Seminars and Colloquia by Series

Rigidity of critical points of hydrophobic capillary functionals among sets of finite perimeter

Series
Math Physics Seminar
Time
Friday, March 20, 2026 - 11:00 for 1 hour (actually 50 minutes)
Location
Skiles 006
Speaker
Robin NeumayerCarnegie Mellon University

The capillary energy functional is used to model the equilibrium shape of a liquid drop meeting a substrate at a prescribed interior contact angle. We will discuss a rigidity theorem for volume-preserving critical points of the capillary energy in the half-space: among all sets of finite perimeter, every such critical configuration corresponding to a prescribed contact angle between 90 degrees and 120 degrees must be a finite union of spheres and spherical caps with the correct contact angle. Assuming that the tangential part of the capillary boundary is $\mathcal{H}^n$-null, this rigidity extends to the full hydrophobic range of contact angles between 90 degrees and 180 degrees. We will also present an anisotropic counterpart, establishing rigidity under suitable lower density assumptions. This talk is based on joint work with A. De Rosa and R. Resende.
 

Semi-classical commutator estimates in Hartree theory

Series
Math Physics Seminar
Time
Friday, March 6, 2026 - 11:00 for 1 hour (actually 50 minutes)
Location
Skiles 006
Speaker
Esteban CárdenasUniversity of Michigan

In this talk we consider the Hartree energy functional for an ensemble of identical fermions. We prove that the minimizers satisfy an important set of semi-classical commutator estimates (SCEs), which encode the uniform regularity of the states in the semi-classical parameter. In the recent years, the SCEs have been shown to play a key role in the quantitative derivation of Hartree-Fock and Vlasov dynamics from large systems of fermions, and are typically implemented as assumptions in the initial data. Proving the validity of such estimates is, however, not an easy task; up to recently only the linear smooth case was understood. In our work, we provide the first set of examples of states satisfying the SCEs which arise from a nonlinear minimization problem. In particular,  two-body interactions up to the repulsive Coulomb potential are included.  If time allows it, I will present — as an application — the quantitative convergence of the fermonic N-body ground state, towards the minimizer of the Vlasov functional.  Based on joint work with L. Lafleche (ENS Lyon).

Extremal eigenvalue problems for metric and quantum graphs

Series
Math Physics Seminar
Time
Friday, February 27, 2026 - 11:00 for 1 hour (actually 50 minutes)
Location
Skyles 006
Speaker
Evans HarrellGeorgia Institute of Technology

I'll review a few known results about quantum graphs that maximize or minimize eigenvalues or combinations of eigenvalues, and will then concentrate on ratios of eigevalues under topological constraints on the graph.  In particular a new discovery with James Kennedy and Gabriel Ramos is that the largest ratio of the first two eigenvalues of the Laplacian on a finite tree graph with Dirichlet conditions at the ends is achieved by equilateral stars. Some related, Weyl-sharp estimates of arbitrary eigenvalue ratios can be obtained using similar ideas.  If time permits, I will also describe some optimal results about differences and other combinations of eigenvalues.

Incommensurate Twisted Bilayer Graphene: emerging quasi-periodicity and stability

Series
Math Physics Seminar
Time
Friday, February 20, 2026 - 11:00 for 1 hour (actually 50 minutes)
Location
Skyles 006
Speaker
Vieri MastropietroUniversita' di Roma “La Sapienza”, Department of Physics, Rome, Italy
We consider a lattice model of twisted bilayer graphene (TBG) for incommensurate twist angles, focusing on the role of large-momentum-transfer Umklapp terms. These terms, which nearly connect the Fermi points of different layers, are typically neglected in effective continuum descriptions but could, in principle, destroy the Dirac cones; they are indeed closely analogous to those appearing in fermions within quasi-periodic potentials, where they play a crucial role. We prove that, for small but finite interlayer coupling, the semimetallic phase is stable provided the angles belong to a fractal set of large measure (which decreases with the hopping strength) characterized by a number theoretic Diophantine condition. In particular, this set excludes the (zero measure) commensurate angles. Our method combines a Renormalization Group (RG) analysis of the imaginary-time, zero temperature Green’s functions, with number theoretic properties, and is similar to the technique used in the Lindstedt series approach to Kolmogorov-Arnold-Moser (KAM) theory. The convergence of the resulting series allows us to rule out non-perturbative effects. The result provides a partial justification of the effective continuum description of TBG in which such large-momentum interlayer hopping processes are neglected.
Work in collaboration with Ian Jauslin
 
Available on zoom at: 
https://gatech.zoom.us/j/92212527205?jst=4
 

A framework to study twisted bilayer graphene in a tight binding model

Series
Math Physics Seminar
Time
Friday, February 6, 2026 - 11:00 for 1 hour (actually 50 minutes)
Location
Skiles 006
Speaker
Ian JauslinRutgers University

The study of the electronic properties of twisted bilayer graphene (TBG) has garnered much attention from the condensed matter community recently. TBG is obtained by stacking two graphene monolayers on top of each other, and rotating one of them with respect to the other. Theoretical and experimental analyses have found that the electronic properties of TBG depend very strongly on the angle between the layers. In fact, a handful of “magic” angles have been predicted at which TBG becomes a superconductor, and this has even been verified experimentally. The model commonly used to study TBG is an effective one, and was derived by Bistritzer and MacDonald. In this talk, I will present recent results on developing a framework to study TBG from first principles. To be more exact, we consider a tight-binding model for the electrons, but make no further approximations. Using a renormalization group technique, we construct a perturbative expansion to study TBG that is convergent when the twisting angle satisfies certain diophantine conditions. This is joint work with V. Mastropietro.

Deterministic Delocalization

Series
Math Physics Seminar
Time
Friday, January 30, 2026 - 11:00 for 1 hour (actually 50 minutes)
Location
Skiles 006
Speaker
David DamanikRice University

We present joint work with Artur Avila on delocalizing Schr\"odinger operators in arbitrary dimensions via arbitrarily small perturbations of the potential. As a consequence we obtain an analog of Simon's Wonderland Theorem for the case of dynamically defined potentials. We will discuss a mechanism based on the Feynman-Hellmann Theorem, whose infinite volume limit is instrumental in establishing delocalization in infinite volume. Furstenberg's correspondence principle then yields the desired delocalization statement in finite volume.

Universality limits for orthogonal polynomials

Series
Math Physics Seminar
Time
Friday, January 23, 2026 - 11:00 for 1 hour (actually 50 minutes)
Location
Skiles 006
Speaker
Milivoje LukicEmory University

The local spacing of zeros of orthogonal polynomials is studied using scaling limits of Christoffel--Darboux kernels. Different limit kernels are associated with different universality classes, e.g. sine kernel with bulk universality and locally asymptotically uniform zero spacing. In recent years, new results have been obtained by using the de Branges theory of canonical systems. This includes necessary and sufficient conditions for a family of scaling limits corresponding to homogeneous de Branges spaces; this family includes bulk universality, hard edge universality, jump discontinuities in the weight, and other notable universality classes. It also includes local behaviors beyond scaling limits. The talk is based on joint works with Benjamin Eichinger, Brian Simanek, Harald Woracek, Peter Yuditskii.

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.

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