MAGNETOCRYSTALLINE ANISOTROPY ENERGY OF TRANSITION-METAL THIN-FILMS -A NONPERTURBATIVE THEORY

The magnetocrystalline anisotropy energy E-anis of free-standing monol ayers and thin films of Fr and Ni is determined using two different se miempirical schemes. Within a right-binding calculation for the 3d ban ds alone, we analyze in detail the relation between band structure and E-anis, treating spin-orbit coupling (SOC) nonperturbatively. We find important contributions to E-anis due to the lifting of band degenera cies near the Fermi level by SOC. The important role of degeneracies i s supported by the calculation of the electron temperature dependence of the magnetocrystalline anisotropy energy, which decreases with the temperature increasing on a scale of several hundred K. In general, E- anis scales with the square of the SOC constant lambda(so). Including 4s bands and s-d hybridization, the combined interpolation scheme yiel ds anisotropy energies that quantitatively agree well with experiments for Fe and Ni monolayers oil Cu(001). Finally, the anisotropy energy is calculated for systems of up to 14 layers. Even after including s b ands and for multilayers, the importance of degeneracies persists. Con sidering a fixed fct-Fe structure, we find a reorientation of the magn etization from perpendicular to in-plane at about 4 layers. For Ni. we find the correct in-plane easy axis for the monolayer. However. since the anisotropy energy remains nearly constant. we do not find the exp erimentally observed reorientation.