TY - JOUR
T1 - Magnetic order and hyperfine interactions in RFe6Al6 (R = rare earth)
AU - Felner, I.
AU - Seh, M.
AU - Rakavy, M.
AU - Nowik, I.
PY - 1981
Y1 - 1981
N2 - The systems RFe6Al6(R = Y, Eu, Gd, Tb, Dy, Ho, Er, Tm and Yb) crystallize in the tetragonal body centered I4/mmm structure. In striking contrast to the magnetic behaviour of RFe4Al8 (weakly coupled R and Fe sublattices, complicated magnetic structure, low Tc ~ 130 K), in the RFe6Al6 systems all magnetic sublattices order simultaneously at a relatively high temperature. The magnetization curves start with low values at low temperatures and rise to very high values at Tmax ~ 230 K and then drop to 0 at Tc ~ 330 K. All samples show strong hysteresis effects at temperatures just below Tmax. Mossbauer studies of 57Fe in the (f) and (j) sites and 151Eu, 155Gd, 161Dy, 166Er and 170Yb in the (a) site yield all hyperfine interaction parameters and temperature dependence of the local magnetic moments. All Mossbauer and magnetization experimental results can be explained in a self consistent way with a simple molecular field model. The Fe in the (j) site plays the dominant role in its strong intrasublattice ferromagnetic exchange and its strong antiferromagnetic exchange with the rare earth site. The Fe in the (f) site have an antiferromagnetic intrasublattice exchange, they have a canted strcuture with the ferromagnetic component parallel to the (j) sublattice magnetization.
AB - The systems RFe6Al6(R = Y, Eu, Gd, Tb, Dy, Ho, Er, Tm and Yb) crystallize in the tetragonal body centered I4/mmm structure. In striking contrast to the magnetic behaviour of RFe4Al8 (weakly coupled R and Fe sublattices, complicated magnetic structure, low Tc ~ 130 K), in the RFe6Al6 systems all magnetic sublattices order simultaneously at a relatively high temperature. The magnetization curves start with low values at low temperatures and rise to very high values at Tmax ~ 230 K and then drop to 0 at Tc ~ 330 K. All samples show strong hysteresis effects at temperatures just below Tmax. Mossbauer studies of 57Fe in the (f) and (j) sites and 151Eu, 155Gd, 161Dy, 166Er and 170Yb in the (a) site yield all hyperfine interaction parameters and temperature dependence of the local magnetic moments. All Mossbauer and magnetization experimental results can be explained in a self consistent way with a simple molecular field model. The Fe in the (j) site plays the dominant role in its strong intrasublattice ferromagnetic exchange and its strong antiferromagnetic exchange with the rare earth site. The Fe in the (f) site have an antiferromagnetic intrasublattice exchange, they have a canted strcuture with the ferromagnetic component parallel to the (j) sublattice magnetization.
UR - https://www.scopus.com/pages/publications/0019676966
U2 - 10.1016/0022-3697(81)90044-5
DO - 10.1016/0022-3697(81)90044-5
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AN - SCOPUS:0019676966
SN - 0022-3697
VL - 42
SP - 369
EP - 377
JO - Journal of Physics and Chemistry of Solids
JF - Journal of Physics and Chemistry of Solids
IS - 5
ER -