Search results for "Nuclear physic"

showing 10 items of 5307 documents

Antihydrogen production within a Penning-Ioffe trap.

2008

Slow antihydrogen (H) is produced within a Penning trap that is located within a quadrupole Ioffe trap, the latter intended to ultimately confine extremely cold, ground-state H[over ] atoms. Observed H[over ] atoms in this configuration resolve a debate about whether positrons and antiprotons can be brought together to form atoms within the divergent magnetic fields of a quadrupole Ioffe trap. The number of detected H atoms actually increases when a 400 mK Ioffe trap is turned on.

Condensed Matter::Quantum GasesPhysicsAntiparticleGeneral Physics and AstronomyPenning trapTrap (computing)Nuclear physicsAntiprotonAntimatterQuadrupolePhysics::Atomic and Molecular ClustersPhysics::Atomic PhysicsIon trapAtomic physicsAntihydrogenPhysical review letters
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Antiproton confinement in a Penning-Ioffe trap for antihydrogen.

2007

Antiprotons ((p) over bar) remain confined in a Penning trap, in sufficient numbers to form antihydrogen ((H) over bar) atoms via charge exchange, when the radial field of a quadrupole Ioffe trap is added. This first demonstration with (p) over bar suggests that quadrupole Ioffe traps can be superimposed upon (p) over bar and e(+) traps to attempt the capture of (H) over bar atoms as they form, contrary to conclusions of previous analyses.

Condensed Matter::Quantum GasesPhysicsAntiparticleHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyPenning trapJNuclear physicsAntiprotonAntimatterQuadrupoleddc:550Physics::Atomic and Molecular ClustersHigh Energy Physics::ExperimentPhysics::Atomic PhysicsIon trapAtomic physicsQuadrupole ion trapAntihydrogenPhysical review letters
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Ion traps in nuclear physics—Recent results and achievements

2016

Abstract Ion traps offer a way to determine nuclear binding energies through atomic mass measurements with a high accuracy and they are routinely used to provide isotopically or even isomerically pure beams of short-living ions for post-trap decay spectroscopy experiments. In this review, different ion-trapping techniques and progresses in recent nuclear physics experiments employing low-energy ion traps are discussed. The main focus in this review is on the benefit of recent high accuracy mass measurements to solve some key problems in physics related to nuclear structure, nuclear astrophysics as well as neutrinos. Also, several cases of decay spectroscopy experiments utilizing trap-purifi…

Condensed Matter::Quantum GasesPhysicsNuclear and High Energy Physics010308 nuclear & particles physicsBinding energyNuclear structure01 natural sciencesAtomic massIonNuclear physics0103 physical sciencesNuclear astrophysicsPhysics::Atomic PhysicsNeutrino010306 general physicsSpectroscopyProgress in Particle and Nuclear Physics
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Searches for neutral Higgs bosons in e+e− collisions at centre-of-mass energies from 192 to 202 GeV

2000

Searches for neutral Higgs bosons are performed with the 237 pb-1 of data collected in 1999 by the ALEPH detector at LEP, for centre-of-mass energies between 191.6 and 201.6 GeV. These searches apply to Higgs bosons within the context of the Standard Model and its minimal supersymmetric extension (MSSM) as well as to invisibly decaying Higgs bosons. No evidence of a signal is seen. A lower limit on the mass of the Standard Model Higgs boson of 107.7 GeV/c2 at 95% confidence level is set. In the MSSM, lower limits of 91.2 and 91.6 GeV/c2 are derived for the masses of the neutral Higgs bosons h and A, respectively. For a Higgs boson decaying invisibly and produced with the Standard Model cros…

Condensed Matter::Quantum GasesPhysicsNuclear and High Energy PhysicsAlephParticle physics010308 nuclear & particles physicsElectron–positron annihilationHigh Energy Physics::PhenomenologyFOS: Physical sciencesTechnicolorContext (language use)Supersymmetry01 natural sciencesHigh Energy Physics - ExperimentStandard ModelNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Higgs bosonHigh Energy Physics::Experiment010306 general physicsParticle Physics - ExperimentBosonPhysics Letters B
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Antihydrogen production in a combined trap

1993

In this paper we study the properties of a Paul trap with a superimposed magnetic field (combined trap) and discuss the possibility of using this trap to simultaneously store positrons and antiprotons to form antihydrogen.

