“…in Figure 2 in the previous review article (2). Recent updates include ferromagnetic EuO (15), two-dimensional (2D) ferromagnetic Cr2Si2Te6, Cr2Ge2Te6 (16,17), ferrimagnetic garnet ferrites R3Fe5O12 (R = Eu, Tb, Dy, Tm) (18,19,20), Y3−xRxFe5O12 with R being 14 rare-earth elements from La to Lu (except for Pm) (21), Lu2Bi1Fe4Ga1O12 (22), spinel ferrites ZnFe2O4 (23), γ-Fe2O3 (24), LiFe5O8 (25), Ni0.65Zn0.35Al0.8Fe1.2O4 (26), Mg 0.5−δ Mn0.5Fe2O4 (27), Y-type hexagonal ferrites Ba2Co2Fe12O22, Ba2Zn2Fe12O22 (28), orthorhombic ferrimagnetic ε-Fe2O3 (29), molecular-based ferrimagnetic Cr II [Cr III (CN)6] (30), various antiferromagnetic (AF) insulators such as NiO (31,32,33,34), FeF2 (35), α-Fe2O3 (36,37), MnCO3 (38), α-Cu2V2O7 (39), SrFeO3 (40), SrMnO3 (41), DyFeO3 (42), and other intriguing materials including a chiral helimagnet Cu2OSeO3 with a skyrmion lattice phase (43,44) and quantum magnets Sr2CuO3 (45,46), CuGeO3 (47), Pb2V3O9 (48), LiCuVO4 (49). In particular, the ferrimagnetic insulator YIG has been essential (1,2), as it exhibits the lowest magnetic damping, high Curie temperature (TC ∼ 560 K), and high resistivity and also is a playground to reveal the role of magnon polarization in SSEs (see Section 6).…”