Abstract
The density of states (DOS) in open chaotic billiards is studied semiclassically in the presence of Coulomb interaction. The exchange and Hartree corrections to the DOS as a function of energy ε relative to the Fermi energy are calculated at zero temperature including higher-order interaction effects. It is shown that the DOS decreases with increasing | ε | in the low-energy regime and begins to increase around | ε |≈ t B -1 , where t B is the classical escape time. For t B -1 ≪| ε |, a logarithmic increase of the DOS is shown to appear. This anomalous ε -dependence is due to competition between the exchange and Hartree corrections.
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