Term 1 | ||
Wed 13.10 16:00 |
Alexander Povolotsky (Dubna) |
Generalized TASEP between KPZ and jamming regimesTotally Asymmetric Simple Exclusion Process (TASEP) with generalized update is an integrable stochastic model of interacting particles, which differs from the standard TASEP by the presence of an additional interaction controlling the degree of particle clustering. As the strength of the interaction varies, the system suffers the transition from the regime in which the fluctuations of the particle flow are described by standard random processes associated with the Kardar-Parisi-Zhang (KPZ) universality class, to the jamming regime, in which all particles stick to one cluster and move synchronously as the simple random walk. I will focus on the limiting laws of fluctuations of distances travelled by tagged particles both in the KPZ and in the transitional regime for two types of initial conditions. In particular new transitional processes interpolating between the known limiting cases will be discussed. |
Wed 20.10 16:00 |
Eveliina Peltola (Bonn and Espoo) |
Large deviations of SLEs, real rational functions, and zeta-regularized determinants of LaplaciansWhen studying large deviations (LDP) of Schramm-Loewner evolution (SLE) curves, we recently introduced a “Loewner potential” that describes the rate function for the LDP. This object turned out to have several intrinsic, and perhaps surprising, connections to various fields. For instance, it has a simple expression in terms of zeta-regularized determinants of Laplace-Beltrami operators. On the other hand, minima of the Loewner potential solve a nonlinear first order PDE that arises in a semiclassical limit of certain correlation functions in conformal field theory, arguably also related to isomonodromic systems. Finally, and perhaps most interestingly, the Loewner potential minimizers classify rational functions with real critical points, thereby providing a novel proof for a version of the now well-known Shapiro-Shapiro conjecture in real enumerative geometry.This talk is based on joint work with Yilin Wang (MIT). |
Wed 27.10 16:00 |
Matan Harel (Boston) |
Quantitative estimates on the effect of disorder on low-dimensional lattice modelsIn their seminal work, Imry and Ma predicted that the addition of an arbitrarily small random external field to a low-dimensional statistical physics model causes the usual first-order phase transition to be `rounded-off.' This phenomenon was proven rigorously by Aizenman and Wehr in 1989 for a vastly general class of spin systems and random perturbations. Recently, the effect was quantified for the random-field Ising model, proving that it exhibits exponential decay of correlations at all temperatures. Unfortunately, the analysis relies on the monotonicity (FKG) properties which are not present in many other classical models of interest. This talk will present quantitative versions of the Aizenman-Wehr theorems for general spin systems with random disorder, including Potts, spin O(n), spin glasses. This is joint work with Paul Dario and Ron Peled. |
Wed 03.11 16:00 |
Ariel Yadin (Beer Sheva) |
Realizations of random walk entropyRandom walk entropy is a numerical measure of the behaviour of the random walk at infinity. Out of all random walks on groups generated by d elements, the free group has the maximal entropy. One may ask naturally which intermediate values between 0 and the full entropy of the free group can be realized as entropies of random walks on groups. This question is still open. We analyze a related question, which is a "stochastic" version of the above open question. Here we are able to provide a full answer for quotients of the free group, and even a bit further than that. Generalizing results of Bowen (Inventiones 2014), we show that all possible "IRS entropy" values can be realized on the free group. These notions will be precisely explained during the talk.Based on joint works with Yair Hartman and Liran Ron-George. |
Wed 10.11 16:00 |
Slim Kammoun (Toulouse) |
Longest Common Subsequence of Random PermutationsBukh and Zhou conjectured that the expectation of the length of the longest common subsequence (LCS) of two i.i.d random permutations of size n is greater than √ n.This problem is related to the Ulam-Hammersley problem; Ulam conjectured that the expectation of the length of the longest increasing subsection (LIS) for a uniform permutation behaves like c √ n . The conjecture was solved in 1977, but few results are known for non-uniform permutations. The LIS and LCS are closely related, and solving the conjecture of Bukh and Zhou is equivalent to minimize the expected value of LIS for random permutations that can be written as ρ_{n}○ σ_{n}, where σ_{n} and ρ_{n} are i.i.d. random permutations. We recall the classical results for the uniform case as well as partial answers for the conjugation invariant case. |
