47 research outputs found
Retention of a Paramagnetic Ground State at Low Temperatures in a Family of Structurally Related U<sup>IV</sup> Phosphates
A new
uranium fluoride phosphate, UFPO<sub>4</sub>, was synthesized
via a mild hydrothermal route and characterized optically, thermally,
and magnetically. Two thermal transformation products, U<sub>2</sub>OÂ(PO<sub>4</sub>)<sub>2</sub> and U<sup>IV</sup>U<sup>VI</sup>O<sub>2</sub>(PO<sub>4</sub>)<sub>2</sub>, were discovered to be structurally
related, and were subsequently synthesized for bulk property measurements.
All three materials failed to follow Curie–Weiss behavior at
low temperatures, attributed to the nearly ubiquitous singlet ground
state of UÂ(IV), transitioning into a Curie–Weiss paramagnetic
regime at high temperatures. Neutron diffraction experiments were
performed on UFPO<sub>4</sub> and U<sup>IV</sup>U<sup>VI</sup>O<sub>2</sub>(PO<sub>4</sub>)<sub>2</sub> in order to characterize this
unusual magnetic behavior
[Co(H<sub>2</sub>O)<sub>6</sub>]<sub>3</sub>[U<sub>2</sub>O<sub>4</sub>F<sub>7</sub>]<sub>2</sub>: A Model System for Understanding the Formation of Dimensionally Reduced Materials
A cobalt containing mixed-anion uranyl
oxide-fluoride was synthesized
using a mild hydrothermal crystal growth method. The uranyl ions are
condensed into a one-dimensional chain motif separated by isolated
cobalt hexa-aqua centers. The 1-D uranyl material was characterized
by single-crystal and powder X-ray diffraction. The optical, thermal,
and magnetic properties were studied and are reported herein. Using
the reported composition as a model, a system was derived to predict
the dimensionality of hypothetical structures to advance our ability
to rationally predict solid-state materials
Understanding the Formation of Salt-Inclusion Phases: An Enhanced Flux Growth Method for the Targeted Synthesis of Salt-Inclusion Cesium Halide Uranyl Silicates
Salt-inclusion
compounds (SICs) are known for their structural
diversity and their potential applications, including luminescence
and radioactive waste storage forms. Currently, the majority of salt-inclusion
phases are grown serendipitously and the targeted growth of SICs has
met with only moderate success. We report an enhanced flux growth
method for the targeted growth of SICs. Specifically, the use of (1)
metal halide reagents and (2) reactions with small surface area to
volume ratios are found to favor the growth of salt-inclusion compounds
over pure oxides and thus enable a more targeted synthetic route for
their preparation. The Cs–X–U–Si–O (X
= F, Cl) pentanary phase space is used as a model system to demonstrate
the generality of this enhanced flux method approach. Single crystals
of four new salt-inclusion uranyl silicates, [Cs<sub>3</sub>F]Â[(UO<sub>2</sub>)Â(Si<sub>4</sub>O<sub>10</sub>)], [Cs<sub>2</sub>Cs<sub>5</sub>F]Â[(UO<sub>2</sub>)<sub>2</sub>(Si<sub>6</sub>O<sub>17</sub>)], [Cs<sub>9</sub>Cs<sub>6</sub>Cl]Â[(UO<sub>2</sub>)<sub>7</sub>(Si<sub>6</sub>O<sub>17</sub>)<sub>2</sub>(Si<sub>4</sub>O<sub>12</sub>)], and [Cs<sub>2</sub>Cs<sub>5</sub>F]Â[(UO<sub>2</sub>)<sub>3</sub>(Si<sub>2</sub>O<sub>7</sub>)<sub>2</sub>], were grown using this enhanced flux
