0000000001002736

AUTHOR

Tetsuo Hyodo

showing 15 related works from this author

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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Theoretical study of the Ξ(1620) and Ξ(1690) resonances in Ξc→π+MB decays

2017

Nonleptonic weak decays of ${\mathrm{\ensuremath{\Xi}}}_{c}$ into ${\ensuremath{\pi}}^{+}$ and a meson $(M)$-baryon $(B)$ final state, $MB$, are analyzed from the viewpoint of probing $S=\ensuremath{-}2$ baryon resonances, i.e., $\mathrm{\ensuremath{\Xi}}(1620)$ and $\mathrm{\ensuremath{\Xi}}(1690)$, of which spin-parity and other properties are not well known. We argue that the weak decay of ${\mathrm{\ensuremath{\Xi}}}_{c}$ is dominated by a single quark-line diagram, preferred by the Cabibbo-Kobayashi-Maskawa coefficient, color recombination factor, the diquark correlation, and the kinematical condition. The decay process has an advantage of being free from meson resonances in the ${\ens…

PhysicsParticle physicsUnitarityMeson010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyResonanceState (functional analysis)Lambda01 natural sciencesBaryonDiquark0103 physical sciencesInvariant mass010306 general physicsPhysical Review C
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Λ(1405)production in theπ−p→K0πΣreaction

2003

We discuss the mechanisms that lead to $\ensuremath{\Lambda}(1405)$ production in the ${\ensuremath{\pi}}^{\ensuremath{-}}p\ensuremath{\rightarrow}{K}^{0}\ensuremath{\pi}\ensuremath{\Sigma}$ reaction. The problem has gained renewed interest after different works converge to the conclusion that there are two resonances around the region of $1400\phantom{\rule{0.3em}{0ex}}\text{MeV}$, rather than one, and that they couple differently to the $\ensuremath{\pi}\ensuremath{\Sigma}$ and $\overline{K}N$ channels. We look at the dynamics of that reaction and find two mechanisms which eventually filter each one of the resonances, leading to very different shapes of the $\ensuremath{\pi}\ensuremath{\S…

PhysicsNuclear and High Energy PhysicsDistribution (mathematics)FactorizationUnitarityQuantum mechanicsHyperonSigmaProduction (computer science)Invariant massLambdaMathematical physicsPhysical Review C
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Two-meson cloud contribution to the baryon antidecuplet self-energy

2005

We study the self-energy of the SU(3) antidecuplet coming from two-meson virtual clouds. Assuming that the exotic Theta+ belongs to an antidecuplet representation with N(1710) as nucleon partner, we derive effective Lagrangians that describe the decay of N(1710) into N pi pi with two pions in s- or p-wave. It is found that the self-energies for all members of the antidecuplet are attractive, and the larger strangeness particle is more bound. From two-meson cloud, we obtain about 20 % of the empirical mass splitting between states with different strangeness.

PhysicsNuclear and High Energy PhysicsParticle physicsMesonNuclear Theorybusiness.industryNuclear TheoryFOS: Physical sciencesFísicaCloud computingStrangenessBaryonNuclear physicsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)Self-energyNucleonbusinessNuclear ExperimentNuclear theory
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A narrow quasi-bound state of the DNN system

2013

Abstract We have investigated a charmed system of DNN (composed of two nucleons and a D meson) by a complementary study with a variational calculation and a Faddeev calculation with fixed-center approximation (Faddeev-FCA). In the present study, we employ a DN potential based on a vector–meson exchange picture in which a resonant Λ c ( 2595 ) is dynamically generated as a DN quasi-bound state, similarly to the Λ ( 1405 ) as a K ¯ N one in the strange sector. As a result of the study of variational calculation with an effective DN potential and three kinds of NN potentials, the D N N ( J π = 0 − , I = 1 / 2 ) is found to be a narrow quasi-bound state below Λ c ( 2595 ) N threshold: total bin…

PhysicsNuclear and High Energy PhysicsScatteringNuclear TheoryBinding energyD mesonBound stateCenter (category theory)State (functional analysis)Atomic physicsNuclear ExperimentWave functionNucleonNuclear Physics A
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Two-meson cloud contribution to the baryon antidecuplet binding

2004

We study the two-meson virtual cloud contribution to the self-energy of the SU(3) antidecuplet, to which the Theta+ pentaquark is assumed to belong. This is motivated by the large branching ratio of the N(1710) decay into two pions and one nucleon. We derive effective Lagrangians that describe the N(1710) decay into N-pi-pi with two pions in s or p wave. We obtain increased binding for all members of the antidecuplet and a contribution to the mass splitting between states with different strangeness which is at least 20 % of the empirical one. We also provide predictions for three-body decays of the pentaquark antidecuplet.

