Abstract
In electrostatic quantum plasmas, the Wigner–Poisson system plays the same rôle as the Vlasov–Poisson system in classical plasmas. This chapter considers the basic properties of the Wigner–Poisson system, including the essentials on the Wigner function method and the derivation of the Wigner–Poisson system in the context of a mean field theory. This chapter also contains a discussion on the Schrödinger–Poisson system as well as extensions to include correlation and collisional effects. The Wigner–Poisson system is shown to imply, in the high-frequency limit, the Bohm–Pines dispersion relation for linear waves, which is the quantum analog of the Bohm–Gross dispersion relation for classical plasmas.
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Haas, F. (2011). The Wigner–Poisson System. In: Quantum Plasmas. Springer Series on Atomic, Optical, and Plasma Physics, vol 65. Springer, New York, NY. https://doi.org/10.1007/978-1-4419-8201-8_2
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