Search results for "AOS"

showing 10 items of 330 documents

Active Brownian Motion Models and Applications to Ratchets

2008

We give an overview over recent studies on the model of Active Brownian Motion (ABM) coupled to reservoirs providing free energy which may be converted into kinetic energy of motion. First, we present an introduction to a general concept of active Brownian particles which are capable to take up energy from the source and transform part of it in order to perform various activities. In the second part of our presentation we consider applications of ABM to ratchet systems with different forms of differentiable potentials. Both analytical and numerical evaluations are discussed for three cases of sinusoidal, staircase-like and Mateos ratchet potentials, also with the additional loads modeled by…

PhysicsStatistical Mechanics (cond-mat.stat-mech)RatchetPerturbation (astronomy)FOS: Physical sciencesFluctuation phenomena random processes noise Brownian motion Nonlinear dynamics and chaosWhite noiseCondensed Matter - Soft Condensed MatterCondensed Matter PhysicsKinetic energyElectronic Optical and Magnetic MaterialsClassical mechanicsPhysics - Data Analysis Statistics and ProbabilityMolecular motorDirectionalitySoft Condensed Matter (cond-mat.soft)Differentiable functionBrownian motionData Analysis Statistics and Probability (physics.data-an)Condensed Matter - Statistical Mechanics
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Nonlinearity and Disorder in the Statistical Mechanics of Integrable Systems

1992

Attention is drawn to a theory of the statistical mechanics (SM) of the integrable models in 1+1 dimension — a theory of ‘soliton statistical mechanics’ classical and quantum [1–17]. This SM provides a generic example of integrable nonlinearity interacting with disorder. In the generic classical examples, such as the classical SM of the sine-Gordon model, phonons provide disorder in which sit coherent structures — the kink-like solitons. But these solitons are dressed by the disorder, in equilibrium, while the breather-like solitons break up to form the disordered structures which are the phonons in thermal equilibrium. On the other hand quantum solitons, dressed by both the vacuum and fini…

PhysicsThermal equilibriumNonlinear Sciences::Exactly Solvable and Integrable SystemsIntegrable systemPhononBreatherQuantum mechanicsSolitonStatistical mechanicsNonlinear Sciences::Pattern Formation and SolitonsQuantumQuantum chaosMathematical physics
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Modelling of Boltzmann transport equation for freeze-out

2005

The freeze-out (FO) in high-energy heavy-ion collisions is assumed to be continuous across finite layer in space–time. Particles leaving local thermal equilibrium start to freeze out gradually till they leave the layer, where all the particles are frozen out. To describe such a kinetic process we start from Boltzmann transport equation (BTE). However, we will show that the basic assumptions of BTE, such as molecular chaos or spatial homogeneity do not hold for the above-mentioned FO process. The aim of the presented work is to analyse the situation, discuss the modification of BTE and point out the physical causes, which yield to these modifications of BTE for describing FO.

PhysicsThermal equilibriumNuclear and High Energy PhysicsWork (thermodynamics)Yield (engineering)Molecular chaosStatistical physicsSpatial homogeneityPhysics::Classical PhysicsKinetic energyBoltzmann equationJournal of Physics G: Nuclear and Particle Physics
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Intrinsic quantum chaos and spectral fluctuations within the protactinium atom

2018

Physicschemistry0103 physical sciencesProtactiniumchemistry.chemical_elementAtom (order theory)Atomic physics010306 general physics01 natural sciencesQuantum chaos010305 fluids & plasmasPhysical Review A
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Lorenz–Haken instability in a laser with arbitrary mirrors reflectivity

2000

Abstract We study the Lorenz–Haken instability in a laser with arbitrary mirrors reflectivity R . In the limit of slow population difference we demonstrate that in order to observe the instability the reflectivity must exceed the critical value R c ≃0.5379, which coincides with that found recently for the multimode (Risken–Nummedal–Graham–Haken) instability. Several other differences with respect to the uniform field limit R →1 are presented.

Physicseducation.field_of_studyMulti-mode optical fiberbusiness.industryPopulationLaserCritical valueOptical chaosInstabilityReflectivityAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic Materialslaw.inventionOpticslawLimit (mathematics)Electrical and Electronic EngineeringPhysical and Theoretical ChemistrybusinesseducationOptics Communications
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Stability and Chaotic Attractors of Memristor-Based Circuit with a Line of Equilibria

2019

This report investigates the stability problem of memristive systems with a line of equilibria on the example of SBT memristor-based Wien-bridge circuit. For the considered system, conditions of local and global partial stability are obtained, and chaotic dynamics is studied. peerReviewed

Physicskaaosteoriaelektroniset piiritChaoticpartial stabilitymemristoritMemristorTopologyStability (probability)Line (electrical engineering)law.inventionComputer Science::Emerging Technologieshidden attractorsPartial stabilitylawAttractorkaaosmatemaattiset mallitmemristor
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Exact results for the homogeneous cooling state of an inelastic hard-sphere gas

1998

The infinite set of moments of the two-particle distribution function is found exactly for the uniform cooling state of a hard-sphere gas with inelastic collisions. Their form shows that velocity correlations cannot be neglected, and consequently the 'molecular chaos' hypothesis leading to the inelastic Boltzmann and Enskog kinetic equations must be questioned. © 1998 Cambridge University Press.

