학술논문

Transport properties in amorphous U/sub x/-T/sub 1//sub -//sub x/ films (T = Fe, Ni, Gd, Tb, and Yb) (invited)
Document Type
Journal Article
Author
Source
J. Appl. Phys.; (United States); 64:10
Subject
36 MATERIALS SCIENCE GADOLINIUM ALLOYS
MAGNETORESISTANCE
IRON ALLOYS
NICKEL ALLOYS
TERBIUM ALLOYS
URANIUM ALLOYS
YTTERBIUM ALLOYS
AMORPHOUS STATE
ANISOTROPY
ELECTRIC CONDUCTIVITY
FERROMAGNETIC MATERIALS
SPIN GLASS STATE
TEMPERATURE DEPENDENCE
THIN FILMS
ACTINIDE ALLOYS
ALLOYS
ELECTRICAL PROPERTIES
FILMS
MAGNETIC MATERIALS
MATERIALS
PHYSICAL PROPERTIES
RARE EARTH ALLOYS 360104* -- Metals & Alloys-- Physical Properties
Language
English
Abstract
We describe the competing magnetic, localization, and phonon effects on the transport properties of amorphous magnetic U/sub x/T/sub 1-//sub x/ films, with T = Fe, Ni, Gd, Tb, and Yb. Amorphous U/sub x/Fe/sub 1-//sub x/ films change from collinear to random ferromagnetism as x increases, and the temperature dependence of the resistivity denotes the competing effects of spin-flip and non-spin-flip exchange scattering processes. The resistivity has a minimum at T/sub f/ rising sharply below this temperature. The sign of the magnetic resistivity and the magnetoresistance indicates >0, while the anisotropic magnetoresistance indicates a local exchange gap. Amorphous U/sub x/Gd/sub 1-//sub x/ and a-U/sub x/Tb/sub 1-//sub x/ are, respectively, spin glasses and random anisotropy dominated systems. The resistivity increases smoothly through T/sub f/ and has a slight upturn at low temperatures that we associate with weak localization. The magnetoresistance is negative in both systems and the anisotropic magnetoresistance is null, although the applied field induces anisotropic behavior in the Tb containing films (asperomagnets). All samples show quadratic and positive field dependence of magnetoresistance well inside the paramagnetic regime, and a linear regime below T/sub f/. At low temperatures and in the a-U/sub x/Gd/sub 1-//sub x/ films, negative (H)/sup 1/2/ and H/sup 2/ regimes occur and are associated with weak localization processes dominated by the inelastic mean free path.