskite-type nanosheets should be associated with restricted nucleation and crystal growth peculiar to such ultrathin 2D bound systems. The stable high-<i>k</i> dielectric response (Īµ<sub>r</sub> = 210) and highly insulating nature (<i>J</i> < 10<sup>ā7</sup> A cm<sup>ā2</sup>) remained substantially unchanged even after the nanosheet film was annealed up to 600 Ā°C. This study demonstrates the high thermal stability of 2D perovskite-type niobate nanosheets in terms of structure and dielectric properties, which suggests promising potential for future high-<i>k</i> devices operable over a wide temperature range
Correction to āSynthesis and Atomic Characterization of a Ti<sub>2</sub>O<sub>3</sub> Nanosheetā
Correction to āSynthesis and Atomic Characterization of a Ti<sub>2</sub>O<sub>3</sub> Nanosheet
Synthesis and Atomic Characterization of a Ti<sub>2</sub>O<sub>3</sub> Nanosheet
Titanium oxide nanosheets have been attracting much attention owing to their photocatalytic property. Here, we synthesized a Ti<sub>2</sub>O<sub>3</sub> nanosheet by the reduction of a titania nanosheet (Ti<sub>0.87</sub>O<sub>2</sub>) that was one or two atoms in thickness. The atomic structure of the Ti<sub>2</sub>O<sub>3</sub> nanosheet was quantitatively revealed by electron diffraction analysis, electron energy-loss spectroscopy, and high-resolution transmission electron microscopy (TEM). A titania nanosheet (Ti<sub>0.87</sub>O<sub>2</sub>) consisting of edge-shared TiO<sub>6</sub> octahedra was transformed to a Ti<sub>2</sub>O<sub>3</sub> nanosheet consisting of face-shared octahedra by electron beam irradiation. This represents a stable crystal phase of titania nanosheets like the Magneli phase in oxygen-deficient environments. The atomic arrangement of the Ti<sub>2</sub>O<sub>3</sub> nanosheet was directly observed by newly developed aberration-corrected TEM
Tuning the Surface Charge of 2D Oxide Nanosheets and the Bulk-Scale Production of Superlatticelike Composites
The surface charge of various anionic
unilamellar nanosheets, such
as graphene oxide (GO), Ti<sub>0.87</sub>O<sub>2</sub><sup>0.52ā</sup>, and Ca<sub>2</sub>Nb<sub>3</sub>O<sub>10</sub><sup>ā</sup> nanosheets, has been successfully modified to be positive by interaction
with polycations while maintaining a monodispersed state. A dilute
anionic nanosheet suspension was slowly added dropwise into an aqueous
solution of high molecular weight polycations, which attach on the
surface of the anionic nanosheets via electrostatic interaction. Surface
modification and transformation to positively charged nanosheets were
confirmed by various characterizations including atomic force microscopy
and zeta potential measurements. Because the sizes of the polycations
used are much larger than the nanosheets, the polymer chains may run
off the nanosheet edges and fold to the fronts of the nanosheets,
which could be a reason for the continued dispersion of the modified
nanosheets in the suspension. By slowly adding a suspension of polycation-modified
nanosheets and pristine anionic nanosheet dropwise into water under
suitable conditions, a superlatticelike heteroassembly can be readily
produced. Characterizations including transmission electron microscopy
and X-ray diffraction measurements provide evidence for the formation
of the alternately stacked structures. This approach enables the combination
of various pairs of anionic nanosheets with different functionalities,
providing a new opportunity for the creation of unique bulk-scale
functional materials and their applications
Atomic Layer Engineering of HighāĪŗ Ferroelectricity in 2D Perovskites
Complex perovskite
oxides offer tremendous potential for controlling
their rich variety of electronic properties, including high-<i>T</i><sub>C</sub> superconductivity, high-Īŗ ferroelectricity,
and quantum magnetism. Atomic-scale control of these intriguing properties
in ultrathin perovskites is an important challenge for exploring new
physics and device functionality at atomic dimensions. Here, we demonstrate
atomic-scale engineering of dielectric responses using two-dimensional
(2D) homologous perovskite nanosheets (Ca<sub>2</sub>ĀNa<sub><i>m</i>ā3</sub>ĀNb<sub><i>m</i></sub>ĀO<sub>3<i>m</i>+1</sub>; <i>m</i> = 3ā6).
In this homologous 2D material, the thickness of the perovskite layers
can be incrementally controlled by changing <i>m</i>, and
such atomic layer engineering enhances the high-Īŗ dielectric
response and local ferroelectric instability. The end member (<i>m</i> = 6) attains a high dielectric constant of ā¼470,
which is the highest among all known dielectrics in the ultrathin
region (<10 nm). These results provide a new strategy for achieving
high-Īŗ ferroelectrics for use in ultrascaled high-density capacitors
and post-graphene technology