Éric Brunet

Function:
Professor assistant (« maître de conférences ») at Jussieu (Paris VI)
Address:
Laboratoire de Physique Statistique
École Normale Supérieure
24, rue Lhomond
75230 Paris Cedex 05; France
e-mail:
Eric.Brunet@lps.ens.fr
 
Office:
E238
Phone number:
01 44 32 34 91
Fax number:
01 44 32 34 33

Lectures notes (in french)

Subjects

I am mainly working on systems out of equilibrium, such as propagating fronts, growing surfaces or transport phenomenas. The goal is to study how the dynamics lead to a steady state, what are the properties of that steady state and, most important, what are the effects of noise on such systems. Another subject, which is, of course, closely related are disordered systems and, in particular, directed polymers in a random medium.

HDR

My HDR dissertation is titled Some aspects of the Fisher-KPP equation and the branching Brownian motion It has been defended on November the 3rd, 2016.

Publications

Papers in scientific journals

  1. Éric Brunet and Bernard Derrida, Shift in the velocity of a front due to a cutoff, Physical Review E 1997, 56 (3), 2597-2604.
    arXiv, PRE, pdf.
    We consider the effect of a small cut-off ε on the velocity of a traveling wave in one dimension. Simulations done over more than ten orders of magnitude as well as a simple theoretical argument indicate that the effect of the cut-off ε is to select a single velocity which converges when ε goes to 0 to the one predicted by the marginal stability argument. For small ε, the shift in velocity has the form K(log ε)-2 and our prediction for the constant K agrees very well with the results of our simulations. A very similar logarithmic shift appears in more complicated situations, in particular in finite size effects of some microscopic stochastic systems. Our theoretical approach can also be extended to give a simple way of deriving the shift in position due to initial conditions in the Fisher-Kolmogorov or similar equations.
    PACS numbers: 02.50.Ey, 03.40.Kf, 47.20.Ky
  2. Éric Brunet and Bernard Derrida, Microscopic models of traveling wave equations, Computer Physics Communications, 1999 121-122, 376-381.
    arXiv, CPC, pdf.
    Reaction-diffusion problems are often described at a macroscopic scale by partial derivative equations of the type of the Fisher or Kolmogorov-Petrovsky-Piscounov equation. These equations have a continuous family of front solutions, each of them corresponding to a different velocity of the front. By simulating systems of size up to N=1016 particles at the microscopic scale, where particles react and diffuse according to some stochastic rules, we show that a single velocity is selected for the front. This velocity converges logarithmically to the solution of the F-KPP equation with minimal velocity when the number N of particles increases. A simple calculation of the effect introduced by the cutoff due to the microscopic scale allows one to understand the origin of the logarithmic correction.
    PACS numbers: 02.50.Ey, 03.40.Kf, 47.20.Ky
  3. Éric Brunet and Bernard Derrida, Ground state energy of a non-integer number of particles with δ attractive interactions, Physica A 2000, 279 (1-4), 398-407.
    arXiv, Phys. A, pdf.
    We show how to define and calculate the ground state energy of a system of quantum particles with delta attractive interactions when the number of particles n is non-integer. The question is relevant to obtain the probability distribution of the free energy of a directed polymer in a random medium. When one expands the ground state energy in powers of the interaction, all the coefficients of the perturbation series are polynomials in n, allowing to define the perturbation theory for non-integer n. We develop a procedure to calculate all the cumulants of the free energy of the directed polymer and we give explicit, although complicated, expressions of the first three cumulants.
    PACS numbers: 05.40.+j, 02.50.-r, 82.20.-w.
  4. Éric Brunet and Bernard Derrida, Probability distribution of the free energy of a directed polymer in a random medium, Physical Review E 2000, 61 (6), 6789-6801.
    arXiv, PRE, pdf.
