The theory of polynomial functors allows one to make sense of the stable polynomial representation theory of the general linear group over a field of characteristic 0. It also has a good notion of specialization, so that calculations done in the "infinite limit" can be used to get information in the usual finite-dimensional siutation. (At the combinatorial level this is understood as the theory of symmetric functions vs. symmetric polynomials.) Such a theory is less well-understood in the other classical groups, but the analogous category has been introduced by Olshanskii and Penkov-Strykas. However, the specialization from the infinite case to the finite case (which is needed for applications) was not previously understood. This talk will explain joint work with Andrew Snowden and Jerzy Weyman where such a specialization is constructed and its properties analyzed. Time permitting, I will explain how this is intricately connected with the invariant theory and commutative algebra surrounding determinantal varieties. I will not assume prior knowledge of polynomial functors and representation theory of classical groups.
The local Langlands correspondence is a relationship between representations of the Galois group of a p-adic field F and the rerepresentations of GL_n(F). Understanding the behavior of the local Langlands correspondence as one varies Galois representations in families is an important ingredient in Emerton's recent proof of many cases of the Fontaine-Mazur conjecture. I will explain this question, and its connection to questions involving the Bernstein center, an algebra that acts naturally on a category of representations of GL_n(F).
In this talk, I will report on a joint project with Yichao Tian. Let p be a prime unramified in a totally real field F. The Goren-Oort stratification is defined by the vanishing locus of the partial Hasse-invariants; it is an analog of the stratification of modular curve mod p by the ordinary locus and the supersingular locus. We give explicit global description of the Goren-Oort stratification of the special fiber of the Hilbert modular variety for F.
We continue with an introduction to the principle ISP and its relatives as well as their connections to supercompact cardinals and the proper forcing axiom. In particular, we prove that PFA implies ISP.
Kohn-Sham density functional theory (KSDFT) is the most widely used electronic structure theory for condensed matter systems. The standard method for solving KSDFT requires solving N eigenvectors for an O(N) * O(N) Kohn-Sham Hamiltonian matrix, with N being the number of electrons in the system. The computational cost for such procedure is expensive and scales as O(N^3). We have developed pole expansion plus selected inversion (PEXSI) method, in which KSDFT is solved by evaluating the selected elements of the inverse of a series of sparse symmetric matrices, and the overall algorithm scales at most O(N^2) for all materials including metallic and insulating systems. The PEXSI method can be used with orthogonal or nonorthogonal basis set, and the electron density, total energy, Helmholtz free energy and atomic force are calculated simultaneously and accurately without using the eigenvalues and eigenvectors. Combined with atomic orbital basis functions, the PEXSI method can be applied to study the electronic structure of nanotube systems with more than 10,000 atoms with minimum basis set even with on single processor. The recently developed parallel PEXSI method further allows the accurate treatment of layered graphene-like structure with more than 20,000 atoms, and can be efficiently parallelized to more than 10,000 processors on leadership class machines.
We discuss self-organized dynamics of agent-based models
with focus on a prototype model driven by non-symmetric self-alignment
introduced in [1].
Unconditional consensus and flocking emerge when the self-alignment is
driven by global interactions with a sufficiently slow decay rate. In
more realistic models, however, the interaction of self-alignment is
compactly supported, and open questions arise regarding the emergence
of clusters/flocks/consensus, which are related to the propagation of
connectivity of the underlying graph.
In particular, we discuss heterophilious self-alignment: here, the
pairwise interaction between agents increases with the diversity of
their positions and we assert that this diversity enhances
flocking/consensus. The methodology carries over from agent-based to
kinetic and hydrodynamic descriptions.
[1] A new model for self-organized dynamics and its flocking behavior, J.
Stat. Physics 144(5) (2011) 923-947.
Congratulations to Math Department faculty members, Dr. Sarah Eichhorn and Dr. Rachel Lehman, and Math graduate student, May Mei! They will be recognized at the 19th annual Celebration of Teaching Ceremony. Sarah and Rachel have been awarded the 2013 Instructional Technology Innovation Award for their work with online courses.
I will present a new PDE approach to obtain large time behavior
of Hamilton-Jacobi equations. This applies to usual Hamilton-Jacobi
equations, as well as the degenerate viscous cases, and weakly coupled
systems. The degenerate viscous case was an open problem in last 15 years.
This is the joint work with Cagnetti, Gomes, and Mitake.
Over the last few years, a number of dynamical density functional theories (DDFT)
have been developed for describing the dynamics of the one-body density of both
colloidal and atomic fluids. The DDFT is capable of describing the dynamics of the
fluid down to the scale of the individual fluid particles. DDFT is particularly
successful for colloidal fluids, for which one may assume that the particles have
stochastic equations of motion and from the resulting Fokker-Plank equation one is
able to derive the DDFT. I will give an overview of the DDFT and show applications
to various inhomogeneous fluid dynamical phenomena such as colloidal sedimentation
and evaporative dewetting of nanoparticle suspensions, which exhibit pattern
formation.