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Andrew P. Hammond

Publications and source records attributed to Andrew P. Hammond.

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Experimental observation of the marginal glass phase in a colloidal glass

The replica theory of glasses predicts that in the infinite dimensional mean field limit there exist two distinct glassy phases of matter: stable glass and marginal glass. We have developed a technique to experimentally probe these phases of matter using a colloidal glass. We avoid the difficulties inherent in measuring the long time behavior of glasses by instead focusing on the very short time dynamics of the ballistic to caged transition. We track a single tracer particle within a slowly densifying glass and measure the resulting mean squared displacement (MSD). By analyzing the MSD we find that upon densification our colloidal system moves through several states of matter. At lowest densities it is a sub-diffusive liquid. Next it behaves as a stable glass, marked by the appearance of a plateau in the MSD whose magnitude shrinks with increasing density. However, this shrinking plateau does not shrink to zero, instead at higher densities the system behaves as a marginal glass, marked by logarithmic growth in the MSD towards that previous plateau value. Finally, at the highest experimental densities the system returns to the stable glass phase. This provides direct experimental evidence for the existence of a marginal glass in 3d.

cond-mat.soft

Direct measurement of the ballistic motion of a freely floating colloid in Newtonian and viscoelastic fluids

A thermal colloid suspended in a liquid will transition from a short time ballistic motion to a long time diffusive motion. However, the transition between ballistic and diffusive motion is highly dependent on the properties and structure of the particular liquid. We directly observe a free floating tracer particle's ballistic motion and its transition to the long time regime in both a Newtonian fluid and a viscoelastic Maxwell fluid. We examine the motion of the free particle in a Newtonian fluid and demonstrate a high degree of agreement with the accepted Clercx-Schram model for motion in a dense fluid. Measurements of the functional form of the ballistic-to-diffusive transition provide direct measurements of the temperature, viscosity, and tracer radius. We likewise measure the motion in a viscoelastic Maxwell fluid and find a significant disagreement between the theoretical asymptotic behavior and our measured values of the microscopic properties of the fluid. We observe a greatly increased effective mass for a freely moving particle and a decreased plateau modulus.

cond-mat.soft