Search results for "charmed baryon"

showing 10 items of 54 documents

Observation of an Excited Charm BaryonΩc*Decaying toΩc0γ

2006

We report the first observation of an excited singly-charm baryon OmegaC* (css) in the radiative decay OmegaC0 Gamma, where the OmegaC0 baryon is reconstructed in the decays to the final states Omega-pi+, Omega-pi+pi0, Omega-pi+pi-pi+, and Cascade-K-pi+pi+. This analysis is performed using a dataset of 230.7 fb$-1} collected by the BABAR detector at the PEP-II asymmetric-energy B Factory at the Stanford Linear Accelerator Center. The mass difference between the OmegaC* and the OmegaC0 baryons is measured to be 70.8 +/- 1.0 (stat) +/- 1.1 (syst) MeV/c2. We also measure the ratio of inclusive production cross sections of OmegaC* and OmegaC0 in e+e- annihilation.

PhysicsParticle physicsAnnihilation010308 nuclear & particles physicsElectron–positron annihilationGeneral Physics and Astronomy01 natural sciences7. Clean energyB-factoryCharmed baryonsBaryonNuclear physicsParticle decayPositronPair production0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysical Review Letters
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Observation of a Charmed Baryon Decaying toD0pat a Mass Near2.94  GeV/c2

2007

A search for charmed baryons decaying to $D^0 p$ reveals two states: the $\Lambda_c(2880)^+$ baryon and a previously unobserved state at a mass of [$2939.8\pm 1.3 \text{(stat.)}\pm 1.0 \text{(syst.)}$]~\mevcc and with an intrinsic width of [$17.5\pm 5.2 \text{(stat.)}\pm 5.9 \text{(syst.)}$]~\mev. Consistent and significant signals are observed for the $K^-\pi^+$ and $K^-\pi^+\pi^-\pi^+$ decay modes of the $D^0$ in 287 ${\rm fb}^{-1}$ annihilation data recorded by the BaBar detector at a center-of-mass energy of 10.58~${\rm GeV}/c^2$. There is no evidence in the $D^+ p$ spectrum of doubly-charged partners. The mass and intrinsic width of the $\Lambda_c(2880)^+$ baryon and relative yield of …

PhysicsParticle physicsAnnihilation010308 nuclear & particles physicsElectron–positron annihilationGeneral Physics and AstronomyLambda01 natural sciencesBaryonNuclear physicsCharmed baryonsParticle decayPion0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsEnergy (signal processing)Physical Review Letters
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Masses of doubly charmed baryons in the extended on-mass-shell renormalization scheme

2016

In this work, we investigate the mass corrections of the doubly charmed baryons up to $N^2LO$ in the extended-on-mass-shell (EOMS) renormalization scheme, comparing with the results of heavy baryon chiral perturbation theory. We find that the terms from the heavy baryon approach are a subset of those obtained in the EOMS scheme. By fitting the lattice data, we can determine the parameters $\tilde{m}$, $\alpha$, $c_1$ and $c_7$ from the Lagrangian, while in the heavy baryon approach no information on $c_1$ can be obtained from the baryons mass. Correspondingly, the masses of $m_{\Xi_{cc}}$ and $m_{\Omega_{cc}}$ are predicted, in the EOMS scheme, extrapolating the results from different value…

PhysicsParticle physicsHeavy baryon chiral perturbation theory010308 nuclear & particles physicsHigh Energy Physics::LatticeLattice field theoryNuclear TheoryHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesLattice QCD01 natural sciencesCharm quarkCharmed baryonsBaryonRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticePionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsNuclear Experiment
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Ab initio three-loop calculation of the W -exchange contribution to nonleptonic decays of double charm baryons

2019

We have made an ab initio three-loop quark model calculation of the $W$-exchange contribution to the nonleptonic two-body decays of the doubly charmed baryons $\Xi_{cc}^{++}$ and $\Omega_{cc}^{+}$. The $W$-exchange contributions appear in addition to the factorizable tree graph contributions and are not suppressed in general. We make use of the covariant confined quark model previously developed by us to calculate the tree graph as well as the $W$-exchange contribution. We calculate helicity amplitudes and quantitatively compare the tree graph and $W$-exchange contributions. Finally, we compare the calculated decay widths with those from other theoretical approaches when they are available.

