Seminarium Zakładu Fizyki Teoretycznej

The main feature of the electronic systems in atoms, molecules and solids is that external potential as well as mutual interaction between electrons has the form of Coulomb potential. In such a case, the knowledge of the one-particle density determines not only the ground state energy of the electronic system but also the full Hamiltonian of the systems. Therefore, the very special properties of the Coulomb density allow for formulation of an exact time-independent density functional theory (DFT) of ground and excited states of Coulomb systems [1].