Universal Finite-Size Effects in the Two-Dimensional Asymmetric Coulomb Gas on a Sphere
arXiv:cond-mat/0104363 · doi:10.1016/S0378-4371(01)00191-1
Abstract
We consider an asymmetric version of a two-dimensional Coulomb gas, made up of two species of pointlike particles with positive and negative -1/Q charges; Q=1 corresponds to the symmetric two-component plasma and the limiting case is related to the one-component plasma. The system lives on the surface of a sphere, and it is studied in both canonical and grand-canonical ensembles. By combining the method of stereographic projection of the sphere onto an infinite plane with the technique of a renormalized Mayer series expansion it is explicitly shown that the finite-size expansions of the free energy and of the grand potential have the same universal term, independent of model's details. As a by-product, the collapse temperature and the Kosterlitz-Thouless transition point (in the limit of a vanishing hard-core attached to particles) are conjectured for any value of .
20 pages, Latex
Cited by in corpus (5)
- Thermodynamics and structure of simple liquids in the hyperbolic plane
- Finite-Size Corrections for Coulomb Systems in the Debye-Huckel Regime
- Debye-Huckel theory for two-dimensional Coulomb systems living on a finite surface without boundaries
- General Considerations on the Finite-Size Corrections for Coulomb Systems in the Debye-Huckel Regime
- Logarithmic Finite-Size Correction in Non-neutral Two-Component Plasma on Sphere