    We calculate exactly the first cumulants of the free energy of a directed polymer in a random medium for the geometry of a cylinder. By using the fact that the n-th moment <Zn> of the partition function is given by the ground state energy of a quantum problem of n interacting particles on a ring of length L, we write an integral equation allowing to expand these moments in powers of the strength of the disorder γ or in powers of n. For n small and n ~ (L γ)-1/2, the moments <Zn> take a scaling form which allows to describe all the fluctuations of order 1/L of the free energy per unit length of the directed polymer. The distribution of these fluctuations is the same as the one found recently in the asymmetric exclusion process, indicating that it is characteristic of all the systems described by the Kardar-Parisi-Zhang equation in 1+1 dimensions.
    P.A.C.S. numbers: 05.30, 05.70, 64.60 Cn.
  5. Éric Brunet and Bernard Derrida, Effect of Microscopic Noise on Front Propagation, Journal of Statistical Physics 2001, 103 (1-2), 269-282.
    JSP, pdf.
    We study the effect of the noise due to microscopic fluctuations on the position of a one dimensional front propagating from a stable to an unstable region in the “linearly marginal stability case”. By simulating a very simple system for which the effective number N of particles can be as large as N=10150, we measure the N dependence of the diffusion constant DN of the front and the shift of its velocity vN. Our results indicate that DN ~ (log N)-3. They also confirm our recent claim that the shift of velocity scales like vmin - vN~ K(log N)-2 and indicate that the numerical value of K is very close to the analytical expression Kapprox obtained in our previous work using a simple cut-off approximation.
  6. Éric Brunet, Fluctuations of the winding number of a directed polymer in a random medium , Physical Review E 2003, 68, 041101.
    arXiv, PRE, pdf.
    For a directed polymer in a random medium lying on an infinite cylinder, that is in 1+1 dimensions with finite width and periodic boundary conditions on the transverse direction, the winding number is simply the algebraic number of turns the polymer does around the cylinder. This paper presents exact expressions of the fluctuations of this winding number due to, first, the thermal noise of the system and, second, the different realizations of the disorder in the medium.
  7. Éric Brunet and Bernard Derrida, Exactly soluble noisy traveling-wave equation appearing in the problem of directed polymers in a random medium, Physical Review E 2004, 70, 016106.
    arXiv, PRE, pdf.
    We calculate exactly the velocity and diffusion constant of a microscopic stochastic model of N evolving particles which can be described by a noisy traveling wave equation with a noise of order N-1/2. Our model can be viewed as the infinite range limit of a directed polymer in random medium with N sites in the transverse direction. Despite some peculiarities of the traveling wave equations in the absence of noise, our exact solution allows us to test the validity of a simple cutoff approximation and to show that, in the weak noise limit, the position of the front can be completely described by the effect of the noise on the first particle.
  8. Daniel ben-Avraham and Éric Brunet, On the relation between one-species diffusion-limited coalescence and annihilation in one dimension, Journal of Physics A 2005, 38, 3247-3252.
    arXiv, J. Phys. A, pdf.
    The close similarity between the hierarchies of multiple-point correlation functions for the diffusion-limited coalescence and annihilation processes has caused some recent confusion, raising doubts as to whether such hierarchies uniquely determine an infinite particle system. We elucidate the precise relations between the two processes, arriving at the conclusion that the hierarchy of correlation functions does provide a complete representation of a particle system on the line. We also introduce a new hierarchy of probability density functions for finding particles at specified locations and none in between. This hierarchy is computable for coalescence, through the method of empty intervals, and is naturally suited for questions concerning the ordering of particles on the line.
  9. Éric Brunet, Bernard Derrida, Alfred H. Mueller and Stéphane Munier, A phenomenological theory giving the full statistics of the position of fluctuating pulled fronts, Physical Review E 2006, 73, 056126,
    arXiv, PRE, pdf.
