Hydrothermal crystallization pathways of amorphous ceric phosphate gels were found to be determined by the ammonia concentration in a reaction medium. This allows for highly selective hydrothermal synthesis of various finely crystal-
Two new cerium(IV) phosphates were obtained: cerium(IV) hydroxidophosphate, Ce(OH)PO4, and cerium(IV) oxidophosphate, Ce2O(PO4)2, which were shown to complement the classes of isostructural compounds M(OH)PO4 and R2O(PO4)2, where M=Th, U and R=Th, U, Np, Zr. Ce2O(PO4)2 oxidophosphate is formed by elimination of H2O from the crystal structure of Ce(OH)PO4 during its thermal decomposition. The structures of Ce(OH)PO4 and Ce2O(PO4)2 are related to each other with the same Cmce space group and similar unit cell parameters (a=6.9691(3) Å, b=9.0655(4) Å, c=12.2214(4) Å, V=772.13(8) Å3, Z=8; a=7.0220(4) Å, b=8.9894(5) Å, c=12.544(1) Å, V=791.8(1) Å3, Z=4, respectively).
Intermetallic compounds
with semiconducting properties are rare,
but they give rise to advanced materials for energy conversion and
saving applications. Here, we present ReGa2Ge, a new electron-precise
narrow-gap intermetallic semiconductor. The compound crystallizes
in the IrIn3 structure type (space group P42/mnm, a = 6.5734(3)
Å, c = 6.7450(8) Å, and Z = 4), where Re atoms occupy the Ir site, while Ga and Ge jointly
populate the In sites. 69,71Ga nuclear quadrupole resonance
spectroscopy indicates nonstatistical partially ordered distribution
of Ga and Ge over two available crystallographic sites; however, the
Ga:Ge ratio is exactly 2:1 without noticeable homogeneity range. The
stoichiometry of ReGa2Ge ensures its precise valence electron
count, which is 17 e– per formula unit. Accordingly,
a narrow energy gap opens up at the Fermi energy in the electronic
structure. Electrical resistivity, Seebeck coefficient, and thermal
conductivity are in agreement with the semiconducting behavior deduced
from the electronic structure calculations and point to prospective
thermoelectric properties at high temperatures. Bonding analysis reveals
dominant covalency in Re–E (E = Ga, Ge) and Re–Re interactions.
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