DescriptionImagine the infinite square lattice each site of which is either vacant (state 0) or occupied (state 1). An interacting particle system is a Markov chain on configurations of zeros and ones, in which the dynamics at each site depends on the states of neighbouring sites.The simplest example is Richardson's growth model. Here the dynamics of sites is very simple:
Let now the rate for a vacant site to become occupied be still ![]() Suppose again that initially only the origin is occupied. Some of the key questions are: will the process die out (ie., all sites eventually become vacant) for ![]() ![]() Other classical examples include the voter model, in which individual sites flip their state (to the opposite) at the rate depending on the number of neighbours in that state, or the exclusion process, in which pairs of neighbouring sites, if in the opposite states, simultaneously flip (thus imitating a jump of a particle from an occupied site to a vacant neighbour). To get some intuition one can play with the simulation appletts of a contact process or an ecological system from Interactivate (you will need to modify your parameters accordingly!). The aim of the project is to explore some of these models and to get some experience with the exciting world of stochastic geometry. Prerequisites2H Probability and 3H Stochastic Processes are essential; 4H Probability could be helpful.ResourcesIf interested, feel free to play with the applets above and/or search online for further properties of these models (see. eg., Wiki pages for contact process, voter model or Google some of the terms mentioned above). The Lecture notes by R. Durrett provide a taster of mathematical tools and results in the area. Some further references might be suggested once the project is underway.Get in touch, if you have any questions or if you would be interested in doing some simulations! |
email: Ostap Hryniv