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Probabilistic pick−up
Deterministic pick−up
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Fig. 3. Time evolution of the density of the largest cluster. Squares (resp. circles)
correspond to the model with probabilistic (resp. deterministic) pick-up.
Figure 4 shows, for probabilistic pick-up, the number N ( t ) of clusters as a
function of time (in Log-Log scale) and the density of the largest cluster for
different numbers M of ants. Here M takes the values 100, 200, 400, 800 and
1600. At t =0, N ( t ) is of the order of N 0 . After between 400 000 and 2 000 000
iterations, depending on M , there remains only one large cluster, hence N ( t )=1.
With respect to performance, we wish to point out that the CPU-time of an
iteration depends little on M . Indeed, most of the simulation time is devoted
to the domain traversal, which occurs at each update of the CA. Therefore,
there should be an optimal M , depending on the other fixed parameters, which
produces the best performances.
In figure 4, N ( t ) appears as a stair function. The increasing length steps
indicate a slowing down of the clustering process. Indeed, large compact clusters
are more robust, requiring thus on average more time to vanish.
After an initial start-up of a few thousand iterations in which small clusters
appear, N ( t ) enters a power-law regime. Here, the clustering activity has reached
its normal level and N ( t ) gradually decreases towards 1. The power-law expo-
nent is approximately 3 / 4. It is interesting to compare this exponent with the
exponents 1 / 2of a diffusion process and 1 of a global pick up and deposit
anywhere algorithm. An exponent of 3 was measured in [4] for Deneubourg's
model, but however for a relatively short intermediate power-law regime. The
final regime leading from a dozen of clusters to a single one, was very noisy and
rather slow. In our CA model, the power-law regime survives until the end. In
the deterministic case, the exponent is 1 / 2. Therefore, adding in some intelli-
gence, via probabilistic pick-up, shows that our algorithm actually does better
 
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