2019
DOI: 10.1038/s41598-019-51225-6
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Volume explored by a branching random walk on general graphs

Abstract: Branching processes are used to model diverse social and physical scenarios, from extinction of family names to nuclear fission. However, for a better description of natural phenomena, such as viral epidemics in cellular tissues, animal populations and social networks, a spatial embedding—the branching random walk (BRW)—is required. Despite its wide range of applications, the properties of the volume explored by the BRW so far remained elusive, with exact results limited to one dimension. Here we present analy… Show more

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Cited by 8 publications
(15 citation statements)
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“…However, in interacting many-particle systems, such a description is not available in general. Instead, we may choose to use the Doi–Peliti formalism [ 55 , 56 , 57 , 58 , 59 , 60 , 61 , 62 , 63 ] to describe the system, since it provides a systematic approach based on the microscopic dynamics and which retains the particle entity.…”
Section: Discussion and Concluding Remarksmentioning
confidence: 99%
“…However, in interacting many-particle systems, such a description is not available in general. Instead, we may choose to use the Doi–Peliti formalism [ 55 , 56 , 57 , 58 , 59 , 60 , 61 , 62 , 63 ] to describe the system, since it provides a systematic approach based on the microscopic dynamics and which retains the particle entity.…”
Section: Discussion and Concluding Remarksmentioning
confidence: 99%
“…More explicitly in a branching process, an existing individual waits until a branching event occurs. In many models, the waiting time between branching events is fixed [1,23,24], however in the present work, we consider only exponentially distributed waiting times [8,11,25]. At a branching event, an individual is replaced by its offspring, which is a random number K ∈ N 0 of individuals.…”
Section: Introductionmentioning
confidence: 99%
“…As is explained in great detail in [35][36][37], and briefly discussed in App. A, the visit probability Q(x, t) can be expressed as a field-theoretic expectation value under a Doi-Peliti field theory by introducing two additional auxiliary ("trace"-) fields ψ(x, t) and ψ(x, t) with a joint distribution…”
mentioning
confidence: 99%
“…describing a field with vanishing mass ε > 0 which regularises the infrared, ensures causality [35,38], and is to be taken to ε → 0 + at the end of any calculation. The deposition action is derived in [36] and reads…”
mentioning
confidence: 99%
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