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Superconductivity and spin fluctuations in the actinoid-platinum metal borides {Th, U} Pt sub(3) B
Investigating the phase relations of the system {Th, U}-Pt-B at 900[degrees]C the formation of two compounds has been observed: cubic ThPt sub(3) B with Pm3m structure as a representative of the perovskites, and tetragonal UPt sub(3) B with P4mm structure being isotypic to the noncentrosymmetric str...
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Published in: | Physical review. B, Condensed matter and materials physics Condensed matter and materials physics, 2015-07, Vol.92 (2) |
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Main Authors: | , , , , , , , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Online Access: | Get full text |
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Summary: | Investigating the phase relations of the system {Th, U}-Pt-B at 900[degrees]C the formation of two compounds has been observed: cubic ThPt sub(3) B with Pm3m structure as a representative of the perovskites, and tetragonal UPt sub(3) B with P4mm structure being isotypic to the noncentrosymmetric structure of CePt sub(3) B. The crystal structures of the two compounds are defined by combined x-ray diffraction and transmission electron microscopy. Characterization of physical properties for ThPt sub(3) B reveals a superconducting transition at 0.75 K and an upper critical field at T = 0 exceeding 0.4 T. For nonsuperconducting UPt sub(3) B a metallic resistivity behavior was found in the entire temperature range; at very low temperatures spin fluctuations become evident and the resistivity [rho](T) follows non-Fermi liquid characteristics, [rho] = [rho] sub(0) + AT super(n)with n = 1.6. Density functional theory (DFT) calculations were performed for both compounds for both types of structures. They predict that the experimentally claimed cubic structure of ThPt sub(3) B is thermodynamically not stable in comparison to a tetragonal phase, with a very large enthalpy difference of 25 kJ/mol, which cannot be explained by the formation energy of B vacancies. However, the presence of random boron vacancies possibly stabilizes the cubic structure via a local strain compensation mechanism during the growth of the crystal. For UPt sub(3) B the DFT results agree well with the experimental findings. |
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ISSN: | 1098-0121 1550-235X |