Search results for "Strangeness production"

showing 9 items of 9 documents

Formation Of Hypernuclei In Evaporation And Fission Processes

2016

There are excellent opportunities to produce excited heavy hyper residues in relativistic hadron and peripheral heavy-ion collisions. We investigate the disintegration of such residues into hyper nuclei via evaporation of baryons and light clusters and their fission. Previously these processes were well known for normal nuclei as the decay channels at low excitation energies. We have generalized these models for the case of hyper-matter. In this way we make extension of nuclear reaction studies at low temperature into the strange sector. We demonstrate how the new decay channels can be integrated in the whole disintegration process. Their importance for mass and isotope distributions of pro…

Nuclear reactionPhysicsParticle physicsNuclear TheoryIsotope010308 nuclear & particles physicsFissionHadronNuclear TheoryHyperonStrangeness productionFOS: Physical sciencesNuclear matter01 natural sciencesNuclear physicsBaryonNuclear Theory (nucl-th)0103 physical sciences010306 general physicsNuclear Experiment
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Formation of hypernuclei in heavy-ion collisions around the threshold energies

2016

In relativistic ion collisions there are excellent opportunities to produce and investigate hyper-nuclei. We have systematically studied the formation of hypernuclear spectator residues in peripheral heavy-ion collisions with the transport DCM and UrQMD models. The hyperon capture was calculated within the potential and coalescence approaches. We demonstrate that even at the beam energies around and lower than the threshold for producing Lambda hyperons in binary nucleon-nucleon interactions a considerable amount of hypernuclei, including multi-strange ones, can be produced. This is important for preparation of new experiments on hypernuclei in the wide energy range. The uncertainties of th…

Particle physicsNuclear TheoryNuclear TheoryFOS: Physical sciencesBinary numberLambda01 natural sciencesIonHigh Energy Physics - ExperimentNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear theoryNuclear ExperimentPhysicsCoalescence (physics)010308 nuclear & particles physicsHyperonStrangeness productionHigh Energy Physics - PhenomenologyHeavy ion
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Multiplicity dependence of K*(892)0 and ϕ(1020) production in pp collisions at s=13 TeV

2020

The striking similarities that have been observed between high-multiplicity proton-proton (pp) collisions and heavy-ion collisions can be explored through multiplicity-differential measurements of identified hadrons in pp collisions. With these measurements, it is possible to study mechanisms such as collective flow that determine the shapes of hadron transverse momentum ( pT ) spectra, to search for possible modifications of the yields of short-lived hadronic resonances due to scattering effects in an extended hadron-gas phase, and to investigate different explanations provided by phenomenological models for enhancement of strangeness production with increasing multiplicity. In this paper,…

PhysicsNuclear and High Energy PhysicsMeson010308 nuclear & particles physicsScatteringNuclear TheoryHadronStrangeness productionStrangeness01 natural sciencesSpectral lineNuclear physicsPion0103 physical sciencesMultiplicity (chemistry)Nuclear Experiment010306 general physicsPhysics Letters B
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Do p annihilations at rest choose the Eightfold way?

1993

Dynamical selection rules observed in pp annihilation at rest are linked to relations between SU(3) invariant amplitudes. The ϱπ puzzle, the KK suppression in P wave, and the unexplained production rates of πa2 (1320) are shown to be manifestions of one SU(3) amplitude ratio. The dynamical selection rules observed in the production of strange mesons lead to symmetries in SU(3) amplitudes. We conjecture that these symmetries reflect the underlying quark-gluon dynamic. It is shown that the contribution of annihilation diagrams to important annihilation channels like ϱ0π0 or ηω is small or vanishes. Hence rearrangement must play an important role. The use of SU(3) relations in the context of N…

PhysicsNuclear and High Energy PhysicsParticle physicsAnnihilationAmplitudeMesonBranching fractionEightfold WayHomogeneous spaceStrangeness productionInvariant (physics)Physics Letters B
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Antistrange meson-baryon interaction in hot and dense nuclear matter

2014

We present a study of in-medium cross sections and (off-shell) transition rates for the most relevant binary reactions for strange pseudoscalar meson production close to threshold in heavy-ion collisions at FAIR energies. Our results rely on a chiral unitary approach in coupled channels which incorporates the $s$- and $p$-waves of the kaon-nucleon interaction. The formalism, which is modified in the hot and dense medium to account for Pauli blocking effects, mean-field binding on baryons, and pion and kaon self-energies, has been improved to implement full unitarization and self-consistency for both the $s$- and $p$-wave interactions at finite temperature and density. This gives access to i…

