“…2 by the closed symbols, both the real and imaginary parts of the ac susceptibility of ErFe 11 Ti exhibit sharp peaks at 50 K, peaks which are undoubtedly assigned to the spin reorientation observed at this temperature. Indeed, in ErFe 11 Ti, the easy magnetization direction is known 18 to change from parallel to the c axis above 50 K to canted from the c axis below 50 K. Because in the RFe 11 Ti structure, the iron sublattices favor a uniaxial magnetic anisotropy parallel to the c axis and erbium, like samarium, has a positive second-order Stevens coefficient, ␣ J , which reinforces the uniaxial magnetic anisotropy, ErFe 11 Ti would be expected to maintain this uniaxial anisotropy at all temperatures. However, the sixth-order crystal-field term is particularly important for erbium because of its large positive Stevens coefficient, ␥ J .…”