Effect of Size Dispersity On the Melting Transition
We present a molecular dynamics simulation study of the liquid-solid transition in a two dimensional system consisting of particles of two different sizes interacting via a truncated Lennard-Jones potential. We work with equal number of particles of each kind and the dispersity $Δ$ in the sizes of the particles is varied by changing the ratio of the particle sizes only. For the monodisperse case ($Δ= 0$) and for small values of $Δ$, we find a first order liquid-solid transition on increasing the volume fraction $ρ$ of the particles . As we increase $Δ$, the first-order transition coexistence region weakens gradually and completely disappears at high dispersities around $Δ= 0.10$ . At these values of dispersity the high density phase lacks long range translational order but possesses orientational order with a large but finite correlation length. The consequences of this effect of dispersity on the glass transition and on the melting transition in general are discussed.