Distance matrix approach applied to a kinetically constrained lattice gas
This page serves as an archive for accompanying movies to the recent publication 'Dynamic Facilitation Explains Democratic Particle
Motion of Metabasin Transitions', L.O. Hedges and J.P. Garrahan arXiv:0706.0902. Please refer to the paper for specific details of
each movie.
Distance Matrix
The distance matrix (DM) provides a convenient means of exploring the microscopic nature of particle motion within a sub-region of an extended
system and is defined as follows
Click on each figure to view a full size image.
Particle TrajectoriesTo further illustrate the dynamical feature highlighted using the distance matrix approach it is useful to directly analyse the particle motion along the trajectory. The following movies indicate the position of particles within the sub-region at 200 time points. Comparing the motion to the corresponding DM above it is clear that the blue square-like regions correspond to periods when the majority of particles within the region are blocked and remain frozen in position. A rapid burst of motion results from a series of unlocking events that temporarily allows a significant number of particles to move a substantial amount in a relatively small amount of time. As mobility passes the system is left in another fully or partially blocked configuration. Click on a movie to view or right click to download.
Average squared kinksConsider the distance matrix along a diagonal. For a given super (or sub) diagonal at a chosen offset the average squared kinks shows extended minima of little activity and sharp peaks of sudden motion. At the peaks the fraction of sites within the sub-region that experience a high degree of activity (particles entering or leaving) is substantial, i.e. a rapid rearrangement of a large number of particles. This is illustrated in the following figure (corresponding to the 10 x 10 subsystem), please refer to the reference for further information. Click on the figure to view a full size image.
The right hand panel shows snapshots of the particle field at the times inidcated in the left hand figure. Coloured black are those particles which have moved in the time interval. At a time corresponding to one of the peaks in the average squared kinks there is a large rearrangement of a significant number of particles within the sub-region. Last updated © 2007-05-06 by Lester Owen Hedges |
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