Physics – Condensed Matter – Mesoscale and Nanoscale Physics
Scientific paper
1998-06-26
Phys. Rev. B 59, 10473 (1999)
Physics
Condensed Matter
Mesoscale and Nanoscale Physics
31 pages, 11 figures
Scientific paper
10.1103/PhysRevB.59.10473
We apply the diagram-technique formalism beyond the Hartree-Fock approximation to a two-dimensional nearly ideal electron gas in a weak perpendicular magnetic field. The case of an almost completely filled upper Landau level (filling factor $\nu_0 \lesssim 1$) with a quantum number $N_0 \gg 1$ is considered. We uncover two regimes of renormalization by electron-electron interactions. In the first regime, where $N^{1/2}_0(1-\nu_0) \ll 1$, these interactions lead to a splitting of the Landau levels. In the second regime, where $N^{1/2}_0(1-\nu_0) \gg 1$, apart of the splitting, a renormalization of the bare Zeeman splitting occurs. The intermediate case $N^{1/2}_0 (1-\nu_0)\approx 1$ cannot be studied within our approach. The applicability of the Fermi-liquid description is investigated for both regimes.
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