Physicssymbols.namesakeInfinite setClassical mechanicsDistribution functionBoltzmann constantsymbolsInelastic collisionMolecular chaosHard spheresInelastic scatteringCondensed Matter PhysicsBoltzmann equationJournal of Plasma Physics
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Condensation and thermalization of classsical optical waves in a waveguide

2011

http://pra.aps.org/; International audience; We consider the long-term evolution of a random nonlinear wave that propagates in a multimode optical waveguide. The optical wave exhibits a thermalization process characterized by an irreversible evolution toward an equilibrium state. The tails of the equilibrium distribution satisfy the property of energy equipartition among the modes of the waveguide. As a consequence of this thermalization, the optical field undergoes a process of classical wave condensation, which is characterized by a macroscopic occupation of the fundamental mode of the waveguide. Considering the nonlinear Schrödinger equation with a confining potential, we formulate a wav…

Physics::OpticsOptical field01 natural sciencesWaveguide (optics)Electromagnetic radiationoptical instabilitiesSchrödinger equation010309 opticssymbols.namesakeand lossesQuantum mechanics0103 physical sciencesDynamics of nonlinear optical systemssolitons010306 general physicsPropagationGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)ComputingMilieux_MISCELLANEOUSUltraviolet catastrophePhysics[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]and optical spatio-temporal dynamicsscatteringComputerSystemsOrganization_COMPUTER-COMMUNICATIONNETWORKSWave equationAtomic and Molecular Physics and Optics[MATH.MATH-PR]Mathematics [math]/Probability [math.PR]ThermalisationCross-polarized wave generationsymbolsoptical chaos and complexityMathematicsofComputing_DISCRETEMATHEMATICS
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Texture Discrimination Using Hierarchical Complex Networks

2008

Texture analysis represents one of the main areas in image processing and computer vision. The current article describes how complex networks have been used in order to represent and characterized textures. More speci?cally, networks are derived from the texture images by expressing pixels as network nodes and similarities between pixels as network edges. Then, measurements such as the node degree, strengths and clustering coe?cient are used in order to quantify properties of the connectivity and topology of the analyzed networks. Because such properties are directly related to the structure of the respective texture images, they can be used as features for characterizing and classifying te…

Pixelbusiness.industryComputer scienceNode (networking)ComputingMethodologies_IMAGEPROCESSINGANDCOMPUTERVISIONChaos gamePattern recognitionImage processingComplex networkTexture (geology)Computer Science::Computer Vision and Pattern RecognitionArtificial intelligenceCluster analysisbusinessTopology (chemistry)
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Une relation trophique originale : la vection entomophile d'agents pathogènes

2013

Bgpi : équipe 6 chapitre 34; Une relation trophique originale : la vection entomophile d'agents pathogènes

Plante hôteInsectahttp://aims.fao.org/aos/agrovoc/c_2615[SDV]Life Sciences [q-bio]Relation plante animalVertèbreÉvolutionRelation hôte pathogènehttp://aims.fao.org/aos/agrovoc/c_26802virusAgent pathogènePhytoplasmehttp://aims.fao.org/aos/agrovoc/c_5985http://aims.fao.org/aos/agrovoc/c_34142[SDV.BV]Life Sciences [q-bio]/Vegetal Biologyhttp://aims.fao.org/aos/agrovoc/c_8196[SDV.BV] Life Sciences [q-bio]/Vegetal Biologypathologie végétaleTransmission des maladieshttp://aims.fao.org/aos/agrovoc/c_11621ComputingMilieux_MISCELLANEOUSH20 - Maladies des planteshttp://aims.fao.org/aos/agrovoc/c_2329Contrôle de maladieshttp://aims.fao.org/aos/agrovoc/c_2745http://aims.fao.org/aos/agrovoc/c_2327Virus des végétauxH10 - Ravageurs des plantesMaladie transmise par vecteur[SDV] Life Sciences [q-bio]Épidémiologiehttp://aims.fao.org/aos/agrovoc/c_5630http://aims.fao.org/aos/agrovoc/c_3890Vecteur de maladieEntomologiemaladie viraleSciences du vivanthttp://aims.fao.org/aos/agrovoc/c_8164http://aims.fao.org/aos/agrovoc/c_34017http://aims.fao.org/aos/agrovoc/c_2588http://aims.fao.org/aos/agrovoc/c_32513Biologie végétale
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