Using active matter to introduce spatial heterogeneity to the susceptible infected recovered model of epidemic spreading

The widely used susceptible-infected-recovered (S-I-R) epidemic model assumes a uniform, well-mixed population, and incorporation of spatial heterogeneities remains a major challenge. Understanding failures of the mixing assumption is important for designing effective disease mitigation approaches....

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Bibliographic Details
Main Authors: Forgács, P. (Author), Hengartner, N. (Author), Libál, A. (Author), Reichhardt, C. (Author), Reichhardt, C.J.O (Author)
Format: Article
Language:English
Published: Nature Research 2022
Online Access:View Fulltext in Publisher
LEADER 01743nam a2200181Ia 4500
001 10.1038-s41598-022-15223-5
008 220718s2022 CNT 000 0 und d
020 |a 20452322 (ISSN) 
245 1 0 |a Using active matter to introduce spatial heterogeneity to the susceptible infected recovered model of epidemic spreading 
260 0 |b Nature Research  |c 2022 
856 |z View Fulltext in Publisher  |u https://doi.org/10.1038/s41598-022-15223-5 
520 3 |a The widely used susceptible-infected-recovered (S-I-R) epidemic model assumes a uniform, well-mixed population, and incorporation of spatial heterogeneities remains a major challenge. Understanding failures of the mixing assumption is important for designing effective disease mitigation approaches. We combine a run-and-tumble self-propelled active matter system with an S-I-R model to capture the effects of spatial disorder. Working in the motility-induced phase separation regime both with and without quenched disorder, we find two epidemic regimes. For low transmissibility, quenched disorder lowers the frequency of epidemics and increases their average duration. For high transmissibility, the epidemic spreads as a front and the epidemic curves are less sensitive to quenched disorder; however, within this regime it is possible for quenched disorder to enhance the contagion by creating regions of higher particle densities. We discuss how this system could be realized using artificial swimmers with mobile optical traps operated on a feedback loop. © 2022, The Author(s). 
700 1 |a Forgács, P.  |e author 
700 1 |a Hengartner, N.  |e author 
700 1 |a Libál, A.  |e author 
700 1 |a Reichhardt, C.  |e author 
700 1 |a Reichhardt, C.J.O.  |e author 
773 |t Scientific Reports