3 research outputs found
Syntheses, Crystal Structures, Transport Properties, and Theoretical Studies of Five Members of the MAn(2)Q(5) Family: SrU2S5, BaU2Se5, PbU2S5, BaTh2S5, and BaU2Te5
International audienceFive compounds of the MAn(2)Q(5) family, namely, SrU2S5, BaU2Se5, PbU2S5, BaTh2S5, and BaU2Te5, have been synthesized by high-temperature solid-state reactions. The crystal structures of these compounds were determined by single-crystal X-ray diffraction studies. SrU2S5, BaU2Se5, PbU2S5, and BaTh2S5 crystallize in the PbU2Se5 structure type in space group C(2)h(5)P(21)/c of the monoclinic system, whereas BaU2Te5 adopts the (NH4)Pb2Br5 structure type in space group D(4)h(18)I(4/mcm) of the tetragonal system. There are no QQ bonds in these structures, so the formulas charge balance as M2+(An(2)(4+)Q(5)(2). The An atoms in the monoclinic structure are seven- or eight-coordinated by Q atoms; the U atoms in the tetragonal structure are eight-coordinated. The M atoms in the monoclinic structure are coordinated to either eight or nine Q atoms, depending on the monoclinic beta angle; the M atoms in the tetragonal structure are 10-coordinated. Resistivity studies on single crystals of SrU2S5, BaU2Se5, and PbU2S5 show metallic behavior with resistivities of 0.24, 10, and 3.3 mO.cm, respectively, at 298 K. Spin-polarized density functional theory in the generalized gradient approximation applied to the four U compounds suggests that they are ferromagnetic. In each compound, the density of states of one spin channel is found to be finite at the Fermi level, whereas there is a gap in the density of states of the other spin channel; this is characteristic of a half-metal
Syntheses, Crystal Structures, Transport Properties, and Theoretical Studies of Five Members of the MAn<sub>2</sub>Q<sub>5</sub> Family: SrU<sub>2</sub>S<sub>5</sub>, BaU<sub>2</sub>Se<sub>5</sub>, PbU<sub>2</sub>S<sub>5</sub>, BaTh<sub>2</sub>S<sub>5</sub>, and BaU<sub>2</sub>Te<sub>5</sub>
Five compounds of the MAn<sub>2</sub>Q<sub>5</sub> family, namely, SrU<sub>2</sub>S<sub>5</sub>, BaU<sub>2</sub>Se<sub>5</sub>, PbU<sub>2</sub>S<sub>5</sub>, BaTh<sub>2</sub>S<sub>5</sub>, and BaU<sub>2</sub>Te<sub>5</sub>, have been synthesized
by high-temperature solid-state reactions. The crystal structures
of these compounds were determined by single-crystal X-ray diffraction
studies. SrU<sub>2</sub>S<sub>5</sub>, BaU<sub>2</sub>Se<sub>5</sub>, PbU<sub>2</sub>S<sub>5</sub>, and BaTh<sub>2</sub>S<sub>5</sub> crystallize in the PbU<sub>2</sub>Se<sub>5</sub> structure type
in space group <i>C</i><sub>2<i>h</i></sub><sup>5</sup>–<i>P</i>2<sub>1</sub>/<i>c</i> of the monoclinic system, whereas BaU<sub>2</sub>Te<sub>5</sub> adopts the (NH<sub>4</sub>)Pb<sub>2</sub>Br<sub>5</sub> structure type in space group <i>D</i><sub>4<i>h</i></sub><sup>18</sup>–<i>I</i>4/<i>mcm</i> of the tetragonal
system. There are no Q–Q bonds in these structures, so the
formulas charge balance as M<sup>2+</sup>(An<sup>4+</sup>)<sub>2</sub>(Q<sup>2–</sup>)<sub>5</sub>. The An atoms in the monoclinic
structure are seven- or eight-coordinated by Q atoms; the U atoms
in the tetragonal structure are eight-coordinated. The M atoms in
the monoclinic structure are coordinated to either eight or nine Q
atoms, depending on the monoclinic β angle; the M atoms in the
tetragonal structure are 10-coordinated. Resistivity studies
on single crystals of SrU<sub>2</sub>S<sub>5</sub>, BaU<sub>2</sub>Se<sub>5</sub>, and PbU<sub>2</sub>S<sub>5</sub> show metallic behavior
with resistivities of 0.24, 10, and 3.3 mΩ·cm, respectively,
at 298 K. Spin-polarized density functional theory in the generalized
gradient approximation applied to the four U compounds suggests that
they are ferromagnetic. In each compound, the density of states of
one spin channel is found to be finite at the Fermi level, whereas
there is a gap in the density of states of the other spin channel;
this is characteristic of a half-metal
Positional Flexibility: Syntheses and Characterization of Six Uranium Chalcogenides Related to the 2H Hexagonal Perovskite Family
International audienceSix new uranium chalcogenides, Ba4USe6, Ba3FeUSe6, Ba3MnUSe6, Ba3MnUS6, Ba3.3Rb0.7US6, and Ba3.2K0.8US6, related to the 2H hexagonal perovskite family have been synthesized by solid-state methods at 1173 K. These isostructural compounds crystallize in the K4CdCl6 structure type in space group D-3d(6) R3 (\₎c of the trigonal system with six formula units per cell. This structure type is remarkably flexible. The structures of Ba3FeUSe6, Ba3MnUSe6, and Ba3MnUS6 consist of infinite (1)(infinity)[MUQ(6) (6-)] chains (M = Fe or Mn; Q = S or Se) oriented along the c axis that are separated by Ba atoms. These chains are composed of alternating M-centered octahedra and U-centered trigonal prisms sharing triangular faces; in contrast, in the structures of Ba4USe6, Ba3.3Rb0.7US6, and Ba3.2K0.8US6, there are U-centered octahedra alternating with Ba-, Rb-, or K-centered trigonal prisms. Moreover, the Ba4USe6, Ba3FeUSe6, Ba3MnUSe6, and Ba3MnUS6 compounds contain U4+, whereas Ba3.3Rb0.7US6 and Ba3.2K0.8US6 are mixed U4+/5+ compounds. Resistivity and mu-Raman spectroscopic measurements and DFT calculations provide additional insight into these interesting subtle structural variations