“…However, explicit relativistic exchange-correlation functionals for TRSB systems (with a dependence on the particlenumber density n, the magnetization vector m = [m x , m y , m z ], as well as the SOC-induced orbital-current density vector j = [j x , j y , j z ], and the three spin-current density vectors J x = [J xx , J xy , J xz ], J y = [J yx , J yy , J yz ], J z = [J zx , J zy , J zz ]) are still to be devised. [12][13][14][15][16][17]46 In practice, relativistic calculations are usually performed with the so-called collinear or non-collinear formulations of the DFT, where use is made of standard nonrelativistic functionals modified to only include the explicit dependence on n and m z (collinear) or n and m (non-collinear). 9,16,[18][19][20][21][22][23][24][25][26][27][28][29][30] In this paper we analyze some of the limitations due to the lack of such explicit relativistic functionals for calculations on TRSB materials and we present a strategy to overcome most of them.…”