Magnetic, thermal, and transport properties of single-crystalline U3Fe4Ge4
► U3Fe4Ge4 represents pure uranium magnetism as iron has no ordered magnetic moment. ► Magnetic, thermal, and transport properties were studied on a U3Fe4Ge4 single crystal. ► U3Fe4Ge4 is a strongly itinerant 5f ferromagnet. ► A strong easy-axis anisotropy is observed that results in a gap excitatio...
Saved in:
Published in | Journal of alloys and compounds Vol. 555; pp. 304 - 310 |
---|---|
Main Authors | , , , , , , |
Format | Journal Article |
Language | English |
Published |
Elsevier B.V
05.04.2013
|
Subjects | |
Online Access | Get full text |
Cover
Loading…
Summary: | ► U3Fe4Ge4 represents pure uranium magnetism as iron has no ordered magnetic moment. ► Magnetic, thermal, and transport properties were studied on a U3Fe4Ge4 single crystal. ► U3Fe4Ge4 is a strongly itinerant 5f ferromagnet. ► A strong easy-axis anisotropy is observed that results in a gap excitation behavior.
Magnetic, thermal, and transport properties of a U3Fe4Ge4 single crystal have been studied. The compound crystallizes in the orthorhombic Gd3Cu4Ge4 structure type. U3Fe4Ge4 displays ferromagnetic order below the Curie temperature TC=18K. The magnetism originates from the uranium sublattice, as iron atoms have no ordered magnetic moments. U3Fe4Ge4 exhibits a pronounced easy-axis anisotropy with the anisotropy field exceeding 60T. The spontaneous magnetic moment is Ms=1.2μB/f.u. at T=2K. Magnetic contribution to specific heat shows a gap excitation behavior with Δ=4meV, which can be related to the magnon gap due to the anisotropy. The Sommerfeld coefficient of the electronic specific heat is γ=57mJ/(mol-UK2) in the ordered state, whereas it is much higher (145mJ/(mol-UK2) if derived from the paramagnetic state. Electrical resistivity has very high values on the mΩcm range. |
---|---|
Bibliography: | ObjectType-Article-2 SourceType-Scholarly Journals-1 ObjectType-Feature-1 content type line 23 |
ISSN: | 0925-8388 1873-4669 |
DOI: | 10.1016/j.jallcom.2012.12.092 |