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Alejandro Vizcarra-Rendón

Publications and source records attributed to Alejandro Vizcarra-Rendón.

3 recordsLinked to original sources

Dynamic equivalence between atomic and colloidal liquids

We show that the kinetic-theoretical self-diffusion coefficient of an atomic fluid plays the same role as the short-time self-diffusion coefficient D_S in a colloidal liquid, in the sense that the dynamic properties of the former, at times much longer than the mean free time, and properly scaled with D_S, will indistinguishable from those of a colloidal liquid with the same interaction potential. One important consequence of such dynamic equivalence is that the ratio D_L/ D_S of the long-time to the short-time self-diffusion coefficients must then be the same for both, an atomic and a colloidal system characterized by the same inter-particle interactions. This naturally extends to atomic fluids a well-known dynamic criterion for freezing of colloidal liquids[Phys. Rev. Lett. 70, 1557 (1993)]. We corroborate these predictions by comparing molecular and Brownian dynamics simulations on (soft- and hard-sphere) model systems, representative of what we may refer to as the "hard-sphere" dynamic universality class.

cond-mat.soft

Equilibration of Concentrated Hard Sphere Fluids

We report a systematic molecular dynamics study of the isochoric equilibration of hard-sphere fluids in their metastable regime close to the glass transition. The thermalization process starts with the system prepared in a non-equilibrium state with the desired final volume fraction ϕ but with a prescribed non-equilibrium static structure factor S_0(k; ϕ). The evolution of the α- relaxation time τα (k) and long-time self-diffusion coefficient DL as a function of the evolution time tw is then monitored for an array of volume fractions. For a given waiting time the plot of τα (k; ϕ, tw) as a function of ϕ exhibits two regimes corresponding to samples that have fully equilibrated within this waiting time (ϕ \leq ϕ(c) (tw)), and to samples for which equilibration is not yet complete (ϕ \geq ϕ(c) (tw)). The crossover volume fraction ϕ(c) (tw) increases with tw but seems to saturate to a value ϕ(a) \equiv ϕ(c) (tw \rightarrow \infty) \approx 0.582. We also find that the waiting time t^(eq)_w(ϕ) required to equilibrate a system grows faster than the corresponding equilibrium relaxation time, t^(eq)(ϕ) \approx 0.27 \times [τα (k; ϕ)]^1.43, and that both characteristic times increase strongly as ϕ approaches ϕ^(a), thus suggesting that the measurement of equilibrium properties at and above ϕ(a) is experimentally impossible.

cond-mat.soft

First-principles Predictor of the Location of Ergodic-Non-ergodic Transitions

This letter presents a remarkably simple approach to the first-principles determination of the ergodic-non-ergodic transition in monodisperse colloidal suspensions. It consists of an equation for the long-time asymptotic value $γ$ of the mean squared displacement of the colloidal particles, whose finite real solutions signal the non-ergodic state, and determines the non-ergodic parameter $f(k)$. We illustrate its concrete application to three simple model colloidal systems, namely, hard-spheres, hard-spheres plus repulsive (screened Coulomb) Yukawa interaction, and hard-sphere plus attractive Yukawa tail. The results indicate that this is quite a competitive theory, similar in spirit to, but conceptually independent from, the well-known mode coupling theory.

cond-mat.mtrl-sci