Search results for "Reaccions nuclears"

showing 10 items of 11 documents

Chiral unitary approach to eta'N scattering at low energies

2010

We study the \eta' N interaction within a chiral unitary approach which includes \pi N, \eta N and related pseudoscalar meson-baryon coupled channels. Since the SU(3) singlet does not contribute to the standard interaction and the \eta' is mostly a singlet, the resulting scattering amplitude is very small and inconsistent with experimental estimations of the \eta' N scattering length. The additional consideration of vector meson-baryon states into the coupled channel scheme, via normal and anomalous couplings of pseudoscalar to vector mesons, enhances substantially the \eta' N amplitude. We also exploit the freedom of adding to the Lagrangian a new term, allowed by the symmetries of QCD, wh…

Nuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryHigh Energy Physics::LatticeNuclear Theory01 natural sciencesQuantum mechanics0103 physical sciencesMesons (Nuclear physics)Mesons (Física nuclear)010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysicsUnitarityReaccions nuclears010308 nuclear & particles physicsScatteringHigh Energy Physics::PhenomenologyFísicaCromodinàmica quàntica Partícules (Física nuclear)Scattering lengthBaryonPseudoscalarScattering amplitudeHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNuclear reactionsQuantum chromodynamics
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Progress on nuclear reaction rates affecting the stellar production of 26Al

2023

Abstract The radioisotope 26Al is a key observable for nucleosynthesis in the Galaxy and the environment of the early Solar System. To properly interpret the large variety of astronomical and meteoritic data, it is crucial to understand both the nuclear reactions involved in the production of 26Al in the relevant stellar sites and the physics of such sites. These range from the winds of low- and intermediate-mass asymptotic giant branch stars; to massive and very massive stars, both their Wolf–Rayet winds and their final core-collapse supernovae (CCSN); and the ejecta from novae, the explosions that occur on the surface of a white dwarf accreting material from a stellar companion. Several r…

RadioisotopesRadioisotopeisotoopitNuclear and High Energy PhysicsIsòtops radioactiuscore-collapse supernovae (CCSN)tähdet:Física [Àrees temàtiques de la UPC]astrofysiikkaReaccions nuclears--TarifesnucleosynthesisNuclear reactions--Ratesnuclear reaction rateNuclear reaction rateydinreaktiotkääpiötähdetsupernovatradioisotope 26AlradioisotopealumiiniWolf-Rayet (WR) windsydinfysiikkaNucleosynthesisNucleosíntesi
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Critical review of [K- ppn] bound states

2008

We make a thorough study of the process of three body kaon absorption in nuclei, in connection with a recent FINUDA experiment which claims the existence of a deeply bound kaonic state from the observation of a peak in the Lambda d invariant mass distribution following K- absorption on Li6. We show that the peak is naturally explained in terms of K- absorption from three nucleons leaving the rest as spectators. We can also reproduce all the other observables measured in the same experiment and used to support the hypothesis of the deeply bound kaon state. Our study also reveals interesting aspects of kaon absorption in nuclei, a process that must be understood in order to make progress in t…

PhysicsNuclear and High Energy PhysicsParticle physicsReaccions nuclearsNuclear TheoryNuclear TheoryHyperonOrder (ring theory)FísicaFOS: Physical sciencesObservablePartícules (Física nuclear)Nuclear physicsNuclear Theory (nucl-th)Bound stateInvariant massAbsorption (logic)Nuclear reactionsConnection (algebraic framework)NucleonNuclear ExperimentParticles (Nuclear physics)
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Proton emission off nuclei induced by kaons in flight

2010

We study the (K-, p) reaction on nuclei with a 1 GeV/c momentum kaon beam, paying special attention to the region of emitted protons having kinetic energy above 600 MeV, which was used to claim a deeply attractive kaon nucleus optical potential. Our model describes the nuclear reaction in the framework of a local density approach and the calculations are performed following two different procedures: one is based on a many-body method using the Lindhard function and the other is based on a Monte Carlo simulation. The simulation method offers flexibility to account for processes other than kaon quasielastic scattering, such as K- absorption by one and two nucleons, producing hyperons, and all…

Nuclear reactionNuclear and High Energy PhysicsParticle physicsNuclear TheoryMesonHadronNuclear TheoryFOS: Physical sciencesElementary particle7. Clean energy01 natural sciencesNuclear Theory (nucl-th)MomentumNuclear physics0103 physical sciencesProton emission010306 general physicsNuclear ExperimentBosonPhysicsReaccions nuclears010308 nuclear & particles physicsSpecific reactions and phenomenologyFísicaFenomenologia (Física)High Energy Physics::ExperimentNuclear reactionsNucleon
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Atmospheric neutrino observations and flavor changing interactions

1999

Flavor changing (FC) neutrino-matter interactions can account for the zenith-angle dependent deficit of atmospheric neutrinos observed in the SuperKamiokande experiment, without directly invoking neither neutrino mass, nor mixing. We find that FC $\nu_\mu$-matter interactions provide a good fit to the observed zenith angle distributions, comparable in quality to the neutrino oscillation hypothesis. The required FC interactions arise naturally in many attractive extensions of the Standard Model.

PhysicsSterile neutrinoParticle physicsReaccions nuclearsSolar neutrinoAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyFísicaFOS: Physical sciencesSolar neutrino problemPartícules (Física nuclear)Standard ModelNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Measurements of neutrino speedHigh Energy Physics::ExperimentNuclear reactionsNeutrinoNeutrino oscillationZenithParticles (Nuclear physics)
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Does the Sun Shine byppor CNO Fusion Reactions?