Condensed Matter::Quantum GasesPhysicsNuclear and High Energy PhysicsCondensed Matter PhysicsAtomic and Molecular Physics and OpticsMagnetic fieldTrap (computing)Nuclear physicsAntiprotonPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentPhysics::Atomic PhysicsIon trapPhysical and Theoretical ChemistryAtomic physicsAntihydrogenHyperfine Interactions
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Extremely cold antiprotons for antihydrogen production

1993

The possibility to produce, trap and study antihydrogen atoms rests upon the recent availability of extremely cold antiprotons in a Penning trap. Over the last five years, our TRAP Collaboration has slowed, cooled and stored antiprotons at energies 1010 lower than was previously possible. The storage time exceeds 3.4 months despite the extremely low energy, which corresponds to 4.2 K in temperature units. The first example of measurements which become possible with extremely cold antiprotons is a comparison of the antiproton inertial masses which shows they are the same to a fractional accuracy of 4×10−8. (This is 1000 times more accurate than previous comparisons and large additional incre…

Condensed Matter::Quantum GasesPhysicsNuclear and High Energy PhysicsCondensed Matter PhysicsPenning trapAtomic and Molecular Physics and OpticsNuclear physicsTrap (computing)Low energyAntiprotonHigh Energy Physics::ExperimentPhysics::Atomic PhysicsPhysical and Theoretical ChemistryAtomic physicsNuclear ExperimentAntihydrogenHyperfine Interactions
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EBIT trapping program

1993

The LLNL electron beam ion trap provides the world's only source of stationary highly charged ions up to bare U. This unique capability makes many new atomic and nuclear physics experiments possible.

Condensed Matter::Quantum GasesPhysicsNuclear and High Energy PhysicsCyclotron resonanceTrappingCondensed Matter PhysicsMass spectrometryAtomic and Molecular Physics and OpticsCharged particleIonNuclear physicsPhysics::Plasma PhysicsPhysics::Accelerator PhysicsPhysics::Atomic PhysicsPhysical and Theoretical ChemistryAtomic physicsRadioactive decayElectron ionizationElectron beam ion trapHyperfine Interactions
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Search for Higgs bosons of the minimal supersymmetric standard model in pp¯ collisions at s=1.96 TeV

2012

We report results from searches for neutral Higgs bosons produced in p-pbar collisions recorded by the Dzero experiment at the Fermilab Tevatron Collider. We study the production of inclusive neutral Higgs boson in the tautau final state and in association with a b quark in the btautau and bbb final states. These results are combined to improve the sensitivity to the production of neutral Higgs bosons in the context of the minimal supersymmetric standard model (MSSM). The data are found to be consistent with expectation from background processes. Upper limits on MSSM Higgs boson production are set for Higgs boson masses ranging from 90 to 300 GeV. We exclude tanBeta>20-30 for Higgs boson ma…

Condensed Matter::Quantum GasesPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyElementary particleTechnicolor01 natural sciences7. Clean energyBottom quarkStandard ModelNuclear physicssymbols.namesake0103 physical sciencessymbolsHiggs bosonHigh Energy Physics::Experiment010306 general physicsHiggs mechanismMinimal Supersymmetric Standard ModelBosonPhysics Letters B
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Bose-Einstein correlations in W-pair decays

2000

Bose-Einstein correlations are studied in semileptonic (WW --> q (q) over bar lv) and fully hadronic (WW --> q (q) over bar q (q) over bar) W-pair decays with the ALEPH detector at LEP at centre-of-mass energies of 172, 183 and 189 GeV. They are compared with those made at the Z peak after correction for the different flavour compositions. A Monte Carlo model of Bose-Einstein correlations based on the JETSET hadronization scheme was tuned to the Z data and reproduces the correlations in the WW --> q (q) over bar lv events. The same Monte Carlo reproduces the correlations in the WW --> q (q) over bar q (q) over bar channel assuming independent fragmentation of the two W's. A variant of this …

Condensed Matter::Quantum GasesPhysicsNuclear and High Energy PhysicsParticle physicsBose Einstein correlations010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyLEPBose–Einstein correlations01 natural sciencesALEPH ExperimentNuclear physicsALEPH Experiment; LEP; Bose Einstein correlations0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::Experiment010306 general physicsALEPH experimentParticle Physics - Experiment
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A single trapped antiproton and antiprotons for antihydrogen production

1993

During the last several years, our TRAP collaboration has pioneered techniques for slowing, trapping, cooling and indefinitely storing antiprotons to energies more than 1010 times lower than previously possible. The radio signal from a single trapped antiproton is now being used for precision measurements. Many cold antiprotons are “stacked” as another important step toward the eventual production of antihydrogen, and positrons have been trapped in vacuum.

Condensed Matter::Quantum GasesPhysicsNuclear and High Energy PhysicsParticle physicsTrappingCondensed Matter PhysicsAtomic and Molecular Physics and OpticsTrap (computing)Nuclear physicsAntiprotonRadio signalPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentPhysics::Atomic PhysicsPhysical and Theoretical ChemistryAntihydrogenHyperfine Interactions
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