Search results for "baryon"

showing 10 items of 759 documents

Chiral Dynamics of the two Lambda(1405) States

2004

Using a chiral unitary approach for the meson--baryon interactions, we show that two octets of J^{\pi}=1/2^- baryon states, which are degenerate in the limit of exact SU(3) symmetry, and a singlet are generated dynamically. The SU(3) breaking produces the splitting of the two octets, resulting in the case of strangeness S=-1 in two poles of the scattering matrix close to the nominal \Lambda(1405) resonance. These poles are combinations of the singlet state and the octets. We show how actual experiments see just one effective resonance shape, but with properties which change from one reaction to another.

Nuclear TheoryLambda(1405)High Energy Physics::Latticeinelastic scattering [meson baryon]Nuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaSU(3) [symmetry]singlet [baryon]symmetry breakingcoupled channelHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Phenomenologyddc:530elastic scattering [meson baryon]chiral [effective Lagrangian]numerical calculationsNuclear Experimentoctet [baryon]analytic properties [scattering amplitude]
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Transition form factors of the N(*()1535) as a dynamically generated resonance

2007

We discuss how electromagnetic properties provide useful tests of the nature of resonances, and we study these properties for the N*(1535) which appears dynamically generated from the strong interaction of mesons and baryons. Within this coupled channel chiral unitary approach, we evaluate the A_1/2 and S_1/2 helicity amplitudes as a function of Q^2 for the electromagnetic N*(1535) to gamma* N transition. Within the same formalism we evaluate the cross section for the reactions gamma N to eta N. We find a fair agreement for the absolute values of the transition amplitudes, as well as for the Q^2 dependence of the amplitudes, within theoretical and experimental uncertainties discussed in the…

Nuclear Theorydispersion relationamplitude analysis [helicity]Nuclear Theoryform factor [N(1535)]FOS: Physical sciencesscattering amplitude [meson baryon]Nuclear Theory (nucl-th)nonrelativistictransition [form factor]ddc:530higher-order [Feynman graph]ratio [channel cross section]numerical calculationsNuclear Experimentphotoproduction [eta]chiral [symmetry]effective LagrangianFísicaenergy dependence [channel cross section]coupled channelradiative decay [N(1535)]relativisticinelastic scattering [electron nucleon]inelastic scattering [photon nucleon]
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Collectivity in ${}^{\mathrm{196,198}}$Pb isotopes probed in Coulomb-excitation experiments at REX-ISOLDE

2017

The neutron-deficient ${}^{\mathrm{196,198}}$Pb isotopes have been studied in Coulomb-excitation experiments employing the Miniball γ-ray spectrometer and radioactive ion beams from the REX-ISOLDE post-accelerator at CERN. The reduced transition probabilities of the first excited 2+ states in 196Pb and 198Pb nuclei have been measured for the first time. Values of $B(E2)={18.2}_{-4.1}^{+4.8}$ W.u. and $B(E2)={13.1}_{-3.5}^{+4.9}$ W.u., were obtained, respectively. The experiment sheds light on the development of collectivity when moving from the regime governed by the generalised seniority scheme to a region, where intruding structures, associated with different deformed shapes, start to com…

Nuclear and High Energy Physics3106Coulomb excitationREX-ISOLDESHELLHadronElementary particleCoulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]114 Physical sciences01 natural sciencesNuclear physicsSHAPE COEXISTENCE0103 physical sciencesSCATTERINGradioactive ion beamsACCELERATED RADIOACTIVE BEAMS010306 general physicsPhysicsPb isotopesNUCLEI010308 nuclear & particles physicsBaryongamma-ray spectroscopyEXCITED-STATESCoulomb-excitation experimentExcited stateAtomic physicsGround stateNucleongamma transitions and level energiesEnergy (signal processing)
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Measurement of the spin of the Xi(1530) resonance

