Category Archives: Fall 2026

Many-body physics via second quantisation

The HADES seminar on Tuesday, September 29th, will be at 3:30pm in Room 736.

Speaker: Maciej Zworski

Abstract: The purpose of the talk is to provide an introduction to basic aspects of second quantisation and its relevance to many body physics. It will be done from a perspective of a non-expert with the principal source being the appendix by Kevin Stubbs to the Lecture Notes with Zhongkai Tao https://math.berkeley.edu/~zworski/Notes_279.pdf. I will introduce quantum many body Hamiltonians, switching then to an abstract formulation using the fermionic Fock spaces, and eventually writing those Hamiltonians in that language.  That will lead to the formulation of the Hartree–Fock minimisation problem.  Creation and annihilation operators will play a central role and I will explain how, in some settings relevant to condensed matter physics, they can be operator valued distributions. The talk provides some (optional) background for a Wednesday talk in the Spectral Theory Seminar.

Self-gravitating charged scalar fields and the extremal black hole threshold

The HADES seminar on Tuesday, September 22nd, will be at 3:30pm in Room 736.

Speaker: Ryan Unger

Abstract: Extremal black holes are special solutions of Einstein’s equations with maximal spin or charge for their mass. In this talk, I will describe a series of conjectures explaining the role of extremal black holes in gravitational collapse. I will focus on upcoming progress on these conjectures in the context of the spherically symmetric Einstein—Maxwell-charged scalar field model. This is joint work with Yannis Angelopoulos (University of Crete) and Christoph Kehle (University of Zürich).

A conditional Lagrangian clock barrier at the $C^{1,\frac{1}{3}}$ threshold for axisymmetric Euler without swirl

The HADES seminar on Tuesday, September 15th, will be at 3:30pm in Room 736.

Speaker: Ovidiu Avadanei

Abstract: We consider axisymmetric no-swirl solutions to the three-dimensional incompressible Euler equations, with initial velocity in $C^{1,\alpha}\cap L^2$, where $\alpha\in\left[\frac{1}{3},1\right)$. In a major breakthrough, Shkoller introduced a clock-and-driver framework that he used in order to prove finite-time type I blow-up below the $C^{1,\frac{1}{3}}$ threshold. Motivated by this, we define Lagrangian classes of coherent initial data and conditional solutions for which the same mechanism yields a supercritical-critical barrier to blow-up when $\alpha\geq\frac{1}{3}$. When $\alpha>\frac{1}{3}$, the aforementioned barrier is genuinely depleted, whereas at the critical endpoint $\alpha=\frac{1}{3}$, we obtain an exponential bound preventing blow-up. In the general case, we formulate a matrix-clock criterion in terms of the smallest singular value of the deformation gradient and show that, under cusp-tail, Dini coherence, near-field compatibility, and bounded transverse-distortion hypotheses, this singular value cannot collapse in finite time. In the on-axis case, the criterion reduces to the scalar clock inequality $\displaystyle \dot{J}(t)\gtrsim -B(t)J(t)-CJ(t)^{3\alpha}$, which rules out Shkoller-type clock collapse for $\alpha\geq\frac{1}{3}$. These results do not enlarge the known Lorentz-space global regularity classes. Rather, they in particular identify the supercritical Lagrangian obstruction dual to Shkoller’s subcritical blow-up mechanism in the case $\alpha>\frac{1}{3}$.

This talk is an extended version of yesterday’s Analysis and PDE Seminar, in the sense that it will contain additional details.