Search results for "beam"

showing 10 items of 2126 documents

The new nuclide225U

1989

In the bombardment of a 270μg/cm 2 180Hf target with48 Ca projectiles at a primary beam energy of E/A=4.24 MeV/u the new nuclide225U was produced. The experiment was performed at the velocity filter SHIP. 225U was found to decay by α emission with Eα=(7880 ±20) keV (≈90%), (7830±20) keV (≈10%) and has a half-life ofT 1/2=(80 −20 +40 ms).

PhysicsNuclear physicsNuclear and High Energy Physics010308 nuclear & particles physicsProjectileFilter (video)0103 physical sciencesNuclear fusionNuclide010306 general physics7. Clean energy01 natural sciencesBeam energyZeitschrift f�r Physik A Atomic Nuclei
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Total cross section measurement for the three double pion photoproduction channels on the proton

1995

Abstract The total cross sections for the three γp → Nππ reactions have been measured for photon energies from 400 to 800 MeV. The γ p → p π 0 π 0 and γ p → n π + π 0 cross sections have never been measured before while the γ p → p π + π − results are much improved compared to earlier data. These measurements were performed with the large acceptance hadronic detector DAPHNE, at the tagged photon beam facility of the MAMI microtron in Mainz.

PhysicsNuclear physicsNuclear and High Energy PhysicsCross section (physics)Particle physicsPhotonPionProtonHadronDetectorPhoton beamMicrotronPhysics Letters B
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In-beam electron spectrometer used in conjunction with a gas-filled recoil separator

2004

The conversion-electron spectrometer SACRED has been redesigned for use in conjunction with the RITU gas-filled recoil separator. The system allows in-beam recoil-decay-tagging (RDT) measurements of internal conversion electrons. The performance of the system using standard sources and in-beam is described.

PhysicsNuclear physicsNuclear and High Energy PhysicsInternal conversionSpectrometerPhysics::Instrumentation and DetectorsConjunction (astronomy)Physics::Accelerator PhysicsElectronNuclear ExperimentBeam electronInstrumentationRecoil separatorNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Beamline for low-energy transport of highly charged ions at HITRAP

2015

Abstract A beamline for transport of highly charged ions with energies as low as a few keV/charge has been constructed and commissioned at GSI. Complementary to the existing infrastructure of the HITRAP facility for deceleration of highly charged ions from the GSI accelerator, the new beamline connects the HITRAP ion decelerator and an EBIT with the associated experimental setups. Therefore, the facility can now transport the decelerated heavy highly charged ions to the experiments or supply them offline with medium-heavy highly charged ions from the EBIT, both at energies as low as a few keV/charge. Here we present the design of the 20 m long beamline with the corresponding beam instrument…

PhysicsNuclear physicsNuclear and High Energy PhysicsLow energyBeamlinePhysics::Instrumentation and DetectorsPhysics::Accelerator PhysicsBeam instrumentationAtomic physicsInstrumentationCharged particleIonNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Neutrino oscillation physics with a higher-γ β-beam

2004

The precision measurement and discovery potential of a neutrino factory based on boosted radioactive ions in a storage ring (“β-beam”) is re-examined. In contrast with past designs, which assume ion γ factors of ∼100 and baselines of L=130 km, we emphasize the advantages of boosting the ions to higher γ and increasing the baseline proportionally. In particular, we consider a “medium-γ” scenario (γ∼500, L∼730 km) and a “high-γ” scenario (γ∼2000, L∼3000 km). The increase in statistics, which grow linearly with the average beam energy, the ability to exploit the energy dependence of the signal and the sizable matter effects at this longer baseline all increase the discovery potential of such a…

PhysicsNuclear physicsNuclear and High Energy PhysicsNeutrino FactoryNeutrino oscillationBeam energyStorage ringBeam (structure)Energy (signal processing)Ion
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New results on hyperon decays from NA48

2001

In 1999 the NA48 experiment at CERN had two short data taking periods (8h and 40h) with a high intensity KS beam. Together with the KS mesons a large number of neutral hyperons, e.g. Λ and Ξ0, are produced. During these periods a large sample of Ξ0 decays was collected. About 115,000 events of the decay mode Ξ0 → Λπ0, about 500 of Ξ0 → Λγ, about 400 of Ξ0 → Σ0γ and about 60 events of Ξ0 → Σ+ e have been reconstructed. The status of the analyses of the above decay modes is presented.

