Search results for "Integrable system"

showing 10 items of 354 documents

Highlights of top quark cross-section measurements at ATLAS

2017

The highlights of the measurements of top quark production in proton-proton collisions at the Large Hadron Collider with the ATLAS detector are presented. The inclusive measurements of the top-pair production cross section have reached high precision and are compared to the best available theoretical calculations. The differential cross section measurements, including results using boosted top quarks, probe our understanding of top-pair production in the TeV regime. The results are compared to Monte Carlo generators implementing LO and NLO matrix elements matched with parton showers. Measurements of the single top quark production cross section are presented in the t -channel and s -channel…

QuarkPhysicsTop quarkParticle physicsLarge Hadron Collider010308 nuclear & particles physicsPhysicsQC1-999Monte Carlo methodHigh Energy Physics::PhenomenologyParton7. Clean energy01 natural sciencesNuclear physicsCross section (physics)Matrix (mathematics)medicine.anatomical_structureNonlinear Sciences::Exactly Solvable and Integrable SystemsAtlas (anatomy)0103 physical sciencesmedicinePhysics::Atomic and Molecular ClustersHigh Energy Physics::Experiment010306 general physicsParticle Physics - ExperimentEPJ Web of Conferences
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Search for Direct Top Squark Pair Production in Final States with One Isolated Lepton, Jets, and Missing Transverse Momentum ins=7  TeVppCollisions U…

2012

A search is presented for direct top squark pair production in final states with one isolated electron or muon, jets, and missing transverse momentum in proton-proton collisions at root s = 7 TeV. The measurement is based on 4.7 fb(-1) of data collected with the ATLAS detector at the LHC. Each top squark is assumed to decay to a top quark and the lightest supersymmetric particle (LSP). The data are found to be consistent with standard model expectations. Top squark masses between 230 GeV and 440 GeV are excluded with 95% confidence for massless LSPs, and top squark masses around 400 GeV are excluded for LSP masses up to 125 GeV.

QuarkPhysicsTop quarkParticle physicsStop squarkLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyGeneral Physics and Astronomy01 natural sciences7. Clean energyLightest Supersymmetric ParticleNuclear physicsNonlinear Sciences::Exactly Solvable and Integrable SystemsPionPair production0103 physical sciencesPhysics::Atomic and Molecular ClustersHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsMinimal Supersymmetric Standard ModelPhysical Review Letters
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L p-Spaces and the Radon–Nikodym Theorem

2020

In this chapter, we study the spaces of functions whose pth power is integrable. In Section 7.2, we first derive some of the important inequalities (Holder, Minkowski, Jensen) and then in Section 7.3 investigate the case p=2 in more detail.

Radon–Nikodym theoremSection (fiber bundle)symbols.namesakePure mathematicsIntegrable systemMinkowski spaceHilbert spacesymbolsMathematicsNormed vector space
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AKNS and NLS hierarchies, MRW solutions, $P_n$ breathers, and beyond

2018

We describe a unified structure of rogue wave and multiple rogue wave solutions for all equations of the Ablowitz-Kaup-Newell-Segur (AKNS) hierarchy and their mixed and deformed versions. The definition of the AKNS hierarchy and its deformed versions is given in the Sec. II. We also consider the continuous symmetries of the related equations and the related spectral curves. This work continues and summarises some of our previous studies dedicated to the rogue wave-like solutions associated with AKNS, nonlinear Schrodinger, and KP hierarchies. The general scheme is illustrated by the examples of small rank n, n ⩽ 7, rational or quasi-rational solutions. In particular, we consider rank-2 and …

Rank (linear algebra)BreatherStructure (category theory)Statistical and Nonlinear PhysicsWave equation01 natural sciences010305 fluids & plasmasNonlinear systemsymbols.namesakeNonlinear Sciences::Exactly Solvable and Integrable Systems[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]0103 physical sciencesHomogeneous spacesymbolsRogue wave010306 general physicsNonlinear Sciences::Pattern Formation and SolitonsMathematical PhysicsSchrödinger's catMathematicsMathematical physics
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Remarks on Infinite-Dimensional Representations of the Heisenberg Algebra

2017

Infinite-dimensional representations of Lie algebras necessarily invoke the theory of unbounded operator algebras. Starting with the familiar example of the Heisenberg Lie algebra, we sketch the essential features of this interaction, distinguishing in particular the cases of integrable and nonintegrable representations. While integrable representations are well understood, nonintegrable representations are quite mysterious objects. We present here a short and didactical-minded overview of the subject.

