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Simulation comment: The simulations were performed in the constant NVT ensemble [14], at a temperature of 298 K where the Bjerum length is 7.14 Å. Hard-core radii of all system components (rod, surface charges, counter-ions) were taken to be 4 Å, and all charges to be unit charges. Each rod was placed lengthwise on the surface directly adjacent to a row of surface charges. The solvent was modeled as a dielectric continuum with a dielectric constant of 78.54 (water). We employed two movement algorithms for the mobile counter-ions. One moved an ion in a random direction by a random distance of less than 5 Å. The other attempted to move an ion to a random position within the box [14]. Interactions were calculated using Lekner's [15] method. Movements were accepted or rejected using the standard Metropolis algorithm [14].
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