0000000000061438

AUTHOR

Ihor Lubashevsky

showing 13 related works from this author

Noise-Induced Phase Transitions

2009

PhysicsPhase transitionGeometric Brownian motionNoise inducedStochastic processFokker–Planck equationStatistical physicsBrownian motion
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Stochastic description of traffic breakdown

2003

We present a comparison of nucleation in an isothermal-isochoric container with traffic congestion on a one-lane freeway. The analysis is based, in both cases, on the probabilistic description by stochastic master equations. Further we analyze the characteristic features of traffic breakdowns. To describe this phenomenon we apply the stochastic model regarding the jam emergence to the formation of a large car cluster on the highway.

Physics::Physics and SocietyMathematical optimizationEngineeringTraffic congestion reconstruction with Kerner's three-phase theoryStochastic modellingbusiness.industryTraffic flowTraffic congestionMaster equationContainer (abstract data type)Three-phase traffic theorybusinessTraffic generation modelSimulationSPIE Proceedings
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The Master Equation

2009

Continuous-time stochastic processsymbols.namesakeStochastic differential equationQuantum stochastic calculusStochastic processMaster equationKinetic schemesymbolsStatistical physicsChapman–Kolmogorov equationMathematics
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The Langevin Equation

2009

PhysicsLangevin equationStochastic differential equationGeometric Brownian motionClassical mechanicsQuantum stochastic calculusDiffusion processBrownian dynamicsFokker–Planck equationBrownian motion
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Nucleation in Supersaturated Vapors

2009

SupersaturationNucleationThermodynamics
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Probabilistic description of traffic flow

2005

Abstract A stochastic description of traffic flow, called probabilistic traffic flow theory, is developed. The general master equation is applied to relatively simple models to describe the formation and dissolution of traffic congestions. Our approach is mainly based on spatially homogeneous systems like periodically closed circular rings without on- and off-ramps. We consider a stochastic one-step process of growth or shrinkage of a car cluster (jam). As generalization we discuss the coexistence of several car clusters of different sizes. The basic problem is to find a physically motivated ansatz for the transition rates of the attachment and detachment of individual cars to a car cluster…

PhysicsMicroscopic traffic flow modelStochastic cellular automatonStochastic processMaster equationPhysical systemGeneral Physics and AstronomyThree-phase traffic theoryStatistical physicsTraffic flowFundamental diagram of traffic flowPhysics Reports
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One-Dimensional Diffusion

2009

PhysicsHeterogeneous random walk in one dimensionOne dimensional diffusionAnomalous diffusionStochastic processStatistical physicsDiffusion (business)Random walk
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Probabilistic description of traffic breakdowns

2001

We analyze the characteristic features of traffic breakdown. To describe this phenomenon we apply to the probabilistic model regarding the jam emergence as the formation of a large car cluster on highway. In these terms the breakdown occurs through the formation of a certain critical nucleus in the metastable vehicle flow, which enables us to confine ourselves to one cluster model. We assume that, first, the growth of the car cluster is governed by attachment of cars to the cluster whose rate is mainly determined by the mean headway distance between the car in the vehicle flow and, may be, also by the headway distance in the cluster. Second, the cluster dissolution is determined by the car …

PhysicsStatistical Mechanics (cond-mat.stat-mech)Stochastic processFOS: Physical sciencesCondensed Matter - Soft Condensed MatterTraffic flowMaster equationHeadwayCluster (physics)Soft Condensed Matter (cond-mat.soft)ClimbFokker–Planck equationStatistical physicsCondensed Matter - Statistical MechanicsWeibull distributionPhysical Review E
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The Ornstein-Uhlenbeck Process

2009

PhysicsEconophysicsStochastic processOrnstein–Uhlenbeck processStatistical physics
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Stochastic approach to highway traffic

2004

We analyze the characteristic features of jam formation on a circular one-lane road. We have applied an optimal velocity model including stochastic noise, where cars are treated as moving and interacting particles. The motion of N cars is described by the system of 2 N stochastic differential equations with multiplicative white noise. Our system of cars behaves in qualitatively different ways depending on the values of control parameters c (dimensionless density), b (sensitivity parameter characterising the fastness of relaxation), and α (dimensionless noise intensity). In analogy to the gas-liquid phase transition in supersaturated vapour at low enough temperatures, we observe three differ…

Langevin equationPhase transitionStochastic differential equationCritical phenomenaThermodynamicsStatistical physicsCritical exponentNoise (electronics)Multiplicative noiseDimensionless quantityMathematicsSPIE Proceedings
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Many-Particle Systems

2009

PhysicsParticle systemStochastic processStatistical physics
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Bounded Drift-Diffusion Motion

2009

Stochastic processBounded functionMathematical analysisMotion (geometry)Sturm–Liouville theoryDiffusion (business)Liouville field theoryMathematics
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The Fokker-Planck Equation

2009

PhysicsStochastic differential equationSystem size expansionStochastic processFokker–Planck equationStatistical physics
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