Two‐ion anisotropic interaction from band f electron hybridization and magnetic ordering in uranium intermetallics
暂无分享,去创建一个
We have generalized the Coqblin‐Schrieffer type two‐ion anisotropic interaction to f2 and f3 configurations (U4+ and U3+). This interaction between ions occurs via the hybridization with the intervening sea of band electrons (i.e., via resonant mixing at each site with f component of band electrons when expressed in spherical waves about that site). With the addition of small antiferromagnetic Heisenberg (isotropic Ruderman‐Kittel) interaction and crystal‐field interaction, we obtain a 2k noncollinear ground state with a type I collinear antiferromagnetic state at slightly higher energy. It appears likely that this ordering of states will provide a transition with increasing temperature from a noncollinear 2k magnetic structure to a type I collinear structure as observed experimentally in UP and UAs.
[1] J. Rossat-Mignod,et al. Magnetic ordering in cerium and uranium monopnictides , 1980 .
[2] B. Cooper,et al. Planar Coupling Mechanism Explaining Anomalous Magnetic Structures in Cerium and Actinide Intermetallics , 1980 .
[3] J. Schrieffer,et al. EXCHANGE INTERACTION IN ALLOYS WITH CERIUM IMPURITIES. , 1969 .
[4] N. A. Curry. The magnetic structure of uranium monophosphide , 1966 .