Abstract
Any many-body theory needs some initial approximate description. If for example we discuss the properties of a multi-electron system and the density n s is small enough, just so the average Coulomb energy \({V_c}\sim {e^2}n_3^{\frac{1}{2}}/\varepsilon\) is small with respect to the temperature T, we can assume it is a quasi-ideal electron gas. Here e is the electron charge, and e is the dielectric constant. The momentum (or quasi-momentum) of an individual electron in such a system is a good eigennumber, and electron energy is a function of this momentum.
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Shikin, V. (1997). 2D Coulomb Crystals on a Liquid Substrate. In: Andrei, E.Y. (eds) Two-Dimensional Electron Systems. Physics and Chemistry of Materials with Low-Dimensional Structures, vol 19. Springer, Dordrecht. https://doi.org/10.1007/978-94-015-1286-2_3
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DOI: https://doi.org/10.1007/978-94-015-1286-2_3
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