Abstract

A combination of fundamental measure density functional theory and Monte Carlo computer simulation is used to determine the orientation-resolved interfacial tension and stiffness for the equilibrium hard-sphere crystal-fluid interface. Microscopic density functional theory is in quantitative agreement with simulations and predicts a tension of 0.66k(B)T/sigma(2) with a small anisotropy of about 0.025k(B)T and stiffnesses with, e.g., 0.53k(B)T/sigma(2) for the (001) orientation and 1.03k(B)T/sigma(2) for the (111) orientation. Here k(B)T is denoting the thermal energy and sigma the hard-sphere diameter. We compare our results with existing experimental findings.