Wed 17.11 16:00 |
Fabio Toninelli (Vienna) |
Diffusion in the curl of the 2-dimensional Gaussian Free FieldI will discuss the large time behaviour of a Brownian diffusion in two dimensions, whose drift is divergence-free, ergodic and given by the curl of the 2-dimensional Gaussian Free Field. Together with G. Cannizzaro and L. Haundschmid, we prove the conjecture by B. Toth and B. Valko that the mean square displacement is of order √ log t;. The same type of superdiffusive behaviour has been predicted to occur for a wide variety of (self)-interacting diffusions in dimension d = 2: the diffusion of a tracer particle in a fluid, self-repelling polymers and random walks, Brownian particles in divergence-free random environments, and, more recently, the 2-dimensional critical Anisotropic KPZ equation. To the best of our authors’ knowledge, ours is the first instance in which √ log t; superdiffusion is rigorously established in this universality class. |
Wed 24.11 16:00 |
Sarah Penington (Bath) |
Genealogy of the N-particle branching random walk with polynomial tailsThe N-particle branching random walk is a discrete time branching particle system with selection consisting of N particles located on the real line. At every time step, each particle is replaced by two offspring, and each offspring particle makes a jump from its parent's location, independently from the other jumps, according to a given jump distribution. Then only the N rightmost particles survive; the other particles are removed from the system to keep the population size constant. I will discuss recent results and open conjectures about the long-term behaviour of this particle system when N, the number of particles, is large. In the case where the jump distribution has regularly varying tails, building on earlier work of J. Bérard and P. Maillard, we prove that at a typical large time the genealogy is given by a star-shaped coalescent, and that almost the whole population is near the leftmost particle on the relevant space scale. Based on joint work with Matt Roberts and Zsófia Talyigás. |
Wed 01.12 16:00 |
Ofer Zeitouni (Rehovot and New York) |
High moments of partition function for 2D polymers in the weak disorder regime (joint with Clement Cosco)abstract |
Wed 8.12 16:00 |
Cyril Labbé (Paris) |
Mixing points on an intervalConsider N points on the unit interval. Resample each point at rate one uniformly in between its two nearest neighbours. The question is: how much time is needed to reach equilibrium (the uniform measure on the simplex) starting from the worst initial condition ? I will present results in collaboration with Pietro Caputo and Hubert Lacoin where we identified the asymptotic of the mixing times and showed a cutoff phenomenon for the distance to equilibrium. |
Term 2 | ||
Wed 12.01 16:00 |
Zied Ammari (Rennes) |
On well-posedness for the Gross-Pitaevskii and Hartree Hierarchy EquationsGross-Pitaevskii and Hartree hierarchies are infinite systems of coupled PDEs related to mean field theory of Bose gases. Due to their physical and mathematical relevance, the issues of well-posedness and uniqueness for these hierarchies have recently been studied thoroughly using specific nonlinear and combinatorial techniques. In this talk I will introduce a new approach based on a duality between hierarchies and Liouville equations. Several new results are obtained as an outcome of this approach. |
Wed 19.01 16:00 |
Shahar Mendelson (Warwick) |
Approximating Lₚ balls via samplingLet X be a centred random vector in Rⁿ. The Lₚ norms that X endows on Rⁿ are defined by ‖v‖_L__ₚ= (E| |
Wed 26.01 16:00 |
Benjamin Lees |
The random path representation of classical spin systemsMany models in statistical mechanics can be written in terms of a collection of (random) geometric objects. This may consist of a "soup" of random walks/loops, random currents, or random transpositions. I will introduce a model of random paths that includes several interesting models when its parameters are chosen appropriately. One such example is the spin O(N) model. Unlike similar representations of this model, the random path model is defined in terms of a product of local terms which allows many nice techniques, such as reflection positivity, to be used. I will show how to use this model to prove exponential decay of correlations for spin O(N) with an external field. The idea of the proof is very simple and applies much more generally than the alternative Lee-Yang method. |
