Error message

Notice: Undefined offset: 0 in include() (line 35 of /home/it/www/www-icts/sites/all/themes/riley/templates/views/views-view-fields--related-file-field-collection-view.tpl.php).
Seminar
Speaker
Deepak Dhar (Indian Institute of Science Education and Research, Pune)
Date & Time
Wed, 16 December 2020, 15:00 to 16:30
Venue
Online seminar
Resources
Abstract

Chase-escape percolation is a variation of the standard epidemic spread models.  In this model, each site can be in one of three states: unoccupied, occupied by a single prey, or occupied by a single predator.  Prey particles spread to neighbouring empty sites at rate $p$, and predator particles spread only to neighbouring sites occupied by prey particles at rate $1$, killing the prey particle that existed at that site. It is found that the prey can survive with non-zero probability, if  $p>p_c$ with $p_c<1 $. Earlier simulations showed that $ p_c$  is very close to $1/2$.  Using Monte Carlo simulations, we estimate the  value of  $p_c$ to be $0.49453 \pm 0.00003$ and the critical exponents  are   consistent with  the $2D$ undirected percolation universality class. We further show  that for  all  $p < p_c$ on a $D-$dimensional hypercubical lattice,   the probability that the number of predators in the absorbing configuration is greater than $s$  is bounded from below by $ \exp( -K  p^{-1} s^{1/D)$, where $K$ is some $p$-independent constant, in contrast to the exponentially decaying cluster size distribution of the isotropic percolation problem.    Even so, the scaling function for the cluster size distribution  for $p$ near $p_c$  decays exponentially, and the stretched exponential behavior dominates  for    $ s \gg s^*$, and $s^*$ diverges near $p_c$.  We also  study the problem starting  from an initial condition with predator particles on all lattice points of the line $y=0$ and prey particles on the line $y=1$.  In this case,  for $p_c<p < 1$, the center of mass of the fluctuating  prey and predator fronts   travel at the same speed.  We find that the speed of the pinned Chase-Escape front is strictly smaller than the speed of the Eden front when its spreading rate is equal to $p$ and show that it is caused by the prey sites at the leading edge being eaten up by the predator.  The fluctuations seem to follow KPZ scaling across the depinning transition.

Please click on the link https://zoom.us/j/92952046040?pwd=enpMYm84MEhpWE9wd3pZZU95eGtlZz09 to join the meeting.                                     

Meeting ID: 929 5204 6040
Passcode: 859958