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. 2015 Mar 27;10(3):e0120053. doi: 10.1371/journal.pone.0120053

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© 2015 Christophe et al

This is an open-access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are properly credited.

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Fig 4 — (A) Evolution of the probability of the nodule eradication (P _S) when an attraction strength is added to the (default) symmetric random walk dynamic, number going from 0.01 to 0.75 indicate increasing attraction. (B) Mean time of nodule eradication ((T _S)) when attraction is added to the default symmetric random walk dynamic of an increasing number of CTL. Results are represented as mean ± standard deviation of 50 numerical simulations.

Inline graphic — (A) Evolution of the probability of the nodule eradication (P _S) when an attraction strength is added to the (default) symmetric random walk dynamic, number going from 0.01 to 0.75 indicate increasing attraction. (B) Mean time of nodule eradication ((T _S)) when attraction is added to the default symmetric random walk dynamic of an increasing number of CTL. Results are represented as mean ± standard deviation of 50 numerical simulations.