Abstract
Random sequential adsorption of straight rigid rods of length (-mers) on a simple cubic lattice has been studied by numerical simulations and finite-size scaling analysis. The calculations were performed by using a new theoretical scheme, whose accuracy was verified by comparison with rigorous analytical data. The results, obtained for \textit{k} ranging from 2 to 64, revealed that (i) in the case of dimers (), the jamming coverage is . Our estimate of differs significantly from the previously reported value of [Y. Y. Tarasevich and V. A. Cherkasova, Eur. Phys. J. B \textbf{60}, 97 (2007)]; (ii) exhibits a decreasing function when it is plotted in terms of the -mer size, being the value of the limit coverage for large 's; and (iii) the ratio between percolation threshold and jamming coverage shows a non-universal behavior, monotonically decreasing with increasing .
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