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Theory of the Strongly Coupled 2-D Plasma with the 1/r Potential

  • Kenneth I. Golden
Part of the NATO ASI Series book series (volume 154)

Abstract

The classical two-dimensional (2-d) Coulomb fluid of electrons trapped in surface states above a liquid-helium surface is a fascinating one-component-plasma (ocp) configuration which has been of experimental and theoretical interest since the early 1970’s. In the actual laboratory setup1, extra electrons are deposited in a monolayer just above the free surface of liquid helium and are confined there by means of image binding. The electrons are accordingly constrained to execute only horizontal (parallel-to-the-surface) motions, and they interact via the ϕ (r) = e2/r potential (r is the horizontal range). A compensating uniform positive background is provided by an electrode placed below the liquid surface. At a temperature T ~ 0.5K and over the range 105 < n< 109 cm-2 of areal densities realized in the Grimes-Adams experiments1c,1d, β EF<.06 and 1.5 < Γ=β e2√πn< 150; we may therefore consider the electrons to be classical strongly correlated particles.

Keywords

Approximation Scheme Weak Coupling Pair Correlation Function Plasma Mode BBGKY Hierarchy 
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Copyright information

© Plenum Press, New York 1987

Authors and Affiliations

  • Kenneth I. Golden
    • 1
  1. 1.Department of Computer Science and Electrical EngineeringThe University of VermontBurlingtonUSA

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