arXiv subjects

J. L. Lebowitz

Publications and source records attributed to J. L. Lebowitz.

At least 19 recordsLinked to original sources

arXiv2024

Approach to Hyperuniformity in the One-Dimensional Facilitated Exclusion Process

For the one-dimensional Facilitated Exclusion Process with initial state a product measure of density $\rho=1/2-\delta$, $\delta\ge0$, there exists an infinite-time limiting state $\nu_\rho$ in which all particles are isolated and hence cannot move. We study the variance $V(L)$, under $\nu_\rho$, of the number of particles in an interval of $L$ sites. Under $\nu_{1/2}$ either all odd or all even sites are occupied, so that $V(L)=0$ for $L$ even and $V(L)=1/4$ for $L$ odd: the state is hyperuniform, since $V(L)$ grows more slowly than $L$. We prove that for densities approaching 1/2 from below there exist three regimes in $L$, in which the variance grows at different rates: for $L\gg\delta^{-2}$, $V(L)\simeq\rho(1-\rho)L$, just as in the initial state; for $A(\delta)\ll L\ll\delta^{-2}$, with $A(\delta)=\delta^{-2/3}$ for $L$ odd and $A(\delta)=1$ for $L$ even, $V(L)\simeq CL^{3/2}$ with $C=2\sqrt{2/\pi}/3$; and for $L\ll\delta^{-2/3}$ with $L$ odd, $V(L)\simeq1/4$. The analysis is based on a careful study of a renewal process with a long tail. Our study is motivated by simulation results showing similar behavior in higher dimensions; we discuss this background briefly.

math.PR↗

arXiv2024

Time evolution of the Boltzmann entropy for a nonequilibrium dilute gas

We investigate the time evolution of the Boltzmann entropy of a dilute gas of N particles, N>>1, as it undergoes a free expansion doubling its volume. The microstate of the system, a point in the 4N dimensional phase space, changes in time via Hamiltonian dynamics. Its entropy, at any time $t$, is given by the logarithm of the phase space volume of all the microstates giving rise to its macrostate at time $t$. The macrostates that we consider are defined by coarse graining the one-particle phase space into cells $\Delta_\alpha$. The initial and final macrostates of the system are equilibrium states in volumes $V$ and $2V$, with the same energy $E$ and particle number $N$. Their entropy per particle is given, for sufficiently large systems, by the thermodynamic entropy as a function of the particle and energy density, whose leading term is independent of the size of the $\Delta_\alpha$. The intermediate (non-equilibrium) entropy does however depend on the size of the cells $\Delta_\alpha$. Its change with time is due to (i) dispersal in physical space from free motion and to (ii) the collisions between particles which change their velocities. The former depends strongly on the size of the velocity coarse graining $\Delta v$: it produces entropy at a rate proportional to $\Delta v$. This dependence is investigated numerically and analytically for a dilute two-dimensional gas of hard discs. It becomes significant when the mean free path between collisions is of the same order or larger than the length scale of the initial spatial inhomogeneity. In the opposite limit, the rate of entropy production is essentially independent of $\Delta v$ and is given by the Boltzmann equation for the limit $\Delta v\rightarrow 0$. We show that when both processes are active the time dependence of the entropy has a scaling form involving the ratio of the rates of its production by the two processes.

cond-mat.stat-mech↗

arXiv2024

Approach to Hyperuniformity of Steady States of Facilitated Exchange Processes

We consider the fluctuations in the number of particles in a box of size L^d in Z^d, d>=1, in the (infinite volume) translation invariant stationary states of the facilitated exclusion process, also called the conserved lattice gas model. When started in a Bernoulli (product) measure at density rho, these systems approach, as t goes to infinity, a "frozen" state for rho<=rho_c, with rho_c=1/2 for d=1 and rho_c<1/2 for d>=2. At rho=rho_c the limiting state is hyperuniform, that is, the variance of the number of particles in the box grows slower than L^d. We give a general description of how the variances at different scales of L behave as rho increases to rho_c. On the largest scale, L>>L_2, the fluctuations are normal (in fact the same as in the original product measure), while in a region L_1< =2.)

cond-mat.stat-mech↗

arXiv2022

Stationary States of the One-Dimensional Discrete-Time Facilitated Symmetric Exclusion Process

We describe the extremal translation invariant stationary (ETIS) states of the facilitated exclusion process on $\mathbb{Z}$. In this model all particles on sites with one occupied and one empty neighbor jump at each integer time to the empty neighbor site, and if two particles attempt to jump into the same empty site we choose one randomly to succeed. The ETIS states are qualitatively different for densities $ρ<1/2$, $ρ=1/2$, and $1/2<ρ<1$, but in each density region we find states which may be grouped into families, each of which is in natural correspondence with the set of all ergodic measures on $\{0,1\}^{\mathbb{Z}}$. For $ρ<1/2$ there is one such family, containing all the ergodic states in which the probability of two adjacent occupied sites is zero. For $ρ=1/2$ there are two families, in which configurations translate to the left and right, respectively, with constant speed 2. For the high density case there is a continuum of families. We show that all ETIS states at densities $ρ\le1/2$ belong to these families, and conjecture that also at high density there are no other ETIS states. We also study the possible ETIS states which might occur if the conjecture fails.

