Crystal-melt stiffness of colloidal hard spheres gains a gravity-dependent term ˜γ = ˜γ0 + g''ξ² that reconciles long-standing experiment-simulation discrepancies.
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Sedimentation equilibrium and gravity dependent stiffness coefficients of colloidal hard-spheres
Crystal-melt stiffness of colloidal hard spheres gains a gravity-dependent term ˜γ = ˜γ0 + g''ξ² that reconciles long-standing experiment-simulation discrepancies.