“…For instance, there are several f -electron materials possessing the lattice structures without local inversion symmetry, such as ferromagnetic superconductors UGe 2 , [28][29][30] URhGe, [31][32][33] and UCoGe, [34][35][36] the zig-zag chain compounds LnM 2 Al 10 (Ln=Ce, Nd, Gd, Dy, Ho, and Er; M=Fe, Ru, and Os), [37][38][39][40][41][42][43][44] the distorted honeycomb compounds αand β-YbAlB 4 , [45][46][47] and the diamond-structure compounds RT 2 X 20 (R=Pr, La, Yb, and U, T =Fe, Co, Ti, V, Nb, Ru, Rh, and Ir, and X =Al and Zn). [48][49][50][51][52][53][54][55][56][57][58][59] Although these materials can be candidates for unusual odd-parity multipole ordering through the local parity mixing, their properties have not been studied from such a viewpoint. In order to stimulate experiments and theories, it is important to clarify the microscopic mechanism for odd-parity multipole ordering.…”