RepresentationsUnbounded operatorAlgebraLie aalgebraPure mathematicsIntegrable systemSettore MAT/05 - Analisi MatematicaLie algebraSubject (philosophy)Algebra over a fieldSketchMathematics
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"Table 3" of "Comprehensive measurements of $t$-channel single top-quark production cross sections at $\sqrt{s} = 7$ TeV with the ATLAS detector"

2014

The cross sections for top-quark and top-antiquark production in the t-channel, together with the cross-section ratio.

SIG/SIGP P --> TOP XHigh Energy Physics::LatticeRapidity DependenceHigh Energy Physics::PhenomenologyTop7000.0DSIG/DYRAPSIGComputer Science::Computers and SocietySingle Differential Cross SectionP P --> TOPBAR XInclusiveNonlinear Sciences::Exactly Solvable and Integrable SystemsTotal cross-sectionProton-Proton ScatteringPhysics::Atomic and Molecular ClustersCross-section ratio
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Poisson-Nijenhuis structures and the Vinogradov bracket

1994

We express the compatibility conditions that a Poisson bivector and a Nijenhuis tensor must fulfil in order to be a Poisson-Nijenhuis structure by means of a graded Lie bracket. This bracket is a generalization of Schouten and Frolicher-Nijenhuis graded Lie brackets defined on multivector fields and on vector valued differential forms respectively.

Schouten–Nijenhuis bracketGraded Lie algebraAlgebraFrölicher–Nijenhuis bracketPoisson bracketAdjoint representation of a Lie algebraNonlinear Sciences::Exactly Solvable and Integrable SystemsMathematics::Quantum AlgebraPoisson manifoldLie bracket of vector fieldsLie derivativeMathematics::Differential GeometryGeometry and TopologyMathematics::Symplectic GeometryAnalysisMathematicsAnnals of Global Analysis and Geometry
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On Determinants of Integrable Operators with Shifts

2013

Integrable integral operator can be studied by means of a matrix Riemann--Hilbert problem. However, in the case of so-called integrable operators with shifts, the associated Riemann--Hilbert problem becomes operator valued and this complicates strongly the analysis. In this note, we show how to circumvent, in a very simple way, the use of such a setting while still being able to characterize the large-$x$ asymptotic behavior of the determinant associated with the operator.

Semi-elliptic operatorPure mathematicsOperator (computer programming)Multiplication operatorIntegrable systemGeneral MathematicsMathematical analysisFinite-rank operatorOperator theoryCompact operatorMathematicsQuasinormal operatorInternational Mathematics Research Notices
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Orbital Structure of the Two Fixed Centres Problem

1999

The set of orbits of the Two Fixed Centres problem has been known for a long time (Charlier, 1902, 1907; Pars, 1965), since it is an integrable Hamiltonian system.

Set (abstract data type)Equilibrium pointPhysicsHamiltonian mechanicssymbols.namesakeClassical mechanicsIntegrable systemStructure (category theory)symbolsPeriodic orbitsCelestial mechanicsHamiltonian system
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The Kp Hierarchy

1989

As an application of the theory of infinite-dimensional Grassmannians and the representation theory of gl1 we shall study in this chapter certain nonlinear “exactly solvable” systems of differential equations. Exactly solvable means here that the nonlinear system can be transformed to an (infinite-dimensional) linear problem. A prototype of the equations is the Korteweg-de Vries equation $$\frac{{\partial u}}{{\partial t}} = \frac{3}{3}u\frac{{\partial u}}{{\partial x}} + \frac{1}{4}\frac{{{\partial ^3}u}}{{\partial {x^3}}}$$ . It turns out that it is more natural to consider an infinite system of equations like that above, for obtaining explicit solutions. The set of equations is called th…

Set (abstract data type)Pure mathematicsNonlinear systemNonlinear Sciences::Exactly Solvable and Integrable SystemsHierarchy (mathematics)Differential equationGrassmannianKdV hierarchySystem of linear equationsRepresentation theoryMathematics
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