Liqin Ke1,Yongbin Lee1,Ralph Skomski2,Xindong Wang3,Arjun Pathak4,Bruce Harmon1,Rob McQueeney5
Ames Laboratory1,University of Nebraska–Lincoln2,Sophycs Technology LLC3,Buffalo State College4,Iowa State University of Science and Technology5
Liqin Ke1,Yongbin Lee1,Ralph Skomski2,Xindong Wang3,Arjun Pathak4,Bruce Harmon1,Rob McQueeney5
Ames Laboratory1,University of Nebraska–Lincoln2,Sophycs Technology LLC3,Buffalo State College4,Iowa State University of Science and Technology5
Using ab initio methods, we systematically investigate the electronic structures and intrinsic magnetic properties in RMn<sub>6</sub>Sn<sub>6</sub> with R = Gd, Tb, Dy, Ho, and Er. The calculations show that TbMn<sub>6</sub>Sn<sub>6</sub> has an easy-axis anisotropy, DyMn<sub>6</sub>Sn<sub>6</sub> and HoMn<sub>6</sub>Sn<sub>6</sub> have easy-cone anisotropy, and ErMn<sub>6</sub>Sn<sub>6</sub> has an easy-plane anisotropy, all agreeing well with experiments and explained by the Mn coordination of the rare-earth atoms. The Mn sublattice is found to have an easy-plane anisotropy of similar amplitude in all RMn<sub>6</sub>Sn<sub>6</sub> compounds. Band structures of various RMn<sub>6</sub>Sn<sub>6</sub> compounds share great similarities near the Fermi level as they mostly consist of non-4f bands. Multiple Dirac crossings occur at the BZ corners and are opened by spin-orbit coupling; most of them are strongly kz-dependent. The most prominent 2D-like (barely-kz-dependent) Dirac crossing at K lies 0.6–0.7 eV above the Fermi level. However, additional on-site correlations within Mn-d electrons can have profound effects on crossing energies and gap sizes. Finally, we discuss the effects of spin reorientation and surface on the topological band structures.