PhysicsParticle physicsLoop (graph theory)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyQuark modelAb initioFOS: Physical sciencesComputer Science::Digital Libraries01 natural sciencesHelicityOmegaCharmed baryonsBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::ExperimentCharm (quantum number)010306 general physicsPhysical Review D
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Magnetic moments of heavy baryons

2000

6 páginas, 2 figuras, 4 tablas.-- PACS number(s): 12.39.Fe, 12.39.Hg, 14.20.Lq, 14.20.Mr

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryMagnetic momentHigh Energy Physics::LatticeHadronNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesPartícules (Física nuclear)BaryonCharmed baryonsRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Order (group theory)Nuclear Experiment
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Spectra of the lightest baryons containing two heavy quarks in a potential model

2000

The spectra of baryons which include two heavy quarks can be treated as a two-body system, where the two heavy quarks constitute a bosonic diquark. We derive the effective potential between the light quark and the heavy diquark in terms of the Bethe-Salpeter equation. To obtain the spectra, several serious problems need to be solved: (1) the operator ordering, (2) the errors caused by the nonrelativistic expansion, (3) spin-spin coupling, and (4) the mixing between the scalar-diquark-baryon and vector-diquark-baryon. In this work we take reasonable approaches to deal with them.

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeOperator (physics)Nuclear TheoryHigh Energy Physics::PhenomenologyOmega baryonGluonBaryonCharmed baryonsDiquarkHigh Energy Physics::ExperimentNuclear ExperimentMixing (physics)Physical Review D
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Prediction of NarrowN*andΛ*Resonances with Hidden Charm above 4 GeV

2010

Up to now, all established baryons can be ascribed into 3-quark (qqq) configurations [1], although some of them were suggested to be meson-baryon dynamically generated states [2–8] or states with large (qqqq¯ q) components [9–11]. A difficulty to pin down the nature of these baryon resonances is that the predicted states from various models are around the same energy region and there are always some adjustable ingredients in each model to fit the experimental data. In this letter, we report a study of the interactions between various charmed mesons and charmed baryons within the framework of the coupled channel unitary approach with the local hidden gauge formalism. Several meson-baryon dyn…

PhysicsQuarkParticle physicsMesonNuclear TheoryHigh Energy Physics::PhenomenologyHadronQuark modelGeneral Physics and AstronomyElementary particlePentaquarkCharmed baryonsBaryonHigh Energy Physics::ExperimentNuclear ExperimentPhysical Review Letters
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Spin, helicity and flavour patterns in exclusive decays of bottom mesons into baryon-antibaryon pairs

1989

I use the constituent quark model to calculate the exclusive decays of bottom mesons into ground state baryon-antibaryon pairs mediated by the weakb→c and b→u transitions. TheW-exchange contributions to these decays are found to be negligible. For theW-decay contributions I find that the simple colour-flavour structure of the 1/2+ and 3/2+ ground state baryons together with the current-current nonleptonic Hamiltonian leads to many simple and testable predictions. Notable among these is the predicted vanishing of decays involving 3/2+ baryons as in\(\overline {B^0 } (B^ - ) \to 3/2^ + \overline {1/2^ + } \) and\(\overline {B^0 } (B^ - ) \to 3/2^ + \overline {3/2^ + } \). An experimental veri…

PhysicsQuarkParticle physicsPhysics and Astronomy (miscellaneous)MesonNuclear TheoryHigh Energy Physics::PhenomenologyHyperonConstituent quarkHelicityNuclear physicsCharmed baryonsBaryonHigh Energy Physics::ExperimentNuclear ExperimentGround stateEngineering (miscellaneous)Zeitschrift für Physik C: Particles and Fields
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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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Faddeev study of heavy baryon spectroscopy

2007

16 pages, 3 figures.-- PACS nrs.: 12.39.Jh, 12.39.Pn, 14.20.-c.-- ISI Article Identifier: 000246249100015.-- ArXiv pre-print available at: http://arxiv.org/abs/hep-ph/0703257

QuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeNuclear TheoryConstituent quarkFOS: Physical sciencesPosition and momentum spaceBottom quarkHyperfine interactionsHigh Energy Physics - Phenomenology (hep-ph)ChromodynamicsSymmetry breakingCharm (quantum number)Nuclear ExperimentPhysicsCharmed baryonsNonrelativistic quark modelsHigh Energy Physics::PhenomenologyFísicaQuantum numberFlip-flop modelBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNucleon-nucleon interactionBaryon spectra
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