Search results for "Proton"

showing 10 items of 5886 documents

Single-neutron orbits near 78 Ni: Spectroscopy of theN=49isotope 79 Zn

2015

Single-neutron states in the Z=30, N=49isotope 79Zn have been populated using the 78Zn(d,p)79Zn transfer reaction at REX-ISOLDE, CERN. The experimental setup allowed the combined detection of protons ejected in the reaction, and of γrays emitted by 79Zn. The analysis reveals that the lowest excited states populated in the reaction lie at approximately 1MeV of excitation, and involve neutron orbits above the N=50shell gap. From the analysis of γ-ray data and of proton angular distributions, characteristic of the amount of angular momentum transferred, a5/2+configuration was assigned to a state at 983keV. Comparison with large-scale-shell-model calculations supports a robust neutron N=50shell…

Nuclear reactionNuclear and High Energy PhysicsAngular momentumProtonAstrophysics::High Energy Astrophysical PhenomenaNuclear Theorygamma-Ray transitions[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesTransfer reactions0103 physical sciencesNuclear Physics - ExperimentNeutronNuclear structureNuclear Experiment010306 general physicsSpectroscopyComputingMilieux_MISCELLANEOUSN=50 shell closure[PHYS]Physics [physics]PhysicsElastic scatteringNUCLEIRICH ISOTOPES010308 nuclear & particles physicslcsh:QC1-999ELASTIC-SCATTERINGExcited stateAtomic physicsγ-Ray transitionsNucleonlcsh:PhysicsPhysics Letters B
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Fast and nonselective on-line mass separation of neutron-rich isotopes produced in proton-induced fission

1989

Abstract On-line mass separation of short-lived radionuclides, based on the use of thermalized primary ions from nuclear reactions, termed as an ion guide method, has recently been widely applied in the spectroscopy of both proton-rich and neutron-rich exotic nuclei. The technique has been found to be applicable to all elements and it has allowed the detection of the mass-analyzed activities with half-lives as short as 0.1 ms. The ion guide isotope separator on-line, IGISOL, has recently been used to discover over ten new short-lived isotopes or isomers produced in the nearly symmetric fission of uranium induced by 20 MeV protons. In addition to applications in nuclear-structure physics and…

Nuclear reactionNuclear and High Energy PhysicsIsotopeProtonFissionChemistryNuclear Theorychemistry.chemical_elementUraniumIonNuclear physicsIonizationNeutronNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Study of Proton and 3He Induced Reactions on 235U at Low Energies

2014

Abstract Highly enriched 235 U targets were irradiated with 6.5 − 16.1 MeV protons and 20.4 − 42.0 MeV 3 He ions. The irradiated targets were measured with γ and α spectrometric methods to identify and quantify the produced reaction products. After primary activity measurements the targets were dissolved, and interesting Pu and Np reaction products were chemically separated from the target material, and measured for activity again. From the activity results it was possible to calculate the reaction cross sections for differently produced nuclides. The data obtained from the experiment resulted in earlier unknown excitation functions on proton and 3 He induced nuclear reactions on 235 U.

Nuclear reactionNuclear and High Energy PhysicsMaterials scienceProtonta114010308 nuclear & particles physicsRadiochemistryNuclear data7. Clean energy01 natural sciencesIonNuclear physicsActivity measurements0103 physical sciencesNuclideIrradiationAtomic physics010306 general physicsExcitationta119ta217Nuclear Data Sheets
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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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Probing the limit of nuclear existence: Proton emission from 159Re

2006

WOS: 000240847400007

Nuclear reactionNuclear and High Energy PhysicsSi detectorsProtonNuclear Theory[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]measured E (p) (t)1 / 201 natural sciences7. Clean energyNuclear physicsEp0103 physical sciencesEnriched targetsNeutronNuclideProton emissionNuclear Experiment010306 general physics106Cd at 300 MeV beam energyPhysicsIsotope010308 nuclear & particles physics21.10.Hw; 21.10.Tg; 23.50.+z; 27.70.+q58Nit1/2NUCLEAR REACTIONS Ni-58+Cd-106 at 300 MeV beam energy13. Climate actionNuclear reactionsGas-filled recoil separatorAtomic physicsNucleonMeasuredRadioactive decayPhysics Letters B
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Beta-decay strength and isospin mixing studies in the sd and fp-shells

1998

We have studied beta decays of MT<0 nuclei in sd and fp shells. The decay of 41Ti shows a large, 10(8) %, isospin mixing of IAS and the Gamow-Teller strength is observed to be quenched by a factor of q2=0.64. These results can be reproduced qualitatively in our shell model calculations. We have observed for the first time proton and gamma decay of the isobaric analogue state in 23Mg. Our results on the isospin mixing of the isobaric analogue state agrees well with the shell model calculations. The obtained proton branch of the IAS is used to extract the transition strength for the reaction 22Na(p,γ)23Mg.

