2 research outputs found
Glassy Distribution of Bi<sup>3+</sup>/Bi<sup>5+</sup> in Bi<sub>1–<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>1–<i>x</i></sub>Pb<sub><i>x</i></sub>NiO<sub>3</sub> (<i>x</i> ≤ 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>1̅ triclinic structure for <i>x</i> ≤
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 ∼500 K
A‑Site and B‑Site Charge Orderings in an <i>s–d</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