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2.4- Weak Links

In the random graph model that we have examined so far, a node is able to infect only a few other nodes in the graph (at least for the typical situation in which tex2html_wrap_inline1618 ). Although it is probably true that most users share most of their programs with a small number of other individuals, there is generally a much larger group of other individuals with whom they exchange programs every once in a while. To what extent will these extra pathways enable viruses to spread?

We study the effect of infrequent sharing with a large number of other individuals by modifying the random graph model slightly, giving a node a small but finite chance of infecting any node which is not explicitly connected to it. In addition to the previously-defined infection rate tex2html_wrap_inline1620 , which we shall now refer to as the ``strong'' infection rate, we define the ``weak'' infection rate tex2html_wrap_inline1622 . As before, the average total infection rate through the ``strong'' links is given by tex2html_wrap_inline1624 . The average total infection rate through the ``weak'' links is tex2html_wrap_inline1626 . Thus the total infection rate through all links is:

 

equation369

where

 

equation375

is the ratio between the total weak and strong infection rates.

Figure 6 displays the effect upon the extinction probability and the average number of infections in equilibrium of various ratios tex2html_wrap_inline1628 . The results for tex2html_wrap_inline1630 are simply those of Fig. 5, i.e., there are no weak links. When tex2html_wrap_inline1632 is increased to 0.2, the qualitative behavior of both the extinction probability and the average number of infections is the same, but the transition region is shifted towards more tenuous connectivities. For example, a graph with tex2html_wrap_inline1634 , which is practically impervious to infection when there are no weak links, becomes behaviorally equivalent to a graph with tex2html_wrap_inline1636 : the extinction probability drops to nearly 1/2, and nearly half of the population is infected in equilibrium. When tex2html_wrap_inline1638 is increased further to 0.5, the transition region disappears. Thus for tex2html_wrap_inline1640 there is a finite probability (0.40) for an epidemic to occur, and the average number of infected individuals in equilibrium is 40. These limiting values are easily understood by completely disregarding the strong links, in which case we have from Eq. 16 that the effective value of tex2html_wrap_inline1642 is 1/3 of its nominal value, or tex2html_wrap_inline1644 . Since tex2html_wrap_inline1646 , the conditions for an epidemic to occur are satisfied by the weak links alone, with an effective value of tex2html_wrap_inline1648 , in agreement with the simulation.

  
Figure 6: Extinction probability (a) and average number of infections (b) vs. connectivity tex2html_wrap_inline1650 for random graph with weak links. Three different values of the ratio tex2html_wrap_inline1652 between the sum of the weak-link infection rates and the sum of the strong-link infection rates are presented. As usual, the infection and cure rates are tex2html_wrap_inline1654 and tex2html_wrap_inline1656 . Each point represents an average over 2500 simulation runs on 100-node graphs. As the weak links become stronger, the extinction probability and the average number of infections approach their homogeneous limits over a wider range of connectivities.

The simulation results of Figs. 5 and 6 suggest that the homogeneous limit is reasonably good when the total infection rate is spread among a sufficient number of nodes. However, when too much of the total infection rate is concentrated into too few nodes, epidemics have a much harder time establishing themselves than would be predicted by the homogeneous approximation. For example, according to Fig. 6a, when the connectivity tex2html_wrap_inline1658 and there are no weak links, the epidemic threshold is approximately tex2html_wrap_inline1660 , which is five times the classical value. Other simulations that we have not presented here indicate that, for tex2html_wrap_inline1662 , the epidemic threshold is about twice the classical value. These results are unaffected by the number of nodes N in the graph, provided that N exceeds about 100. Weak links diminish the increase in the threshold, but do not eliminate it. For example, when the total infection rate through the weak links is 0.2 times the total infection rate through the strong links ( tex2html_wrap_inline1668 ), the threshold can be five times the classical value, but only if the graph is twice as tenuous ( tex2html_wrap_inline1670 ) as it needs to be when there are no weak links.


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