Seminars and Colloquia by Series

On quantitative chaos of rescaled states

Series
Math Physics Seminar
Time
Friday, November 14, 2025 - 11:00 for 1 hour (actually 50 minutes)
Location
Zoom and streamed in Skiles 006
Speaker
Hagop TossounianUniversidad de Concepción

Please Note: In order to derive his equation, Boltzmann used the assumption that the probability density function f(t,x1,v1, x2,v2, ..., xN,vN), describing the positions and velocities of a gas of N identical particles at time t, stays close to a product g(t,x1,v1) g(t,x2,v2)...g(t,xN,vN). Here g is the common 1-particle distribution. Mark Kac introduced a probabilistic model for N particles, for which Boltzmann's assumption is valid as N goes to infinity in a specific sense, provided that it is valid at an initial time. Kac's requirement concerning the N particle density functions at some initial time is nowadays known as chaos (or molecular chaos), and Kac's result is known as propagation of chaos. The aim of this talk is to retake the question, first asked and studied in [CCLLV] : For which density functionals g can we produce a family of symmetric densities {fN} supported on the constant energy sphere {v1^2+v2^2+ ... + vN^2 = N} which are chaotic to g? Using rescaled states, we show [CT] that the class of admissible g, obtained in [CCLLV] using other methods, can be expanded. We also mention some new ideas in this direction. This talk is introductory. References: [CCLLV] Carlen, Eric A., et al. "Entropy and chaos in the Kac model." Kinetic and Related Models 3.1 (2010): 85-122. [CT] Cortez, Roberto, and Hagop Tossounian. "Chaos for rescaled measures on Kac’s sphere." Electronic Journal of Probability 28 (2023): 1-29.

First critical field in the 3D Ginzburg-Landau model for inhomogeneous type-II superconductors

Series
Math Physics Seminar
Time
Friday, October 31, 2025 - 11:00 for 1 hour (actually 50 minutes)
Location
SKiles 006
Speaker
Matias Diaz VeraGeorgia Tech

We characterize global minimizers below the so-called first critical field of the inhomogeneous version of the Ginzburg-Landau energy functional in a three-dimensional setting. Minimizers of this functional describe the behavior of type-II superconductors exposed to an external magnetic field, which is characterized by the presence of codimension 2 singularities called vortices where superconductivity is locally suppressed. We will talk about how to adapt the results from the standard Ginzburg-Landau theory into an inhomogeneous framework and present results from a recent work in collaboration with Carlos Roman (Pontificia Universidad Catolica de Chile).

Quantum variance and fluctuations for Walsh-quantized baker's maps

Series
Math Physics Seminar
Time
Friday, October 17, 2025 - 11:00 for 1 hour (actually 50 minutes)
Location
Skiles 006
Speaker
Laura ShouUniversity of Maryland

The Walsh-quantized baker's maps are models for quantum chaos on the torus. We show that for all baker's map scaling factors D\ge2 except for D=4, typically (in the sense of Haar measure on the eigenspaces, which are degenerate) the distribution of the matrix element fluctuations for a randomly chosen eigenbasis looks Gaussian in the semiclassical limit N\to\infty, with variance given in terms of classical baker's map correlations. This determines the precise rate of convergence in the quantum ergodic theorem for these eigenbases. The presence of the classical correlations highlights that these eigenstates, while random, have microscopic correlations that differentiate them from Haar random vectors. For the single value D=4, the Gaussianity of the matrix element fluctuations depends on the values of the classical observable on a fractal subset of the torus.

Some questions and results on the hard sphere model

Series
Math Physics Seminar
Time
Friday, October 3, 2025 - 11:00 for 1 hour (actually 50 minutes)
Location
Skiles 006
Speaker
Will PerkinsGeorgia Tech Department of Computer Science

The hard sphere model is a simple to define and long studied mathematical model of gas, in which the only interactions are the hard-core constraint that two spheres cannot overlap in space.  In three dimensions it is expected to exhibit a gas-to-crystal phase transition.  Despite its simplicty, rigorous results on the model are rather sparse.  I will introduce the model, discuss some of the main open questions, and present some results new and old.

Filamentations of vortex caps for the Euler equation

Series
Math Physics Seminar
Time
Friday, September 26, 2025 - 11:00 for 1 hour (actually 50 minutes)
Location
Skiles 006
Speaker
Gian Marco MarinGeorgia Tech

We rigorously prove the filamentation phenomenon for a class of weak solutions to the Euler equations known as vortex caps. Vortex caps are characteristic functions representing time-evolving sets of Lagrangian type, with energy preserved at all times. The filamentation of vortex caps is characterized by L^1 -stability alongside unbounded growth of the perimeter of their interfaces. We recall the existence and stability results for vortex caps on the sphere, based on Yudovich theory. Using L^1 -stability, we derive a lower bound for the growth of the perimeter of vortex caps over time.