    We propose a phenomenological description for the effect of a weak noise on the position of a front described by the Fisher-Kolmogorov-Petrovsky-Piscounov equation or any other travelling wave equation in the same class. Our scenario is based on four hypotheses on the relevant mechanism for the diffusion of the front. Our parameter-free analytical predictions for the velocity of the front, its diffusion constant and higher cumulants of its position agree with numerical simulations.
  10. Éric Brunet, Bernard Derrida, Alfred H. Mueller and Stéphane Munier, Noisy traveling waves: effect of selection on genealogies, Europhysics Letters 2006, 76 (1), 1-7,
    arXiv, EPL, pdf.
    For a family of models of evolving population under selection, which can be described by noisy traveling-wave equations, the coalescence times along the genealogical tree scale like lnα N, where N is the size of the population, in contrast with neutral models for which they scale like N. An argument relating this time scale to the diffusion constant of the noisy traveling wave leads to a prediction for α which agrees with our simulations. An exactly soluble case gives trees with statistics identical to those predicted for mean-field spin glasses by Parisi's theory.
  11. Éric Brunet, Bernard Derrida, Alfred H. Mueller and Stéphane Munier, Effect of selection on ancestry: An exactly soluble case and its phenomenological generalization , Physical Review E 2007, 76, 041104,
    arXiv, PRE, pdf.
    We consider a family of models describing the evolution under selection of a population whose dynamics can be related to the propagation of noisy traveling waves. For one particular model that we shall call the exponential model, the properties of the traveling wave front can be calculated exactly, as well as the statistics of the genealogy of the population. One striking result is that, for this particular model, the genealogical trees have the same statistics as the trees of replicas in the Parisi mean-field theory of spin glasses. We also find that in the exponential model, the coalescence times along these trees grow like the logarithm of the population size. A phenomenological picture of the propagation of wave fronts that we introduced in a previous work, as well as our numerical data, suggest that these statistics remain valid for a larger class of models, while the coalescence times grow like the cube of the logarithm of the population size.
  12. Igor M. Rouzine, Éric Brunet and Claus O. Wilke, The traveling wave approach to asexual evolution: Muller's ratchet and speed of adaptation, Theoretical Population Biology 2008, 73, 24–46,
    arXiv, Theor. pop. biol., pdf.
    We use traveling-wave theory to derive expressions for the rate of accumulation of deleterious mutations under Muller's ratchet and the speed of adaptation under positive selection in asexual populations. Traveling-wave theory is a semi-deterministic description of an evolving population, where the bulk of the population is modeled using deterministic equations, but the class of the highest-fitness genotypes, whose evolution over time determines loss or gain of fitness in the population, is given proper stochastic treatment. We derive improved methods to model the highest-fitness class (the stochastic edge) for both Muller's ratchet and adaptive evolution, and calculate analytic correction terms that compensate for inaccuracies which arise when treating discrete fitness classes as a continuum. We show that traveling-wave theory makes excellent predictions for the rate of mutation accumulation in the case of Muller's ratchet, and makes good predictions for the speed of adaptation in a very broad parameter range. We predict the adaptation rate to grow logarithmically in the population size until the population size is extremely large.
  13. Éric Brunet, Igor M. Rouzine and Claus O. Wilke, The stochastic edge in adaptive evolution, Genetics 2008, 179, 603–620,
    arXiv, Genetics, pdf.
