This workshop is funded by the EPSRC project Emergence of condensation in stochastic systems. It will be held at the University of Bath from the 4th to the 6th of July. Anyone interested in attending the workshop is welcome to email the organisers Stefan Grosskinsky, Peter Mörters and Cécile Mailler.
The workshop will take place in the Wolfson lecture theatre in the maths department (building 4W, room 1.7). For more information about how to get there, please see below.
Inés Armendáriz (University of Buenos Aires) Márton Balázs (University of Bristol) Volker Betz (University of Darmstadt) Alessandra Bianchi (University of Padova) Ginestra Bianconi (Queen Mary University of London) Paul Chleboun (University of Warwick) Amin Coja-Oghlan (Goethe University, Francfort) Steffen Dereich (University of Münster) Claude Godrèche (CEA Saclay) Watthanan (Mim) Jatuviriyapornchai (University of Warwick) Jonathan Jordan (University of Sheffield) |
Michail Loulakis (National TU of Athens) Sam Moore (University of Bath) Stephen Pagett (University of Bath) Tom Rafferty (University of Warwick) Frank Redig (TU Delft) Gunter Schütz (Jülich Research Centre) Batı Şengül (University of Bath) Anna Senkevich (University of Bath) Alexandre Stauffer (University of Bath) Juraj Szavitz-Nossan (University of Edinburgh) Erik Törnblad (University of Uppsala) Daniel Ueltschi (University of Warwick) |
Monday | Tuesday | Wednesday | |
---|---|---|---|
9:00 -- 9:30 | Welcome | Amin Coja-Oghlan | Alessandra Bianchi |
9:30 -- 10:00 | Gunter Schütz | ||
10:00 -- 10:30 | coffee | coffee | |
10:30 -- 11:00 | coffee | Steffen Dereich | Batı Şengül |
11:00 -- 11:30 | Claude Godrèche | ||
11:30 -- 12:00 | Volker Betz | Paul Chleboun | |
12:00 -- 12:30 | Mim Jatuviriyapornchai | ||
12:30 -- 13:00 | lunch | lunch | lunch |
13:00 -- 13:30 | |||
13:30 -- 14:00 | |||
14:00 -- 14:30 | Michail Loulakis | Juraj Szavitz-Nossan | |
14:30 -- 15:00 | |||
15:00 -- 15:30 | Inés Armendáriz | Ginestra Bianconi | |
15:30 -- 16:00 | |||
16:00 -- 16:30 | coffee | coffee | |
16:30 -- 17:00 | Daniel Ueltschi | Frank Redig | |
17:00 -- 17:30 | |||
wine and pizza reception | dinner |
Zero-range processes with decreasing jump rates are known to exhibit condensation, where a finite fraction of all particles concentrates on a single lattice site. We will consider two such models. In a first result, we study a zero-range process on a one-dimensional lattice with periodic boundary conditions in the thermodynamic limit with fixed, super-critical particle density. We show that the process exhibits metastability with respect to the condensate location, and the suitably accelerated process of the rescaled location converges to a limiting Markov process on the unit torus. In a second result we consider a zero-range process in the totally connected graph with L vertices and a number N~log(L) of particles that determine a vanishing density. We show that for this model the fluid configurations, where each site contains at most one particle are metastable as well. Moreover, for the right choice of parameters, the best way to perform a transition between condensate configurations is to go through the fluid, while each condensate well is deeper that the fluid set. Joint work with S. Grosskinsky, M. Loulakis, A de Masi and E. Presutti.
Spatial random permutations are made so that they favor permutations that map points to nearby points. The strength of this effect is encoded in a parameter alpha > 0, where larger alpha means stronger bias toward short jumps. I will introduce some variants of the model, and explain the connections to the theory of Bose-Einstein condensation. Then I will present a few older results, as well as very recent progress made jointly with Lorenzo Taggi (TU Darmstadt) for the regime of large alpha. Finally, I will discuss two conjectures suggested by numerical simulation: in two dimensions, the model appears to exhibit a Kosterlitz-Thouless phase transition, and there are reasons to believe that in the phase of algebraic decay of correlations, long cycles are Schramm-Löwner curves, with parameter between 4 and 8 depending on alpha.
