“…Since in the Hamiltonian, for a combined electrostatic and magnetic hyperfine interaction a term 3 cos 2 θ − 1 is present (θ being the angle between the principal axis of the EFG tensor and the hyperfine field), the crystallographically identical sites may become magnetically inequivalent if the easy axis of magnetization is not oriented along the [001] direction. In the case of a [111] easy axis, a ratio of 3:1 is obtained for the inequivalent sites, corresponding to the angles θ = 70.5 • (3×) and 0 • (1×) [4,5]. In fact, two sextets with an area ratio 3:1 are observed for ZrFe 2 (figure 1, top, and table 4).…”