On scaling properties for two-state problems

Series
Math Physics Seminar
Time
Friday, September 12, 2025 - 11:00 for 1 hour (actually 50 minutes)
Location
Skiles 006
Speaker
Bogdan RaitaGeorgetown University

We study differential inclusions of the type $A v=0$ and $v \in K$, where $v$ is a vector field satisfying a linear PDE system $A$ and $K$ is a compact set. We are particularly interested in the case when $K$ consists of two vectors (\textit{two-state problem}). We consider Dirichlet boundary conditions for $v$, in which case the differential inclusion typically has no solutions. We study a suitable relaxation of the system, in which we penalize the surface energy required to switch between the two states. We study the asymptotics of the regularized energy integral. We show that the asymptotics depend polynomially on the regularization parameter with a quantification which — somewhat surprisingly — depends on the order of the linear PDE system $A$. Joint work with A. R\”{u}land, C. Tissot, A. Tribuzio.

Uniform estimates for heavy-tailed random matrix products and applications to Anderson Localization

Series
Math Physics Seminar
Time
Friday, August 22, 2025 - 11:00 for 1 hour (actually 50 minutes)
Location
Skiles 006
Speaker
Omar HurtadoGeorgia Tech

Random matrix products perhaps among some of the most extensively studied examples of random dynamical systems, and moreover are central to the study of one-dimensional disordered systems. We discuss recent results by the author (joint with S. Raman) obtaining estimates on heavy-tailed random matrix products which are robust under perturbations in an appropriate sense, and hence "uniform" on compact sets of measures in an appropriate topology. We also discuss recent localization results for the Anderson model with heavy tails which make use of these uniform bounds.

Programmable Matter and Emergent Computation

Series
Math Physics Seminar
Time
Friday, April 18, 2025 - 11:00 for 1 hour (actually 50 minutes)
Location
005
Speaker
Dana RandallGeorgia Tech

Programmable matter explores how collections of computationally limited agents acting locally and asynchronously can achieve some useful coordinated behavior.  We take a stochastic approach using techniques from randomized algorithms and statistical physics to develop distributed algorithms for emergent collective behaviors that give guarantees and are robust to failures.  By analyzing the Gibbs distribution of various fixed-magnetization models from equilibrium statistical mechanics, we show that particles moving stochastically according to local affinities can solve various useful collective tasks. Finally, we will briefly introduce new tools that may prove fruitful in nonequilibrium settings as well.

Solvability of Some Integro-Differential Equations with Transport and Concentrated Sources

Series
Math Physics Seminar
Time
Friday, April 11, 2025 - 11:00 for 1 hour (actually 50 minutes)
Location
ONLINE
Speaker
Vitali VougalterUniversity of Toronto

The work deals with the existence of solutions of an integro-differential equation in the case of the normal diffusion and the influx/efflux term proportional to the Dirac delta function in the presence of the drift term. The proof of the existence of solutions relies on a fixed point technique. We use the solvability conditions for the non-Fredholm elliptic operators in unbounded domains and discuss how the introduction of the transport term influences the regularity of the solutions.

https://gatech.zoom.us/j/94295986362?pwd=8euEJ3ojkWl5c3Y3hLyXTiKBts3Rrq.1

Interpolating between the optimal transport problems of Monge and Kantorovich

Series
Math Physics Seminar
Time
Friday, February 21, 2025 - 11:00 for 1 hour (actually 50 minutes)
Location
Skiles 005
Speaker
Brendan PassUniversity of Alberta

I will present joint work in progress with Gero Friesecke.  We introduce a two parameter family of variational problems; varying the first parameter interpolates between a regularized version of Monge's optimal transport (OT) problem and Kantorovich's relaxed version.  The first limit problem has the advantage over Monge's original problem of always admitting a solution.  In cases where a (sufficiently regular) Monge map exists, the solution will be of such a form; if not, the limit problem essentially minimizes the transportation cost among all best approximations of the target measure by  pushforwards of the source.  When the source measure is discrete, we show that this is equivalent to the optimal quantization of the target measure, with the additional constraint that the weights of the approximating discrete masses are prescribed.  The second parameter controls the regularity of the pseudo-Monge map. In both the high and low regularity limits, the problem converges to the classical Kantorovich problem, under mild assumptions.

 

Part of the motivation for this problem is to understand whether the strictly correlated electron ansatz is valid in the semi-classical limit of density functional theory (DFT).  We will briefly discuss the corresponding application of OT to DFT, and outline what is known about the existence of Monge solutions (or, equivalently, the validity of the strictly correlated electron ansatz).

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