A novel ternary uranium-based intermetallic U34Fe4−xGe33: Structure and physical properties
Creators
- 1. Campus Tecnológico e Nuclear, Instituto Superior Técnico, Universidade de Lisboa, CFMC-UL, Estrada Nacional 10, 2695-066 Bobadela (Portugal)
- 2. CRISMAT, UMR CNRS 6508, 6 bd. Maréchal Juin, 14050 Caen (France)
- 3. Institut des Sciences Chimiques de Rennes, Chimie du Solide et Matériaux, Université Rennes 1, UMR CNRS 6226, 263 Avenue du Général Leclerc, 35042 Rennes (France)
Description
Highlights: • A new uranium intermetallic compound U34Fe4−xge33 was prepared and characterized. • It crystallizes in the tetragonal system with an original structure-type. • U lattice stacking is made of cupolae, orthobicupola and irregular cubes. • U34Fe4−xGe33 orders magnetically at TC = 28 K, with pure U magnetism. • TC and electrical resistivity increase with applied magnetic field. - Abstract: The new ternary phase U34Fe4−xGe33 has been synthesized and characterized by means of single crystal X-ray diffraction, magnetization, Mössbauer spectroscopy, specific heat, electrical resistivity, magnetoresistivity and thermopower measurements. It crystallizes in its own tetragonal structure type which can be described as derived from the one of the binary USi (U34Si34.5 structure-type, space group I4/mmm), with lattice parameters at room temperature, a = 10.873(5) Å and c = 25.274(3) Å. Structure refinement confirmed six inequivalent U atoms, occupying sites with dissimilar coordination, the Ge atoms staying on seven positions and Fe on two positions, one of the Fe sites with a partial occupancy. The U sub-lattice is composed by the stacking of a square cupola, two distorted cubes and a square orthobicupola. U34Fe4−xGe33 with x = 0.68 undergoes a ferromagnetic-type transition below 28 K. Mössbauer spectroscopy shows that the magnetism is ruled by the U sub-lattice, as Fe atoms have no ordered moments. The Sommerfeld coefficient of the electronic specific heat is γ = 131 mJ/(molU K2), whereas the estimated magnetic entropy at TC is 0.22Rln2. A residual resistivity of 314 μΩ cm and a resistivity ratio of 1.1 were found in the electrical resistivity curve, which also exhibits an upturn below TC that shifts towards higher temperatures with the applied magnetic field. This behavior may be related to some disorder in the non-magnetic lattice and/or partial ordering of the magnetic lattice
Availability note (English)
Available from http://dx.doi.org/10.1016/j.jallcom.2014.03.189Additional details
Identifiers
- DOI
- 10.1016/j.jallcom.2014.03.189;
- PII
- S0925-8388(14)00813-5;
Publishing Information
- Journal Title
- Journal of Alloys and Compounds
- Journal Volume
- 606
- Journal Page Range
- p. 154-163
- ISSN
- 0925-8388
- CODEN
- JALCEU
INIS
- Country of Publication
- Netherlands
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 46060953
- Subject category
- S36: MATERIALS SCIENCE;
- Descriptors DEI
- ALLOYS; ELECTRIC CONDUCTIVITY; ENTROPY; LATTICE PARAMETERS; MAGNETIC FIELDS; MAGNETISM; MAGNETIZATION; MONOCRYSTALS; SPACE GROUPS; SPECTROSCOPY; TETRAGONAL LATTICES; URANIUM; X-RAY DIFFRACTION
- Descriptors DEC
- ACTINIDES; COHERENT SCATTERING; CRYSTAL LATTICES; CRYSTAL STRUCTURE; CRYSTALS; DIFFRACTION; ELECTRICAL PROPERTIES; ELEMENTS; METALS; PHYSICAL PROPERTIES; SCATTERING; SYMMETRY GROUPS; THERMODYNAMIC PROPERTIES
Optional Information
- Copyright
- Copyright (c) 2014 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.