2 research outputs found
A<sub>2</sub>TiO<sub>5</sub> (A = Dy, Gd, Er, Yb) at High Pressure
The
structural evolution of lanthanide A<sub>2</sub>TiO<sub>5</sub> (A
= Dy, Gd, Yb, Er) at high pressure is investigated using synchrotron
X-ray diffraction. The effects of A-site cation size and of the initial
structure are systematically examined by varying the composition of
the isostructural lanthanide titanates and the structure of dysprosium
titanate polymorphs (orthorhombic, hexagonal, and cubic), respectively.
All samples undergo irreversible high-pressure phase transformations,
but with different onset pressures depending on the initial structure.
While each individual phase exhibits different phase transformation
histories, all samples commonly experience a sluggish transformation
to a defect cotunnite-like (<i>Pnma</i>) phase for a certain
pressure range. Orthorhombic Dy<sub>2</sub>TiO<sub>5</sub> and Gd<sub>2</sub>TiO<sub>5</sub> form <i>P</i>2<sub>1</sub><i>am</i> at pressures below 9 GPa and <i>Pnma</i> above
13 GPa. Pyrochlore-type Dy<sub>2</sub>TiO<sub>5</sub> and Er<sub>2</sub>TiO<sub>5</sub> as well as defect-fluorite-type Yb<sub>2</sub>TiO<sub>5</sub> form <i>Pnma</i> at ∼21 GPa, followed by <i>Im</i>3<i>̅m</i>. Hexagonal Dy<sub>2</sub>TiO<sub>5</sub> forms <i>Pnma</i> directly, although a small amount
of remnants of hexagonal Dy<sub>2</sub>TiO<sub>5</sub> is observed
even at the highest pressure (∼55 GPa) reached, indicating
kinetic limitations in the hexagonal Dy<sub>2</sub>TiO<sub>5</sub> phase transformations at high pressure. Decompression of these materials
leads to different metastable phases. Most interestingly, a high-pressure
cubic X-type phase (<i>Im</i>3<i>Ì…m</i>)
is confirmed using high-resolution transmission electron microscopy
on recovered pyrochlore-type Er<sub>2</sub>TiO<sub>5</sub>. The kinetic
constraints on this metastable phase yield a mixture of both the X-type
phase and amorphous domains upon pressure release. This is the first
observation of an X-type phase for an A<sub>2</sub>BO<sub>5</sub> composition
at high pressure
Structure and Reactivity of X‑ray Amorphous Uranyl Peroxide, U<sub>2</sub>O<sub>7</sub>
Recent
accidents resulting in worker injury and radioactive contamination
occurred due to pressurization of uranium yellowcake drums produced
in the western U.S.A. The drums contained an X-ray amorphous reactive
form of uranium oxide that may have contributed to the pressurization.
Heating hydrated uranyl peroxides produced during <i>in situ</i> mining can produce an amorphous compound, as shown by X-ray powder
diffraction of material from impacted drums. Subsequently, studtite,
[(UO<sub>2</sub>)Â(O<sub>2</sub>)Â(H<sub>2</sub>O)<sub>2</sub>]Â(H<sub>2</sub>O)<sub>2</sub>, was heated in the laboratory. Its thermal
decomposition produced a hygroscopic anhydrous uranyl peroxide that
reacts with water to release O<sub>2</sub> gas and form metaschoepite,
a uranyl-oxide hydrate. Quantum chemical calculations indicate that
the most stable U<sub>2</sub>O<sub>7</sub> conformer consists of two
bent (UO<sub>2</sub>)<sup>2+</sup> uranyl ions bridged by a peroxide
group bidentate and parallel to each uranyl ion, and a μ<sub>2</sub>-O atom, resulting in charge neutrality. A pair distribution
function from neutron total scattering supports this structural model,
as do <sup>1</sup>H- and <sup>17</sup>O-nuclear magnetic resonance
spectra. The reactivity of U<sub>2</sub>O<sub>7</sub> in water and
with water in air is higher than that of other uranium oxides, and
this can be both hazardous and potentially advantageous in the nuclear
fuel cycle