Chiral Symmetry and Electron-Electron Interaction in Many-Body Gap Formation in Graphene

Many-body effects in Auger electron emission from Graphene

Electron-electron interaction in the magnetoresistance of graphene.

We investigate the magnetotransport in large area graphene Hall bars epitaxially grown on silicon carbide. In the intermediate field regime between weak localization and Landau quantization, the observed temperature-dependent parabolic magnetoresistivity is a manifestation of the electron-electron interaction. We can consistently describe the data with a model for diffusive (magneto)transport t...

Electron–electron interaction in high-quality epitaxial graphene

Weak localization is studied in two high-quality epitaxial graphene samples grown on silicon-faced 6H-SiC substrates. Following the methodology of Kozikov et al (2010 Phys. Rev. B 82 075424), we measured the temperature dependence of carrier conductivity at zero and low magnetic (B) fields. In both samples, a logarithmic temperature dependence of the carrier conductivity was observed at B = 0 a...

Electron transport, interaction and spin in graphene and graphene nanoribbons

Since the isolation of graphene in 2004, this novel material has become the major object of modern condensed matter physics. Despite of enormous research activity in this field, there are still a number of fundamental phenomena that remain unexplained and challenge researchers for further investigations. Moreover, due to its unique electronic properties, graphene is considered as a promising ca...

Role of Chiral Symmetry in the Nuclear Many-Body Problem

The role of chiral (pion) dynamics in nuclear matter is reviewed. Contributions to the energy per particle from oneand two-pion exchange are calculated systematically, and it is demonstrated that already at order k f in the Fermi momentum, two-pion exchange produces realistic nuclear binding together with very reasonable values for the compressibility and the asymmetry energy. Further implicati...