Search results for "Proton"

showing 10 items of 5886 documents

Two-body photodisintegration of the deuteron from 100 to 800 MeV

1996

Abstract The total and the differential cross sections for the D(γ,p)n reaction have been measured over the photon energy range 100-800 MeV at the 855 MeV MAMI Microtron in Mainz. Using the large acceptance detector DAPHNE in conjunction with the Glasgow tagging spectrometer, high precision results with small systematic errors were obtained. The data are presented in the form of thirty-five angular distributions at c.m. proton angles between 30°–160° in 10° intervals and at photon energies in steps of 20 MeV. Previous experimental work is reassessed in the light of the present results and comparison with some recent theoretical calculations.

Nuclear physicsNuclear reactionPhysicsNuclear and High Energy PhysicsPhotonProtonDeuteriumSpectrometerPhotodisintegrationPhysics::Accelerator PhysicsPhoton energyNuclear ExperimentMicrotronNuclear Physics A
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Lifetimes of yrast states in 110Cd

1993

Abstract Lifetimes or lifetime limits of 20 yrast levels in 110 Cd have been measured using the recoil-distance method and the NORDBALL array of Compton-suppressed Ge detectors. From the reduced transition probabilities competing rotational and vibrational behaviour of 110 Cd is revealed. Also non-collective states, associated with proton configurations, have been observed.

Nuclear physicsNuclear reactionPhysicsNuclear and High Energy PhysicsProtonYrastAtomic physicsNuclear ExperimentNuclear Physics A
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Gamow-Teller Transitions and β-decay Half-life in Proton Rich pf-shell Nuclei

2010

In violent neutrino‐induced reactions at the core‐collapse stage of type II supernovae, Gamow‐Teller (GT) transitions starting from stable as well as unstable pf‐shell nuclei play important roles. In the β‐decay study of these unstable pf‐shell nuclei, half‐lives can be measured rather accurately. On the other hand, in high‐resolution (3He,t) charge‐exchange reactions at 0°, individual GT transitions up to high excitations can be studied. Assuming the isospin symmetry for the strengths of Tz = ±2→±1 analogous GT transitions, we present a “merged analysis” for the determination of GT transition strengths starting from proton‐rich Tz = −2 nuclei. We applied this analysis to the A = 52, T = 2 …

Nuclear physicsNuclear reactionPhysicsProtonIsospinNuclear TheoryHadronFermionAtomic physicsNuclear ExperimentNucleonIsotopes of heliumRadioactive decayAIP Conference Proceedings
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On the Road to FAIR: 1st Operation of AGATA in PreSPEC at GSI

2013

International audience; The Facility for Antiproton and Ion Research (FAIR), under construction at Darmstadt will provide intense relativistic beams of exotic nuclei at its Superconducting-FRagment Separator. High-resolution in-beam γ-ray spectroscopy will be performed in the HISPEC experiment, using the European Advanced GAmma-ray Tracking Array (AGATA). The PreSPEC-AGATA campaign is the predecessor of HISPEC and runs from 2012 to 2014 at GSI Helmholtzzentrum für Schwerionenforschung GmbH. Up to19 AGATA modules were used at GSI's F Ragment Separator in 2012. We report on the status of the experiment including preliminary results from performance commissioning.

Nuclear physicsPhysics010308 nuclear & particles physicsPhysicsQC1-9990103 physical sciencesSubatomic PhysicsFacility for Antiproton and Ion ResearchAGATA[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]010306 general physics7. Clean energy01 natural sciencesEPJ Web of Conferences
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Fragment mass distribution in superasymmetric region in proton-induced fission of U and Th

1998

Fission fragment mass distributions down to super-asymmetric mass region and both pre- and post-scission neutron multiplicity for238U(p,fission) reaction atEp = 20, 35, 50, 60 MeV and for232Th(p, fission) reaction atEp = 50, 60 MeV were measured using HENDES set-up. The results indicate enhancement for super-asymmetric mass division at intermediate excitation energies.

