Search results for " Helium"

showing 10 items of 151 documents

Physics at CERN's Antiproton Decelerator

2013

The Antiproton Decelerator of CERN began operation in 1999 to serve experiments for studies of CPT invariance by precision laser and microwave spectroscopy of antihydrogen ($\bar{\rm H}$) and antiprotonic helium ($\bar{p}{\rm He}^+$). The first 12 years of operation saw cold $\bar{\rm H}$ synthesized by overlapping clouds of positrons ($e^+$) and antiprotons ($\bar{p}$) confined in magnetic Penning traps. Cold $\bar{\rm H}$ was also produced in collisions between Rydberg positronium atoms and $\bar{p}$. Ground-state $\bar{\rm H}$ was later trapped for up to $\sim 1000$ s in a magnetic bottle trap, and microwave transitions excited between its hyperfine levels. In the $\bar{p}{\rm He}^+$ ato…

Nuclear and High Energy PhysicsAtomic Physics (physics.atom-ph)Other Fields of PhysicsFOS: Physical sciences7. Clean energy01 natural sciencesPhysics - Atomic PhysicsHigh Energy Physics - ExperimentPositroniumHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentHyperfine structureAntiprotonic heliumPhysicsMagnetic moment010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyMass ratioAntiproton Decelerator13. Climate actionAntiprotonHigh Energy Physics::ExperimentRotational spectroscopyAtomic physics
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Cryogenic helium as stopping medium for high-energy ions

2008

We have investigated the survival and transport efficiency of Ra-219 ions emitted by a Ra-223 source in high-density cryogenic helium gas, with ionisation of the gas induced by a proton beam. The combined efficiency of ion survival and transport by an applied electric field was measured as a function of ionisation rate density for electric fields up to 160 V/cm and for three temperature and density combinations: 77 K, 0.18 mg/cm(3), 10 K, 0.18 mg/cm(3) and 10 K, 0.54 mg/cm(3). At low beam intensity or high electric field, an efficiency of 30%, is obtained, confirming earlier results. A sharp drop in efficiency is observed at a "threshold" ionisation rate density which increases with the squ…

Nuclear and High Energy PhysicsEXTRACTIONSHIPTRAPCATCHERField (physics)ProtonChemistrychemistry.chemical_elementRECOMBINATIONElectronPlasmaBEAMSIonCryogenic helium gasGets catcherSUPERFLUID-HELIUMGASIonizationElectric fieldIons in heliumAtomic physicsInstrumentationRadioactive ion beamsHeliumNuclear Instruments & Methods in Physics Research Section B-Beam Interactions with Materials and Atoms
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High-precision measurement of the electron spin g factor of trapped atomic nitrogen in the endohedral fullerene N@C60

2018

Abstract The electronic g factor carries highly useful information about the electronic structure of a paramagnetic species, such as spin-orbit coupling and dia- or paramagnetic (de-)shielding due to local fields of surrounding electron pairs. However, in many cases, a near “spin-only” case is observed, in particular for light elements, necessitating accurate and precise measurement of the g factors. Such measurement is typically impeded by a “chicken and egg situation”: internal or external reference standards are used for relative comparison of electron paramagnetic resonance (EPR) Larmor frequencies. However, the g factor of the standard itself usually is subject to a significant uncerta…

Nuclear and High Energy PhysicsElectron pairMaterials scienceFullereneLiquid heliumBiophysics02 engineering and technologyElectronic structure010402 general chemistry021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesBiochemistryArticle0104 chemical scienceslaw.inventionParamagnetismlawPhysics::Atomic and Molecular ClustersEndohedral fullereneMolecular orbitalAtomic physics0210 nano-technologyElectron paramagnetic resonanceJournal of Magnetic Resonance
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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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Structure of exotic 7He and 9He

2004

The heavy helium isotopes 7,9 He were studied via their isobaric analog states (IAS) in 7,9 Li. The IAS were populated via resonance reactions of protons with radioactive beams of 6,8 He. The isospin-conserving neutron decay of T=3/2 resonances in 7 Li and proton decay of T=5/2 resonances in 9 Li were measured. New spectroscopic information on these states were obtained, and compared with the properties of levels in 7,9 He.

