The considered degree of relativistic physics differs for core and valence electrons. The strong localization of core electrons due to the singularity of the effective potential at the atomic nucleus is connected to large kinetic energy contributions and thus a fully relativistic treatment is desirable and common. For the determination of the radial functions u l , α α ( r α α , E l , α α ) and u ˙ ˙ l , α α ( r α α , E l , α α ) the common approach is to make an approximation to the fully relativistic description. This may be the scalar-relativistic approximation (SRA) or similar approaches. The dominant effect neglected by these approximations is the spin-orbit coupling. As indicated above the construction of the Hamiltonian matrix within such an approximation is trivial. Spin-orbit coupling can additionally be included, though this leads to a more complex Hamiltonian matrix setup or a second variation scheme, connected to increased computational demands. In the interstitial region it is reasonable and common to describe the valence electrons without considering relativistic effects.