Term 1  
Thu 08.10 14:00 
Naomi Feldheim (Bar Ilan) 
Persistence of Gaussian stationary processesLet f:R→R be a Gaussian stationary process, that is, a random function which is invariant to real shifts and whose marginals have multinormal distribution. What is the probability that f remains above a certain fixed line for a long period of time?This simple question which was posed by mathematicians and engineers more than 60 years ago (e.g. Rice, Slepian), has some surprising answers which were discovered only recently. I will describe how a spectral point of view leads to those results. Based on joint works with O. Feldheim, F. Nazarov, S. Nitzan, B. Jaye and S. Mukherjee. 
Fri 16.10 15:00 
Firas Rassoul Agha (Utah) 
Geometry of geodesics through Busemann measures in directed lastpassage percolationWe consider planar directed lastpassage percolation on the square lattice with general i.i.d. weights and describe geometry properties of the full set of semiinfinite geodesics in a typical realization of the random environment . The main tool is the Busemann functions viewed as a stochastic process indexed by the asymptotic direction. In the exactly solvable exponential model we give a complete characterization of the uniqueness and coalescence structure of the entire family of semiinfinite geodesics. Part of our results concerns the existence of exceptional (random) directions in which new interesting instability structures occur.This is joint work with Christopher Janjigian and Timo Seppäläinen. 
Fri 23.10 15:00 
Inés Armendáriz (Buenos Aires) 
Gaussian random permutations and the boson point processWe construct an infinite volume spatial random permutation associated to a Gaussian Hamiltonian, which is parametrized by the point density and the temperature. Spatial random permutations are naturally related to boson systems through a representation originally due to Feynman (1953). BoseEinstein condensation occurs for dimensions 3 or larger, above a critical density, and is manifest in this representation by the presence of cycles of macroscopic length. For subcritical densities we define the spatial random permutation as a Poisson process of finite unrooted loops of a random walk with Gaussian increments that we call Gaussian loop soup, analogous to the Brownian loop soup of Lawler and Werner (2004). We also construct Gaussian random interlacements, a Poisson process of doublyinfinite trajectories of random walks with Gaussian increments analogous to the Brownian random interlacements of Sznitman (2010). For dimensions greater than or equal to 3 and supercritical densities, we define the spatial permutation as the superposition of independent realizations of the Gaussian loop soup at critical density and Gaussian random interlacements at the remaining density. We show some properties of these spatial permutations, in particular that the point marginal is the boson point process, for any point density.This is joint work with P.A. Ferrari and S. Yuhjtman. 
Fri 30.10 15:00 
Perla Sousi (Cambridge) 
The uniform spanning tree in 4 dimensionsA uniform spanning tree of Z^{4} can be thought of as the "uniform measure" on trees of Z^{4}. The past of 0 in the uniform spanning tree is the finite component that is disconnected from infinity when 0 is deleted from the tree. We establish the logarithmic corrections to the probabilities that the past contains a path of length n, that it has volume at least n and that it reaches the boundary of the box of side length n around 0. Dimension 4 is the upper critical dimension for this model in the sense that in higher dimensions it exhibits "meanfield" critical behaviour. An important part of our proof is the study of the Newtonian capacity of a loop erased random walk in 4 dimensions. This is joint work with Tom Hutchcroft. 
Fri 06.11 15:00 
Renan Gross (Weizmann) 
Stochastic processes for Boolean profitNot even influence inequalities for Boolean functions can escape the long arm of stochastic processes. I will present a (relatively) natural stochastic process which turns Boolean functions and their derivatives into jumpprocess martingales. There is much to profit from analyzing the individual paths of these processes: Using stopping times and level inequalities, we will reprove an inequality of Talagrand relating edge boundaries and the influences, and say something about functions which almost saturate the inequality. The technique (mostly) bypasses hypercontractivity.Work with Ronen Eldan. For a short, animated video about the technique (proving a different result, don't worry), see here 
Fri 13.11 15:00 
Ewain Gwynne (Cambridge) 
Tightness of supercritical Liouville first passage percolationLiouville first passage percolation (LFPP) with parameter ξ>0 is the family of random distance functions on the plane obtained by integrating e^{ξ hε} along paths, where h_{ε} for ε>0 is a smooth mollification of the planar Gaussian free field. Previous work by DingDubédatDunlapFalconet and GwynneMiller showed that there is a critical value ξ_{crit}>0 such that for ξ<ξ_{crit}, LFPP converges under appropriate rescaling to a random metric on the plane which induces the same topology as the Euclidean metric: the socalled γLiouville quantum gravity metric for γ = γ(ξ)∈ (0,2).Recently, Jian Ding and I showed that LFPP admits nontrivial subsequential scaling limits for all ξ > 0. For ξ >ξ_{crit}, the subsequential limiting metrics do not induce the Euclidean topology. Rather, there is an uncountable, dense, Lebesgue measurezero set of points z ∈ C such that D_{h}(z,w) = ∞ for every w∈C\{z}. We expect that the subsequential limiting metrics are related to Liouville quantum gravity with matter central charge in (1,25). I will discuss the properties of the subsequential limiting metrics, their connection to Liouville quantum gravity, and several open problems. 
