4 research outputs found
PolarāNonpolar Transition-Type Negative Thermal Expansion with 11.1% Volume Shrinkage by Design
Chemical substitution for the tuning of the working temperature
of phase-transition-type negative thermal expansion (NTE) materials
generally reduces the volume shrinkage during the transition. We have
investigated the effects of electron doping and reduction of 6s2 lone-pair activity in PbVO3 with a large polar
distortion (c/a = 1.23) and found
that the combination of Bi and Sr substitutions for Pb enables a temperature-induced
polar to non-polar transition with 11% volume shrinkage, even larger
than the pressure-induced volume collapse of PbVO3 (ā¼10.6%),
and is the largest value among the NTE materials reported so far.
The domain structure of the coexisting cubic and tetragonal phases
with such a huge volume difference was successfully observed by high-angle
annular dark-field scanning transmission electron microscopy and the
spatial distribution of domains by Bragg coherent X-ray diffraction
imaging. The temperature hysteresis is reduced by repeated heating/cooling
cycles, suggesting that the changes in the domain structure dominate
the NTE properties
Glassy Distribution of Bi<sup>3+</sup>/Bi<sup>5+</sup> in Bi<sub>1ā<i>x</i></sub>Pb<sub><i>x</i></sub>NiO<sub>3</sub> and Negative Thermal Expansion Induced by Intermetallic Charge Transfer
The valence distribution and local
structure of Bi<sub>1ā<i>x</i></sub>Pb<sub><i>x</i></sub>NiO<sub>3</sub> (<i>x</i> ā¤ 0.25)
were investigated by comprehensive studies
of Rietveld analysis of synchrotron X-ray diffraction (SXRD) data,
X-ray absorption spectroscopy (XAS), hard X-ray photoemission spectroscopy
(HAXPES), and pair distribution function (PDF) analysis of synchrotron
X-ray total scattering data. Disproportionation of Bi ions into Bi<sup>3+</sup> and Bi<sup>5+</sup> was observed for all the samples, but
it was a long-ranged one with distinct crystallographic sites in the <i>P</i>1Ģ
triclinic structure for <i>x</i> ā¤
0.15, while the ordering was short-ranged for <i>x</i> =
0.20 and 0.25. An intermetallic charge transfer between Bi<sup>5+</sup> and Ni<sup>2+</sup>, leading to large volume shrinkage, was observed
for all the samples upon heating at ā¼500 K
Pressure Induced Amorphization of Pb<sup>2+</sup> and Pb<sup>4+</sup> in Perovskite PbFeO<sub>3</sub>
Perovskite-type
oxides have been the subject of intense
research
due to their various fascinating physical properties stemming from
their charge degree of freedom. PbFeO3 has an unusual Pb2+0.5Pb4+0.5Fe3+O3 charge distribution with a long-ranged ordering of
Pb2+ and Pb4+ and two inequivalent Fe3+ sites in a perovskite structure. Combined synchrotron X-ray diffraction
and MoĢssbauer spectroscopy revealed a change to an orthorhombic
GdFeO3 structure with a unique Fe3+ site and
randomly distributed Pb2+ and Pb4+ at 29.0 GPa,
namely, pressure-induced amorphization of Pb2+ and Pb4+. The absence of a charge transfer transition to the Pb2+Fe4+O3 phase, which was expected from
the comparison with PbCrO3 and PbCoO3, was verified
using ab initio density functional theory calculations in the range
of 0ā70 GPa
AāSite and BāSite Charge Orderings in an <i>sād</i> Level Controlled Perovskite Oxide PbCoO<sub>3</sub>
Perovskite PbCoO<sub>3</sub> synthesized
at 12 GPa was found to have an unusual charge distribution of Pb<sup>2+</sup>Pb<sup>4+</sup><sub>3</sub>Co<sup>2+</sup><sub>2</sub>Co<sup>3+</sup><sub>2</sub>O<sub>12</sub> with charge orderings in both
the A and B sites of perovskite ABO<sub>3</sub>. Comprehensive studies
using density functional theory (DFT) calculation, electron diffraction
(ED), synchrotron X-ray diffraction (SXRD), neutron powder diffraction
(NPD), hard X-ray photoemission spectroscopy (HAXPES), soft X-ray
absorption spectroscopy (XAS), and measurements of specific heat as
well as magnetic and electrical properties provide evidence of lead
ion and cobalt ion charge ordering leading to Pb<sup>2+</sup>Pb<sup>4+</sup><sub>3</sub>Co<sup>2+</sup><sub>2</sub>Co<sup>3+</sup><sub>2</sub>O<sub>12</sub> quadruple perovskite structure. It is shown
that the average valence distribution of Pb<sup>3.5+</sup>Co<sup>2.5+</sup>O<sub>3</sub> between Pb<sup>3+</sup>Cr<sup>3+</sup>O<sub>3</sub> and Pb<sup>4+</sup>Ni<sup>2+</sup>O<sub>3</sub> can be stabilized
by tuning the energy levels of Pb 6<i>s</i> and transition
metal 3<i>d</i> orbitals