Search results for "37"

showing 10 items of 1060 documents

Rotation Forms and Local Hamiltonian Monodromy

2017

International audience; The monodromy of torus bundles associated with completely integrable systems can be computed using geometric techniques (constructing homology cycles) or analytic arguments (computing discontinuities of abelian integrals). In this article, we give a general approach to the computation of monodromy that resembles the analytical one, reducing the problem to the computation of residues of polar 1-forms. We apply our technique to three celebrated examples of systems with monodromy (the champagne bottle, the spherical pendulum, the hydrogen atom) and to the case of non-degenerate focus-focus singularities, re-obtaining the classical results. An advantage of this approach …

[ MATH ] Mathematics [math]Pure mathematicsIntegrable systemFOCUS-FOCUS SINGULARITIESmath-phFOS: Physical sciencesDynamical Systems (math.DS)Homology (mathematics)01 natural sciencesSingularityMathematics::Algebraic Geometrymath.MPSYSTEMS0103 physical sciencesFOS: Mathematics0101 mathematicsAbelian groupMathematics - Dynamical Systems[MATH]Mathematics [math]010306 general physicsMathematics::Symplectic GeometryMathematical PhysicsMathematicsNEIGHBORHOODS[PHYS]Physics [physics][ PHYS ] Physics [physics]010102 general mathematicsSpherical pendulumStatistical and Nonlinear PhysicsTorusMathematical Physics (math-ph)37JxxMonodromyStatistical and Nonlinear Physics; Mathematical PhysicsGravitational singularityPOINTSmath.DS
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A Franks' lemma that preserves invariant manifolds

2009

A well-known lemma by John Franks asserts that one obtains any perturbation of the derivative of a diffeomorphism along a periodic orbit by a $C^1$-perturbation of the whole diffeomorphism on a small neighbourhood of the orbit. However, one does not control where the invariant manifolds of the orbit are, after perturbation. We show that if the perturbated derivative is obtained by an isotopy along which some strong stable/unstable manifolds of some dimensions exist, then the Franks perturbation can be done preserving the corresponding stable/unstable semi-local manifolds. This is a general perturbative tool in $C^1$-dynamics that has many consequences. We give simple examples of such conseq…

[ MATH.MATH-DS ] Mathematics [math]/Dynamical Systems [math.DS][MATH.MATH-DS]Mathematics [math]/Dynamical Systems [math.DS]FOS: Mathematics37C25 37C29 37C20 37D10[MATH.MATH-DS] Mathematics [math]/Dynamical Systems [math.DS]Dynamical Systems (math.DS)Mathematics - Dynamical Systems
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Ping-pong configurations and circular orders on free groups

2017

We discuss actions of free groups on the circle with "ping-pong" dynamics; these are dynamics determined by a finite amount of combinatorial data, analogous to Schottky domains or Markov partitions. Using this, we show that the free group $F_n$ admits an isolated circular order if and only if n is even, in stark contrast with the case for linear orders. This answers a question from (Mann, Rivas, 2016). Inspired by work of Alvarez, Barrientos, Filimonov, Kleptsyn, Malicet, Menino and Triestino, we also exhibit examples of "exotic" isolated points in the space of all circular orders on $F_2$. Analogous results are obtained for linear orders on the groups $F_n \times \mathbb{Z}$.

[ MATH.MATH-GR ] Mathematics [math]/Group Theory [math.GR][ MATH.MATH-DS ] Mathematics [math]/Dynamical Systems [math.DS][MATH.MATH-DS]Mathematics [math]/Dynamical Systems [math.DS]MSC2010: Primary 20F60 57M60. Secondary 20E05 37C85 37E05 37E10 57M60.Extension (predicate logic)Group Theory (math.GR)Dynamical Systems (math.DS)Space (mathematics)20F60 57M60[MATH.MATH-GR]Mathematics [math]/Group Theory [math.GR]CombinatoricsFree groupsOne-dimensional dynamicsFree groupPing pongFOS: MathematicsDiscrete Mathematics and CombinatoricsOrder (group theory)Geometry and TopologyMathematics - Dynamical SystemsMathematics - Group TheoryMathematicsOrders on groups
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Fractal Weyl law for open quantum chaotic maps

2014

We study the semiclassical quantization of Poincar\'e maps arising in scattering problems with fractal hyperbolic trapped sets. The main application is the proof of a fractal Weyl upper bound for the number of resonances/scattering poles in small domains near the real axis. This result encompasses the case of several convex (hard) obstacles satisfying a no-eclipse condition.

