Abstract
Friedel oscillations1 are spatial modulations of the electron density n(r) which occur in microscopic zero-temperature calculations of metallic properties, whenever the metal is subject to a local disturbance. Static Friedel oscillations take the form of a standing-wavelike perturbation in the electron density, falling off with distance from the disturbance. These oscillations are most clearly derived in the jellium model in which the positive metal ions are represented by a uniform positive background. This suppresses periodic crystalline density oscillations and leaves the Friedel oscillations plainly visible. One example is provided by the electron density profile n(z) in calculations2 of the jellium metal surface (Fig. 1): here the surface itself constitutes the “disturbance”, and the wavenumber of the oscillations is twice the Fermi momentum in the bulk metal, 2kF. The oscillations die as z−2 where −z is the depth into the metal.
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Dobson, J.F. (1995). Friedel Oscillations in Condensed Matter Calculations. In: Neilson, D., Das, M.P. (eds) Computational Approaches to Novel Condensed Matter Systems. Springer, Boston, MA. https://doi.org/10.1007/978-1-4757-9791-6_7
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