Abstract
Hall-effect measurements have been made on single crystals of gadolinium (hcp) in magnetic fields up to 30 kOe applied along the [112¯0] (a axis), [101¯0] (b axis), and [0001] (c axis) directions. The temperature range covered was 4.2-340°K. Large anisotropy and strong temperature dependence were observed for both R0, the ordinary Hall coefficient, and R1, the extraordinary Hall coefficient. These results are interpreted in terms of Fermi-surface anisotropy and exchange splitting of the conduction band. Hall-effect measurements have been made on single crystals of lutetium (hcp) and yttrium (hcp) in magnetic fields up to 7.8 kOe applied along the a, b, and c axes. The temperature range covered was 8-320°K. The Hall coefficients of these metals showed large anisotropy and strong temperature dependence. The anisotropy is interpreted in terms of Fermi-surface anisotropy and the temperature dependence is explained in terms of a transition from impurity scattering at low temperatures to scattering from phonons at high temperatures.