First-principles study of the structural, electronic, and magnetic properties of double perovskite Sr2FeReO6 containing various imperfections
Zhang Yan1, †, , Duan Li1, Ji Vincent2, Xu Ke-Wei3
       

The spin charge density of imperfect Sr2FeReO6 of 4 f.u. containing (a) Fe antisite (FeRe) at (0.5, 0.5, 0.5) site, (b) Re antisite (ReFe) at (0, 0.5, 0.5) site, (c) Fe1–Re1 interchange (Fe1–Re1) at (0, 0, 0) and (0, 0, 0.5) sites, (d) Fe1–Re4 interchange (Fe1–Re4) at (0, 0, 0) and (0.5, 0.5, 0.5) sites, (e) Fe vacancy (VFe) at (0, 0.5, 0.5) site, (f) Re vacancy (VRe) at (0.5, 0.5, 0.5) site, (g) O vacancy (VO) at (0.5, 0.5, 0.25) site, or (h) Sr vacancy (VSr) at (0.75, 0.75, 0.75) site. The spin charge density of the perfect Sr2FeReO6 of 4 f.u. is also shown in panel (i) for comparison. The yellow (turquoise) isosurfaces represent positive (negative) charge density of 0.005 e3 and thus an up-spin (down-spin) moment. In the (100) cross sections, the colors blue, turquoise, and green represent the values of spin charge density in increasing order.