    In a recent article, Desai and Fisher (2007) proposed that the speed of adaptation in an asexual population is determined by the dynamics of the stochastic edge of the population, that is, by the emergence and subsequent establishment of rare mutants that exceed the fitness of all sequences currently present in the population. Desai and Fisher perform an elaborate stochastic calculation of the mean time τ until a new class of mutants has been established, and interpret 1/τ as the speed of adaptation. As they note, however, their calculations are valid only for moderate speeds. This limitation arises from their method to determine τ: Desai and Fisher back-extrapolate the value of τ from the best-fit class' exponential growth at infinite time. This approach is not valid when the population adapts rapidly, because in this case the best-fit class grows non-exponentially during the relevant time interval. Here, we substantially extend Desai and Fisher's analysis of the stochastic edge. We show that we can apply Desai and Fisher's method to high speeds by either exponentially back-extrapolating from finite time or using a non-exponential back-extrapolation. Our results are compatible with predictions made using a different analytical approach (Rouzine et al. 2003, 2007), and agree well with numerical simulations.
  14. Éric Brunet, Bernard Derrida and Damien Simon, Universal tree structures in directed polymers and models of evolving populations , Physical Review E 2008, 78, 061102,
    arXiv, PRE, pdf.
    By measuring or calculating coalescence times for several models of coalescence or evolution, with and without selection, we show that the ratios of these coalescence times become universal in the large size limit and we identify a few universality classes.
  15. Éric Brunet and Bernard Derrida, Statistics at the tip of a branching random walk and the delay of traveling waves, Europhysics Letters 2009, 87, 60010
    arXiv, Eur. Phys. L., pdf.
    We study the limiting distribution of particles at the frontier of a branching random walk. The positions of these particles can be viewed as the lowest energies of a directed polymer in a random medium in the mean-field case. We show that the average distances between these leading particles can be computed as the delay of a traveling wave evolving according to the Fisher-KPP front equation. These average distances exhibit universal behaviors, different from those of the probability cascades studied recently in the context of mean field spin-glasses.
  16. Éric Brunet, Bernard Derrida and Antoine Gerschenfeld, Fluctuations of the heat flux of a one-dimensional hard particle gas , Europhysics Letters 2010, 90, 20004
    arXiv, abstract, pdf.
    Momentum-conserving one-dimensional models are known to exhibit anomalous Fourier's law, with a thermal conductivity varying as a power law of the system size. Here we measure, by numerical simulations, several cumulants of the heat flux of a one-dimensional hard particle gas. We find that the cumulants, like the conductivity, vary as power laws of the system size. Our results also indicate that cumulants higher than the second follow different power laws when one compares the ring geometry at equilibrium and the linear case in contact with two heat baths (at equal or unequal temperatures).
  17. Julien Berestycki, Éric Brunet, John W. Harris and Simon C. Harris, The almost-sure population growth rate in branching Brownian motion with a quadratic breeding potential , Statistics and Probability Letters 2010, 80, 1442-1446,
    arXiv, Stat. & Prob. L. pdf.
    In this note we consider a branching Brownian motion (BBM) on ℝ in which a particle at spatial position y splits into two at rate βy², where β>0 is a constant. This is a critical breeding rate for BBM in the sense that the expected population size blows up in finite time while the population size remains finite, almost surely, for all time. We find an asymptotic for the almost-sure rate of growth of the population.
  18. Éric Brunet and Bernard Derrida, A branching random walk seen from the tip, Journal of Statistical Physics 2011, 143, 420-446,
    arXiv, J. Stat. Phys., pdf.
    We show that all the time-dependent statistical properties of the rightmost points of a branching Brownian motion can be extracted from the traveling wave solutions of the Fisher-KPP equation. The distribution of all the distances between the rightmost points has a long time limit which can be understood as the delay of the Fisher-KPP traveling waves when the initial condition is modified. The limiting measure exhibits the surprising property of superposability: the statistical properties of the distances between the rightmost points of the union of two realizations of the branching Brownian motion shifted by arbitrary amounts are the same as those of a single realization. We discuss the extension of our results to more general branching random walks.
  19. Éric Brunet and Bernard Derrida, How genealogies are affected by the speed of evolution, Philosophical Magazine 2012, 92, 255-271,