Fri 20.11 15:00 
Michael Damron (Georgia Tech) 
Critical firstpassage percolation in two dimensionsIn 2d firstpassage percolation (FPP), we place nonnegative i.i.d. weights (t_{e}) on the edges of Z^{2} and study the induced weighted graph pseudometric T = T(x,y). If we denote by p = P(t_{e} = 0), then there is a transition in the largescale behavior of the model as p varies from 0 to 1. When p < 1/2, T(0,x) grows linearly in x, and when p > 1/2, it is stochastically bounded. The critical case, where p = 1/2, is more subtle, and the sublinear growth of T(0,x) depends on the behavior of the distribution function of t_{e} near zero. I will discuss my work over the past few years that (a) determines the exact rate of growth of T(0,x), (b) determines thetime constantfor the siteFPP model on the triangular lattice and, more recently (c) studies the growth of T(0,x) in a dynamical version of the model, where weights are resampled according to independent exponential clocks. These are joint works with J. Hanson, D. Harper, W.K. Lam, P. Tang, and X. Wang. 
Fri 27.11 15:00 
Horatio Boedihardjo (Warwick) 
The signature of a pathThere has been a lot of activities recently pingrov pathwise results for stochastic differential equations. Some of these activities has been inspired by rough path theory which enables integration against the irregular sample paths to be defined in a pathwise, as opposed to L^{2}, sense. While there have been many existence and uniqueness results, a natural next step is to develop descriptive pathwise theory for differential equations driven by specific path. In this talk, we study a particular example of differential equation and its solution, known as the signature. It is one of the simplest equations studied in rough path theory and has some interesting properties that general equations do not have. 
Fri 04.12 15:00 
Kieran Ryan (QMUL) 
The quantum Heisenberg XXZ model and the Brauer algebraSeveral quantum spin systems have probabilistic representations as interchange processes. Some of these processes can be thought of as continuous time random walks on the symmetric group, which in turn has led to study using representation theory. We will in particular discuss the spin½ quantum Heisenberg XXZ model (and analogous models in higher spins, which are not the XXZ). This model, in a similar way to study using the symmetric group for other models, can be studied using the Brauer algebra. We will introduce this algebra, and its representation theory. Using this we obtain the free energy of the system when the underlying graph is the complete graph, which further lets us determine phase diagrams. 
Fri 11.12 15:00 
Herbert Spohn (Münich) 
Generalized Gibbs measures of the Toda latticeAccording to statistical mechanics, Gibbs measures for a manyparticle system are constructed from number, momentum, and energy, which are believed to be generically the only locally conserved fields. The classical Toda lattice is an integrable system and thus possesses a countable list of local conservation laws. Accordingly Gibbs measures of the Toda chain are indexed by an infinite set of parameters, rather than only three. This is the meaning of “generalised" in the title.Specifically for the Toda lattice, we will discuss the structure of generalised Gibbs measures and point out the connection to the onedimensional log gas. This information is a central building block when writing down the appropriate Euler type equations for the Toda lattice. 
Term 2  
Wed 13.01 16:00 
Bálint Virág (Toronto) 
The heat and the landscapeIf lengths 1 and 2 are assigned randomly to each edge in the planar grid, what are the fluctuations of distances between far away points? This problem is open, yet we know, in great detail, what to expect. The directed landscape, a universal random plane geometry, provides the answer to such questions. In some models, such as directed polymers, the stochastic heat equation, or the KPZ equation, random plane geometry hides in the background. Principal component analysis, a fundamental statistical method, comes to the rescue: BBP statistics can be used to show that these models converge to the directed landscape. 
