The Keller-Segel equations model chemotaxis of bio-organisms. In a reduced form, considered in this talk, they are related to Vlasov equation for self-gravitating systems and are used in social sciences in description of crime patterns.
It is relatively easy to show that in the critical dimension 2 and for mass of the initial condition greater than 8 \pi, the solutions 'blowup' (or 'collapse') in finite time. This blowup is supposed to describe the chemotactic aggregation of the organisms and understanding its mechanism, especially its universal features, would allow to compare theoretical results with experimental observations. Understanding this mechanism turned out to be a very subtle problem defying solution for a long time.
In this talk I discuss recent results on dynamics of solutions of the (reduced) Keller-Segel equations in the critical dimension 2 which include a formal derivation and partial rigorous results on the blowup dynamics of solutions. The talk is based on the joint work with S. I. Dejak, D. Egli and P.M. Lushnikov.
More than 30,000 papers are published each year
in which modern density functional calculations are performed.
However, there is presently no systematic route to finding useful
approximations. Over 40 years ago, Lieb and Simon demonstrated
that the original version of density functional theory, Thomas-Fermi
theory, becomes relatively exact in a very particular
non-relativistic limit of large electron number. I will explain why I believe this
holds the key to a systematic treatment of such approximations, and
what my group has done in the last 8 years to use this insight.
There are many examples in mathematics, both pure and applied, in which
problems with symmetric formulations have non-symmetric solutions.
Sometimes this symmetry breaking is total, as in the example of
turbulence, but often the symmetry breaking is only partial. One technique
that can sometimes be used to constrain the symmetry breaking is
reflection positivity. It is a simple and useful concept that will be
explained in the talk, together with some examples. One of these concerns
the minimum eigenvalues of the Laplace operator on a distorted hexagonal
lattice. Another example that we will discuss is a functional inequality
due to Onofri.
The talk is based on joint work with E. Lieb.
I will discuss the properties of discrete random Schrödinger operators in which the random part of the potential is supported on a sublattice. For the standard Anderson model, no results concerning localization/delocalization transition are rigorously established. For trimmed Anderson model described above, one can trace out the onset of the localization breakup, in the strong disorder regime (for some examples). This is a joint work with Sasha Sodin.