Crystal Chemistry and Magnetism of Ternary Actinoid Boron Carbides UB 1- xC 1+ x and U 1- xMxB 2C with M = Sc, Lu, and Th

Abstract

Within the homogeneous range of uranium monocarbide UB 1- x C 1+ x , the crystal structures of stoichiometric UBC and of the carbon-rich solid solution UB 0.78C 1.22, have been refined from single-crystal X-ray counter data. From X-ray analysis crystal symmetry in both cases is consistent with the centro-symmetric space group Cmcm and there are no indications of superstructure formation. In contrast to the fully ordered atom arrangement revealed for stoichiometric UBC ( a = 0.35899(4), b = 1.19781(12), c = 0.33474(3) nm), random occupation by boron and carbon atoms is observed for the boron site in UB 0.78C 1.22 ( a = 0.35752(4), b = 1.18584(3), c = 0.33881(4) nm). For 279(278) reflections (|F 0| > 3σ) the obtained reliability factors R x = ∑|ΔF|/∑| F 0| were R x = 0.069 for UBC and R x = 0.050 for UB 0.78C 1.22. Neutron powder diffraction experiments at 9 and 295 K unambiguously revealed full occupancy by the nonmetal atoms in UB 0.78C 1.22 and prove the statistical occupation of B and C atoms in the B-sites. For the orthorhombic symmetry Cmcm, refinement was not better than R 1 = 0.044. A model calculation in monoclinic symmetry C12/ m1, however, resulted in a significant reduction of the residual value to R 1 = 0.030, releasing spatial constraints on the boron atoms. Thus the boron-boron chain in Cmcm (B-B = 0.1874 nm) is dissolved into boron pairs (B-B = 0.1706 nm) which are loosely bound at a distance of 0.2043 nm. The formation of C-B-B-C groups corresponds to the structure types of ThBC and Th 3B 2C 3. The magnetic behavior has been investigated in the temperature range from 4.2 K to 1000 K for UB 1- x C 1+ x (UBC-type) and U 1- x M x B 2C (ThB 2C-type for the high temperature modification and 1-UB 2C-type for the low temperature modification) with U partially substituted by Th or Sc, Lu. From magnetic susceptibilities, the alloys UB 1- x C 1+ x reveal temperature independent paramagnetism with typical intermediate valence fluctuation behavior ( T SF ∼ 350 K). ThB 2C and 1-UB 2C both are temperature independent paramagnets, whereas h-UB 2C is a ferromagnet with the rather high Curie temperature T M = 80(2) K. T M and the saturation magnetiziation per U atom both successively decrease on substitution of U by Th, Sc, or Lu in UB 2C, whereas the U-moments remain practically unchanged at μ eff(U) ∼ 1.9 μ B. Uranium L 3-XANES (X-ray Absorption Near Edge Structure) spectroscopy revealed increased d-band localization, comparable to uranium-transition metal alloys, in nonmagnetic UB 1- x C 1+ x ( x = 0, 0.22). No superconductivity was observed down to 1.5 K; no hydrogen uptake was observed for UB 2C and ThB 2C even under hydrogen pressures as high as 7 × 10 7 Pa at 670 K.