Stochastic Electronic Branching in Graphene
When waves propagate in weakly disordered media they experience focusing and defocusing effects that lead to the formation of stochastic branches, i.e. coalescing of rays and formation of singular caustic points. These phenomena appear in geophysical flows but also in optical ray propagation and electronic flow in disordered metals. Recent work by teams from the University of Crete and Harvard University showed that similar phenomena may occur also in the two dimensional “exceptional-materials” such as graphene and other Dirac solids. Caption: Two-dimensional numerical ray-simulations determine the onset of a caustic event in a disordered potential with std σ=0.1 and for a deterministic potential whose strength is quantified by the amplitude α = [0, 0.01, 0.1]. Left panels: The lower panel shows the random potential. The remaining images represent the density of rays. The green dashed line shows that the first caustic time τ_{c} increases linearly with α. Right panels: The ray density of branched flow in a graphene sheet for α=0 and α=0.1. The team by M. Mattheakis and E. Kaxiras (Harvard University) and G.P. Tsironis (University of Crete) mapped the mathematical problem into a simpler stochastic differential equation that was solved analytically and numerically. This equation gave a statistical prediction on the location of caustic events that was compared with direct simulations. The results show that graphene branching flow is relatively simple yet intricate and the phenomenon may be of physical and technological utility. Article: “Emergence and dynamical properties of stochastic branching in the electronic flows of disordered Dirac solids", Marios Mattheakis, G. P. Tsironis, and Efthimios Kaxiras, Europhysics Letters, Volume 122, Number 2 (2018). |
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