growth method. A detailed discussion of the factors that favor salt-inclusion
phases during synthesis and why specifically uranyl silicates make
excellent frameworks for salt-inclusion phases is given
A Family of A‑Site Cation-Deficient Double-Perovskite-Related Iridates: Ln<sub>9</sub>Sr<sub>2</sub>Ir<sub>4</sub>O<sub>24</sub> (Ln = La, Pr, Nd, Sm)
The
compositions of the general formula Ln<sub>11–<i>x</i></sub>Sr<sub><i>x</i></sub>Ir<sub>4</sub>O<sub>24</sub> (Ln = La, Pr, Nd, Sm; 1.37 ≥ <i>x</i> ≥
2) belonging to a family of A-site cation-deficient double-perovskite-related
oxide iridates were grown as highly faceted single crystals from a
molten strontium chloride flux. Their structures were determined by
single-crystal X-ray diffraction. On the basis of the single-crystal
results, additional compositions, Ln<sub>9</sub>Sr<sub>2</sub>Ir<sub>4</sub>O<sub>24</sub> (Ln = La, Pr, Nd, Sm), were prepared as polycrystalline
powders via solid-state reactions and structurally characterized by
Rietveld refinement. The compositions Ln<sub>9</sub>Sr<sub>2</sub>Ir<sub>4</sub>O<sub>24</sub> (Ln = La, Pr, Nd, Sm) contain IrÂ(V)
and IrÂ(IV) in a 1:3 ratio with an average iridium oxidation state
of 4.25. The single-crystal compositions La<sub>9.15</sub>Sr<sub>1.85</sub>Ir<sub>4</sub>O<sub>24</sub> and Pr<sub>9.63</sub>Sr<sub>1.37</sub>Ir<sub>4</sub>O<sub>24</sub> contain relatively less IrÂ(V), with
the average iridium oxidation states being 4.21 and 4.09, respectively.
The magnetic properties of Ln<sub>9</sub>Sr<sub>2</sub>Ir<sub>4</sub>O<sub>24</sub> (Ln = La, Pr, Nd, Sm) were measured, and complex magnetic
behavior was observed in all cases at temperatures below 30 K
Synthetic Strategies for the Synthesis of Ternary Uranium(IV) and Thorium(IV) Fluorides
A series of new UÂ(IV)
and ThÂ(IV) fluorides, Na<sub>7</sub>U<sub>6</sub>F<sub>31</sub> (<b>1</b>), NaUF<sub>5</sub> (<b>2</b>), NaU<sub>2</sub>F<sub>9</sub> (<b>3</b>), KTh<sub>2</sub>F<sub>9</sub> (<b>4</b>), NaTh<sub>2</sub>F<sub>9</sub> (<b>5</b>), (H<sub>3</sub>O)ÂTh<sub>3</sub>F<sub>13</sub> (<b>6</b>), and (H<sub>3</sub>O)ÂU<sub>3</sub>F<sub>13</sub> (<b>7</b>), was obtained using
hydrothermal and low-temperature flux methods. Mild hydrothermal reactions
with uranyl acetate as a precursor yielded <b>1</b>, <b>7</b>, and the monoclinic polymorph of NaU<sub>2</sub>F<sub>9</sub>, whereas
direct reactions between UF<sub>4</sub> and NaF led to the formation
of <b>2</b> and orthorhombic NaU<sub>2</sub>F<sub>9</sub> (<b>3</b>). This highlights an unexpected difference in reaction products
when different starting uranium sources are used. All seven compounds
were characterized by single-crystal X-ray diffraction, and their
structures are compared on the basis of cation topology, revealing
a close topological resemblance between fluorides on the basis of
the layers observed in NaUF<sub>5</sub>(H<sub>2</sub>O). Phase-pure
samples of <b>1</b>, <b>2</b>, and both polymorphs of
NaU<sub>2</sub>F<sub>9</sub> were obtained, and their spectroscopic
