4 research outputs found
Stereochemically Active Lone Pairs: Unraveling the Electronic Origin of Dielectric Response in Nonlinear Optical TeO<sub>2</sub>
Tellurite glasses have emerged as
a promising candidate for nonlinear
optics (NLO) due to their high refractive index and third-order optical
susceptibility (χ3). In this work, we focus on the
electronic structure of crystalline TeO2, a precursor to
numerous TeO2-based glasses. All three crystalline TeO2 polymorphs are wide-gap semiconductors and have electronic
contributions from the Te4+ 5s2 lone pairs near the Fermi level, which affect optical properties.
Based on the formation energies, the formation of oxygen vacancies
is strongly favorable during synthesis. Introduction of an oxygen
vacancy induces notable changes in the chemical environment in the
pristine α-TeO2 structure and the response of the
Te 5s2 lone pairs. Comparative analysis
to the measured refractive indices and static dielectric constant
(a second-rank tensor) shows that the calculated values of α-TeO2 with the presence of an oxygen vacancy (α-TeO2:Ov) agree well with experimental data. The high distortion
index and stereochemical activity ratio of α-TeO2:Ov contribute to its polarizable asymmetric electron
density. High polarization and faster orientation of the dipoles in
α-TeO2 with the presence of an oxygen vacancy make
it an excellent NLO material for ultrafast optical switch applications.
This study can help to guide design principles and improve our understanding
of the electronic origin of NLO materials containing lone pairs
Vacancy-Driven Disorder and Elevated Dielectric Response in the Pyrochlore Pb<sub>1.5</sub>Nb<sub>2</sub>O<sub>6.5</sub>
Lone pair-driven distortions are a hallmark of many technologically
important lead (Pb)-based materials. The role of Pb2+ in
polar perovskites is well understood and easily manipulated for applications
in piezo- and ferroelectricity, but the control of ordered lone pair
behavior in Pb-based pyrochlores is less clear. Crystallographically
and geometrically more complex than the perovskite structure, the
pyrochlore structure is prone to geometric frustration of local dipoles
due to a triangular arrangement of cations on a diamond lattice. The
role of vacancies on the O′ site of the pyrochlore network
has been implicated as an important driver for the expression and
correlation of stereochemically active lone pairs in pyrochlores such
as Pb2Ru2O6.5 and Pb2Sn2O6. In this work we report on the structural, dielectric,
and heat capacity behavior of the cation- and anion-deficient pyrochlore
Pb1.5Nb2O6.5 upon cooling. We find
that local distortions are present at all temperatures that can be
described by cristobalite-type cation ordering, and this ordering
persists to longer length scales upon cooling. From a crystallographic
perspective, the material remains disordered and does not undergo
an observable phase transition. In combination with density function
calculations, we propose that the stereochemical activity of the Pb2+ lone pairs is driven by proximity to O′ vacancies,
and the crystallographic site disorder of the O′ vacancies
prohibits long range correlation of lone pair-driven distortions.
This in turn prevents a low-temperature phase transition and results
in an elevated dielectric permittivity across a broad temperature
range
Structures and Phase Transitions of CePd<sub>3+<i>x</i></sub>Ga<sub>8‑<i>x</i></sub>: New Variants of the BaHg<sub>11</sub> Structure Type
New distorted variants of the cubic BaHg<sub>11</sub> structure
type have been synthesized in Ga flux. Multiple phases of CePd<sub>3+<i>x</i></sub>Ga<sub>8‑<i>x</i></sub>, which include an orthorhombic <i>Pmmn</i> structure (<i>x</i> = 3.21(2)), a rhombohedral <i>R</i>3̅<i>m</i> structure (<i>x</i> = 3.13(4)), and a cubic <i>Fm</i>3̅<i>m</i> superstructure (<i>x</i> = 2.69(6)), form preferentially depending on reaction cooling rate
and isolation temperature. Differential thermal analysis and <i>in situ</i> temperature-dependent powder X-ray diffraction patterns
show a reversible phase transition at approximately 640 °C between
the low temperature orthorhombic and rhombohedral structures and the
high temperature cubic superstructure. Single crystal X-ray diffraction
experiments indicate that the general structure of BaHg<sub>11</sub>, including the intersecting planes of a kagomé-type arrangement
of Ce atoms, is only slightly distorted in the low temperature phases.
A combination of Kondo, crystal electric field, and magnetic frustration
effects may be present, resulting in low temperature anomalies in
magnetic susceptibility, electrical resistivity, and heat capacity
measurements. In addition to CePd<sub>3+<i>x</i></sub>Ga<sub>8‑<i>x</i></sub>, the rare earth analogues REPd<sub>3+<i>x</i></sub>Ga<sub>8‑<i>x</i></sub>, RE = La, Nd, Sm, Tm, and Yb, were successfully synthesized and
also crystallize in one of the lower symmetry space groups
Structures and Phase Transitions of CePd<sub>3+<i>x</i></sub>Ga<sub>8‑<i>x</i></sub>: New Variants of the BaHg<sub>11</sub> Structure Type
New distorted variants of the cubic BaHg<sub>11</sub> structure
type have been synthesized in Ga flux. Multiple phases of CePd<sub>3+<i>x</i></sub>Ga<sub>8‑<i>x</i></sub>, which include an orthorhombic <i>Pmmn</i> structure (<i>x</i> = 3.21(2)), a rhombohedral <i>R</i>3̅<i>m</i> structure (<i>x</i> = 3.13(4)), and a cubic <i>Fm</i>3̅<i>m</i> superstructure (<i>x</i> = 2.69(6)), form preferentially depending on reaction cooling rate
and isolation temperature. Differential thermal analysis and <i>in situ</i> temperature-dependent powder X-ray diffraction patterns
show a reversible phase transition at approximately 640 °C between
the low temperature orthorhombic and rhombohedral structures and the
high temperature cubic superstructure. Single crystal X-ray diffraction
experiments indicate that the general structure of BaHg<sub>11</sub>, including the intersecting planes of a kagomé-type arrangement
of Ce atoms, is only slightly distorted in the low temperature phases.
A combination of Kondo, crystal electric field, and magnetic frustration
effects may be present, resulting in low temperature anomalies in
magnetic susceptibility, electrical resistivity, and heat capacity
measurements. In addition to CePd<sub>3+<i>x</i></sub>Ga<sub>8‑<i>x</i></sub>, the rare earth analogues REPd<sub>3+<i>x</i></sub>Ga<sub>8‑<i>x</i></sub>, RE = La, Nd, Sm, Tm, and Yb, were successfully synthesized and
also crystallize in one of the lower symmetry space groups