Search results for "hyperon"

showing 10 items of 118 documents

Role of correlated two-pion exchange in $K^+ N$ scattering

1995

A dynamical model for S-- and P--wave correlated $2 \pi$ (and $K \bar K$) exchange between a kaon and a nucleon is presented, starting from corresponding $N \bar N \rightarrow K \bar K$ amplitudes in the pseudophysical region, which have been constructed from nucleon, $\Delta$--isobar and hyperon ($\Lambda$, $\Sigma$) exchange Born terms and a realistic meson exchange model of the $\pi \pi \rightarrow K \bar K$ and $K \bar K \rightarrow K \bar K$ amplitude. The contribution in the s--channel is then obtained by performing a dispersion relation over the unitarity cut. In the $\rho$--channel, considerable ambiguities exist, depending on how the dispersion integral is performed. Our model, sup…

PhysicsNuclear and High Energy PhysicsParticle physicsUnitarityMesonNuclear TheoryNuclear TheoryHigh Energy Physics::PhenomenologyHyperonFOS: Physical sciencesNuclear Theory (nucl-th)PionDispersion relationProduction (computer science)High Energy Physics::ExperimentNucleonNuclear ExperimentBar (unit)
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Hyperons, Charm and Beauty Hadrons: Conclusion and Outlook

2001

In this concluding talk, the advances in the Flavour Problem studies are discussed, following the structure of the presentations in the Conference. The subjects touched are organized as follows: Baryons, K-physics, Charm and Beauty production, Charm and Beauty decays, B-Mixing and CP-Violation, Heavy Quarkonium.

PhysicsNuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectHadronFlavourHyperonFísicaFOS: Physical sciencesQuarkoniumAtomic and Molecular Physics and OpticsBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)BeautyCharm (quantum number)media_common
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Heavy-to-light semileptonic decays ofΛbandΛcbaryons in the covariant confined quark model

2014

We present a detailed analysis of the heavy-to-light semileptonic decays of theb andc baryons �b → pl ¯ νl andc → nl + νl in the covariant confined quark model. We calculate the invariant and helicity amplitudes of the two processes which are then used to analyze their angular decay distributions, their rates and asymmetry parameters.

PhysicsNuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyQuark modelHyperonHelicityAsymmetryBaryonAmplitudeHigh Energy Physics::ExperimentCovariant transformationInvariant (mathematics)media_commonPhysical Review D
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Measurement of theγp→K0Σ+reaction with the Crystal Ball/TAPS detectors at the Mainz Microtron

2013

The gamma p -> K-0 Sigma(+) reaction has been measured from threshold to E-gamma = 1.45 GeV (W-CM = 1.9 GeV) using the Crystal Ball and TAPS multiphoton spectrometers together with the photon tagging facility at the Mainz Microtron MAMI. In the present experiment, this reaction was searched for in the 3 pi(0)p final state, by assuming K-S(0) -> pi(0)pi(0) and Sigma(+) -> pi(0)p. The experimental results include total and differential cross sections as well as the polarization of the recoil hyperon. The new data significantly improve empirical knowledge about the gamma p -> K-0 Sigma(+) reaction in the measured energy range. The results are compared to previous measurements and model predict…

PhysicsNuclear and High Energy PhysicsPhotonSpectrometerProton010308 nuclear & particles physicsHyperonSigma01 natural sciencesNuclear physicsRecoil0103 physical sciences010306 general physicsMicrotronCrystal BallPhysical Review C
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Production of Θ+ hypernuclei with the (K+,π+) reaction

2005

Abstract We present results on the production of bound states of Θ + in nuclei using the ( K + , π + ) reaction. By taking into account the states obtained within a wide range of strength of the Θ + nucleus optical potential, plus the possibility to replace different nucleons of the nucleus, we obtain an excitation spectra with clearly differentiated peaks. The magnitude of the calculated cross sections is well within reachable range.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Nuclear TheoryHyperonOptical potentialmedicine.anatomical_structureExotic baryonBound statemedicineProduction (computer science)Atomic physicsNuclear ExperimentNucleonNucleusPhysics Letters B
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A study of strange particle production in nu(mu) charged current interactions in the NOMAD experiment

