ABSTRACT
We study a classical system of identically charged counter-ions near a planar wall carrying a uniform surface charge density. The equilibrium statistical mechanics of the system depends on a single dimensionless coupling parameter. A new self-consistent theory of the correlation-hole type is proposed which leads to a modified Poisson–Boltzmann integral equation for the density profile, convenient for analytical progress and straightforward to solve numerically. The exact density profiles are recovered in the limits of weak and strong couplings. In contrast to previous theoretical attempts of the test-charge family, the density profiles fulfil the contact-value theorem at all values of the coupling constant and exhibit the mean-field decay at asymptotically large distances from the wall, as expected. We furthermore show that the density corrections at large couplings exhibit the proper dependence on coupling parameter and distance to the charged wall. The numerical results for intermediate values of the coupling provide accurate density profiles which are in good agreement with those obtained by Monte Carlo simulations. The crossover to mean-field behaviour at large distance is studied in detail.
GRAPHICAL ABSTRACT
![](/cms/asset/911be737-014b-4d29-a1e7-22030614ae94/tmph_a_1471234_uf0001_c.jpg)
Disclosure statement
No potential conflict of interest was reported by the authors.
Notes
1 Yet, as alluded to above, reaching the z-range where the log correction is relevant becomes in practice impossible when increasing Ξ. For instance, we would need for
and already
for
. Thus, the log correction can only be probed at
.