Finite-Size Effects in Non-Neutral Two-Dimensional Coulomb Fluids
arXiv:1702.06778 · doi:10.1007/s10955-017-1808-9
Abstract
Thermodynamic potential of a neutral two-dimensional (2D) Cou\-lomb fluid, confined to a large domain with a smooth boundary, exhibits at any (inverse) temperature a logarithmic finite-size correction term whose universal prefactor depends only on the Euler number of the domain and the conformal anomaly number . A minimal free boson conformal field theory, which is equivalent to the 2D symmetric two-component plasma of elementary charges at coupling constant , was studied in the past. It was shown that creating a non-neutrality by spreading out a charge at infinity modifies the anomaly number to . Here, we study the effect of non-neutrality on the finite-size expansion of the free energy for another Coulomb fluid, namely the 2D one-component plasma (jellium) composed of identical pointlike -charges in a homogeneous background surface charge density. For the disk geometry of the confining domain we find that the non-neutrality induces the same change of the anomaly number in the finite-size expansion. We derive this result first at the free-fermion coupling and then, by using a mapping of the 2D one-component plasma onto an anticommuting field theory formulated on a chain, for an arbitrary coupling constant.
14 pages
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