PhysicsNuclear and High Energy PhysicsParticle physicsMesonBranching fractionHigh Energy Physics::LatticeNuclear TheoryQuark modelFOS: Physical sciencesFísicaStrangenessPentaquarkNuclear physicsBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PionHigh Energy Physics::ExperimentNuclear ExperimentNucleonPhysical Review C
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Two-, Three-, Many-body Systems Involving Mesons. Multimeson Condensates

2015

In this talk we review results from studies with unconventional many hadron systems containing mesons: systems with two mesons and one baryon, three mesons, some novel systems with two baryons and one meson, and finally systems with many vector mesons, up to six, with their spins aligned forming states of increasing spin. We show that in many cases one has experimental counterparts for the states found, while in some other cases they remain as predictions, which we suggest to be searched in BESIII, Belle, LHCb, FAIR and other facilities.

PhysicsParticle physicsNuclear TheoryMesonSpins010308 nuclear & particles physicsHadronHigh Energy Physics::PhenomenologyNuclear TheoryGeneral Physics and AstronomyFOS: Physical sciences01 natural sciencesMany bodyBaryonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesMathematics::Metric GeometryHigh Energy Physics::Experiment010306 general physicsNuclear ExperimentSpin-½Acta Physica Polonica B
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Antikaon-nucleon interaction and Lambda(1405) in chiral SU(3) dynamics

2016

The properties of the Lambda(1405) resonance are key ingredients for determining the antikaon-nucleon interaction in strangeness nuclear physics, and the novel internal structure of the Lambda(1405) is of great interest in hadron physics, as a prototype case of a baryon that does not fit into the simple three-quark picture. We show that a quantitative description of the antikaon-nucleon interaction with the Lambda(1405) is achieved in the framework of chiral SU(3) dynamics, with the help of recent experimental progress. Further constraints on the Kbar N subthreshold interaction are provided by analyzing pi Sigma spectra in various processes, such as the K-d -> pi Sigma n reaction and the…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theory010308 nuclear & particles physicsHadronNuclear TheoryFOS: Physical sciencesMolecular configurationStrangeness16. Peace & justice01 natural sciencesResonance (particle physics)Spectral lineBaryonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNucleonWave functionNuclear Experiment
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Determining the Θ+ quantum numbers through the K+p→π+K+n reaction

2004

Abstract We study the K+p→π+K+n reaction with some kinematics suited to the production of the Θ+ resonance recently observed. We show that, independently of the quantum numbers of the Θ+, a resonance signal is always observed in the K+ forward direction. In addition, we also show how a combined consideration of the strength at the peak, and the angular dependence of polarization observables can help determine the Θ+ quantum numbers using the present reaction.

PhysicsNuclear and High Energy PhysicsPolarization observablesFísicaΘ+ baryonPolarization (waves)Quantum numberBaryonSpin parity determinationQuantum mechanicsAngular dependenceResonance signalAtomic physicsNuclear theoryPhysics Letters B
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First study of the two-body scattering involving charm hadrons

2022

Physical review / D 106(5), 052010 (2022). doi:10.1103/PhysRevD.106.052010

:Kjerne- og elementærpartikkelfysikk: 431 [VDP]charmed mesoncorrelation [momentum]heavy flavourhiukkasfysiikkaHigh Energy Physics - ExperimentnukleonitHigh Energy Physics - Experiment (hep-ex)ALICENucleon-scatteringscattering [p p][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]BaryonsCollisionsNuclear Experiment (nucl-ex)EXCHANGENuclear ExperimentNuclear ExperimentBARYONSMesonscharm hadronsstrong interactionnucleonVDP::Kjerne- og elementærpartikkelfysikk: 431MESONSexperimental results ; pp: scattering ; momentum: correlation ; nucleon ; isospin ; charmed meson ; D- ; D+ ; strong interaction ; ALICE ; scattering length ; correlation: two-particle ; Coulomb:Nuclear and elementary particle physics: 431 [VDP]PARTIAL-WAVE ANALYSISVDP::Nuclear and elementary particle physics: 431D+D-Particle Physics - ExperimentHeavy-ion physics heavy flavour charm hadronscorrelation: two-particleCOLLISIONSp p: scatteringNuclear and High Energy PhysicsFOS: Physical sciencesPARTIAL-WAVE ANALYSIS; NUCLEON-SCATTERING; COLLISIONS; EXCHANGE; BARYONS; MESONS[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]530114 Physical sciencesheavy-ion physics; charm; heavy flavourNUCLEON-SCATTERINGisospinHeavy Ion ExperimentsPartial-wave analysisNuclear Physics - Experimentsirontaddc:530two-particle [correlation]Nuclear PhysicsHigh Energy Physics::Phenomenologymomentum: correlationExchangeHeavy-ion physicsscattering lengthCoulombcharmexperimental results
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Weak decay ofΛc+for the study ofΛ(1405)andΛ(1670)