    arXiv, Ph. Mag., pdf.
    In a series of recent works it has been shown that a class of simple models of evolving populations under selection leads to genealogical trees whose statistics are given by the Bolthausen-Sznitman coalescent rather than by the well-known Kingman coalescent in the case of neutral evolution. Here we show that when conditioning the genealogies on the speed of evolution, one finds a one-parameter family of tree statistics which interpolates between the Bolthausen-Sznitman and Kingman coalescents. This interpolation can be calculated explicitly for one specific version of the model, the exponential model. Numerical simulations of another version of the model and a phenomenological theory indicate that this one-parameter family of tree statistics could be universal. We compare this tree structure with those appearing in other contexts, in particular in the mean field theory of spin glasses.
  20. Elie Aïdékon, Julien Berestycki, Éric Brunet and Zhan Shi, Branching Brownian motion seen from its tip, Probab. Theory Relat. Fields, 2013, 157, 405-451
    arXiv, Probab. Theory Relat. Fields, pdf.
    It has been conjectured since the work of Lalley and Sellke (Ann. Probab., 15, 1052-1061, 1987) that branching Brownian motion seen from its tip (e.g. from its rightmost particle) converges to an invariant point process. Very recently, it emerged that this can be proved in several different ways (see e.g. Brunet and Derrida, A branching random walk seen from the tip, 2010, Poissonian statistics in the extremal process of branching Brownian motion, 2010; Arguin et al., The extremal process of branching Brownian motion, 2011). The structure of this extremal point process turns out to be a Poisson point process with exponential intensity in which each atom has been decorated by an independent copy of an auxiliary point process. The main goal of the present work is to give a complete description of the limit object via an explicit construction of this decoration point process. Another proof and description has been obtained independently by Arguin et al. (The extremal process of branching Brownian motion, 2011).
  21. Éric Brunet and Bernard Derrida, Genealogies in simple models of evolution, J. Stat. Mech. 2013, P01006,
    arXiv, J. Stat. Mech., pdf.
    We review the statistical properties of the genealogies of a few models of evolution. In the asexual case, selection leads to coalescence times which grow logarithmically with the size of the population in contrast with the linear growth of the neutral case. Moreover for a whole class of models, the statistics of the genealogies are those of the Bolthausen-Sznitman coalescent rather than the Kingman coalescent in the neutral case. For sexual reproduction, the time to reach the first common ancestors to the whole population and the time for all individuals to have all their ancestors in common are also logarithmic in the neutral case, as predicted by Chang []. We discuss how these times are modified in a simple way of introducing selection.
  22. Julien Berestycki, Éric Brunet, John W. Harris, Simon C. Harris and Matthew I. Roberts, Growth rates of the population in a branching Brownian motion with an inhomogeneous breeding potential, Stoch. Proc. Appl. 2015, 5, 2096-2145
    arXiv, Stoch. Proc. Appl., pdf.
    We consider a branching particle system where each particle moves as an independent Brownian motion and breeds at a rate proportional to its distance from the origin raised to the power p, for p∈[0,2). The asymptotic behaviour of the right-most particle for this system is already known; in this article we give large deviations probabilities for particles following “difficult” paths, growth rates along “easy” paths, the total population growth rate, and we derive the optimal paths which particles must follow to achieve this growth rate.
  23. Éric Brunet and Bernard Derrida, An exactly solvable travelling wave equation in the Fisher-KPP class, Journal of Statistical Physics 2015, 161 (4), 801-820.
    arXiv, J. Stat. Phys, pdf.
