Abstract
Density functional theory (DFT) is among the most powerful quantum mechanical methods for calculating the electronic structure of atoms, molecules and solids [1, 2, 3]. In this introduction we present a brief overview of DFT, putting particular emphasis on the appearance of orbital functionals. To describe the electronic many-body system, we have to deal with the Hamiltonian
where
denotes the kinetic-energy operator,
represents the Coulomb interaction between the electrons, and
contains all external potentials acting on the electrons, typically the Coulomb potentials of the nuclei.
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Gross, E.K.U., Kreibich, T., Lein, M., Petersilka, M. (1999). Orbital Functionals in Static and Time-Dependent Density Functional Theory. In: Gonis, A., Kioussis, N., Ciftan, M. (eds) Electron Correlations and Materials Properties. Springer, Boston, MA. https://doi.org/10.1007/978-1-4615-4715-0_24
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