2001

A study of strange particle production in $\nu_\mu$ charged current interactions has been performed using the data from the NOMAD experiment. Yields of neutral strange particles ($K^0_s, \Lambda, \bar{\Lambda}$) have been measured. Mean multiplicities are reported as a function of the event kinematic variables $E_\nu$, $W^2$ and $Q^2$ as well as of the variables describing particle behaviour within a hadronic jet: $x_F$, $z$ and $p_T^2$. Decays of resonances and heavy hyperons with identified $K^0_s$ and $\Lambda$ in the final state have been analyzed. Clear signals corresponding to $\rm {K^\star}^\pm$ $\rm {\Sigma^\star}^\pm$, $\rm \Xi^-$ and $\rm \Sigma^0$ have been observed. A study of s…

PhysicsNuclear and High Energy PhysicsStrange quarkParticle physics010308 nuclear & particles physicsStar (game theory)HadronHyperonFísicaLambda01 natural sciencesNuclear physics0103 physical sciencesneutrino interactions; strange particle productionProduction (computer science)High Energy Physics::ExperimentNeutrino010306 general physicsNuclear ExperimentCharged currentParticle Physics - Experiment
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Low lying S=-1 excited baryons and chiral symmetry

2001

The s-wave meson-baryon interaction in the $S = -1$ sector is studied by means of coupled-channels, using the lowest-order chiral Lagrangian and the N/D method to implement unitarity. The loops are regularized using dimensional renormalization. In addition to the previously studied $\Lambda (1405)$, employing this chiral approach leads to the dynamical generation of two more s-wave hyperon resonances, the $\Lambda(1670)$ and $\Sigma(1620)$ states. We make comparisons with experimental data and look for poles in the complex plane obtaining the couplings of the resonances to the different final states. This allows us to identify the $\Lambda (1405)$ and the $\Lambda(1670)$ resonances with $\b…

PhysicsNuclear and High Energy PhysicsUnitarityNuclear TheoryHigh Energy Physics::PhenomenologyHyperonFísicaSigmaFOS: Physical sciencesLambdaBaryonRenormalizationNuclear Theory (nucl-th)Excited stateComplex planeMathematical physics
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Hyperon Semileptonic Decays and CKM Unitarity

2005

We perform a new numerical analysis of hyperon semileptonic decays emphasizing the systematic uncertainties. The poor understanding of SU(3) symmetry breaking effects at second order in the vector form factor translates into a large error of |V(us)|. Using our determination |V(us)| = 0.226 +/- 0.005 together with those coming from other sources we test the unitarity of the CKM matrix.

PhysicsNuclear physicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)UnitarityCabibbo–Kobayashi–Maskawa matrixHyperonForm factor (quantum field theory)FOS: Physical sciencesSymmetry breakingAtomic and Molecular Physics and Optics
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New results on hyperon decays from NA48

2001

In 1999 the NA48 experiment at CERN had two short data taking periods (8h and 40h) with a high intensity KS beam. Together with the KS mesons a large number of neutral hyperons, e.g. Λ and Ξ0, are produced. During these periods a large sample of Ξ0 decays was collected. About 115,000 events of the decay mode Ξ0 → Λπ0, about 500 of Ξ0 → Λγ, about 400 of Ξ0 → Σ0γ and about 60 events of Ξ0 → Σ+ e have been reconstructed. The status of the analyses of the above decay modes is presented.

PhysicsNuclear physicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderMesonHyperonNA48 experimentAtomic and Molecular Physics and OpticsBeam (structure)Large sampleNuclear Physics B - Proceedings Supplements
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Studies of Hyperons and Antihyperons in Nuclei

2010

Stored antiproton beams at the international FAIR facility will provide unique opportunities to study hyperons as well as antihyperons in nuclear systems. Precise γ-spectroscopy of multistrange hypernuclei will serve as a laboratory for the hyperon-hyperon interaction. Exclusive hadron-antihadron pair production close to threshold can measure the potential of a antihadron relative to that of the coincident hadrons. In the present work we explore the production of excited states in double hypernuclei following the micro-canonical break-up of an initially excited double hypernucleus which is created by the absorption and conversion of a stopped Ξ− hyperon. Generally the formation of excited h…

PhysicsNuclear physicsPionPair productionMesonAntiprotonExcited stateNuclear TheoryHadronHyperonHigh Energy Physics::ExperimentNuclear ExperimentHypernucleusProceedings of XLVIII International Winter Meeting on Nuclear Physics in Memoriam of Ileana Iori — PoS(BORMIO2010)
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