Search results for "RESONANCES"

showing 10 items of 67 documents

Search for new particles in two-jet final states in 7 TeV proton-proton collisions with the ATLAS detector at the LHC

2010

19 páginas, 2 figuras, 1 tabla.-- et al.(ATLAS Collaboration).

ProtonAtlas detectorPhysics::Instrumentation and DetectorsPhysics beyond the Standard ModelGeneral Physics and AstronomyJet (particle physics)particle physic01 natural sciencesSettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)12.60.Rcddc:550[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]13.87.CeQCPhysicsPACS numbers: 13.85.Rm 12.60.Rc 13.87.Ce 14.80.-jLarge Hadron ColliderLuminosity (scattering theory)Cross sectionAcceleradors de partículesSettore FIS/01 - Fisica Sperimentale14.80.-jATLASnumbers: 13.85.Rm3. Good healthDijetsmedicine.anatomical_structureComputingMethodologies_DOCUMENTANDTEXTPROCESSINGTWO-JETSLHCParticle Physics - ExperimentjetsFinal stateParticle physicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Partícules (Física nuclear)Nuclear physicsCross section (physics)Excited QuarksAtlas (anatomy)0103 physical sciencesmedicine010306 general physicsIntegrated luminosityProton proton collisionsParton Distributions010308 nuclear & particles physicsATLAS detectorsHigh Energy Physics::PhenomenologyFísicaPARTON DISTRIBUTIONS HADRON COLLIDERS EXCITED QUARKS DIJETSHadron CollidersHeavy particlesLHC ; ATLAS ; Collisions ; 7 TeV ; Two jets ; ResonancesExperimental High Energy PhysicsNEW PARTICLESproton-proton collisionsHigh Energy Physics::Experimentcollider
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Resonances for nonanalytic potentials

2009

We consider semiclassical Schr"odinger operators on $R^n$, with $C^infty$ potentials decaying polynomially at infinity. The usual theories of resonances do not apply in such a non-analytic framework. Here, under some additional conditions, we show that resonances are invariantly defined up to any power of their imaginary part. The theory is based on resolvent estimates for families of approximating distorted operators with potentials that are holomorphic in narrow complex sectors around $R^n$.

QUANTUM RESONANCESNumerical AnalysisSchroedinger operatorsresonancesApplied MathematicsSEMICLASSICAL ANALYSIS35B3447A1035P99Breit–Wigner peaksQuantum mechanics81Q20SCHROEDINGER OPERATORAnalysisMathematicsAnalysis & PDE
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Charmed baryon resonances with heavy-quark symmetry

2009

We study charmed baryon resonances that are generated dynamically from a coupled-channel unitary approach that implements heavy-quark symmetry. Some states can already be identified with experimental observations, such as $\Lambda_c(2595)$,$\Lambda_c(2660)$, $\Sigma_c(2902)$ or $\Lambda_c(2941)$, while others need a compilation of more experimental data as well as an extension of the model to include higher order contributions. We also compare our model to previous SU(4) schemes.

QuarkDYNAMICSNuclear and High Energy PhysicsParticle physicsNuclear Theorycharmed baryon resonancesFOS: Physical sciencesLambdaUnitary stateHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)Heavy-quark symmetryHigh Energy Physics - Phenomenology (hep-ph)Condensed Matter::SuperconductivitySU(8) and SU(4) spin-flavor symmetryInstrumentationNuclear theoryPhysicsHigh Energy Physics::PhenomenologySigmaOrder (ring theory)FísicaCharmed baryon resonancesAstronomy and AstrophysicsCOUPLED-CHANNELSymmetry (physics)BaryonHigh Energy Physics - Phenomenologyheavy-quark symmetryHigh Energy Physics::ExperimentChinese physics c
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Weak decays of heavy hadrons into dynamically generated resonances

2016

In this paper, we present a review of recent works on weak decay of heavy mesons and baryons with two mesons, or a meson and a baryon, interacting strongly in the final state. The aim is to learn about the interaction of hadrons and how some particular resonances are produced in the reactions. It is shown that these reactions have peculiar features and act as filters for some quantum numbers which allow to identify easily some resonances and learn about their nature. The combination of basic elements of the weak interaction with the framework of the chiral unitary approach allow for an interpretation of results of many reactions and add a novel information to different aspects of the hadron…

QuarkNuclear and High Energy PhysicsParticle physicsFinal state interactionNuclear TheoryMesonNuclear TheoryHadronBaryon weak decaysFOS: Physical sciencesGeneral Physics and AstronomyHadronsLambda01 natural sciencesHeavy mesonNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesMesons (Nuclear physics)Mesons (Física nuclear)Nuclear Experiment010306 general physicsWave functionWeak interactions (Nuclear physics)PhysicsMesonic and baryonic resonances010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyInteraccions febles (Física nuclear)State (functional analysis)BaryonHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentProduction (computer science)International Journal of Modern Physics E
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Exotic dynamically generated baryons with negative charm quantum number

2010

Following a model based on the SU(8) symmetry that treats heavy pseudoscalars and heavy vector mesons on an equal footing, as required by heavy quark symmetry, we study the interaction of baryons and mesons in coupled channels within an unitary approach that generates dynamically poles in the scattering T-matrix. We concentrate in the exotic channels with negative charm quantum number for which there is the experimental claim of one state.

QuarkNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciences01 natural sciencesUnitary statePartícules (Matèria)Properties of specific particlesHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesBaryons010306 general physicsNuclear ExperimentBarionsPhysics010308 nuclear & particles physicsScatteringHigh Energy Physics::PhenomenologyFísicaExotic hadronCOUPLED-CHANNELSymmetry (physics)BaryonCharmed baryonsHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentRESONANCES
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Hidden beauty molecules within the local hidden gauge approach and heavy quark spin symmetry

2013

Using a coupled channel unitary approach, combining the heavy quark spin symmetry and the dynamics of the local hidden gauge, we investigate the meson-meson interaction with hidden beauty and obtain several new states. Both I = 0 and I = 1 states are analyzed, and it is shown that in the I = 1 sector, the interactions are too weak to create any bound states within our framework. In total, we predict with confidence the existence of six bound states and six more possible weakly bound states. The existence of these weakly bound states depends on the influence of the coupled channel effects.

QuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsBound statesMeson resonancesHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaGauge (firearms)01 natural sciencesUnitary stateHigh Energy Physics - ExperimentHigh Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesBound stateMoleculeSpin symmetryNuclear Experiment (nucl-ex)010306 general physicsNuclear Experiment
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The role of f(0)(1710) in the phi omega threshold peak of J/Psi -> gamma phi omega

2013

We study the process J/Psi -> gamma phi omega, measured by the BES experiment, where a neat peak close to the phi omega threshold is observed and is associated to a scalar meson resonance around 1800 MeV. We make the observation that a scalar resonance coupling to phi omega unavoidably couples strongly to K (K) over bar, but no trace of a peak is seen in the K (K) over bar spectrum of the J/Psi -> gamma K (K) over bar at this energy. This serves us to rule out the interpretation of the observed peak as a signal of a new resonance. After this is done, a thorough study is performed on the production of a pair of vector mesons and how its interaction leads necessarily to a peak in the J/Psi ->…

ResonancesFísicaHigh Energy Physics::ExperimentDecays
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Graphical Schemes Designed to Display and Study the Long-term Variations of Schumann Resonance

2019

This work proposes and illustrates a graphical approach aimed at studying a wide range of features of the ELF horizontal magnetic field signal recorded at the Sierra Nevada station (Spain). In addition to the traditional long-term variations in the parameters of the first three Schumann resonances (their amplitudes, central frequencies and widths), many other properties such as the saturations of the magnetometers, anomalous values for the parameters or spectra with any kind of particularities are taken into consideration in this work. These features can provide us with complementary information about the long-term variation of Schumann resonances, give an estimation of the extent up to whi…

Signal processingSchumann resonancesMagnetometer020206 networking & telecommunications02 engineering and technologySignalLightningTerm (time)law.inventionComputational physicsAmplitudelaw0202 electrical engineering electronic engineering information engineeringRange (statistics)020201 artificial intelligence & image processingGeology2019 27th European Signal Processing Conference (EUSIPCO)
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Solar storm effects during Saint Patrick's Days in 2013 and 2015 on the Schumann resonances measured by the ELF station at Sierra Nevada (Spain)

2016

Solar storm of 1859PhysicsGeophysics010504 meteorology & atmospheric sciencesSchumann resonancesSpace and Planetary Science0103 physical sciencesSAINTAtmospheric sciences010303 astronomy & astrophysics01 natural sciences0105 earth and related environmental sciencesJournal of Geophysical Research: Space Physics
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First measurement of the charge asymmetry in boosted top quark pair production in the ATLAS experiment using the Grid-based Tier-3 facility at IFIC-V…

2016

The Large Hadron Collider (LHC) at CERN is the largest collider ever built. It is assembled in the same 27 km tunnel where Large Electron-Positron Collider (LEP) used to be, $\sim$ 100 m underground, near Geneva (Switzerland). The main interaction points have four experiments installed: ATLAS, CMS, ALICE and LHCb. The LHC is designed to collide two proton beams, that circulate in opposite directions, each with an energy of up to 7 TeV, reaching a centre-of-mass energy up to 14 TeV. %%%%%%%%% The ATLAS experiment is a general-purpose detector designed to exploit the potential of the LHC. With a total weight of 7000 tonnes, ATLAS is the heaviest experiment at the LHC. It has 42 m of total len…

TierresonancesHigh Energy Physics::Phenomenologycharge asymmetryFísicaHigh Energy Physics::ExperimentboostedLHCATLASgridAltas energíastop quark
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