“…The undimensional Hamiltonian operator describing pseudospin in single-layer graphene, spin-orbital interaction, electric and magnetic field (the last is normal to graphene layer) has the following matrix form [1][2][3][4][6][7][8] Here (x,y) and (x,y) are coefficients of extrinsic, or Rashba, and intrinsic spin-orbit coupling, respectively [8], M(x,y) is proportional to the coefficient of interaction and magnetization of substrate (which can include an inhomogeneous or periodical ferromagnetic structure); U(x,y) is scalar electrostatic potential describing inhomogeneous bias electric field, A y A(x,y) is the vectorpotential of the magnetic field. The spin-orbital Rashba interaction appears due to lacking of inversion symmetry, for example due to substrate at one side of the graphene layer.…”