Asymptotic behavior of the Brownian frog model
| dc.contributor.author | Beckman, E | |
| dc.contributor.author | Dinan, E | |
| dc.contributor.author | Durrett, R | |
| dc.contributor.author | Huo, R | |
| dc.contributor.author | Junge, M | |
| dc.date.accessioned | 2018-10-21T02:46:03Z | |
| dc.date.available | 2018-10-21T02:46:03Z | |
| dc.date.updated | 2018-10-21T02:46:02Z | |
| dc.description.abstract | We introduce an extension of the frog model to Euclidean space and prove properties for the spread of active particles. The new geometry introduces a phase transition that does not occur for the frog model on the lattice. Fix $r>0$ and place a particle at each point $x$ of a unit intensity Poisson point process $\mathcal P \subseteq \mathbb R^d - \mathbb B(0,r)$. Around each point in $\mathcal{P}$, put a ball of radius $r$. A particle at the origin performs Brownian motion. When it hits the ball around $x$ for some $x \in \mathcal P$, new particles begin independent Brownian motions from the centers of the balls in the cluster containing $x$. Subsequent visits to the cluster do nothing. This waking process continues indefinitely. For $r$ smaller than the critical threshold of continuum percolation, we show that the set of activated sites in $\mathcal P$ behaves like a linearly expanding ball. Moreover, in any fixed ball the set of active particles converges to a unit intensity Poisson point process. Lastly, we prove that the model expands at rate at least $t^{2- \epsilon}$ when $d=2$ and $r$ equals the critical threshold in continuum percolation. | |
| dc.identifier.uri | ||
| dc.publisher | Institute of Mathematical Statistics | |
| dc.subject | math.PR | |
| dc.subject | math.PR | |
| dc.subject | 60J25 | |
| dc.title | Asymptotic behavior of the Brownian frog model | |
| dc.type | Journal article | |
| pubs.organisational-group | Student | |
| pubs.organisational-group | Duke | |
| pubs.organisational-group | Mathematics | |
| pubs.organisational-group | Trinity College of Arts & Sciences |