    For a simple one dimensional lattice version of a travelling wave equation, we obtain an exact relation between the initial condition and the position of the front at any later time. This exact relation takes the form of an inverse problem: given the times tn at which the travelling wave reaches the positions n, one can deduce the initial profile. We show, by means of complex analysis, that a number of known properties of travelling wave equations in the Fisher-KPP class can be recovered, in particular Bramson's shifts of the positions. We also recover and generalize Ebert-van Saarloos' corrections depending on the initial condition.
  24. Julien Berestycki, Éric Brunet and Zhan Shi, The number of accessible paths in the hypercube, Bernoulli 2016, 22 (2), 653-680
    arXiv, Bernoulli.
    Motivated by an evolutionary biology question, we study the following problem: we consider the hypercube {0,1}L where each node carries an independent random variable uniformly distributed on [0,1], except (1,1,...,1) which carries the value 1 and (0,0,...,0) which carries the value x ∈ [0,1]. We study the number θ of paths from the root (0,0,...,0) to the opposite corner (1,1,...,1) along which the values on the nodes form an increasing sequence. We show that if the value on the root is set to x=X/L then θ/L converges in law as L goes to infinity to exp(-X) times the product of two standard independent exponential variables.
    As a first step in the analysis we study the same question when the graph is that of a tree where the root has arity L, each node at level 1 has arity L-1, .., and the nodes at level L-1 have only one offspring which are the leaves of the tree (all the leaves are assigned the value 1, the root the value x ∈ [0,1]).
  25. Julien Berestycki, Éric Brunet and Zhan Shi, Accessibility percolation with backsteps, ALEA 2017, 14, 45-62
    arXiv, ALEA, pdf.
    Consider a graph in which each site is endowed with a value called fitness. A path in the graph is said to be "open" or "accessible" if the fitness values along that path is strictly increasing. We say that there is accessibility percolation between two sites when such a path between them exists. Motivated by the so called House-of-Cards model from evolutionary biology, we consider this question on the L-hypercube {0,1}L where the fitness values are independent random variables. We show that, in the large L limit, the probability that an accessible path exists from an arbitrary starting point to the (random) fittest site is no more than x*1/2=1-1/2 sinh-1(2)=0.27818... and we conjecture that this probability does converge to x*1/2. More precisely, there is a phase transition on the value of the fitness x of the starting site: assuming that the fitnesses are uniform in [0,1], we show that, in the large L limit, there is almost surely no path to the fittest site if x>x*1/2 and we conjecture that there are almost surely many paths if x<x*1/2. If one conditions on the fittest site to be on the opposite corner of the starting site rather than being randomly chosen, the picture remains the same but with the critical point being now x*1=1-sinh-1(1)=0.11863.... Along the way, we obtain a large L estimation for the number of self-avoiding paths joining two opposite corners of the L-hypercube.
  26. Julien Berestycki, Éric Brunet, Simon C. Harris and Matthew I. Roberts, Vanishing corrections for the position in a linear model of FKPP fronts Communications in Mathematical Physics 2017, 349, 857-893,
    arXiv, CIMP, pdf.
    Take the linearised FKPP equation ∂t h=∂xx h+h with boundary condition h(m(t),t)=0. Depending on the behaviour of the initial condition h0(x)=h(x,0) we obtain the asymptotics — up to a o(1) term r(t) — of the absorbing boundary m(t) such that ω(x):=limth(x +m(t),t) exists and is non-trivial. In particular, as in Bramson's results for the non-linear FKPP equation, we recover the celebrated −(3/2)log t correction for initial conditions decaying faster than xνex for some ν<−2. Furthermore, when we are in this regime, the main result of the present work is the identification (to first order) of the r(t) term which ensures the fastest convergence to ω(x). When h0(x) decays faster than xνex for some ν<−3, we show that r(t) must be chosen to be −3(π/t)1/2 which is precisely the term predicted heuristically by Ebert-van Saarloos in the non-linear case. When the initial condition decays as xνex for some ν∈[−3,−2), we show that even though we are still in the regime where Bramson's correction is −(3/2)log t, the Ebert-van Saarloos correction has to be modified. Similar results were recently obtained by Henderson using an analytical approach and only for compactly supported initial conditions.
