• Chemical bonding and geometric structure

    Already in the electronic ground state, there is a delicate balance between the nuclei, electrons, electrostatics, and quantum mechanics. For many systems, density-functional theory (DFT) allows to treat the quantum mechanics of the many-electron system, to energy-optimize the geometry, and to understand details of chemical bonding.

  • Excited states: optical spectra

    Optical spectra (continous spectra, excitons, charge-transfer states, and localized states like self-trapped excitons) are heavily influenced by electronic correlation, as well, in particular by electron-hole interaction effects. Such issues are important both for the characterization of systems, as well as for applications like optielectronics or photovoltaics.

  • Interrelation between electrons and the atomic geometry

    Since the electronic structure deoends on the atom positions, it is not surprising that the atom positions depend on the electronic structure, as well. In particular, the geometry may change if the electronic structure is excited. A number of consequences arise, like vibrational broadening of electronic transitions, Stokes shifts between light absorption and emission, self trapping of excitons, and fragmentation of the system.

  • Femtosecond dynamics

    Excitations often happen via states that are not eigenstates of the electronicstructure, thus giving rise to state propagation in time which typically happens on a femtosecond time scale. Two prominent examples are resonant charge transfer processes (e.g., from an adsorbate to the substrate) and decay mechanisms dueto the finite lifetime of electronic states resulting from electron-electron interaction.

  • Picosecond dynamics

    Closely related to the electron-geometry interrelation, the motion of the geometry can also be investigated in real time, employing molecular-dynamics techniques that are common for geometry optimization, non-linear vibrations, and chemical reactions. For the determination of excited-state dynamics, however, the excited-state potential-energy surface and the corresponding forces must be evaluated first, which is more demanding than the ground-state forces for ground-state dynamics.

  • STM Simulation

    In experiment, very detailed information about geometric and electronic structures can be obtained from scanning-tunneling microscopy (STM). The simulation ofSTM images is thus an important tool at the interface between theory and experiment.

  • Theoretical concept

    The spectral properties of a many-electron system are determined by transitionsbetween its ground state and the excited states. For the problems we have in mind two classes of excited states are relevant: states with an electron number changing by plus/minus 1 (i.e., hole-like and electron-like excitations, whose energies define the band structure), as well as excited states without changing thenumber of electrons (in particular, electron-hole pairs that are relevant for optical excitations). Correspondingly, the mathematical description and its numerical realization of these concepts on powerful computer platforms is carried outin several consecutive steps.

    1. Determination of the ground state by density-functional theory (DFT)
      This step is necessary for ground-state geometry optimiztation and to provide the basis for the following considerations.
    2. Determination of the single-particle spectrum by many-body perturbation theory (MBPT)
      By solving the equation of motion of the single-particle Green function, the band structure of electrons and holes is obtained. As the crucial quantity, the electron self energy must be evaluated, describing the exchange and correlation effects among the electrons. This is done within the so-called GW approximation. The key aspect of this approximation is the inclusion of dielectric creening effects, that dominate the Coulomb interaction between charged particles in condensed matter. This concept has first been suggested in the years of 1965-1970; since about 1985 it has become possible to employ it for real systems,as well, including numerically demanding systems like complex surfaces and large molecules.
    3. Investigation of optical excitations within MBPT
      Optical transitions can only be described if electron-hole correlation isincluded in the excitation process. This leads to the problem of solving an equation of motion of a two-particle Green function (given by the Bethe-Salpeter equation); this is a consequent extension of MBPT. The ''perturbation'' is again dominated by the electron self-energy operator. This method allows to investigatethe entire linear optical spectrum, both in the frequency range of bound excitons and in the range of resonant states above the fundamental energy gap.
    4. Solution of the time-depending Schroedinger equation
      By evaluating the time propagation for excited electronic states (either for single quasiparticles or for coupled electron-hole states), the dynamics of charge carriers, resonant charge transfer, etc. is addressed. This step is easilydone within MBPT, just taking the MBPT Hamiltonian as time propagator.
    5. Evaluation of excited-state atom dynamics
      This step requires the calculation of total energies, of the resulting potential surfaces, and the resulting forces these potentials, thus allowing to solve the atoms' equation of motion by conventional molecular-dynamics techniques.