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Title: Magnetism of randomly distributed f atoms in (U{sub 1{minus}x}Nd{sub x})Co{sub 2}Ge{sub 2} solid solutions

Journal Article · · Physical Review, B: Condensed Matter
 [1]; ; ; ;  [1];  [2]
  1. Nuclear Research Centre-Negev, P.O. Box 9001, 84190 Beer-Sheva (Israel)
  2. Ben-Gurion University of the Negev, P.O. Box 653, 84105 Beer-Sheva (Israel)

Solid solutions of the (U{sub 1{minus}x}Nd{sub x})Co{sub 2}Ge{sub 2} system (x=0.25, 0.50, 0.75) are found by neutron diffraction to have tetragonal ThCr{sub 2}Si{sub 2}-type crystal structure (space group I4/mmm), same as their end compounds (x =0, 1). In the solid solutions, U and Nd atoms are randomly distributed in the basal planes. The end compounds and the solid solutions are paramagnetic at room temperature. At 12 K the (U,Nd) sublattice has the antiferromagnetic AF-I magnetic structure [+{minus}+{minus} stacking of ferromagnetic (U,Nd) planes along c], with moments parallel to the c axis. It is found that within a ferromagnetic basal plane the U magnetic moments are parallel to the Nd magnetic moments, unlike (U,Tb), where they are antiparallel. This shows that the {open_quotes}spin charge{close_quotes} rule for lanthanides extends to U-lanthanide systems. Neutron-diffraction and ac-susceptibility results are compared in order to investigate the character of the magnetic transition in the solid solutions. {copyright} {ital 1998} {ital The American Physical Society}

OSTI ID:
565884
Journal Information:
Physical Review, B: Condensed Matter, Vol. 57, Issue 1; Other Information: PBD: Jan 1998
Country of Publication:
United States
Language:
English