  27. Julien Berestycki, Éric Brunet, A note of the convergence of the Fisher-KPP front centred around its α-level preprint 2016
    arXiv.
    We consider the solution u(x,t) of the Fisher-KPP equation ∂tu=∂x2u+uu2 centred around its α-level μt(α) defined as u(μt(α),t)=α. It is well known that for an initial datum that decreases fast enough, then u( μt(α)+x,t) converges as t→∞ to the critical travelling wave. We study in this paper the speed of this convergence and the asymptotic expansion of μt(α) for large t. It is known from Bramson that for initial conditions that decay fast enough, one has μt(α)=2t−(3/2)ln t+Cste+o(1). Work is under way [] to show that the o(1) in the expansion is in fact a k(α)/√t+O(tϵ−1) for any ϵ>0 for some k(α), where it is not clear at this point whether k(α) depends or not on α. We show that, unless the time derivative of μt(α) has a very unexpected behaviour at infinity, the coefficient k(α) does not, in fact, depend on α. We also conjecture that, for an initial condition that decays fast enough, one has in fact μt(α)=2t−(3/2)ln t+Cste−(3π)/√t+g ln(t)/t+o(1/t) for some constant g which does not depend on α.
  28. Julien Berestycki, Éric Brunet, Simon C. Harris and Piotr Miłoś, Branching Brownian motion with absorption and the all-time minimum of branching Brownian motion with drift, accepted in 2017 by the Journal of Functional Analysis.
    arXiv.
    We study a dyadic branching Brownian motion on the real line with absorption at 0, drift μ∈ℝ and started from a single particle at position x>0. When μ is large enough so that the process has a positive probability of survival, we consider K(t), the number of individuals absorbed at 0 by time t and for s≥0 the functions ωs(x):=𝔼x[sK(∞)]. We show that ωs<∞ if and only of s∈[0,s0] for some s0>1 and we study the properties of these functions. Furthermore, for s=0, ω(x):=ω0(x)=ℙx(K(∞)=0) is the cumulative distribution function of the all time minimum of the branching Brownian motion with drift started at 0 without absorption. We give three descriptions of the family ωs, s∈[0,s0] through a single pair of functions, as the two extremal solutions of the Kolmogorov-Petrovskii-Piskunov (KPP) traveling wave equation on the half-line, through a martingale representation and as an explicit series expansion. We also obtain a precise result concerning the tail behavior of K(∞). In addition, in the regime where K(∞)>0 almost surely, we show that u(x,t):=ℙx(K(∞)=0) suitably centered converges to the KPP critical travelling wave on the whole real line.
  29. Julien Berestycki, Éric Brunet and Bernard Derrida, Exact solution and precise asymptotics of a Fisher-KPP type front, submitted in 2017 to Journal of Physics A
    arXiv.
    The present work concerns a version of the Fisher-KPP equation where the nonlinear term is replaced by a saturation mechanism, yielding a free boundary problem with mixed conditions. Following an idea proposed in [BrunetDerrida.2015], we show that the Laplace transform of the initial condition is directly related to some functional of the front position μt. We then obtain precise asymptotics of the front position by means of singularity analysis. In particular, we recover the so-called Ebert and van Saarloos correction [EbertvanSaarloos.2000], we obtain an additional term of order log t / t in this expansion, and we give precise conditions on the initial condition for those terms to be present.

Phd thesis

Influence des effets de taille finie sur la propagation d'un front — Distribution de l'énergie libre d'un polymère dirigé en milieu aléatoire (2000)
(gzipped postscript of 2.5 Mo, in french)

Book

  1. A. Aspect, F. Bouchet, É. Brunet, C. Cohen-Tannoudji, J. Dalibard, T. Damour, O. Darrigol, B. Derrida, P. Grangier, F. Laloë et J.-P. Pocholle, Einstein aujourd'hui, EDP sciences (2005)
    Ce livre a pour objectif de montrer combien les idées d'Einstein continuent à inspirer la science de ce début du XXIe siècle, après avoir révolutionné celle du XXe. Le livre contient sept contributions : une introduction historique et six articles retraçant les travaux les plus importants d'Einstein et leur impact sur la physique d'aujourd'hui : intrication de systèmes quantiques, condensation de Bose-Einstein, émission stimulée et laser, fluctuations et mouvement brownien, relativité générale, cosmologie.

Communications in conferences