Wed 20.01 16:00 
John Sylvester (Glasgow) 
Multiple Random Walks on Graphs: Mixing Few to Cover ManyIn this talk we will consider k random walks that are run independently and in parallel on a finite, undirected and connected graph. Alon et al. (2008) showed that the effect of increasing k, the number of walkers, does not necessarily effect the cover time (time until each vertex has been visited by at least one walk) in a straightforward manner. Despite subsequent progress in the area, the problem of finding a general characterisation of multiple cover times for worstcase start vertices remains an open problem.We shall present some of our recent results concerning the multiple cover time from independent stationary starting vertices. Firstly, we improve and tighten various bounds, which allow us to establish the stationary cover times of multiple walks on several fundamental networks up to constant factors. Secondly, we present a framework characterising worstcase cover times in terms of stationary cover times and a novel, relaxed notion of mixing time for multiple walks called partial mixing time. Roughly speaking, the partial mixing time only requires a specific portion of all random walks to be mixed. Using these new concepts, we can establish (or recover) the worstcase cover times for many networks including expanders, preferential attachment graphs, grids, binary trees and hypercubes. This is joint work with Nicolás Rivera and Thomas Sauerwald arXiv:2011.07839 
Wed 27.01 16:00 
Alexander Dunlop (NYU) 
A forwardbackward SDE from the 2D nonlinear stochastic heat equationI will discuss a twodimensional stochastic heat equation in the weak noise regime with a nonlinear noise strength. I will explain how pointwise statistics of solutions to this equation, as the correlation length of the noise is taken to 0 but the noise is attenuated by a logarithmic factor, can be related to a forwardbackward stochastic differential equation (FBSDE) depending on the nonlinearity. In the linear case, the FBSDE can be explicitly solved and we recover the lognormal behavior proved by Caravenna, Sun, and Zygouras. Joint work with Yu Gu (CMU). 
Wed 03.02 16:00 
Jess Jay (Bristol) 
Interacting Particle Systems and Jacobi Style IdentitiesThe study of nearest neighbour interacting particle systems on the integer line has a rich history. Although most work in this area concerns the case of translation invariant measures, it can be fruitful to look beyond this case. In 2018, Balazs and Bowen considered product blocking measures for ASEP and ZRP. By relating the two they found a probabilistic proof of the Jacobi triple product identity, a wellknown classical identity appearing throughout Mathematics and Physics.Naturally, one asks if other systems give rise to identities with combinatorial significance, via their blocking measures. In this talk we parameterise such a family and show that it gives rise to new 3 variable combinatorial identities. (This is joint work with M. Balazs and D. Fretwell). 
Wed 10.02 16:00 
Federico Camia (NYU – Abu Dhabi) 
Scaling behavior and decay of correlations in the critical and nearcritical planar Ising modelThe Ising model, introduced by Lenz in 1920 to describe ferromagnetism, is one of the most studied models of statistical mechanics. Its two dimensional version has played a special role in rigorous statistical mechanics since Peierls’ proof of a phase transition in 1936 and Onsager’s derivation of the free energy in 1944. This continues to be the case today, thanks to new results that make the connection between the planar Ising model and the corresponding Euclidean field theory increasingly more explicit. In this talk, I will introduce the Ising model and discuss recent results on its critical and nearcritical scaling limits. I will focus in particular on the scaling behavior of the magnetization field at criticality and on the decay of correlations in the nearcritical regime. (Based on joint work with R. Conijn, C. Garban, J. Jiang, D. Kiss, and C.M. Newman.) 
Wed 17.02 16:00 
Davide Gabrielli (L'Aquila) 
Invariant measures of the Box Ball System having independent soliton componentsThe BoxBall System (BBS) is a onedimensional cellular automaton on the integer lattice. It is related to the Kortewegde Vries (KdV) equation and exhibits solitonic behaviour. It has been introduced by Takahashi and Satsuma, who identified conserved quantities called solitons. Ferrari, Nguyen, Rolla and Wang codify a configuration of balls by a double infinite array of integer numbers called the soliton components. We illustrate the original construction and an equivalent one based on a branching decomposition of the trees associated to the excursions of the walk of a ball configuration. Building over this codification, we give an explicit construction of a large family of invariant measures for the Box Ball System that are also shift invariant, including Markov and Bernoulli product measures. The construction is based on the concatenation of i.i.d. excursions of the associated walk trajectory. The corresponding random array of components has a product distribution with geometric marginals of parameters depending on the size of the solitons. The values of the parameters are obtained by a recursive equation.Joint work with P.A. Ferrari. 
Wed 24.02 16:00 
Gady Kozma (Weizmann) 
The correlation length for percolationFor nearcritical percolation, there is a special scale, called the correlation length, such that below this scale the process looks like critical percolation, while above this scale the process looks like super or subcritical percolation, as the case may be. We will discuss what is known about this value, with special emphasis on the most mysterious case, that of 3 dimensions. All terms would be explained in the talk.Based on joint work with Hugo DuminilCopin and Vincent Tassion (in the special volume in memory of Vladas Sidoravicius), and some unpublished work with Gil Kalai and Noam Lifshitz. 
Wed 03.03 16:00 
Jon Keating (Oxford) 
Moments of moments and Gaussian Multiplicative ChaosI will discuss connections between the moments of moments of the characteristic polynomials of random unitary (CUE) matrices and Gaussian Multiplicative Chaos, focusing in particular on the criticalsubcritical case. 
Wed 10.03 16:00 
Axel Saenz Rodriguez (Warwick) 

Wed 13.01 16:00 
Vittoria Silvestri (Roma – La Sapienza) 