We located the melting line of the Yukawa system by determining the free energy of both fluid and solid phases by computer simulations. At the high densities the fluid freezes into a body-centered-cubic (bcc) solid, whereas for low densities it freezes into a face-centered-cubic (fcc) solid. For both the bcc-fluid and the fcc-fluid part of the melting line two coexistence points were determined. We observed that the relative root-mean-square displacement in the solid (Lindeman ratio) varies considerably along the melting line. At the bcc-fluid part of the melting line the Lindeman ratio equals 0.19, whereas at the fcc-solid part of the melting line it is smaller than 0.16.
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Meijer et al. (1991) studied this question.
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