TY - JOUR
T1 - Magnetism and hyperfine interactions in EuM2Ge2 and GdM2Ge2(M = Mn, Fe, Co, Ni, Cu)
AU - Felner, Israel
AU - Nowik, Israel
PY - 1978
Y1 - 1978
N2 - X-ray, magnetic susceptibility and 151Eu, 155Gd Mössbauer effect studies of EuM2Ge2 and GdM2Ge2 were performed. All compounds crystallize in the ThCr2Si2 body centered tetragonal structure. In all compounds, except those with M = Mn and in EuM2Ge2, the M component carries no magnetic moment. All compounds except those with Mn are antiferromagnetic at low temperatures. In EuMn2Ge2 the Mn moments order ferromagnetically at 330 K and change to antiferromagnetic order when the Eu moments order ferromagnetically (9 K). This behaviour is different from that in GdMn2Ge2, where the Mn sublattice orders antiferromagnetically at 365 K and becomes ferromagnetic and antiparallel to the ferromagnetic Gd sublattice at 96 K. The Mössbauer studies of 151Eu and 151Gd provide values for the magnetic hyperfine fields, the quadrupole interactions and the orientation of the magnetic moments relative to the local fourfold axis (c-axis). It turns out that in the Eu compounds the easy axis of magnetization is close to the c-axis, while in the Gd compounds it is in the basal plane. In all systems, excluding those with Mn, the interatomic rare earth-rare earth distances have the dominant effect on the conduction electron charge density and polarization at the rare earth site and on the Curie point.
AB - X-ray, magnetic susceptibility and 151Eu, 155Gd Mössbauer effect studies of EuM2Ge2 and GdM2Ge2 were performed. All compounds crystallize in the ThCr2Si2 body centered tetragonal structure. In all compounds, except those with M = Mn and in EuM2Ge2, the M component carries no magnetic moment. All compounds except those with Mn are antiferromagnetic at low temperatures. In EuMn2Ge2 the Mn moments order ferromagnetically at 330 K and change to antiferromagnetic order when the Eu moments order ferromagnetically (9 K). This behaviour is different from that in GdMn2Ge2, where the Mn sublattice orders antiferromagnetically at 365 K and becomes ferromagnetic and antiparallel to the ferromagnetic Gd sublattice at 96 K. The Mössbauer studies of 151Eu and 151Gd provide values for the magnetic hyperfine fields, the quadrupole interactions and the orientation of the magnetic moments relative to the local fourfold axis (c-axis). It turns out that in the Eu compounds the easy axis of magnetization is close to the c-axis, while in the Gd compounds it is in the basal plane. In all systems, excluding those with Mn, the interatomic rare earth-rare earth distances have the dominant effect on the conduction electron charge density and polarization at the rare earth site and on the Curie point.
UR - http://www.scopus.com/inward/record.url?scp=0000319652&partnerID=8YFLogxK
U2 - 10.1016/0022-3697(78)90012-4
DO - 10.1016/0022-3697(78)90012-4
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AN - SCOPUS:0000319652
SN - 0022-3697
VL - 39
SP - 767
EP - 773
JO - Journal of Physics and Chemistry of Solids
JF - Journal of Physics and Chemistry of Solids
IS - 7
ER -