The inclusion process is a stochastic lattice gas where particles perform random walks subjected to mutual attraction, thus providing the natural bosonic counterpart of the well-studied exclusion process. Due to attractive interaction between the particles, the inclusion process can exhibit a condensation transition, where a finite fraction of all particles concentrates on a single site. In this talk we characterize the dynamics of the condensate for the reversible inclusion process on a finite set S, in the limit of total number of particles going to infinity. By potential theoretic techniques, we determine the time-scales associated to the transitions of the condensate from one site to another, and we show that the limiting dynamics of the condensate is a suitable continuous time random walk on S. Joint work with S. Dommers and C. Giardinà.
In this talk I will provide an overview of the Bose-Einstein condensation in simple complex networks providing both analytical and extensive numerical results describing the detailed stochastic dynamics of the Bianconi-Barabási model above and below the condensation transition. These results indicate that in the network at there is a subextensive number of nodes that acquire a finite fraction of the links. I will discuss an interesting variation of the model to describe weighted complex networks where there is a condensation transition in which few links acquire a finite fraction of all the weight of the network. Finally I will show that the Bianconi-Barabasi model is a subcase of a wider model called Network Geometry with Flavor describing simplicial complexes whose statistical properties depend on quantum statistics and I will describe the phase transition occurring in this model.
Stochastic monotonicity is an extremely useful property of many interacting particle systems, combined with coupling methods it is a key tool in determining the set of invariant measures for certain process and obtaining hydrodynamic limits. We study stochastic particle systems that conserve the particle density and exhibit a condensation transition due to the particle interaction. On a fixed lattice the condensation transition occurs as the total number of particles diverges, the system separates into homogeneous phase distributed at the maximal invariant measure, and a condensate where a diverging number of particles concentrates on a single lattice site. We study spatially homogeneous processes which exhibit this phenomena, and have product stationary measures. Such processes include zero-range process and more general misanthrope processes. All known examples are not stochastically monotone. We are able to show that in fact all such processes, with finite critical density, are necessarily non-monotone. Condensation can occur on finite lattices even if the critical density is not finite, we discuss an example that appears to be both condensing and monotone. This is joint work with Thomas Rafferty and Stefan Grosskinsky.
Factor graph models have been used to describe a wide range of objects in physics, combinatorics, information theory and computer science. In particular, this includes `mean-field' models of disordered systems such as glasses. Physics methods predict that in many of these objects a condensation phase transition occurs, which is similar in nature to the Kauzmann phase transition in glasses. In this talk I will explore this phenomenon from the abstract perspective of limits of discrete measures.
In 2001 Bianconi and Barabási observed an intriguing condensation phenomenon in preferential attachment models with fitness. In the condensation phase, in the limit, there is a comparably small set of vertices (the condensate) that attracts a constant fraction of new links established by new vertices. We provide new results on the formation of the condensate in the case where the fitness distribution is bounded and has polynomial tails.
We study the coarsening dynamics of a prototypical model of condensing ZRP, with hopping rate u_k = 1+b/k^\sigma, (0<\sigma<1).
Zero-range processes and inclusion processes are well known to exhibit a condensation transition under certain conditions on the jump rates, and the dynamics of this transition continues to be a subject of current research interest. Starting from homogeneous initial conditions, the time evolution of the condensed phase exhibits an interesting coarsening phenomenon of mass transport between cluster sites. The single site dynamics of the processes form a birth death chain describing the coarsening behaviour. We introduce a size-biased version of the single site process, which provides an effective tool to analyze the dynamics of the condensed phase without finite size effects.
The conditional distribution of i.i.d. random variables with thin tails subject to a large deviation of their sum is described by Gibbs' conditioning principle. We will present a version of Gibbs' conditioning principle for subexponential random variables and show how this result explains condensation in the Evans model for Zero Range Processes. Further, we will derive how the condensate emerges around the critical density. Joint work with Inés Armendáriz and Stefan Grosskinsky.
