摘要

The phase transition of the two-dimensional (2D) Coulomb plasma is studied with the help of the equivalence to a quantum sine-Gordon system in 2D Euclidean space. The minimum and the stability of the grand canonical potential are derived by making use of the variational effective potential method. The phase diagram thus obtained shows a larger region of plasma phase in the parameter plane than the parallel result in the (1+1)-dimensional Minkowski space. The origin of this difference is discussed in connection with the manner of the large momentum cut off being taken.