PhysicsNuclear and High Energy PhysicsParticle physicsMesonNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Nuclear TheoryHyperonFOS: Physical sciencesStrangeness productionStrangenessNuclear matterPseudoscalar meson3. Good healthNuclear Theory (nucl-th)Nuclear physicsBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Pion[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Nuclear Experiment
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Prospects for hypernuclear physics at Mainz: From KAOS@MAMI to PANDA@FAIR

2013

Abstract At the Mainz Microtron hypernuclei are produced by ( e , e ′ K ) reactions. A dedicated kaon spectrometer located at 0° with respect to the electron beam is used to detect kaons emitted in forward direction thus tagging events involving strangeness production. By measuring the momenta of pions from two body weak decays using high resolution magnetic spectrometers one gains direct access to the ground state masses of the produced hyperfragments. At FAIR the PANDA Collaboration intends to produce double-hypernuclei by numbers with an antiproton beam and study their high resolution γ -spectroscopy thus providing for the first time precise information on the level structure of these nu…

PhysicsNuclear and High Energy PhysicsParticle physicsSpectrometerNuclear TheoryStrangeness productionHypernucleusNuclear physicsPionAntiproton beamhypernuclei; weak decay; spectroscopyKAOSGround stateNuclear ExperimentMicrotron
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Progress and open questions in the physics of neutrino cross sections at intermediate energies

2014

New and more precise measurements of neutrino cross sections have renewed the interest in a better understanding of electroweak interactions on nucleons and nuclei. This effort is crucial to achieve the precision goals of the neutrino oscillation program, making new discoveries, like the CP violation in the leptonic sector, possible. We review the recent progress in the physics of neutrino cross sections, putting emphasis on the open questions that arise in the comparison with new experimental data. Following an overview of recent neutrino experiments and future plans, we present some details about the theoretical development in the description of (anti)neutrino-induced quasielastic scatter…

PhysicsParticle physics010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::PhenomenologyNuclear TheoryGeneral Physics and AstronomyStrangeness productionFísica01 natural sciences7. Clean energyPion0103 physical sciencesCP violationHigh Energy Physics::ExperimentNeutrino010306 general physicsNucleonNeutrino oscillationNuclear ExperimentEvent (particle physics)
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Kaon Tagging at 0° Scattering Angle for High-Resolution Decay-Pion Spectroscopy

2014

At the Mainz Microtron hypernuclei can be studied by (e,e'K) reactions. By detecting the kaon which is emitted in forward direction, with the KAOS spectrometer placed at 0 scattering angle, reactions involving open strangeness production are tagged. High-resolution magnetic spectrometers are then used to coincidentally detect the mono- energetic decay-pions from mesonic two-body weak decays of light hypernuclei at rest. As a pioneering experiment has confirmed, the KAOS spectrometer is exposed to a large flux of background particles, mostly positrons from bremsstrahlung pair production. In order to increase the e ciency of kaon identification the KAOS spectrometer was modi- fied to suppress…

PhysicsParticle physicsSpectrometerScatteringPhysicsQC1-999Nuclear TheoryBremsstrahlungStrangeness productionNuclear physicsMomentumPionPair productionElectron Scattering; Hypernuclei; MAMI; KAOS; Decay-Pion SpectroscopyHigh Energy Physics::ExperimentNuclear ExperimentMicrotronEPJ Web of Conferences
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Strangeness production inp�p annihilation at rest and the quark ? diquark structure of nucleons

1988

The importance of approximate isospin selection rules observed inN¯ N annihilation at rest into two strange mesons is emphasized. The selection rules are traced back to a symmetry between amplitudes describing annihilation by the flux of quarks. Presumably the symmetry reflects the symmetry of ¯qq annihilation vertices. The relation of the symmetry to a quark — diquark substructure of the nucleon is discussed.

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsAnnihilationMesonHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryStrangeness productionSymmetry (physics)Nuclear physicsDiquarkIsospinHigh Energy Physics::ExperimentNuclear ExperimentNucleonZeitschrift f�r Physik A Atomic Nuclei
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