2008

The properties of the Xi(1530) resonance are investigated in the Lambdac+ --> Xi- pi+ K+ decay process. The data sample was collected with the BaBar detector at the SLAC PEP-II asymmetric-energy e+ e- collider operating at center of mass energies 10.58 and 10.54 GeV. The corresponding integrated luminosity is approximately 230 inverse fb. The spin of the Xi(1530) is established to be 3/2. The existence of an S-wave amplitude in the Xi- pi+ system is inferred, and its interference with the Xi(1530)0 amplitude provides the first clear demonstration of the Breit-Wigner phase motion expected for the Xi(1530). The P_1(cos[theta(Xi-)]) Legendre polynomial moment indicates the presence of a sig…

Nuclear and High Energy PhysicsBABARElectron–positron annihilationFOS: Physical sciencesDalitz plotMASSPARTICLE PHYSICS; PEP2; BABAR01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Particle decay0103 physical sciencesPEP2MASS; PARITY; WIDTH[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsPhysicsPARITY010308 nuclear & particles physicsHyperonWIDTHResonanceBABAR detectorHEPCharmed baryonsAmplitudeBaBarPARTICLE PHYSICSCenter of massFísica de partículesExperiments
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Measurement of the absolute branching fraction for Λc+→Λμ+νμ

2017

Abstract We report the first measurement of the absolute branching fraction for Λ c + → Λ μ + ν μ . This measurement is based on a sample of e + e − annihilation data produced at a center-of-mass energy s = 4.6  GeV , collected with the BESIII detector at the BEPCII storage rings. The sample corresponds to an integrated luminosity of 567  pb − 1 . The branching fraction is determined to be B ( Λ c + → Λ μ + ν μ ) = ( 3.49 ± 0.46 ( stat ) ± 0.27 ( syst ) ) % . In addition, we calculate the ratio B ( Λ c + → Λ μ + ν μ ) / B ( Λ c + → Λ e + ν e ) to be 0.96 ± 0.16 ( stat ) ± 0.04 ( syst ) .

Nuclear and High Energy PhysicsBESIII детекторElectron–positron annihilationAnalytical chemistryAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesLuminosityNOлептоны0103 physical sciencesAbsolute branching fraction010306 general physicsNuclear ExperimentPhysicsAnnihilation010308 nuclear & particles physicsBranching fraction?c +Absolute branching fraction; BESIII; Semi-leptonic decay; Λc+; Nuclear and High Energy PhysicsBESIIIΛc+lcsh:QC1-999BaryonBEPCII коллайдерSemi-leptonic decayHigh Energy Physics::ExperimentAstrophysics::Earth and Planetary Astrophysicslcsh:Physics
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Properties of the ground-state baryons in chiral perturbation theory

2010

15th High Energy Physics International Conference on Quantum Chromodynamics. Montpellier (FRANCE). JUN 28-JUL 02, 2010

Nuclear and High Energy PhysicsChiral perturbation theoryNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryLattice field theoryExtrapolationFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)Theoretical physicsHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeChiral perturbation theoryNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentPhysicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyHyperonLattice QCDAtomic and Molecular Physics and OpticsBaryonHigh Energy Physics - PhenomenologyCoupling (physics)Baryon structureGround stateNuclear Physics B - Proceedings Supplements
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Constraints on neutrino masses from Planck and Galaxy clustering data

2013

We present here bounds on neutrino masses from the combination of recent Planck cosmic microwave background (CMB) measurements and galaxy clustering information from the Baryon Oscillation Spectroscopic Survey, part of the Sloan Digital Sky Survey-III. We use the full shape of either the photometric angular clustering (Data Release 8) or the 3D spectroscopic clustering (Data Release 9) power spectrum in different cosmological scenarios. In the Lambda CDM scenario, spectroscopic galaxy clustering measurements improve significantly the existing neutrino mass bounds from Planck data. We find Sigma m(v) < 0.39 eV at 95% confidence level for the combination of the 3D power spectrum with Planck C…

Nuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Age of the universeCosmic microwave backgroundDark matterFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysics01 natural sciencesPartícules (Física nuclear)symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesPlanck010303 astronomy & astrophysicsDigital sky surveyPhysicsCosmologia010308 nuclear & particles physicsHigh Energy Physics - Phenomenology13. Climate actionsymbolsDark energyBaryon acoustic-oscillationsBaryon acoustic oscillationsNeutrinoAstrophysics - Cosmology and Nongalactic AstrophysicsHubble's lawPhysical Review D
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Probing chemical freeze-out criteria in relativistic nuclear collisions with coarse grained transport simulations

2020

We introduce a novel approach based on elastic and inelastic scattering rates to extract the hyper-surface of the chemical freeze-out from a hadronic transport model in the energy range from E$_\mathrm{lab}=1.23$ AGeV to $\sqrt{s_\mathrm{NN}}=62.4$ GeV. For this study, the Ultra-relativistic Quantum Molecular Dynamics (UrQMD) model combined with a coarse-graining method is employed. The chemical freeze-out distribution is reconstructed from the pions through several decay and re-formation chains involving resonances and taking into account inelastic, pseudo-elastic and string excitation reactions. The extracted average temperature and baryon chemical potential are then compared to statistic…

Nuclear and High Energy PhysicsNuclear TheoryNuclear TheoryHadronFOS: Physical scienceshiukkasfysiikkaStrangenessInelastic scattering53001 natural sciencesNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Phenomenology (hep-ph)Pion0103 physical sciencesddc:530Nuclear Experiment (nucl-ex)Nuclear Experiment010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyBaryonHigh Energy Physics - PhenomenologyQuark–gluon plasmarelativistic nuclear collisionsHigh Energy Physics::ExperimentydinfysiikkaEnergy (signal processing)LeptonThe European Physical Journal A
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Chiral Symmetry of Baryons

2001

We study chiral symmetry aspects of the positive and negative parity baryons by identifying them with linear representations of the chiral group $SU(N_{f}) \otimes SU(N_{f})$. It is shown that there are two distinctive schemes: naive and mirror assignments. We construct linear sigma models for baryons in the two assignments and examine their physical implications. Then we investigate properties of the naive and mirror nucleons microscopically by using QCD interpolating fields. Finally, we propose experiments to distinguish the two chiral assignments for the nucleon.

Nuclear and High Energy PhysicsParticle physicsChiral perturbation theoryPhysics and Astronomy (miscellaneous)Spontaneous symmetry breakingmedia_common.quotation_subjectHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesAsymmetryGroup representationPionHigh Energy Physics - Phenomenology (hep-ph)Nambu–Jona-Lasinio modelNuclear Experimentmedia_commonChiral anomalyQuantum chromodynamicsPhysicsChiral symmetryHigh Energy Physics::PhenomenologySigmaParity (physics)BaryonHigh Energy Physics - PhenomenologyChiral symmetry breakingNucleon
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Probing interactions within the dark matter sector via extra radiation contributions

2013

The nature of dark matter is one of the most thrilling riddles for both cosmology and particle physics nowadays. While in the typical models the dark sector is composed only by weakly interacting massive particles, an arguably more natural scenario would include a whole set of gauge interactions which are invisible for the standard model but that are in contact with the dark matter. We present a method to constrain the number of massless gauge bosons and other relativistic particles that might be present in the dark sector using current and future cosmic microwave background data, and provide upper bounds on the size of the dark sector. We use the fact that the dark matter abundance depends…

Nuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)media_common.quotation_subjectDark matterCosmic microwave backgroundFOS: Physical sciencesAstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsCosmologyPartícules (Física nuclear)symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)PlanckDigital sky surveymedia_commonPhysicsHigh Energy Physics::PhenomenologyUniverseHigh Energy Physics - PhenomenologyWeakly interacting massive particlessymbolsBaryon acoustic-oscillationsBaryon acoustic oscillationsAstrophysics - Cosmology and Nongalactic AstrophysicsHubble's law
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