math.PR↗

arXiv2021

Stationary States of the One-dimensional Facilitated Asymmetric Exclusion Process

We describe the translation invariant stationary states (TIS) of the one-dimensional facilitated asymmetric exclusion process in continuous time, in which a particle at site $i\in\mathbb{Z}$ jumps to site $i+1$ (respectively $i-1$) with rate $p$ (resp. $1-p$), provided that site $i-1$ (resp. $i+1$) is occupied and site $i+1$ (resp. $i-1$) is empty. All TIS states with density $ρ\le1/2$ are supported on trapped configurations in which no two adjacent sites are occupied; we prove that if in this case the initial state is i.i.d.~Bernoulli then the final state is independent of $p$. This independence also holds for the system on a finite ring. For $ρ>1/2$ there is only one TIS. It is the infinite volume limit of the probability distribution that gives uniform weight to all configurations in which no two holes are adjacent, and is isomorphic to the Gibbs measure for hard core particles with nearest neighbor exclusion.

math.PR↗

arXiv2020

The Discrete-Time Facilitated Totally Asymmetric Simple Exclusion Process

We describe the translation invariant stationary states of the one dimensional discrete-time facilitated totally asymmetric simple exclusion process (F-TASEP). In this system a particle at site $j$ in $Z$ jumps, at integer times, to site $j+1$, provided site $j-1$ is occupied and site $j+1$ is empty. This defines a deterministic noninvertible dynamical evolution from any specified initial configuration on $\{0,1\}^{Z}$. When started with a Bernoulli product measure at density $ρ$ the system approaches a stationary state, with phase transitions at $ρ=1/2$ and $ρ=2/3$. We discuss various properties of these states in the different density regimes $0<ρ<1/2$, $1/2<ρ<2/3$, and $2/3<ρ<1$; for example, we show that the pair correlation $g(j)=\langleη(i)η(i+j)\rangle$ satisfies, for all $n\in Z$, $\sum_{j=kn+1}^{k(n+1)}g(j)=kρ^2$, with $k=2$ when $0 \le ρ\le 1/2$ and $k=3$ when $2/3 \le ρ\le 1$, and conjecture (on the basis of simulations) that the same identity holds with $k=6$ when $1/2 \le ρ\le 2/3$. The $ρ<1/2$ stationary state referred to above is also the stationary state for the deterministic discrete-time TASEP at density $ρ$ (with Bernoulli initial state) or, after exchange of particles and holes, at density $1-ρ$.

math-ph↗

arXiv2019

Exact Solution of the F-TASEP

We obtain the exact solution of the facilitated totally asymmetric simple exclusion process (F-TASEP) in 1D. The model is closely related to the conserved lattice gas (CLG) model and to some cellular automaton traffic models. In the F-TASEP a particle at site $j$ in $\mathbb{Z}$ jumps, at integer times, to site $j+1$, provided site $j-1$ is occupied and site $j+1$ is empty. When started with a Bernoulli product measure at density $ρ$ the system approaches a stationary state. This non-equilibrium steady state (NESS) has phase transitions at $ρ=1/2$ and $ρ=2/3$. The different density regimes $0<ρ<1/2$, $1/2<ρ<2/3$, and $2/3<ρ<1$ exhibit many surprising properties; for example, the pair correlation $g(j)=\langleη(i)η(i+j)\rangle$ satisfies, for all $n\in\mathbb{Z}$, $\sum_{j=kn+1}^{k(n+1)}g(j)=kρ^2$, with $k=2$ when $0\leρ\le1/2$, $k=6$ when $1/2\leρ\le2/3$, and $k=3$ when $2/3\leρ\le1$. The quantity $\lim_{L\to\infty}V_L/L$, where $V_L$ is the variance in the number of particles in an interval of length L, jumps discontinuosly from $ρ(1-ρ)$ to 0 when $ρ\to1/2$ and when $ρ\to2/3$.