Wed 02.02 16:00 |
Vedran Sohinger (Warwick) |
Interacting loop ensembles and Bose gasesWe study interacting quantum Bose gases in thermal equilibrium on a lattice. In this framework, we establish convergence of the grand-canonical Gibbs states to their mean-field (classical field) and large-mass (classical particle) limit. Our analysis is based on representations in terms of ensembles of interacting random loops, namely the Ginibre loop ensemble for quantum Bose gases and the Symanzik loop ensemble for classical scalar field theories. For small enough interactions, we obtain corresponding results in the infinite volume limit by means of cluster expansions. This is joint work with Juerg Froehlich, Antti Knowles, and Benjamin Schlein. |
Wed 09.02 16:00 |
Oriane Blondel (Lyon) |
Kinetically constrained models out of equilibriumKinetically constrained models are interacting particle systems on Z^{d}, in which particles can appear/disappear only if a given local constraint is satisfied. This condition complexifies significantly the dynamics. In particular, it deprives the system of monotonicity properties, which leaves us with few tools to study the dynamics when it is initially not at equilibrium. I will review the results and techniques we have in this direction. |
Wed 16.02 16:00 |
Pietro Caputo (Rome) |
Rapid mixing of Gibbs samplers: Coupling, Spectral Independence, and Entropy factorizationsWe discuss some recent developments in the analysis of convergence to stationarity for the Gibbs sampler of general spin systems on arbitrary graphs. These are based on two recently introduced concepts: Spectral Independence and Block Factorization of Entropy. We show that if a system is spectrally independent then its entropy functional satisfies a general block factorization, which in turn implies a modified log-Sobolev inequality and a tight control of the mixing time for the Glauber dynamics as well as for any other heat bath block dynamics. Moreover, we show that the existence of a contractive coupling for a local Markov chain implies that the system is spectrally independent. As a corollary, we obtain new optimal bounds on the mixing time of a large class of sampling algorithms for the ferromagnetic Ising/Potts models in the so-called tree-uniqueness regime, including non-local Markov chains such as the Swendsen-Wang dynamics. The methods also apply to spin systems with hard constraints such as q-colorings of a graph and the hard-core gas. Based on some recent joint works with Antonio Blanca, Zongchen Chen, Daniel Parisi, Alistair Sinclair, Daniel Stefankovic, and Eric Vigoda. |
Wed 23.02 16:00 |
Peter Nandori (New York) |
Flexibility of the central limit theorem in smooth dynamical systemsWe say that a diffeomorphism that preserves a smooth probability measure satisfies the CLT if the ergodic sums of all sufficiently smooth functions converge to a Gaussian low. Many diffeomorphisms are known to satisfy the CLT under the usual scaling sqrt(n). Most of these examples also share many other chaotic properties, such as ergodicity, mixing, positive entropy, K property, Bernoulli property. In this talk, I will present new examples of diffeomorphisms that satisfy the CLT but in a more exotic way. For example, the scaling may be regularly varying with index 1, or several ergodic properties from the above list may fail. The main idea of the construction goes back to random walks in random sceneries. This is a joint work with D. Dolgopyat, C. Dong and A. Kanigowski. |
Wed 02.03 16:00 |
Frank den Hollander (Leiden) |
Spatial populations with seed-bankabstract |
Wed 09.03 16:00 |
Marta Sanz-Solé (Barcelona) |
