Search results for "baryon"

showing 10 items of 759 documents

Very Heavy Flavored Dibaryons

2020

We explore the possibility of very heavy dibaryons with three charm quarks and three beauty quarks, $bbbccc$, using a constituent model which should drive to the correct solution in the limit of hadrons made of heavy quarks. The six-body problem is treated rigorously, in particular taking into account the orbital, color and spin mixed-symmetry components of the wave function. Unlike a recent claim based on lattice QCD, no bound state is found below the lowest dissociation threshold.

QuarkParticle physicswave function[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Nuclear TheoryHigh Energy Physics::LatticeHadronLattice field theoryNuclear TheoryGeneral Physics and AstronomyFOS: Physical sciencesdissociationspin01 natural sciencesCharm quarkquarkNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciencesBound stateheavy quark010306 general physicsWave functionconstituentNuclear ExperimentNuclear theoryPhysics010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics - Lattice (hep-lat)High Energy Physics::Phenomenologylattice field theoryLattice QCDcolordibaryon: heavybound stateHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Elementary Particles and FieldsHigh Energy Physics::ExperimenthadroncharmPhysical Review Letters
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Search for pentaquarks states in Z decays

2004

Exotic hadrons made of five quarks (pentaquarks) are searched for in hadronic Z decays collected by the ALEPH detector at LEP. No significant signal is observed. At 95% C.L. upper limits are set on the production rates N of such particles and their charge-conjugate state per Z decay: N Θ(1535)+·BR(Θ(1535)+→pK S0)<6.2×10-4, N Ε(1862)-·BR(Ε(1862)-→Ε -π-)<4.5×10-4, N Ε(1862)0·BR(Ε(1862)0→Ε -π+)<8.9×10-4, N Θc(3100)0·BR(Θc(3100) 0→D*-p)<6.3×10-4, N Θc(3100)0·BR(Θc(3100) 0→D-p)<31×10-4. © 2004 Elsevier B.V. All rights reserved.

QuarkPhysics1221Particle physicsAlephNuclear and High Energy Physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHadronNuclear TheoryHigh Energy Physics::PhenomenologyExotic hadronState (functional analysis)01 natural sciencesPentaquarkNuclear physicsbaryons mass soliton model0103 physical sciencesQC770[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Physique des particules élémentairesProduction (computer science)High Energy Physics::Experiment010306 general physicsNuclear Experiment
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Hadron correlators and the structure of the quark propagator

1994

The structure of the quark propagator of $QCD$ in a confining background is not known. We make an Ansatz for it, as hinted by a particular mechanism for confinement, and analyze its implications in the meson and baryon correlators. We connect the various terms in the K\"allen-Lehmann representation of the quark propagator with appropriate combinations of hadron correlators, which may ultimately be calculated in lattice $QCD$. Furthermore, using the positivity of the path integral measure for vector like theories, we reanalyze some mass inequalities in our formalism. A curiosity of the analysis is that, the exotic components of the propagator (axial and tensor), produce terms in the hadron c…

QuarkPhysicsHigh Energy Physics - TheoryPhysics and Astronomy (miscellaneous)MesonHigh Energy Physics::LatticeHadronHigh Energy Physics::PhenomenologyPropagatorFOS: Physical sciencesFísicaBaryonTheoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Path integral formulationHigh Energy Physics::ExperimentGauge theoryEngineering (miscellaneous)Ansatz
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Top quark mass measurements in ATLAS

2014

The top quark is a fundamental constituent of the Standard Model (SM). The properties of this quark are accurately predicted by this theory, except for its mass, which remains a fundamental parameter of the SM. With the advent of the Large Hadron Collider (LHC), many million of top-antitop quark pairs are available for study. With such statistics, the physics of the top quark has entered the precision era. In this note, the most recent experimental results by ATLAS concerning the top quark mass are reported.

QuarkPhysicsHistoryStop squarkTop quarkParticle physicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyTop quark condensateOmega baryonBottom quarkComputer Science ApplicationsEducationSigma baryonNuclear physicsPhysics::Atomic and Molecular ClustersHigh Energy Physics::ExperimentB mesonParticle Physics - ExperimentJournal of Physics: Conference Series
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Top physics studies at the LHC in the standard model and beyond with the ATLAS detector

2009

The LHC will be a Top quark factory, producing large numbers of Top quarks even at the initial low luminosities. This will enable a rich program of Top quark Physics to be explored, both within the Standard Model and using Top quarks as probes of Physics Beyond the Standard Model. Recent studies from ATLAS will be presented, including prospects for the measurements of the production of Top pairs and single Top production, angular correlations in the Top decay, and the precision measurement of the Top quark mass. The search for Physics beyond the Standard Model will be illustrated with searches for rare Top decays involving Flavour Changing Neutral Currents, and the reconstruction of tt-bar …