cond-mat.stat-mech↗

arXiv2016

Translation invariant extensions of finite volume measures

We investigate the following questions: Given a measure $μ_Λ$ on configurations on a subset $Λ$ of a lattice $\mathbb{L}$, where a configuration is an element of $Ω^Λ$ for some fixed set $Ω$, does there exist a measure $μ$ on configurations on all of $\mathbb{L}$, invariant under some specified symmetry group of $\mathbb{L}$, such that $μ_Λ$ is its marginal on configurations on $Λ$? When the answer is yes, what are the properties, e.g., the entropies, of such measures? Our primary focus is the case in which $\mathbb{L}=\mathbb{Z}^d$ and the symmetries are the translations. For the case in which $Λ$ is an interval in $\mathbb{Z}$ we give a simple necessary and sufficient condition, local translation invariance (LTI), for extendibility. For LTI measures we construct extensions having maximal entropy, which we show are Gibbs measures; this construction extends to the case in which $\mathbb{L}$ is the Bethe lattice. On $\mathbb{Z}$ we also consider extensions supported on periodic configurations, which are analyzed using de~Bruijn graphs and which include the extensions with minimal entropy. When $Λ\subset\mathbb{Z}$ is not an interval, or when $Λ\subset\mathbb{Z}^d$ with $d>1$, the LTI condition is necessary but not sufficient for extendibility. For $\mathbb{Z}^d$ with $d>1$, extendibility is in some sense undecidable.

cond-mat.stat-mech↗

arXiv2015

The Truncated Moment Problem on $\mathbb{N}_0$

We find necessary and sufficient conditions for the existence of a probability measure on $\mathbb{N}_0$, the nonnegative integers, whose first $n$ moments are a given $n$-tuple of nonnegative real numbers. The results, based on finding an optimal polynomial of degree $n$ which is nonnegative on $\mathbb{N}_0$ (and which depends on the moments), and requiring that its expectation be nonnegative, generalize previous results known for $n=1$, $n=2$ (the Percus-Yamada condition), and partially for $n=3$. The conditions for realizability are given explicitly for $n\leq5$ and in a finitely computable form for $n\geq6$. We also find, for all $n$, explicit bounds, in terms of the moments, whose satisfaction is enough to guarantee realizability. Analogous results are given for the truncated moment problem on an infinite discrete semi-bounded subset of $\mathbb{R}$.

math.PR↗

arXiv2015

Central limit theorems, Lee-Yang zeros, and graph-counting polynomials

We consider the asymptotic normalcy of families of random variables $X$ which count the number of occupied sites in some large set. We write $Prob(X=m)=p_mz_0^m/P(z_0)$, where $P(z)$ is the generating function $P(z)=\sum_{j=0}^{N}p_jz^j$ and $z_0>0$. We give sufficient criteria, involving the location of the zeros of $P(z)$, for these families to satisfy a central limit theorem (CLT) and even a local CLT (LCLT); the theorems hold in the sense of estimates valid for large $N$ (we assume that $Var(X)$ is large when $N$ is). For example, if all the zeros lie in the closed left half plane then $X$ is asymptotically normal, and when the zeros satisfy some additional conditions then $X$ satisfies an LCLT. We apply these results to cases in which $X$ counts the number of edges in the (random) set of "occupied" edges in a graph, with constraints on the number of occupied edges attached to a given vertex. Our results also apply to systems of interacting particles, with $X$ counting the number of particles in a box $Λ$ whose size approaches infinity; $P(z)$ is then the grand canonical partition function and its zeros are the Lee-Yang zeros.

math.CO↗

arXiv2014

KPZ universality class and the anchored Toom interface

We revisit the anchored Toom interface and use KPZ scaling theory to argue that the interface fluctuations are governed by the Airy_1 process with the role of space and time interchanged. There is no free parameter. The predictions are numerically well confirmed for space-time statistics in the stationary state. In particular the spatial fluctuations of the interface are given by the GOE edge distribution of Tracy and Widom.

math-ph↗

arXiv2013

Time evolution of electron flow in a model diode: Non-perturbative analysis

Using a combination of Eulerian and Lagrangian variables we obtain some exact results and good approximation schemes for the time evolution of the electron flow from a no-current state to a final stationary current state in a planar one-dimensional diode. The electrons can be injected externally or generated by the cathode via field emission governed by a current-field law. The case of equipotential electrodes and fixed injection is studied along with a positive anode potential. When the current is fixed externally the approach to the stationary state goes without oscillations if the initial electron velocity is high enough and the anode can absorb the injected flow. Otherwise the accumulated space charge creates a potential barrier which reflects the flow and leads to its oscillations, but our method of analysis is invalid in such conditions. In the field emission case the flow goes to its stationary state through a train of decaying oscillations whose period is of the order of the electron transit time, in agreement with earlier studies based on perturbation techniques. Our approximate method does not permit very high cathode emissivity, though the method works when the stationary current density is only about 10% smaller than the Child-Langmuir limit.