[ NLIN.NLIN-CD ] Nonlinear Sciences [physics]/Chaotic Dynamics [nlin.CD][PHYS.MPHY]Physics [physics]/Mathematical Physics [math-ph]FOS: Physical sciencesSemiclassical physicsDynamical Systems (math.DS)35B34 37D20 81Q50 81U05Upper and lower boundsMSC: 35B34 37D20 81Q50 81U05Fractal Weyl lawQuantization (physics)Mathematics - Analysis of PDEs[ MATH.MATH-AP ] Mathematics [math]/Analysis of PDEs [math.AP]Mathematics (miscellaneous)Fractal[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]FOS: Mathematics[MATH.MATH-AP]Mathematics [math]/Analysis of PDEs [math.AP]Mathematics - Dynamical SystemsQuantumMathematical physicsMathematicsScattering[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]Nonlinear Sciences - Chaotic DynamicsWeyl lawResonancesQuantum chaotic scattering[NLIN.NLIN-CD]Nonlinear Sciences [physics]/Chaotic Dynamics [nlin.CD][ PHYS.MPHY ] Physics [physics]/Mathematical Physics [math-ph]Chaotic Dynamics (nlin.CD)Statistics Probability and UncertaintyOpen quantum mapComplex planeAnalysis of PDEs (math.AP)Annals of Mathematics
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Observation of laser-induced field-free permanent planar alignment of molecules

2011

International audience; Permanent planar alignment of gas-phase linear molecules is achieved by a pair of delayed perpendicularly polarized short laser pulses. The experiment is performed in a supersonic jet, ensuring a relatively high number density of molecules with moderately low rotational temperature. The effect is optically probed on a femtosecond time scale by the use of a third short pulse, enabling a time-resolved birefringence detection performed successively in two perpendicular planes of the laboratory frame. The technique allows for an unambiguous estimation of the molecular planar delocalization produced within the polarization plane of the pulse pair after the turn-off of the…

[ PHYS.PHYS.PHYS-ATOM-PH ] Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]Linear molecular geometry01 natural sciencesMolecular physicslaw.invention010309 opticsRotational dynamicsPlanarOpticslaw0103 physical sciencesUltrafast nonlinear optics010306 general physicsOptical Kerr effectPhysicsNumber densityBirefringence[PHYS.PHYS.PHYS-ATOM-PH]Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]Molecular alignmentbusiness.industryFemtosecond phenomenaRotational temperature3710Vz 4250Hz 4250MdLaserPolarization (waves)Atomic and Molecular Physics and OpticsOptical polarigraphyFemtosecondbusiness
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An attempt to classification of the quasi rational solutions to the NLS equation

2015

Based on a representation in terms of determinants of order 2N , an attempt to classification of quasi rational solutions to the one dimensional focusing nonlinear Schrödinger equation (NLS) is given and several conjectures about the structure of the solutions are also formulated. These solutions can be written as a product of an exponential depending on t by a quotient of two polynomials of degree N (N + 1) in x and t depending on 2N −2 parameters. It is remarkable to mention that in this representation, when all parameters are equal to 0, we recover the PN breathers.

[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph][ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph][MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]37K10 33Q55 4710A- 4735Fg 4754Bd
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N-order rational solutions to the Johnson equation depending on 2N - 2 parameter

2017

International audience; We construct rational solutions of order N depending on 2N-2 parameters. They can be written as a quotient of 2 polynomials of degree 2N(N+1) in x, t and 2N(N+1) in y depending on 2N-2 parameters. We explicitly construct the expressions of the rational solutions of order 4 depending on 6 real parameters and we study the patterns of their modulus in the plane (x,y) and their evolution according to time and parameters a1,a2,a3,b1,b2,b3.

[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph][ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph][MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]PACS numbers : 33Q55 37K10 47.10A- 47.35.Fg 47.54.Bd
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Multi-parametric families solutions to the Burgers equation

2021

We construct 2N real parameter solutions to the Burgers' equation in terms of determinant of order N and we call these solutions, N order solutions. We deduce general expressions of these solutions in terms of exponentials and study the patterns of these solutions in functions of the parameters for N = 1 until N = 4.