and magnetic properties were measured. The UV–vis data are
dominated by the presence of U<sup>4+</sup> cations and agree well
with the electronic transitions. Effective magnetic moments of the
studied compounds were found to range from 3.08 to 3.59 ÎĽ<sub>B</sub>
Flux versus Hydrothermal Growth: Polymorphism of A<sub>2</sub>(UO<sub>2</sub>)Si<sub>2</sub>O<sub>6</sub> (A = Rb, Cs)
Single
crystals of two new uranyl silicates were grown from mixed alkali
fluoride/alkali chloride fluxes. Polymorphism is observed in Cs<sub>2</sub>(UO<sub>2</sub>)ÂSi<sub>2</sub>O<sub>6</sub>, where hydrothermal
conditions lead to the α polymorph and flux growth favors the
β polymorph. Rb<sub>2</sub>(UO<sub>2</sub>)ÂSi<sub>2</sub>O<sub>6</sub> crystallizes in a monoclinic distortion of the α-Cs<sub>2</sub>(UO<sub>2</sub>)ÂSi<sub>2</sub>O<sub>6</sub> structure type
with space group <i>I</i>2/<i>a</i> and lattice
parameters <i>a</i> = 14.9932(5) Ă…, <i>b</i> = 14.8032(5) Ă…, <i>c</i> = 16.2377(9) Ă…, and
β = 90.7220(10)°. β-Cs<sub>2</sub>(UO<sub>2</sub>)ÂSi<sub>2</sub>O<sub>6</sub> constitutes a new polymorph of Cs<sub>2</sub>(UO<sub>2</sub>)ÂSi<sub>2</sub>O<sub>6</sub> and crystallizes
in the monoclinic space group <i>C</i>2 with lattice parameters <i>a</i> = 12.136(2) Å, <i>b</i> = 10.0426(17) Å, <i>c</i> = 7.7896(13) Å, and β = 95.849(4)°. The
two structures are compared, the driving force behind the observed
polymorphism is discussed, and the luminescence properties are reported
for each compound
Breaking a Paradigm: Observation of Magnetic Order in the Purple U(IV) Phosphite: U(HPO<sub>3</sub>)<sub>2</sub>
The
hydrothermal crystal growth of a new uranium phosphite, UÂ(HPO<sub>3</sub>)<sub>2</sub>, is reported. This material was found to exhibit
optical and magnetic properties not commonly observed in UÂ(IV) containing
materials, specifically purple coloration and low temperature magnetism.
We discuss the synthesis, structure determination, and characterization
of the title compound and comment on its optical, thermal, and magnetic
properties. The magnetic behavior is consistent with frustrated antiferromagnetism
that arises from the hexagonal honeycomb lattice of UÂ(IV) ions. This
material gives rare evidence for UÂ(IV) ions participating in magnetic
order
Hydroflux Crystal Growth of Platinum Group Metal Hydroxides: Sr<sub>6</sub>NaPd<sub>2</sub>(OH)<sub>17</sub>, Li<sub>2</sub>Pt(OH)<sub>6</sub>, Na<sub>2</sub>Pt(OH)<sub>6</sub>, Sr<sub>2</sub>Pt(OH)<sub>8</sub>, and Ba<sub>2</sub>Pt(OH)<sub>8</sub>
Crystals of five
complex metal hydroxides containing platinum group metals were grown
by a novel low-temperature hydroflux technique, a hybrid approach
between the aqueous hydrothermal and the molten hydroxide flux techniques.
Sr<sub>6</sub>NaPd<sub>2</sub>(OH)<sub>17</sub> (<b>1</b>) crystallizes
in orthorhombic space group <i>Pbcn</i> with lattice parameters <i>a</i> = 19.577(4) Ă…, <i>b</i> = 13.521(3) Ă…,
and <i>c</i> = 6.885(1) Ă…. This compound has a three-dimensional
framework structure with SrÂ(OH)<sub><i>n</i></sub> polyhedra,
NaÂ(OH)<sub>6</sub> octahedra, and PdÂ(OH)<sub>4</sub> square planes.
