Search results for "Physics::Accelerator Physics"

showing 10 items of 1235 documents

Neutron-rich nuclei and fission; recent developments and future aspects

2002

Production and studies of neutron-rich nuclei produced in fission are reviewed. Some recent experiments performed with the ISOL technique at the IGISOL and the ISOLDE facilities are reviewed. The manipulation of neutron-rich nuclei is discussed with a special focus on radioactive ion cooling and trapping techniques under construction worldwide. Perspectives of obtaining intense post accelarated beams of fission products are discussed.

Nuclear physicsPhysicsNuclear and High Energy PhysicsFission productsIon coolingFissionNuclear engineeringNuclear TheoryPhysics::Accelerator PhysicsNuclear fusionNeutronNuclear ExperimentThe European Physical Journal A
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A spin rotator for producing a longitudinally polarized electron beam with MAMI

1993

Abstract The design and performance characteristics of a full 4 π-space spin rotator for 100 keV electrons are described. The spin rotator was developed as part of the acceleration scheme for polarized electrons in the MAINZ race track microtron cascade MAMI [1]. It allows to orientate the polarization vector in any direction before injection. Thus it is possible to optimize the longitudinal polarization component, required for experiments with polarized high energy electrons, at target position. With this scheme various experimental halls can be supplied with longitudinally polarized electrons in the full energy range of MAMI between 180 and 855 MeV.

Nuclear physicsPhysicsNuclear and High Energy PhysicsHigh energyCascadeCathode rayPhysics::Accelerator PhysicsElectronNuclear ExperimentPolarization (waves)InstrumentationMicrotronRace trackNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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High-resolution γ-ray spectroscopy: a versatile tool for nuclear β-decay studies at TRIUMF-ISAC

2005

High-resolution γ-ray spectroscopy is essential to fully exploit the unique, high-quality beams available at the next generation of radioactive ion beam facilities such as the TRIUMF isotope separator and accelerator (ISAC). The 8π spectrometer, which consists of 20 Compton-suppressed HPGe detectors, has recently been reconfigured for a vigorous research programme in weak interaction and nuclear structure physics. With the addition of a variety of ancillary detectors it has become the world's most powerful device dedicated to β-decay studies. This paper provides a brief overview of the apparatus and highlights from recent experiments.

Nuclear physicsPhysicsNuclear and High Energy PhysicsIon beamSpectrometerPhysics::Accelerator PhysicsHigh resolutionGamma spectroscopyWeak interactionNuclear ExperimentHpge detectorSpectroscopyRadioactive decayJournal of Physics G: Nuclear and Particle Physics
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Energy and range focusing of in-flight separated exotic nuclei – A study for the energy-buncher stage of the low-energy branch of the Super-FRS

2003

Abstract The relative momentum spread of in-flight separated exotic nuclear beams produced in fragmentation and/or fission reactions is of the order of a few percent. A new technique is presented, which reduces the momentum spread significantly, and first experimental results obtained with relativistic projectile fragments are shown. This technique is the key to experiments with slowed-down and stopped beams, in particular for the efficient stopping of relativistic exotic nuclei in gas-filled stopping cells. It will be employed at the energy-buncher stage of the low-energy branch of the Super-FRS facility. The ion-optical design of the energy buncher is presented and a brief outlook to the …

Nuclear physicsPhysicsNuclear and High Energy PhysicsLow energyFissionProjectileNuclear TheoryPhysics::Accelerator PhysicsNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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New experimental efforts along the rp-process path

2007

The level structure just above the proton threshold of the nucleus 30S has been studied using the neutron removal process on fast radioactive beams at the National Superconducting Cyclotron Laboratory (NSCL) at Michigan State University. In this work we provide a description of the experimental setup. The present status of the analysis is also discussed.

Nuclear physicsPhysicsNuclear and High Energy PhysicsSuperconducting cyclotronProtonNuclear TheoryPath (graph theory)Physics::Accelerator PhysicsLevel structureNeutronrp-processNuclear ExperimentJournal of Physics G: Nuclear and Particle Physics
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Radioactive beams at GSI

2001

Abstract After a brief introduction the production of relativistic beams of exotic nuclei will be discussed and some characteristic examples from the ongoing GSI nuclear structure research programme are presented, such as: nuclear reactions with exotic beams to explore nuclear skins, the structure of halo nuclei, and direct mass measurements in a storage ring. Heavy-element research will be addressed briefly. A possible next generation exotic beam facility at GSI will be outlined.

Nuclear physicsPhysicsNuclear reactionNuclear and High Energy PhysicsNuclear TheoryNuclear structurePhysics::Accelerator PhysicsHaloNuclear ExperimentStorage ringBeam (structure)Progress in Particle and Nuclear Physics
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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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Measurement of differentialJ/ψproduction cross sections and forward-backward ratios inp + Pbcollisions with the ATLAS detector

2015

Measurements of differential cross sections for J/psi production in p + Pb collisions at root S-NN= 5.02 TeV at the CERN Large Hadron Collider with the ATLAS detector are presented. The data set us ...

Nuclear physicsPhysicsQuarkNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderPhysics::Instrumentation and DetectorsAtlas detectorAtlas (topology)Physics::Accelerator PhysicsHigh Energy Physics::ExperimentForward backwardNuclear ExperimentPhysical Review C
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Future Experimental Developments for Few-Body Physics at Mainz

1986

The racetrack microtron MAMI B [1] now under construction at Mainz will provide a high-intensity electron beam with energies up to 840 MeV. The 100% duty factor, high-quality beam is considered to be ideal for the investigation of the nucleus in the medium energy region. Coincidence experiments with the detection of the scattered electron and the hadronic reaction products will become possible in a wide kinematical range yielding the information about the response of the nucleus to the transferred energy and momentum. By the method of bremsstrahlung tagging intense secondary photon beams with high monochromacity and well known fluxes will be available for photonuclear research work. Further…

Nuclear physicsPhysicsRange (particle radiation)HadronBremsstrahlungCathode rayPhysics::Accelerator PhysicsElectronNuclear ExperimentMicrotronBeam (structure)Coincidence
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Mass Analyzing Recoil Apparatus, MARA

2019

An in-flight zero-angle mass separator, MARA, has been recently constructed and commissioned at the University of Jyväskylä, Finland. MARA is a double focusing device, consisting of a quadrupole driplet, electrostatic deflector, and magnetic dipole. This separator is built for nuclear structure studies to be performed around the N∼Z line and at beyond the proton drip line. peerReviewed

Nuclear physicsPhysicsRecoilta114research equipmentnuclear physicsNuclear TheorytutkimuslaitteetGeneral Physics and AstronomyPhysics::Accelerator PhysicsNuclear ExperimentydinfysiikkaActa Physica Polonica B
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