Search results for "Proton"

showing 10 items of 5886 documents

First Antiprotons in an Ion Trap

1987

Measurements of the antiproton mass[2,3,4,5] are represented in Fig. 1. All of these are deduced from measurements of the energy of x-rays radiated from highly excited exotic atoms. For example, if an antiproton is captured in a Pb atom, it can make radiative transitions from its n = 20 to n = 19 state. The antiproton is still well outside the nucleus in this case, so that nuclear effects can be neglected. The measured transition energy is essentially proportional to the reduced mass of the nucleus and hence the antiproton mass can be deduced by comparing the measured values with theoretical values, corrected for QED effects. The most accurate quoted uncertainty is 5 × 10-5 and is consisten…

Nuclear physicsPhysicsProtonAntiprotonExcited stateAtomPhysics::Accelerator PhysicsPhysics::Atomic PhysicsElectronReduced massNuclear ExperimentStorage ringExotic atom
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The HypHI project at GSI and FAIR

2008

Even though both experimental and theoretical activities on hypernuclear physics have been extended by a number of international projects, direct measurements on hypernuclear magnetic moments and studies of hypernuclei at extreme isospins have never been performed. The international HypHI collaboration proposes to perform hypernuclear spectroscopy with stable heavy ion beams and rare isotope beams at GSI and FAIR in order to study neutron and proton rich hypernuclei and to measure directly hypernuclear magnetic moments. The project is divided into four phases. In the first Phase 0 experiment, the feasibility of precise hypernuclear spectroscopy with heavy ion beams will be demonstrated by o…

Nuclear physicsPhysicsProtonIsotopeMagnetic momentNuclear TheoryNeutronHeavy ionNuclear ExperimentSpectroscopyNucleonPhysics::History of Physics
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Proton-Neutron QRPA

2007

We discussed proton—neutron two-quasiparticle excitations and their electromagnetic and beta decays in Chap. 15. In Chap. 17 we introduced the pn-QTDA, the simplest configuration mixing scheme of these excitations. The vacuum of the pnQTDA is the BCS vacuum, and the solutions of the pn-QTDA satisfy a variational principle.1

Nuclear physicsPhysicsProtonMatrix elementNeutronBeta (velocity)Beta decayMixing (physics)
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Decay Spectroscopy for Nuclear Astrophysics: β-delayed Proton Decay

2011

In several radiative proton capture reactions important in novae and XRBs, the resonant parts play the capital role. We use decay spectroscopy techniques to find these resonances and study their properties. We have developed techniques to measure beta- and beta-delayed proton decay of sd-shell, proton-rich nuclei produced and separated with the MARS recoil spectrometer of Texas A&M University. The short-lived radioactive species are produced in-flight, separated, then slowed down (from about 40 MeV/u) and implanted in the middle of very thin Si detectors. This allows us to measure protons with energies as low as 200 keV from nuclei with lifetimes of 100 ms or less. At the same time we measu…

Nuclear physicsPhysicsProtonProton decayAstrophysics::High Energy Astrophysical PhenomenaIsotopes of chlorineNuclear astrophysicsAtomic physicsNuclear ExperimentNucleonBeta decayParticle detectorRadioactive decayAIP Conference Proceedings
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<title>Studies of the activation background in CsI(Tl) detectors</title>

1993

CsI scintillation crystals are widely used as detection in (gamma) -ray astronomy observations. In the MeV energy region, one of the most important background sources in CsI is the (beta) decays induced in the crystal by cosmic ray protons and their secondaries. One recent idea for reducing this background is to use discrete detector arrays to reject the large amount of localized (beta) decay events. Two experiments were carried out with 1 cm3 CsI crystals bombarded with energetic proton beams and fast/thermal neutrons, with the aim of evaluating the effectiveness of this method in pixelated (1 cm3) CsI detectors. The ratio of the number of decays resulting in single site and multiple site …

Nuclear physicsPhysicsScintillationPhotonProtonPhysics::Instrumentation and DetectorsDetectorSpallationCosmic rayNeutronNuclear ExperimentNeutron temperatureSPIE Proceedings
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A new plunger device to measure lifetimes of unbound states in tagged exotic nuclei

2012

A new plunger device has been designed and is being built at the University of Manchester to measure lifetimes of unbound states in exotic nuclei approaching the proton drip-line. The device is designed to work in both vacuum and gas environments and will be used in conjunction with the gas filled separator RITU and the vacuum-mode separator MARA at the University of Jyvaskyla, Finland. This will enable the accurate measurement of excited state lifetimes identified via isomer and charged-particle tagging. The plunger will be used to address many key facets of nuclear structure physics with particular emphasis on the effect of deformation on proton emission rates.

Nuclear physicsPlungerHistoryChemistryExcited stateNuclear TheoryNuclear structureSeparator (oil production)Atomic physicsProton emissionNuclear ExperimentComputer Science ApplicationsEducationJournal of Physics: Conference Series
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Experiments on threshold pion electroproduction

2008

Experimental techniques to access the reactions p(e, e′ p)π0 and d(e, e′ d)π0 at low four momentum transfer and close to threshold are presented. For p(e, e′ p)π0 results at Q 2=0.1 GeV2/c 2 are given and compared to chiral perturbation theory. A new experimental program on d(e, e′ d)π0 is presented.

Nuclear physicsRecoil protonPhysicssymbols.namesakeParticle physicsTransfer (group theory)Chiral perturbation theoryPionLorentz transformationsymbolsFour-momentum
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Proton-Deuteron Elastic Scattering for E > 0

1999

We report on the first reliable numerical results for proton-deuteron elastic scattering observables for energies above the deuteron breakup thresh- old, for the Paris potential. The calculations have been performed within the screening and renormalisation approach. The theoretical results are compared with recent experimental data.

Nuclear physicsScattering amplitudePhysicsElastic scatteringQuasielastic scatteringPhonon scatteringProtonNuclear TheoryScattering lengthInelastic scatteringNuclear ExperimentBreakup
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Real and Virtual Compton Scattering (experiments)

1999

This paper deals with Real and Virtual Compton Scattering off the proton at threshold and the way to deduce information about the nucleon polarizabilities.

Nuclear physicsScattering cross-sectionPhysicsAnomalous magnetic dipole momentProtonAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryPhysics::Atomic and Molecular ClustersCompton scatteringNuclear ExperimentNucleon
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Beta delayed alpha emission from the neutron deficient rare earth isotopes [sup 152]Tm and [sup 150]Ho

2011

The study of beta‐delayed proton emission is a well known method to aid the determination of the beta strength distribution in nuclei far from the stability line. At the neutron deficient side of the nuclear chart the process of proton or alpha emission from excited states is energetically allowed when one goes far enough from stability. However, beta‐delayed alphas have seldom been measured for nuclei heavier than A  =  20. Here we present a study of the beta‐delayed alpha‐particle emission from 152Tm and 150Ho and their importance in the full B(GT) distribution. © 2011 American Institute of Physics

Nuclear physicsTotal absorption spectroscopyProtonChemistryNuclear TheoryNeutronAlpha particleAlpha decayProton emissionAtomic physicsNuclear ExperimentBeta decayRadioactive decayAIP Conference Proceedings
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