2002

We show that solar neutrino experiments set an upper limit of 7.8% (7.3% including the recent KamLAND measurements) to the fraction of energy that the Sun produces via the CNO fusion cycle, which is an order of magnitude improvement upon the previous limit. New experiments are required to detect CNO neutrinos corresponding to the 1.5% of the solar luminosity that the standard solar model predicts is generated by the CNO cycle.

Astrophysics and AstronomyAstrofísica nuclearCNO cycleNuclear TheoryPhysics::Instrumentation and DetectorsSolar neutrinoSolar luminosityFOS: Physical sciencesGeneral Physics and AstronomyAstrophysicsAstrophysics7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesAstrophysics::Solar and Stellar AstrophysicsNuclear fusionNuclear Experiment (nucl-ex)010306 general physicsNeutrino oscillationNuclear ExperimentAstrophysics::Galaxy AstrophysicsPhysicsStandard solar modelReaccions nuclears010308 nuclear & particles physicsAstrophysics (astro-ph)FísicaHigh Energy Physics - PhenomenologyPhysics::Space PhysicsNuclear astrophysicsHigh Energy Physics::ExperimentNuclear reactionsNeutrinoOrder of magnitudePhysical Review Letters
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Neutron and proton spectra from the decay of Lambda hypernuclei

1996

We have determined the spectra of neutrons and protons following the decay of $\Lambda$ hypernuclei through the one- and two-nucleon induced mechanisms. The momentum distributions of the primary nucleons are calculated and a Monte Carlo simulation is used to account for final state interactions. From the spectra we calculate the number of neutrons ($N_n$) and protons ($N_p$) per $\Lambda$ decay and show how the measurement of these quantities, particularly $N_p$, can lead to a determination of $\Gamma_n / \Gamma_p$, the ratio of neutron to proton induced $\Lambda$ decay. We also show that the consideration of the two-nucleon induced channel has a repercussion in the results, widening the ba…

Monte Carlo methodEstructura nuclearNuclear TheoryReaccions nuclearsAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryFísicaNuclear structureNuclear reactionsMètode de MontecarloNuclear Experiment
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Covariant description of kinetic freeze out through a finite space-like layer

2005

The problem of Freeze Out (FO) in relativistic heavy ion reactions is addressed. We develop and analyze an idealized one-dimensional model of FO in a finite layer, based on the covariant FO probability. The resulting post FO phase-space distributions are discussed for different FO probabilities and layer thicknesses.

PhysicsNuclear and High Energy PhysicsNuclear TheoryReaccions nuclearsFOS: Physical sciencesKinetic energyThermodynamic modelNuclear Theory (nucl-th)Distribution (mathematics)Classical mechanicsCollisions (Nuclear physics)Phase spaceCol·lisions (Física nuclear)Covariant transformationNuclear reactionsLayer (object-oriented design)Nuclear ExperimentNuclear theoryMathematical physics
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The 33S(n,α)30Si cross section measurement at n TOF-EAR2 (CERN): From 0.01 eV to the resonance region

2017

The 33S(n,α)30Si cross section measurement, using 10B(n,α) as reference, at the n TOF Experimental Area 2 (EAR2) facility at CERN is presented. Data from 0.01 eV to 100 keV are provided and, for the first time, the cross section is measured in the range from 0.01 eV to 10 keV. These data may be used for a future evaluation of the cross section because present evaluations exhibit large discrepancies. The 33S(n,α)30Si reaction is of interest in medical physics because of its possible use as a cooperative target to boron in Neutron Capture Therapy (NCT).

Nuclear reactionnTOFNeutron therapyQC1-999chemistry.chemical_elementNeutron01 natural sciencesResonance (particle physics)Nuclear physicsCross section (physics)Physics and Astronomy (all)0103 physical sciencesCERNNeutronddc:530010306 general physicsBoronPhysicsNeutrons:Energies::Energia nuclear [Àrees temàtiques de la UPC]Range (particle radiation)Large Hadron Collidercross sectionReaccions nuclears:Física [Àrees temàtiques de la UPC]010308 nuclear & particles physicsPhysicsNuclear reactionNeutron capturechemistryNuclear reactions
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The 236U neutron capture cross-section measured at the n TOF CERN facility

2016

International audience; The $^{236}$U isotope plays an important role in nuclear systems, both for future and currently operating ones. The actual knowledge of the capture reaction of this isotope is satisfactory in the thermal region, but it is considered insufficient for Fast Reactor and ADS applications. For this reason the $^{236} \text{U}(n, \gamma)$ reaction cross-section has been measured for the first time in the whole energy region from thermal energy up to 1 MeV at the n_TOF facility with two different detection systems: an array of C$_6$D$_6$ detectors, employing the total energy deposited method, and a 4$\pi$ total absorption calorimeter (TAC), made of 40 BaF$_2$ crystals. The t…

Nuclear reactionnTOFQC1-999Neutron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyNuclear physicsPhysics and Astronomy (all)Cross section (physics)0103 physical sciencesCERNNeutron cross sectionNuclear Physics - Experimentddc:530Neutron010306 general physicsAbsorption (electromagnetic radiation)PhysicsNeutrons:Energies::Energia nuclear [Àrees temàtiques de la UPC]IsotopeCross sectionReaccions nuclears:Física [Àrees temàtiques de la UPC]010308 nuclear & particles physicsPhysicsResonanceNuclear reactionCalorimeter13. Climate actionNuclear reactions
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