47 research outputs found

    Retention of a Paramagnetic Ground State at Low Temperatures in a Family of Structurally Related U<sup>IV</sup> Phosphates

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    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>O­(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 U­(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

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    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

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    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]­[(UO<sub>2</sub>)­(Si<sub>4</sub>O<sub>10</sub>)], [Cs<sub>2</sub>Cs<sub>5</sub>F]­[(UO<sub>2</sub>)<sub>2</sub>(Si<sub>6</sub>O<sub>17</sub>)], [Cs<sub>9</sub>Cs<sub>6</sub>Cl]­[(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]­[(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)

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    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 Ir­(V) and Ir­(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 Ir­(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

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    A series of new U­(IV) and Th­(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)­Th<sub>3</sub>F<sub>13</sub> (<b>6</b>), and (H<sub>3</sub>O)­U<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 μ<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)

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    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>)­Si<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>)­Si<sub>2</sub>O<sub>6</sub> crystallizes in a monoclinic distortion of the α-Cs<sub>2</sub>(UO<sub>2</sub>)­Si<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) Å, <i>b</i> = 14.8032(5) Å, <i>c</i> = 16.2377(9) Å, and β = 90.7220(10)°. β-Cs<sub>2</sub>(UO<sub>2</sub>)­Si<sub>2</sub>O<sub>6</sub> constitutes a new polymorph of Cs<sub>2</sub>(UO<sub>2</sub>)­Si<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>

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    The hydrothermal crystal growth of a new uranium phosphite, U­(HPO<sub>3</sub>)<sub>2</sub>, is reported. This material was found to exhibit optical and magnetic properties not commonly observed in U­(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 U­(IV) ions. This material gives rare evidence for U­(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>

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    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) Å, <i>b</i> = 13.521(3) Å, and <i>c</i> = 6.885(1) Å. This compound has a three-dimensional framework structure with Sr­(OH)<sub><i>n</i></sub> polyhedra, Na­(OH)<sub>6</sub> octahedra, and Pd­(OH)<sub>4</sub> square planes. Isostructural phases Li<sub>2</sub>Pt­(OH)<sub>6</sub> (<b>2</b>) and Na<sub>2</sub>Pt­(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) Å and <i>c</i> = 4.5684(9) Å and <i>a</i> = 5.7984(8) Å and <i>c</i> = 4.6755(9) Å, respectively. Structures of these materials consist of layers of A­(OH)<sub>6</sub> (A = Li (<b>2</b>), Na (<b>3</b>)) and Pt­(OH)<sub>6</sub> octahedra. Sr<sub>2</sub>Pt­(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) Å, <i>b</i> = 10.997(1) Å, <i>c</i> = 6.0158(6) Å, and β = 113.155(2)°, while Ba<sub>2</sub>Pt­(OH)<sub>8</sub> (<b>5</b>) crystallizes in orthorhombic space group <i>Pbca</i> with lattice parameters <i>a</i> = 8.574(2) Å, <i>b</i> = 8.673(2) Å, and <i>c</i> = 10.276(2) Å. Both of these compounds have three-dimensional structures composed of Pt­(OH)<sub>6</sub> octahedra surrounded by either Sr­(OH)<sub>8</sub> or Ba­(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>Pt­(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)

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    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)

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    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) Å, <i>b</i> = 13.0011(6) Å, and <i>c</i> = 13.8811(7) Å. 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) Å, <i>b</i> = 12.6678(9) Å, and <i>c</i> = 13.5077(9) Å) on average, with an approximately 6-fold superstructure along the <i>c</i> axis. The materials were further characterized by UV–vis reflectance spectroscopy
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