Nuclear reactionNuclear physicsPhysicsProtonDouble beta decayIsospinNuclear TheoryHadronAtomic physicsNuclear ExperimentNucleonBeta decayRadioactive decayExotic nuclei and atomic masses (ENAM 98)
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Large-angle production of charged pions by 3 GeV/c - 12.9 GeV/c protons on beryllium, aluminium and lead targets

2008

Measurements of the double-differential pi(+/-) production cross-section in the range of momentum 100 MeV/c <= p < 800 MeV/c and angle 0.35 rad <= theta < 2.15 rad in proton-beryllium, proton-aluminium and proton-lead collisions are presented. The data were taken with the HARP detector in the T9 beam line of the CERN PS. The pions were produced by proton beams in a momentum range from 3 GeV/c to 12.9 GeV/c hitting a target with a thickness of 5% of a nuclear interaction length. The tracking and identification of the produced particles was performed using a small-radius cylindrical time projection chamber (TPC) placed inside a solenoidal magnet. Incident particles were identified by an elabo…

Nuclear reactionParticle physicsMesonProtonPhysics and Astronomy (miscellaneous)Physics::Instrumentation and DetectorsHadronNuclear TheoryFOS: Physical sciencesddc:500.201 natural sciences7. Clean energyHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Pion0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear interaction length010306 general physicsNuclear ExperimentEngineering (miscellaneous)PhysicsTime projection chamberLarge Hadron Collider010308 nuclear & particles physicsSettore FIS/01 - Fisica SperimentaleFísicaSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)Physics::Accelerator PhysicsHigh Energy Physics::ExperimentParticle Physics - Experiment
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Large-angle production of charged pions by 3 GeV/c-12 GeV/c protons on carbon, copper and tin targets

2008

A measurement of the double-differential pi(+/-) production cross-section in proton-carbon, proton-copper and proton-tin collisions in the range of pion momentum 100 MeV/c <= p <800 MeV/c and angle 0.35 rad <= theta < 2.15 rad is presented. The data were taken with the HARP detector in the T9 beam line of the CERN PS. The pions were produced by proton beams in a momentum range from 3 GeV/c to 12 GeV/c hitting a target with a thickness of 5% of a nuclear interaction length. The tracking and identification of the produced particles was done using a small-radius cylindrical time projection chamber (TPC) placed in a solenoidal magnet. An elaborate system of detectors in the beam line ensured th…

Nuclear reactionParticle physicsPhysics and Astronomy (miscellaneous)ProtonMesonPhysics::Instrumentation and DetectorsHadronNuclear TheoryFOS: Physical sciencesddc:500.201 natural sciences7. Clean energyHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Pion0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear interaction length010306 general physicsNuclear ExperimentEngineering (miscellaneous)PhysicsTime projection chamberLarge Hadron Collidercross section010308 nuclear & particles physicsSettore FIS/01 - Fisica SperimentaleFísicaSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)Physics::Accelerator PhysicsHigh Energy Physics::ExperimentParticle Physics - ExperimentEUROPEAN PHYSICAL JOURNAL C
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Low-energy (anti)neutrino physics with Borexino: Neutrinos from the primary proton-proton fusion process in the Sun

2014

The Sun is fueled by a series of nuclear reactions that produce the energy that makes it shine. The primary reaction is the fusion of two protons into a deuteron, a positron and a neutrino. These neutrinos constitute the vast majority of neutrinos reaching Earth, providing us with key information about what goes on at the core of our star. Several experiments have now confirmed the observation of neutrino oscillations by detecting neutrinos from secondary nuclear processes in the Sun; this is the first direct spectral measurement of the neutrinos from the keystone proton-proton fusion. This observation is a crucial step towards the completion of the spectroscopy of pp-chain neutrinos, as we…

Nuclear reactionPhysics - Instrumentation and DetectorsProtonneutrino: solarPhysics::Instrumentation and Detectors01 natural sciences7. Clean energynuclear reactionHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)PositronstarPrimary (astronomy)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment (nucl-ex)[ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear ExperimentNuclear Experiment[ PHYS.PHYS.PHYS-INS-DET ] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]BorexinoPhysicsSPECTROSCOPYInstrumentation and Detectors (physics.ins-det)SOLAR NEUTRINOSAstrophysics - Solar and Stellar AstrophysicsBorexinoNeutrinomodel: solardeuteronGRAN SASSOParticle physicsNuclear and High Energy PhysicsAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]talk: Conca Specchiulla 2014/09/07[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]0103 physical sciences[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsNeutrino oscillationDETECTORSolar and Stellar Astrophysics (astro-ph.SR)neutrino: modelp p: fusion010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyDeuterium13. Climate actionspectralHigh Energy Physics::Experimentneutrino: oscillationexperimental results
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C12(γ,p)11B cross section from 80 to 157 MeV

1995

The $^{12}\mathrm{C}$(\ensuremath{\gamma},p${)}^{11}$B differential cross section has been measured over proton angles ranging from 58\ifmmode^\circ\else\textdegree\fi{} to 128\ifmmode^\circ\else\textdegree\fi{}, using tagged photons of energy 80--157 MeV, for low-lying regions of residual excitation energy in $^{11}\mathrm{B}$. The data have been compared with four different types of calculation. It is shown that scaling of the cross section with momentum mismatch occurs for both the ground-state and excited-state data.

Nuclear reactionPhysicsBaryonNuclear and High Energy PhysicsProtonHadronElementary particleIsotopes of boronAtomic physicsNucleonEnergy (signal processing)Physical Review C
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