Journal
JOURNAL OF SOLID STATE CHEMISTRY
Volume 183, Issue 10, Pages 2343-2351Publisher
ACADEMIC PRESS INC ELSEVIER SCIENCE
DOI: 10.1016/j.jssc.2010.07.046
Keywords
Rare-earth metal boride carbide; Crystal structure; Electronic structure; Extended Huckel calculations; Rare-earth metal magnetism
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The ternary rare-earth boride carbides R15B4C14 (R=Y, Gd-Lu) were prepared from the elements by arc-melting followed by annealing in silica tubes at 1270 K for 1 month. The crystal structures of Tb15B4C14 and Er15B4C14 were determined from single crystal X-ray diffraction data. They crystallize in a new structure type in space group P4/mnc (Tb15B4C14: a =8.1251(5) angstrom, c=15.861(1) angstrom, Z=2, R-1=0.041 (wR(2)=0.088) for 1023 reflections with I-0 > 2 sigma(I-o); Er15B4C14: a=7.932(1) angstrom, c=15.685(2) angstrom, Z=2, R-1 = 0.037 (wR(2)=0.094) for 1022 reflections with I-o > 2 sigma(I-o)). The crystal structure contains discrete carbon atoms and bent CBC units in octahedra and distorted bicapped square antiprisms, respectively. In both structures the same type of disorder exists. One R atom position needs to be refined as split atom position with a ratio 9:1 indicative of a 10% substitution of the neighboring C4- by C-2(4-). The actual composition has then to be described as R15B4C14.2. The isoelectronic substitution does not change the electron partition of R15B4C14 which can be written as (R3+)(15)(C4-)(6)(CBC5-)(4)center dot(e-). The electronic structure was studied with the extended Huckel method. The investigated compounds Tb15B4C14, Dy15B4C14 and Er15B4C14 are hard ferromagnets with Curie temperatures T-C=145, 120 and 50 K, respectively. The coercive field B-C=3.15 T for Dy15B4C14 is quite remarkable. (C) 2010 Elsevier Inc. All rights reserved.
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