Global solutions to stochastic wave equations with superlinear coefficients.We consider the nonlinear stochastic wave equation on ℝᵈ, d=1,2,3, ∂_t² u(t,x) − Δₓ u(t,x) = b(u(t,x)) + σ(u(t,x)) ∂_tW(t,x), (t,x) ∈ (0,T] × ℝᵈ, with given initial conditions. The process ∂_tW is a space−time white noise if d=1, while for d=2,3 it is white in time and coloured in space. For coefficients b and σ satisfying |b(z)| ≤ b₁ + b₂ |z| (ln |z|)ᵟ¹, |σ(z)| ≤ σ₁ + σ₂ |z| (ln |z|)ᵟ², when |z|→∞, we find conditions on the superlinear exponents and also on the noise when d=2,3, ensuring global existence (and uniqueness) of a random field solution. Examples of relevant noises are also provided. Recent results by M. Foondun and E. Nualart (2021) provide some partial information on the critical values of the growth exponents. The proof relies on sharp moment estimates of the solution, and of increments in time and space of them, of a sequence of stochastic wave equations closely related to the above equation, with globally Lipschitz continuous coefficients. The research is joint work with A. Millet. We were motivated by a paper from R. Dalang, D. Khoshnevisan and T. Zhang (2019) where a similar question is addressed for a nonlinear stochastic heat equation on [0,1]. |
Wed 16.03 16:00 |
Sabine Jansen (Munich) |
Cluster expansions: necessary and sufficient convergence conditionsCorrelation functions of Gibbs measures in general cannot be computed explicitly, but at low density / for weak interactions they are amenable to a power series expansion around the ideal gas (Poisson point process). The convergence of these series has been studied at least since the 60s, but sufficient convergence conditions keep being developed, raising the question if there is a theoretical limit to the improvements - an if and only if condition that cannot be surpassed. The talk presents such an if and only if condition for repulsive interactions. It is based on Kirkwood-Salsburg equations and alternating sign properties and it generalizes a result by Bissacot, Fernández and Procacci. For possibly attractive potentials, the criterion yields new sufficient convergence conditions. Based on joint work with Leonid Kolesnikov (arXiv:2112.13134 [math.ph]). |
Term 3 | ||
Wed 4.05 16:00 |
Daniel Valesin (Warwick) |
The contact process on random d-regular graphs, static and dynamicWe consider the contact process on random d−regular graphs, briefly presenting earlier work on the case where the graph is static, and focusing on more recent work where the graph evolves simultaneously with (and independently of) the contact process. In both cases, the analysis involves fixing the infection rate of the contact process and the graph parameters, taking the number of vertices N to infinity and studying the asymptotic behaviour of τ_{N}, the time it takes for the infection to disappear. Concerning the static graph, we prove that this behaviour undergoes a phase transition: there is a value λ_{c} such that τ_{N} is of order log(N) if λ < λ_{c}, whereas τ_{N} grows exponentially with N if λ > λ_{c}. The latter situation is called the metastable regime. Turning to the dynamic graph setting, our choice of graph evolution is a Markovian edge−switching mechanism, whose rate is chosen so that the evolving local landscape seen by a fixed vertex approaches a limiting dynamic graph process. We again show the existence of a metastable regime for the contact process on these graphs, and notably, we show that this regime occurs for values of λ that would be subcritical in the static graph. Joint work with Jean−Christophe Mourrat (static graphs) and with Gabriel Baptista da Silva and Roberto Imbuzeiro Oliveira (dynamic graphs). |
Wed 11.05 16:00 |
Kevin Yang (Stanford) |
KPZ and Boltzmann-Gibbs PrincipleFluctuation theory for hydrodynamic limits of interacting particle systems in (1+1)-dimensions is conjectured to generally be governed by linear and (KPZ) quadratic corrections. Boltzmann-Gibbs principles are supposed to provide a general method of rigorously establishing something of this type. Much is known for stationary systems with sufficiently explicit invariant measures, while little is known for non-stationary systems outside a class of “partially integrable” models such as ASEP. In this talk, we broadly discuss KPZ equation fluctuations for general non-stationary systems. We then specialize to a perturbation of ASEP, where the main problem is deriving the aforementioned linear-type corrections with a method that should extend quite generally. |
Wed 18.05 16:00 |
Franco Severo (Zurich) |
