Using Gaussian decompositions of the electron potential energy and the 4f and 5d-electron wave functions, we have derived short analytical formulae for calculating the parameters of the odd crystal field on rare-earth ions. Extended charge contributions to the intrinsic parameters a(1), a(2), a(3), a(4), a(5), and a(6) were evaluated using Hartree-Fock wave functions of Pr3+-O2- and of Tm3+-O2- pairs.
n approximation of a distribution of zero field splitting (ZFS) parameters by using two-dimensional normal distributions in discrete representation is proposed. The results of modelling the X-band EPR spectra of human serum transferrin are in a good accordance with experiment. For a number of studied EPR spectra, it was found that the desired distribution consists of two components with various rhombicity parameters. The first component is characterized by a relative high degree of correlation between the parameters E and D. For the second component of ZFS, which we associate with iron bound to the C-lobe iron site of human serum transferrin, a high dispersion of the correlation coefficient is observed.
This article uses density functional theory calculations to explore the structural, electronic, and magnetic features of a ferromagnet/ferroelectric Fe/BaTiO3 heterostructure, which possesses a complex non-collinear magnetic structure. The presented research focuses on the evolution of spin systems under the influence of external fields, namely the reorientation of magnetic moments driven by electric-field-induced polarization switching and lattice strain. We demonstrated that the electronic and magnetic properties of the thin ferromagnetic Fe film can be effectively tuned by applying an external electric field - simply by altering the polarization direction of the ferroelectric BaTiO3. By incorporating spin-orbit coupling into the computation scheme, we evaluated the relative structural distortions, magnetic moments in atomic layers, atom- and orbital-resolved density of states, magnetic anisotropy energies, and easy magnetization directions.