Published September 5, 2014 | Version v1
Journal article

A novel ternary uranium-based intermetallic U34Fe4−xGe33: Structure and physical properties

  • 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.2014.03.189

Additional 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

Optional Information

Copyright
Copyright (c) 2014 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.