Nuclear physicsPhysicsCold fissionCluster decayMass distributionProtonFissionFragment (computer graphics)Nuclear TheoryAtomic physicsNuclear ExperimentNeutron multiplicityExcitationIl Nuovo Cimento A
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Antiproton annihilation at rest in liquid deuterium into π−π0π0pS

1994

With the Crystal Barrel detector, the final state π−π0π0pS at rest in liquid deuterium was measured for the first time. A preliminary partial-wave analysis was performed, which required two interesting features: besides the ρ(770), a second pole was needed in the ππP-wave and a narrow resonance in the ππS-wave, slightly above 1500 MeV/c2. With the same parametrization a high-statistics π+π−π0 data set could also be well described.

Nuclear physicsPhysicsCrystalAnnihilationDeuteriumAntiprotonPartial wave analysisResonanceDalitz plotAtomic physicsParametrizationIl Nuovo Cimento A Series 11
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Proton-Rich Light Nuclei

1989

A basic question for a given element of how few or how many neutrons can be contained in its nucleus and still result in a “bound” system, and the resulting consequences on our present concept of nuclear structure, have been the focus of much recent research on highly unstable nuclei. It is only during the last several years that the limit of nuclear stability has been reached in a few areas of the nuclear chart. Except among the lightest elements, knowledge of the limit on the neutron-excess side is still beyond our experimental capability. For the heavier elements, the gap between the most neutron-rich isotope known and the isotope which is predicted to define the neutron drip-line more o…

Nuclear physicsPhysicsIsotopeProtonProton bindingNeutron numberNuclear TheoryNuclear structureNeutronAtomic numberNuclideNuclear Experiment
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Prospects for a DVCS measurement at COMPASS

2010

The high energy polarised muon beam available at CERN with the option of using positive or negative muons with opposite polarisation gives COMPASS an excellent possibility to study generalised parton distributions via deeply virtual Compton scattering. In a first step we propose to use an unpolarised proton target to study the slope of the t dependence of the differential cross section as a function of xB j to observe a possible shrinkage of the nucleon with increasing xB j. Furthermore, the beam charge and spin difference will be measured over a wide kinematical range to determine the Compton form factor related to the GPD H. As a second step we consider to use a transversely polarised pro…

Nuclear physicsPhysicsLarge Hadron ColliderMuonProtonCompassForm factor (quantum field theory)Compton scatteringPartonNuclear ExperimentNucleonProceedings of XVIII International Workshop on Deep-Inelastic Scattering and Related Subjects — PoS(DIS 2010)
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Facilities and Methods: Heavy Element Spectroscopy at JYFL

2007

A central theme throughout the history of experimental nuclear physics has been the pursuit of nuclei at the extremes. These extremes, be they in terms of mass, proton-to-neutron ratio, or spin and excitation energy, provide the most stringent tests for our current nuclear structure theories. The pursuit of these extremes also provides impetus to develop and exploit new techniques and instrumentation. At the Department of Physics of the University of Jyvaskyla (JYFL), a major part of the experimental program is devoted to the study of heavy nuclei along the proton dripline and superheavy nuclei in the transfermium region. This program was initiated in the mid-1990s when a small array of TES…

Nuclear physicsPhysicsNuclear and High Energy PhysicsCardinal pointProtonInstrumentationNuclear TheoryNuclear structureRadiationNuclear ExperimentSpin (physics)ExcitationCharged particleNuclear Physics News
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Superasymmetric fission at intermediate energy and production of neutron-rich nuclei with A < 80

1997

Abstract The yields of neutron-rich Ni, Cu, Zn, Ga and Ge-isotopes were measured in 25 MeV proton induced fission of 238 U using the ion guide-based isotope separator technique. The results indicate enhancement for superasymmetric mass division at intermediate excitation energy of the fissioning nucleus and show the potential of this reaction for the production of neutron-rich exotic nuclei around Z = 28.

Nuclear physicsPhysicsNuclear and High Energy PhysicsCold fissionCluster decayProtonIsotopeFissionNuclear fissionNuclear TheoryNeutronFission product yieldNuclear ExperimentPhysics Letters B
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