Abstract
It is shown that for a quasi–two-dimensional electron gas embedded in a material with a large dielectric constant ε, the plasma frequency ωp(q) for small momenta q may be less than the quasi-particle excitation energy υ(kF) ∙ q. Under this condition, the screening of the Coulomb interaction is determined by the single-particle density of states. This gives rise to a significant increase of the velocity υ near the Fermi surface and, in turn, to an anomalous renormalization of the transport properties. The results are applied to explain the normal properties of the high-Tcsuperconductors.
| Original language | English |
|---|---|
| Pages (from-to) | 505-511 |
| Number of pages | 7 |
| Journal | EPL |
| Volume | 19 |
| Issue number | 6 |
| DOIs | |
| State | Published - 15 Jul 1992 |
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