physics.plasm-ph↗

arXiv2013

Propagation of Chaos for a Thermostated Kinetic Model

We consider a system of N point particles moving on a d-dimensional torus. Each particle is subject to a uniform field E and random speed conserving collisions. This model is a variant of the Drude-Lorentz model of electrical conduction. In order to avoid heating by the external field, the particles also interact with a Gaussian thermostat which keeps the total kinetic energy of the system constant. The thermostat induces a mean-field type of interaction between the particles. Here we prove that, starting from a product measure, in the large N limit, the one particle velocity distribution satisfies a self consistent Vlasov-Boltzmann equation.. This is a consequence of "propagation of chaos", which we also prove for this model.

math-ph↗

arXiv2013

Lyapunov functionals for boundary-driven nonlinear drift-diffusions

We exhibit a large class of Lyapunov functionals for nonlinear drift-diffusion equations with non-homogeneous Dirichlet boundary conditions. These are generalizations of large deviation functionals for underlying stochastic many-particle systems, the zero range process and the Ginzburg-Landau dynamics, which we describe briefly. As an application, we prove linear inequalities between such an entropy-like functional and its entropy production functional for the boundary-driven porous medium equation in a bounded domain with positive Dirichlet conditions: this implies exponential rates of relaxation related to the first Dirichlet eigenvalue of the domain. We also derive Lyapunov functions for systems of nonlinear diffusion equations, and for nonlinear Markov processes with non-reversible stationary measures.

math.AP↗

arXiv2012

The blockage problem

We investigate the totally asymmetric exclusion process on Z, with the jump rate at site i given by r_i=1 for i nonzero, r_0=r. It is easy to see that the maximal stationary current j(r) is nondecreasing in r and that j(r)=1/4 for r>=1; it is a long outstanding problem to determine whether or not the critical value r_c of r such that j(r)=1/4 for r>r_c is strictly less than 1. Here we present a heuristic argument, based on the analysis of the first sixteen terms in a formal power series expansion of j(r) obtained from finite volume systems, that r_c=1 and that for r less than 1 and near 1, j(r) behaves as 1/4-γ\exp[-{a/(1-r)}] with a approximately equal to 2. We also give some new exact results about this system; in particular we prove that j(r)=J_max(r), with J_max(r) the hydrodynamic maximal current defined by Seppalainen, and thus establish continuity of j(r). Finally we describe a related exactly solvable model, a semi-infinite system in which the site i=0 is always occupied. For that system, the critical r is 1/2 and the analogue j_s(r) of j(r) satisfies j_s(r)=r(1-r) for r<=1/2; j_s(r) is the limit of finite volume currents inside the curve |r(1-r)|=1/4 in the complex r plane and we suggest that analogous behavior may hold for the original system.

math-ph↗

arXiv2012

Non-equilibrium stationary state of a harmonic crystal with alternating masses

We analyze the non-equilibrium steady states (NESS) of a one dimensional harmonic chain of $N$ atoms with alternating masses connected to heat reservoirs at unequal temperatures. We find that the temperature profile defined through the local kinetic energy $T(j) \equiv { }/{m_j}$, oscillates with period two in the bulk of the system. Depending on boundary conditions, either the heavier or the lighter particles in the bulk are hotter. We obtain exact expressions for the bulk temperature profile and steady state current in the limit $N \rightarrow \infty$. These depend on whether $N$ is odd or even. We also study similar temperature oscillations in the NESS of systems with noise in the dynamics. These die out as $N \rightarrow \infty$.

math-ph↗

arXiv2012

Approach to equilibrium for the stochastic NLS

We study the approach to equilibrium, described by a Gibbs measure, for a system on a $d$-dimensional torus evolving according to a stochastic nonlinear Schrödinger equation (SNLS) with a high frequency truncation. We prove exponential approach to the truncated Gibbs measure both for the focusing and defocusing cases when the dynamics is constrained via suitable boundary conditions to regions of the Fourier space where the Hamiltonian is convex. Our method is based on establishing a spectral gap for the non self-adjoint Fokker-Planck operator governing the time evolution of the measure, which is {\it uniform} in the frequency truncation $N$. The limit $N\to\infty$ is discussed.

math-ph↗

arXiv2011

Analysis of Droplets in Lattice Systems with Long-range Kac Potentials

We investigate the geometry of typical equilibrium configurations for a lattice gas in a finite macroscopic domain with attractive, long range Kac potentials. We focus on the case when the system is below the critical temperature and has a fixed number of occupied sites.We connect the properties of typical configurations to the analysis of the constrained minimizers of a mesoscopic non-local free energy functional, which we prove to be the large deviation functional for a density profile in the canonical Gibbs measure with prescribed global density. In the case in which the global density of occupied sites lies between the two equilibrium densities that one would have without a constraint on the particle number, a "droplet" of the high (low) density phase may or may not form in a background of the low (high) density phase. We determine the critical density for droplet formation, and the nature of the droplet, as a function of the temperature and the size of the system, by combining the present large deviation principle with the analysis of the mesoscopic functional given in CCELM

cond-mat.stat-mech↗