PhysicsNuclear physicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderMesonHyperonNA48 experimentAtomic and Molecular Physics and OpticsBeam (structure)Large sampleNuclear Physics B - Proceedings Supplements
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Recent results from experiments at MAMI

2012

Abstract The Mainz Microtron MAMI is an ideal tool for studying the structure of strongly interacting systems with an electromagnetic probe. With the new HDSM accelerator stage of MAMI C, a continuous-wave electron beam with an energy of up to 1604 MeV and excellent beam quality is available for precision experiments. In addition, polarisation degrees of freedom can be exploited with polarised beams and either polarised targets or recoil polarimetry. This paper presents selected results of the A1, A2, and A4 collaborations.

PhysicsNuclear physicsNuclear and High Energy PhysicsRecoilDegrees of freedom (statistics)PolarimetryCathode rayPhysics::Accelerator PhysicsLaser beam qualityNuclear ExperimentElectron scatteringMicrotronProgress in Particle and Nuclear Physics
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In-beam studies of203, 205Bi and shell-model features of odd-a bismuth isotopes

1982

States in203, 205Bi are populated using the reaction203, 205Tl(3He,3n). Theπi13/2 single-proton states and all the members of thev(21+)⊗π h9/2 quintuplet are identified in both nuclei. The half-lives of the isomericJπ=21/2+ states in both isotopes are measured and found to be 90±7 ns and 100±6 ns, and from these values suggestions for the half-lives of the previously reportedJπ=25/2+ isomers are made. The structures of the multiplets of the formv(Pb)⊗π h9/2 are calculated in the framework of the shell model and it is shown that the main features can be derived from theπ−v−1 effective interaction. The wave functions of the 41+ and 40+ states in202, 204pb are deduced indirectly from the calcu…

PhysicsNuclear physicsNuclear and High Energy PhysicschemistryIsotopeSHELL modelNuclear fusionchemistry.chemical_elementAtomic physicsBeam (structure)BismuthZeitschrift f�r Physik A Atoms and Nuclei
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Correlated e+ e− peaks observed in heavy-ion collisions

1990

Abstract Three very narrow e + e − sum-energy peaks around 610, 750, and 810 keV have been observed in U+Th as well as in U+Ta collisions at beam energies around the Coulomb barrier. As no processes involving conventional atomic and nuclear physics were found to describe their origin, the data were in particular confronted with the hypothesis that the lines are due to the two-body decay of neutral objects in an e + e + pair. Although the 810 keV sum-energy line observed in U+Th is consistent with the prompt two-body e + e − decay of a neutral object if created nearly at rest in the heavy-ion center-of-mass system, the other lines require at least a considerably more complicated scenario if …

PhysicsNuclear physicsNuclear and High Energy PhysicschemistryTantalumCoulomb barrierThoriumchemistry.chemical_elementContext (language use)Heavy ionAtomic physicsBeam (structure)Line (formation)Physics Letters B
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In-beam study of 102In, 104In and 106In

1995

Proton-rich odd-odd In isotopes have been investigated by in-beam spectroscopic methods using the NORDBALL detector array. A Ni-58 beam with an energy of 270 MeV was used to bombard a Fe-54 target. ...

PhysicsNuclear physicsNuclear reactionNuclear and High Energy PhysicsIsotopeNuclear TheoryPhysics::Accelerator PhysicsAtomic physicsDetector arrayNuclear ExperimentBeam (structure)Energy (signal processing)Nuclear Physics A
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