Critical behavior of density of states near Fermi energy in low-dimensional disordered metals
arXiv:0908.3042 · doi:10.1103/PhysRevB.79.035123
Abstract
We study the effect of electron-electron interaction on the one-particle density of states (\emph{DOS}) of low-dimensional disordered metals near Fermi energy within the framework of the finite temperature conventional impurity diagram technique. We consider only diffusive limit and by a geometric re-summation of the most singular first order self-energy corrections via the Dyson equation we obtain a non-divergent solution for the \emph{DOS} at low energies, while for higher energies the well-known Altshuler-Aronov corrections are recovered. At the Fermi level , this indicates that interacting disordered two- and quasi-one-dimensional systems are in insulating state at zero temperature. The obtained results are in good agreement with recent tunneling experiments on two-dimensional GaAs/AlGaAs heterostructures and quasi-one-dimensional doped multiwall carbon nanotubes.
8 pages, 4 figures
References in corpus (8)
- Weak localisation magnetoresistance and valley symmetry in graphene
- Metal-insulator transition in two-dimensional electron systems
- High Resolution Spectroscopy of Two-Dimensional Electron Systems
- Interaction effects on magnetooscillations in a two-dimensional electron gas
- Metal-insulator transition from combined disorder and interaction effects in Hubbard-like electronic lattice models with random hopping
- Quantum Correction to Conductivity Close to Ferromagnetic Quantum Critical Point in Two Dimensions
- Metal-insulator transition in Hubbard-like models with random hopping
- Emergence of quasi-metallic state in disordered 2D electron gas due to strong interactions