Organic Conductors and Superconductors
Organic conductors are ideal model systems to investigate unconventional phenomena emerging from strong electron-electron interactions, including charge-ordered and Mott insulators, quantum spin liquids, unconventional superconductors, Fermi liquids and the effects of low dimensionality, such as the Luttinger liquid. The low energy scales allow to cover the entire phase diagram with comparably small temperature and pressure scales.
Dirac and Weyl Semimetals
Weyl and Dirac semimetals posses three-dimensional linearly dispersing electronic bands with crossings near the Fermi level. The low-energy excitations of these systems (i.e. Weyl or Dirac fermions) are described by relativistic Weyl or Dirac equations, rather than by conventional Schrodinger equation used for parabolic bands. At PI1, we investigate the optical response of Weyl and Dirac semimetals at terahertz and infrared frequencies in order to probe the low-energy dynamics of Weyl and Dirac fermions in solids.
Low Energy Electrons in Solids
How can we understand unconventional electronic states such as found in superconductors, quantum-critical metals, or spin systems? We employ optical spectroscopy at low energies, meaning at GHz and THz frequencies and at very low temperatures, to probe charge and spin dynamics in a wide variety of materials. This opens a unique experimental access to the fundamental properties of some of the most fascinating materials physicists can study.
Optics of Metallic Nanostructures
The subject of nanoscience is the preparation and investigation of structures well below one micron. The macroscopic properties of materials strongly alter, when the size is significantly reduced. Nanostructures are also very interesting in optics. Especially for metal-dielectric nanostructures with "unit cells" much smaller than the wavelength a large number of unexpected new phenomena are predicted like superlensing and cloaking. It is expected that with these so called Metamaterials new photonic devices with freely tuneable permittivity and permeability can be built. These theoretical approaches rely on the assumption of idealized effective optical parameters.