2015

We study the ${\mathrm{\ensuremath{\Lambda}}}_{c}$ decay process to ${\ensuremath{\pi}}^{+}$ and the meson-baryon final state for the analysis of $\mathrm{\ensuremath{\Lambda}}$ resonances. Considering the Cabibbo-Kobayashi-Maskawa matrix, color suppression, diquark correlation, and the kinematical condition, we show that the final meson-baryon state should be in a pure $I=0$ combination, when the meson-baryon invariant mass is small. Because the $I=1$ contamination usually makes it difficult to analyze $\mathrm{\ensuremath{\Lambda}}$ resonances directly from experiments, the ${\mathrm{\ensuremath{\Lambda}}}_{c}$ decay is an ideal process to study $\mathrm{\ensuremath{\Lambda}}$ resonances.…

BaryonPhysicsNuclear and High Energy PhysicsParticle physicsUnitarityCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyHigh Energy Physics::ExperimentInvariant massCharge (physics)Ideal (ring theory)Lambda baryonLambdaPhysical Review C
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The nature of Lambda (1405) hyperon resonance in chiral dynamics

2010

10th International Conference on Hypernuclear and Strange Particle Physics. Tokai, JAPAN, SEP 14-18, 2009

CouplingPhysicsNuclear and High Energy PhysicsParticle physicsKaon induced Lambda (1405) productionNuclear TheoryScatteringHadronSpectrum (functional analysis)HyperonStructure of Lambda (1405)FOS: Physical sciencesFísicaResonance (particle physics)Spectral lineNuclear Theory (nucl-th)K(K)over-barN quasibound stateChiral unitary modelHigh Energy Physics::ExperimentInvariant massAtomic physics
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Energy and width of a narrowI=1/2DNNquasibound state

2012

The energies and widths of $DNN$ quasi-bound states with isospin I=1/2 are evaluated in two methods, the fixed center approximation to the Faddeev equation and the variational method approach to the effective one-channel Hamiltonian. The $DN$ interactions are constructed so that they dynamically generate the $\Lambda_c(2595)$ (I=0, $J^{\pi} =1/2^-$) resonance state. We find that the system is bound by about 250 MeV from the $DNN$ threshold, $\sqrt{s} \sim 3500$ MeV. Its width including both the mesonic decay and the $D$ absorption, is estimated to be about 20-40 MeV. The I=0 $DN$ pair in the $DNN$ system is found to form a cluster that is similar to the $\Lambda_c(2595)$.

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsNuclear TheoryFew-body systemsLambda01 natural sciencessymbols.namesakeVariational methodQuantum mechanicsIsospin0103 physical sciencessymbolsAtomic physicsNuclear Experiment010306 general physicsHamiltonian (quantum mechanics)Nuclear theoryPhysical Review C
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Narrow Bound States of the DNN System

2012

We report on a recent calculation of the properties of the $DNN$ system, a charmed meson with two nucleons. The system is analogous to the $\bar K NN$ system substituting a strange quark by a charm quark. Two different methods are used to evaluate the binding and width, the Fixed Center approximation to the Faddeev equations and a variational calculation. In both methods we find that the system is bound by about 200 MeV and the width is smaller than 40 MeV, a situation opposite to the one of the $\bar K NN$ system and which makes this state well suited for experimental observation.

Strange quarkFaddeev equationsParticle physicsMesonNuclear TheoryBar (music)Nuclear TheoryFOS: Physical sciences01 natural sciencesCharm quarkNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesBound stateNuclear Experiment010303 astronomy & astrophysicsPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaState (functional analysis)16. Peace & justiceAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNucleon
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Photoproduction of K∗ for the study of Λ(1405)

2004

Abstract The photo-induced K ∗ vector meson production is investigated for the study of the Λ(1405) resonance. This reaction is particularly suited to the isolation of the second pole in the Λ(1405) region which couples dominantly to the K N channel. We obtain the mass distribution of the Λ(1405) which peaks at 1420 MeV, and differs from the nominal one. Combined with several other reactions, like the π−p→K0πΣ which favours the first pole, this detailed study will reveal a novel structure of the Λ(1405) state.

PhysicsNuclear and High Energy PhysicsMesonMass distributionElementary particleLambda baryonResonance (particle physics)Nuclear physicsPionChiral unitary approachMass spectrumVector mesonAtomic physicsΛ(1405)Physics Letters B
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