5 research outputs found
Epitaxial Strain-Controlled Ionic Conductivity in Li-Ion Solid Electrolyte Li<sub>0.33</sub>La<sub>0.56</sub>TiO<sub>3</sub> Thin Films
Ionic conductive Li<sub>0.33</sub>La<sub>0.56</sub>TiO<sub>3</sub> (LLT) epitaxial thin films were
grown on perovskite SrTiO<sub>3</sub> (100), NdGaO<sub>3</sub> (110),
and (LaAlO<sub>3</sub>)<sub>0.3</sub>-(SrAl<sub>0.5</sub>Ta<sub>0.5</sub>O<sub>3</sub>)<sub>0.7</sub> (100)
single crystal substrates by pulsed laser deposition. The use of Li-rich
Li<sub>0.84</sub>La<sub>0.56</sub>TiO<sub>3+δ</sub> target together
with an optimized laser fluence resulted in the growth of phase pure
LLT thin films with high growth rate of 2 nm/min. The <i>a</i>-axis and <i>c</i>-axis oriented films were selectively
grown by choosing the substrates. Ionic conductivity at room temperature
of LLT epitaxial film on NdGaO<sub>3</sub> (110) substrate was close
to that of bulk previously reported, representing the highly crystalline
quality. In addition, the unequally strained lattice due to different
in-plane lattice constants of orthorhombic NdGaO<sub>3</sub> substrate
resulted in laterally anisotropic ionic conductivity with different
activation energy perpendicular to NdGaO<sub>3</sub> [11Ì…0]
and [001], 6.7 × 10<sup>–4</sup> S·cm<sup>–1</sup> with 0.34 eV and 4.3 × 10<sup>–4</sup> S·cm<sup>–1</sup> with 0.36 eV, respectively. This result suggests
that the lattice engineering can provide a way to control Li ionic
conduction
Lateral Solid-Phase Epitaxy of Oxide Thin Films on Glass Substrate Seeded with Oxide Nanosheets
We developed a technique to fabricate oxide thin films with uniaxially controlled crystallographic orientation and lateral size of more than micrometers on amorphous substrates. This technique is lateral solid-phase epitaxy, where epitaxial crystallization of amorphous precursor is seeded with ultrathin oxide nanosheets sparsely (≈10% coverage) deposited on the substrate. Transparent conducting Nb-doped anatase TiO<sub>2</sub> thin films were fabricated on glass substrates by this technique. Perfect (001) orientation and large grains with lateral sizes up to 10 μm were confirmed by X-ray diffraction, atomic force microscopy, and electron beam backÂscattering diffraction measurements. As a consequence of these features, the obtained film exhibited excellent electrical transport properties comparable to those of epitaxial thin films on single-crystalline substrates. This technique is a versatile method for fabricating high-quality oxide thin films other than anatase TiO<sub>2</sub> and would increase the possible applications of oxide-based thin film devices
Enhanced Electrical Conduction in Anatase TaON via Soft Chemical Lithium Insertion toward Electronics Application
Metal oxynitride
semiconductors with the d<sup>0</sup> or d<sup>10</sup> electron configuration
are promising materials for nontoxic
pigments and photocatalysts, but their electrical properties have
scarcely been studied. Anatase TaON (δ-TaON) is a metastable
polymorph of TaON, and its epitaxial thin films show good semiconducting
properties such as a wide tunability of electrical conductivity and
a rather high electron mobility comparable to that of anatase TiO<sub>2</sub>. However, the density of carrier electrons (<i>n</i><sub>e</sub>) provided by anion vacancies is limited to ∼1
× 10<sup>20</sup> cm<sup>–3</sup>, so establishing a method
for carrier doping of anatase TaON remains a critical issue for its
use in electronics applications. In this report, we used soft chemical
insertion of Li into interstitial sites of anatase TaON epitaxial
thin films by using an <i>n</i>-butyllithium solution, and
the resulting material showed a higher <i>n</i><sub>e</sub> (3.5 × 10<sup>20</sup> cm<sup>–3</sup>) than anion-deficient
anatase TaON films. Additionally, the Li-inserted anatase TaON showed
an enhanced Hall mobility (μ<sub>H</sub>) of over 30 cm<sup>2</sup>V<sup>–1</sup>s<sup>–1</sup> and a lower resistivity
of 6.7 × 10<sup>–4</sup> Ωcm at room temperature.
In contrast, direct vapor phase deposition of Li-doped TaON caused
Li substitution for Ta, where a large difference in charges between
Li<sup>+</sup> and Ta<sup>5+</sup> was compensated by an increase
in the O/N ratio. These results indicate that soft chemical insertion
of Li after growth of the host crystal is an effective method for
carrier doping of anatase TaON
Strain Engineering for Anion Arrangement in Perovskite Oxynitrides
Mixed-anion perovskites such as oxynitrides,
oxyfluorides, and
oxyhydrides have flexibility in their anion arrangements, which potentially
enables functional material design based on coordination chemistry.
However, difficulty in the control of the anion arrangement has prevented
the realization of this concept. In this study, we demonstrate strain
engineering of the anion arrangement in epitaxial thin films of the
Ca<sub>1–<i>x</i></sub>Sr<sub><i>x</i></sub>TaO<sub>2</sub>N perovskite oxynitrides. Under compressive epitaxial
strain, the axial sites in TaO<sub>4</sub>N<sub>2</sub> octahedra
tend to be occupied by nitrogen rather than oxygen, which was revealed
by N and O K-edge linearly polarized X-ray absorption near-edge structure
(LP-XANES) and scanning transmission electron microscopy combined
with electron energy loss spectroscopy. Furthermore, detailed analysis
of the LP-XANES indicated that the high occupancy of nitrogen at the
axial sites is due to the partial formation of a metastable <i>trans-</i>type anion configuration. These results are expected
to serve as a guide for the material design of mixed-anion compounds
based on their anion arrangements
Reversible Changes in Resistance of Perovskite Nickelate NdNiO<sub>3</sub> Thin Films Induced by Fluorine Substitution
Perovskite
nickel oxides are of fundamental as well as technological interest
because they show large resistance modulation associated with phase
transition as a function of the temperature and chemical composition.
Here, the effects of fluorine doping in perovskite nickelate NdNiO<sub>3</sub> epitaxial thin films are investigated through a low-temperature
reaction with polyvinylidene fluoride as the fluorine source. The
fluorine content in the fluorinated NdNiO<sub>3–<i>x</i></sub>F<sub><i>x</i></sub> films is controlled with precision
by varying the reaction time. The fully fluorinated film (<i>x</i> ≈ 1) is highly insulating and has a bandgap of
2.1 eV, in contrast to NdNiO<sub>3</sub>, which exhibits metallic
transport properties. Hard X-ray photoelectron and soft X-ray absorption
spectroscopies reveal the suppression of the density of states at
the Fermi level as well as the reduction of nickel ions (valence state
changes from +3 to +2) after fluorination, suggesting that the strong
Coulombic repulsion in the Ni 3d orbitals associated with the fluorine
substitution drives the metal-to-insulator transition. In addition,
the resistivity of the fluorinated films recovers to the original
value for NdNiO<sub>3</sub> after annealing in an oxygen atmosphere.
By application of the reversible fluorination process to transition-metal
oxides, the search for resistance-switching materials could be accelerated