Tuning Higher Order Structure in Colloidal Fluids

TL;DR

This study investigates how external AC electric fields influence the formation of string-like structures in colloidal fluids, combining experiments and simulations to analyze higher-order correlations and cluster formations.

Contribution

It introduces a detailed analysis of higher-order structural measures and minimum energy clusters in colloidal fluids under electric fields, with no fitting parameters.

Findings

Good agreement between experiment and simulation at two-body level

Discrepancies increase at higher field strengths, especially in higher-order correlations

Cluster populations are dominated by minimum energy clusters at high field strengths

Abstract

Colloidal particles self assemble into a wide range of structures under external AC electric fields due to induced dipolar interactions [Yethiraj and Van Blaaderen Nature 421 513 (2003)]. As a result of these dipolar interactions, at low volume fraction the system is modulated between a hard-sphere like state (in the case of zero applied field) and a "string fluid" upon application of the field. Using both particle-resolved experiments and Brownian dynamics simulations, we investigate the emergence of the string fluid with a variety of structural measures including two-body and higher-order correlations. The higher-order structure we probe using three-body spatial correlation functions and a many-body approach based on minimum energy clusters of a dipolar-Lennard-Jones system. This yields a series of geometrically distinct minimum energy clusters upon increasing the strength of the dipolar interaction, which are echoed in the higher-order structure of the colloidal fluids we study here. We find good agreement between experiment and simulation at the two-body level, although some discrepancies are found at higher field strength, where the system falls out of equilibrium. Higher-order correlations exhibit reasonable agreement between experiment and simulation, again with more discrepancy at higher field strength for three--body correlation functions. At higher field strength, the cluster population in our experiments and simulations is dominated by the minimum energy clusters for all sizes $8 \leq m \leq 12$. The agreement that we find here is notable considering that there is no fit parameter in our mapping between experiment and simulation.