# Finite-Size Effects in Non-Neutral Two-Dimensional Coulomb Fluids

## TL;DR

This paper investigates how non-neutrality affects finite-size corrections in 2D Coulomb fluids, revealing that non-neutrality modifies the conformal anomaly number similarly across different plasma models and coupling constants.

## Contribution

It demonstrates that non-neutrality induces a universal change in the conformal anomaly number in the finite-size expansion of 2D Coulomb fluids, extending previous results to the one-component plasma.

## Key findings

- Non-neutrality modifies the anomaly number to c(Q,Γ) = -1 + 3ΓQ^2.
- The change in anomaly number is consistent across different geometries and coupling constants.
- Results are derived at the free-fermion coupling and extended to arbitrary coupling via a field theory mapping.

## 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 $\beta$ a logarithmic finite-size correction term whose universal prefactor depends only on the Euler number of the domain and the conformal anomaly number $c=-1$. A minimal free boson conformal field theory, which is equivalent to the 2D symmetric two-component plasma of elementary $\pm e$ charges at coupling constant $\Gamma=\beta e^2$, was studied in the past. It was shown that creating a non-neutrality by spreading out a charge $Q e$ at infinity modifies the anomaly number to $c(Q,\Gamma) = - 1 + 3\Gamma Q^2$. 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 $e$-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 $\Gamma\equiv\beta e^2=2$ 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.