Structural signature of jamming transition in thermal amorphous systems
arXiv:0911.1576
Abstract
In thermal amorphous systems, the first peak of the pair correlation function $g(r)$ shows a maximum height $g_1^{\rm max}$ at a volume fraction $Ï=Ï_v$ that increases with the temperature. $g_1^{\rm max}$ diverges at the T=0 jamming transition at $Ï=Ï_c$. Molecular dynamics simulations show that some typical quantities, such as the pressure, bulk modulus, shear modulus, and boson peak frequency that behave power law scalings with $Ï-Ï_c$ in marginally jammed solids at T=0, all show scalings with $Ï-Ï_c$ when $Ï> Ï_v$, while the scalings break down when $Ï< Ï_v$. The presence of $g_1^{\rm max}$ is thus not only a thermal vestige of the T=0 jamming transition, but more importantly the structural signature of the jamming transition.
This paper has been withdrawn by the author and replaced by the most recent paper arxiv:1112.2429