Isostructural phases Li<sub>2</sub>PtÂ(OH)<sub>6</sub> (<b>2</b>) and Na<sub>2</sub>PtÂ(OH)<sub>6</sub> (<b>3</b>) crystallize
in trigonal space group <i>P</i>-3 with lattice parameters
of <i>a</i> = 5.3406(8) Ă… and <i>c</i> =
4.5684(9) Ă… and <i>a</i> = 5.7984(8) Ă… and <i>c</i> = 4.6755(9) Ă…, respectively. Structures of these
materials consist of layers of AÂ(OH)<sub>6</sub> (A = Li (<b>2</b>), Na (<b>3</b>)) and PtÂ(OH)<sub>6</sub> octahedra. Sr<sub>2</sub>PtÂ(OH)<sub>8</sub> (<b>4</b>) crystallizes in monoclinic
space group <i>P</i>2<sub>1</sub>/<i>c</i> with
lattice parameters <i>a</i> = 5.9717(6) Ă…, <i>b</i> = 10.997(1) Ă…, <i>c</i> = 6.0158(6) Ă…,
and β = 113.155(2)°, while Ba<sub>2</sub>PtÂ(OH)<sub>8</sub> (<b>5</b>) crystallizes in orthorhombic space group <i>Pbca</i> with lattice parameters <i>a</i> = 8.574(2)
Ă…, <i>b</i> = 8.673(2) Ă…, and <i>c</i> = 10.276(2) Ă…. Both of these compounds have three-dimensional
structures composed of PtÂ(OH)<sub>6</sub> octahedra surrounded by
either SrÂ(OH)<sub>8</sub> or BaÂ(OH)<sub>9</sub> polyhedra. Decomposition
of these materials into condensed metal oxides, which is of importance
to possible catalytic applications, was monitored via thermogravimetric
analysis. For example, Na<sub>2</sub>PtÂ(OH)<sub>6</sub> (<b>3</b>) converts cleanly via dehydration into α-Na<sub>2</sub>PtO<sub>3</sub>
Design and Crystal Growth of Magnetic Double Perovskite Iridates: <i>Ln</i><sub>2</sub>MIrO<sub>6</sub> (<i>Ln</i> = La, Pr, Nd, Sm-Gd; M = Mg, Ni)
A series
of monoclinic distorted double perovskites of the general
formula <i>Ln</i><sub>2</sub>MIrO<sub>6</sub> (<i>Ln</i> = La, Pr, Nd, Sm–Gd; M = Mg, Ni) were grown as highly faceted
single crystals from a potassium hydroxide flux. The structural distortions
and the magnetic interactions in A<sub>2</sub>BB′O<sub>6</sub> double perovskites can be “designed” via a judicious
choice of A, B, and B′ cation sizes and by selecting magnetic
or nonmagnetic ions to occupy the A, B, and/or B′ sites. A
study of the relationship between the number of magnetic ions, the
degree of monoclinic distortion, and the resulting magnetic interactions
was conducted. Magnetic susceptibility and field dependent magnetization
measurements were performed for all synthesized compounds. It was
determined that smaller A-site lanthanide cations cause more pronounced
monoclinic distortions, resulting in smaller M–O–Ir
(M = Mg, Ni) bond angles that correlate with higher magnetic ordering
temperatures. The magnetic susceptibility and field dependent magnetization
data were both consistent with canted antiferromagnetism for most
titled compositions, indicating a possible trend of increased spin
canting, and thus increased ferromagnetic-like interactions, as a
function of smaller lanthanide A site cation size
Flux Crystal Growth and Optical Properties of Two Uranium-Containing Silicates: <i>A</i><sub>2</sub>USiO<sub>6</sub> (<i>A</i> = Cs, Rb)
Single crystals of
two uranium silicates, Cs<sub>2</sub>USiO<sub>6</sub> and Rb<sub>2</sub>USiO<sub>6</sub>, have been grown from
molten fluoride fluxes and structurally characterized by single-crystal
X-ray diffraction. Cs<sub>2</sub>USiO<sub>6</sub> crystallizes in
the body-centered orthorhombic space group, <i>Immm</i>,
with <i>a</i> = 8.5812(4) Ă…, <i>b</i> = 13.0011(6)
Ă…, and <i>c</i> = 13.8811(7) Ă…. The size of Rb
is slightly too small to fit into this structural framework without
effecting slight structural changes that result in a 6-fold superstructure.
Sharp satellite peaks were observed in the single-crystal X-ray diffraction
data, indicating the existing of a superstructure. The crystals were
examined by electron diffraction, the results of which suggest that
the structure can be thought of as the <i>Immm</i> isotype
(<i>a</i> = 8.4916(6) Ă…, <i>b</i> = 12.6678(9)
Ă…, and <i>c</i> = 13.5077(9) Ă…) on average, with
an approximately 6-fold superstructure along the <i>c</i> axis. The materials were further characterized by UV–vis
reflectance spectroscopy