
arXiv: 1303.4236
We consider a one-dimensional gas of positive and negative unit charges interacting via a logarithmic potential, which is in thermal equilibrium at the (dimensionless) inverse temperature $��$. In a previous paper [Samaj, L.: J. Stat. Phys. 105, 173-191 (2001)], the exact thermodynamics of the unrestricted log-gas of pointlike charges was obtained using an equivalence with a (1+1)-dimensional boundary sine-Gordon model. The present aim is to extend the exact study of the thermodynamics to the log-gas on a line with alternating $\pm$ charges. The formula for the ordered grand partition function is obtained by using the exact results of the Thermodynamic Bethe ansatz. The complete thermodynamics of the ordered log-gas with pointlike charges is checked by a small-$��$ expansion and at the collapse point $��_c=1$. The inclusion of a small hard core around particles permits us to go beyond the collapse point. The differences between the unconstrained and ordered versions of the log-gas are pointed out.
23 pages, 4 figures
exact thermodynamics, thermodynamic Bethe ansatz, Statistical Mechanics (cond-mat.stat-mech), charge ordering, two-component log-gas, FOS: Physical sciences, Statistical mechanics of plasmas, Classical equilibrium statistical mechanics (general), Condensed Matter - Statistical Mechanics
exact thermodynamics, thermodynamic Bethe ansatz, Statistical Mechanics (cond-mat.stat-mech), charge ordering, two-component log-gas, FOS: Physical sciences, Statistical mechanics of plasmas, Classical equilibrium statistical mechanics (general), Condensed Matter - Statistical Mechanics
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