We introduce a recent model from econo-physics, the so-called immediate exchange model. This is a model with two-agent exchanges where the wealth of each agent is uniformly split in two parts, top-parts are exchanged, and the new parts are added up again. We show that this has a discrete dual which in turn is related to the symmetric inclusion process via thermalization. This immediately yields a generalization to a two parameter family of models (where the splitting is Beta distributed) having similar properties. This then further leads to a quite general class of models where a discrete or continuous quantity is split, exchanged and added up again. We discuss how derive to self-dualities for such models, via additive structure of symmetries. As a consequence, one can characterize stationary measures and ergodic behaviour. Based on joint work with Federico Sau (Delft)
We study the asymmetric zero-range process (ZRP) with L sites and open boundaries, conditioned to carry an atypical current. Using a generalized Doob h-transform we compute explicitly the transition rates of an effective process for which the conditioned dynamics are typical. This effective process is a zero-range process with renormalized hopping rates, which are space dependent even when the original rates are constant. This leads to non-trivial density profiles in the steady state of the conditioned dynamics, and, under generic conditions on the jump rates of the unconditioned ZRP, to an intriguing supercritical bulk region where condensates can grow. These results provide a microscopic perspective on macroscopic fluctuation theory (MFT) for the weakly asymmetric case: It turns out that the predictions of MFT remain valid in the non-rigorous limit of finite asymmetry. In addition, the microscopic results yield the correct scaling factor for the asymmetry that MFT cannot predict.
The interchange process on a finite graph is obtained by placing a particle on each vertex of the graph, then at rate 1, selecting an edge uniformly at random and swapping the two particles at either end of this edge. We consider this process on the 2-dimensional Hamming graph. The main result is a phase transition: in the subcritical phase, all of the cycles of the process have length O(log n), whereas in the supercritical phase a positive density of vertices lie in cycles of length at least n^{2-\eps}. This is joint work with Piotr Miƚoś.).
We study a reflected random walk (random walk that stays non-negative), conditioned to atypical area and local time (the number of returns to the origin). For the double exponential (Laplace) jump distribution, we show that the process exhibits condensation phenomenon by which a single random walk excursion (path between two successive returns to the origin) takes a macroscopic fraction of the total area. Our results can be mapped to stochastic lattice gases with pair-factorised steady states, providing an alternative explanation for the spatially-extended (interaction-driven) condensation from the standpoint of the large deviation theory.
We study random permutations of the vertices of the hypercube. The permutations are given by products of (uniform, independent) random transpositions on edges. We establish the existence of a phase transition accompanied by cycles of diverging lengths. (Joint work with R. Kotecký and P. Miƚoś.).
The closest airport to Bath is Bristol airport. Once there, you can take either the A4 bus to Bath or the Airport Flyer bus to Bristol main train station (Temple Meads) and then the train to Bath. The A4 bus is a big green bus that runs every 30 minutes in day time and every hour early morning and late evening; it costs £20 a return (pay to the driver in cash) and takes you directly to Bath, near the train station, in 50 minutes. The Airport Flyer is more frequent, costs approximately £7 (pay to the driver in cash) and takes you to Bristol Temple Meads in 20 minutes. There, you can buy a single trip to Bath for approximately £7. The overall journey will take approximately 50 minutes.
If you can't find a convenient flight to Bristol airport, it's most likely that you'll find a flight to London. The most convenient airport to come to Bath is definitely London Heathrow. From there, there are different options to join Bath. You can take the Heathrow Express to London Paddington (approx. 30 minutes) and there take a direct train to Bath (90 minutes). You can book your train tickets online, for example on the First Great Western website. The second option is coach: National Express runs regular direct buses from Heathrow to Bath, the fastest ones take two hours and this option is generally cheaper that the previous one - you can book your tickets online on the National Express website. The third option is to take the RailAir bus from Heathrow to Reading and there a direct train to Bath. It takes approximately two hours.
The university is not very far from the train station and, looking at a map, you could be tempted to walk there. Be aware that the university is on top of a steep hill and the walk up might not be as pleasant as it seems: the walk down, on the other hand, is very pleasant and offers nice views on the city (at least when it's not raining).
To go from the train station to the university, you can take the bus (U1 or U18) and pay to the driver when you jump on. The bus stop is in front of the bus station, near the Sainsbury's local. The U1 and the U18 are run by two different companies, meaning that if you buy a return, it will only be accepted in the corresponding company for the way back. The university is the last stop of the bus.
The workshop will take place in the Wolfson Lecture theatre. It is in the 4W building, on the lowest floor. From the bus stop, walk up the stairs onto the parade (follow the people that were on the same bus). Continue walking straight until you pass the Librairy on your right. Continue straight after the Librairy. The 4W building will then be on your left (with glass automated doors). Enter the building: the Tiki café is on your right and the Student services on your left. Take the stairs in front of you to the lowest level: the Wolfson theatre is on your left, after the pigeon holes and the lifts.
The organisers have booked rooms in town for the participants. Details will be emailed to them closer to the time. The participants will be able to commute by bus to the university, using the buses U1 and U18 (same route, different companies).