Nuclear physicsPhysicsNuclear and High Energy PhysicsProton decayNuclear TheoryIsobaric processResonanceNeutronAtomic physicsNuclear ExperimentIsotopes of heliumNuclear Physics A
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Comparison of T[sub z] = ±1→0 GT Transitions

2010

Gamow‐Teller (GT) transitions can be studied in both β‐decay and charge exchange(CE) reactions. If isospin is a good quantum number, then the Tz = −1→0 and Tz = +1→0 GT mirror transitions, are identical. Therefore, a comparison of the results from studies of β decay and CE should shed light on this assumption. Accordingly we have studied the β decay of the Tz = −1 fp‐shell nuclei, 54Ni, 50Fe, 46Cr, and 42Ti, produced in fragmentation and we have compared our results with the spectra from (3He, t) measurements on the mirror Tz = +1 target nuclei studied in high resolution at RCNP, Osaka. The β‐decay experiments were performed as part of the STOPPED beam RISING campaign at GSI.

Nuclear physicsPhysicsNuclear reactionIsospinHelium-3Atomic physicsQuantum numberIsotopes of heliumBeta decayRadioactive decaySpectral lineAIP Conference Proceedings
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Gamow-Teller Transitions Studied in ([sup 3]He, t) Reaction and Analogous β decay

2010

Due to the simplicity of the στ operator that causes Gamow‐Teller (GT) transitions, they are the most popular nuclear weak process in the Universe. The GT transitions in pf‐shell nuclei, for example, starting from stable Tz = +1 and proton‐rich Tz = +1 nuclei, where Tz = (N−Z)/2, play important roles in the supernova‐explosion or rp‐process nucleosynthesis. In the β‐decay study of pf‐shell nuclei, half‐lives can be measured rather accurately. On the other hand, in a high‐resolution (3He, t) charge‐exchange reaction at 0°, individual GT transitions up to high excitations can be studied. In order to derive reliable GT transition strengths B(GT), we present a unique analysis that combines the …

Nuclear physicsPhysicsNuclear reactionNucleosynthesisIsospinHadronElementary particleAtomic physicsNucleonIsotopes of heliumRadioactive decayAIP Conference Proceedings
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Comparison of T[sub z] = ±1→0 GT Transitions Studied in β—decay and CE Reactions

2010

Gamow‐Teller (GT) transitions can be studied in both β‐ decay and charge exchange(CE) reactions. If isospin is a good quantum number, then the Tz = −1→0 and Tz = +1→0 GT mirror transitions, are identical. Therefore, a comparison of the results from studies of β decay and CE should shed light on this assumption. Accordingly we have studied the β decay of the Tz = −1 fp‐shell nuclei, 54Ni, 50Fe, 46Cr, and 42Ti, produced in fragmentation and we have compared our results with the spectra from (3He, t) measurements on the mirror Tz = +1 target nuclei studied in high resolution at RCNP, Osaka. The experiments were performed as part of the STOPPED beam RISING campaign at GSI.

Nuclear reactionChemistryExcited stateIsospinHelium-3Atomic physicsIsotopes of heliumBeta decayCharged particleRadioactive decayAIP Conference Proceedings
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Heat and Helium Production during Exothermic Reactions between Gases through Palladium Geometrical Elements Loaded with Hydrogen

2000

In this research, the effect of the shape of hydrogen-loaded palladium elements on exothermic reactions between gases is shown. It was found that an element with parts of its surface next to each o...

Nuclear reactionExothermic reactionMaterials scienceHydrogenGeneral Engineeringchemistry.chemical_elementCold fusionChemical engineeringchemistryNuclear fusionAtomic physicsIsotopes of heliumHeliumPalladiumFusion Technology
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TheNd150(He3,t) andSm150(t,He3) reactions with applications toββdecay ofNd150

2011

The {sup 150}Nd({sup 3}He,t) reaction at 140 MeV/u and {sup 150}Sm(t,{sup 3}He) reaction at 115 MeV/u were measured, populating excited states in {sup 150}Pm. The transitions studied populate intermediate states of importance for the (neutrinoless) {beta}{beta} decay of {sup 150}Nd to {sup 150}Sm. Monopole and dipole contributions to the measured excitation-energy spectra were extracted by using multipole decomposition analyses. The experimental results were compared with theoretical calculations obtained within the framework of the quasiparticle random-phase approximation, which is one of the main methods employed for estimating the half-life of the neutrinoless {beta}{beta} decay (0{nu}{b…

Nuclear reactionPhysicsNuclear and High Energy Physics010308 nuclear & particles physicsResonance01 natural sciencesBeta decayHelium-3Double beta decay0103 physical sciencesAtomic physicsNeutrino010306 general physicsIsotopes of heliumRadioactive decayPhysical Review C
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