Temporal percolation of the susceptible network in an epidemic spreading
- PMID: 23028498
- PMCID: PMC3441612
- DOI: 10.1371/journal.pone.0044188
Temporal percolation of the susceptible network in an epidemic spreading
Abstract
In this work, we study the evolution of the susceptible individuals during the spread of an epidemic modeled by the susceptible-infected-recovered (SIR) process spreading on the top of complex networks. Using an edge-based compartmental approach and percolation tools, we find that a time-dependent quantity ΦS(t), namely, the probability that a given neighbor of a node is susceptible at time t, is the control parameter of a node void percolation process involving those nodes on the network not-reached by the disease. We show that there exists a critical time t(c) above which the giant susceptible component is destroyed. As a consequence, in order to preserve a macroscopic connected fraction of the network composed by healthy individuals which guarantee its functionality, any mitigation strategy should be implemented before this critical time t(c). Our theoretical results are confirmed by extensive simulations of the SIR process.
Conflict of interest statement
Figures
and
.
as a function of
(
) obtained in Refs. , and
as a function of
(solid line) obtained from Eqs. (3)–(2) and (12)–(13) with
and mean connectivity 4.07 in the giant component for (A) a ER network with
and (B) SF network with
,
and
. In the insets we show
as a function of
from the simulations (symbols) and from Eqs. (3)–(2) and (12)–(13) (solid line) for
(
) and
(
). (Color online).
. From the initial condition
,
and
, satisfies Eq. (12). For
we have two solutions that correspond to
. When
reaches the maximum of the function
,
, the giant susceptible component is destroyed. The dashed lines are used as a guide to show the possible solutions of Eq. (12).
for
and
(
) and mean connectivity
in the giant component for (A) a ER network with
(
) and (B) a SF networks with
, minimal connectivity
and
(
). The symbols correspond to the simulations with the time shifted to
when
% of the individuals are infected, and the solid lines correspond to the theoretical solutions
(blue solid line) of Eqs. (12)–(13). In the insets we show the size of the second biggest susceptible cluster
(red solid line) and the evolution of
(black solid line) obtained from simulations. The value of
(dashed line) was obtained from Eq. (16).
has been amplified by a factor of 50 in order to show it on the same scale as the rest of the curves. The simulations are averaged over 1000 network realizations with
. (Color online).References
-
- Boccaletti S, Latora V, Moreno Y, Chavez M, Hwang D (2006) Complex networks: Structure and dynamics. Physics Reports 424: 175–308.
-
- Anderson RM, May RM (1992) Infectious Diseases of Humans: Dynamics and Control. Oxford University Press, Oxford.
-
- Lagorio C, Migueles M, Braunstein L, López E, Macri P (2009) Effects of epidemic threshold definition on disease spread statistics. Physica A: Statistical Mechanics and its Applications 388: 755–763.
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