[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph][MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]PACS numbers : 33Q55 37K10 47.10A- 47.35.Fg 47.54.BdBurgers equation
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Higher-order Kerr terms allow ionization-free filamentation in gases

2010

International audience; We show that higher-order nonlinear indices (n4 , n6 , n8 , n10) provide the main defocusing contribution to self-channeling of ultrashort laser pulses in air and Argon at 800 nm, in contrast with the previously accepted mechanism of filamentation where plasma was considered as the dominant defocusing process. Their consideration allows to reproduce experimentally observed intensities and plasma densities in self-guided filaments.

[PHYS.PHYS.PHYS-ATOM-PH]Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]Molecular alignmentPhysics::Plasma PhysicsFemtosecond phenomenaPlasmasSelf-focusing[ PHYS.PHYS.PHYS-ATOM-PH ] Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]Physics::Optics42.65.Jx 37.10.Vz 42.65.Tg 78.20.CiUltrafast nonlinear optics[PHYS.PHYS.PHYS-ATOM-PH] Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]Optical Kerr effectLaser filamentation
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Evaluation agroécologique de systèmes de culture en zone tropicale humide : Cas de la mise en valeur agricole d'une savane herbacée acide (Plaine des…

2013

Dans les régions tropicales humides, concilier intensification agricole et protection des ressources naturelles est un défi majeur et difficile à relever. Dans les savanes acides du nord-est laotien, des systèmes de culture de semis direct sur couverture végétale (SCV), basés sur les trois principes du non-labour, d’une couverture permanente du sol, et sur la pratique de rotations culturales diversifiées, sont proposés comme alternative technique à l’intensification agricole conventionnelle basée sur le labour. Si ces systèmes ont connu une diffusion importante et rapide dans les grandes agricultures mécanisées, leur diffusion reste néanmoins à ce jour limitée en contexte de petite agricult…

[SDE] Environmental SciencesH01 - Protection des végétaux - Considérations généralesSemis directhttp://aims.fao.org/aos/agrovoc/c_28568http://aims.fao.org/aos/agrovoc/c_28766solF08 - Systèmes et modes de culturesavane tropicale acideagroécologieBiologie du solhttp://aims.fao.org/aos/agrovoc/c_7193Performance de cultureNon-travail du sol[SDV.BV] Life Sciences [q-bio]/Vegetal Biologyhttp://aims.fao.org/aos/agrovoc/c_2018Savanehttp://aims.fao.org/aos/agrovoc/c_8511http://aims.fao.org/aos/agrovoc/c_3145http://aims.fao.org/aos/agrovoc/c_35657Petite agricultureévaluation agroécologiquehttp://aims.fao.org/aos/agrovoc/c_7182Sol acidehttp://aims.fao.org/aos/agrovoc/c_25803http://aims.fao.org/aos/agrovoc/c_1919http://aims.fao.org/aos/agrovoc/c_765http://aims.fao.org/aos/agrovoc/c_92381[SDV] Life Sciences [q-bio]Pratique culturaleLaosagriculture de conservationhttp://aims.fao.org/aos/agrovoc/c_7979Micro-organisme du solhttp://aims.fao.org/aos/agrovoc/c_89Zone tropicaleP33 - Chimie et physique du solÉcologieExploitation agricole familialehttp://aims.fao.org/aos/agrovoc/c_37938Spectroscopie infrarougeChampignonAnalyse coût avantageCulture sous couvert végétalMatière organique du solhttp://aims.fao.org/aos/agrovoc/c_36167http://aims.fao.org/aos/agrovoc/c_4176http://aims.fao.org/aos/agrovoc/c_12076http://aims.fao.org/aos/agrovoc/c_35199Propriété physicochimique du solécologie microbienneBacteriaProductivité des terressemis direct sur couverture végétaleP35 - Fertilité du solÉvaluation de l'impacthttp://aims.fao.org/aos/agrovoc/c_7160P34 - Biologie du solE80 - Économie familiale et artisanaleAnalyse économiqueTaxonomiehttp://aims.fao.org/aos/agrovoc/c_25706structure agrairehttp://aims.fao.org/aos/agrovoc/c_6825http://aims.fao.org/aos/agrovoc/c_2787Système de culturehttp://aims.fao.org/aos/agrovoc/c_2469http://aims.fao.org/aos/agrovoc/c_1971http://aims.fao.org/aos/agrovoc/c_17299U30 - Méthodes de recherchePlante de culturehttp://aims.fao.org/aos/agrovoc/c_2467http://aims.fao.org/aos/agrovoc/c_1972Cycle du carbonehttp://aims.fao.org/aos/agrovoc/c_7631
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