On the off-critical level sets of smooth Gaussian fieldsWe consider the level sets of smooth Gaussian fields on R^{d} below a parameter ℓ∈R. As ℓ varies this defines a percolation model, whose critical point is denoted by ℓ_{c}. In this talk we will discuss the behaviour of these level sets on the off-critical regime, i.e. for ℓ ≠ ℓ_{c}. Our main result states that, for fields with positive and sufficiently fast decaying correlations, the connection probabilities decay exponentially for ℓ < ℓ_{c} and percolation occurs in sufficiently thick 2D slabs for ℓ> ℓ_{c}. This result, often referred to as (subcritical and supercritical, respectively) sharpness of phase transition, is typically the starting point for the study of finer properties of the off-critical phases. The result follows from a global comparison with a truncated and discretised version of the model, which may be of independent interest. The proof of this comparison relies on an interpolation scheme that integrates out the long-range and infinitesimal correlations of the model while compensating them with a small change in the parameter ℓ. |
Wed 25.05 16:00 |
Will FitzGerald (Sussex) |
Fredholm Pfaffians in random matrices and interacting particle systemsI will describe how probabilistic methods can be used to find asymptotics for Fredholm determinants and Fredholm Pfaffians. This has applications to the tail behaviour of the largest real eigenvalue for non-Hermitian random matrices, persistence probabilities for coalescing and annihilating Brownian motions and the probability that random polynomials have no real roots. |
Wed 1.06 16:00 |
Alexander Marynych (Kyiv) |
Lah distribution: properties and applicationsMotivated by a problem arising in the analysis of convex hulls of high-dimensional random walks, we introduce a new class of discrete probability distributions, which we call Lah distributions, and which involve Stirling numbers of both kinds. We provide a combinatorial interpretation of the Lah distributions in terms of random compositions and records and prove various limit theorems for them. This talk is based on a recent joint work with Zakhar Kabluchko (Münster, Germany). |
Wed 8.06 16:00 |
Pierre Tarrès (Shanghai) |
The *-Edge Reinforced random walk, bayesian statistics and statistical physicsWe will introduce recent non-reversible generalizations of the Edge-Reinforced Random Walk and its motivation in Bayesian statistics for variable order Markov Chains. The process is again partially exchangeable in the sense of Diaconis and Freedman (1982), and its mixing measure can be explicitly computed. It can also be associated to a continuous process called the *-Vertex Reinforced Random Walk, which itself is in general not exchangeable. We will also discuss some properties of that process.Based on joint work with S. Bacallado and C. Sabot. |
Wed 15.06 16:00 |
Makiko Sasada (Tokyo) |
KdV- and Toda-type discrete locally-defined dynamics and generalized Pitman’s transformThe Korteweg-de Vries equation (KdV equation) and the Toda lattice are typical and well-known classical integrable systems. For the KdV equation, the (almost-sure) well-posedness of a solution starting from a general ergodic random field on the line is still an open problem, though the invariance, as well as the well-posedness of a solution, of the white noise was proved recently by Killip, Murphy and Visan recently. In this talk, I will consider discretized versions of KdV equation and Toda lattice on the infinite one-dimensional lattice. These systems are understood as "deterministic vertex model”, which are discretely indexed in space and time, and their deterministic dynamics is defined locally via lattice equations. They have another formulation via the generalized Pitman’s transform, which is a new and crucial observation for our result. We show that there exists a unique solution to the initial value problem when the given data lies within a certain class, which includes the support of many shift ergodic measures. Also, a detailed balance criterion is presented that, amongst the measures that describe spatially independent and identically/alternately distributed configurations, characterizes those that are temporally invariant in distribution. This talk is based on a joint work with David Croydon and Satoshi Tsujimoto. |
Wed 22.06 16:00 |
Alice Guionnet (Lyon) |
Large deviations for the largest eigenvalue of random matriceThe understanding of the typical behaviour as well as the fluctuations of the spectrum has made tremendous progresses during the last thirty years. Yet, the study of large deviations has been so far restricted to integrable cases where the joint law of the eigenvalues is explicit or toheavy tailscases where large deviations are created by large entries. In this talk I will discuss the large deviations of the largest eigenvalue in the case of sub-Gaussian entries. This talk is based on joint works with F. Augeri, N. Cook, R. Ducatez and J. Husson. |
Wed 29.06 16:00 |
Anna Ben-Hamou (Paris) |