QuarkPhysicsHistoryTop quarkParticle physicsLarge Hadron Collider010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFlavourTop quark condensateOmega baryon01 natural sciencesComputer Science::Computers and SocietyComputer Science ApplicationsEducationSigma baryonNonlinear Sciences::Chaotic DynamicsNuclear physicsNonlinear Sciences::Exactly Solvable and Integrable Systems0103 physical sciencesPhysics::Atomic and Molecular ClustersHigh Energy Physics::ExperimentDetectors and Experimental Techniques010306 general physicsJournal of Physics: Conference Series
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The soliton-soliton interaction in the Chiral Dilaton Model

2012

We study the interaction between two B = 1 states in the Chiral Dilaton Model where baryons are described as nontopological solitons arising from the interaction of chiral mesons and quarks. By using the hedgehog solution for B = 1 states we construct, via a product ansatz, three possible B = 2 configurations to analyse the role of the relative orientation of the hedgehog quills in the dynamics of the soliton-soliton interaction and investigate the behavior of these solutions in the range of long/intermediate distance. One of the solutions is quite binding due to the dynamics of the pi and sigma fields at intermediate distance and should be used for nuclear matter studies. Since the product…

QuarkPhysicsNuclear and High Energy PhysicsMesonNuclear TheoryHigh Energy Physics::PhenomenologyNuclear TheoryFOS: Physical sciencesFísicaAstronomy and AstrophysicsInteraction energyAtomic and Molecular Physics and OpticsNuclear Theory (nucl-th)BaryonScale invarianceNonlinear Sciences::Exactly Solvable and Integrable SystemsBound stateNontopological solitonsDilatonSolitonChiral symmetriesDense matterMathematical physicsAnsatz
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Radiative decays of double heavy baryons in a relativistic constituent three-quark model including hyperfine mixing

2010

We study flavor-conserving radiative decays of double heavy baryons using a manifestly Lorentz covariant constituent three-quark model. Decay rates are calculated and compared to each other in the full theory, keeping masses finite, and also in the heavy quark limit. We discuss in some detail hyperfine mixing effects.

QuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeQuark modelHadronNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesElementary particleFermion01 natural sciencesBaryonNuclear physicsCharmed baryonsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesRadiative transferHigh Energy Physics::Experiment010306 general physicsNuclear Experiment
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Heavy Baryons and electromagnetic decays

2000

In this talk I review the theory of electromagnetic decays of the ground state baryon multiplets with oneheavy quark, calculated using Heavy Hadron Chiral Perturbation Theory. The M1 and E2 amplitudes for (S^{*}-&gt; S gamma), (S^{*} -&gt; T gamma) and (S -&gt; T gamma)are separately analyzed. All M1 transitions are calculated up to O(1/��_��^2). The E2 amplitudes contribute at the same order for (S^{*}-&gt; S gamma), while for (S^{*} -&gt; T gamma) they first appear at O(1/(m_Q ��_��^2))and for (S -&gt; T gamma) are completely negligible. Once the loop contributions is considered, relations among different decay amplitudes are derived. Furthermore, one can obtain an absolute prediction for…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyHadronFOS: Physical sciencesOrder (ring theory)LambdaAtomic and Molecular Physics and OpticsBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)AmplitudeGround stateNuclear Physics B - Proceedings Supplements
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Charmed and Bottom Baryons: a Variational Approach based on Heavy Quark Symmetry

2003

The use of Heavy Quark Symmetry to study bottom and charmed baryons leads to important simplifications of the non-relativistic three body problem, which turns out to be easily solved by a simple variational ansatz. Our simple scheme reproduces previous results (baryon masses, charge and mass radii, $...$) obtained by solving the Faddeev equations with simple non-relativistic quark--quark potentials, adjusted to the light and heavy--light meson spectra. Wave functions, parameterized in a simple manner, are also given and thus they can be easily used to compute further observables. Our method has been also used to find the predictions for strangeness-less baryons of the SU(2) chirally inspire…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsFaddeev equationsMesonNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaCharge (physics)BaryonCharmed baryonsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNuclear ExperimentAnsatz
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Quark exchange in deep inelastic scattering

1995

We use a model for baryons that links the constituent structure to the deep inelastic (current) properties. The approach consists in a laboratory partonic description (based on a model of hadron structure), to which a low momentum scaleQ 0 is adscribed, which is evolved to high momenta by means of the renormalization group. A generalization of the model by means of the hadronic quark cluster decomposition, provides a description of the structure functions of nuclei and is the starting point to study the effects that the antisymmetrization at the quark level has on the structure function of a model deuteron. The analysis contains conventional and high momentum partonic components. We next st…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHadronHigh Energy Physics::PhenomenologyNuclear TheoryFísicaRenormalization groupDeep inelastic scatteringBaryonNuclear physicsMomentumsymbols.namesakePauli exclusion principlesymbolsNuclear fusionHigh Energy Physics::ExperimentNuclear ExperimentParticle Physics - Phenomenology
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