3 research outputs found
Structural and Vibrational Properties of the Ordered Y<sub>2</sub>CaGe<sub>4</sub>O<sub>12</sub> Germanate: A Periodic Ab Initio Study
DFT
calculations with six LDA, GGA, and hybrid functionals have
been performed using the CRYSTAL09 code to describe the crystal structure
and vibrational spectra of Y<sub>2</sub>CaGe<sub>4</sub>O<sub>12</sub> cyclotetragermanate, a new optical host. Two space groups <i>P</i>4/<i>nbm</i> and <i>Cmme</i> have been
considered. The former corresponds to a mixed (0.5 Ca + 0.5 Y) distribution
at the octahedral sites found from the results of Rietveld refinement
of room temperature powder XRD pattern; the latter refers to the model
of crystallographically nonequivalent calcium and yttrium atomic setting
in distorted oxygen octahedrons. The most accurate geometry description
has been obtained with the WC1LYP and PBE (<i>n</i> = 6)
hybrid functionals, while the B3LYP calculation provides the best
agreement between the recorded infrared and Raman spectra and their
computed counterparts. Assignments of most of the observed bands to
vibrational modes are given. The comparison between calculated and
experimental frequencies shows a general good agreement for the spectra
below 600 cm<sup>–1</sup>. The relationship between selected
infrared bands and Raman lines, internal vibrations of the [Ge<sub>4</sub>O<sub>12</sub>] unit, and external modes is briefly discussed
New Antiferromagnetic Perovskite CaCo<sub>3</sub>V<sub>4</sub>O<sub>12</sub> Prepared at High-Pressure and High-Temperature Conditions
A new
perovskite, CaCo<sup>2+</sup><sub>3</sub>V<sup>4+</sup><sub>4</sub>O<sub>12</sub>, has been synthesized at high-pressure and high-temperature
(HP-HT) conditions. The properties of this perovskite were examined
by a range of techniques. CaCo<sub>3</sub>V<sub>4</sub>O<sub>12</sub> was found to adopt a double-perovskite cubic lattice [<i>a</i> = 7.3428(6) Ă…] with <i>Im</i>3Ě… symmetry. We
have established that this new perovskite is stable at ambient conditions,
and its oxidation and/or decomposition at ambient pressure begins
above 500 °C. It undergoes an abrupt antiferromagnetic transition
around 98 K. Electrical resistivity data suggest semimetallic conductivity
in the temperature range of 1.6–370 K. We have established
that the Co<sup>2+</sup> ions in CaCo<sub>3</sub>V<sub>4</sub>O<sub>12</sub> are in the high-spin state with a sizable orbital moment,
even though their square-planar oxygen coordination could be more
suitable for the low-spin state, which is prone to Jahn–Teller
distortion. Electrical resistivity curves also exhibit a distinct
steplike feature around 100 K. CaCo<sub>3</sub>V<sub>4</sub>O<sub>12</sub> is a first example of perovskite in which the sites A′
are fully occupied by Co<sup>2+</sup> ions, and hence its synthesis
opens the door to a new class of double perovskites, ACo<sub>3</sub>B<sub>4</sub>O<sub>12</sub>, that may be derived by chemical substitution
of the A sublattice by lanthanides, sodium, strontium, and bismuth
and by other elements and/or of the B sublattice by some other transition
metals
Structural and Magnetic Transitions in CaCo<sub>3</sub>V<sub>4</sub>O<sub>12</sub> Perovskite at Extreme Conditions
We investigated the structural, vibrational,
magnetic, and electronic
properties of the recently synthesized CaCo<sub>3</sub>V<sub>4</sub>O<sub>12</sub> double perovskite with the high-spin (HS) Co<sup>2+</sup> ions in a square-planar oxygen coordination at extreme conditions
of high pressures and low temperatures. The single-crystal X-ray diffraction
and Raman spectroscopy studies up to 60 GPa showed a conservation
of its cubic crystal structure but indicated a crossover near 30 GPa.
Above 30 GPa, we observed both an abnormally high “compressibility”
of the Co–O bonds in the square-planar oxygen coordination
and a huge anisotropic displacement of HS-Co<sup>2+</sup> ions in
the direction perpendicular to the oxygen planes. Although this effect
is reminiscent of a continuous HS → LS transformation of the
Co<sup>2+</sup> ions, it did not result in the anticipated shrinkage
of the cell volume because of a certain “stiffing” of
the bonds of the Ca and V cations. We verified that the oxidation
states of all the cations did not change across this crossover, and
hence, no charge-transfer effects were involved. Consequently, we
proposed that CaCo<sub>3</sub>V<sub>4</sub>O<sub>12</sub> could undergo
a phase transition at which the large HS-Co<sup>2+</sup> ions were
pushed out of the oxygen planes because of lattice compression. The
antiferromagnetic transition in CaCo<sub>3</sub>V<sub>4</sub>O<sub>12</sub> at 100 K was investigated by neutron powder diffraction
at ambient pressure. We established that the magnetic moments of the
Co<sup>2+</sup> ions were aligned along one of the cubic axes, and
the magnetic structure had a 2-fold periodicity along this axis, compared
to the crystallographic one